TW200919527A - Fluorescent discharge lamp tube of novel structure and LCD display device - Google Patents

Abstract

The invention provides a fluorescent discharge lamp tube, which comprises independent inner and outer circuits of electron flow and has the character of high light-up. Around electric insulated particles covered with metal electrodes, the inner circuit is employed to form electron cloud and ion cloud produced from electricity discharge gas ionization for use as the power source. The gas discharges while the electron of the electron cloud migrates to the ion cloud. The electron and the ion are combined into gas and the inner circuit is then closed. Gas discharging is performed without inputting electron into the outer circuit, without the exposure of metal and without metal evaporation so that the lifetime can be longer. As the electron of initial speed close to zero is used, the cathode voltage drop (40 percent of the entirety) inevitably encountered in the conventional skill can be avoided to greatly reduce light-up electricity. Fluorescent film is made from the mixed powder of electron beam phosphor and photo-phosphor. The electron flow of conduction on the surface of the fluorescent film is applied to leading the start of the discharge, thereby achieving the instantaneous light-up and the entire surface light-up in about 10 milliseconds. If several fluorescent discharge lamp tubes of the invention are applied to backlight of LCD for proceeding linearly sequential scan, the picture quality of LCD screen can be greatly enhanced.

Description

200919527 IX. Description of the Invention: [Technical Field] The present invention relates to a fluorescent discharge lamp which emits a mixed gas of argon (Ar) and mercury (Hg) vapor by inelastic collision of electrons. And by using the fluorescent film coated on the inner wall surface of the fluorescent discharge lamp to convert the strong 254 nm invisible ultraviolet light emitted by Hg into visible light, and more specifically, the present invention relates to a novel fluorescent light. A discharge lamp tube and an LCD (Liquid Crystal Display) display device using the same, by changing the basic structure of the fluorescent discharge lamp, although the power consumption of the discharge lamp is lower than that of the conventional fluorescent lamp The discharge lamp is lit, but can be illuminated with a high brightness of more than twice the brightness of the conventional light discharge lamp. [Prior Art] [Preferred discharge lamp and outline of the present invention] The discharge of a conventional fluorescent discharge lamp is a cold cathode electrode (c〇id Ca-de Flu〇rescent Lamps, coffee) or a hot cathode electrode (5) (10) ode Fluoresceni Lamps, HCFL) removes the electrons required for discharge. The common thing about J et al. is that the electrons taken out from the electrode have high energy.

Set: and the method of strong traveling gas space is adopted, so there is a complicated phenomenon during the period until the electric power is required to discharge the gas L ... b, and :: causing the cathode electric power to be greatly reduced. The cathode electricity repeatedly reduces the total disk illuminating value to the energy required for the above-mentioned oxygen discharge of the ancient ship, "the overall required energy is about 40%. And the non-self-metal electrode takes out the gas discharge tube at both ends of the tube. The electrons are separated from each other; the electricity is discharged in the discharge tube with the gas discharge in the ion cloud 'removed from the electron cloud ^ ^ §| , . The gas is caused to discharge in the process, and the electrons reaching 1 + are separated from the ions by the counter ion cloud ^ ^ and 0 5 . With the gas on the inside of the electrician, the electronic cloud is used to form the hip, and the enemy is used as the driving source. The electrons taken out from Leigong can be reduced to the above-mentioned cathode voltage. When the 'mouth is ' and the same tube lighter + surname, compared with the .tet ^ pen lamp, the fluorescent light of the present invention can be illuminated by 40% or less. The invention is based on the invention, and the fluorescent discharge lamp of the present invention is eliminated by the change of the cathode discharge voltage caused by the decrease of the cathode voltage of the fluorescent discharge lamp. ...... The result is that the tube end of the self-discharge lamp spreads over the entire surface & with uniform intensity. The conventional illusion surface ^ rp, . m . The internal cause emits electricity and the electric power is lowered, and the heat is used. However, the fluorescent light of the present invention, the Leizhong bean official, does not produce sputum, and the sputum is exposed to the metal electrode in the gas, so too & The sub-destroy is very long. Therefore, the gas discharge of the fluorescent lamp of the present invention is known as the gas discharge of the fluorescent discharge lamp ^ _ JL pa θ§ ρ , the existence of the long J is not solved ^ ^ ^ The mechanism of the point redundancy is not Clearly, therefore, the various improvements are only the point of application to the fluorescent discharge lamp tube based on the urinary test. The inventors have for the first time clarified the gas control system. 5 + 'Electrical points are affected by the main machine 2* U The control of the surface conduction electrons that migrate on the fluorescent film. The gas discharges him from the Dian point shell. The problem can be solved by the βΛ% release of the phosphor coated in the fluorescent discharge tube and the arrangement of the selected phosphor particles. The result is & The fluorescent discharge lamp has a characteristic that the fluorescent discharge lamp is instantaneously lit in about 1 millisecond. Even if the brightness of the fluorescent film is increased, the brightness of the fluorescent film 200919527 is saturated. The saturation phenomenon is 5〇. For the rest of the year—there is no solution. This saturation restricts the brightness of the fluorescent discharge lamp, resulting in the necessary room illumination 9 and must be more than two in the room: Firefly: Discharge lamp. The present invention also solves this problem. Because of the negative repulsive repulsion of the phosphor particles arranged in the uppermost layer of the working film, the electrons in the anode region cannot be close to the fluorescent film, and the anode region is contained in the negative charge of the fluorescent film (sbe SUrface-b〇und -electrons, the surface of the electrons in the sheath. If the SBE sheath is removed from the phosphor film, the anode region extends to the phosphor film, and the light output of the phosphor film is proportional to the input power. The house can be reduced by the increase in brightness. Photo day ^ : The number of fluorescent discharge lamps used has a clear power saving effect, and contributes greatly to environmental protection by reducing the oxidation of rabbit gas. [Summary of the Invention] Human life is rapidly progressing due to the development of a light source that illuminates the darkness. The history began with campfires, and later developed into burning torches, vegetable oils, oil, and gas, and gradually improved the illumination. As the basis of modern science, the discovery of the t-electronics made the history of the illumination of the light source change: change. After the discovery of electrons, the development of the use of electronic movement of the crane lamp and the sub-photovoltaic discharge k'A is widely used in the world. Recently, there are light-emitting diodes (light_emiuing di〇de, led electric field) that also utilize electrical behavior. m light (^ mine 〇 1UmineSCenCe, EL), and organic electric field. The proposal of ic light_emiuing di〇de, 〇led), and a practical evaluation. Various sources of light using electronic behavior can be scientifically evaluated as follows. The tungsten filament lamp heats the town metal to a high temperature (3, (9) generation) by using Joule heat 200919527 generated by the resistance of the electron movement. The energy conversion efficiency of input power to visible light is low, 〇 8%, but the conversion efficiency can be maintained until the high temperature of the metal softening point, so that a wider range of luminosity can be obtained by increasing or decreasing the input power. Therefore, the current tungsten filament lamp is still widely used as an illumination source inside and outside the house. The most users are ordinary families. Tungsten wire f is the light source that can be manufactured at the cheapest price, and is used as a simple illumination source in most households around the world. The shortcomings are short life (5 hours). The heated metal will evaporate, so as the lighting time passes, the crane wire will become thinner and the resistance will increase and the wire will be broken. The fluorescent discharge lamp converts the invisible ultraviolet ray of W gas into a visible light source by coating the t-light film on the inner surface of the glass tube, and the energy conversion efficiency is about 42 G%. The problem is different from the crane light. The light intensity of the fluorescent film is saturated with respect to the input, and the amount of light taken out from a single glare discharge lamp has a limit. The saturation level is lower than 9 degrees, so multiple fluorescent discharge lamps are arranged in the door requiring high brightness illumination. Compared with tungsten lamps, fluorescent discharge lamps are expensive, 35 energy conversion efficiency is high, and generate less heat, so they are used for the main lighting in the office of a large building in an industrialized society. Industrialization In the country, it is widely used as a power-saving lighting source to the ordinary family. The reason for the life of the singer-sounding fluorescent lamp is mainly caused by the cation of the electron-emitting electrode (4). Other reasons (4) Adsorption on the surface of the light film: The organic residual gas in the light discharge official, and the ultraviolet light reaches the light film. The adsorbed gas layer absorbs the ultraviolet light. The organic residual gas is discharged according to the degree of the degassing step in the manufacturing process of the lamp tube and the large amount of organic gas generated in the initial stage of activation of the 6Hg amalgam and the Ba collector. Great changes can be made to a level that can be ignored. The current life of fluorescent discharge lamps is longer than the life of tungsten lamps, which is about 2,000 hours. LED is a developer of an application example of modern electronics industry technology. The LED is fabricated by an element in which a thin film of an inorganic element is stacked in multiple layers. In order to cause the LED to emit light, electrons are injected into the thin film layer of the LED, and light is emitted when the injected electrons and the holes are recombined in the light emission. The problem with LEd is that although about half of the injected electrons help to illuminate, one of the remaining electrons cannot be illuminated at the center of the luminescence, but instead is converted to heat. Although the luminous intensity is proportional to the number of electrons injected, the temperature of the LED also becomes proportionally high. Even if the LED is heated to about 70 〇c, the change in luminous intensity over time can be ignored. When the LED is heated to 1 〇〇〇c or more, the luminescence (misc) in the film spreads out from the inside of the film due to heat, so the number of light centers decreases with time. Luminous intensity is rapidly diminished with temperature and time. Under the operating conditions of practical LED brightness, the coffee is: 〇C or so. Although the afterimage effect of brightness is visually observed by the eye, Sa emits light to prevent temperature rise, but does not substantially solve the problem. Γ / 攸艮 解决 solve the fever problem. The problem of the life of a bright coffee. And, by the principle of lamination of thin films of inorganic material elements, LPD knows that the light-emitting diodes and the holes are combined in the heart.

Ding. The thickness of each film layer is much larger than that of L. The thickness of the high voltage μ must be applied. This is to reduce the EL. The luminous intensity is proportional to the input voltage. The discharge breakdown is limited. The discharge breakdown is limited. The media layer will produce JJ's large shell. Lifetime 200919527 The diffusion of the illuminating center causes the brightness to deteriorate. The research and development of EL has lasted for more than 5 years, and the practical products have been reported many times, but they are not essential. The above problems have been improved, and the products have disappeared without appearing in the market. This duplication has been produced by large companies in Asian countries, but large companies in Europe and the United States have not been produced. 〇led has the same problems as EL, bright LED Continuous lighting will have life problems. Using 0LED _ with low illumination can alleviate the problem, thus limiting the scope of use of OLEDs. The illumination sources developed as described above have not solved the main problems in practical use. The light source is a camping light discharge lamp. The development of camp light discharge lamp has been researched for more than 50 years, as the discharge of glory discharge lamp: scientific research is longer than (10) years. According to this situation Ordinary investors and business operators believe that the technology of fluorescent discharge lamps has been developed. The inventors have established the most important theory of discharge theory so far, and the basis for the re-examination of δ is started. The gentleman black eight, ° fruit know, think that the technology of fluorescent discharge lamp has been developed is not correct, in order to improve the basic structure of the fluorescent discharge lamp. Before the discharge phenomenon, the old loss Considering the necessary illumination of the light source. Even if it illuminates the darkness, the main activity of the non-night person is the daytime activity between 5 million years. At present, our evil spirits should be brighter during the day. It does not adapt to the sunny daytime..., —, jin, has 'but adapted to the true degree of daytime micro _. The light system has fluctuating photons, and this 2 tries to smash the peasant’s energy. The flat berth is more green with 2.3 eV energy, and the daytime scenery depends on the illumination of the day during the sag, and the illumination illuminates (10) photons in the slight yin. Unit area The amount is 3.7χ〗, 19 10 200919527 Therefore, the above illumination reaches 80 w/cm2 曰< Ϊ. The light source emitting the number of photons in the illumination source is most comfortable for the human eye. w/ 2 ^ Bt _ Right 1 conversion The cumulative efficiency is 80 W/cm and the necessary input for the development of the 3 ^ rush source can be calculated. As such a light source, various light sources have been developed. Dan Aluminium Xenon discharge lamp was selected as a suitable light source 'in the past 6 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 车 然而 然而 然而 然而 然而 然而 然而 然而Improve the lighting sound of each fluorescent discharge tube, witness, upper, ^ ..., and reduce the number of fluorescent discharge lamps used in lighting, and thus reduce the consumption of electricity. In addition, in order to reduce the power consumption, the fluorescent discharge lamp is 镅I Μ, and the electric-" In order to solve these problems, people #Ρ1, we have put a lot of effort, but the satisfaction is far from enough. Firefly: The epoch-making improvement of discharge lamps is still expected. Tian: The construction of the fluorescent discharge lamp used is very simple. Vacuum sealed glass, g contains 3 suitable Ar gas and Hg gas, metal electrode contains <glass & g both ends' and the inner wall of the glass tube is coated with a light film that converts ultraviolet light to 2 . The metal electrode is connected to the external power source via the conductor of the metal bar. The discharge system applies a sinusoidal alternating current high potential to the metal electrode, extracts electrons from the metal electrode in a vacuum, accelerates the extracted electrons, and makes a space between the electrodes at both ends of the discharge tube and the gas stone. in. , causing a discharge. The invisible 254 nm ultraviolet light (uitravi〇iet, uv) emitted by the excited Hg gas during discharge has a significant effect. The invisible UV light emitted is irradiated onto the working film applied to the soil surface of the discharge lamp. A fluorescent film converts invisible uv light into visible light to produce a fluorescent discharge lamp. Due to the simple structure, the technician of the fluorescent discharge lamp 200919527 has been optimized for a long time. Rong has been in business for more than 60 years, and the annual production = release of the company's technology from the market to the fluorescent discharge lamp has been two:: Second, it is generally believed that the above optimization system 4 is not incomprehensible. However, he has not established a review of the basic structure of the first discharge lamp in the scope of the structure. According to the driving of the solid element and the liquid lamp, it is essential to introduce the above-mentioned camp light discharge air-emitting electron material: electrons are injected into the lamp tube. Yu Zhen 1 shoots electrons in the modern science of the metal with a small work function (10) found that 'if the metal is twisted, straight ^A.Edlson in 1884, $ can be launched into the vacuum埶electronic. Cold cover The major discovery of thermal electron emission is the use of peroxide to improve the :::) coverage heating to 8. . . . The tungsten wire is easy to emit the best effect of the emitter/the Ba-oxide emitting hot electrons. The cathode of the fluorescent lamp and the lamp officer is covered with a Ba• oxide. The development of a tube diameter of 25 _ or more p, ^ ( ΗΓΡΤ ^ . Chiyou discharge lamp ® ' and popular as a hot cathode discharge U (HCFL). (D) years, found the gold ^ straight ^ between FI - N〇 With the effect of rdheim, the shape of the metal electrode such as the surface irregularity of the metal plate and the second fishing bell type was reviewed. As a result, the metal electrode of the bell-shaped type was used. The metal electrode can be processed into a smaller one, so the diameter of the metal electrode can be as small as possible. 15_Following, especially as a liquid crystal display (LCD display), it is commonly used as a cold cathode fluorescent discharge lamp (CCFL) with an inner diameter of 2 mm or less. In the electrode of the fluorescent discharge lamp using the above metal cathode, the evaporation of the electrode of the cathode 12 200919527 is explained by the problem that both the metal and the CCFL are evaporated. The cation with a higher mass in the gas collides with the cathode. The collision of the cation causes a very small portion of the metal electrode to be instantaneously heated to a high temperature at which the metal evaporates. The evaporated metal element is deposited on the fluorescent film coated on the inner wall of the glass tube around the lower temperature electrode. This phenomenon is called Tibetan plating. In the film formed by sputtering of metal elements, the gas and Hg gas in the discharge tube are adsorbed, and the degree of gas reduction in the t-light discharge lamp is increased with the passage of time, thereby making the fluorescent discharge tube The life is shortened. The average life of the fluorescent discharge lamp due to sputtering is 2, 〇〇〇 small. As a method of reducing the sputtering phenomenon of the metal cathode electrode, the electrode metal material and the sealing gas pressure have been reviewed based on experience, but the problem has not been fundamentally solved. ... There are several unresolved issues in common between HCFL and CCFL. One of the major problems is the fact that the applied voltage at the narrow distance between the cathode of the fluorescent discharge lamp using a metal electrode and the front of the anode greatly changes. In the range where the applied voltage is rapidly changing, eight illuminating and non-illuminating streaks are observed. The luminescent stripes are named after the original observer. The finder is Aston dark, Cathode gl〇w, Cr〇〇ke, s such as spit'

Negative Glow > Faraday dark ^ Positive Column ^ Anode Glow, and Anode Dark. Although the stripes are generally illustrated, the description is limited to the scope of the observations and does not clarify the scientific basis for the generation of luminescent stripes. These irregular luminescence are more pronounced at the cathode. The sudden change of the applied voltage around the cathode is collectively referred to as the reduction of the cathode voltage and the loss of the cathode voltage, and the energy of the overall lighting energy of the fluorescing electric tube is reduced. The elimination of the cathode voltage is developed. 13 200919527 Power saving An important issue in the glory discharge lamp, but the cause is unknown, so it is still solved by two methods. The above-mentioned phenomenon of splashing and reduction of cathode electric M is an important research topic of light-discharge lamps, but even if the published special editions are published, the scientific basis for such phenomena is still unclear, and it is always stuck in the phenomenon of measurement. Description. Due to the inability to understand the production of 'significant' reasons for fresh births, it is an unresolved issue. The development of the basic technology of the discharge lamp official has not been completed. The inventors of the present invention have a low cathode magnetism and a splashing problem. Science [The inventor's elaboration and thoughts] No. =::: SBE is formed in the discharge tube of the metal cathode 7', and the publications related to gas discharge are not in the state. From the metal cathode emitted into the hole in the metal (hole of electron, wide! Residual effect after emitting electrons. The fact that the function of generating gas discharge is shown is that if the electron e is taken out In the vacuum, there is a hole h in the metal. Because of the electric body, it is assumed that the hole is immediately filled by the electron supplied from the power supply. (2) There is an error in the conventional thinking. The electron supplied from the power source to the metal electrode 30 , the resistance to the metal electrode is hindered by the metal resistance, η ό t law), and not instantaneous... (4): There is a time difference between the power supply electron and the metal cathode % emission γ 。. When statistical processing is carried out, the resistance of the material::: the surface of the polar metal 'the existence of the hole is due to the change of the cathode metal hole Γ::;:, but there will be a steady number of *the fruit can not be ignored. The hole h of the surface layer and the electron e emitted to the real work are strongly attracted to each other by the electrostatic force, and the electricity in the vacuum 14 200919527 is again combined. The positive electric field of the hole h located in the metal surface layer covers the vacuum. The electric + e emitted into the vacuum is attracted by the positive electric field of the hole h of the metal surface layer, and does not have the energy to re-enter the metal, so that it is in a vacuum slightly away from the metal surface (about 5 μmη) and the metal The hole h in the electrode is combined. This is the surface bound electron (sbe, surface_b〇und_ electrons). The surface of the metal cathode in the fluorescent discharge tube is covered by sbe. At the beginning of the work (1 900s), SBE was observed as a space electron cloud present on the surface of the cathode when the SBE was observed from the vacuum side. The recently published Cathodoluminescence and Photoluminescence; Theories and Practical Applications, CRC Press , Taylor and Francis G,,Β_ Μ. L〇nd〇n,

NeWY〇rk, Pp30_37 and 69_76, 2〇〇7 (non-patent document 〇, the measurement of the relationship between the electron beam energy and the luminescence intensity of the fluorescent film irradiated onto the fluorescent film by the cathode ray illuminating) is presumed to be formed on the surface of the cathode The negative potential of the view. (4) The size is 1〇6eV/cm. In order to take out the electricity from the surface of the cathode, a positive potential greater than the negative potential of the suspension must be applied to the electrons. The electrons taken out at high energy are accelerated to high speed. The discharge phenomenon written Μ has the phenomenon that the electrons of high energy # enter the gas space, and the observation results are all obscured by the behavior of the high-speed electrons exceeding the necessary. In the gas space, the distance of non-interaction (the negligible atom ^ (4) Refilling a gas with a neutral atom. Each gas ', sub-filled with electrons surrounding a plurality of electron shells of the nucleus, her negative charge, and the cation charge of the nucleus are balanced, and the electrical properties of each gas atom are medium 15 200919527 Sex. However, the negative electric field (5xl〇5 eV) of the outermost shell electron of the atom in the gas space continues to expand, so the gas space is filled with a strong negative electric field. The high energy (106 eV) above the negative electric field (5X105 eV) and the electrons entering the gas space cannot enter the gas atoms blocked by the electrons filled in the electron shell, so repeating multiple inelastic collisions with the gas atoms The electrons of the sub-shell are emitted into the vacuum. The ionization of the gas atoms is accompanied by the generation of heat. Therefore, a plurality of gas atoms are ionized with heat dissipation. This is the cause of the temperature rise around the cathode of the fluorescent discharge lamp. The ionized electrons are the same as the ion charge Coulomb, but there is a big difference in mass. The mass of the electron is 9_lxl〇-u gram, and the mass of the ion varies slightly with the atom type, but both are 1.7. X 1 〇-24 grams or so, about 1 times the electrons of Berry. Electrons are easily migrated by the electric field applied to the gas, but the migration of ions is slightly slower and less. Although detailed reasons are not explained here. However, the difference between the migration distance of electrons and ions causes the light-emitting streaks of the cathode nearby. ', The error that must be pointed out here is that, in the initial stage of studying the gas discharge, the gas discharge is defined as From the invisible gas, the light is discharged. For this reason, the study of gas discharge measures the intensity of light from the discharge tube, and the discharge is explained based on the result. It is difficult to scientifically clarify the discharge only by measuring the light. The discharge of the gas must be analyzed according to the electronic behavior determined by the multiplication of the electrons entering the gas medium and the gas atoms. If the characteristics of the fluorescent discharge lamp are analyzed according to this new viewpoint, it is known that the problem that has not been solved so far can be solved. The current manufacturing technology of fluorescent discharge lamps has not been completed. 16 200919527 The characteristics of fluorescent discharge lamps are determined by the electronic behavior of the body. The decision is made another important to the practice of fluorescent discharge lamps. The review of the characteristics of the knowledge was omitted. That is, the physical properties of each of the phosphor particles in the fluorescent film coated on the inner wall surface of the φ++amp; Μ Only consider (4) money to convert the invisible υν light emitted by the gas into visible light. According to the study of the present inventors, the physical properties of the phosphor particles are not only related to the phenomenon of luminescence. Each of the phosphor particle-based crystallized particles 'is also a crystal having an asymmetric crystal structure, and when placed in a discharge tube, exhibits a crystallized substance and has a significant influence on the electron behavior in gas discharge. Practically, the reason why the phosphor particles have an asymmetric crystal structure is as follows: occupying the luminescent center of the asymmetric lattice point, allowing electron migration which is not allowed in the luminescent center of the symmetrical lattice point, and allowing the electron migration probability to be abnormally high . This is the reason why the luminescent properties of commercially available phosphors are abnormally south. However, most researchers who study solid-state physics believe that phosphor particles are not single crystals, but polycrystals containing a plurality of crystal axes, and are crystal particles containing a plurality of crystal defects. Namely, the knowledge that solid state physics is judged is not applicable to crystals containing a plurality of crystal defects. This judgment is not correct according to the paper published in Chemical Review 'Volume 103, No. 1 〇, ρρ3835·3855, 2003 (Non-Patent Document 2), which determines the size of the crystal field of electron transfer in the luminescent center, which is a very narrow range. The completion degree of the crystal field (with a radius of 5 〇〇) is independent of the crystallinity of the particles as a whole. This is because the commercially available phosphor particles are irregular in shape and the phosphor particles are illuminated at the same efficiency. The phosphor particles are polycrystalline, and the optimization of the particle size of the polycrystal is determined by the coating conditions. Using an external ultraviolet light source to investigate the actual presence of fluorescent light in the laboratory. In the case of light bodies, the luminous efficiency of the commercially available phosphors is the highest. However, even if the light is placed on the wall:: the commercially available CL·fluorescent body is coated on the wall of the pipe, the light of the lamp is not able to obtain the bright lamp D, so the light discharge lamp of the camp Lao Guang: A fluorescent body that is found based on experience. Root #A Firefly System The result of the experience is lack of rationality. Therefore, the majority of the Aluminium light system selected by the light directly stimulates the phosphor of the illuminating center by light (PL Rong

The company's "boiler" 帛 precursor) < column, even if you look at the 〇 HM body manual, did not find out why the use of p theory. The beauty of the body is applied to the inner wall of the fluorescent discharge lamp. The following problems remain unresolved. Even if the electrons from the metal cathode are used, the gas in the fluorescent discharge tube will not be easily discharged. Although the fluorescent discharge lamp is improved to make the gas discharge in one place, the fluorescent discharge lamp that has not yet developed the instantaneous discharge has not been developed. The speed of electrons that come out in one direction is very fast, which is 2χ1〇5 ec. Why is the electron analysis of the high-speed advancement of the cathode and the anode in the direction of the cathode? The scientific analysis of the instantaneous discharge of the glare discharge lamp is completely lacking, so that ==

theory_. The skilled technicians and technicians only stay in the experience stage. X Total Production = Other unresolved issues exist. Increasing the fluorescence discharge after discharge. When the person is on, the light output is easily saturated. The higher the uv Ewing phosphor particles of the fluorescent film layer, the refractive index (n? 2), first reflected on the surface of the uppermost layer of the first film, ...uv The light is also arranged in the phosphor particles in the lower part of the fluorescent film. Participation in luminescence on the fluorescent film The number of effective phosphor particles can be determined experimentally. It can be calculated that the number of illuminating centers included in the number of phosphor particles is 18 200919527. The calculated number of illuminating centers is about 10 times the number of photons of uv light irradiated on the fluorescent film. Camp Light Discharge The number of excitations in the luminescent center of the fluorescent film inside the lamp is not saturated. Brightness saturation refers to the intensity of the UV light that reaches the fluorescent film. Despite this, the technicians of fluorescent discharge lamps are still looking to increase the brightness of the fluorescent film by increasing the luminous efficiency of the phosphor (2 to 3%). This thinking is not correct. There must be countermeasures against the uv light unsaturation that is irradiated to the fluorescent film, but there is still no paper that quantitatively discusses the UV light saturation phenomenon. According to the findings of the present inventors, it has been found that the electronic behavior in the discharge tube is greatly affected by the electrical characteristics of the phosphor particles arranged in the uppermost layer of the phosphor film. Another important factor in controlling the electronic behavior of the discharge tube is the selection of a suitable phosphor and a phosphor film that suitably aligns the phosphor particles. In order to solve these problems, the knowledge of the physical properties of the glory body disclosed in the reference i can be used. As described above, the fluorescent discharge lamp can be modified from the basic configuration. Ben 2 Ming = Fluorescent Discharge Lamp System Scientifically solves the problem that the fluorescent light can not be solved

$ All problems with the lamp. As a result, the fluorescent discharge lamp T necessary for the brightness of the fluorescent discharge lamp can be remarkably improved and the proper illumination of the room can be reduced. Moreover, the lighting time of the fluorescent discharge lamp can be extended by the level at which the number of bits can be increased, so that the production unit price of the f-discharge lamp tube is lower than that of other sources. Since the structure of the fluorescent discharge lamp can be simplified, the manufacturing steps are shortened. The 'fluorescent discharge lamp of the present invention can greatly contribute to power saving, and less than the gas emissions strongly demanded by the society' It is also reported that the material is large and is read by 3 people. 19 200919527 Non-Patent Document 1: Cathodoluminescence and Photoluminescence; Theories and Practical Applications, CRC Press, Taylor and Francis Group, Boca Raton, London, New York, pp 30-37 and 69-76, 2007 Non-Patent Document 2: Chemical Review Volume 103, No. 10, pp 3835-3855, 2003 Non-Patent Document 3: Cathodoluminescence, Kodansha, 1990, p 104-120 Non-Patent Document 4: Applied Physics Letters, 43, pp 1073-4, 1983 Non-Patent Document 5 : Physical Review Letters, Vol. 27,1 9715 P1345 Non-Patent Document 6: Journal Physics D Applied Physics, 32 (1999), pp 5 13-517 [Embodiment] [Problems to be Solved by the Invention] As described above, The conventional fluorescent discharge lamp has accumulated many problems as follows. The first problem is that the cathode voltage around the cathode is lowered, and the energy loss is about 4% of the total lighting energy of the fluorescent discharge lamp. The second problem is that the cathode voltage is lowered, and a stripe pattern of light emission and non-light emission is generated in the vicinity of the electrode - giL, &&&&&&&&&&&&&&&&&&&&&&& The cathode collides to evaporate the metal cathode, form an evaporation film on the fluorescent film, and the light discharges a hole in the body, which causes the discharge life and the life of the xenon discharge lamp f to shorten the electric lamp tube. The mother is fluorescent, and the monthly illumination is much lower than the required illumination. In practice, it is necessary to arrange 20 200919527 multiple fluorescent discharge tubes, which is difficult to save energy, and

Pa eg , Λ _ ^ R captured in the limit. After the flute S is connected to the power supply, it starts to discharge until it is lit. "Different 5 becomes a hindrance to rapid lighting. And for a long time, the purpose of 匕本奂明 is that, based on the action of the heavy-duty lamp on the basis of ffi, the principle of light-receiving is discussed. 4After the cathode voltage is lowered, the day near the electrode is eliminated. The light-dark stripe pattern near the electric enamel recognizes sg q', and brightness from the further object of the present invention. Also, - a metal cathode helmet j is provided. Knowing to improve the single fluorescent light in φ Xin Μ ..., shell consumption, discharge discharge lamp, and Jiang also, speed point redundant fluorescence ... ", - the species with the use of the fluorescent discharge tube back source The LCD display device (liquid crystal display device). The first step [the means to solve the problem] The present invention is to solve the μ, +, π form system - the type of firefly = the maker of the 'the invention' The tube is coated with a fluorescent film on a fluorescent discharge, a 兮 technology, an electric/and a glass inner wall surface, and a fluorescent discharge lamp is characterized in that the glass is

The discharge of the discharge gas is generated by the glass S 盥 being connected to φ, β, and the external circuit of the 电源 坩 抓 独立 独立 独立 独立 独立 独立 独立 独立 独立 独立 独立 独立 独立 。 。 。 。 。 。 The second aspect of the adjacent electric power is a fluorescent discharge lamp, wherein the inner crucible is separately formed on the electron source and the ion source gentleman, and the electrotype g円邛 is compiled from the above. ~ Gas discharge in the lamp discharge lamp =: When the electrons taken out by the electron source move toward you in the gas space 吝-^mr, the electrons of the above electron _ 'h migrate to the ion source IX, the ion again Combine and close the above internal circuits. In the third aspect of the present invention, in the glory discharge lamp tube, the system is covered with an electrical insulator particle 21 200919527 metal electrode and the metal electrode electrode; The other ...::: in the light discharge lamp tube is formed by the electric horn particles, which are covered with a layer of electric ray. Gastric electricity alone as the upper sputum ion source form The fourth form of this month is a kind of electric potential of the above-mentioned metal Π upper 逑 electronic metal electrode of the fluorescent discharge lamp source forming electrode, and the above-mentioned. Electrode, and 邑 体 体 粒子 粒子 , , _ _ _ _ 由 由 _ 由 + + 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由 自由Electrons are combined with positive charges in the electrical insulator particles in the two electrical insulator particles to form an inter-work electron cloud, and the space electron cloud is used as the electron source; and the above-mentioned ion source forming electrode The n-electrode applies a potential of a negative polarity, and the electrical insulator particles of the metal electrode are memorized. The attraction of the negative electric charge of the electrically insulating limb particles after the ionization of the ions generated by the ionization of the electrode periphery is subjected to the dielectric polarization. The ions are combined with the potting negative charges of the electrical insulator particles to form an ion group, and the ion group is used as a source. < Engraving The fifth aspect of the present invention is a fluorescent discharge lamp in which electrons are taken out from the electron source to the surface of the fluorescent film, # is conducted by the surface of the fluorescent film: electron acceleration 'accelerates the electron system as a gas Initiating the cause of the discharge, the accelerating electrons are bent into the gas space by the negatively charged phosphor particles, so that the gas of the fluorescent discharge lamp is instantaneously lit and discharged, thereby generating no cathode voltage reduction. Gas discharge. The sixth form of the above-mentioned fluorescent light-emitting device is a fluorescent discharge lamp 22 200919527. The surface of the film is alternately arranged with negatively charged phosphor particles and negatively charged phosphors = sub' and the above-mentioned fluorescent light At a plurality of locations on the surface of the film, the accelerated electrons are bent toward the gas space side by the negatively charged phosphor particles. According to a seventh aspect of the invention, there is provided a fluorescent discharge lamp, wherein the camping film coated on an inner wall surface of the glass tube of the glare discharge lamp is an electron beam luminescent phosphor powder and a photo luminescent phosphor powder. The mixed powder is composed. The eighth aspect of the present invention is a fluorescent discharge lamp, wherein the photoluminescence phosphor powder is composed of three kinds of rare earth light-emitting "light phosphors" which emit three-color light separately, and the electron beam illumination The phosphor powder is composed of a low voltage electron beam luminescent phosphor powder. The ninth aspect of the present invention is a fluorescent discharge lamp in which the phosphor powder which emits green light in the rare earth-based photoluminescent phosphor powder is replaced by π-light-emitting acid phosphor powder. The first aspect of the present invention is a fluorescent discharge lamp, wherein the above-mentioned rare earth photoluminescence phosphor powder emits green light illuminant powder by cl electro-optic zinc silicate phosphor powder Xiao pL纟Replaced with the mixed powder of glacial acid zinc powder. The first aspect of the invention is a fluorescent discharge lamp, wherein the particles of the low-voltage electron beam illuminating phosphor are arranged to be discontinuously distributed on a surface of the fluorescent film in the fluorescent film. A twelfth aspect of the invention is directed to a fluorescent discharge lamp, wherein the fluorescent film is composed of a mixed powder of a photoluminescent phosphor powder and a low-voltage electron beam emitting phosphor powder which emit white light alone. 23 200919527 A thirteenth aspect of the present invention is a fluorescent light-emitting film which is formed by emitting a white enamel. The photoluminescence system consists of a phosphorous _ 11 light: the 14th form of a fluorescent discharge lamp, which is in the above-mentioned working body. The fifteenth aspect of the present invention is an LCD display device characterized in that one or a plurality of fluorescent discharge lamps of the first form to the f14 form are arranged in a plane. Comes back to the backlight of the LCD display device. According to a sixteenth aspect of the present invention, in a liquid crystal display device, a plurality of the light-emitting discharge lamps are disposed in a vertical direction or in a horizontal direction, and each of the glare discharge tubes is individually or a plurality of glare discharge lamps are used as a group in a line sequence. The method of sweeping the 4 fields is sequentially ordered, and the image of the line sequence is reflected on the entire screen. [Effect of the Invention] According to the first aspect of the present invention, a fluorescent discharge lamp can be provided, and the discharge of the discharge gas in the glass s is an internal circuit independent of the flow of electrons, and is connected to the power source. The external circuit generates, and the source of the generated electrons is ionized by the discharge gas itself, so that the electrons for discharge are not supplied from the external circuit. Therefore, during the entire discharge process, the electric gas is separated from the external circuit by the electric discharge gas, and the discharge gas itself is continuously ionized and recombined, so that the discharge gas is not consumed, and the life of the discharge lamp is long. Moreover, since the electrons are not supplied from the external power source, there is no cathode voltage drop, so that the power consumption of the external power source can be reduced, and the commercial power supply 24 200919527 source need not be said, even if it is detrimental ~, the battery power supply 'battery battery The consumption is also small, so the discharge lamp and its long circuit can be realized. In other words, the present invention can provide a discharge lamp official of the epoch η, even if it is necessary to use the battery electric 'π power supply, ', the rare night, the region, the mountain area, etc. due to no business, can also be buried by the animal battery and used Ray $ # 曰-age... Official. Further, since the above-mentioned cathode does not exist, the pattern of the light and dark stripes disappears, and the vicinity of the electrode is also brightly illuminated as a whole, thereby improving the illumination. ^ The internal circuit according to the present invention is formed by ionization of a discharge eclipse, and the electronic circuit is formed by the above-mentioned Hr source, and the internal electric circuit is formed by the above-mentioned Hr source. π is completely blocked, and the electrons are transferred from the above-mentioned electric source to the above-mentioned ions, and the same electrons are transferred, and the heavy discharge phenomenon occurs. The discharge repeats the incoherent collision of the common gas atoms, and the optical film is made by ultraviolet rays. Continuously emitting light, and the above-mentioned electrons are closed to the above-mentioned circuit. The present invention provides a fluorescent discharge lamp in which a smoother film continuously emits light by the above-mentioned discharge enthalpy. In combination with the electric rolling body, the external circuit is completely blocked, so that there is almost no energy loss of the object. Moreover, the present invention provides a camping light that does not supply electrons from an external circuit to an internal circuit, and thus is not decompressed. Lowering, which can greatly reduce the low current drive of the external power supply. The driving current of the power supply, and the electrode for forming the metal electrode according to the present invention, by the third form of the month, by layer covering The insulator particles constitute the electrode for forming an electron source and the ion source may be separated from the metal electrode 25 by the electrical insulator particle layer and the metal evaporation, and the internal circuit is completely separated from the external circuit element. The electron emission of the electrode and the metal base = : Therefore, there is no consumption of the metal electrode, and the conduction (10) phenomenon disappears, so that the long life of the glory discharge lamp can be realized = the electron emission of the electrode, but the external current flowing through the external circuit is only the electrode The induction current of the dielectric particles on the insulator particles and the low current drive of the current fluorescent discharge lamp, j: the result is that energy saving effect can be achieved. 35. According to the fourth aspect of the present invention, The external power source applies a positive potential to the metal electrode of the electron '', the electrode for formation, and the bit is placed to make the electrical insulator layer dissipate the external χ main 啄 "啄 layer, 丨 electrode, fine by the polarization charge The electric field is used to attract the electrons generated by the ionization of the discharge gas, thereby forming a space electron cloud around the poly rt electrode. As the electron source. The electrons constituting the Erhai "subsource are all electrons generated by the ionization of the discharge gas, and the electrons are not supplied from the external circuit at all. Therefore, there is no voltage drop of the internal circuit, so that the power consumption of the external circuit can be remarkably reduced. Similarly, a negative potential is applied to the metal electrode of the ion source forming electrode at the other end inside the discharge lamp tube. The electric insulator layer is dielectrically polarized by the negative potential, and the polarization is polarized by polarization. The electric field attracts the cations by ionization of the discharge gas to form a group of cations clustered around the periphery of the metal electrode as an ion source. The ion source is completely insulated from the negative metal electrode by an electrical insulator layer. The electrons of the electron source migrate toward the ion source while performing gas discharge, and return to the neutral emulsion by recombination of electrons and ions.镥 From the continuous action of the micro-process, the glory experience emits visible light by the ultraviolet rays generated by the discharge, so it can be used to release the low-current drive energy-saving type. Since there is no reduction from the external circuit to the cathode, the supply and the 'electron' can realize the use of the discharge lamp; the discharge lamp of the know-how is ultra-low cost and long life. Chemical. The above-mentioned insulator particle layer $丨 m m ' is formed on the opposite surface (surface) of the discharge junction formed between the electrodes, and the metal is evaporated to block the electron supply from the external circuit. In order to enhance the intertwining property, the insulator particle layer may be formed on the entire surface, the same surface, the back surface, and the side of the metal electrode, and may be formed on the opposite surface and the side surface, or on the opposite surface and the back surface. Here, the back surface refers to a joint surface with an external circuit. According to the fifth aspect of the present invention, a fluorescent discharge lamp tube can be realized, which accelerates a gas by accelerating electrons taken out from the electron source by surface conduction of a surface of the phosphor film, and is negatively charged by the fluorescent film. The phosphor particles bend the orbit of the accelerating electrons into the gas space, thereby instantaneously lighting and discharging the gas of the fluorescent lamp=lamp. Thereby, it is possible to provide an energy-saving fluorescent discharge lamp which does not have a cathode voltage drop, which can increase the luminous intensity (illuminance) and can be driven at a low current. Usually, a photoluminescence phosphor (PL glaze) is contained in the negatively charged phosphor particles. Impurities present in the particles of the photoluminescence phosphor capture electrons, resulting in permanent internal polarization due to the trapped electrons (PIP, persistent internal p〇laHzati〇W, permanent internal polarization electrons appearing in the fluorescent film The negative charge is formed on the surface, and the accelerated electron is bent into the discharge space. Therefore, if the photoluminescence phosphor is disposed in advance at a position where acceleration of the electron is desired, the photoluminescence phosphor at the position is negative. The charge acts on the above-mentioned accelerated electron bend 27 200919527. The size of the negative charge can be adjusted by selecting the phosphor, thereby accelerating the collision between the surface conduction electrons on the phosphor film and the discharge gas, thereby achieving discharge. The rapid illumination in the space eliminates the delay in the conventional occurrence of the fluorescent discharge lamp. According to the sixth form of the present invention, a high-efficiency electric lamp can be provided, which alternates on the surface of the above-mentioned working film. Configuring a negatively charged scorpion and a negatively charged illuminant particle, and at the position of the surface of the fluorescent film, the above-mentioned negatively charged honor particles Acceleration 2 ^ to the side of the corpus callosum, so that the light-emitting body particles that are quickly lit and the entire surface is not negatively charged usually contain an electron beam illuminator (CL phosphor). Especially low-power electron beam illuminating Light body with less surface contamination, no 6 , 俨 pole # page negative electricity what nature, and therefore has no charge nine.. The sub-beam first fluorescent body will appear surface stained wood 'also exists to charge negative charge Lei Shao, the lack of the shape of the 驷 ri. In this form, the area of the light-extracting body without negative charge is not produced in the peak temple, and the Moxi Φ produces a repulsion of the net, so the upper surface of the fluorescent film can be made. The electronic acceleration of the guide. In the phosphor area of the negative charge of the city, the accelerating electrons are forced to discharge by the Coulomb repulsion, and the discharge lamp will be fast! The electric discharge is wide... The discharge gas is negative. ~ It is both fascinating and cumbersome. In this case, a plurality of areas are distributed in the surface conduction direction of the electrons, so the discharge lamp is replaced by a discharge lamp. Therefore, the entire discharge lamp can be brightly illuminated. Negatively charged phosphor particles along accelerated electrons The Coulomb repulsion of the electrons distributed on the fluorescent film, and the negative electrons in the negative electrons and the negative charge discharge space, and forced to bend the accelerated electrons by accelerating electrons and discharges The gas collides in the entire region of the multi-region, and the discharge is generated in the entire region of the discharge space, so that the discharge lamp capable of simultaneously illuminating the plate and the i-hip is illuminated at the same time.

According to a seventh aspect of the present invention, there is provided a fluorescent discharge lamp I for coating an inner wall surface of a glass tube of the above-mentioned camping discharge lamp tube: an electron beam illuminating body powder and a photoluminescence body It is composed of powder mixed with human powder. As described above, the electron beam luminescent phosphor powder does not have a negative charge: and the photoluminescence campsite powder has a negative charge, so if two camp lights are mixed in advance: the powder is applied to the discharge lamp, the negative charge The region and the neutral region are alternately arranged in the direct control of the powder, and the acceleration regions of the infinite number of surface conduction electrons are alternately arranged with the curved regions. Therefore, it is possible to provide a discharge lamp which emits light in the body region in the discharge lamp tube, and instantaneously realizes a discharge lamp which is quickly lit and the entire surface is spotted and which achieves high illumination with low power. According to an eighth aspect of the present invention, a luminescence discharge lamp can be provided, wherein the photoluminescence phosphor powder is composed of three rare-earth photoluminescence phosphor powders that emit three-color light alone, and the electron beam illumination is performed. The phosphor powder is composed of a low voltage electron beam luminescent phosphor powder. If red, neon, and blue are selected as the two colors, the composite color is white, so a white fluorescent discharge tube can be provided. Further, the three kinds of rare earth photoluminescent phosphor powders are negatively charged phosphors, and the low voltage electron beam emitting phosphor powders are non-negatively charged phosphors, so that rapid lighting and illumination of the entire surface can be achieved. According to a ninth aspect of the present invention, there is provided a fluorescent discharge lamp, wherein the photoluminescent luminescent phosphor powder emitting green light in the rare earth photoluminescent phosphor powder is replaced by a CL luminescent zinc silicate phosphor powder. . When the green light photoluminescence phosphor powder in the eighth embodiment is replaced by electron beam light emission (CL light) 29 200919527 矽SiL zinc phosphor powder, since it does not contain rare earth as a rare element, the material becomes It’s cheap, and it’s bright and beautiful. According to a first aspect of the present invention, a fluorescent discharge lamp can be provided, wherein a photoluminescence phosphor powder emitting green light in a rare earth photoluminescence glomerium powder is produced by a CL-cut zinc oxide The powder is replaced with a mixed powder of pL hair-cutting acid-dealing precursor powder. Because it does not contain rare earths as rare elements: the material is cheap, and by adjusting the mixing ratio of the luminescent acid powder and the PU zinc silicate phosphor powder, the illuminating brightness and the NTsc port TelevisiGn can be obtained. System CGmmittee, the clarity and brightness adjustment of the green color specified by the American Television Systems Committee. According to a U-shaped aspect of the present invention, a fluorescent discharge lamp can be provided, and a fluorescent film is disposed, and the particles of the low-voltage electron beam emitting phosphor are distributed on the surface of the fluorescent film discontinuously. . As described above, a low electron beam luminescent fluorescent system does not have a negatively charged phosphor, = a continuously distributed configuration, meaning that a region without a negative charge (also referred to as: ... a charge region) is discontinuous, a dead helmet + # For the change of 5, the negative charge region is formed with ..., the electric region and the region are alternately matched with the m-mw. Therefore, in the negatively charged region, the yield of the electrons is accelerated by the conduction electrons, so that it is possible to surely illuminate the entire surface and the entire surface. According to a twelfth aspect of the present invention, there is provided a fluorescent discharge lamp, wherein the fluorescent film is made of a photoluminescence phosphor powder and a low voltage electron beam illumination white color which are white light alone. It is composed of Yu Shu's mixed powder. ν, singularly private negative-charged phosphors, and low-voltage φ sub-beam luminescent phosphors are helmets, m丄μ, and other fluorescent materials, which can be realized by mixing two kinds of powders, 30 200919527 Fast lighting and the entire surface is lit. If three kinds of photoluminescence phosphors corresponding to the two primary colors of light are not used, but a photoluminescence phosphor powder that emits white light alone is used, the glory body is reduced to I. The light-emitting discharge lamp of the present invention has no brightness saturation phenomenon, and the brightness of the fluorescent film does not change with the pipe diameter. The brightness of the fluorescent discharge lamp with a diameter of 25 匪 or more can be improved by the home illumination, and the fluorescent discharge lamp with a diameter of 5 mm or less used for the backlight of the LCD can obtain and use rare earth. The luminescence of a phosphor-like luminescence lamp is equivalent or above. The camping discharge lamp can also be used in a lamp-like power-saving fluorescent lamp which is bent many times, which can greatly reduce the manufacturing cost of the power-saving type 2 light lamp, and can obtain a long life of more than 10,000 hours. Make a greater contribution to the interests of the needs. According to a thirteenth aspect of the present invention, there is provided a fluorescent discharge lamp, wherein the photoluminescence glory body which emits white light alone in the fluorescent film of the basin is composed of a phosphoric acid (tetra) phosphor.歯 _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ According to a fourteenth aspect of the present invention, there is provided a fluorescent discharge lamp, wherein: the first and second fluorescent films are additionally provided with a sub-beam oxidized oxidized phosphor. Although the tooth phosphoric acid phosphor alone emits white light, it does not contain red light when it is color-separated. Therefore, it is composed of three primary colors of light by adding electrons 2 to oxidize the seed polish. In particular, when used as a backlight source for the LCD display device described below, it is necessary to add the red electron beam oxidizing oxidant precursor of the fourteenth aspect, and to realize the three primary colors. 31 200919527

According to the aspect of the fifth aspect of the present invention, there is provided an LCD display device characterized in that the soap or the plurality of the first form to the 14th two-those-fluorescent discharge lamp are arranged on the single and the μ1jl_〇. And used as the backlight of the CD display device (3), the backlight source of the device uses a cold cathode tube (CCFL), but the degree of immunity is low, and the poisonous right Κ ρ ancient ^ ΐ π is limited. The brightness of the fluorescent discharge lamp of the present invention is long and is suitable for use as a source of the first month. That is, the fluorescent host of the present invention can be used as a liquid crystal display source, which has low power consumption and low-power backlighting, and is inexpensive, long-lived, and thus becomes a high-quality and low-resolution backlight source. According to the sixth aspect of the present invention, an LCD display device can be realized in the heart of the phoenix, and the fluorescent discharge lamp is disposed on the luminescent light discharge lamp of the above-mentioned 丨5 form. For the group, the y is broadcasted in line or in a way that multiple fluorescent images are reflected to the Γ field, and the shadow H of the line sequence is placed on the entire screen. The fluorescent discharge lamp of the invention can realize rapid lighting and the entire 矣 "cage line xenon lamp tube m wide surface point party, even if a plurality of fluorescent discharge lamps are arranged, the sub-injection line scan, the ground instantaneously Point * L "The speed of the speed of the speed of the speed of the speed of the two" is therefore available - a variety of suitable for scanning lighting glory L (3) ... 2: Scanning LCD display device. Known ..., used in the device The crp cannot scan the line sequence. The fast lighting speed is in seconds, [More Detailed Description of the Invention] The present inventors have studied the most basic part of the electric field and the electric phenomenon. The operating condition is to supply the electrons in the discharge tube to discharge the gas = the basic electricity that stops at the electricity. In the case of using the currently used gold 32 200919527 ki., it is subject to the inevitable formation of SBE on the cathode surface ( 1 〇6 eV/cm), so the electron has 1〇6 ev/cm or more 13⁄4 *§" -rf' JL· λ and is taken out from the cathode surface. Observable discharge phenomenon, presence and energy Influence" and cannot be removed by analysis In order to investigate the basics of gas discharge, it is necessary to use an electrode that does not form an SBE. This month, a person who uses the surface formed on the surface of the insulator particle t SBE 1 to emit a new type of electron (the discharge Μ) to supply electrons with an initial velocity close to zero: 5 'The original § uses the electrons from the electronic supply source to adjust the details of the gas discharge in the fluorescent discharge tube that has not been clarified so far. From: It can clarify all the unresolved issues. A fluorescent discharge lamp with significantly improved discharge characteristics can be developed. A novel electron supply source is obtained in the following manner. In the layer of gold insulator particles, after applying a potential to the metal electrode and the human metal electrode, the insulator The particle production plate is full, and the polarity of the charge after the electrode is polarized. Although the polarity of the metal electrode is opposite, the electric potential in the electric V ^ x L 7 is proportional to the potential g applied to the electrode. The constant uses insulation = εν本 - 1 &<" 芄 数 ε and q % table... Capacitance of insulator particles (dielectric potential 2 is induced by insulator particles Δ ''', + 丄e Vc~ Q /c= εν /C 矣 矣, because c is a constant, so ε ν / times g to the table ε value of 3 to 50, so polarized electricity, 'the height of the 邑 体 体 ... 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用/. The potential of the electric potential of the metal electrode. If the gas is placed in the gas space, the peak is applied to the metal electrode! ~5kV, the frequency; the metal electrode 'high-frequency electric field, the gas around the electrode ^~7 He will ionize in the A-frequency electric field, 33 200919527 thus forming free electrons and free ions around the electrode. Compared with the attraction of the electric field of the metal electrode electric tVg, the free electron and the free ion are more affected by the insulation experience of the souther than the south, and the electric field is attracted by the electric potential. Although the free electrons and the free ions are attracted by the dielectric polarization of different polarities, they do not have the intrusion into the insulator, and they accumulate in the polarization, respectively. The vacuum is then applied to the surface of the insulator particles. The use of electrons and ions accumulated on the surface of the polarized insulator particles separately to cause the gas discharge in the camping discharge tube to be a schematic diagram showing the principle of the discharge mode. When a power supply voltage is applied to the electric and/or electrode 3, the insulator particles + 4 placed on the electrodes 2 and 3 will be dielectrically polarized as shown. The polarity of the dielectric polarization on the gas space side coincides with the polarity of the electrode. The polarity of the electrode 2 and the front 3 will vary with the high frequency voltage, and the state of the moment is displayed in the _i. The free electrons generated by ionization are attracted by the positive polarity induced by the polarization of the insulator particles, and stay in the vacuum in the vicinity of the insulator particles 4, and are bonded to the positive polarity of the edge particles 4. The electrons that are in contact with the surface of the insulator particles 4 serve as a new electron source 7 for gas discharge. The ionized Ar+ is attracted by the negative polarity of the polarization induced in the dielectric polarization of the insulator particles, and stays in the vacuum near the insulator particles 4, and is sharply bonded to the negative electrode of the insulator particles 4 to form an ion source (accumulated ions). )8. The discharge 5 is generated by migration of electrons taken out from the electron source 7 to the accumulated ions 8. The electrons participating in the discharge are supplied by the gas in the discharge tube, and are not supplied from the insulator particles. electronic. The electrons participating in the discharge are combined with ions in the discharge tube to return to the outside of the discharge tube. , 34 200919527 & The question here is that the electrons accumulated on the surface of the insulator particles are not easily removed due to the pairing with the particles. Electric (four) Γ! The combination of the ground shape...' changes the frequency of the induced electric charge from the electric field around the electrode to the high frequency, and the polarity of the induced charge of the insulator particles changes rapidly. ^ ^ ^ ^ _ The result is that the electrons of the electron supply source 7 are suspended in the vacuum Τ in a short time. The charge of the insulator particles is superimposed on the charge of the suspension. In the vacuum, the binding force of the electrons is better. Weak, electrons are prone to migration in weaker frequency electric fields. The electrons in the vacuum suspended near the surface of the insulator particles are taken out by ^. , and the initial velocity of the electrons is close to zero. The electron source of the invention is obtained only when a high-frequency electric field is present, and when the high-frequency wave number is small, and when a direct-current voltage is applied, the electron source is not generated. The amount of polarization charge Q induced by the insulator particles varies with the value of the dielectric constant ε of the insulator. The inventors have found that although ordinary insulator particles can be used, when insulator particles of the same size are used, a larger induced voltage is induced in the insulator particles to facilitate gas discharge. An insulator having a large dielectric constant ε is preferable in order to obtain a large induced voltage. As such an insulator particle, it is preferably an electron beam luminescent phosphor (a phosphor) particle which has been put to practical use. The high-efficiency luminescent CL light body has a lattice point that is not right, and the crystallization center occupies an asymmetric lattice point. The luminescence center occupying the asymmetric lattice point can perform electron migration which is not allowed by the luminescence center occupying the crystallization point of the symmetry crystal, and the electron migration probability is extremely large. : Practical phosphor particles are all reasons for crystals with asymmetry. And the amorphous crystal has (4) characteristics and has a large dielectric constant, p. For this reason, the camping particles are suitable for covering the metal electrode. The insulator amount is 0 35 200919527. The insulator induced charge amount Q and the insulator The surface area varies in proportion. In the case where the insulator is a thin film, the surface area of the insulator is larger when the particles are particles. The surface area of the particles densely arranged in a plane is indicated by _. This is the particle diameter. According to the description of Cath〇d〇luminescence, K〇dansha, _, P104-120 (Non-Patent Document 3), the particles to be surfaced on the predetermined surface are not related to the particle diameter, but are arranged. The number of particles is determined. The total number of particles to be attached is about three. For this reason, the insulator particles actually on the surface of the metal electrode are not one, but the particles of about three layers are attached to the metal electrode. The surface is attached to the whole genus; the insulator particle of the extreme surface i, which is the size of the electric raft, is limited by the adhesion of the particle to the metal surface. A plurality of particles are used. The particle size of the plurality of particles is not uniform - Straight: It is distributed by the normal distribution of the logarithm. The particles of the distribution are represented by the average value or the number of bits. The insulator particles are attached to the surface of the metal electrode by van der Waals force. The best results can be obtained by using the adhesive without the use of an adhesive. The adhesion (4) of the particles of the micro-mirror is between 1 μη and 7 μηι. μηΐ~5 μ Between ιη. The particle size is relatively weak, and it is easy to be due to mechanical vibration. Since then, the particle of the main force i (4) has fallen off from the surface of the metal electrode. The particle size is smaller than the water, and the air is condensed by air. Adsorption in the fluorescent discharge tube =::granule + child' is therefore not available. When the gas of the discharge lamp is discharged and there is a new electron source of the above condition, the current is not from the first characteristic of the metal electrode, L Θ , and the rim particle. The gas f is ionized by the gas and the electrons required for the white A I body discharge are taken from the gas space by ionization and disappear with the accumulated ions. That is, the discharge tube is a closed internal circuit. The inner claw is generated in the discharge tube, and the electric circuit is formed in the discharge tube without an electronic self-discharge circuit. The circuit (external circuit) of the internal discharge lamp is flooded. The current flows, but does not directly form an external circuit, and has an inductive power, and the internal circuit supplies the electrons. If the flow of electrons is limited, the sub-power circuit is independent. The electric circuit forming the internal circuit 2:::Fig. ^ Until now::: The internal circuit 15 and the external circuit 12 described above. The electric circuit of the drive circuit (4) The investigation of the discharge phenomenon of the tube is determined by measuring the electric light outside the electric tube. When the probe is connected to the camp light of the present invention and ...', the electric signal can be detected. There is a misunderstanding here. = Release the misunderstanding. Flow through the external circuit of Figure 2. The current, which is the dielectric polarization of the insulator particles of the electrode and the current flowing in the depolarization and the current flowing in the circuit (15). Currently, there is no way to detect the current of the internal circuit. Push: '', the electron flow from the external circuit can be gas discharge, then the internal current required for body discharge. Suppose an electron excitation calculates the radical: the sub-sub-generation produces a photon of light. Under this assumption, the discharge can be counted as the maximum electron flow of the body atom. The maximum current required can be determined by the amount of gas atoms normally filled in the fluorescent η. The number: When the internal volume of the fluorescent discharge lamp is known, the number of moles of the gas can be calculated according to the B〇yie_c-wavenumber, check:: law. The number of atoms contained in the mole number calculated using Α-gas ^. By converting the calculated number of pore atoms into a current, the current 37 200919527 in most fluorescent discharge lamps is about ο·ι mA. In fact, the electronic electrons constituting the internal circuit of the present invention can be reused. Therefore, if the discharge lamp is discharged, the fluorescent source is used to make the fluorescent light under ideal conditions. The consumption of the fluorescent lamp is smaller. A sound-saving fluorescent discharge lamp can be developed, but the helmet flow. Despite the lightning in the external circuit: the power in the discharge lamp is measured, but even so, compared to the power consumption of the usual U. Gas discharge thunder ^ " 鸯 first discharge lamp ' can greatly reduce the phase: the internal circuit of the electronic behavior is complex, even the electricity two; phase two results are also quite different. In order to realize the power-saving type of labor-saving discharge, the complicated electronic 月 is thus optimized for electronic behavior. The speed of the electrons taken out from the accumulated electrons on the surface of the self-polarizing insulator particles is close to zero. Because of the use of the commercially available discharge lamp, the field is used by the 丨 丨, / 士 匕 — ^ ^ „ „ „ „ „ „ „ „ „ „ „ „ „ „ „ „ „ „ „ ; ";; ρ1073-4, 1983 (Non-Patent Document 4) paper 'The sale of commercial light-emitting particles must have the capture of electrons and holes. 'The phosphor particles have a permanent internal: PIP. PIP charge The electric field expands outside the phosphor particles. Most of the time: the electric field outside the 'Xu phosphor particle expands to a negative electric field. The electron capture from the trap to the conduction band when the photo film 'day It' catches', the result is that the electric field of pip disappears. Fluorescent materials are widely used in electrophotographic photos or photosensitive materials for dry photocopiers. Commercially available discharge lamps use phosphors < ριρ as a photo-sensitive material, although the characteristics are weak, so it is not used as a photosensitive material, but the city Sold out = PIP' with crab light has a sufficient effect on the lower energy to the glory film: near, electron. This situation is difficult to detect in the experiment using the discharge lamp. According to Reference 3, PP141-149 Record, Yu Lei Kangzhao In the investigation of the characteristics of the fluorescent film under the iU· and the electric π 士, the quantitative analysis of the ριρ存38 200919527 is used. The size of the negative electric field of the PIP of the commercially available discharge lamp phosphor can be based on the phosphor. The film irradiation is determined by an experiment of an electron beam that accelerates the voltage change. The negative potential on the fluorescent film determined by the measurement is between ii 〇 v and i5 〇 v. From the back of the glass substrate coated with the fluorescent film. On the side, when a positive electric field of v or more is applied to the fluorescent film, the negative charge of PIP disappears from the fluorescent film and a positive charge occurs. The irradiated electrons reach the fluorescent film and emit light, and the external electric field is applied to cause the ΡΙΡ to disappear and disappear. The phenomenon is the same as that of the electrophotographic photo or the dry photocopying machine. It can be repeated many times. The developer of the fluorescent discharge lamp that does not understand the existence of the commercially available phosphor particles is to remove the fluorescent film. HP has a charge and hard work. It has been developed - a kind of instantaneously lit fluorescent discharge lamp, with a conductive film on the underside or surface of the fluorescent film 'or a conductive film on the outer wall of the discharge tube, or near the discharge tube Metal part of the outer wall An external circuit that applies a positive potential to the conductors only at the initial stage of discharge, and the lighting time is changed in units of seconds to minutes. As a method of lighting at a faster time, the film is attached to the fluorescent film around the electrodes. The accumulation of the film of the heterogeneous Cs atom or the irradiation of the fluorescent film, etc., the shortening of the discharge start time remains in the second unit

degree,. As described above, it is difficult to shorten the discharge start time, and it is related to the effect of P which is composed of the illuminant particles constituting the fluorescent film. As long as the fluorescent film can be removed, the fluorescent discharge lamp can be truly illuminated at a moment below 10 milliseconds. The instantaneous point of the fluorescent discharge lamp; g; m π ’', is a difficult problem, and therefore will be described in more detail. After the initial velocity is close to t 2 ^ into the fluorescent discharge tube, the electrons cannot be brought close to the fluorescent film due to the PIP generated by the phosphor particles. Even 39 200919527 can not enter the gas filled with gas atoms to do pq, u遐 two. The ++曰/丁幻员 electric field (5xl〇5 eV) of the electrons filling the outermost electron orbit of the gas in the gas space expands into the gas space, is blocked by its negative electric field, and the electrons cannot enter the gas space. Therefore, the fluorescent discharge lamp does not discharge. In order to discharge the gas to the body, the PIP of the phosphor film must be changed so that there is no negative potential on the surface of each phosphor particle. The best method is to use a CL phosphor to make a fluorescent film that emits light at a low voltage electron beam of 150 eV or less. This kind of love light body does not capture electrons in the phosphor particles, so it does not have PIP. If a low-voltage CL fluorescent system is used as the fluorescent film, the electric sputum that is taken out from the accumulated electron source easily enters the surface of the fluorescent film, and advances in one direction on the fluorescent film, and the surface is conductive. The electron collides with the convex portion of the fluorescent film with a slight unevenness to generate the phosphor particles to perform CL light emission. Therefore, it is confirmed that the surface conduction electrons are unidirectionally observed on the fluorescent film, but the light emission intensity is extremely low. The phosphor technician and the technician of the laboratorium have neglected the low dust η 2 light body because of its low luminous intensity. The present inventors are more concerned with the fact that the CL phosphor of the brightly-emitting light under the electron f has a lower glory film in the fluorescent discharge lamp than the light-emitting intensity. The experiment of low-electricity I CL phosphor film provides very important information related to the glory discharge lamp to the basis of her power mechanism. When using the electron supply source of the present invention and the low-energy illuminating CL fluorescent film, the gas of the fluorescent discharge lamp is instantaneously generated by the first reading of "1G" for the fluorescent discharge lamp. The instantaneous discharge has made various efforts', but this fact has lost its meaning by using the 丄鸯 丄鸯 丄鸯 , , , , , , , , , , , , , , 选择 选择 选择 选择 选择 电子 电子 电子 电子 电子 电子 电子 电子 电子 电子 电子 电子 电子 电子 电子 电子 电子 电子The tube instantaneously found 'scientificly promoted the bright hair in the fluorescent discharge tube 40 200919527 The explanation of the discharge mechanism of light. The 'electrode and anode lightning poles are asked; the electric field existing between the electrodes is one-way. If so thinking Then the electronic movement is also one-way. The case of encountering can be met. The electrons and gas atomic phases of the belt/outward movement are directly controlled by the horse and the son are 5·6χ10-13 cm. If the electron and the atom are 6χΓ〇: area As the atomic diameter, the volume of the electrons moving in one direction is cm / cm. At room temperature, 1 mole is the volume of the milk of the molar at 1 atm. / 2 / 1G (10). The diameter is m, the length of the tube is Μ, and the volume of the tube is one. The force is (M atmospheric pressure (7. Το-.τ.... Therefore, the number of moles of Ar gas in the 々 can be 1χ1〇.3mol (= 23/22 4χΐ〇·3). 6χ]02〇孔体The number of AV〇gadr turns is 6x 1 023, so the CCFL tube::::r body atoms are randomly distributed (Boltzmann points... one-way: path: contained... the number of atoms is very small, for... It is believed that ΐ does not collide with gas atoms. The electron velocity ',,, and the calculation clearly indicates the following facts. The discharge is now divided into two kilograms; the above calculation is one-way advancement in the gas space. This is not an electronic conclusion. ^The mouth is the most important factor for the one-way surface conduction on the fluorescent film when the oxygen is discharged. (10,7...fu...the gas meets with the oxygen atom. (m), the gas of the discharge tube cannot be observed. Thundering ^ 吏 gas discharge 'can force the unidirectional conduction surface conduction rail:: make the (4) trajectory of the electrons of the kinetic energy bend toward the gas space =: the road X to the curved acceleration electron and the gas atom non-elastic sheep Larger. Commercially available fluorescent discharge lamps with the use of the light-emitting particles - the application of 41 200919527 to bend the electronic track. Mixing low-voltage I in an appropriate ratio. When a lamp is used to produce a camping film with a light-emitting particle, it is possible to produce a fluorescent light that has both the surface conduction and the function of bending the track. There is a method of changing the fact that the phosphor particles granules and the planar shape of the fluorescent film are changed. The above fact can be confirmed by using a zinc silicate phosphor (Zn2Si〇4: Mn) which emits green light. The Zn2S1〇4:Mn phosphor can be produced by two methods. The first material is more than the chemical reaction meter, and the surface of the Zn2S1〇4:Mn phosphor particles is made. On the top, fine particles of Si〇2 which are unreacted due to excessive addition are attached. The attached particles of Si〇2 cannot be removed chemically or physically. After the phosphor is applied to the wall of the fluorescent discharge tube and a high voltage of 5 kV is applied to the electrode, the fluorescent discharge lamp emits green light of the bright shell. The s丨〇2 microparticles do not absorb the ultraviolet rays, and the negative charge of the charged SiO2 microparticles acts to repel the electrons into the gas space. However, @'s electrons cannot be placed close to the fluorescent film, so the anode region is housed in the SBE sheath formed on the Si 2 particles, and the fluorescence of the extractable fluorescent film is saturated. Even if the phosphor film of the CRT (cathode-ray tube) is formed by the phase (four) light body and the electron beam of the 15 〇 eV is irradiated to the camping film, the fluorescent film does not emit light. The reason for this is that the Si 〇 2 fine particles attached to the surface of the phosphor particles are negatively charged, and the electrons close to the fluorescent film are repelled. In this case, add 2% by weight of oxidized Zn〇 to the mixed raw materials, and use 5H>Kunming original tooth hopper@ to make fluorescent enamel. A large amount of unreacted Zn 〇 fine particles are attached to the surface of the produced phosphor particles. In order to remove chemically 42 200919527

ZnO microparticles are etched with phosphor powder prepared by ammonia solubilization & (NH4〇h liquid), and ZnSi 除去 which removes Zn 〇 microparticles can be obtained: Mn Laoguang ugly right is made with 6 ray phosphor CRT fluorescent film and irradiate the fluorescent film! The eV's electron beam 'fluorescent 臈 will be bright green CL# light. Apply the same mortar to the inner wall of the fluorescent discharge tube and apply a high voltage to the electrode. The fluorescent discharge lamp emits very dark green light. Thereafter, the phosphor powder prepared by excessively adding si〇2 at a weight ratio of 7:3 was mechanically mixed, and the glaze powder etched from the NH4 〇H liquid prepared by excessive addition of ZnO was prepared. In the fluorescent discharge tube, the surface of the γ γ # # # # # # 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此 此Brighter (enhanced force σ 3 ()%). Although the above experiment emits bright light when cl emits light, (4) it can be verified by emitting a darker phosphor in the fluorescent film of the fluorescent discharge lamp. For example, there is a case where the surface is chemically and physically cleaned by Y202S: Tb green poly-stop + μ, which is a fluorescent body of a color. The facts of this experiment are clearly shown to be important items that must be considered when manufacturing a fluorescent discharge lamp that emits light. Fluorescent discharge lamps with an inner diameter of 25 mm or more have long been used: rich, inexpensive, and recorded by white light of the phosphors. (4) (4) Phosphors [3Ca3(p〇4) 2CaFci: sbMn]. In the #1g_ below #光光灯, it is called (4) from the (four) price Μη ^ body brightness is very low and can not be used, but the use of the existence of resources exhaustion = halogen phosphorus (four) phosphors < 1G times the price of the mix White luminescent glory film of trichrome rare earth glory. Even if you consult the published book [cannot be a 3Ca3 (P〇4) 2CaFci: Sb: Mn can not be used in the lower diameter of the labor 43 200919527 light discharge lamp. The inventors have ridiculed the cause. (PO4) The luminescence of the 2CaFC1:Sb:Mn laborer is directly punctured by the Z + luminescence center, and the blue light emitted by Sb3 + is absorbed by the —* in the same particle to cause the yellow W+ to emit light. By the light emission of *(10)+ and Mn2+, white light is emitted from the phosphor particles. There is no absorption of the matrix crystal during the luminescence process. Thus, the phosphor has the characteristics of the insulator crystal under the irradiation of electrons. When the insulator crystal particles are placed in the electric tube, it is easy to form a strong < SBE on the surface of the particles. As a result, the gas discharge pole region is housed in the SBE sheath. When the discharge vessel diameter is reduced, the intensity of the SBE on the phosphor film is not high. Therefore, only the diameter of the anode region becomes small, and the gas discharge amount is saturated. In the same manner as the above-mentioned phosphor, a white light-emitting CLZn 〇 phosphor powder was mechanically mixed at a low voltage in a redundant (P04) 2CaFCl:Sb:Mn phosphor powder. Apply the = precursor powder to the inner wall of a CCFL fluorescent discharge tube with an inner diameter of 1G mm. The CCFL instantaneous discharge discharges white light with a brightness higher than that of the fluorescent film of the conventional fluorescent discharge lamp having an inner diameter of Μ _ or more. The above experiment shows that the fluorescent film in the fluorescent discharge lamp is brightly illuminated. A more detailed investigation of the electronic behavior of migration in gas spaces. One: Again. Acceleration of inelastic collisions of electrons produces excitation of gas atoms == ionization. When the accelerating electron has an appropriate size for exciting the gas atom, the I only produces an excitation of the gas atom, thereby emitting light (discharge). The electrons after inelastic collision with the gas atoms lose energy, change the orbit and stay in the gas space, accelerate again by the next high-frequency wave, and inelastically collide with other gas atoms. With this repetition, electrons are advanced toward the opposite electrode in the anode region in the discharge tube 44 200919527. The distance (mean free path) at which the electrons advance during the inelastic collision can be obtained from the determination (pd) of the measurement of the pasehen curve. The average free path found is 1 〇 _ in the HCFL and 〇 2 _ in the CCFL. Based on the potential applied between the cathode and the pole, the electric field strength per unit length is calculated, and the electric field strength in the mean free path is calculated. The representative CCFL has a tube length of 73 (10), and the peak potential applied between the electrodes is 匕V, so the peak value can be calculated as $〇.2x1〇-3v/〇2_. This value is far from the energy (10_4 eV) required to excite Hg (4) by inelastic collision of electrons. It is generally believed that electrons are accelerated by the potential gradient of the anode region, and in this idea, it is impossible to accelerate electrons that lose energy due to inelastic collisions. Thus the conventional idea is not correct. As mentioned above, the mass of the electron is 9X1G.28g, and the mass of the ion is 2 X 1 〇 4g. The amount of charge is not right. The difference between U and U is I (five) Ο.丨9 coulomb. Assuming that it is lighter = the sub-easily moves by the wave of the high-frequency electric field, the i-wavelength of the most frequent frequency wave obtained empirically is consistent with the average free-travel shore obtained from experiments. Calculate according to the experience, the length of one wavelength is changed with the applied frequency (1), ai = 〇-2 μια = 〇······································ 2X 1 〇-4 (2 ) Xcal = 0.3 μιη = 〇·3 χ 1 〇-4 ^ ) ^cal = 1.0 μιη ~ ι 〇χ j q-4 (4 ) 丨=1 0 μιη :=; ι ·〇 ι ι 〇·4 Average from the experiment from cm ( = 1 cm/5〇xl〇3 Hz) 50 kHz cm (= 1 cm/3〇xl〇3 Hz) 30 kHz cm (= 1 cm/l〇 Xi〇3 Hz) i〇kHz cm (= 1 cm/lxi〇3 Hz) j kHz is caused by the stroke within the error range of the measurement and the length of 45 200919527 1 wavelength. This agreement indicates that the first electron after the inelastic collision does not disappear from the gas space, but the energy from the high frequency electric field is again obtained by the wave of the high frequency electric field (peak voltage is 1,500 V). That is, the electrons present in the gas space do not disappear in the middle of the discharge tube, but proceed in the direction of (four) in the discharge tube with the resonance of the = wave, and the inelastic collision with the gas source 2 is repeated repeatedly. The anode region generated in the glory discharge tube is equivalent; the electrons of the excitation energy of the milk atom resonate with the high-frequency wave, and the electrons are generated by the electrons and the high-frequency resonance is generated by the electrons and the high-frequency resonance. In the direction of the forward mode, the potential gradient in the anode region is, 'Verify the past a large number of measurements 杳 · Large test 疋 抖 , , , , , , , = = = = = = = = = = = = = = = = = = It is considered that there is a potential gradient in the anode region, I, the reliability of the most recent measurement data accelerated by the potential gradient, and there is a problem in the technical aspect, and the method needs to be confirmed. In addition: the number of electrons detected in the cathode and the anode (4), so it is difficult to accept the collision of the gas and the gas atom to increase the number of electrons. When the charging state of each of the high-frequency crab light particles is optimized, the giant view: electron: the peak potential is greatly reduced. The resonance between the electron and the high-frequency wave is a phenomenon observed during the movement of the electron, and the electronic behavior of the microscopic observation of the electron beam of the electron beam is greatly affected by the state of charge of the coat surface of the camping film. _. When the other t high-frequency wave condition (50 k is called the average free path is 0.2 ^ 10,000 faces), the average particle size of the phosphor particles is i π and the electrons of the high-frequency wave resonate with each other, reaching the same-fluorescence The surface of the body is up to 2"-- 46 200919527 Accelerated into the CL phosphor particles of the fluorescent film, but according to the reference 1 3, it is impossible to form SBE on the surface of the CL phosphor, but to convert into surface conduction. By repeating the above-mentioned motion, the electrons are pushed in the discharge tube along the tube axis direction, and the accumulated ions accumulated at the other end of the discharge lamp tube are returned to the gas atoms. The high-efficiency fluorescent discharge lamp film must be Allowing lightning + 矣 矣 and shallow light. The surface conduction of the first electron must also have the function of making the surface pass the sub-orbit to the gas space. The fluorescent film of the above fluorescent film is instantaneous even in the dark. Further, since the electrons generated when the electrons enter the mortar particles, there is no coffee, and the brightness of the fluorescent film is eliminated. The present invention eliminates the major obstacles to the thermal solution in the conventional use of the fluorescent film. Can solve the above All problems related to electron supply = and fluorescent krypton, gas discharge: The invention provides a high-brightness and power-saving fluorescent discharge lamp fluorescent discharge lamp; ^ ΐ 3ζ-e * 1 atom Maximize the discharge' while minimizing the driving power of the FL. This is the other 43⁄4 / 3 lack of the first discharge lamp, which greatly prolongs the life of the fluorescent lamp. ° People buy a glory for a lifetime. The life-saving use of the fluorescent discharge lamp is related to the subject of the invention. The invention also provides a fluorescent discharge lamp that contributes greatly to the environmental protection course that has become a problem in recent years. [Embodiment] Detailed description using the drawings The invention - the electric product f FT inner valley. The lighting of the so-called fluorescent discharge lamp (FL) in the description refers to the following steps: The tycoon is connected to the metal electrode of the driving circuit, so that the discharge lamp is The discharge film of the inner wall of the discharge lamp glass is discharged, and by coating, will be excited by the gas. 47 200919527 Invisible ultraviolet light is converted into visible # ^, M ^ Brother Discharge lamp camp metal electrode Adding voltage and lighting the step._ Black 7^Tension light tube, the electronic device that stretches and thunder is not like the well-known firefly. "All the items are lightning & ^. The Meng electrode connected to the power circuit is directly injected into the discharge tube. The part is extracted by ionization u, and the electrons are taken out from the electron source inside the discharge lamp tube, and the surface of the door body particle is newly produced. After the electricity is generated, the disk and the electron are concentrated in the discharge tube. The other end of the separation. That is, the 4 + P junction, the internal circuit is sealed first discharge lamp. The lighting does not enter the Thunder technology, the electric 8 is also the external 4 will be the electronic injection B, but the discharge The inside of the lamp is supplied with electrons, and the Φ in the pipe is supplied into the *, ... 丨 1, ... 冤 ' ' and the discharge lamp is lost, the same two: heart, 'xiao consumption. The electrons entering the gas space do not disappear. The electrons are repeatedly repeated with the gas atoms to advance in the direction of the axis inside the discharge lamp. Gas:: Bounce, the gas contained in the electric tube is less than the number of atoms in the milk. The calculated current per flow rate is the internal mA of the wind-powered lamp, but the internal current is not directly measured and therefore cannot be confirmed. Fluorescent method, the electric current flowing through the system is determined by measuring the external circuit electricity. The power consumption of the fluorescent discharge lamp of the present invention is also wrongly determined by measuring the internal consumption of the external electric discharge lamp, and is not the same as the insulation current of the metal electrode of the cover metal. The polarization and polarization dissociation of the bulk particles are in agreement with the number of insulator particles covering the % pole of the gold Μ 虹 虹 捭 捭 金属 金属 金属 金属 金属 金属 金属 金属 金属 金属 金属 金属 金属 金属 金属 金属 金属 金属 幻 幻 幻 幻 幻 幻. If the induced current is also minimized, the watch is... The external circuit of the invention The reduction of the power consumption of the inventive Xenon discharge discharge lamp is reduced. The power consumption of this discharge lamp is _, 隹... The power consumption is conventional fluorescent. Further, since the electron supply of the present invention 48 200919527 = there is no metal exposed to the discharge gas at all in use, there is no metal money caused by the cation, so that there is no double due to the machine: the supply source is reduced. When there is no organic residual gas in the #light discharge lamp, the cause of the decrease in brightness in the discharge tube also disappears. As a result, the lighting life of the 'slip-discharge lamp tube is extended to the length of the horseman of the conventional fluorescent discharge lamp. Lighting life can be initial brightness protection _ (10)

More than above. J The electron motion in the fluorescent discharge lamp of the present invention is different from the electron motion in solid and liquid. The conduction of the atoms in the regularly arranged solids is limited. The liquid in which the atoms are arranged in an orderly manner... = the concentration of the two sub- or electrons is proportional. Although the discharge in the glory discharge lamp is different from that of (4) and the liquid, it is greatly affected by the charge distribution of the light-detecting film, and it is determined by the ohms. It is not used in the electronic light-emitting tube in the discharge lamp tube. 氺 氺 ^ ^ ^ 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 'The electrons and the high-frequency electric field resonate from the high-frequency electric field and the 曰政寨孙妗止v,, ^g又阿<阿月&s electron. The outer line has no charge, so the conventional discharge is not , the main ... the role of the charge on the film. The fluorescent film φ / think, face $, with the charge of the electrons and the migration of the electron sub-orbital ring to change the internal light of the electro-optical body particles ... It is inevitable that sf/ glory will be avoided in the presence of trace insulators on the surface of the surface-bound electrons (SBE) formed on the surface of the fluorescing. The electric field, the camping body particles are obscured. The Coulomb repulsion of these negative electric fields on the light film keeps the electrons away from the fluorescent 臈, and the fruit is placed in the negative charge of the gas discharge circuit, and is separated from the fluorescent film by SBE. There is a gas discharge path (anode region) at the distance. There is a non-excited (10) gas in the gap between the anode region and the fluorescent film, which effectively absorbs the result of the 254 nm f outer line emitted from the gas discharge path, and reaches the 254 (four) ultraviolet light of the Laoguang boat. The amount is saturated. That is, the presence of the SBE sheath causes the brightness saturation of the conventional fluorescent discharge lamp to limit the maximum brightness. The present inventors have found that mixing the phosphor particles in the appropriate proportions and maintaining the fluorescence of the coffee The bulk particles, and the use of the mixture to form a fluorescent film, can obtain high brightness from the fluorescent film', thereby providing a novel structure of fluorescent discharge lamp with high brightness, long life, and significantly reduced power consumption. Description of the principle of the FLi discharge mechanism of the present invention. The metal electrode 2 and the metal electrode 3 directly connected to the drive circuit of the discharge lamp are placed in the gas discharge lamp tube i, and are located outside the discharge lamp. The power source 6 applies an alternating-current high-frequency electric field to the metal electrode. For convenience of explanation, each of the metal electrode 2 and the metal electrode 3 is placed with an insulator particle 4. After the voltage is applied to the metal electrode 2 and the metal electrode 3, the insulator particle 4 is applied. It is instantaneously polarized in the polarization direction shown in Fig. 1. Generally, the dielectric enthalpy ε of the insulator particles is large, so the potential of the polarization charge induced by the insulator particles 4 is higher than the potential of the metal electrode 2 and the metal electrode 3. In the polarization charge induced by the insulator particles 4, the charge on the gas space side expands the electric field into the gas space. When the insulator particles 4 and the metal electrode 2 and the metal electrode 3 are placed in the ac high-frequency electric field, the periphery of the metal electrode The gas is instantaneously ionized by deducting the high frequency 50 200919527 electric field, and the distance of the electron 4 is. That is, the A white knives are opened until they do not produce mutual ώ ^ become free electrons and free ions. Free Thunder Gold Free ion in the gas air /, close. Greed, ... 'knife is not close to the polarization of the dielectric as the opposite electrode. The sin is near to the free electrons (the energy from the particles, from ... has entered the insulator electrons through the interface and the positive f* / in the insulator. Μ by the tongue. s #小胆Π < 罨 罨 错 错 5 The repetition is repeated, and the electron surface area is combined with the passage of time to form an electron supply source 7 on the surface of the insulator particles + 4 and the edge particles.

The water source 8 forms an ion source 8 formed of Ar+ on the surface of the insulator particle 4. The gas in the first discharge lamp is illuminated. The positive ion s from Ar+ is generated during the thunder of the electron transfer section taken out from the electron source 7. As described above, the entire lamp tube required for discharge is supplied and consumed in the lamp tube, and the gas discharge 5 is supplied from outside the discharge lamp tube. This is a feature of the on/off and discharge 5 of the electron of the present invention. Fig. 2 shows the flash circuit of the present invention. The two equivalent diagrams of the external lamp 12 for driving the discharge lamp and the internal circuit 15 for the discharge circuit V are shown. The external ~12 shown in Fig. 2(A) is composed of two capacitors 13 and a power source 6. The capacitor if the insulator electrode 4 of the metal electrode 2 and the metal electrode 3 is covered; in the circuit 12, the cb is buried and the polarization and polarization dissociation of the body are driven by the ac south frequency (with capacitance = rim The inductive electricity of the current (4) and then after the electrons move inside the discharge lamp will have electricity from the inside of the discharge tube... 'In the external circuit 12 12, when the circuit is not 12% plus & voltage, the electric circuit in the circuit is It is not maneuverable, and the discharge lamp is not discharged. Figure 51 (b) shows 51 200919527 The internal circuit 15 is taken from the electron supply source i6 to the positive ion source 17 of the discharge in the discharge tube, and the source 16 and the accumulation are positive. The ion source is composed of an ion source. The discharge is determined by electron supply, and the electron movement in the fluorescent discharge is generated. There is no direct electron flow according to the drawing. Between the circuit 15 and the external circuit 12, FIG. 3 shows a brief use of the present invention. Fig. Fluorescence discharge produced ~ operation glory discharge lamp 9 You accounted for and the valley is made of vacuum sealed glass tube 9 f. In the glass tube 9 ^ " 9 ^ 夕入 & ^ 臧 has multiple Metal electrode 2 and metal covered with insulator particles 4 Extremely 卞4 Covering | The radiant body particles (the inner wall surface of the size of the glass tube 9 is glare 1 〇- ^ 'μΠ1 or so) is coated with the fluorescent second discharge anode area u can not approach the light. Open some distance and arrange it on the broken glass tube 9: Yang: The UV light emitted by the area 11 does not have a thunder. 4 ^ Because it is in %, it is not affected by the charge of the phosphor particles in the fluorescent film. The body ^ a , 茧 膜 film 10 , is converted into visible light in the fluorescent film 10 . In the anode region u with rong, vapor. The non-excited mercury-based gas in the yang A 0 in the non-excited mercury ... w polar region u In the middle of the illuminating (4) absorbing the Μ before absorbing (self-absorption) 目,, and receiving) UV first, so the luminescence appears saturated. 4 fine case is described in the following fluorescent film. The invention consists of two parts The electron source 6 formed on the surface of the insulator particles on the metal electrode serving as the supply source of electrons in the first-system discharge lamp and the accumulation of the positive ions 17. The second system migrates in the discharge lamp and causes the gas to emit light. The behavior of electrons is affected by the charge of each of the phosphor particles that make up the glory film. The role of 'therefore is the job of finding the optimum conditions for applying the charge of the sub-body. Aiyou Body Particles 52 200919527 The fluorescent discharge lamp of the invention does not use a hot cathode as an electron supply source. The novel electron source of the present invention shields the cold with insulator particles. The metal electrode of the cathode () uses electrons accumulated on the insulator particles as a supply source. The substrate is a metal electrode of CCFL. Fig. 4 shows that the cold cathode electrode considered according to CCFL is covered with insulator particles 4 to cover the commonly used metal ^ Electrode structure of the surface. The most commonly used metal electrode is the bell-type electrode 19 shown in Fig. 4 (A). Although the bell-shaped electrode 19 can be used, the surface area of the bell-shaped electrode μ is large, and the number of insulator particles covering the surface is large, and the charging of the insulator particles causes a large induced current to flow in the external circuit, which is disadvantageous for practical use. . In order to minimize the induced current flowing to the external circuit by charging and discharging the insulator particles, the shape of the metal electrode can be flat. In Fig. 8 (8), the plate-shaped metal electrode 21 is placed, and the insulator particles 4 are adhered to the discharge metal surface of the flat metal electrode 21. The removal of electrons present in the electrode structure on the surface of the insulator exhibits significant anisotropy. As described above, the bell electrode 19 and the flat metal electrode 21 are connected to the lead electrode 18 for applying the voltage of the outer port 15. According to the paper of 1111}^(^1]^_1^^3¥.127 P1345 (Non-Patent Document 5), electrons have higher mobility when moving in parallel directions along the interface of the insulator, and if they are perpendicular to the surface Q In the conventional light discharge lamp, electrons are taken out at a right angle to the cathode surface, so there is a problem in taking power and δ. In order to instantaneously discharge the fluorescent discharge lamp, the order can be Η) (4) The speed causes the fluorescent discharge lamp f to directly enter the gas space, and the sub-supply source is taken out; first, the film is taken out, and the electrons are accelerated to be scattered toward the gas space. Gold 53 200919527 The genus electrode 21 is very suitable for taking out electrons in this order. Moreover, the electrons taken out from the flat metal electrode 21 are returned to the electrons between the laser π 1 of 1 mm to 3 mm from the tube of the fluorescent discharge lamp, so Apply the fluorescent film to a distance of about e蜢1 mm, and the full length of the fluorescent light will be evenly illuminated. In the CCFL of the driver, due to the size of the metal electrode, there is a defect that it will become darker than the end of the tube 丨〇mm, and in the .m ^ ^ ttLFL, due to the size of the hot cathode, it exists between the longer 2~3 cm. The variation from the muon is darkening the defect. This problem is solved when the flat metal electrode u of Fig. 4(B) of the present invention is employed. The human eye cannot perceive the difference in lighting speed of about 1 second of the fluorescent discharge tube used for house lighting. Therefore, even if the inventive fluorescent discharge lamp is used in house lighting, the human eye cannot perceive the 4 π point redundancy. difference. However, when the light-emitting discharge lamp of the present invention is used for a light source (backlight) of a display device such as an LCD, the speed of the speed of 10 milliseconds or less can be realized, and the line scan of the backlight can be realized. ...the result is 'reducing the dependence of the enamel presented on the screen on the characteristics of the lcd'. The human eye can clearly identify the improvement in enamel. As a result, the main image of the blood is trembled or distorted, and when it is based on carbon black, it is formed by the contrast between the illumination of 350 Cd/m2 as the illuminance of the light of the sky. Clear image. When viewing the current image on the current lcd screen for a long time, there is brightness at the black level. From this level, the high contrast value is used, so the upper limit is brighter and higher, which is equivalent to the image of the daylight that is directly exposed to the sun. $ And depending on the characteristics of the LCD, long-term viewing of unclear images that cannot be clearly identified can cause permanent damage to the human eye. As a result, glasses must be replaced every year. This problem can be solved by using the lcd of the CCFL of the present invention. Not only permanent damage to the individual's eyes. The power consumption of the LCD is also greatly reduced. Coffee 54 200919527 The light transmission rate is 8%. ^« Unable to carry out the line ^敕, the lighting speed is about 1 second, so the light is shining, and the right-handed line scan is used to make the back scan ratio inversely proportional. Reduced by the - time function. When the number is strip, the power consumption of the backlight is reduced to a very small number. If the number of lines is 20, the power consumption is 20%: 2 The power consumption decreases directly, causing the LCD display to save power. . The first diameter electrode 21 is favorable for the discharge tube glass right discharge * the glass inner diameter is less than 1 < 51 surface, if only one side of the insulator particles can not be taken out, a sufficient amount of electricity is not coated, two is not, in the flat plate Metal-like electricity... two surfaces are two". If you use Figure 4 (the electrode of the crucible, you can manufacture

Coffee with a brightness of above 71 and high brightness. Furthermore, in Fig. 4 (phantom ~ Fig. 4 (C), the small glass tube 2 is followed by a small break of the Ar gas and the Hg gas: tube, =

Si: The glass tube 9 is sealed and sealed. Heart =: The polarization of the 4 body particles is irrelevant, so there is no special requirement for flat gold. 'But is the workability better when using a material with a high hardness? = The electrode thickness of the metal electrode 21 varies depending on the metal material used. In order to maintain the insulator particles and the manufacturing process, I- 隹 令 易 易 易 易 设定 设定 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 The aspect that must be considered is the adsorption of organic and inorganic gases due to the surface of the worm. If there is a 'adsorption', the lifetime of the fluorescent discharge lamp, especially the luminescence of the glory film, will be weakened by the "body adsorption". Therefore, attention must be paid to the case where the alloy is used. 2 — _. 55 200919527 The diameter of the flat metal electrode 21 varies with the light discharge used, but in a fluorescent discharge tube with an inner diameter of 15 _ or more, a flat plate having a diameter of 1 〇 can be used. The metal electrode 21 is such that the maximum diameter of the flat metal electrode 21 is 1 Λ von 10 mm. When the diameter of the fluorescent discharge tube is between 5 mm and 15 mm, the straight and the metal electrodes are compared. The inner diameter is as small as 2 mm. When the diameter of the tube in the fluorescent discharge tube is 2_~5mm, the inner diameter of the large electrode of the metal electrode is 1 mm. The diameter of the tube inside the discharge tube is 2 mm. When you are in shape, the size of the metal electrode is smaller than the inner diameter by 〇5 mm. When the inside of the fluorescent discharge tube is 9 T, and the S horse is less than 2 mm, the test is done to the flat metal. Electrode 2〗 The work of prostitutes can be used in the same way as the work of the same kind of rod metal electrode. Figure 5 ( A) is an example of a rod-shaped metal. The surface of the rod-shaped metal electrode is coated with an insulator nt & the pole 22 is only squirted by a fusion splicer at the front end of the emet line sealed by the glass, and then the insulator particles are melted, so that it is finer The thickness of the metal rod attached to the metal bar is excellent in workability. The length is at o5mm 5 jobs ~1, the thickness is not limited. Of course, larger or smaller than this cup can also be used as an electrode. The surface of the metal electrode: the surface is a thick chain surface 'so that the insulator particles are easy to adhere to the chemically etched 'but preferably not The rough surface is formed by chemical etching. The surface of X 4 is difficult to adhere to the insulator particles + particles, and the 3 series is smooth, and the particle size of the insulator is slightly smaller than that of the crumb, and the powder is preferably used. The particle size 'and the particle size of the polishing agent. 卞3 value is 1~3 μπι powder 56 200919527 In order to make the insulator particles adhere more firmly to the metal surface, first (4) the surface of the genus is attached to the amorphous powder glass 23, Λ After the hot main horse has a temperature above 1嘁 = '绝 = body particle' And heating again, after the powder glass crucible is smelted: the portion to the room temperature 'insulator particles are firmly followed by the molten powder glass crucible. However, the performance is better if the powder glass is not used. The insulator coated on the metal electrode If the material 4 is an insulator having a dielectric constant ε of 3 to 50, (4) insulator particles can be used. If a dielectric 常 8 is used as an insulating 卩 on the 50 Μ, the ac voltage of the external circuit rises with this:: It The lighting speed of the discharge lamp is slowed down, and the power is also increased, so it is not good. Generally speaking, the evaporation temperature of the inorganic insulating material is also very stable. Therefore, there is no influence on the life of the fluorescent discharge lamp. $,, Deng Guang ^ The positive ions of the official towel do not directly collide with the insulator particles, as shown in Figure 1, and do not collide with the metal cathode of the negative potential. Therefore, there is no sub-existence in the fluorescent lamp s of the present invention due to the influence of the cathode on the life of the fluorescent discharge lamp: 'here', the life of the fluorescent discharge lamp is further described. I. "The other factor determining the fate of the discharge lamp g is the time-lapse of the brightness of the fluorescent film. The published book clearly states that the brightness of the luminescent film deteriorates with time, and is caused by the destruction of the luminescent center of the phosphor. Deterioration, but it is said that the illuminating center of the crystal lattice point is very stable. However, the phosphor particles > s ^, the vicinity of the 1 surface is unstable, and a large number of crystal lattices are generated during manufacturing. In particular, an anion having a large ionic radius has a y lattice detachment at the crystal interface and an anion defect between the atomic layer and the bottom 5 layers, and θ becomes an anion defect. When a phosphor is produced in a reducing gas atmosphere In the middle and high...', the number of oxygen defects is forcibly increased. The residual gas in the fire-emitting element discharger produced by the phosphor particle adsorption of the anion defect 57 200919527. The organic shale on the surface of the phosphor particle The experience absorbs the 254 nm extraneous line that is irradiated to the fluorescent film', so it reaches the first 352 ¥ + Μ 之 之 之 之 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线 紫外线A method of completely removing an anion defect. The main cause of deterioration of a fluorescent film is an organic residual gas. The residual gas can be removed to a negligible degree in a degassing step in the manufacture of a fluorescent discharge lamp. That is, if the fluorescent discharge lamp is improved The process of the tube can ignore the shadow of the residual gas: the organic residual gas is removed to a negligible degree. The fluorescent light-receiving lamp of the present invention can maintain the initial brightness due to neglecting all the factors related to the life, ιοο, οοο Above. Return to the topic of insulating materials. In the insulator particles used, each particle must be an independent particle. It is important that the particles are not contained. If the powder contains 0. 5 μηη or less particles, the powder is preserved. The contact surface of the smaller particles adsorbs the water in the air due to capillary condensation. The electrochemical reaction between the adsorbed water and the surface of the insulator particles causes the particles to agglomerate. Therefore, it is desirable that the insulator powder used does not contain antimony. · Particles below 5 μηι. The average particle size of the insulator particles is determined by the microscope to be 1 μηι~ It can be used between 10 μm, especially if an insulator particle having an average particle diameter of between 1 μm and 7 μm is used. The insulator particle material can be used as the inorganic oxide disclosed in the chemical handbook. The preferred oxides include Mg〇, SiO 2 , A 120 3 , CaO, SrO, BaO, Y203, La203, CaA103, citrate and lysine, and complexes thereof, etc. In addition, there is firefly 58 200919527

The base of the light body crystallizes. Some of the phosphors & B ® granules < steroidal crystals have asymmetric lattice points and have a high dielectric constant, which is advantageous. The phosphor particles 'which can be used as an insulator material' are Y2〇3, Y2〇2S, YV〇4, Yp〇4, ZnS,

ZnO, (Y, Gd) 2 〇 3, (Y, Gd) B 〇 3, γ (ρ ν) 〇 4, Lap 〇 4, and

BaMgAl10O17 #. It is also possible to use, in the base crystal of the above-mentioned phosphor, a phosphor particle which is an activator which is a center of the phosphor and which is a center of the phosphor. The compound containing S which is chemically active reacts with Hg vapor to form HgS (black substance), so it cannot be used. It can be used if the particle surface layer does not contain S. The surface of the particles used is chemically compatible with the surface: the surface that is cleaned. In addition to the above compounds, perovskite particles having a large dielectric constant are known. As a representative of pottery, there are PbZr03, pbTi〇3, CaTi03, SrTiO,

BaTl〇3, a solid solution of pbTi〇3 and pbZr〇3 (PZT), and a solid solution of PhT; n ^ 1〇3 and CaTi〇3. The dielectric constant of the perovskite particles is very large. ^ As mentioned above, even the particles of the material with a large amount of dielectric control are even free of electrons and ions of the 4 A, I仗槚, and the external electrons, and the external lightning is caused by the charge and discharge of calcium and taishiguang particles. The current induced current of the circuit is slow and cannot be used. The new electron source of the present invention is processed as a part of the manufacture of the A. By way of example, the method of έ田ΛΛ, 'D brothers and months as a new electron source for parts” [Example 1] The parts of the electron source of the present invention are wounded on the metal electrode to be appropriate Thickness cloth, and 邑 体 body particles. Since the insulating ν ν 体 粒子 缘 缘 缘 缘 缘 缘 缘 缘 缘 缘 缘 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 59 200919527 The commonly used media contains two media solutions as shown by I i. The same result can be obtained regardless of which solution is used. μ Media A ____ L~,丄” Butyl Acetate 100 e -------- Nitrocellulose 1 0 Media B ------- & Xylene 100 g ---- Ethyl Cellulose 2.0 [Table 2]

Material weight mixing ratio (2) ----- Y(V,P)〇1:Eu 100 medium A 150 ----J at Ni metal rod electrode selection Y(v,p)〇4:Eu red The light body powder was used as an insulator particle, and a slurry was prepared using the vehicle A.纟2 indicates the mixing ratio. Use the scale to accurately weigh the material of Table 2 and mix the two to make a slurry. The Ni metal rod electrode is immersed in the slurry and immediately pulled out, and then the slurry is attached to the surface of the rod electrode. The number of layers of the insulator particles to be attached was adjusted by changing the mixing ratio shown in Table 2. The layer of the insulator particles on the metal rod electrode that has been pulled out is wetted by the slurry, so that hot air of about 5 Torr is blown and dried. After drying, the electrode was placed in a capless oven and heated for 10 to 30 minutes. Heating causes the organic matter to oxidize and form water vapor and carbon dioxide gas to diffuse into the air. When the temperature of the Ni metal bar electrode was lowered to room temperature, a Ni metal bar electrode coated with a white powder of y(v,p)〇4:Eu red phosphor was obtained. The metal rod electrode coated with the white powder can be used as a CCFL electrode. [Example 2] Y2〇3:Eu red phosphor powder was selected as an insulator particle on a Nl-Cr disc-shaped metal electrode, and the vehicle B was selected to be mixed into a mash. Table 3 ^ Mixing ratio when no slurry is prepared. Use the scale to accurately weigh the material of Table 3 and mix the two to make a destructive solution. The Ni_Cr disc-shaped metal electrode was immersed in the slurry and pulled out, and the poly-liquid was attached to both surfaces of the disc-shaped metal electrode. The number of layers of insulator particles attached can be adjusted by changing the mixing ratio of 纟3. The insulating particle layer on the pulled-out Ni_Cr disc-shaped metal electrode is wetted by the breaking liquid, so that it is dried by blowing a slight hot air. Dry welding puts the electrode into the helmet cover, λ, after hiding, m 5〇C heating for 10~30 minutes, then the organic matter: decomposes by: and forms water vapor and carbon dioxide gas to diffuse to the air. When the temperature of the disc-shaped metal electrode is lowered to room temperature, the Ni_Cr disc-shaped metal of the white powder coated with the +0:EU red illuminant is obtained: the white powder disc metal electrode can be used as the nr L·疋 electrode And use.

[Example 3J Ba 〇 insulator particles and vehicle B were selected from the ruthenium metal rod electrode, and 61 200919527 was prepared into a slurry. Table 4 shows the mixing ratio thereof. The manufacturing steps are the same as those in the embodiment 丄 and the second embodiment, and thus the description thereof will be omitted. A Ni metal rod electrode coated with the white powder can be used as a CCFLi electrode.

---Li_4] Material Weight mixing ratio (g) 100 --- — BaO ---— Medium liquid B 150 ---—J

[Example 4] A BaMgAliG〇i7 insulator particle and a vehicle A' were selected from a Ni cup electrode to prepare a slurry. Table 5 shows the mixing ratio thereof. The manufacturing steps are the same as those described in the first embodiment and the second embodiment, and thus the description thereof will be omitted. The Ni cup electrode coated with the white powder can be used as the electrode of C (:FL. -_ϋ 5) Material ------- a weight mixing ratio of BaMgAlin〇_100 A liquid of A medium, therefore Although the same results as those shown in Examples 2 to 4 can be obtained by using oxides and polyoxygens which are not shown in the examples, the above description of the examples is also included in the present invention. [Example 5] For example, when the hot cathode of the HCFL Zhongguang 62 200919527 is replaced by the electron source of the present invention, it can be solved which is the most widely used electrode type hot cathode in the world. The hot cathode system uses oxygen, 〇 00〇Γ,^This is a cathode formed by heating a tungsten wire to the left and right sides of the crucible with BaO. The white is self-disposed on the upper surface of the heated BaO layer: Ba emits electrons into the vacuum. The temperature of the official wall near the electrode is higher than that of the other parts. The power-saving HCFL with an internal control of less than 1 〇mm is added to the high temperature (5 ° °, the hand can not touch) C~6〇(2). The reason why the temperature of the tube wall around the electrode rises is not Therefore, no countermeasure can be taken. According to the study of the present inventors, the surface of the cathode is covered by the inevitably formed surface-bound electron SBE (iQ5v/em), and electrons are taken out from the cathode to exceed the negative electric field of the SBE, and it is necessary to apply 1 to the cathode.阳极5 WCm or more of anode electric dust. The electrons taken out from the cathode are of course high-speed electricity with energy of V/cm α. The high-speed electrons entering the gas space filled with gas atoms are one of the stronger between the cathode and the anode. In the direction of the electric field, the electrons move toward one side, and the direction is advanced. The high-speed electrons that advance in one direction do not provoke the 'flower body atoms and pass through a certain distance in the gas space, and collide with the gas atoms inelastically. @ μ s ^ ionizes the atom of the milk and separates it into electrons and ions. Each person ionizes heat due to the change of the entropy of the gas atom. The temperature of the wall of the discharge lamp in the wider range around the hot cathode rises. High. High-speed electronic side: complex ', gas atoms undergo inelastic collision - face-to-point loss of energy, = cathode moves a certain distance, 'the energy of migration electrons is reduced to stimulate the disorder The energy of the electrons. The electrons excite the gas atoms without accompanying the heat production. This: The temperature of the tube wall is fixed at the length of the tube axis in the future. The first problem of the s soil/span rise hcfl near the cathode is the first problem. The following is the gas atom generated by the main discharge of the 夯 夯 μ μ μ μ μ 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 2009 Feng "Electronic correction, HCFL becomes CCFL, the energy of electrons from the electron source is close to zero speed, and does not cause ionization of gas atoms. Therefore, the temperature around the end of the fluorescent discharge tube in the lighting of the fluorescent discharge lamp = Therefore, the lighting power of the CCFL using the electron source of the present invention is less than that of the conventional HCFL disk CCFI. The lighting power of the first light bulb is significantly reduced. The first problem is that the cathode voltage generated by the cathode is reduced. The energy of all the energy of the singer discharge lamp is lost due to the decrease in the cathode voltage. Cathode voltage drops also occur in CCFLs and are therefore generally considered to be inherent in sub-thermal electronic cathodes. As described above, electrons are directly taken out into a vacuum, and are extremely covered by a view of a strong negative charge (1〇5 V/cm) which is inevitably formed. In order to take out electrons from the cathode, it is necessary to apply an anode voltage of i 〇 5 or more to the cathode. The electrons taken by the enemy φ 4 are strobed by an electric field in one of the stronger directions between the cathode and the anode, and proceed toward the direction of an ancient-a 4 gate. The high-speed electrons advancing in one direction 'inelastic collision with gas atoms during the process of passing through the gas space without exciting the emulsion atoms' cause the gas atoms to be ionized and separated into electrons and ions. The high-speed electrons repeat the inelastic collision with the gas atoms - the energy loss from the surface-points. At the distance from the cathode to the fixed distance, the energy of the transferred electrons is reduced to the level of the energy of the excited gas atoms. As described above, the generation of heat is not accompanied by the excitation of gas atoms by electrons. The electrons participating in the subsequent discharge are determined by the electronic behavior of the energy of the ancient milk & a _ /, which has the level of the atomic state of the milk, and becomes the discharge of the effect of the SBE which is not smashed and smashed on the U pole. . This discharge is the release of the anode region. The difference in the range of cathode voltage drop is consistent with the surface of the cathode 200919527 to the beginning of the anode region. Within this range, 'mixed with one from the cathode? Idle electrons with different energy values according to the location, free ions and free electrons generated by ionization of gas atoms, but the charged particles are not uniform, and are irregular according to the distance from the cathode surface. Variety. The 彳 && + > 语 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 々 The number of electrons is small. Other electrons and ions with energy | ^ ^ do not make gas atoms, and the factors in the electrons are poor. Ionization produces ion 盥 卞 卞 罨 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 τ is distributed in small spoons. The electric field of the ion distributed in the opposite direction (in the opposite direction to the anode electric field) acts on the light and moving electrons. In the month b, the values of the fast-moving electrons and the partial product are different. The complex distribution of the electrons that are easy to move according to the electric field strength, the ions of the 彳 彳 彳 傕 及 及 及 及 及 及 及 及 及 及 及 及 及 及 及 及 及 及 及 及 及 及And the resulting linear illuminating stripes. The range in which the cathode voltage is lowered is equivalent to the generation of linear luminescent stripes. If a conventional cathode is used, SBE is unavoidably generated on the cathode surface, so that a decrease in the cathode voltage is inevitable. The cathode voltage reduction can be completely eliminated from the conventional discharge lamp by replacing the conventional cathode electric power with the electron source of the present invention. As a result, the power consumption of the original CCFL using the electron source of the present invention is reduced by about 40% compared with the conventional product, so that it is erected. U makes a big contribution to the problem of %楗π dyeing. The third (four) is the lighting life of the fluorescent discharge lamp. The reason why the life of the discharge lamp used is shortened is that the positive ions generated around the electrode metal are elastically collided with the cathode by the cathode potential, and the portion of the cathode metal 65 200919527 is heated to a high temperature, thereby evaporating the metal vapor. If the electron source of the present invention is used, there is no metal exposed to the cation in the discharge gas. Therefore, life can be greatly extended. The details of the invention described above are improvements in the electron supply source of the fluorescent discharge lamp. If the electron source of the present invention is used, gll ώ can be used to extract the initial & The result of τ is that it can clarify the phenomenon that it is difficult to find the light in the study of light discharge lamps. The reason for the delay in the start time of the current (4) fluorescent spot, the storage time of the anode area, and the like is that the phosphor particles constituting the fluorescent film are: The physical properties of the particles, so the thermal method clarifies that the respect can explain the state of the charged center of the phosphor particles and the state of the discharge electrons. In Fig. 6, the four types of the fluorescent film of the fluorescent film which affects the gas discharge in the Ε Τ Τ & &## ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ ^ Figure ό (A) is attached to the fluorescent lamp 官 官 、 、 、 、 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市 市Figure. The whole particle of the commercially available PL phosphor is self-dressing & day f, then r, τ shows the long-term internal polarization (PIP), the negative charge of PIP, the scoop 丄5 〇v) + PL The light body produces a 'field that reaches the outside of the particle. It is a matter of course to use a commercial sale. When the negative surface of the fluorescent film 24 from the electrons is covered with the negative charge of the PIP, the electron e is close to the electron e whose initial velocity close to zero is ριρ. The electrostatic repulsion of the field cannot enter the glory film. Not only is it filled with a negative electric field due to the electrons of the outer shell of the outermost shell of the filled gas atoms. That is, the gas discharge / 6 # cannot enter the gas space. The gas atoms are not lit. 66 200919527 You can enter the fluorescent discharge camp. The interview with the knowledge of the wind is only the high-energy electricity. The discharge lamp tube takes high-energy electrons from the cathode and can enter the gas space, but the high energy: the child conduction, so the helmet method 上#上进仃The surface body is electrically activated. The gas of the fluorescent discharge lamp must be directed to the glory film before the gas discharge: : The high-energy electrons used advance in one direction, and the electrons are scattered and cannot be the same as the electric field of the light film. When a conductor is placed around the glory film and a positive voltage of about 300 V is applied to it, the phenomenon of the start of the discharge lamp will be discovered based on experience. Special CRT developers also know from experience that the positive electric field above = Luminous film...Glory: 4. The presence of PIP and its elimination method can be applied to dry photocopiers and electrophotographic photoplates. Phosphor materials can also be used as low-strength of photoreceptor plates, so they cannot be put into practical use. The glory film "ριρ is also used in special CRT (storage tube). As the starting method of the discharge of the fluorescent discharge lamp, the technician of the fluorescent discharge lamp has discovered the elimination method of the fluorescent film by experience." The law understands the existence of PIP itself, so it does not understand the principle of pot action. It is troubled by the elimination of problems caused by the elimination of HP, and the method discovered by experience becomes a secret inside the company. The inventor selects the glory body by selecting The PIP problem can be completely solved. If the phosphor type and the manufacturing method are controlled, a phosphor without a PIP in the fluorescent film can be produced. Fig. 6(B) shows that the phosphor particles are not used with the pip. When an electron with an initial velocity close to zero is introduced into the fluorescent film 25 made of a light body coat, the state of the electrons is transmitted on the surface of the fluorescent film. As a phosphor without ριρ, it is a CL that emits light under the irradiation of a low electron beam below ΜV. Fluorescent body. Representing the glory 67 200919527 m white-green light or at 39. A zinc oxide (zn〇) mortar with a peak and a pointed shape, and a blue light vulcanization without using steel as a refining agent (zns:Ag:cl) f light body, zinc sulfide (zns:cu:A1) phosphor emitting green light, and Mg〇 produced under special conditions. When the electron energy irradiated to the fluorescent film rises 4 i2 〇v is additionally produced by oxidizing excess The sulphate (Zn2Si〇4: Mn) glory, a strontium sulfate or butyl sulphate produced by chemical etching on the surface, and an oxidized period (¥2〇 or 劳光体) produced without using (4). The example of Fig. 6(8) shows the case where the honing film is made of Zn◦ phosphor. Since there is no pip g snow, the mouth is in the negative electric field, so the low-speed electrons entering the surface of the fluorescent film easily enter the fluorescent film, i The electric field accelerated by the accumulated ions 8 at the other end of the discharge tube advances in one direction on the surface of the phosphor film, reaches the accumulated ions 8 and recombines with the accumulated ions 8 to form gas atoms. In the usual FL tube ( Tube length 50 cm) on the electron orbit in one direction = the probability of a gas atom is calculable. The value is 1 〇 _6, and it can be considered that the probability of a unidirectional forward acceleration electron gas gas atom collision is zero. There is no gas emitted by the surface conduction electrons. Further, there is no method of directly measuring electrons that conduct surface conduction on a fluorescent iridium. Since a large induced current can be detected indirectly in the conductor disposed on the outer wall of the discharge tube, it is understood that a large surface conduction current flows. The following facts can be observed. The ho fluorescent film is a smooth surface. Therefore, after the accelerated electrons collide with the protruding portion of the fluorescent film on the surface of the fluorescent film, the fluorescent plate of the portion emits CL. Although the CL light is weak, it is confirmed that the accelerated electrons are moving in one direction. If the fluorescent film is completely smooth, it is impossible to detect the electronic motion. If the accelerated electron detection uses a fluorescent film of HjU phosphor (which emits light under the electron irradiation of V), the following facts can be observed. Y2〇3: A small number of phosphor particles in the Eu phosphor have defects. By the negative charge of the particles, the electrons that advance in one direction are bent, and the electrons accelerated by the surface conduction enter the gas filled with gas atoms. In space. The orbital acceleration electrons bent into the gas space inelastically collide with the gas atoms in the gas space. Gas atoms (Hg) that acquire energy due to inelastic collisions are excited to emit ultraviolet light. The emitted ultraviolet light is irradiated onto the fluorescent film, and the fluorescent light is emitted. The electrons that bend the orbit due to inelastic collisions stay in the body space and are accelerated by the high-frequency electric field applied to the gas space to excite other gas atoms in the milk space. This repetition occurs in the gas space, and the :: atom begins to discharge. The number of particles in the unidirectionally advanced electronic track contained in the glory film is small, so the PL luminescence intensity is low, but more than the ZnO phosphor film, there are many light particles in the #pL luminescence. In this way, the # PIj illuminating can clearly detect the acceleration electrons in one-way advancement, and the method in which the orbit of the electron is bent toward the gas space to excite the gas atoms. The same is true for the phosphor of Zn2Si〇4:Mn or red phosphor Y2〇2S:Eu=Μ. However, the light emission of the film made by these phosphors alone is lower than that of the practical level. The above: the inspection of the discharge lamp technology that pays attention to the practice, and because of the low brightness, it will be p-y» ', and as mentioned above, it is easy to provide the fluorescent film that is very important to provide the scientific information. Allowing low-speed electrons to conduct conductance on the fluorescent film, thereby accelerating electrons (the role of incentives), but does not directly contribute to the gas excitation in the fluorescent discharge 69 200919527. If a negatively charged phosphor particle is present in the phosphor film, the accelerated electron orbit is bent at the negatively charged phosphor particle to enter the gas space, and the gas atom is excited. The excited gas atoms emit ultraviolet light. The electrons of the inelastic collision stay in the gas space, are accelerated by the high frequency electric field, and excite other gas atoms. The gas discharge starts by this repetition. This is a mechanism for instantaneously lighting the gas discharge of a practical fluorescent discharge lamp. This observation is a very important finding for the scientific analysis of fluorescent discharge lamps. In Fig. 6(C), in order to confirm the above findings, Zn〇 phosphor particles 25 (no ριρ) are coated on a small area of the end of the fluorescent film of the fluorescent discharge lamp, and the remaining large area is arranged by a commercially available one. The fluorescent film 24 (with IP) of the PL phosphor particles covers the inner wall surface of the fluorescent discharge tube. Experimentally, PL phosphor particles were commercially available first on the inner wall surface of the glass, and after drying, the binder was incinerated. After the glass-side fluorescent film was wiped off with a soft cloth, Zn 萤 phosphor particles 25 were applied to the surface of the glass after wiping. The binder is incinerated after drying. The fluorescent film of Fig. 6(C) can be produced by this method. The X-ray film is further provided with the electron source of the present invention, and the initial velocity is close to that "electron electrons are accelerated at the arrangement of the ZnO phosphor particles 25, and /, there is energy of a politic gas atom. Acceleration electrons cannot enter. Commercially available on the fluorescent film 24, the curved electrons enter the gas space. The electrons entering the gas space collide with the gas atoms in an inelastic collision to excite the gas atoms to illuminate the discharge of the body space. The gas of the discharge lamp is instantaneously lit. The electrons of the inelastic collision acquire the appropriate energy from the 153-frequency electric field by the high-frequency wave in the gas space, and stimulate the gas atoms under the hair by the inelastic collision. The electron side of the high-frequency wave resonance of the road excites the gas source + by the repetition, and the surface migrates to the tube end in the discharge tube: finally, it disappears by combining with the ions. When people observe the Luguang discharge S and the A-wave with the eyes When resonating and migrating electrons, it is considered that the fluorescent discharge lamp g is a fluorescent film that emits light with uniform intensity. However, an important fact is omitted. The electrons migrated in the discharge circuit are added by It has energy and inelastic collision with the gas of 7 atoms. The orbital direction of the electrons in the inelastic collision is random. The electrons scattered in the random direction have electrons with the opportunity to be close to the camping film, but exist in the fluorescent film. The negative charge of PIP26, so the electrons...the method is close to the fluorescent film, but returns to the anode region. The range of electrons that illuminate the gas atoms by resonance with the high-frequency wave is not the entire two of the gas discharge tubes, and 疋 is limited to The gas space in the center of the discharge tube is kept at a fixed distance from the fluorescent film. The space is accommodated in the anode region of the PIP sheath 26. The electrical properties of the gas atoms are neutral and are not affected by the electric field and electric charge. Uniform concentration distribution. Between the anode region and the fluorescent film contained in the PIP sheath 26, gas atoms (unexcited gas atoms) are distributed at a uniform concentration. If the light emitted from the 2 anode region is excited by gas atoms The energy can be shifted to the ground state energy P white electrons to generate 'the light that is allowed to be emitted by the gas atoms. In this case, the light emitted from the anode region is between the anode region and the fluorescent film. The gas atom is absorbed and reaches the residual light after absorption by the light of the fluorescent film. In the case of the fluorescent discharge lamp, the light is emitted by the low-pressure Hg vapor. The light-emitting system is from the excitation energy level 6p of Hg to the ground state energy level. Migration, so it is absorbed by the Hg vapor existing between the anode region and the fluorescent film. The light system has no charged particles, so it is only affected by the PIP, only the Hg vapor exists between the anode region and the fluorescent film 71 200919527 The light remaining after absorption reaches the fluorescent medium. The phosphor particles have a large refractive index of the 2 ^ potassium 耵 sheep particles, so that one part of the ultraviolet light enters the glory particles arranged on the surface of the glory film and is directly illuminated. The center absorbs and emits visible light. The ultraviolet light reflected by the surface layer particles becomes scattered light, and enters the phosphor particles of the deep portion of the camping film to emit light. To increase the amount of ultraviolet light in the fluorescent film of the f-light discharge lamp, it is preferably The fluorescent film is not covered by ριρ negative. That is, it is preferred that the PIP sheath is not formed. If a positively charged PIP charge is applied to a conductor disposed close to the phosphor film. If you want to set up the company, the PIP sheath 20 disappears and the anode area expands to the fluorescent film to increase the brightness, but this is not the case. The 纟 不 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥 蝥The surface conduction of the advancement, the brightness of the fluorescent discharge lamp is significantly reduced. The high-intensity light-emitting film must have a combination of the phosphor particles that accelerate the electrons due to the conduction of the upper surface of the phosphor film and the phosphor particles that deflect the electron orbit toward the gas space. In practice, the force ριρ can not work. The anode area can be set, allowing the self-absorption of the atom, and the larger fluorescent discharge lamp with a diameter of 25 mm or more is used, and the best conditions are obtained empirically. This is a conventional fluorescent discharge lamp that allows self-absorption of 254 ultraviolet rays emitted from Hg in the anode region, and practically uses a glare discharge lamp having a phenomenon of luminescence saturation. According to the result of Fig. 5, as shown in Fig. 6(D), a commercially available PL camping body 24 having PIP and a low voltage CL phosphor 25 having no PIP are alternately arranged on the inner surface of the glass tube. It can be seen that the effect of ριρ26 is greatly reduced, the gas discharge 72 200919527 starts faster, and the anode region expands to cause the brightness to rise. The low voltage CL phosphor 25 must be selected here. An alternative to the low voltage CL illuminator 25 has been described above. Not all of these phosphors can be used. In the above-mentioned phosphors which are commercially available, fine particles having an insulator attached to the surface are treated as a surface treatment. In other cases, the processing of the phosphor is insufficient, and the residue remains on the surface of the particles. The electrons that have been irradiated from the anode region to the phosphor particles by scattering enter the phosphor particles, and the secondary electrons are emitted from the phosphor particles into the vacuum. At this time, holes are left in the phosphor particles. The hole 盥 · 欠 electrons are combined in a vacuum, and SBE is formed on the surface of the particle by the same mechanism as in the case of the metal cathode. If there are adhesion impurities, the luminescence of the gamma-based phosphor particles is also formed on the surface of the impurity, and a large number of holes and electrons are generated in the phosphor particles by the injection of electrons, and the holes and electrons are generated. The glowing nails are combined to illuminate. If the surface of the CL phosphor particles is clean, the ^ ^ ^ ^ hole on the surface of the shell J CL phosphor particles. The electrons in the vacuum that lost the object become free electrons, breaking the acceleration and bending the electron orbit toward the anode region' to facilitate discharge. Problem: The view produced by the impurities attached to the surface of the particles. It has a function with ^. The difficulty is that the SBE on the impurities cannot be eliminated. For this reason, it is very important that the low %* repeated CL swells, _ eve, and scale # · τ (four). The most reliable low-cost CL fluorescent work light body. Here, the brightness of the CL camper is greater than that of the PL lamp. Enter the number of singular injection electrons in the photon particle / the logarithmic scattering of the pen and the hole (about _). Another::,:Gate to order non-elastic - a photon can only excite a luminescence / on the one hand, PL illuminator particles " This is the reason why the CL phosphor is bright 73 200919527. It is most difficult to manufacture the PL phosphor 28 and the low voltage cl phosphor 25 adjacent to the inner wall surface of the fluorescent discharge lamp to produce a fluorescent film. According to the published paper, Journal Physics D Applied Physics, 32, (1999), pp5 13-5 17 (Non-Patent Document 6), the best fluorescent film thickness of fl is three layers of phosphor particles. The particles which are incident on the electrons of the fluorescent film are only arranged in the uppermost layer. The ultraviolet rays are not affected by the charge of the particles and enter the fluorescent film. When the depth of entry is expressed as the number of layers of particles, it is 3 layers. For this reason, the present invention can be manufactured by applying three layers of commercially available phosphor particles 24' after drying on the inner wall surface of the glass tube and then coating the low-voltage CL phosphor 25 so as to be spread on the commercially available phosphor layer 24. Fluorescent film. Fig. 7(A) shows a schematic view of the thus produced fluorescent film. Coating the phosphor film twice, resulting in a complicated work procedure. A method of fabricating a fluorescent film by coating a phosphor slurry once is designed. The average particle size of the commercially available pL light-appearing body is 4 μιη. The particle size of the low-voltage CL phosphor is 2 μ to the weight of the PL phosphor: CL phosphor = 7:3, and the two kinds of phosphor powders are weighed and placed, and the powder is placed in the weighing powder. In a mixing bottle, and mixing uniformly, a phosphor coating liquid is prepared and applied to the inner wall of the discharge tube glass. When the coating liquid is not dried, the PL is selectively collected near the glass tube wall. The phosphor particles 24 are collected on the surface of the fluorescent film: a small number of CL phosphor particles 25 are obtained, so that the glory shown in Fig. 7 (b) is obtained, and the fluorescent film of Fig. 7 (B) is used to produce the fluorite. In the light discharge lamp, the CL phosphor particles in the table=the SM do not form the SM, so the electrons having the south energy in the anode region reach the CL phosphor particles. As a result, the anode region is close to the fluorescent film by 74 200919527 and emits ultraviolet rays. The ultraviolet rays do not have unexcited Hg atoms between the anode region and the phosphor film, so that most of the ultraviolet rays are incident on the pL phosphor layer. As a result, the PL intensity of the fluorescent film increases. Here, when the average particle diameter of the PL phosphor is 4 μηι, the average value of the size of the CL phosphor particles used is 1 μηι to 3 μηι, and good results are obtained. The particle size of the Ik PL phosphor changes. It should be noted that when the phosphor particles are small and below 丨μηη, the particles are not arranged on the surface of the fluorescent film, but are concentrated at the bottom of the fluorescent film when the fluorescent film is dried. The effect of the light body particles becomes small. The fluorescent film will be described in more detail below using examples. [Example 6] An example of a mortar film in which the low-voltage light-emitting CL phosphor of the present invention was mixed was described. The fluorescent film was produced by mixing the phosphor powder shown in Table 6. As a low-voltage CL phosphor having good performance, a ZnS-based phosphor is present, but the sulfur S of the matrix crystal is chemically reacted with Hg vapor during discharge to form HgS, so that the zns-based phosphor is avoided. Weigh the weight of each phosphor powder of the meter 6 and place it in a mixing bottle, and fill it with the phosphor powder weighed. To the mixed powder, 媒5 克 of the vehicle A' was added and stirred to sufficiently disperse the phosphor particles in the slurry. The smoothing slurry was introduced into a glass tube having an outer diameter of 5 mm, and after a short period of time, the slurry was removed from the glass tube, and the phosphor particles were attached to the inner wall surface of the glass. The wuguang film was applied to the inner wall surface of the glass tube. After the hot film is dried by hot air, it is heated in a capless furnace at 600 ° C for 30 minutes, and the organic binder in the camping film is made into water vapor and carbon dioxide gas by thermal decomposition and removed from the tube 75 200919527. A glory film composed only of phosphor particles remains on the wall of the glass tube. The fluorescent film located at the end of the glass tube wall was wiped with a soft cloth. For wiping the glass ^. In the clamp position, any of the electrodes of Example 4 and Example 5 was inserted. One of the ends of the tube seals the electrode by melting a glass tube. The glass tube of the other tube end is slightly melted to make the tube diameter thin. After the Hg amalgam and the Ba collector are placed at the tip of the tapered pipe diameter, the small glass tube 2〇 of the opening is connected to the exhaust device, and the air in the glass tube is removed by a vacuum pump. The entire glass tube was placed in a furnace and heated to 500, except for the portion of the glass tube provided with the water >= i M Ba collector. The material inside the glass tube is degassed by the left and right sides. If the degassing step is over, the temperature is lowered to near room temperature. Thereafter, the Hg amalgam and the Ba collector are slightly heated, and the gas is discharged from the gases. Pumping

gas. Thereafter, an Ar gas of about 70 Torr was introduced, and a conventional glass containing Hg amalgam and a Ba collector was melted and the glass tube was disconnected from the exhaust device. After the disconnection, the Hg amalgam is heated and activated by the Ba collector. After that, the exhaust pipe of the electrode portion is melted and sealed, and a CCFL discharge discharge lamp having an outer diameter of 5 mm can be obtained. The Haihai CCFL lights up at a speed of about 1 second. Of course, the lighting speed does not change even in the dark. In the discharge lamp, there was no decrease in the cathode voltage, and the lighting power measured by the external circuit was reduced by 3 G% compared with the conventional CCFL. Further, there is no limitation on the size of the anode region, so that 13% or more of the light can be obtained from the fluorescent film of the fluorescent discharge lamp. 76 200919527 [Table 6] Phosphor 4 Drop Weight Mix Ratio (g) PL Blue Phosphor BaMgAl10O17: Eu2+ 15 PL Green Phosphor LaP04: Ce3+: Tb3+ 60 PL Red Phosphor (Y, Gd) B〇vEu3+ 25 Low Voltage CL Phosphor ZnO 10 Vehicle A 150 [Example 7] Table 7 is another example of a fluorescent film of the low voltage light-emitting CL phosphor powder of the present invention. A commercially available PL fluorescent system is a mixture of a chemical formula (Ca, Sr, Ba, Mg) (P04) 6Cl:Eu2+ emitting blue light, BaMgAl10O17:Eu2 + :Mn2+ emitting green light, and Y (V,P) emitting red light. 04: Eu3 + phosphor is prepared by emitting white light, and ZnO phosphor powder is added to the low voltage CL phosphor. The manufacturing steps of the fluorescent film and the manufacturing steps of the fluorescent discharge lamp are the same as those in the sixth embodiment, and thus the description thereof will be omitted. [Table 7] Fluorescent chemical formula Weight mixing ratio (g) PL blue phosphor (Ca, Sr, Ba, Mg) (P04) 6Cl: Eu2+ 20 PL green phosphor BaMgAlin0lv: Eu2+: Mn2+ 58 PL red Light body Y(V,P)04:Eu3+22 Low voltage CL phosphor ZnO 15 Medium A 120 77 200919527 [Example 8] Table "Foam film of low voltage light-emitting CL phosphor powder of the present invention Another other example. The rare earth elements used in the phosphors used in Examples 6 and 7 were very expensive. In particular, a large number of Tb elements that are gradually depleted of resources are used. There is an urgent need to develop a bright fluorescent discharge lamp that does not use these precious elements. In the x_y chromaticity coordinate = of NTSC, a bright green light Zn2Si〇4:Mn2+ phosphor is emitted. The phosphor powder has two different manufacturing methods depending on the PL and the CL. In the fluorescent lamp tube of the prior art, Zr^SiO^Mn2-phosphor powder is used for the user's pL, that is, the phosphor particle powder having a large amount of insulating fine particles attached to the surface of the particle. The phosphor powder can be used in a fluorescent discharge lamp having a large diameter, and the anode region is formed on the fluorescent film to form a stronger one.

In the SBE sheath, it cannot be used for the fluorescent film of a fluorescent tube with a small diameter. SBEi ZnjiOrMn2-fluorescent powder is not formed on the inner wall surface of the fluorescent discharge lamp, and is a bright CL-emitting Zn2Si04:Mn2+ phosphor powder irradiated by an electron beam of 120 eV. When the CL-emitting Zn2Si〇4:Mn2+ fluorescent moon a roll is mixed with the rare earth-activated blue phosphor powder and the red phosphor powder, a white light-emitting phosphor powder can be obtained. When the phosphor film of the phosphor powder is coated on the inner wall of a CCFL tube having a diameter of 15 mm or less, the luminescent Zn2Si (the sbe is not formed on the particles of the V_Mn2+ phosphor powder, and the anode region is close to the fluorescent film) Bright luminescence is performed. Therefore, the CL-emitting Zn2Sl〇4:Mn2+ phosphor powder can be used for mixing with multi-color Pl phosphor powder; the knife can be used to produce a white-light fluorescent film. CCFL with a fine e of 15 mm or less. It is possible to obtain a CCFL emitting white 78 200919527 without using a large amount of valuable Tb. Table 8 shows a mixture of phosphor powders obtained with a white fluorescent film with green NTSC chromaticity coordinates. The mixed powder is not limited to the PL phosphor powder shown in Table 8, and the other type of PL blue luminescent phosphor powder used in CCFL and other types of PL red phosphor powder are also used. The same results were obtained. The manufacturing steps of the fluorescent film and the manufacturing steps of the fluorescent discharge lamp were the same as those in Example 6, and therefore the description thereof will be omitted. [Table 8] Fluorescence * Theoretical weight mixing ratio (g ) PL Blue Phosphor BaMgAl10O17: Eu2+ 20 CL Green Phosphor (120 eV) Z n, Si04: Mn2+ 58 PL red phosphor YBO,: Eu3 + 22 low voltage CL phosphor ZnO 10 medium A 130 [Example 9] According to the results obtained empirically, the fluorescent film of the thin tube CCFL of Example 8 When the composition comprises about 35 wt% of the CL green phosphor powder and 23 wt% of the PL green phosphor powder, the highest brightness is obtained. Table 9 shows the mixing ratio. The mixing of Table 9 is an example of the example, and the mixture is mixed. The PL phosphor is not limited to the PL phosphor shown in Table 9, and other types of PL blue-emitting phosphor powder used in CCFL and other types of PL red phosphor powder may be used. The same results were obtained. The manufacturing steps of the fluorescent film and the manufacturing steps of the fluorescent discharge lamp were the same as those in Example 6, 79 200919527, and the description thereof will be omitted. [Table 9] Phosphorescence * Formula (g) - -20__ PL Blue Phosphor BaMgAlin017: Eu2+ CL Green Phosphor (120 eV) Zn? Si04: Mn2+ ~~-_ Green Phosphor Zn7Si04: Mn2+ - Color Phosphor YBO, :Eu3+ --- One Firefly Light body ZnO — ___ 乂 z —--- -- 1 ςη Media B --- — _ [Example 10] Used in Examples 6 to 9 Phosphor, a small moment and Carat: precious rare earth element in the concern of resource depletion, and therefore the price is very large system, especially four gradual depletion of resources used Shi Tb wash & each element.

:Open=Do not use these precious elements and brightly illuminate the light; the unidentified person looks at the calcium phosphate 2 luminescent phosphor Ca5(P〇4)3 (F, used in the conventional Dengguang discharge lamp) C1): Sb3 + : Mn2+. According to the present inventors: a fluorescent film produced by a letter of her fluorescent body exists in glory ancient? The problem of the lighting of the discharge is caused by the PIP of the middle mesh. Furthermore, the point is cut into a stronger SBE, the anode region (4) is in the (S) SBE line, and the voltage between the anode region and the fluorescent film is & vapor absorption 254 nm ultraviolet mainly by the light wheel of the fluorescent discharge lamp Out. The reason for this phenomenon is that the illuminating center is utilized in the illuminating light of the South glory body. 80 200919527

Sensitization of Sb" and Μβ, in a phosphor particle, μ directly absorbs 254·UV, and the blue light emitted by Sb3+ is partially absorbed by the hidden 2+, and emits light in a wide frequency band of the vapor color. The two sleeves are erroneously illuminating the two light-emitting bands and emitting white light. According to the activation of the sword, the road is dragged, the classification mechanism of the 丨^, d is the direct excitation of the phosphor, the electrons of the matrix crystal, With the moxibustion, you can't participate in the luminescence. This kind of phosphor emits only the darker ΓΤ l l l 。 。 。 。 。 。 。 。 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该'The electrons and holes of the crystal of the matrix do not participate in the luminescence, so the physical properties of the directly excited phosphor particles have the characteristics of an insulator under electron beam irradiation. As described above, on the fluorescent film in the fluorescent discharge lamp, the anode region The direction of advancement of the electrons immediately after the inelastic collision is random, and electrons having energy toward the energy reach the fluorescent film. If the electrons are irradiated to the insulator, the surface of the insulator particles is shaped like SBE. The amount of SBE accumulates over time, and the result is Production Strong t SBE. This causes the brightness of the fluorescent film to appear in the anode region when the anodic (four) light body is used. If the problem of the sheath is solved, the calcium halophosphate phosphor can be applied to the inner diameter. 2mm ccfl fluorescent film. If _phosphate calcium phosphor can be used in CCFL, you can get cheap white luminescent CCFL without using rare earth elements with resource depletion. _ Calcium phosphate phosphor has discharge The problem of the lighting delay of the illuminating light is a problem common to the PL phosphor used in the fluorescent discharge lamp, and the problem can be solved. The following describes the solution according to the embodiment. [Table 1 0] Fluorescent chemical weight mixing ratio ( 2) Calcium halophosphate phosphor Ca5 (P04), (F, Cl): Sb3+: MnH 70 Low voltage CL phosphor ZnO 30 Medium A ------ 150 81 200919527 As shown in Table 10, weigh 70 grams of white light (4) acid and mortar powder and 30 grams of blue-white light low voltage CL zn 〇 phosphor powder, and mixed with the powder. The mixed powder and 15 grams of media A Mixing and making a public liquid. The manufacturing steps of the camp light film are the same as in the sixth embodiment, so Slightly explained. Obtained - # CCFL, the obtained CCFL with inner diameter of 2 faces is instantaneously illuminated in milliseconds, and the glory film can not detect SBE'. The brightness of the light is far from the 翌 left and m遂% know the 25 mm tube fluorescent discharge lamp. The material cost of the calcium phosphate phosphor powder of the present invention is about one tenth lower than that of the currently marketed one. The developed inner diameter is more than 5 mm. The CCFL fluorescent discharge lamp is most suitable for indoor lighting. Especially the outer diameter is B~ another coffee is suitable for the illumination of the house. The development of the glory light is cheap, and the longevity is as long as 1 〇〇, _ hour or more, so the user advantageous. [Embodiment 1 1] When a CCFL of Example 1 is used for backlighting of an LCD, a red glory body. Publish the first 3 systems with Eu, the child as the illuminating center, and the glory body and utility of the actuator. Among them, "0 ev is the bright light that shines under the electron beam. The 3 illuminating light body under the transmission is Y2〇3:EU3 + but not limited to (4) Firefly: an example of the second WE11 帛 precursor enhanced red color.切切' other red phosphors can also be used to enhance red 82 200919527 [Table 11] ----- Phosphorescent chemical weight mixing ratio (g) Calcium halophosphate Cas(P04)3 (F, Cl) :Sb3+:Mn2+ 100 PL Body Y70,:Eu3+ 30 Low Voltage CL Camp ZnO 25 Media A —— 130

Table u is for enhancing the red wavelength range of caJPOddF/lhSb^Mn2·1 emitting white light, and adding Y2〇3:Eu3+ phosphor powder of red light to the mixed phosphor powder of Table 10 (There is a ray wavelength at 611 nm line). The mixed phosphor powder was mixed with the medium A using the medium A. The manufacturing steps of the subsequent fluorescent film are the same as those of the sixth embodiment, and thus the description thereof will be omitted. The obtained CCFL with an outer diameter of 2 mm is color-corrected by the illuminating of the Y2〇3:Eu3+luminescence (lighting at 611 nm line) at a speed of about 1 millisecond, which can be corrected in the backlight of the LCD. use. It also shows that the cathode voltage is not observed, and the characteristics of the SBE cannot be detected on the fluorescent film in the CCFL tube that is lit. [Industrial Applicability] According to the present invention, a glory discharge lamp can be realized, and the cathode voltage is not reduced, thereby saving energy. The current of the external power source can be reduced, and the light and dark stripe pattern near the electrode can be eliminated. Improve the illumination. According to the present invention, a fluorescent luminaire can be realized, and the metal cathode has no loss, so that the life of the fluorescent discharge lamp can be prolonged, and the illuminance of the scented light discharge lamp At the same time, it quickly lights up the surface of the king. The fluorescent discharge 83 200919527 The eunuch includes a straight tube, a curved tube, a ring technique, and a discharge lamp. In addition, this #明〇, Laoguang bulb and other fluorescent day and day display devices), in the right, the shoulder is not extinguished (liquid /, eight have used the fluorescent discharge tube [simplified description] Fig. 1 is an explanatory view of the fluorescent lithography of the present invention. The original drawing of the internal circuit formed in the discharge lamp of the present invention is related to the internal flow of the luminescence discharge lamp of the present invention. Outside the circuit. [5. Description of the drive circuit. Internal diagram of the circuit diagram: = and an illustration of the flow of electrons forming a discharge path for the luminescence discharge lamp. The cover is provided in the glory discharge lamp of the present invention. In the insulator particle two-plate=electrode, an example of a cup-shaped metal electrode and a ten-plate metal plate is used for the shape of the metal electrode. ρ FIG. 5 is an insulator particle disposed in the fluorescent discharge lamp of the present invention. In the electrode, the shape of the metal electrode is an illustration of a metal rod. Fig. 6 is a schematic view showing the state in which the electronic behavior introduced into the surface of the light-retardant film changes with the state of charge of the ruthenium film in the present invention. Invented by low voltage The state of the most light film produced by the sub-beam luminescent phosphor powder and the mixed powder of the photoluminescent phosphor powder. Fig. 8 is a table showing the metal cathode provided inside the conventional fluorescent discharge lamp tube; Explanation of the phenomenon of surface-bound electrons (SBE). [Main component symbol description] 84 200919527 1,9 Fluorescent discharge lamp (or glass tube) 2, 3 Metal electrode 4 Insulator particles 5 Gas discharge 6 External power supply (high Frequency power supply) 7, 16 electron source (electron supply source) 8 ion source (positive ion source) 10 fluorescent film (or phosphor film) 11 anode region 12 external circuit 13 capacitor 14 induced current 15 internal circuit 17 ion source ( Positive ion source or accumulation of positive ions) 18 Guide electrode 19 Bell-shaped electrode 20 Small glass tube 21 Flat metal electrode 22 Rod-shaped metal electrode 23 Glass medium 24 PIP fluorescent film (commercial PL phosphor film) 25 None PIP fluorescent film (CL phosphor film) 26 PIP (PIP negative charge or PIP sheath) 30 Metal cathode 85 200919527 CCFL Cold cathode fluorescent discharge lamp CL Electron beam illumination (Cathode Luminescence) e Electron (emission electron) EL Inorganic electric field emission FL Fluorescent discharge lamp h Hole HCFL Hot cathode electrode LED Light-emitting diode LCD Liquid crystal display OLED Organic electric field display PIP Permanent internal polarization PL photoluminescence ( Photo Luminescence) SBE surface-bound-electrons uv UV

86

Claims (1)

200919527 X. Application for patents: L-type fluorescent discharge lamp, the surface of the soybean meal is coated with a fluorescent film ^ The lighting inside the glass tube of the first discharge lamp is the external circuit of the discharge gas source in the glass And produced. The circuit is connected to the electricity 2. The luminaire discharge lamp of the patent application is composed of a sub-source, and the gas in the fluorescent discharge lamp is moved during the process: the gas is taken in the gas space. When the electrons are moved toward the ion source and the *migrated electrons reach the ion source, the electrons recombine with the ions, and the (4) circuit is closed. For the electric fluorescent lamp tube of the second aspect of the invention, the electrode for forming the pen source is arranged in the layer 1 of the fluorescent discharge lamp tube. The metal electrode of the field + T卞 is used as the electrode for the ion and the electrode for the electrode, and the metal electrode of the electric insulator particle is contained in the fluorescent discharge lamp. And the θ-shaped coating (4): the working light discharge tube according to claim 3, wherein a positive polarity is applied to the metal electrode of the source forming electrode, and the electrical insulator particles of the metal electrode are mesogenic The free electrons generated by the gasization of the gas around the electrode are subjected to the meson # 丨 丨 该 该 该 该 该 该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该 将该a space source formed by combining positive charges in the second"; and applying a negative potential to the gold electrode of the ion source forming electrode, and electrically insulating the electrical insulator particles 87 200919527 of the metal electrode, and the periphery of the electrode The gas generated by the gas ^ jrrr η ^ ionization is subjected to the dielectric polarization of the electrical insulator particles - ϋ % ^, which is attracted by the electron, and the polarization of the ion-particle particles The ion group formed by the °, °, ° σ as the fluorescent discharge lamp of the fourth member of the patent application, the bean is taken out from the electron source to the surface of the fluorescent film, eight #雷; The error is caused by the conduction of the surface of the luminescent film to accelerate the electrons, accelerating the electronic Helmet # 丄 丄: the cause of the start of the discharge, by the negatively charged phosphor particles, and detecting the n, the 忒 accelerates the orbit of the electron to the gas Space, so that the first discharge of the fluorescent tube of the fluorescent tube #1 ^ + 2 凴 discharge, thereby generating a gas discharge with a reduced cathode voltage. 6. The fluorescent discharge lamp of the scope of the patent application, wherein The surface of the fluorescent film is alternately arranged without a V-Bei electric phosphor particle and a negatively charged phosphor particle, and is applied to a plurality of portions of the surface of the fluorescent film by the tape. The negatively charged phosphor particles bend the twisted + text and the electrons toward the gas space side. 7 · The fluorescent discharge lamp g ', Zhong Yiying, as in any one of the main items The fluorescent film coated on the inner wall surface of the glass tube of the light discharge lamp is composed of a mixed powder of an electron beam luminous powder and a photoluminescent working powder. 8·If the patent application scope is 7 Fluorescent discharge lamp, t, the photoluminescent phosphor powder is It is composed of three kinds of rare earth photoluminescent phosphor powders which are three-color light, and the electron beam luminous powder is composed of low-voltage electron beam fluorescent powder. 9. As claimed in the patent item 8 Fluorescent discharge lamp tube, 苴中, the rare earth photoluminescence phosphor is only included] 吏肖CL#光石石酸锌营光88 200919527 Body powder replaces the green light photoluminescence phosphor powder 10. The fluorescent discharge lamp of the eighth aspect of the patent application, wherein the rare earth photoluminescence phosphor powder uses CL light-emitting strontium phosphorate powder and PL-emitting zinc citrate The mixed powder of the light body powder replaces the photoluminescent phosphor powder that emits green light. 11. The fluorescent discharge lamp of claim 8, wherein the phosphor film is arranged such that the particles of the low voltage electron beam emitting phosphor are discontinuously dispersed on the surface of the fluorescent film. 12. The fluorescent discharge lamp of claim 9, wherein the particles of the low voltage electron beam illuminating phosphor are arranged to be discontinuously spread on the surface of the fluorescent film in the 'Hawa film. . The fluorescent discharge lamp of the first aspect of the invention, wherein the particles of the low-voltage electron beam illuminating phosphor are discontinuously spread on the surface of the fluorescent film. For the voltage, the fluorescent discharge lamp of the seventh aspect of the invention, wherein the light film is a photoluminescence phosphor powder and a low beam emission phosphor powder which emit white light in the morning. It is composed of a mixed powder. For example, the scope of the patent application is the only one, the disaster ~ from the eunuch, among them. In the light, the photoluminescence of the self-chromic photoluminescence is composed of a phosphor. 16. If the patent application scope is 帛15; the page is proud of the fluorescent film B*t. 胄, additively added with enhanced red luminescence of the electron beam 钇 phosphor. Ding not seven oxygen first 17 · An LCD display device is characterized by a single or multiple 89 200919527 as claimed in the scope of patents! The light-emitting discharge lamps of the above-mentioned items are arranged on a flat surface as the backlight of the LCD display device. The LCD display of the 17th item of the humiliation and consumption is arranged in the vertical direction, and a plurality of the discharge lamps are arranged in the vertical direction, and the plurality of fluorescent lamps are sequentially placed in the group 1 line sequence scanning. Screens. Redundant, and the image of the line sequence is reflected to the whole of the device. 十一:《式:如次页 90