JP5697387B2 - Method for producing β-sialon - Google Patents
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Description
本発明は、例えば蛍光体として好適なβ型サイアロンの製造法に関する。 The present invention relates to a method for producing β-sialon suitable as, for example, a phosphor.
一次光を発する発光素子と、一次光を吸収して二次光を発する蛍光体とを組み合わせた発光装置は、低消費電力、小型化、高い発光強度かつ広範囲な色の再現性が求められる次世代の発光装置として注目され、活発に研究開発が行なわれている。 A light-emitting device that combines a light-emitting element that emits primary light and a phosphor that absorbs primary light and emits secondary light requires low power consumption, downsizing, high emission intensity, and wide color reproducibility. It is attracting attention as a next-generation light-emitting device, and is actively researched and developed.
例えば、青色から紫色の短波長の可視光を発光する半導体発光素子と蛍光体とを組み合わせ、半導体発光素子の発光と蛍光体により波長変換された光との混色により白色光を得る白色LEDが知られている。 For example, a white LED that obtains white light by combining a semiconductor light-emitting element that emits blue to violet short-wavelength visible light and a phosphor and mixing the light emitted from the semiconductor light-emitting element and light that has been wavelength-converted by the phosphor is known. It has been.
特許文献1には、青色から紫色の短波長の可視光を発光する半導体発光素子と蛍光体とを組み合わせることにより、半導体発光素子の発光と蛍光体により波長変換された光との混色により白色光を得る白色LEDが開示されている。 In Patent Document 1, a combination of a semiconductor light-emitting element that emits blue to violet short-wavelength visible light and a phosphor allows white light to be emitted by mixing the light emitted from the semiconductor light-emitting element and the light wavelength-converted by the phosphor. A white LED for obtaining the above is disclosed.
蛍光体に関しては、ケイ酸塩、リン酸塩、アルミン酸塩、硫化物を母体材料として用い、発光中心に遷移金属もしくは希土類金属を用いたものが広く知られている。 Regarding phosphors, silicates, phosphates, aluminates, and sulfides are widely used as base materials, and transition metals or rare earth metals are used as the emission center.
近年、白色LEDにはより高い出力と、蛍光体の耐熱性、耐久性に対する要求が益々高まっている。これは、使用環境の温度上昇に伴う蛍光体の輝度の低下や、長時間青色光や紫外線の励起源に曝されることによる蛍光体の劣化に原因して、白色LEDとしての輝度低下や色ズレが発生するという問題が生じていることが背景にある。 In recent years, white LEDs have been increasingly demanded for higher output, phosphor heat resistance and durability. This is due to a decrease in luminance and color of white LEDs due to a decrease in luminance of the phosphor due to a temperature increase in the use environment and deterioration of the phosphor due to exposure to an excitation source of blue light or ultraviolet light for a long time. The background is the problem of misalignment.
温度上昇に伴う輝度低下が小さく、耐久性に優れた蛍光体として、最近、結晶構造が安定な窒化物や酸窒化物の蛍光体が注目されている。 Recently, phosphors of nitride or oxynitride having a stable crystal structure have attracted attention as phosphors having a small decrease in luminance due to temperature rise and excellent durability.
窒化物や酸窒化物の蛍光体として、窒化ケイ素の固溶体であるサイアロンが代表的である。窒化ケイ素の結晶構造と同様に、サイアロンには、α型およびβ型の二種類の結晶系が存在する。そして、特定の希土類元素を固溶するα型サイアロンは、有用な蛍光特性を有することが知られており、白色LED等への適用が検討されている(特許文献2〜4参照)。 As a nitride or oxynitride phosphor, sialon which is a solid solution of silicon nitride is typical. Similar to the crystal structure of silicon nitride, sialon has two types of crystal systems, α-type and β-type. And it is known that the alpha sialon which dissolves a specific rare earth element has a useful fluorescence characteristic, and application to white LED etc. is examined (refer patent documents 2-4).
また、希土類元素を固溶するβ型サイアロンも、同様の蛍光特性を有することが見いだされている(特許文献5参照)。 Moreover, it has been found that β-sialon which dissolves rare earth elements also has similar fluorescence characteristics (see Patent Document 5).
β型サイアロンは、β型窒化ケイ素の固溶体であり、β型窒化ケイ素結晶のSi位置にAlが、N位置にOが置換固溶したものである。単位胞(単位格子)に2式量の原子があるので、一般式として、Si6−zAlzOzN8−zが用いられる。ここで、組成zは、0<z<4.2であり、固溶範囲は非常に広く、また(Si、Al)/(N、O)のモル比は、3/4を維持する必要がある。β型窒化ケイ素の結晶構造はP63またはP63/mの対称性を持ち、理想原子位置を持つ構造として定義される(特許文献5参照)。また、一般的に原料としては、窒化ケイ素の他に、酸化ケイ素と窒化アルミニウムとを、或いは酸化アルミニウムと窒化アルミニウムとを加えて加熱することでβ型サイアロンが得られる。 β-type sialon is a solid solution of β-type silicon nitride in which Al is substituted at the Si position and O is substituted at the N position. Since there are two amounts of atoms in the unit cell (unit cell), Si 6-z Al z O z N 8-z is used as a general formula. Here, the composition z is 0 <z <4.2 , the solid solution range is very wide, and the molar ratio of (Si, Al) / (N, O) must be maintained at 3/4. is there. The crystal structure of β-type silicon nitride is defined as a structure having symmetry of P6 3 or P6 3 / m and having an ideal atomic position (see Patent Document 5). In general, as a raw material, β-sialon can be obtained by heating by adding silicon oxide and aluminum nitride or aluminum oxide and aluminum nitride in addition to silicon nitride.
β型サイアロンの結晶構造内にユーロピウム(Eu2+)を含有させると、紫外から青色の光で励起され、520〜550nmの緑色発光を示す蛍光体となり、白色LED等の発光装置の緑色発光成分として使用でき、Eu2+を固溶したβ型サイアロンとして知られている。このEu2+を固溶したβ型サイアロンは、Eu2+を固溶する蛍光体の中でも、発光スペクトルは非常にシャープであるため、青、緑、赤の狭帯域発光が要求される画像処理表示装置又は液晶ディスプレイパネルのバックライト光源に適した素材である。 When europium (Eu 2+ ) is included in the crystal structure of β-sialon, it is excited by ultraviolet to blue light and becomes a phosphor that emits green light of 520 to 550 nm, and as a green light emitting component of a light emitting device such as a white LED. It can be used and is known as β-sialon in which Eu 2+ is dissolved. Β-SiAlON which is a solid solution of the Eu 2+, among the phosphors solid solution Eu 2+, since the emission spectrum is very sharp, blue, green, image processing and displaying apparatus narrowband emission of red are required Or it is a material suitable for the backlight light source of a liquid crystal display panel.
ところで、画像処理表示装置又は液晶ディスプレイ等のバックライト光源に使用する発光装置は、照明用途と異なり、青、緑、赤の3原色の発光スペクトルの幅が狭いことが望まれる。白色光からは、3原色のそれぞれの色のみを透過するフィルターを通して3原色が得られるが、液晶ディスプレイ等のバックライトとして使用するため、蛍光体には発光スペクトル幅の狭い緑色や赤色の光を発光するものが要求されている。 By the way, unlike a lighting application, a light emitting device used for a backlight light source such as an image processing display device or a liquid crystal display is desired to have a narrow emission spectrum width of three primary colors of blue, green, and red. From white light, the three primary colors can be obtained through a filter that transmits only the three primary colors. However, in order to use it as a backlight for a liquid crystal display or the like, green or red light having a narrow emission spectrum width is used as a phosphor. What emits light is required.
しかし、金属ケイ素、窒化アルミニウム、酸化ユーロピウムを用いて製造したEu2+を固溶したβ型サイアロンは、発光ピーク波長が緑色から赤色側、すなわち長波長側にシフトしており、液晶ディスプレイ等のバックライト光源に使用するためには発光スペクトルを短波長化することが求められていた。また、発光スペクトルを更に狭帯域化させることも同時に要求されていた。 However, β-sialon, which is a solid solution of Eu 2+ produced using metallic silicon, aluminum nitride, and europium oxide, has an emission peak wavelength shifted from green to red, that is, a long wavelength side. In order to use it as a light source, it has been required to shorten the emission spectrum. At the same time, it has been required to further narrow the emission spectrum.
ところが、Eu2+を固溶したβ型サイアロンの発光強度と、発光スペクトルの短波長化及び狭帯域化にはトレードオフの関係がある。発光強度を高めた場合には、発光スペクトルの発光ピークが長波長化し、スペクトル幅が広がるため、液晶ディスプレイのバックライト用途に用いた場合に色再現範囲が狭くなる。一方、発光スペクトルを短波長化及び狭帯域化した場合には十分な輝度が得られない。 However, there is a trade-off relationship between the emission intensity of β-sialon in which Eu 2+ is dissolved and the emission spectrum having a shorter wavelength and a narrower band. When the emission intensity is increased, the emission peak of the emission spectrum becomes longer and the spectrum width is widened, so that the color reproduction range is narrowed when used for backlight applications of liquid crystal displays. On the other hand, when the emission spectrum is shortened and narrowed, sufficient luminance cannot be obtained.
上述の課題に鑑み、本発明は、高い発光強度、発光スペクトルの短波長化及び狭帯域発光を実現できるEu2+を固溶したβ型サイアロンの製造方法を提供することを目的とする。 In view of the above-described problems, an object of the present invention is to provide a method for producing β-sialon in which Eu 2+ is dissolved, which can realize high emission intensity, shortening of the emission spectrum, and narrow-band emission.
一般式:Si6−zAlzOzN8−zで示されるβ型サイアロンを母体結晶にEu2+を固溶したβ型サイアロンにおいて、特許文献6に示されているように、Eu固溶β型サイアロン結晶内の酸素固溶量を低くすること、つまり上式のz値を低くすることにより、発光スペクトルを短波長化及び狭帯域化することが可能である。しかしながら、z値を低くすると発光強度が低下するという問題があった。 In a β-type sialon in which Eu 2+ is dissolved in a base crystal of a β-type sialon represented by the general formula: Si 6-z Al z O z N 8-z , as shown in Patent Document 6, Eu solid solution By reducing the amount of oxygen dissolved in the β-type sialon crystal, that is, by reducing the z value in the above equation, the emission spectrum can be shortened and narrowed. However, there is a problem that the emission intensity decreases when the z value is lowered.
本発明者等は、Eu2+を固溶したβ型サイアロンの発光特性について研究を重ねたところ、金属ケイ素、窒化アルミニウム、酸化ユーロピウムを焼成して得られるEu2+を固溶したβ型サイアロンの合成において、原料混合物に含まれる金属ケイ素の窒化反応が発光スペクトルの短波長化及び狭帯域化に影響するという知見を得て、本発明を完成するに至った。 The present inventors have revealed that studying about emission properties of β-sialon obtained by solid solution Eu 2+, metal silicon, aluminum nitride, synthetic solid-dissolved β-SiAlON the Eu 2+ obtained by firing europium oxide Thus, the inventors have obtained the knowledge that the nitridation reaction of metallic silicon contained in the raw material mixture affects the shortening and narrowing of the emission spectrum, and the present invention has been completed.
本発明は、上記目的を達成するため、一般式Si6−zAlzOzN8−zで示されるβ型サイアロンに発光中心としてEu2+を固溶したβ型サイアロンの製造法において、金属ケイ素、アルミニウム化合物及び酸化ユーロピウムを含む混合物を窒素雰囲気下で加熱する窒化処理工程と、窒化処理された混合物を加熱処理する焼成工程とを含む、β型サイアロンの製造法を提供する。
ここで、窒化処理工程の処理条件は、加熱温度が1450℃以上1550℃以下の範囲であって、圧力(y)が加熱温度(x)との関係式:y≦−0.0035x+5.575を満たしている必要がある。
In order to achieve the above object, the present invention provides a process for producing β-sialon in which Eu 2+ is dissolved as a light-emitting center in β-sialon represented by the general formula Si 6-z Al z O z N 8-z. Provided is a method for producing β-sialon, which includes a nitriding treatment step in which a mixture containing silicon, an aluminum compound and europium oxide is heated in a nitrogen atmosphere, and a firing step in which the nitriding mixture is heat-treated.
Here, the processing conditions of the nitriding step are as follows: the heating temperature is in the range of 1450 ° C. or more and 1550 ° C. or less, and the pressure (y) is a relational expression with respect to the heating temperature (x): y ≦ −0.0035x + 5.575. Must meet.
本発明の製造方法によれば、Eu2+を固溶したβ型サイアロン(以下、β型サイアロンという。)の発光特性のバラツキをコントロールすることが可能である。本発明の製造方法により得られたβ型サイアロンは、紫外線から可視光の幅広い波長域で励起され、高い発光強度と緑色の狭帯域で発光するため、緑色の蛍光体として優れている。本発明のβ型サイアロンは、使用環境の変化に対する輝度変化が少なく、単独もしくは他の蛍光体と組み合わせて種々の発光素子、特に紫外LEDと青色LEDを光源とする白色LEDに使用できる。 According to the production method of the present invention, it is possible to control variations in the light emission characteristics of β-sialon (hereinafter referred to as β-sialon) in which Eu 2+ is dissolved. The β-sialon obtained by the production method of the present invention is excellent as a green phosphor because it is excited in a wide wavelength range from ultraviolet to visible light and emits light in a high emission intensity and a narrow green band. The β-sialon of the present invention has little change in luminance with respect to changes in the use environment, and can be used for various light-emitting elements, particularly white LEDs using ultraviolet LEDs and blue LEDs as light sources, alone or in combination with other phosphors.
本発明は、一般式Si6−zAlzOzN8−zで示されるβ型サイアロンに発光中心としてEu2+を固溶したβ型サイアロンの製造法において、金属ケイ素、アルミニウム化合物及び酸化ユーロピウムを含む混合物を窒素雰囲気下で加熱する窒化処理工程と、窒化処理された混合物を加熱処理する焼成工程を含む、β型サイアロンの製造法である。 The present invention relates to a process for producing β-sialon in which Eu 2+ as a luminescent center is dissolved in β-sialon represented by the general formula Si 6-z Al z O z N 8-z. A sialon manufacturing method including a nitriding treatment step of heating a mixture containing nitrile in a nitrogen atmosphere and a firing step of heat-treating the nitrided mixture.
原料としての金属ケイ素、アルミニウム化合物及び酸化ユーロピウムは、粉末であることが望ましい。金属ケイ素には不純物として鉄が含まれていてもよいが、20ppm以下のであることが望ましく、さらには10ppm以下であることが好ましい。 The metal silicon, aluminum compound and europium oxide as raw materials are preferably powders. Metallic silicon may contain iron as an impurity, but is preferably 20 ppm or less, and more preferably 10 ppm or less.
アルミニウム化合物は、窒化アルミニウム、酸化アルミニウム又は加熱により分解して酸化アルミニウムを産生するアルミニウム含有化合物から選ばれる1種以上のアルミニウム化合物をいう。 The aluminum compound refers to one or more aluminum compounds selected from aluminum nitride, aluminum oxide, or an aluminum-containing compound that decomposes by heating to produce aluminum oxide.
窒化処理では、窒素雰囲気下、金属ケイ素、アルミニウム化合物及び酸化ユーロピウムを含む混合物を加圧加熱処理する。処理条件は、加熱温度が1450℃以上1550℃以下の範囲であって、圧力(y)が加熱温度(x)との関係式:y≦−0.0035x+5.575を満たしている必要がある。
加熱温度が低いとEu2+がβ型サイアロン結晶中に入り込むことができないので好ましくない。
また、窒化処理の温度条件又は圧力条件は、後工程である焼成工程との関連で、β型サイアロンの発光波長のピークの赤色側へのシフトに影響を与える。加熱温度が1550℃を越えるか、又は、加熱温度(x)との関係において窒化処理工程の圧力(y)が−0.0035x+5.575の値より高くなると、後工程である焼成によって、β型サイアロンの発光波長のピークが赤色側、すなわち長波長側にシフトするので好ましくない。
In the nitriding treatment, a mixture containing metal silicon, an aluminum compound and europium oxide is subjected to pressure and heat treatment in a nitrogen atmosphere. The treatment condition is that the heating temperature is in the range of 1450 ° C. or more and 1550 ° C. or less, and the pressure (y) needs to satisfy the relational expression with respect to the heating temperature (x): y ≦ −0.0035x + 5.575.
If the heating temperature is low, Eu 2+ cannot enter the β-type sialon crystal, which is not preferable.
In addition, the temperature condition or pressure condition of the nitriding treatment affects the shift of the emission wavelength peak of β-sialon to the red side in relation to the firing process which is a subsequent process. When the heating temperature exceeds 1550 ° C. or the pressure (y) in the nitriding process is higher than the value of −0.0035x + 5.575 in relation to the heating temperature (x), the β-type is formed by the subsequent baking. Since the peak of the emission wavelength of sialon shifts to the red side, that is, the long wavelength side, it is not preferable.
焼成工程は定法の条件に従って窒素雰囲気下で加熱して行えばよい。加熱温度は、1850〜2050℃の範囲が好ましい。加熱温度が高ければEu2+がβ型サイアロンの結晶中に入り込むことができ、十分な発光強度を有するβ型サイアロンが得られる。加熱温度が上述した温度範囲内であれば、非常に高い窒素圧力をかけてβ型サイアロンの分解を抑制する必要がなく、特殊な装置を必要とすることもないので工業的に好ましい。 The firing step may be performed by heating in a nitrogen atmosphere in accordance with the conditions of a regular method. The heating temperature is preferably in the range of 1850 to 2050 ° C. If the heating temperature is high, Eu 2+ can enter the β-sialon crystal, and a β-sialon having sufficient emission intensity can be obtained. If the heating temperature is within the above-mentioned temperature range, it is not necessary to suppress the decomposition of β-sialon by applying a very high nitrogen pressure, and a special apparatus is not required, which is industrially preferable.
焼成物は粒状又は塊状となる。これを解砕、粉砕及び/又は分級操作と組み合わせて所定のサイズの粉末にする。具体的な処理の例としては、焼成物を目開き20〜45μmの篩分級処理し、篩を通過した粉末を得る方法、或いは焼成物をボールミルや振動ミル、ジェットミル等の一般的な粉砕機を使用して所定の粒度に粉砕する方法が挙げられる。後者の方法において、過度の粉砕は、光を散乱しやすい微粒子を生成するだけでなく、粒子表面に結晶欠陥を生成し、発光強度の低下を引き起こす。本発明者らの検討によれば、粉砕処理を行わずに篩分級のみによる処理により得られた粉末が最終的に高い発光強度を示した。 The fired product is granular or massive. This is combined with pulverization, pulverization and / or classification operations to obtain a powder of a predetermined size. Specific examples of the treatment include a method of obtaining a powder that has passed through a sieve by subjecting the fired product to a sieve classification having an opening of 20 to 45 μm, or a general grinder such as a ball mill, a vibration mill, or a jet mill. And a method of pulverizing to a predetermined particle size. In the latter method, excessive pulverization not only generates fine particles that easily scatter light, but also generates crystal defects on the particle surface, causing a decrease in emission intensity. According to the study by the present inventors, the powder obtained by the treatment only by the sieve classification without performing the pulverization treatment finally showed high luminescence intensity.
以下、「粉末混合原料の製造」〜「焼成工程」において、窒化処理の温度(x)と圧力(y)の関係を、y>−0.0035x+5.575の条件としたβ型サイアロンの製造例を比較例1とし、y≦−0.0035x+5.575の条件を満たす製造例を実験例1〜3として以下に示す。 Hereinafter, in “Production of powder mixed raw material” to “Firing process”, a production example of β-sialon in which the relationship between the temperature (x) and the pressure (y) of nitriding is y> −0.0035x + 5.575 Is shown as Comparative Example 1 and Examples of Production satisfying the condition of y ≦ −0.0035x + 5.575 are shown below as Experimental Examples 1 to 3.
まず、本発明の実験例の説明に先立って、比較例を説明する。
[比較例1]
「粉末混合原料の製造」
シリコン粉末(純度99.999%以上、−45μm、高純度化学社製)96.41質量%、窒化アルミニウム粉末(トクヤマ社製Eグレード)1.16質量%、及び酸化ユーロピウム粉末(信越化学工業社製RUグレード)2.43質量%を、窒化ケイ素焼成体製の乳鉢と乳棒を用いて混合し、更に目開き250μmの篩を全通させて凝集を取り除き、粉末混合原料とした。
First, a comparative example will be described prior to the description of the experimental example of the present invention.
[Comparative Example 1]
"Production of powder mixed raw materials"
Silicon powder (purity 99.999% or more, −45 μm, manufactured by Kojun Chemical Co., Ltd.) 96.41% by mass, aluminum nitride powder (E grade manufactured by Tokuyama Co., Ltd.) 1.16% by mass, and europium oxide powder (Shin-Etsu Chemical Co., Ltd.) (RU grade manufactured) 2.43 mass% was mixed using a mortar and pestle made of a silicon nitride fired body, and further passed through a sieve having a mesh size of 250 μm to remove agglomerates to obtain a powder mixed raw material.
「窒化処理工程」
粉末混合原料を直径40mm×高さ30mmの蓋付きの円筒型窒化ホウ素製容器(電気化学工業社製、「N−1」グレード)に充填し、カーボンヒーターの電気炉で0.50MPaの加圧窒素雰囲気中、1550℃で8時間の加熱処理を行った。加熱時の昇温速度は、室温〜1200℃までを20℃/分で、1200〜1550℃までを0.5℃/分とした。得られた生成物は、塊状であり、これを窒化ケイ素焼成体製の乳鉢と乳棒を用いて粉砕した。粉砕した粉末を目開き45μmの篩で分級し、45μm以下の粉末をβ型サイアロン焼成用のEu固溶アルミニウム含有窒化ケイ素粉末とした。さらに、得られたEu固溶アルミニウム含有窒化ケイ素粉末を目開き250μmの篩を全通させ、Eu固溶β型サイアロン用粉末混合原料とした。
"Nitriding process"
The powder mixed raw material is filled into a cylindrical boron nitride container (made by Denki Kagaku Kogyo Co., Ltd., “N-1” grade) with a lid having a diameter of 40 mm and a height of 30 mm, and a pressure of 0.50 MPa is applied in an electric furnace of a carbon heater. Heat treatment was performed at 1550 ° C. for 8 hours in a nitrogen atmosphere. The heating rate during heating was 20 ° C./min from room temperature to 1200 ° C., and 0.5 ° C./min from 1200 to 1550 ° C. The obtained product was massive and was pulverized using a mortar and pestle made of a silicon nitride fired body. The pulverized powder was classified with a sieve having an opening of 45 μm, and the powder of 45 μm or less was used as Eu solid solution aluminum-containing silicon nitride powder for β-type sialon firing. Further, the obtained Eu solid solution aluminum-containing silicon nitride powder was passed through a sieve having an opening of 250 μm to obtain a powder mixed raw material for Eu solid solution β-sialon.
「焼成工程」
Eu固溶β型サイアロン用粉末混合原料を直径60mm×高さ30mmの蓋付きの円筒型窒化ホウ素製容器(電気化学工業社製、「N−1」グレード)に充填し、カーボンヒーターの電気炉で0.8MPaの加圧窒素雰囲気中、2000℃で8時間の加熱処理を行った。得られた生成物は緑色の緩く凝集した塊状物であり、人手で軽く解すことが出来た。こうして、軽度の解砕を行った後、目開き45μmの篩を通過させて比較例1のβ型サイアロンを得た。
"Baking process"
Powder mixed raw material for Eu solid solution β-type sialon is filled into a cylindrical boron nitride vessel (“N-1” grade, manufactured by Denki Kagaku Kogyo Co., Ltd.) with a lid 60 mm in diameter and 30 mm in height, and an electric furnace for a carbon heater Then, heat treatment was performed at 2000 ° C. for 8 hours in a pressurized nitrogen atmosphere of 0.8 MPa. The obtained product was a green loosely agglomerated lump, which could be lightly unraveled manually. In this way, after mild crushing, it was passed through a sieve having an opening of 45 μm to obtain β-sialon of Comparative Example 1.
[実験例1]
窒化処理の加熱温度を1450℃、圧力条件を0.5MPaとした以外は、比較例1と同じ条件でβ型サイアロンを得た。
[Experimental Example 1]
Β-sialon was obtained under the same conditions as in Comparative Example 1 except that the heating temperature for nitriding was 1450 ° C. and the pressure condition was 0.5 MPa.
[実験例2]
窒化処理の加熱温度を1550℃、圧力条件を0.15MPaとした以外は、比較例1と同じ条件でβ型サイアロンを得た。
[Experiment 2]
Β-sialon was obtained under the same conditions as in Comparative Example 1 except that the heating temperature for nitriding was 1550 ° C. and the pressure condition was 0.15 MPa.
[実験例3]
窒化処理の加熱温度を1450℃、圧力条件を0.15MPaとした以外は、比較例1と同じ条件でβ型サイアロンを得た。
[Experiment 3]
A β-sialon was obtained under the same conditions as in Comparative Example 1 except that the heating temperature for nitriding was 1450 ° C. and the pressure condition was 0.15 MPa.
「発光特性の測定方法及び結果」
β型サイアロンの発光特性は次のように評価した。まずβ型サイアロン粉末を凹型のセルに充填し、表面を平滑にして、積分球を取り付けた。この積分球に、発光光源(Xeランプ)から所定の波長に分光した単色光を、光ファイバーを用いて導入した。この単色光を励起源として、β型サイアロン試料に照射し、分光光度計(大塚電子社製、MCPD−7000)を用いて、試料の蛍光及び反射光のスペクトル測定を行った。本実施例では、単色光は、波長455nmの青色光を用いた。
"Measurement method and result of luminescence characteristics"
The light emission characteristics of β-sialon were evaluated as follows. First, β-sialon powder was filled into a concave cell, the surface was smoothed, and an integrating sphere was attached. Monochromatic light that was split into a predetermined wavelength from a light emitting light source (Xe lamp) was introduced into the integrating sphere using an optical fiber. Using this monochromatic light as an excitation source, a β-type sialon sample was irradiated, and the spectrophotometer (MCPD-7000, manufactured by Otsuka Electronics Co., Ltd.) was used to measure the spectrum of the fluorescence and reflected light of the sample. In this example, blue light having a wavelength of 455 nm was used as the monochromatic light.
得られた発光スペクトルにおいて、励起波長が455nmのときの、465〜780nm範囲の波長域のデータからJIS Z8724に準じ、JIS Z8701で規定されるXYZ表色系における色度座標CIExとCIEyを算出した。 In the obtained emission spectrum, the chromaticity coordinates CIEx and CIEy in the XYZ color system defined by JIS Z8701 were calculated from the data in the wavelength range of 465 to 780 nm when the excitation wavelength was 455 nm, according to JIS Z8724. .
発光強度として量子効率を次のようにして求めた。まず試料部に反射率が99%の標準反射板(Labsphere社、スペクトラロン)をセットし、励起光のスペクトルを測定し、励起波長が455nmの場合は450〜465nmの波長範囲のスペクトルから励起光フォトン数(Qex)を算出した。次いで、試料部にβ型サイアロンをセットし、得られたスペクトルデータから励起反射光フォトン数(Qref)及び蛍光フォトン数(Qem)を算出した。 The quantum efficiency was determined as the emission intensity as follows. First, a standard reflector (Labsphere, Spectralon) with a reflectance of 99% is set on the sample part, and the spectrum of the excitation light is measured. When the excitation wavelength is 455 nm, the excitation light is obtained from the spectrum in the wavelength range of 450 to 465 nm. The number of photons (Qex) was calculated. Next, β-sialon was set in the sample portion, and the number of excited reflected light photons (Qref) and the number of fluorescent photons (Qem) were calculated from the obtained spectrum data.
尚、励起反射光フォトン数は、励起光フォトン数と同じ波長範囲で、蛍光フォトン数は、励起光が455nmの場合、465〜800nmの範囲で算出した。 The number of excitation reflected light photons was calculated in the same wavelength range as the number of excitation light photons, and the number of fluorescent photons was calculated in the range of 465 to 800 nm when the excitation light was 455 nm.
得られた三種類のフォトン数から外部量子効率(=Qem/Qex×100)、吸収率(=(Qex−Qref)×100)、内部量子効率(=Qem/(Qex−Qref)×100)を求めた。 The external quantum efficiency (= Qem / Qex × 100), the absorption rate (= (Qex−Qref) × 100), and the internal quantum efficiency (= Qem / (Qex−Qref) × 100) are obtained from the obtained three types of photons. Asked.
また、発光強度を示す別の測定値である相対ピーク強度を次のように測定した。YAG:Ce(P46Y3;化成オプトニクス社製)の発光スペクトルのピーク高さを100%とした蛍光体のピーク高さを相対ピーク強度(%)で表した。比較例1、実験例1〜3のβ型サイアロンの吸収率、内部量子効率、外部量子効率、色度及び相対ピーク強度の測定結果を表1に示す。 Further, the relative peak intensity, which is another measured value indicating the emission intensity, was measured as follows. The peak height of the phosphor with the peak height of the emission spectrum of YAG: Ce (P46Y3; manufactured by Kasei Optonix Co., Ltd.) as 100% was expressed as a relative peak intensity (%). Table 1 shows the measurement results of the absorption rate, internal quantum efficiency, external quantum efficiency, chromaticity, and relative peak intensity of β-sialons of Comparative Example 1 and Experimental Examples 1 to 3.
表1に示すように、波長455nmの青色光で励起した場合、比較例1のβ型サイアロンの吸収率、内部量子効率、外部量子効率はそれぞれ71.9%、41.3%、29.7%であり、CIEx(色度x)は、0.308、発光強度は136%であった。実験例1〜3では、CIEx値が小さく、それぞれのCIEx値及びCIEy値がほぼ同じ値を示し、比較例1に比べて長波長化が抑制されて青色側、すなわち短波長側にシフトしていることがわかる。 As shown in Table 1, when excited with blue light having a wavelength of 455 nm, the absorption rate, internal quantum efficiency, and external quantum efficiency of β-sialon of Comparative Example 1 were 71.9%, 41.3%, and 29.7, respectively. CIEx (chromaticity x) was 0.308, and the emission intensity was 136%. In Experimental Examples 1 to 3, the CIEx value is small, and the CIEx value and the CIEy value are almost the same, and the longer wavelength is suppressed compared to Comparative Example 1, and the blue side, that is, the shorter wavelength side is shifted. I understand that.
図1に、比較例1及び実験例1〜3の結果と、この結果を踏まえて求めた温度−圧力の関係式を示す。y=−0.0035x+5.575(ここでxは加熱温度、yは圧力)の関係式の値を境にして、比較例と実験例1〜3とが分離して分布していることが分かる。すなわち、加熱温度を1450℃以上1550℃以下、圧力(y)をy≦−0.0035x+5.575(ここで、xは加熱温度)を満たす条件として窒化処理を行うことで、β型サイアロンの発光色を青色側にシフトすることができ、また発光領域を緑色の狭帯域発光とする制御が容易になる。
以上、実施例に示したように、Eu固溶β型サイアロン用粉末混合原料を、1450℃以上1550℃以下の温度範囲で、且つ圧力(y)が加熱温度(x)との関係式:y≦−0.0035x+5.575を満たす範囲で窒化することにより、長波長化が抑制され、色度がバラつくことなく、発光強度が向上していることが分かる。
FIG. 1 shows the results of Comparative Example 1 and Experimental Examples 1 to 3, and the temperature-pressure relational expression obtained based on these results. It can be seen that the comparative example and the experimental examples 1 to 3 are distributed separately with respect to the value of the relational expression y = −0.0035x + 5.575 (where x is the heating temperature and y is the pressure). . That is, by performing nitriding under conditions where the heating temperature is 1450 ° C. or more and 1550 ° C. or less and the pressure (y) is y ≦ −0.0035x + 5.575 (where x is the heating temperature), β-sialon emission The color can be shifted to the blue side, and the light emitting area can be easily controlled to emit green narrow band light.
As described above, in the powder mixed raw material for Eu solid solution β-type sialon, the relational expression of the pressure (y) with the heating temperature (x) in the temperature range of 1450 ° C. to 1550 ° C .: y It can be seen that by performing nitriding in a range satisfying ≦ −0.0035x + 5.575, the wavelength increase is suppressed, and the luminescence intensity is improved without variation in chromaticity.
以上、本発明を実施例に基づいて説明したが、この実施例はあくまで例示であり、種々の変形例が可能なこと、またそうした変形例も本発明の範囲にあることが当業者には容易に理解されるところである。 The present invention has been described based on the embodiments. However, the embodiments are merely examples, and it is easy for those skilled in the art that various modifications are possible and that such modifications are also within the scope of the present invention. Is understood.
本発明の製造法によって得られるβ型サイアロンは、紫外から青色光の幅広い波長で励起され、高輝度かつ狭帯化された緑色発光を示すことから、青色又は紫外光を光源とする白色LEDの蛍光体として好適に使用できるものであり、特に、画像表示装置に好適に使用できる。さらに、高温での輝度低下が少なく、また耐熱性や耐湿性に優れることから、上述の画像表示装置分野に適用すれば、使用環境温度の変化に対する輝度および発光色の変化が小さく、長期間の安定性にも優れる特性が発揮できる。 The β-sialon obtained by the production method of the present invention is excited by a wide range of wavelengths from ultraviolet to blue light, and exhibits high luminance and narrow band green light emission. It can be suitably used as a phosphor, and can be particularly suitably used for an image display device. Furthermore, since there is little decrease in brightness at high temperatures and excellent heat resistance and moisture resistance, when applied to the above-mentioned image display device field, changes in brightness and emission color with respect to changes in the operating environment temperature are small, and long-term Excellent stability can be achieved.
Claims (2)
金属ケイ素、アルミニウム化合物及び酸化ユーロピウムを含む混合物を窒素雰囲気下で加熱する窒化処理工程と、窒化処理された混合物を加熱処理する焼成工程とを含み、
前記窒化処理工程の加熱温度条件が1450℃以上1550℃以下の範囲であって、圧力MPa(y)が加熱温度(x)との関係式:y≦−0.0035x+5.575を満たす、β型サイアロンの製造法。 A method for producing a β-type sialon in which Eu 2+ is dissolved as a luminescent center in a β-type sialon represented by the general formula Si 6-z Al z O z N 8-z (0 <z <4.2) ,
Seen containing a nitriding process of silicon metal, aluminum compound and a mixture containing europium oxide is heated under a nitrogen atmosphere, and a firing step of heating a mixture that has been nitrided,
The β-type , wherein the heating temperature condition in the nitriding treatment step is in the range of 1450 ° C. or more and 1550 ° C. or less, and the pressure MPa (y) satisfies the relational expression with the heating temperature (x): y ≦ −0.0035x + 5.575 Sialon manufacturing method.
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