TWI695061B - Phosphors and light-emitting device including the same - Google Patents
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本發明係關於一種螢光材料包含螢光材料之發光裝置,特別係關於一種鎂鋁氮化合物螢光材料及其於發光裝置之應用。The present invention relates to a light-emitting device in which fluorescent materials include fluorescent materials, and particularly to a magnesium-aluminum-nitrogen compound fluorescent material and its application in a light-emitting device.
十九世紀,愛迪生發明了電燈進而改變人類歷史,從此照明設備之發展日新月異。近年來,發光二極體(LED)更是蓬勃發展,而此種固態元件隨著技術改良,已能作為光源使用。發光二極體不但能夠高效率地將電能轉為光能,同時具備省電、環保(無汞)、體積小、演色性佳等優點。在環保意識抬頭、發展再生能源與促進節約能源等趨勢下,傳統白熾燈泡、鹵素燈等照明設備已漸為白光發光二極體所取代。In the nineteenth century, Edison invented the electric lamp and changed the history of mankind. Since then, the development of lighting equipment has changed rapidly. In recent years, light-emitting diodes (LEDs) have developed vigorously, and such solid-state devices have been used as light sources with the improvement of technology. The light-emitting diode can not only efficiently convert electrical energy into light energy, but also has the advantages of power saving, environmental protection (mercury-free), small size, and good color rendering. Under the trend of rising environmental awareness, developing renewable energy and promoting energy saving, traditional incandescent bulbs, halogen lamps and other lighting equipment have been gradually replaced by white light-emitting diodes.
白光發光二極體的原理之一為透過一發光二極體晶片為光源,例如紫外光晶片或藍光晶片,激發螢光材料,使螢光材料放出其他波長的可見光(如綠光、紅光等),藉此混出不同色溫及演色性之白光。One of the principles of white light-emitting diodes is to use a light-emitting diode chip as a light source, such as an ultraviolet chip or a blue light chip, to excite the fluorescent material, so that the fluorescent material emits visible light of other wavelengths (such as green light, red light, etc.) ), thereby mixing out white light with different color temperatures and color rendering.
目前較常被使用的方式為使用藍光發光二極體晶片發出之藍光激發黃色螢光粉以轉換成黃光,未經轉換之藍光與經轉換之黃光混合以形成白光,但其演色性不佳。因此,時至今日,螢光粉開發仍為發光二極體發展之重要課題。At present, the most commonly used method is to use the blue light emitted by the blue light-emitting diode chip to excite the yellow phosphor to convert to yellow light, and the unconverted blue light is mixed with the converted yellow light to form white light, but its color rendering is not good. Therefore, to this day, the development of phosphors is still an important issue in the development of light-emitting diodes.
本發明之一目的在於提供一種螢光材料,其具有以下通式1: A1-x [Mg2 Al2 N4 ]:Cex 3+ [1] 其中,A為Ca、Sr或Ba,Ce3+ 為活化劑,以及0 < x ≤ 0.08。One object of the present invention is to provide a fluorescent material having the following general formula 1: A 1-x [Mg 2 Al 2 N 4 ]: Ce x 3+ [1] where A is Ca, Sr or Ba, Ce 3+ is the activator, and 0 <x ≤ 0.08.
於本發明之部分實施態樣中,該螢光材料係可被一波峰在400 nm至540 nm波長範圍之激發光所激發,以放射一放射光。In some embodiments of the present invention, the fluorescent material may be excited by excitation light having a peak in the wavelength range of 400 nm to 540 nm to emit a radiated light.
於本發明之部分實施態樣中,0.005 < x ≤ 0.08,且該螢光材料可被一波峰在490 nm至540 nm波長範圍之激發光所激發後,放射一最大放射強度在570 nm至585 nm波長範圍的放射光。In some embodiments of the present invention, 0.005 <x ≤ 0.08, and the fluorescent material can be excited by excitation light with a peak in the wavelength range of 490 nm to 540 nm, and emit a maximum emission intensity of 570 nm to 585 Radiated light in the nm wavelength range.
於本發明之部分實施態樣中,0.01 < x ≤ 0.08,且該螢光材料可被一波峰在450 nm至540 nm波長範圍之激發光所激發後,放射一最大放射強度在570 nm至585 nm範圍的放射光。In some embodiments of the present invention, 0.01 <x ≤ 0.08, and the fluorescent material can be excited by excitation light with a peak in the wavelength range of 450 nm to 540 nm, and emit a maximum emission intensity of 570 nm to 585 Emitted light in the nm range.
於本發明之部分實施態樣中,0 < x ≤ 0.01,且該螢光材料可被一波峰在450 nm至470 nm波長範圍之激發光所激發後,放射一最大放射強度在610 nm至625 nm波長範圍的放射光,以及可被一波峰在510 nm至540 nm波長範圍之激發光所激發後,放射一最大放射強度在570 nm至585 nm波長範圍的放射光。In some embodiments of the present invention, 0 <x ≤ 0.01, and the fluorescent material can be excited by excitation light with a peak in the wavelength range of 450 nm to 470 nm, and emit a maximum emission intensity of 610 nm to 625 The emitted light in the wavelength range of nm, and can be excited by the excitation light with a peak in the wavelength range of 510 nm to 540 nm, emits a emitted light with the maximum emission intensity in the wavelength range of 570 nm to 585 nm.
於本發明之部分實施態樣中,該螢光材料可被一波峰在500 nm至520 nm波長範圍之激發光激發時,其放射光譜包含一鞍部結構。In some embodiments of the present invention, when the fluorescent material can be excited by excitation light with a peak in the wavelength range of 500 nm to 520 nm, its emission spectrum includes a saddle structure.
於本發明之部分實施態樣中,通式1中之A為鍶(Sr)。In some embodiments of the present invention, A in Formula 1 is strontium (Sr).
本發明之另一目的在於提供一種發光裝置,包含波峰在400 nm至540 nm波長範圍之第一激發光源,以及如上所述之螢光材料。Another object of the present invention is to provide a light-emitting device including a first excitation light source with a peak in the wavelength range of 400 nm to 540 nm, and the fluorescent material as described above.
於本發明之部分實施態樣中,該第一激發光源係可發出波峰在490 nm至540 nm波長範圍之光或波峰在450 nm至470 nm波長範圍之光。In some embodiments of the present invention, the first excitation light source can emit light with a peak in the wavelength range of 490 nm to 540 nm or light with a peak in the wavelength range of 450 nm to 470 nm.
於本發明之部分實施態樣中,發光裝置更包含一第二激發光源,其中該第一激發光源係可發出波峰在450 nm至470 nm波長範圍之光,該第二激發光源係可發出波峰在490 nm至540 nm波長範圍之光,且於通式1中,0 < x ≤ 0.01。In some embodiments of the present invention, the light-emitting device further includes a second excitation light source, wherein the first excitation light source can emit light with a peak in the wavelength range of 450 nm to 470 nm, and the second excitation light source can emit a peak Light in the wavelength range of 490 nm to 540 nm, and in
為使本發明之上述目的、技術特徵及優點能更明顯易懂,下文係以部分具體實施態樣進行詳細說明。In order to make the above objects, technical features and advantages of the present invention more obvious and understandable, the following is a detailed description with some specific implementations.
以下將具體地描述根據本發明之部分具體實施態樣;惟,在不背離本發明之精神下,本發明尚可以多種不同形式之態樣來實踐,不應將本發明保護範圍解釋為限於說明書所陳述者。此外,除非文中有另外說明,於本說明書中(尤其是在後述專利申請範圍中)所使用之「一」、「該」及類似用語應理解為包含單數及複數形式。The following will specifically describe some specific implementations according to the present invention; however, without departing from the spirit of the present invention, the present invention can be practiced in many different forms, and the scope of protection of the present invention should not be interpreted as being limited to the specification The stated. In addition, unless otherwise stated in the text, "a", "the" and similar terms used in this specification (especially in the scope of patent applications described below) should be understood to include both singular and plural forms.
本發明為一種以鈰(Ce)為活化劑之鎂鋁氮化合物系螢光材料。本發明之螢光材料可以波峰在400 nm至540 nm波長範圍之激發光作為激發光源,且可透過活化劑鈰之濃度與激發光之波長的變化,而得到不同的放射光波段,可應用範圍廣,且可提供具有鞍部的寬放射光譜,有助於提升所應用之發光裝置的演色性,詳細說明如后。The invention is a magnesium aluminum nitrogen compound fluorescent material using cerium (Ce) as an activator. The fluorescent material of the present invention can use excitation light with a peak in the wavelength range of 400 nm to 540 nm as the excitation light source, and can pass through the change of the concentration of the activator cerium and the wavelength of the excitation light to obtain different emission light bands, and the applicable range It is wide and can provide a wide emission spectrum with a saddle, which helps to improve the color rendering of the applied light-emitting device, as detailed below.
特定言之,本發明提供一種具有以下通式1之螢光材料: A1-x [Mg2 Al2 N4 ]:Cex 3+ [1]In particular, the present invention provides a fluorescent material having the following general formula 1: A 1-x [Mg 2 Al 2 N 4 ]: Ce x 3+ [1]
通式1中之A可為Ca、Sr或Ba,於後附實施例之具體實施態樣中係採用Sr。於本發明之螢光材料中,Ce3+ 為螢光材料之活化劑,其含量(即『x』之值)不為0;一般而言,以A與Ce3+ 之總莫耳數計,活化劑Ce3+ 之含量比例係不超過8%,亦即0 < x ≤ 0.08。於後附實施例之具體實施態樣中,係控制x在大於0.005至不超過0.08的範圍(0.005 < x ≤ 0.08)。A in Formula 1 may be Ca, Sr or Ba, and Sr is used in the specific implementation of the following examples. In the fluorescent material of the present invention, Ce 3+ is an activator of the fluorescent material, and its content (that is, the value of "x") is not 0; generally speaking, it is calculated as the total moles of A and Ce 3+ , The content ratio of the activator Ce 3+ is not more than 8%, that is, 0 <x ≤ 0.08. In the specific implementation of the following embodiment, x is controlled to be in the range of greater than 0.005 to not more than 0.08 (0.005 <x ≤ 0.08).
本發明之螢光材料可採用波峰在400 nm至540 nm波長範圍之光作為激發光,且可透過變化激發光之波長來獲得不同的放光波段,尤其可獲得包含一鞍部結構的放射光譜,構成鞍部結構之二波峰的波長可相差超過30 nm,於發光裝置之應用上可有助於演色性之提升。The fluorescent material of the present invention can use light with a peak in the wavelength range of 400 nm to 540 nm as the excitation light, and can obtain different emission bands by changing the wavelength of the excitation light, in particular, an emission spectrum including a saddle structure can be obtained. The wavelengths of the two peaks that constitute the saddle structure can differ by more than 30 nm, which can contribute to the improvement of color rendering in the application of light-emitting devices.
具體而言,於本發明通式1之螢光材料中,在0 < x ≤ 0.08之情況下,例如0.005 < x ≤ 0.08之情況下,螢光材料可受波峰在490 nm至540 nm波長範圍之激發光,所激發,在一實施例中,激發光為綠光,產生一具有鞍部之放射光譜,其中最大放射強度之波峰在570 nm至585 nm波長範圍,次高放射強度之波峰在610 nm至625 nm波長範圍,在一實施例中,放射光為黃光、及/或橘光。若x大於0.01,即0.01 < x ≤ 0.08的情況,則在波峰在450 nm至540 nm波長範圍之激發光的激發下,在一實施例中,激發光為藍光,皆會獲致如上之最大放射強度在570 nm至585 nm範圍且次高放射強度在610 nm至625 nm範圍的具有鞍部的放射光譜,在一實施例中,放射光包含黃光、橘光、及/或橘紅光。若x小於或等於0.01,即0 < x ≤ 0.01的情況,則僅在波峰在510 nm至540 nm波長範圍之激發光的激發下,在一實施例中,激發光為綠光,將獲致如上具鞍部的放射光譜;在波峰在450 nm至470 nm波長範圍之激發光激發下,在一實施例中,激發光為藍光,將獲致一最大放射強度在610 nm至625 nm波長範圍的放射光譜,在一實施例中,放射光為橘光、及/或橘紅光。Specifically, in the fluorescent material of the general formula 1 of the present invention, in the case of 0 <x ≤ 0.08, for example, 0.005 <x ≤ 0.08, the fluorescent material can be subjected to a peak in the wavelength range of 490 nm to 540 nm The excitation light is excited, in one embodiment, the excitation light is green light, which produces an emission spectrum with a saddle, wherein the peak of the maximum emission intensity is in the wavelength range of 570 nm to 585 nm, and the peak of the next highest emission intensity is 610 In the wavelength range from nm to 625 nm, in one embodiment, the emitted light is yellow light and/or orange light. If x is greater than 0.01, that is, 0.01 <x ≤ 0.08, under the excitation of excitation light with a peak in the wavelength range of 450 nm to 540 nm, in one embodiment, the excitation light is blue light, all of which will cause the maximum emission as above An emission spectrum with a saddle having an intensity in the range of 570 nm to 585 nm and a sub-highest emission intensity in the range of 610 nm to 625 nm, in one embodiment, the emitted light includes yellow light, orange light, and/or orange light. If x is less than or equal to 0.01, that is, 0 <x ≤ 0.01, then only under the excitation of excitation light with a peak in the wavelength range of 510 nm to 540 nm, in one embodiment, the excitation light is green light, which will be obtained as above Emission spectrum with a saddle; under excitation of excitation light with a peak in the wavelength range of 450 nm to 470 nm, in one embodiment, the excitation light is blue light, resulting in an emission spectrum with a maximum emission intensity in the wavelength range of 610 nm to 625 nm In one embodiment, the emitted light is orange light and/or orange-red light.
以波峰在510 nm之綠光或波峰在460 nm之藍光作為激發光為例,本發明通式1之螢光材料在不同Ce含量之情況下的放射光表現如下表1所示:Taking the green light with the peak at 510 nm or the blue light with the peak at 460 nm as the excitation light, the radiation performance of the fluorescent material of Formula 1 of the present invention under different Ce contents is shown in Table 1 below:
表1
本發明螢光材料因具備上述特殊的放射光之性能,故在應用於發光裝置上將更具彈性。例如,在0 < x ≤ 0.01的情況中,可透過調整激發光為綠光或藍光,而產生最大放射強度位於不同波長的光,而因應不同的放光需求,使可應用範圍更為廣泛;以及可透過如表1所示之活化劑濃度(x)調整與激發光安排,提供具有具鞍部的放射光譜,此一具有寬的放光波長的放射光譜對於演色性的提升具有明顯助益。以上特殊放射光性能,將於後附實施例中清楚呈現。Since the fluorescent material of the present invention has the above-mentioned special properties of radiated light, it will be more flexible when applied to a light-emitting device. For example, in the case of 0 <x ≤ 0.01, by adjusting the excitation light to green light or blue light, the light with the maximum emission intensity at different wavelengths can be generated, and the application range is wider due to different light emission requirements; And through the activator concentration (x) adjustment and excitation light arrangement as shown in Table 1, an emission spectrum with a saddle portion can be provided. This emission spectrum with a wide emission wavelength has a significant benefit for the improvement of color rendering. The above special radiation performance will be clearly presented in the following examples.
本發明另提供一種應用發光裝置,其包含本發明通式1之螢光材料以及一第一激發光源,第一激發光源之激發光的波峰在400 nm至540 nm波長範圍,俾激發該螢光材料。在一實施態樣中,激發光源為一藍光發光元件,例如:藍光發光二極體晶片(Blue LED chip)。藍光發光元件可發出波峰在440 nm至480 nm之波長範圍之激發光。此外,藍光發光元件也可為藍光雷射。在另一實施態樣中,激發光源為綠光發光元件,其中,綠光發光元件可發出波峰在490 nm至540 nm之波長範圍之激發光。The present invention also provides a light-emitting device which includes the fluorescent material of Formula 1 of the present invention and a first excitation light source. The peak of the excitation light of the first excitation light source is in the wavelength range of 400 nm to 540 nm to excite the fluorescent light material. In one embodiment, the excitation light source is a blue light-emitting device, such as a blue LED chip. The blue light emitting element can emit excitation light with a peak in the wavelength range of 440 nm to 480 nm. In addition, the blue light emitting element may also be a blue laser. In another embodiment, the excitation light source is a green light-emitting element, wherein the green light-emitting element can emit excitation light with a peak in the wavelength range of 490 nm to 540 nm.
另外,鑒於螢光材料放光性能之多樣性,本發明發光裝置亦不排除採用多種激發光源的情況。例如,發光裝置可包含波長範圍不同之第一激發光源及第二激發光源,第一激發光源可發出波峰在450 nm至470 nm波長範圍之光,該第二激發光源可發出波峰在490 nm至540 nm波長範圍之光,在此配置下,當螢光材料滿足0.010 < x ≤ 0.01之條件,將可分別受第一激發光及第二激發光所激發,放出不同的放射光譜,提供應用上的多樣性。在一實施態樣中,激發光源為藍光發光元件,並配合其他可發出綠色波段的螢光粉,例如(Ba,Sr,Ca)2 SiO4 :Eu2+ 。在另一實施態樣中,激發光源包含第一激發光源為藍光發光元件以及第二激發光源為綠光發光元件。In addition, in view of the diversity of the light emitting performance of the fluorescent material, the light-emitting device of the present invention does not exclude the case of using multiple excitation light sources. For example, the light-emitting device may include a first excitation light source and a second excitation light source with different wavelength ranges. The first excitation light source may emit light with a peak in the wavelength range of 450 nm to 470 nm, and the second excitation light source may emit light with a peak in the range of 490 nm to In the 540 nm wavelength range, under this configuration, when the fluorescent material satisfies the condition of 0.010 <x ≤ 0.01, it will be excited by the first excitation light and the second excitation light respectively, emitting different emission spectra, providing applications. Diversity. In one embodiment, the excitation light source is a blue light-emitting element, and cooperates with other phosphors that can emit green wavelength bands, such as (Ba, Sr, Ca) 2 SiO 4 : Eu 2+ . In another embodiment, the excitation light source includes a first excitation light source as a blue light emitting element and a second excitation light source as a green light emitting element.
本發明另提供一種製造本發明之通式1螢光材料之製造方法,所述之製造方法係採用固態燒結法製備,其具有步驟簡易且可大量生產之優點。以製備鎂鋁氮化合物螢光材料(Sr1-x [Mg2 Al2 N4 ]:Cex 3+ )之方法為例,係先將反應物Sr3 N2 、Mg3 N2 、AlN與CeN分別秤重後,放進研缽中研磨使其均勻混合,而後於惰性氣氛(如氮氣氣氛)下進行高溫燒結,即可得到產物。燒結條件例如是1550o C的溫度及0.9帕(Pa)的壓力。The present invention also provides a manufacturing method for manufacturing the fluorescent material of Formula 1 of the present invention. The manufacturing method is prepared by a solid-state sintering method, which has the advantages of simple steps and mass production. Taking the method of preparing magnesium aluminum nitride compound fluorescent material (Sr 1-x [Mg 2 Al 2 N 4 ]: Ce x 3+ ) as an example, the reactants Sr 3 N 2 , Mg 3 N 2 , AlN and After the CeN is weighed separately, it is put into a mortar and grinded to be uniformly mixed, and then sintered at a high temperature under an inert atmosphere (such as a nitrogen atmosphere) to obtain the product. The sintering conditions are, for example, a temperature of 1550 o C and a pressure of 0.9 Pa.
茲以下列實施例進一步例示說明本發明。其中該等實施例僅提供作為說明,而非用以限制本發明之保護範圍。本發明保護範圍係如後附申請專利範圍所示。The following examples further illustrate the invention. These embodiments are only provided as illustrations, rather than to limit the protection scope of the present invention. The protection scope of the present invention is as shown in the appended patent application scope.
實施例Examples
1.1. 螢光材料Fluorescent material 11 至to 77 之製備Preparation
於手套箱內,將Sr3 N2 、Mg3 N2 、AlN與CeN以表2所示重量比例(重量%)分別秤重後,全部放進研缽中研磨二十分鐘,再於0.9帕之氮氣下進行高溫燒結,燒結溫度為1550o C,燒結時間四小時(4h),得到螢光材料1至7:Sr1-x [Mg2 Al2 N4 ]:Cex 3+ ,x分別為0.005、0.01、0.015、0.02、0.04、0.06、及0.08。In the glove box, weigh Sr 3 N 2 , Mg 3 N 2 , AlN and CeN at the weight ratios (weight %) shown in Table 2 and put them in a mortar and grind for 20 minutes, then at 0.9 Pa High-temperature sintering under nitrogen, sintering temperature 1550 o C, sintering time four hours (4h), to obtain fluorescent materials 1 to 7: Sr 1-x [Mg 2 Al 2 N 4 ]: Ce x 3+ , x respectively It is 0.005, 0.01, 0.015, 0.02, 0.04, 0.06, and 0.08.
表2
2.2. 螢光材料之晶相測試Crystal phase test of fluorescent materials
以X光粉末繞射儀(Bruker公司;型號:D2 phaser)分析螢光材料1至7之晶相純度,結果顯示於第1圖。如圖所示,所製得之螢光材料的晶相均為純相,並無雜相生成,純度良好。The crystal phase purity of fluorescent materials 1 to 7 was analyzed with an X-ray powder diffractometer (Bruker; model: D2 phaser). The results are shown in Figure 1. As shown in the figure, the crystal phases of the prepared fluorescent materials are all pure phases, no impurity phases are generated, and the purity is good.
3.3. 螢光材料之激發光譜Excitation spectrum of fluorescent materials
以分光光度計(spectrophotometer)(Horiba公司;型號: FluoroMax-3)分析螢光材料1至7之激發光譜,其中放射光的波峰分別設定為580 nm及620 nm,結果分別顯示於第2a圖及第2b圖。The excitation spectra of fluorescent materials 1 to 7 were analyzed with a spectrophotometer (Horiba; model: FluoroMax-3), where the peaks of the emitted light were set to 580 nm and 620 nm, respectively, and the results are shown in Figure 2a and Figure 2b.
如圖所示,不論放射光的波峰設定於580 nm(第2a圖)或620 nm(第2b圖),螢光材料1至7皆可受波峰於400 nm至550 nm波長範圍之光所激發。As shown in the figure, regardless of whether the peak of the emitted light is set at 580 nm (Figure 2a) or 620 nm (Figure 2b), the fluorescent materials 1 to 7 can be excited by light with a peak in the wavelength range of 400 nm to 550 nm .
4. Ce4. Ce 含量比例對放射光譜的影響Effect of content ratio on emission spectrum
利用分光光度計(spectrophotometer)(Horiba公司;型號: FluoroMax-3)分別以波峰在510 nm波長之綠光及波峰在460 nm波長之藍光激發螢光材料1至7,以分析活化劑(Ce)之含量比例(x值大小)對螢光材料之放射光譜的影響,放射光譜之測試結果分別顯示於第3a圖及第3b圖,對應之色座標圖譜(顯示放射光位置的改變)則分別顯示於第4a圖及第4b圖。Using a spectrophotometer (Horiba; model: FluoroMax-3) to excite fluorescent materials 1 to 7 with green light with a peak at 510 nm and blue light with a peak at 460 nm, respectively, to analyze the activator (Ce) The influence of the content ratio (x value) on the emission spectrum of fluorescent materials. The test results of the emission spectrum are shown in Figure 3a and Figure 3b, respectively, and the corresponding color coordinate spectrum (showing the change in the position of the emitted light) is displayed separately. In Figure 4a and Figure 4b.
具體來說,如圖所示,當以波峰在510 nm波長之綠光激發螢光材料時(第3a圖;對應之色座標圖譜為第4a圖),不論Ce含量比例如何,螢光材料1至7皆產生一具有鞍部的放射光譜,且最大放射強度大約在570 nm至585 nm的波長範圍,次高放射強度大約在610 nm至625 nm的波長範圍。當以波峰在460 nm波長之藍光激發螢光材料時(第3b圖;對應之色座標圖譜為第4b圖),在Ce含量比例不高於0.01(螢光材料1及2,x分別為0.005及0.01),螢光材料產生一最大放射強度大約在610 nm至625 nm波長範圍的放射光譜;當Ce含量比例高於0.01(螢光材料3至7,x分別為0.015、0.02、0.04、0.06及0.08),螢光材料產生具有鞍部的放射光譜,且最大放射強度大約在570 nm至585 nm波長範圍,次高放射強度之大約在610 nm至625 nm波長範圍。上述結果顯示,本發明螢光材料可提供多樣性的放光選擇,可增加應用廣度,並且可提供具有寬放射光波長範圍而成鞍部的放射光譜,此有助於提升所應用之發光裝置的演色性。Specifically, as shown in the figure, when the fluorescent material is excited with green light with a peak at 510 nm (Figure 3a; the corresponding color coordinate spectrum is Figure 4a), regardless of the Ce content ratio, the fluorescent material 1 All of them produce an emission spectrum with a saddle, and the maximum emission intensity is in the wavelength range of about 570 nm to 585 nm, and the next highest emission intensity is in the wavelength range of about 610 nm to 625 nm. When the fluorescent material is excited with blue light with a peak at 460 nm (Figure 3b; the corresponding color coordinate spectrum is Figure 4b), the proportion of Ce content is not higher than 0.01 (fluorescent materials 1 and 2, x are 0.005 respectively) And 0.01), the fluorescent material produces an emission spectrum with a maximum emission intensity in the wavelength range of approximately 610 nm to 625 nm; when the Ce content ratio is higher than 0.01 (
5.5. 激發光波長對放射光譜的影響Effect of excitation light wavelength on emission spectrum
利用分光光度計(spectrophotometer)(Horiba公司;型號: FluoroMax-3)測試螢光材料1及2之放射光譜,其中將激發光之波峰波長從460 nm逐漸變換至510 nm(以10 nm為間隔),以測試激發光波長對於放射光譜的影響,結果分別顯示於第5a圖及第5b圖。Use spectrophotometer (Horiba; model: FluoroMax-3) to test the emission spectrum of fluorescent materials 1 and 2, in which the peak wavelength of the excitation light is gradually changed from 460 nm to 510 nm (at intervals of 10 nm) In order to test the effect of excitation light wavelength on the emission spectrum, the results are shown in Figure 5a and Figure 5b, respectively.
第5a圖係螢光材料1(x = 0.005)之放射光譜隨激發光之波峰波長變化之測試結果,第5b則係螢光材料2(x = 0.01)之放射光譜隨激發光之波峰波長變化之測試結果。如圖所示,在波峰波長為460 nm之激發光所激發下,螢光材料1及2之放射光的波峰波長位置主要落在610 nm至625 nm之波長範圍,隨著激發波長往較長波長區段移動,放射光譜逐漸產生一鞍部,最大放射強度轉移至大約570 nm至585 nm波長範圍,次高放射強度大約在610 nm至625 nm波長範圍。此一結果再次驗證本發明螢光材料之放光多樣性。Figure 5a is the test result of the change of the emission spectrum of the fluorescent material 1 (x = 0.005) with the peak wavelength of the excitation light, and Figure 5b is the change of the emission spectrum of the fluorescent material 2 (x = 0.01) with the peak wavelength of the excitation light Test results. As shown in the figure, under the excitation of excitation light with a peak wavelength of 460 nm, the peak wavelength position of the radiated light of the fluorescent materials 1 and 2 mainly falls in the wavelength range of 610 nm to 625 nm, and the excitation wavelength becomes longer As the wavelength band moves, the emission spectrum gradually produces a saddle, the maximum emission intensity shifts to a wavelength range of about 570 nm to 585 nm, and the next highest emission intensity is about 610 nm to 625 nm. This result verifies the light emitting diversity of the fluorescent material of the present invention again.
上述實施例僅為例示性說明本發明之原理及其功效,並闡述本發明之技術特徵,目的在使本發明所屬領域中具通常知識者,能瞭解本發明之內容並可據以實現,並非用於限制本發明之保護範疇。任何熟悉本技術者在不違背本發明之技術原理及精神下,可輕易完成之改變或安排,均屬本發明所主張之範圍。因此,本發明之權利保護範圍係如後附申請專利範圍所列。The above-mentioned embodiments are only illustrative of the principles and effects of the present invention, and explain the technical features of the present invention. The purpose is to enable those with ordinary knowledge in the field to which the present invention belongs to understand the content of the present invention and implement it accordingly, not Used to limit the protection scope of the present invention. Any change or arrangement that can be easily completed by anyone familiar with the technology without violating the technical principles and spirit of the present invention falls within the scope claimed by the present invention. Therefore, the protection scope of the present invention is as listed in the appended patent application scope.
無。no.
第1圖係本發明螢光材料之數個具體實施態樣之晶相繞射分析結果。Figure 1 shows the results of crystal phase diffraction analysis of several embodiments of the fluorescent material of the present invention.
第2a圖係本發明螢光材料之數個具體實施態樣之激發光譜圖(放射光之波峰設定於580 nm波長)。Figure 2a is the excitation spectrum of several embodiments of the fluorescent material of the present invention (the peak of the emitted light is set at a wavelength of 580 nm).
第2b圖係本發明螢光材料之數個具體實施態樣之激發光譜圖(放射光之波峰設定於620 nm波長)。Figure 2b is the excitation spectrum of several embodiments of the fluorescent material of the present invention (the peak of the emitted light is set at a wavelength of 620 nm).
第3a圖係本發明螢光材料之數個具體實施態樣於波峰在510 nm波長之激發光所激發的放射光譜圖。FIG. 3a is an emission spectrum diagram excited by excitation light with a peak of 510 nm at several specific embodiments of the fluorescent material of the present invention.
第3b圖係本發明螢光材料之數個具體實施態樣於波峰460 nm波長之激發光所激發的放射光譜圖。Fig. 3b is a graph of the emission spectrum excited by the excitation light with a peak wavelength of 460 nm at several specific embodiments of the fluorescent material of the present invention.
第4a圖係本發明螢光材料之數個具體實施態樣於波峰在510 nm波長之激發光所激發的放射光譜所對應的色座標圖譜。FIG. 4a is a color coordinate spectrum corresponding to the emission spectrum excited by the excitation light with a peak of 510 nm at several specific embodiments of the fluorescent material of the present invention.
第4b圖係本發明螢光材料之數個具體實施態樣於波峰在460 nm波長之激發光所激發的放射光譜所對應的色座標圖譜。FIG. 4b is a color coordinate spectrum corresponding to the emission spectrum excited by the excitation light with a peak of 460 nm at several embodiments of the fluorescent material of the present invention.
第5a圖係本發明螢光材料之一具體實施態樣之放射光譜隨波長變化的測試結果。Figure 5a is a test result of the variation of the emission spectrum of the fluorescent material according to one embodiment of the present invention with wavelength.
第5b圖係本發明螢光材料另一具體實施態樣之放射光譜隨波長變化的測試結果。FIG. 5b is a test result of the variation of the emission spectrum of the fluorescent material according to another embodiment of the present invention with wavelength.
無。no.
無no
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| CN103254900A (en) * | 2007-04-18 | 2013-08-21 | 三菱化学株式会社 | Phosphor and its light-emitting device |
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