JP2000118010A - Liquid ejecting device and recording device with scanner - Google Patents

Abstract

(57) [Problem] To achieve high image quality and high gradation printing by setting the ejection frequency of ink droplets ejected to form one pixel. SOLUTION: It has a liquid chamber for storing ink, a plurality of ink ejection ports connected to the liquid chamber via a liquid path, and an energy action section for applying energy to the ink in the liquid path. In response, a pulse signal is input to the energy action section, and by the action force of the energy action section,
Ejecting and flying an ink droplet 24 from the ink ejection port,
In the liquid jet recording apparatus for performing recording by attaching the recording medium to the recording medium 25, the opening area of the ejection port is less than 500 μm ^2, and the frequency of ejection of the ink droplet 24 is 10 kHz or more per ejection port.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

[0001] The present invention relates to an ink jet recording apparatus.

[0002]

2. Description of the Related Art The non-impact recording method has been attracting attention for office use and the like because the noise generation during recording is extremely small to a negligible level. inside that,
The so-called ink jet recording method is an extremely effective recording method that can perform high-speed recording and can perform recording without requiring a special fixing process on plain paper.
Various systems have been proposed or commercialized and put into practical use.

In such an ink-jet recording method, recording is performed by flying small droplets (ink droplets) of a recording liquid called so-called ink and attaching the ink droplets to a recording medium. For example, the applicant has disclosed in Japanese Patent Publication No. 56-9429. Here, in summary of the invention disclosed in Japanese Patent Publication No. 56-9429, the pressure in the ink is increased by heating the ink in the liquid chamber to generate bubbles, and this ink is discharged at the tip of a fine nozzle. The recording is performed by discharging from an ink discharge port.

After that, many inventions have been made utilizing this principle, but there is still an unsolved problem in achieving higher image quality recording.

[0005]

Problems to be Solved by the Invention JP-A-56-9429
Although the invention disclosed in Japanese Patent Application Laid-Open Publication No. H11-209555 discloses the basic principle of a system using bubbles, it is unclear how to perform high-quality recording.

[0006]

According to the first aspect of the present invention,
A liquid chamber for storing ink, a plurality of ink ejection ports connected to the liquid chamber through a liquid path, and an energy action section for applying energy to the ink in the liquid path; In a liquid jet recording apparatus for inputting a pulse signal to an action section and ejecting and flying ink droplets from the ink ejection port by the action force of the energy action section and attaching the ink droplet to a recording medium to perform recording, the ejection port Has an opening area of less than 500 μm ² , and the ink droplets have an ejection frequency of 10 kHz or more per ejection port.

Therefore, not only high-resolution printing is enabled, but also the effect of inertia is small because the ink amount of one drop is very small, and the response as a liquid jet recording head is fast (the ink droplet ejection frequency is low). Large), and high-speed driving became possible.

According to a second aspect of the present invention, in the liquid jet recording apparatus according to the first aspect, the flying speed of the ink droplet is set to 5.2 m / s or more.

Therefore, the pixel position accuracy on the recording medium is maintained with high accuracy, and high-quality recording has become possible.

According to a third aspect of the present invention, a recording apparatus with a scanner is constructed by providing an image reading device in the liquid jet recording apparatus according to the first and second aspects.

Therefore, the realization of a liquid jet recording apparatus capable of extremely fine recording (high-resolution recording) makes it possible to achieve high-quality recording.
A device such as an ink jet copier (copying machine) that outputs an ink jet according to a read image has been realized.

According to a fourth aspect of the present invention, there is provided a liquid chamber for storing ink, a plurality of ink discharge ports communicated with the liquid chamber via a liquid path, and an energy action section for applying energy to the ink in the liquid path. A pulse signal is input to the energy applying unit as needed, and the ink droplet is ejected from the ink ejection port and flies by the acting force of the energy applying unit, and is adhered to the recording medium to perform recording. The liquid ejection recording apparatus for performing the above is provided with a scanner which is an image reading apparatus, and the scanner information is set such that the frequency of the ink droplet ejection is set to 10 kHz or more per one ejection port, and the speed at which the ink droplet flies is 5 kHz. 0.2 m / s or more.

Therefore, conventionally, the recording speed of an ink-jet image has been slow, and it has been difficult to realize a usage like a copier. However, it is necessary to increase the recording speed and to clarify a stable flying condition of ink droplets. Accordingly, it is possible to realize high-quality recording, and to realize an ink-jet copying machine that performs an ink-jet output according to a read image by combining a scanner that is an image reading device.

[0014]

DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described with reference to the drawings. First, FIG. 17 is a side view for explaining one embodiment of the heating element substrate of the first ink jet recording head according to the present invention, in which the first electrode 2, the insulating layer 3, the heater 4, The second electrode 5 and the protective layer 6 are sequentially formed in a laminated state. One end (part A) of the first electrode 2 is a part from which a lead wire is taken out, and the other end (part B).
Is a portion to which one end of the heater 4 is connected.

FIGS. 18 (a) to 18 (d) are views showing a procedure for obtaining the configuration shown in FIG. 17. First, as shown in FIG. Form on top. FIG. 2B shows a case where an insulating layer 3 covering the first electrode 2 is formed, and both ends (parts A and B) of the first electrode 2 are not covered with the insulating layer 3. FIG. 2C shows a heater 4 formed on a part of the insulating layer 3, and FIG. 2D shows a second electrode 5 formed on a part of the insulating layer 3. One end of the second electrode 5 is connected to the other end of the heater 4.

Here, the materials used in the present invention include, for example, Al and Au as materials for the electrodes 2 and 5, which are applied using techniques such as vapor deposition, sputtering and plating, and are well known. As described above, a pattern is formed by a photolithography technique. As a material of the insulating layer 3, SiO ₂ , Si ₃ N ₄ or the like is applied and patterned by the same method. The heater 4 is formed in the same manner, and examples of the material include tantalum nitride, nichrome, and hafnium boride.

In the present invention, for the sake of simplicity, only the minimum required structure has been described. For example, as a method for forming the electrodes 2 and 5, Au or Al is deposited thinly and then plated with Au. It is also conceivable to have a two-layer structure formed thicker, and the insulating layer 3 may have a multilayer structure. Also, it may be necessary to provide the substrate 1 with a heat storage layer that does not allow the heat of the heater 4 to escape.

FIG. 19 is a view showing an embodiment in which the first electrode 2 shown in FIG. 18 serves as a common electrode for the plurality of second electrodes 5 and the heater 4.

In such a manner, the applicant has determined that the heater 4
The heating element substrate having an array density of 48 lines / mm (corresponding to 1200 dpi) was manufactured.
Is 256).

Next, in order to complete the heating element substrate as an ink jet recording head, it is necessary to form ink liquid paths and ink discharge ports. For example, an ink jet recording head is completed by joining a lid substrate 9 having a groove 7 and a concave portion 8 as shown in FIG. 20 to the heating element substrate described above. The arrangement density of the liquid passages is 24 lines / mm, 32 lines / mm.
The recording head was formed by photolithography in order to obtain a high precision liquid path pattern because the density was very high, such as 48 mm / mm.

Next, an example of an ink jet recording head formed by photolithography will be described with reference to FIGS. FIG. 21 shows a heating element substrate, on which a heater 11 and a thin film 12 covering the heater 11 are formed. In this step, a required number of heaters 11 are arranged on a substrate 10 made of a material such as Si, glass, and ceramics.
Further, a thin film 12 of SiO ₂ , Ta ₂ O ₅ , glass, or the like is coated as needed to impart ink resistance and electrical insulation. Although not shown, an electrode for inputting a pulse signal is connected to the heater 11.

In the step shown in FIG. 22, the surface of the thin film 12 obtained through the step of FIG. 21 is cleaned and dried, and then a liquid photoresist is applied by spin coating, followed by pre-baking (for example, 80). 30 ° C
Minutes). The liquid photoresist can also be satisfactorily applied by roll coating, dip coating, or the like. It has been conventionally proposed to use a dry film photoresist to form a liquid path pattern, but the dry film photoresist is intended for its intended use (for forming a pattern on a printed circuit board).
Therefore, it is difficult to form a high-density pattern. At present, it can be formed up to about 16 lines / mm,
Higher density arrays are difficult, and as in the present invention,
It is not suitable for forming a high-density pattern. In the present invention, as a liquid photoresist, BMR manufactured by Tokyo Ohka Kogyo
By using S-1000 and changing the rotation speed during spin coating in the range of 500 to 2500 rpm, the thickness of the photoresist layer 13 to be formed is 7 to 30.
It could be changed down to μm.

Next, after a photomask 14 having a predetermined pattern is overlaid on the photoresist layer 13, exposure is performed from above the photomask 14. At this time, the positioning of the heater 11 and the pattern of the photomask 14 is performed by a known method.

FIG. 23 shows a process in which the unexposed portion of the exposed photoresist layer 13 is dissolved and removed with a developing solution comprising a predetermined organic solvent such as trichloroethane. Then, after the unexposed portion is dissolved and removed with a developing solution, a heat curing treatment (for example, at 150 to 250 ° C. for 30 minutes) is performed to improve the ink resistance of the exposed portion of the photoresist layer 13 left on the substrate 10. ~ 6 hours heating), or
UV irradiation (for example, UV intensity of 50 to 200 mW / cm ² or more) is performed to sufficiently promote the polymerization and curing reaction. It is also effective to perform both the above-mentioned heat curing treatment and ultraviolet irradiation.

FIG. 24 shows a cover substrate which covers the grooves 15 and recesses (not shown) formed in the photoresist layer 13, and is a plate-like member made of a material which transmits electromagnetic waves, for example, a transparent ultraviolet light material. A dry film photoresist 17, which is a photosensitive resin film, is laminated on one side of 16.
The dry film photoresist 17 is laminated by using a commercially available laminator so that air does not enter between the flat plate member 16 and the dry film photoresist 17. In the present invention, SY-325 manufactured by Tokyo Ohka Kogyo Co., Ltd. was used as the dry film photoresist 17.

FIG. 25 shows a step in which the dry film photoresist 17 of the lid substrate shown in FIG. 24 and the photoresist layer 13 on the heating element substrate shown in FIG. 23 are pressed and attached. At the time of this pressing and sticking, ultraviolet irradiation under a non-oxygen atmosphere (for example, 50 to 200 mW)
/ Cm ² or more).
Dry film photoresist 17
Is fully cured. Further, a thermosetting treatment (for example, 13
Heating at 0 to 250 ° C. for 30 minutes to 6 hours) is also effective.

FIG. 26 is a perspective view showing a state after the step shown in FIG. 25 is completed. A liquid passage 18 through which ink flows is formed by covering the groove 15 with a cover substrate. Is covered with a lid substrate to form a liquid chamber 19 for storing ink. The lid substrate is provided with an ink introduction hole 21 to which an ink supply pipe 20 (shown in FIG. 28) for supplying ink into the liquid chamber 19 is connected. Then, the front end portion of the liquid passage 18 is cut along the line AA, and the cut surface is smoothed to form an ink discharge port 22 (shown in FIG. 28). By mounting the ink supply tube 20, the ink jet recording head 23 is completed. The cutting along the line AA is performed in order to optimize the distance between the heater 11 and the ink discharge ports 22, and the region to be cut is appropriately determined. For this cutting, a dicing method usually used in the semiconductor industry is adopted.

FIG. 27 is a sectional view taken along line BB in FIG.
FIG. 28 is a cross-sectional view showing a completed inkjet recording head 23 after cutting along the line AA and attaching the ink supply pipe 20 are completed. is there.

By changing the thickness of the photoresist layer 13 by the method described above, the present inventor has set the ink discharge port 22 and the liquid path 18 from 24 lines / mm to a maximum of 48 lines.
The ink jet recording head was completed by forming the ink at an arrangement density of 1 / mm.

The size of the ink discharge ports 22 at this time is 22 × 22 when the array density is 24 nozzles / mm.
μm, 17 × 1 when the array density is 32 lines / mm
7 μm, 14 × when the array density is 48 lines / mm
14 μm.

In such a configuration, FIG. 1 uses an ink jet recording head 23 formed as described with reference to FIG. 21 to FIG. Body (for example,
FIG. 2 shows a state in which one pixel 26 is formed by adhering to the same place on a sheet (paper) 25. The important point here is that
The present invention is characterized in that each ink droplet 24 is separately ejected and flies in response to the input of a pulse signal to the heater 11 and adheres to the recording medium 25 (Japanese Patent Laid-Open No. 59-20726).
In the invention disclosed in Japanese Patent Application Publication No. 5 (1994), each ink droplet is ejected and flies in a connected state. Another point is that each ink droplet 24 flies in the form of an elongated column (Japanese Patent Application Laid-Open No. 63-5305).
In the invention disclosed in Japanese Patent No. 2, each ink droplet flies in a spherical shape. In addition, the size of the elongated ink droplet 24 is three to ten times as long as the diameter.

Here, the condition for the ink droplet 24 to fly in such an elongated column shape is that the flying speed of the ink droplet 24 is high and the ink droplet 24 is hardly affected by disturbance (for example, the flow of surrounding air). That is. Therefore, the ink drop 24
Between the shape of the ink and the flight speed, and a plurality of ink droplets 2
4 are ink droplets 2 when one pixel 26 is formed.
The relationship between No. 4 and the amount of deviation from the target position on the recording medium 25 was examined, and is shown in Table 1.

[0033]

[Table 1]

The ink jet recording head 23 used here has a size of the ink discharge port 22 of 17 × 17 μm and a size of the heater 11 of 14 × 84 μm. The resistance value of the heater 11 is 75Ω. When measuring the shape of the ink column and the flying speed of the ink droplet, a vehicle having the following components (a transparent liquid obtained by removing a dye component from the ink) was used instead of the ink.

Glycerin 18.0% Ethyl alcohol 4.8% Water 77.2% On the other hand, inks having the following components were used for measuring the pixel position accuracy.

Glycerin 18.0% Ethyl alcohol 4.8% Water 75.0% C.I. I. Direct black 154 2.2% The recording medium 25 to which the ink droplets 24 are adhered is PPC paper 6200 manufactured by Ricoh Co., Ltd., and the frequency of the pulse signal input to the heater 11 is 20 kHz.
And

According to Table 1, I _L / I _D , that is, ink drop 2
When the ratio of the length dimension (I _L ) of the ink droplet 24 to the diameter dimension (I _D ) of the ink droplet 24 is 2.8 or less, the flying speed of the ink droplet 24 is low (not reaching 5.0 m / s), Recording object 2
The ink droplets 24 could not be attached to the target position on the image No. 5 (images deviated by one dot or more would deteriorate the image quality), indicating that this is not practical. That is, the flying ink droplet 2
It can be seen that Sample No. 4 must be ejected under the condition that it has an elongated column shape (I _L / I _D is 3 or more). The flying speed of the ink droplet 24 at that time is 5 to 10 m / s or more, and it is strong against disturbance, has good flight straightness, and can be accurately attached to a target position.

Next, FIG. 2 shows the shape of the ink droplet 24 in more detail. The ink droplet 24 shown in FIG. 3A has the most ideal shape, but as shown in FIG. 3B, the ink droplet 24 flies along with a mist-like very small ink droplet called a satellite 24a. As shown in FIGS. 3C and 3D, two ink droplets 24 (three in some cases)
In some cases, it may fly separately. These differences depend on the size of the ink discharge port 22, the physical properties (viscosity, surface tension) of the ink, the shape of the pulse signal, and the like. In any case, the pulse signal input to the heater 11 is one. Therefore, in this case, as shown in FIGS. 9C and 9D, even when one ink drop 24 which should be one ink drop separates and flies separately, one ink drop 24 corresponds to one pulse signal.
Treated as having been formed. It should be noted that even if the satellite 24a is separated or fly with the satellite 24a as described above, if the flight speed is 5 to 10 m / s or more as described above, the satellite 24a or the separated ink droplet 2
4 adheres to substantially the same position on the recording medium 25, so that the pixels 26 to be formed are close to a perfect circle, and there is no problem that image quality is deteriorated.

FIG. 3 shows one pixel 2 by changing the number of pulse signals continuously input to the heater 11.
6 shows a state in which the number of ink droplets 24 forming 6 changes, and the size of the pixel 26 formed by changing the number of ink droplets 24 changes. In FIG. 1A, one pulse signal is input to the heater 11 and one ink droplet 24 is ejected from the ink ejection port 22, and one ink droplet 24 adheres to the recording medium 25. Thus, the pixel 26 is formed. In FIG. 3B, three pulse signals are input, and three ink droplets 24 are ejected, so that one pixel 26 is formed by the three ink droplets 24. In FIG. 3C, five pulse signals are input, five ink droplets 24 are ejected, and five ink droplets 2 are discharged.
4, one pixel 26 is formed. In FIG. 4D, eight pulse signals are input and eight ink droplets 24 are ejected, and one pixel 26 is formed by the eight ink droplets 24. Note that ink droplet 2
As the number of 4 increases, the size of the pixel 26 formed increases.

Here, in the present invention, in order to obtain a large pixel 26, it is realized by increasing the number of pulse signals continuously input to the heater 11 and increasing the number of ink droplets 24 continuously discharged. However, if the number of pulse signals is increased, the time required to form one pixel 26 is inevitably increased. Therefore, the flying ink droplet 24 is
If the ink droplets 24 are connected to each other as disclosed in JP-A-59-207265, the flight trajectory of the ink droplets deteriorates and the reliability of the print deteriorates as described above. It is an important point to increase the recording speed to generate the ink droplets 24 as frequently as possible within a non-connected range.

Therefore, the present inventor manufactured the following ink jet recording head and examined its conditions in order to find out how much the frequency of forming the ink droplets 24 not connected to each other can be increased.

Ink ejection port size 17 × 17 μm Heater size 14 × 84 μm Heater resistance value 75 Ω Ink ejection port array density 32 lines / mm (about 800 dp
(equivalent to i) Number of ink ejection ports 256 This inkjet recording head 23 has a surface tension of 4
Using a vehicle with 9.3 dyn / cm and a viscosity of 1.39 cp, the driving voltage of the heater 11 is 6 V, the pulse width of the pulse signal is Pw = 4 μs, and the frequency of the pulse signal is 2
When the vehicle was discharged at 0 kHz, good discharge was continuously performed. The ejection speed at this time is 1 at a position 0.5 mm ahead of the ink ejection port 22.
It was 1.7 m / s.

FIG. 4 shows the state of the bubbles at this time observed from above the transparent flat plate-like member 16 (shown in FIGS. 24 to 28), and the change with time is shown in FIG. The signal and the appearance of bubbles are shown on a time axis.
According to this, when a drive signal is turned on and a pulse signal is input, it is slightly delayed (0.2 μs) from the input of the pulse signal.
(After) The generation of bubbles is started, and then the bubbles gradually expand. After the driving voltage is turned off (after 4 μs), the bubbles continue to expand, and the time when the bubble reaches the maximum value is after 4.9 μs. Was. Thereafter, the bubbles began to contract and completely disappeared 14.7 μs after the drive voltage was turned on.

Next, the frequency of the pulse signal is set to 10 kHz.
Similarly, the profile of bubble generation was examined with z, 30 kHz, and 40 kHz.
There is almost no difference in the time at the time of bubble disappearance (the time until the bubble becomes maximum is 4.8 to 5.1 μs, the time at which the bubble disappears is 14.7 to 15 μs), and the profile of bubble generation is pulse. It turns out that it does not depend on the frequency of the signal.

Then, when the frequency of the pulse signal was further increased and the limit of stable ejection of the ink droplets 24 was examined, it was found that the ejection was stable up to a frequency of 51 kHz. The ink droplet 24 at this time
Was 12.5 m / s. When the frequency was further increased to 55 kHz, the ink drop 2
After the ejection of No. 4, the ejection stopped.

In order to investigate the reason, when the frequency is 50 to 5
When the profile of bubble generation was carefully examined between 5 kHz, bubbles from generation to disappearance were performed in a pattern as shown in FIG. 4 up to a frequency of 51 kHz. In contrast, at a frequency of 52 kHz, the first few seconds
Was performed from the generation to the disappearance of the air bubbles in the pattern shown in FIG. 5, but the air bubbles that did not disappear afterwards covered the upper part of the heater 11, and the pattern of the generation, expansion, contraction, and disappearance of the air bubbles was not performed. Therefore, ink drop 2
The ejection of No. 4 also stopped.

Accordingly, the upper limit frequency of the pulse signal for stably repeating the pattern until the bubble is generated and disappears, in other words, the upper limit frequency of the pulse signal for stably ejecting the ink droplet 24. Is 51kHz
It turns out that.

Here, the frequency of the pulse signal is 51 kHz.
FIG. 5 shows the driving voltage and the state of bubbles at the same time along the time axis. In FIG. 5, "T" is the time from the input of the pulse signal to the maximum bubble (in this case, T = 4.
9 μs). From FIG. 5, it can be seen from FIG. 5 that in order to stably generate bubbles in the second and subsequent times in the ink jet recording head 23 used in this experiment, "4T (= 19.6 .mu.s ) ", The next pulse signal should be input. still,
A pulse signal having a frequency of 51 kHz has a period of one pulse signal of 1 / (51 × 1000) seconds, that is, 19.6 μm.
s.

From another viewpoint, the time from when the previous bubble disappears to when the next bubble starts to be generated is referred to as “Ti”.
It can be seen that if the value is set to be larger than the “T”, the bubble generation and the ejection of the ink droplet 24 can be performed almost stably and at the highest occurrence frequency.

The above results show that the size of the ink discharge ports 22 is 17 × 17 μm and the array density of the ink discharge ports 22 is 32
This is a result of examining a profile of bubble generation in an ink jet recording head having the number of ink ejection ports 2 / mm.
Table 2 shows the profiles of bubble generation in other ink jet recording heads having different sizes and arrangement densities of No. 2.
Each time shown in Table 2 is a time after the input of the pulse signal. The frequency of all the pulse signals was 5 kHz.

[0051]

[Table 2]

Next, the frequency of the pulse signal in these ink jet recording heads was gradually increased from 5 kHz, and the limit of bubble generation and, in other words, the discharge limit of the ink droplet 24 were examined. As a result, for an ink jet recording head of 48 lines / mm, the upper limit is about 75 kHz, and the flying speed of the ink droplet 24 at that time is 11.1 m / s.
Met. The upper limit of the ink jet recording head of 24 lines / mm was about 46 kHz, and the flying speed of the ink droplet 24 at that time was 10.7 m / s. And
In these inkjet recording heads, if the frequency of the pulse signal is further increased, the ejection of the ink droplets 24 stops, and the above-described inkjet recording head (the ink ejection port size is 17 × 17 μm, the array density is 32 lines /
As a result, the air bubbles covered the entire surface of the heater.

On the other hand, in the case of an ink jet recording head of 16 lines / mm, when the frequency of the pulse signal is increased to 9 to 9.5 kHz, the ejection of ink droplets is stopped. 6 ~
At the time when the frequency was increased to 7 kHz, the ejection of the ink droplet was stopped.
Therefore, observation of the heaters of these ink jet recording heads revealed that the heaters were broken.

That is, in all the ink jet recording heads, the ejection of the ink droplet is stopped at a certain point when the frequency of the pulse signal is increased, but the cause is different. In the case of an ink jet recording head having an arrangement density of ink ejection ports of 24 lines / mm and 48 lines / mm, similarly to the above-described ink jet recording head of 32 lines / mm, the cycle of bubble generation by the heater reaches the limit and ink droplets are discharged. While the ejection was stopped, in the ink jet recording head having the arrangement density of the ink ejection ports of 16 lines / mm and 8 lines / mm, the ejection of the ink droplet was stopped due to the breakage of the heater.

The cause is considered to depend on the size of the generated bubbles. Generally, it is known that when a bubble collapses and disappears, a very large impact force acts due to cavitation. The impact force acts more strongly on the heater at the time of its disappearance as the generated bubbles are larger. According to the above experimental results, the heater was broken when the frequency of the pulse signal was gradually increased in the ink jet recording head having the arrangement density of the ink discharge ports of 8 lines / mm and 16 lines / mm due to the impact force. It is considered something. In other words, although there was no abnormality when the frequency of the pulse signal was 5 kHz, since the frequency was gradually increased, the number of repetitions of the impact force due to cavitation gradually increased, and the heater could not withstand the impact force and was destroyed. It is thought that it was.

On the other hand, the arrangement density of the ink ejection ports is 24 lines /
It is considered that the reason why the heater of the ink jet recording head of 48 mm / mm was not broken was that the generated bubbles were very small, and therefore the impact force acting on the heater was also small.

In order to investigate this point in more detail, the present inventors input pulse signals in the air and in the vehicle to the heaters of various ink jet recording heads having different arrangement densities of the ink ejection ports, and changed the frequency thereof. The durability of those heaters was examined by changing. In the used inkjet recording head, the arrangement density of the ink ejection ports was 8 lines / mm, 16 lines / mm, 24 lines / mm, 32 lines / mm,
The drive voltage and the pulse width of the pulse signal were 48 lines / mm, and were the same as in the case of examining the profile of bubble generation described above. As a result, when driven in air, the pulse signal was driven for 3 hours with the frequency of the pulse signal being 100 kHz (the pulse signal was input at 10 ⁹ ), but no abnormality was observed in all the heaters of the ink jet recording head. On the other hand, when a similar test was performed in the vehicle,
The results as shown in Table 3 were obtained.

[0058]

[Table 3]

That is, the arrangement density of the ink ejection ports is 8
mm, 16 bubbles / mm, when the bubble generated by the heater is large, the heater is destroyed at the frequency of the pulse signal before reaching the upper limit of the bubble generation cycle. Array density of 2
When the heater generates small bubbles such as 4 lines / mm, 32 lines / mm, and 48 lines / mm, even if the heater is driven near the upper limit of the bubble generation cycle, the heater has a durability of 10 ⁹ or more. I found that there is. In addition, the size of the generated bubbles is 380 μm for a length of 8 bubbles / mm, 195 μm for a length of 16 bubbles / mm,
The one with 24 lines / mm was 115 μm, the one with 32 lines / mm was 90 μm, and the one with 48 lines / mm was 60 μm.

From the above results, in an ink jet recording head in which ink discharge ports are small to some extent and arranged at high density, the upper limit for discharging ink droplets at a high frequency is that the maximum number of bubbles after the pulse signal is input. Assuming that the time required to reach “T” is “T”, the time for inputting the next pulse signal should be “4T” or later after the input of the previous pulse signal. From another viewpoint, if the time from when the previous bubble disappears to when the next bubble starts to be generated is set to be longer than “T”, the ink droplet is almost stable and has the highest frequency of occurrence. It can be seen that the discharge can be performed.

Next, another feature of the present invention will be described. In the present invention, ink droplets are ejected with very little energy compared to the related art. Further, since the ink ejection port of the ink jet recording head used in the present invention is very small, it is conventionally used, for example, Japanese Patent Publication No. 59-43.
Discharge of ink droplets becomes considerably more difficult than when ink droplets are discharged from a large ink discharge port of 50 × 40 μm as disclosed in Japanese Patent No. 312. The first reason is that the ink discharge port becomes smaller and the fluid resistance becomes larger. However, it is also possible to discharge ink droplets stably by finding optimal conditions.

Therefore, the present inventor examined how much energy required for discharging ink droplets per unit area of the ink discharge port was required. It is described below. In the ink jet recording head used here, the arrangement density of the ink ejection ports was 24 lines / mm and 32 lines / mm, respectively.
mm, 48 nozzles / mm, and the size of each ink ejection port is 22 × 22 μm, 17 × 17 μm, 14 × 1
4 μm, and other dimensions and the components of the vehicle used in the experiment are the same as those in the previous experiment. As the contents of the experiment, the driving voltage was changed to change the energy required for discharging the ink droplet, and the flying speed Vi (m / s) of the discharged ink droplet was measured. Further, the frequency of the pulse signal input to the heater of each ink jet recording head was set to be about 10% lower than the use limit (upper limit) of each ink jet recording head. That is, the frequency was set to 40 kHz for a 24 lines / mm inkjet recording head, 45 kHz for a 32 lines / mm inkjet recording head, and 65 kHz for a 48 lines / mm inkjet recording head. Also, the pulse width of the pulse signal is fixed, and for each ink jet recording head,
4.5 μs, 4 μs, and 3 μs. Table 4 shows the results.

[0063]

[Table 4]

As a result, the ratio of the energy required for discharging the ink droplet to the area of the ink discharge port “E / S (J /
cm < ² >) "is less than 0.3, the ink droplet becomes spherical, its flying speed is slow, unstable and impractical. Was found to be destroyed and unusable.

From another viewpoint, a minute ink ejection port (14 × 14 μm to 22 × 2) which is not present in the prior art as in the present invention.
2 μm) to very high frequencies (at least 10 kHz)
Table 4 shows that in order to stably eject ink droplets when an ink droplet is ejected by the above pulse signal, the ink jet recording head having an ink ejection port array density of 24 nozzles / mm is used. 46μJ (at 5V drive voltage)
0.95 μJ (at a drive voltage of 4.1 V) to 8.74 μJ for an ink jet recording head having an ink ejection opening array density of 32 lines / mm (up to a drive voltage of 16 V).
(At a driving voltage of 12.8 V), the ink jet recording head having an ink ejection port array density of 48 lines / mm is 0.62 μm.
J (at a drive voltage of 3.8 V) to 5.97 μJ (drive voltage 1
1.8 V), and when these are combined, 0.6 μJ to 1
It is preferable to use in the range of about 5.0 μJ.

According to the present invention, the size of a pixel formed on a recording medium (for example, paper) is reduced by one very small ink droplet generated at a very high frequency of 10 to 75 kHz.
It is changed by attaching a plurality of them to substantially the same location. Image density information is input to an ink jet recording head in order to cause the one or more ink droplets to adhere to substantially the same location, and one to a plurality of pulse signals corresponding to the pixel density information are used. However, when multiple ink droplets are deposited on a recording medium, there is a limit to the range in which the pixel diameter can be changed. It does not mean that it only needs to be attached to the location.

In view of this point, the present inventor examined the relationship between the number of ink droplets to be generated and the size of the pixels formed on the recording medium. The ink jet recording head used here has an ink ejection port size of 17 × 17 μm, an ink ejection port array density of 32 lines / mm, and other dimensions are the same as those of the ink jet recording head used in the above-described experiment. The composition of the ink used was glycerin 18.0% ethyl alcohol 4.8% water 75.0% C.I. I. Direct black 154 2.2%. Further, the ejection conditions are as follows: the driving voltage is 6 V, the pulse width of the pulse signal is 4 μs, and the frequency of the pulse signal is 45.
kHz. Under these conditions, the number of pulse signals is 1, 2, 3,
.. Were input up to a maximum of 50, and the pixel diameter on the recording medium formed according to the number of pulse signals was measured.
The recording medium is PPC paper 620 manufactured by Ricoh Co., Ltd.
0 and Mitsubishi Matt Coated Paper NM. FIG. 6 shows the result. In the graph of FIG. 6, the horizontal axis represents the number of ink droplets (number of pulse signals) ejected to form one pixel, and the vertical axis represents the pixel diameter of the formed pixel.

As can be seen from the above, the pixel diameter can be increased as the number of ink droplets attached to substantially the same location on the recording medium is increased. However, when the number of ink droplets exceeds a certain value, the pixel diameter becomes larger. Makes little contribution to increasing. Here, the frequency of ink droplet generation, that is, the frequency of the pulse signal is set to 45 kHz. However, since one pixel is formed by a plurality of ink droplets,
The actual frequency of pixel formation depends on the number of ink droplets forming pixels, but is much slower than 45 kHz.

Here, assuming that n ink droplets are used to obtain the maximum pixel, the pixel formation frequency is 45 kHz.
z / n. This pixel formation frequency is the same whether one pixel is formed by one ink droplet or one pixel is formed by n ink droplets. One pixel is formed by n ink droplets. The case is the rule condition. FIG. 7 shows the relationship between the frequency of ink droplet generation and the frequency of pixel formation.

The example shown in FIG. 7 shows an example in which pixels of different sizes are formed by changing the number of ink droplets in the range of 1 to 22 pixels. Assuming that the frequency is 22 kHz, the frequency of forming pixels drops to 1 kHz. Since the frequency of pixel formation determines the speed at which one print is executed, it is better to be as fast as possible. Therefore, if the number of ink droplets for forming one pixel is increased more than necessary, the printing speed is undesirably reduced. From this point of view, FIG.
According to the result, when the number of ink droplets is less than 20, the pixel diameter changes relatively largely according to the number of ink droplets, but when the number falls within the range of 20 to 30, the pixel diameter changes. Slightly grinds. Further, when the number of ink droplets is 30 or more, even if the number of ink droplets is increased, the pixel diameter hardly changes, and it is understood that it is meaningless to attach more ink droplets to the same location on the recording medium.

In other words, in order to print one pixel by changing its diameter, it is desirable to print by changing the number of ink droplets in a range of at most 30 and preferably in a range of up to 20. It is better to change the number of ink droplets with
It is good to change the number of ink droplets in the range up to the number. As is clear from the graph of FIG. 6, the change rate of the pixel diameter is the best in the range where the number of ink droplets is up to ten, and 1
This is because the rate of change is slightly lower in the range of 0 to 20 pieces, and is further reduced in the range of 20 to 30 pieces, and hardly changes in the range of 30 pieces or more.

From another point of view, the present invention is characterized by a pulse signal of 10 kHz or more which cannot be realized by a conventional ink jet recording head having an ink ejection port array density of about 16 nozzles / mm. Demonstrate,
Since the upper limit is 75 kHz, the pixel formation frequency is 0.3 to 7.5 kHz.

Here, the result of actual recording will be described. In addition, the arrangement density of the ink ejection ports is 32 lines / m.
m (the number of ink ejection ports is 256) using four ink jet recording heads, each of which has yellow, magenta,
A4 size paper (mat coated paper NM made by Mitsubishi Paper Mills) was filled with inks of different cyan and black colors.
Various recording conditions are as follows. The frequency of the pulse signal was 45 kHz, and the number of ink droplets for forming one pixel according to image density information was in the range of 1 to 15.
Therefore, the frequency of pixel formation is 3 kHz. Further, the gradation expression not only changes the pixel diameter by the method of the present invention, but also combines a 4 × 4 matrix,
It was decided to change to 256 gradations. Therefore, the pixel density was 32 pixels / mm, but the pixel density was 8 pixels / mm. In order to print on A4 size paper under the above conditions, 34 scans (unidirectional printing) were performed, and the process was completed in less than about 2 minutes. The obtained image had image quality not inferior to silver halide photography.

Next, another feature of the present invention will be described. This feature is that the maximum number of ink droplets 24 that can be attached to the same location on the recording medium 25 is variable. That is, in addition to the original recording mode of the recording apparatus, a mode (draft mode) in which the maximum number of ink droplets 24 that can be attached to the same location on the recording medium 25 is changed. . While the original recording mode forms one pixel with one to ten ink droplets 24, the draft mode forms one pixel with one to five ink droplets 24. Thus, printing can be performed at twice the speed. Such a draft mode is very convenient when it is desired to quickly obtain an overall rough image in the case of printing out even if the highest image quality cannot be obtained.

Further, since the ink jet recording head performs non-impact and non-contact recording, in principle, any recording medium (for example, copy paper, recycled paper, O
(HP sheet, postcard, etc.).
However, the size of the pixel 26 formed on the recording medium 25 varies depending on the type of the recording medium 25,
Table 5 shows an example. In Table 5,
A, B, and C are recording media of different types.
One pixel 2 is formed by five drops, five drops, and ten drops 24 of ink.
6 shows the ink mass and the pixel diameter when No. 6 is formed. The measurement of the ink mass is actually obtained by collecting 6 × 10 ⁵ ink droplets 24 (collecting the ink droplets 24 by discharging the ink droplets 30 with a pulse signal of 20 kHz for 30 seconds) and measuring the weight. The pixel diameter is the pixel 26 on the recording medium 25.
Was measured with an optical microscope equipped with an XY stage,
The average value is shown for 30 pieces.

[0076]

[Table 5]

As is clear from Table 5, the pixel diameter of the pixel 26 formed between the recording medium A and the recording medium B is such that the recording medium B slightly expands, but the recording medium C does not. It can be seen that the recording mediums A and B spread much more. Then, when the same image sample was printed using the recording media A, B, and C under exactly the same conditions, the image on the recording media B was slightly darker than the image on the recording media A, The image on the body C was much darker than the images on the recording bodies A and B. The largest pixel 26 on each of the recording materials A, B, and C at that time is formed by ten ink droplets 24.

Next, the maximum pixel 2 on the recording medium A
When a similar print sample was obtained with the number of ink droplets 24 forming 6 being 11 drops, an image having the same density as the image on the recording medium B was obtained. Further, the recording medium A
A similar print sample was obtained with the number of ink droplets 24 forming the largest pixel 26 being 14 above, and an image having the same density as the image on the recording medium C was obtained. .

From the above results, even if the recording medium changes,
It can be seen that substantially the same image can be obtained by changing the maximum number of ink droplets 24 attached to the same location on the recording medium according to the type of the recording medium. It should be noted that the number of ink droplets 24 adhering to the same location does not change only when the largest pixel 26 is formed, but also changes when the pixel 26 has another size. Nor.

In an ink jet recording apparatus having a scanner as an image reading apparatus, a method of reading an original with a scanner and outputting the original faithfully with an ink jet recording unit is usually used. In some cases, printing is performed darkly, or a dark original is printed lightly. At this time, by changing the maximum number of the ink droplets 24 to be attached to the same location, an image having an arbitrary density can be easily obtained.

As described above, the method of adjusting the density of the image printed on the recording medium 25 by changing the maximum number of the ink droplets 24 adhered to the same portion on the recording medium 25 is as follows. The present invention is not limited to a thermal ink jet recording head of a type in which bubbles are generated by heating the heater 11, but is also applicable to a continuous flow type ink jet head in which ink droplets are ejected by vibrating a piezoelectric vibrator. It is possible.

Next, another feature of the present invention will be described. First, when gradation recording is performed by changing the pixel diameter by changing the number of ink droplets 24 attached to the same location on the recording medium 25 as in the present invention, the ink droplets 24 attached to the same location It is desirable that the relationship between the number and the image density increases linearly until the maximum density is reached as shown in FIG. However, when the relationship between the number of ink droplets 24 attached to the same location and the image density is measured, the result does not increase linearly but results as shown in FIG. The ink jet recording head used in this measurement has a size of the ink discharge port 22 of 17 × 17 μm and a size of the heater 11 of 14 × 84 μm. The resistance value of the heater 11 is 77Ω. The arrangement density of the ink discharge port 22 and the heater 11 is 800 dpi. The ink used had the following components.

Glycerin 18.0% Ethyl alcohol 4.8% Water 75.0% C.I. I. Direct Black 154 2.2% Further, as the recording medium 25 to which the ink droplet 24 is adhered, PPC paper 6200 manufactured by Ricoh Co., Ltd. was used.
The number of ink droplets 24 forming one pixel is 1, 2,
In order to be able to measure concentration in the case of 3, ..., ..., 20, 1
The entire surface was printed in an area of 0 × 10 mm, and the respective densities were measured and plotted.

According to the measurement results shown in FIG. 9, in the range where the image density is low, the image density increases substantially linearly with the increase of the ink droplets 24, but gradually approaches the saturation state as the image density increases. And the increase in the image density becomes gradual with the increase in the number of the ink droplets 24, and the required image density cannot be obtained unless the number of the ink droplets 24 adhered to the same portion on the recording medium 25 is increased significantly. I understand.

Therefore, in the present invention, as shown in FIG. 10, pixels having different sizes by changing the number of ink droplets 24 are designated as D ₁ , D ₂ , D ₃ ,..., D ₁₀ . sometimes,
The number of ink droplets 24 for forming these pixels is 1,
Instead of 2, 3, 4, 5, 6, 7, 8, 9, 10, for example, in the example of the present invention, 1, 2, 3, 4, 5,.
Set to 6, 8, 10, 12, 20 drops. As a result, the image density linearly increases for each pixel (D1 to D10) as shown in FIG. 10, and a desired image density can be easily obtained, and a smooth, high-quality gradation can be obtained. Recording becomes possible.

Next, another feature of the present invention will be described. This feature makes the center position of a pixel 26 formed by one or a plurality of ink droplets 24 substantially coincide with the center position of a region where one pixel is to be formed, and reduces the distance between the centers of adjacent pixels 26. The pulse signal groups are made substantially equal, and the intervals between the center positions of adjacent pulse signal groups for forming one pixel are made substantially equal. These features will be described in detail below.

First, each square frame shown in FIG. 11 shows five areas where one pixel is to be formed on the recording medium 25, and FIG. 12 shows a binary image in each area. This shows a state where recording pixels 26 are formed. In the case of such binary recording, the center of the pixel 26 easily matches the center of the region where the pixel is to be formed, and the center distance La of the region where the pixel is to be formed and the distance between the center of the adjacent pixel 26 Is substantially the same as the center distance Lb.

Next, FIG. 13 shows a conventional example in which one pixel is formed by one to a plurality of ink droplets 24.
Depending on the number of ink droplets 24 forming one pixel, the center position of the pixel 26 does not match the center position of the region where one pixel is to be formed, and furthermore, the center distance Lc ₁ between the adjacent pixels 26, Lc ₂ , Lc ₃ , Lc ₄ are separated,
Finally, there is a problem that the image quality is deteriorated. This is because printing is performed while the ink-jet recording head and the recording medium move relative to each other, and the number of ink droplets 24 forming one pixel changes within a range of one to a plurality of pixels to form one pixel. This is because the time is different. Also, the center position interval Ta between adjacent pulse signal groups for forming one pixel.
₁ , Ta ₂ , Ta ₃ , and Ta ₄ are also different. FIG. 13 shows that the number of the maximum ink droplets 24 forming one pixel is five.
In this case, the pulse signal indicated by the solid line is for discharging the ink droplet 24.

FIG. 14 shows the features of the present invention.
When the number of ink droplets 24 forming a pixel is small (when forming a small pixel), a pulse signal for discharging the ink droplet 24 is generated with a time delay. Specifically, when one pixel is formed by one ink droplet 24, a third pulse signal is generated from five pulse signals that can be generated, and one pixel is formed by two ink droplets 24. In this case, the second and third pulse signals are generated. By doing so, the center position of each pixel 26 substantially coincides with the center position of the region where one pixel is to be formed, and the center distances Ld ₁ , Ld ₁
d ₂ , Ld ₃ , and Ld ₄ substantially match, and the image quality is improved. Here, the expression “substantially coincide with” is used for the ink droplet 24.
1 depending on whether an even or odd number of pulse signals
This is because a position shift of a pulse (one ink drop) occurs. However, the positional shift for one pulse is almost negligible, and when two pixels 24 form one pixel, the third and fourth pulse signals may be generated.

In FIGS. 13 and 14, there is a gap between adjacent pixels 26, but FIG.
This is to avoid complicating the drawing. In actuality, in the case of a connected straight line or solid printing of the entire surface, adjacent pixels 26 overlap each other. In FIGS. 13 and 14, when one pixel 26 is formed by a plurality of ink droplets 24, the pixel 26 is shown to be horizontally long. It is a representation of each pixel 26
Has a substantially round shape.

On the other hand, regarding the pulse signal group for forming one pixel, the center position interval T
b ₁ , Tb ₂ , Tb ₃ , and Tb ₄ are substantially constant. Here, the expression “substantially constant” is used, as in the above-described case, in accordance with whether the pulse signal for generating the ink droplet 24 is an even number or an odd number.
This is because the position shift of (droplet) occurs, but the position shift of one pulse is a value that can be almost ignored.

Next, another feature of the present invention will be described with reference to FIGS. First, in a normal inkjet recording head that performs binary recording, when performing full-screen printing (solid printing), adjacent pixels partially overlap each other to eliminate a white background area where ink droplets do not adhere. I have to. For example, as shown in FIG. 15, when the pixel diameter of each pixel 26 is Dd and the distance between the centers of adjacent pixels 26 is Dp, the white background region is eliminated by setting Dd ≧ √2 · Dp. Specifically, in the case of a printing density of 400 dpi, D _P = 63.5 μ.
m, if Dd ≧ 90 μm, the white background area disappears and the entire surface is printed. In order to obtain such a pixel diameter, for example, the aforementioned Japanese Patent Publication No. Sho 59-4
As disclosed in Japanese Patent No. 3312, a so-called edge shooter type thermal ink jet recording head which discharges ink droplets in a horizontal direction with respect to a heater surface has some fluctuations depending on the material of ink and paper. Is set to approximately 28 × 28 μm.

On the other hand, the present invention relates to an ink jet recording head for performing gradation recording by multi-value recording in which the size of a pixel is changed.
i are formed in a line at a density of i.
It is formed in a size of × 16 μm. The heater 11 is formed in a size of 15 × 60 μm, and its resistance is set to 61.7Ω.

Then, using the ink jet recording head, the ink (glycerin 18
%, Ethyl alcohol 4.8%, water 75%, C.I.
I. When the ink droplets were ejected using Direct Black 154 (2.2%), the ejection of the ink droplets was stabilized with the frequency of the pulse signal input to the heater 11 being up to 53 kHz.

Therefore, as recording paper, Ricoh's P
All the pixels were printed by using the PC paper 6200 and discharging the ink droplets from all the ink discharge ports 22, and the pixel diameter of the formed pixel 26 was measured. Note that the frequency of the pixel signal is 8 kHz because the frequency of the pulse signal at this time is 48 kHz and the number of ink droplets for forming one pixel is changed in the range of 1 to 6. FIG.
(A) shows a state in which one pixel is formed by one ink droplet, and the pixel diameter is 32.1 μm. Similarly, FIG.
Indicates that one pixel is formed by two ink droplets and the pixel diameter is 6
FIG. 3 (c) shows a pixel diameter of 72.5 μm in a state where one pixel is formed by three ink droplets, and FIG. 4 (d) shows a pixel state in a state where one pixel is formed by four ink droplets. 80.9 diameter
(e), the pixel diameter is 88.8 μm when one pixel is formed by five ink droplets, and (f) is the pixel diameter when one pixel is formed by six ink droplets. 96.2 μm. The measurement of the pixel diameter when the adjacent pixels 26 come into contact with each other as shown in FIGS.
This was performed by printing only one pixel alone.

Here, in the case where one pixel is formed by one ink droplet, since the ink ejection port 22 is small and the heater 11 is accordingly small, each ink ejection port 2 is formed.
2 is small, the pixel diameter Dd of each pixel 26 becomes smaller than the square root times the distance Dp between the center points of adjacent pixels (that is, Dd <√2 · Dp), and the adjacent pixels 26 are adjacent to each other. Are separated from each other. Therefore,
Even if all pixels are printed, many white background areas remain, and the entire printing surface becomes pale gray. Then, as the number of ink droplets forming one pixel 26 increases, FIGS.
As shown in (d), the pixel diameter of each pixel 26 increases, the overlapping portion between adjacent pixels gradually increases, the white background region gradually decreases, and the entire printing surface gradually becomes black. Then, in FIG. 16E, the pixel diameter becomes equal to the square root times the distance between the center points of the pixels 26 (that is, D
d = √2 · Dp), the white background area disappears and the printing surface becomes completely black. In FIG. 16 (f), the pixel diameter is larger than the square root of the distance between the center points of the pixels 26, the overlapping portion between the pixels is further increased, and the entire printing surface becomes darker black.

Next, when all the pixels are printed by the above-described ordinary ink jet print head that performs the binary printing, the result becomes the same as that shown in FIG. 16E, and the white background area on the printing surface becomes Disappears. Then, when one pixel was formed alone and the pixel diameter was measured, it was about 95.5 μm
Met. Therefore, in order to perform gradation recording with this ink jet recording head, there is no other way than to perform printing by thinning out pixels, but gradation recording can be performed for a while.
Since the density of 0 dpi cannot be used effectively, the image has a very low resolution.

On the other hand, according to the present invention, when one pixel is formed by one ink droplet, the pixel diameter is very small.
Even if the image is printed at a density of 0 dpi, the adjacent pixels 26 do not overlap, and a sufficiently wide white background area exists between the adjacent pixels 26. Therefore, by changing the number of ink droplets forming one pixel so as to gradually fill the white background area and increasing the pixel diameter, finally eliminating the white background area, gradation recording can be performed. . Further, it is not necessary to thin out the pixels as in the case of performing the gradation recording by the ordinary inkjet recording head for performing the binary recording described above.
Since the printing is performed with the pixel density of dpi, the resolution does not decrease, and very high quality printing can be performed.

[0099]

According to the first aspect of the present invention, there is provided a liquid chamber for storing ink, a plurality of ink discharge ports connected to the liquid chamber via a liquid path, and energy for applying energy to the ink in the liquid path. A pulse signal is input to the energy acting section as required, and an ink droplet is ejected from the ink ejection port, flies, and adheres to the recording medium by the acting force of the energy acting section. In the liquid jet recording apparatus which performs recording by ink jetting, the ejection opening has an opening area of less than 500 μm ^2, and the ink droplet ejection frequency is 10 kHz or more per ejection opening, so that high resolution recording is possible. In addition, the effect of inertia is small because the ink amount of one drop is very small, the response as a liquid jet recording head is fast (the frequency of ink droplet ejection is large), and high-speed driving is possible. This has the effect that it becomes possible.

According to a second aspect of the present invention, in the liquid jet recording apparatus according to the first aspect, since the speed at which the ink droplet flies is set to 5.2 m / s or more, the pixel position accuracy on the recording medium is improved. Is maintained with high accuracy, and high-quality recording is enabled.

According to the third aspect of the present invention, since an image reading apparatus is provided in the liquid jet recording apparatus according to the first and second aspects to constitute a recording apparatus with a scanner, extremely fine recording (high-resolution recording) is possible. With the liquid jet recording apparatus described above, high-quality recording can be performed, and an apparatus such as an ink jet copier (copying machine) that outputs an ink jet according to a read image can be realized by combining an image reading apparatus.

According to a fourth aspect of the present invention, there is provided a liquid chamber for storing ink, a plurality of ink ejection ports connected to the liquid chamber via a liquid path, and an energy action section for applying energy to the ink in the liquid path. A pulse signal is input to the energy applying unit as needed, and the ink droplet is ejected from the ink ejection port and flies by the acting force of the energy applying unit, and is adhered to the recording medium to perform recording. The liquid ejection recording apparatus for performing the above is provided with a scanner which is an image reading apparatus, and the scanner information is set such that the frequency of the ink droplet ejection is set to 10 kHz or more per one ejection port, and the speed at which the ink droplet flies at a speed of 5 kHz. Conventionally, the recording speed of an ink-jet image was low, and it was difficult to realize a usage such as a copying machine. In addition, it is possible to realize high-quality recording by clarifying the flying conditions of stable ink droplets, and to realize an ink-jet copying machine that performs ink-jet output according to a read image by combining a scanner that is an image reading device. It has the effect of.

[Brief description of the drawings]

FIG. 1 is an explanatory diagram showing a flying state of an ink droplet in one embodiment of the present invention.

FIG. 2 is an explanatory diagram showing the shape of a flying ink droplet in detail.

FIG. 3 is an explanatory diagram showing a relationship between the number of pulse signals, the number of ink droplets to be ejected, and the size of a formed pixel.

FIG. 4 is an explanatory diagram showing input of a pulse signal and generation of bubbles.

FIG. 5 is an explanatory diagram showing a pulse signal continuously input and a state of bubble generation.

FIG. 6 is a graph showing the relationship between the number of ink droplets forming one pixel and the pixel diameter.

FIG. 7 is an explanatory diagram showing an ink droplet generation frequency, a pixel formation frequency, and a pixel size.

FIG. 8 is a graph showing an ideal relationship between the number of ink droplets adhering to the same location on a recording medium and the image density.

FIG. 9 is a graph showing the result of measuring the relationship between the number of ink droplets adhering to the same location on a recording medium and the image density.

FIG. 10 is a graph showing the relationship between each pixel and image density.

FIG. 11 is a plan view showing five areas where one pixel is to be formed on a recording medium.

FIG. 12 is a plan view showing a state where pixels for binary recording are formed in each area where one pixel is to be formed on the recording medium.

FIG. 13 is an explanatory diagram showing a positional relationship between an area where one pixel is to be formed and a pixel and a timing of generating a pulse signal in a conventional example in which one pixel is formed by one or a plurality of ink droplets.

FIG. 14 is an explanatory diagram showing a positional relationship between an area where one pixel is to be formed and a pixel and a timing of generating a pulse signal in the present invention in which one pixel is formed by one to a plurality of ink droplets.

FIG. 15 is a plan view showing pixels formed by printing all pixels of a normal inkjet recording head that performs binary recording.

FIG. 16 is a plan view showing the relationship between the number of ink droplets forming one pixel and the pixel diameter, and the relationship between the pixels and the white background area.

FIG. 17 is a side view showing a heating element substrate of one ink jet recording head.

FIG. 18 is a plan view showing a procedure for forming a heating element substrate.

FIG. 19 is a plan view showing a modification of the heating element substrate.

FIG. 20 is a perspective view showing a lid substrate.

FIG. 21 is a front view showing a heating element substrate of the ink jet recording head.

FIG. 22 is a front view showing a step of forming a groove for flowing ink on the heating element substrate.

FIG. 23 is a front view showing a state after the formation of the groove on the heating element substrate is completed.

FIG. 24 is a front view showing a lid substrate.

FIG. 25 is a front view showing a state in which the heating element substrate and the lid substrate are pressed and adhered.

FIG. 26 is a perspective view showing a state in which a heating element substrate and a lid substrate are pressed and adhered.

FIG. 27 is a sectional view taken along line BB in FIG. 26;

FIG. 28 is a vertical sectional side view showing the completed ink jet recording head.

[Explanation of symbols]

 Reference Signs List 4 heater 11 heater 18 liquid path 19 liquid chamber 22 ink discharge port 23 ink jet recording head 24 ink droplet 25 recording medium 26 pixel

Claims (4)

[Claims] A liquid chamber for storing ink, a plurality of ink ejection ports connected to the liquid chamber via a liquid path, and an energy action section for applying energy to the ink in the liquid path; A pulse signal is input to the energy action unit in accordance with
In a liquid jet recording apparatus in which ink droplets are ejected from the ink ejection port, fly, and adhere to a recording medium to perform recording, the ejection port has an opening area of less than 500 μm ^2, and the ink droplet ejection frequency is The liquid jet recording apparatus is characterized in that the frequency is set to 10 kHz or more per discharge port. 2. The flying speed of the ink droplet is 5.2 m.
2. The liquid jet recording apparatus according to claim 1, wherein the speed is not less than / s. 3. A recording apparatus with a scanner, wherein the liquid ejection recording apparatus according to claim 1 is provided with an image reading device. 4. A liquid chamber for storing ink, a plurality of ink ejection ports connected to the liquid chamber via a liquid path, and an energy action section for applying energy to ink in the liquid path. A pulse signal is input to the energy action unit in accordance with
A liquid ejecting recording apparatus that ejects ink droplets from the ink ejection ports, flies, and adheres to a recording medium to perform recording is provided with a scanner, which is an image reading device, and the scanner information indicates the ink droplet ejection frequency. A liquid jet recording apparatus equipped with a scanner, wherein the ejection speed of the ink droplet is set to 5.2 m / s or more, while the ejection speed is set to 10 kHz or more per one ejection port.