JP7712380B2 - AlN single crystal - Google Patents
AlN single crystalInfo
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- JP7712380B2 JP7712380B2 JP2023555066A JP2023555066A JP7712380B2 JP 7712380 B2 JP7712380 B2 JP 7712380B2 JP 2023555066 A JP2023555066 A JP 2023555066A JP 2023555066 A JP2023555066 A JP 2023555066A JP 7712380 B2 JP7712380 B2 JP 7712380B2
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- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B23/00—Single-crystal growth by condensing evaporated or sublimed materials
- C30B23/02—Epitaxial-layer growth
- C30B23/06—Heating of the deposition chamber, the substrate or the materials to be evaporated
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- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B25/00—Single-crystal growth by chemical reaction of reactive gases, e.g. chemical vapour-deposition growth
- C30B25/02—Epitaxial-layer growth
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- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B29/00—Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
- C30B29/10—Inorganic compounds or compositions
- C30B29/38—Nitrides
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Description
本発明は、AlN単結晶に関する。 The present invention relates to an AlN single crystal.
近年、窒化アルミニウム(AlN)単結晶が、AlN系半導体を用いた深紫外線発光素子の下地基板として注目されている。例えば、AlN系半導体として、AlNやAlGaN等が用いられる。これらのAlN系半導体は直接遷移型のバンド構造を有するため、発光デバイスに適しており、深紫外領域のLED(Light Emitting Diode)やLD(Laser Diode)への応用が可能である。In recent years, aluminum nitride (AlN) single crystals have been attracting attention as a base substrate for deep ultraviolet light-emitting devices using AlN-based semiconductors. For example, AlN and AlGaN are used as AlN-based semiconductors. These AlN-based semiconductors have a direct transition band structure, making them suitable for light-emitting devices, and can be applied to deep ultraviolet LEDs (Light Emitting Diodes) and LDs (Laser Diodes).
AlN単結晶の作製方法としては、HVPE法(ハライド気相成長法)、ミストCVD(化学気相成長)、昇華法等が知られている。例えば、非特許文献1(鎌田弘之等、「窒化アルミニウム単結晶」、フジクラ技報、2008年、Vol.2、第114号、pp.42-47)には、昇華法を用いて、種基板上にAlN単結晶を成長させる方法が開示されている。Known methods for producing AlN single crystals include HVPE (halide vapor phase epitaxy), mist CVD (chemical vapor phase epitaxy), sublimation, etc. For example, Non-Patent Document 1 (Kamata Hiroyuki et al., "Aluminum Nitride Single Crystals," Fujikura Technical Report, 2008, Vol. 2, No. 114, pp. 42-47) discloses a method for growing AlN single crystals on a seed substrate using sublimation.
また、作製したAlN単結晶は、その後の研削や研磨によりAlN単結晶の表面を平坦化及び鏡面化することが行われる。例えば特許文献1(特許第4511801号公報)には、AlNと同じ13族元素窒化物に属するGaN単結晶について、高品質な基板を得ることができる研磨方法が開示されている。In addition, the surface of the AlN single crystal thus produced is then flattened and mirror-finished by grinding and polishing. For example, Patent Document 1 (Patent Publication No. 4511801) discloses a polishing method for obtaining a high-quality substrate for GaN single crystal, which belongs to the same group 13 element nitride as AlN.
しかしながら、非特許文献1に開示されるような製法で作製されたAlN単結晶では、研削工程においてチッピング(欠けやクラックといった欠陥)が発生しやすく、AlN単結晶の歩留まりが低下する問題がある。また、AlN単結晶の表面を鏡面化させる研磨工程(すなわち、機械的研磨工程及び化学機械的研磨(CMP)工程)においても同様の問題がある。特許文献1では、上述のとおりGaN単結晶の研磨方法が開示されているが、チッピングの発生の抑制についての言及が無いだけでなく、AlN単結晶についても開示されていない。そこで、AlN単結晶を研磨する際、AlN単結晶に発生するチッピングを抑制することが望まれている。However, in the AlN single crystal produced by the method disclosed in Non-Patent Document 1, chipping (defects such as chips and cracks) is likely to occur in the grinding process, resulting in a problem of reduced yield of the AlN single crystal. In addition, the polishing process (i.e., mechanical polishing process and chemical mechanical polishing (CMP) process) for mirror-finishing the surface of the AlN single crystal also has a similar problem. As mentioned above, Patent Document 1 discloses a method for polishing a GaN single crystal, but not only is there no mention of suppressing the occurrence of chipping, but it does not disclose anything about the AlN single crystal. Therefore, it is desirable to suppress chipping that occurs in the AlN single crystal when polishing the AlN single crystal.
本発明者らは、今般、AlN単結晶に透過スペクトルにおいて特定の波長域で透過率が一定の割合で低下する特性を持たせることで、研削ないし研磨された際にチッピングが発生しにくいAlN単結晶を提供できるとの知見を得た。The inventors have now discovered that by endowing an AlN single crystal with the property that its transmittance decreases at a constant rate in a specific wavelength range in the transmission spectrum, it is possible to provide an AlN single crystal that is less susceptible to chipping when ground or polished.
したがって、本発明の目的は、研削ないし研磨された際にチッピングが発生しにくいAlN単結晶を提供することにある。Therefore, the object of the present invention is to provide an AlN single crystal that is less likely to chip when ground or polished.
本発明によれば、以下の態様が提供される。
[態様1]
AlN単結晶であって、前記AlN単結晶の透過スペクトルにおいて、640~660nmにおける透過率の平均値が、540~560nmにおける透過率の平均値及び780~800nmにおける透過率の平均値の各々よりも低く、640~660nmにおける透過率の平均値が780~800nmにおける透過率の平均値よりも5~20パーセントポイント(%pt)低い、AlN単結晶。
[態様2]
前記AlN単結晶の透過スペクトルにおいて、540~800nmの波長範囲内に半値幅が50~150nmとなる吸収ピークを有し、
前記半値幅は、(i)540~560nmにおける透過率の平均値と780~800nmにおける透過率の平均値のうち小さい方の値をT1とし、640~660nmにおける透過率の平均値をT2としたとき、(ii)T2+(T1-T2)/2から算出される透過率よりも低い透過率を与える波長範囲の幅として定義される、態様1に記載のAlN単結晶。
[態様3]
前記AlN単結晶の透過スペクトルにおいて、640~660nmにおける透過率の平均値が540~560nmにおける透過率の平均値よりも1~10%pt低い、態様1又は2に記載のAlN単結晶。
[態様4]
前記AlN単結晶の透過スペクトルにおいて、640~660nmにおける透過率の平均値が780~800nmにおける透過率の平均値よりも6~18%pt低い、態様1~3のいずれか一つに記載のAlN単結晶。
[態様5]
前記半値幅が70~120nmである、態様2~4のいずれか一つに記載のAlN単結晶。
[態様6]
前記AlN単結晶の透過スペクトルにおいて、640~660nmにおける透過率の平均値が540~560nmにおける透過率の平均値よりも3~8%pt低い、態様3に記載のAlN単結晶。
According to the present invention, the following aspects are provided.
[Aspect 1]
An AlN single crystal, wherein in a transmission spectrum of the AlN single crystal, an average value of the transmittance in the range of 640 to 660 nm is lower than an average value of the transmittance in the range of 540 to 560 nm and an average value of the transmittance in the range of 780 to 800 nm, and the average value of the transmittance in the range of 640 to 660 nm is lower than the average value of the transmittance in the range of 780 to 800 nm by 5 to 20 percentage points (%pt).
[Aspect 2]
In the transmission spectrum of the AlN single crystal, there is an absorption peak with a half-width of 50 to 150 nm within a wavelength range of 540 to 800 nm,
The AlN single crystal according to aspect 1, wherein the half width is defined as (i) the width of a wavelength range that gives a transmittance lower than the transmittance calculated from T2 + ( T1 - T2 ) / 2, where T1 is the smaller of the average transmittance in the range of 540 to 560 nm and the average transmittance in the range of 780 to 800 nm, and T2 is the average transmittance in the range of 640 to 660 nm.
[Aspect 3]
3. The AlN single crystal according to aspect 1 or 2, wherein in a transmission spectrum of the AlN single crystal, an average value of the transmittance in the range of 640 to 660 nm is lower by 1 to 10% pt than an average value of the transmittance in the range of 540 to 560 nm.
[Aspect 4]
The AlN single crystal according to any one of aspects 1 to 3, wherein in a transmission spectrum of the AlN single crystal, the average transmittance in the range of 640 to 660 nm is 6 to 18% pt lower than the average transmittance in the range of 780 to 800 nm.
[Aspect 5]
The AlN single crystal according to any one of aspects 2 to 4, wherein the half-width is 70 to 120 nm.
[Aspect 6]
The AlN single crystal according to aspect 3, wherein in a transmission spectrum of the AlN single crystal, an average value of the transmittance in the range of 640 to 660 nm is 3 to 8% pt lower than an average value of the transmittance in the range of 540 to 560 nm.
AlN単結晶
本発明によるAlN単結晶は、AlN単結晶の透過スペクトルにおいて、640~660nmにおける透過率(%)の平均値が、540~560nmにおける透過率(%)の平均値及び780~800nmにおける透過率(%)の平均値の各々よりも低いものである。また、このAlN単結晶は、640~660nmにおける透過率(%)の平均値が780~800nmにおける透過率(%)の平均値よりも5~20パーセントポイント(%pt)低い。このように、AlN単結晶に透過スペクトルにおいて特定の波長域で透過率が一定の割合で低下する特性を持たせることで、研削ないし研磨された際にチッピングが発生しにくいAlN単結晶を提供することができる。したがって、かかるAlN単結晶を研磨等に付することで、AlN単結晶基板を高い歩留まりで製造することができる。すなわち、前述のとおり、AlN単結晶は、その後の研削や研磨によりAlN単結晶の表面を平坦化及び鏡面化することが行われている。しかしながら、従来のAlN単結晶では、研削ないし研磨工程を経た後、AlN単結晶にチッピングが発生しやすいという問題があった。この点、本発明のAlN単結晶によれば、この問題を好都合に解消することができる。 AlN single crystal The AlN single crystal according to the present invention has a lower average transmittance (%) at 640 to 660 nm than the average transmittance (%) at 540 to 560 nm and the average transmittance (%) at 780 to 800 nm in the transmission spectrum of the AlN single crystal. Moreover, the average transmittance (%) at 640 to 660 nm of this AlN single crystal is 5 to 20 percentage points (%pt) lower than the average transmittance (%) at 780 to 800 nm. In this way, by giving the AlN single crystal a characteristic that the transmittance decreases at a constant rate in a specific wavelength range in the transmission spectrum, it is possible to provide an AlN single crystal that is less likely to chip when ground or polished. Therefore, by subjecting such an AlN single crystal to polishing or the like, it is possible to manufacture an AlN single crystal substrate with a high yield. That is, as described above, the surface of the AlN single crystal is flattened and mirror-finished by subsequent grinding or polishing. However, conventional AlN single crystals have a problem in that chipping is likely to occur in the AlN single crystal after undergoing a grinding or polishing process. The AlN single crystal of the present invention can advantageously solve this problem.
ここで、透過スペクトルにおける特定波長域の「透過率の平均値」とは、特定の波長範囲(例えば、540~560nm、640~660nm、780~800nm等のことをいう)において測定した各波長(nm)の透過率(%)の総和を、測定点数で除することによって求める。例えば、540~560nmの領域において1nm刻みで透過率を測定し、それら透過率の総和が1050であった場合に、その透過率の総和を測定点数である21で除することで透過率の平均値(例えば1050/21=50%)を得ることができる。また、このときの透過率は、AlN単結晶の厚さを100μmに換算した場合の透過率T100μmを用いるのが好ましい。これは、仮に測定するAlN単結晶の厚さにばらつきがあると、それにより透過率も変わるためである。例えば、AlN単結晶が厚いと透過率は低くなり、AlN単結晶が薄いと透過率は高くなる。 Here, the "average transmittance" of a specific wavelength region in the transmission spectrum is obtained by dividing the sum of the transmittance (%) of each wavelength (nm) measured in a specific wavelength range (e.g., 540-560 nm, 640-660 nm, 780-800 nm, etc.) by the number of measurement points. For example, if the transmittance is measured at 1 nm intervals in the 540-560 nm region and the sum of the transmittances is 1050, the average transmittance (e.g., 1050/21=50%) can be obtained by dividing the sum of the transmittances by 21, which is the number of measurement points. In addition, it is preferable to use the transmittance T 100 μm when the thickness of the AlN single crystal is converted to 100 μm. This is because if there is variation in the thickness of the AlN single crystal to be measured, the transmittance will also change accordingly. For example, if the AlN single crystal is thick, the transmittance will be low, and if the AlN single crystal is thin, the transmittance will be high.
透過スペクトルにおける透過率は、例えば以下に示す算出方法により求めることができる。AlN単結晶の全光線透過率Taを分光光度計を用いて測定する。Taの測定値及びAlN単結晶の理論透過率Ttを用いてAlN単結晶の吸収係数αを求める。そして、AlN単結晶の厚さを100μmに換算した場合の透過率T100μmを計算する。このとき、α及びT100μmは下記式:
α=-1/t×ln(Ta/Tt)、及び
T100μm=exp(-α/100)
(式中、tはAlN単結晶サンプルの実際の厚さ(cm)を表す)により求めることができる。なお、透過率が低く吸収係数αの算出が困難なAlN単結晶サンプルについては実際の厚さを薄くして全光線透過率Taを測定すればよい。こうして、厚さを100μmに換算した場合の透過率T100μmに基づく透過スペクトルが得られる。
The transmittance in the transmission spectrum can be calculated, for example, by the following calculation method. The total light transmittance T a of the AlN single crystal is measured using a spectrophotometer. The absorption coefficient α of the AlN single crystal is calculated using the measured value of T a and the theoretical transmittance T t of the AlN single crystal. Then, the transmittance T 100 μm is calculated when the thickness of the AlN single crystal is converted to 100 μm. At this time, α and T 100 μm are calculated by the following formula:
α=-1/t×ln(T a /T t ), and T 100μm =exp(-α/100)
(where t represents the actual thickness (cm) of the AlN single crystal sample). For AlN single crystal samples with low transmittance and for which it is difficult to calculate the absorption coefficient α, the actual thickness may be reduced to measure the total light transmittance Ta . In this way, a transmission spectrum based on the transmittance T100 μm converted to a thickness of 100 μm can be obtained.
AlN単結晶の透過スペクトルにおいて、640~660nmにおける透過率の平均値が540~560nmにおける透過率の平均値よりも、1~10%pt低いのが好ましく、3~8%pt低いのがより好ましい。また、AlN単結晶の透過スペクトルにおいて、640~660nmにおける透過率の平均値が780~800nmにおける透過率の平均値よりも5~20%pt低く、6~18%pt低いのが好ましく、8~13%pt低いのがより好ましい。In the transmission spectrum of the AlN single crystal, the average transmittance at 640 to 660 nm is preferably 1 to 10% pt lower, and more preferably 3 to 8% pt lower, than the average transmittance at 540 to 560 nm. In addition, in the transmission spectrum of the AlN single crystal, the average transmittance at 640 to 660 nm is preferably 5 to 20% pt lower, and more preferably 6 to 18% pt lower, and more preferably 8 to 13% pt lower than the average transmittance at 780 to 800 nm.
本発明のAlN単結晶は、透過スペクトルにおいて、540~800nmの波長範囲内に半値幅が50~150nmとなる吸収ピークを有するのが好ましく、より好ましくは半値幅が70~120nmである。この「吸収ピーク」とは、横軸を波長(nm)、縦軸を透過率(%)とした透過スペクトルにおいて、540~800nmの波長範囲内で透過率が極小となる(すなわち吸収率が極大となる)吸収帯を意味し、そのような吸収帯では透過スペクトルの形状が下に凹んでいる形状(例えば谷状)となる。この半値幅は、(i)540~560nmにおける透過率の平均値と780~800nmにおける透過率の平均値のうち小さい方の値をT1とし、640~660nmにおける透過率の平均値をT2としたとき、(ii)T2+(T1-T2)/2から算出される透過率よりも低い透過率を与える波長範囲の幅として定義される。 The AlN single crystal of the present invention preferably has an absorption peak with a half-width of 50 to 150 nm in the wavelength range of 540 to 800 nm in the transmission spectrum, more preferably with a half-width of 70 to 120 nm. The "absorption peak" means an absorption band in which the transmittance is minimal (i.e., the absorbance is maximal) in the wavelength range of 540 to 800 nm in the transmission spectrum with the horizontal axis being wavelength (nm) and the vertical axis being transmittance (%), and in such an absorption band, the shape of the transmission spectrum is concave downward (e.g., valley-like). The half-width is defined as the width of a wavelength range that gives a transmittance lower than the transmittance calculated from (i) T 2 + (T 1 -T 2 )/ 2 , where T 1 is the smaller of the average transmittance in the range of 540 to 560 nm and the average transmittance in the range of 780 to 800 nm, and T 2 is the average transmittance in the range of 640 to 660 nm.
本発明におけるAlN単結晶とは、c軸方向及びa軸方向の両方に配向している配向層であるのが好ましく、モザイク結晶を含んでいてもよい。モザイク結晶とは、明瞭な粒界は有しないが、結晶の配向方位がc軸及びa軸の一方又は両方とわずかに異なる結晶の集まりになっているものをいう。このような配向層は、略法線方向(c軸方向)、及び面内方向(a軸方向)に結晶方位が概ね揃った構成を有している。このような構成とすることで、その上に、優れた品質、特に配向性に優れた半導体層を形成することが可能となる。すなわち、配向層上に半導体層を形成する際、半導体層の結晶方位は配向層の結晶方位に概ね倣ったものとなる。したがって、AlN単結晶上に形成される半導体膜を配向膜としやすい。The AlN single crystal in the present invention is preferably an oriented layer oriented in both the c-axis direction and the a-axis direction, and may contain mosaic crystals. Mosaic crystals are a collection of crystals that do not have clear grain boundaries, but whose orientation direction is slightly different from one or both of the c-axis and a-axis. Such an oriented layer has a configuration in which the crystal orientation is roughly aligned in the approximately normal direction (c-axis direction) and the in-plane direction (a-axis direction). With such a configuration, it is possible to form a semiconductor layer with excellent quality, particularly excellent orientation, thereon. That is, when a semiconductor layer is formed on the oriented layer, the crystal orientation of the semiconductor layer roughly follows the crystal orientation of the oriented layer. Therefore, it is easy to form a semiconductor film formed on the AlN single crystal into an oriented film.
本発明におけるAlN単結晶における、配向性の評価方法は、特に限定されるものではないが、例えばEBSD(Electron Back Scatter Diffraction Patterns)法やX線極点図等の公知の分析手法を用いることができる。例えば、EBSD法を用いる場合、AlN単結晶の表面(板面)又は板面と直交する断面の逆極点図マッピング、結晶方位マッピングを測定する。得られた逆極点図マッピングにおいて、(A)板面の略法線方向の特定方位(第1軸)に配向していること、(B)第1軸に直交する、略板面内方向の特定方位(第2軸)に配向していること、得られた結晶方位マッピングにおいて、(C)第1軸からの傾斜角度が±10°以内に分布していること、(D)第2軸からの傾斜角度が±10°以内に分布していること、という4つの条件を満たすときに略法線方向と略板面方向の2軸に配向していると定義できる。言い換えると、上記4つの条件を満たしている場合に、c軸及びa軸の2軸に配向していると判断できる。例えば板面の略法線方向がc軸に配向している場合、略板面内方向がc軸と直交する特定方位(例えばa軸)に配向していればよい。AlN単結晶は、略法線方向と略板面内方向の2軸に配向していればよいが、略法線方向がc軸に配向していることが好ましい。略法線方向及び/又は略板面内方向の傾斜角度分布は小さい方がAlN単結晶のモザイク性が小さくなり、ゼロに近づくほど完全な単結晶に近くなる。このため、AlN単結晶の結晶性の観点では、傾斜角度分布は略法線方向、略板面方向共に小さいほうが好ましく、例えば±5°以下が好ましく、±3°以下がさらに好ましい。The method for evaluating the orientation of the AlN single crystal in the present invention is not particularly limited, but known analytical methods such as EBSD (Electron Back Scatter Diffraction Patterns) method and X-ray pole figures can be used. For example, when using the EBSD method, inverse pole figure mapping and crystal orientation mapping of the surface (plate surface) or a cross section perpendicular to the plate surface of the AlN single crystal are measured. In the obtained inverse pole figure mapping, (A) the crystal is oriented in a specific direction (first axis) approximately normal to the plate surface, (B) the crystal is oriented in a specific direction (second axis) approximately in the plate surface direction perpendicular to the first axis, and in the obtained crystal orientation mapping, (C) the inclination angle from the first axis is distributed within ±10°, and (D) the inclination angle from the second axis is distributed within ±10°. When these four conditions are satisfied, the crystal orientation can be defined as being oriented in two axes, approximately normal and approximately plate surface directions. In other words, when the above four conditions are satisfied, it can be determined that the crystal is oriented along two axes, the c-axis and the a-axis. For example, when the approximately normal direction of the plate surface is oriented along the c-axis, the approximately in-plane direction of the plate may be oriented along a specific direction (e.g., the a-axis) perpendicular to the c-axis. The AlN single crystal may be oriented along two axes, the approximately normal direction and the approximately in-plane direction, but it is preferable that the approximately normal direction is oriented along the c-axis. The smaller the inclination angle distribution in the approximately normal direction and/or the approximately in-plane direction, the smaller the mosaic property of the AlN single crystal, and the closer it is to zero, the closer it is to a perfect single crystal. Therefore, from the viewpoint of the crystallinity of the AlN single crystal, it is preferable that the inclination angle distribution in both the approximately normal direction and the approximately in-plane direction is small, for example, ±5° or less, and more preferably ±3° or less.
AlN単結晶は、その片面が、好ましくは20cm2以上、より好ましくは70cm2以上、さらに好ましくは170cm2以上の面積を有する。このようにAlN単結晶基板を大面積化することにより、その上に形成する半導体層の大面積化が可能となる。したがって、一枚の半導体層から半導体素子を多数個取りすることが可能となり、製造コストの低減が期待される。大きさの上限は特に限定されるものではないが、典型的には、片面710cm2以下である。 The AlN single crystal has an area of preferably 20 cm2 or more, more preferably 70 cm2 or more, and even more preferably 170 cm2 or more on one side. By increasing the area of the AlN single crystal substrate in this way, it becomes possible to increase the area of the semiconductor layer formed thereon. Therefore, it becomes possible to obtain a large number of semiconductor elements from one semiconductor layer, and a reduction in manufacturing costs is expected. The upper limit of the size is not particularly limited, but is typically 710 cm2 or less on one side.
製造方法
本発明のAlN単結晶は、透過スペクトルにおいて特定の波長域で透過率が所定量低下するAlN単結晶となる限り様々な方法により製造することができる。種基板を用意しその上にエピタキシャル成膜させてもよいし、種基板を用いずに自発核形成によって直接AlN単結晶を製造させてもよい。また、用いる種基板はホモエピタキシャル成長となるようにAlN基板を用いてもよいし、それ以外の基板を用いてヘテロエピタキシャル成長させてもよい。単結晶の成長には気相成膜法、液相成膜法及び固相成膜法のいずれの方法を用いてもよいが、好ましくは気相成膜法を用いてAlN単結晶を成膜し、その後に必要に応じ種基板部分を研削除去することによって、所望の透過スペクトル特性を持つAlN単結晶を得ることが可能である。気相成膜法の例としては、MOVPE(metal organic vapor phase epitaxy)法、各種CVD(化学気相成長)法(例えば熱CVD法やプラズマCVD法等)、スパッタリング法、ハイドライド気相成長(Hydride vapor phase epitaxy:HVPE)法、分子線エピタキシャル(Molecular beam epitaxy:MBE)法、昇華法、及びパルスレーザーデポジション(Pulsed Laser Deposition:PLD)法等が挙げられ、好ましくは昇華法又はHVPE法である。液相成膜法の例としては、溶液成長法(例えばフラックス法)等が挙げられる。また、種基板上に直接AlN単結晶を成膜せずとも、配向前駆体層を形成する工程、熱処理により配向前駆体層をAlN単結晶層とする工程、及び種基板を研削除去する工程によりAlN単結晶を得ることも可能である。その時の配向前駆体層を成膜する製法としてAD(エアロゾルデポジション)法、及びHPPD(超音速プラズマ粒子堆積)法等が挙げられる。 Manufacturing method The AlN single crystal of the present invention can be manufactured by various methods as long as it is an AlN single crystal whose transmittance decreases by a predetermined amount in a specific wavelength range in the transmission spectrum. A seed substrate may be prepared and epitaxially grown thereon, or an AlN single crystal may be directly manufactured by spontaneous nucleation without using a seed substrate. In addition, an AlN substrate may be used as the seed substrate so as to achieve homoepitaxial growth, or a substrate other than the seed substrate may be used for heteroepitaxial growth. Any of the vapor phase film-forming method, liquid phase film-forming method, and solid phase film-forming method may be used for the growth of the single crystal, but it is preferable to use the vapor phase film-forming method to form the AlN single crystal, and then grind and remove the seed substrate portion as necessary, thereby making it possible to obtain an AlN single crystal having the desired transmission spectrum characteristics. Examples of the vapor phase deposition method include MOVPE (metal organic vapor phase epitaxy), various CVD (chemical vapor deposition) methods (such as thermal CVD and plasma CVD), sputtering, hydride vapor phase epitaxy (HVPE), molecular beam epitaxy (MBE), sublimation, and pulsed laser deposition (PLD), among which sublimation or HVPE is preferred. Examples of the liquid phase deposition method include solution growth (such as flux). In addition, even if the AlN single crystal is not directly formed on the seed substrate, it is possible to obtain the AlN single crystal by a process of forming an orientation precursor layer, a process of converting the orientation precursor layer into an AlN single crystal layer by heat treatment, and a process of grinding and removing the seed substrate. Examples of the manufacturing method for forming the orientation precursor layer include the AD (aerosol deposition) method and the HPPD (supersonic plasma particle deposition) method.
製造工程
上述した固相成膜法、気相成膜法及び液相成膜法のいずれの手法も公知の条件を用いることができるが、例えば昇華法を用いてAlN単結晶を作製する手法について、以下に説明する。具体的には、(a)AlN多結晶粉末の熱処理、(b)AlN単結晶層の成膜、並びに(c)種基板の研削除去及びAlN単結晶層表面の研磨により作製される。Although any of the above-mentioned solid phase deposition method, vapor phase deposition method, and liquid phase deposition methods can use known conditions, the following describes a method for producing an AlN single crystal using, for example, a sublimation method. Specifically, the AlN single crystal is produced by (a) heat treatment of an AlN polycrystalline powder, (b) deposition of an AlN single crystal layer, and (c) grinding and removing the seed substrate and polishing the surface of the AlN single crystal layer.
(a)AlN多結晶粉末の熱処理
この工程は、AlN多結晶粉末を熱処理してAlN原料粉末を得る工程である。図1に示されるように、AlN単結晶の原料としてAlN粉末12を窒化ホウ素(BN)製のサヤ10内に配置し、N2雰囲気で熱処理する。この時サヤ10内にAlN粉末12に直接接触しないように黒鉛粉末14を投入したBN製の坩堝16も配置する。このBN坩堝16はサヤ10内に収納可能な大きさである。黒鉛粉末の投入量はAlN粉末100gに対し、0.015~0.130gが好ましく、より好ましくは0.020~0.120gである。黒鉛粉末の投入量が上記範囲内であると、例えば、透過スペクトルにおいて特定の波長域での透過率が所定量低下するAlN単結晶を得ることが可能である。サヤ10の炉内圧力は0.1~10気圧が好ましく、より好ましくは0.5~5気圧である。熱処理温度は2150℃~2300℃が好ましく、より好ましくは2200~2250℃である。
(a) Heat Treatment of AlN Polycrystalline Powder This step is a step of heat treating AlN polycrystalline powder to obtain AlN raw material powder. As shown in FIG. 1, AlN powder 12 is placed in a boron nitride (BN) sheath 10 as a raw material for AlN single crystal, and heat treated in a N2 atmosphere. At this time, a BN crucible 16 containing graphite powder 14 is also placed in the sheath 10 so as not to directly contact the AlN powder 12. This BN crucible 16 is of a size that can be stored in the sheath 10. The amount of graphite powder to be added is preferably 0.015 to 0.130 g, more preferably 0.020 to 0.120 g, per 100 g of AlN powder. When the amount of graphite powder to be added is within the above range, for example, it is possible to obtain an AlN single crystal in which the transmittance in a specific wavelength range in the transmission spectrum is reduced by a predetermined amount. The pressure inside the sheath 10 is preferably 0.1 to 10 atm, more preferably 0.5 to 5 atm. The heat treatment temperature is preferably 2150°C to 2300°C, and more preferably 2200°C to 2250°C.
(b)AlN単結晶層の成膜
この工程は、結晶成長装置内にて種基板上にAlN単結晶を成膜する工程である。昇華法で用いられる結晶成長装置の一例を図2に示す。図2に示される成膜装置20は、坩堝22と、坩堝22を断熱するための断熱材24と、坩堝22を高温に加熱するコイル26とを備えている。坩堝22は、その下部にAlN原料粉末28を含み、上部にAlN原料粉末28の昇華物を析出させる種基板30を備える。坩堝22内をN2雰囲気下で加圧し、コイル26で坩堝22を加熱してAlN原料粉末28を昇華させる。圧力は10~100kPaが好ましく、より好ましくは20~90kPaである。このとき、坩堝22の下部におけるAlN原料粉末28付近の温度よりも、坩堝22の上部における種基板30付近の温度が低くなるように温度勾配をつける。例えば、坩堝22のAlN原料粉末28付近の部分を1900~2250℃に加熱するのが好ましく、より好ましくは2000~2200℃であり、坩堝22の種基板30付近の部分を1400~2150℃に加熱するのが好ましく、より好ましくは1500~2050℃である。このとき、AlN原料粉末28付近の部分に対して種基板30付近の部分の温度を100~500℃低くするのが好ましく、より好ましくは200~400℃である。上記加熱は2~100時間保持するのが好ましく、より好ましくは4~90時間である。温度管理は、坩堝22を覆った断熱材24の穴を介して、放射温度計(図示せず)で坩堝22の上下部の温度を測定し、温度調節にフィードバックすることにより行うことができる。こうして、種基板30としてSiC単結晶を配置し、その表面上にAlNを再析出させAlN単結晶層32を形成することができる。
(b) Deposition of AlN single crystal layer This step is a step of depositing an AlN single crystal on a seed substrate in a crystal growth apparatus. An example of a crystal growth apparatus used in the sublimation method is shown in FIG. 2. The deposition apparatus 20 shown in FIG. 2 includes a crucible 22, a heat insulating material 24 for insulating the crucible 22, and a coil 26 for heating the crucible 22 to a high temperature. The crucible 22 includes an AlN raw material powder 28 in its lower portion, and a seed substrate 30 on which a sublimate of the AlN raw material powder 28 is deposited in its upper portion. The inside of the crucible 22 is pressurized under an N2 atmosphere, and the crucible 22 is heated by the coil 26 to sublimate the AlN raw material powder 28. The pressure is preferably 10 to 100 kPa, more preferably 20 to 90 kPa. At this time, a temperature gradient is provided so that the temperature in the vicinity of the seed substrate 30 in the upper part of the crucible 22 is lower than the temperature in the vicinity of the AlN raw material powder 28 in the lower part of the crucible 22. For example, the portion of the crucible 22 in the vicinity of the AlN raw material powder 28 is preferably heated to 1900 to 2250°C, more preferably 2000 to 2200°C, and the portion of the crucible 22 in the vicinity of the seed substrate 30 is preferably heated to 1400 to 2150°C, more preferably 1500 to 2050°C. At this time, the temperature of the portion in the vicinity of the seed substrate 30 is preferably lower by 100 to 500°C, more preferably 200 to 400°C, relative to the portion in the vicinity of the AlN raw material powder 28. The heating is preferably maintained for 2 to 100 hours, more preferably 4 to 90 hours. Temperature control can be performed by measuring the temperatures of the upper and lower parts of the crucible 22 with a radiation thermometer (not shown) through holes in the heat insulating material 24 covering the crucible 22 and feeding the measured temperatures back to the temperature adjustment. In this manner, a SiC single crystal is placed as the seed substrate 30, and AlN is reprecipitated on the surface thereof to form an AlN single crystal layer 32.
(c)種基板の研削除去及びAlN単結晶層表面の研磨
この工程は、種基板を研削除去しAlN単結晶層を露出させる研削工程、及びAlN単結晶表面の不規則性や欠陥を除去する研磨工程を含む。SiC基板を種基板として用いて上記(a)及び(b)の工程を経て作製したAlN単結晶層には、SiC単結晶が残留するため、研削加工を施して配向層の表面を露出させる。また、成膜後のAlN単結晶層表面を鏡面加工するため、ダイヤモンド砥粒を用いたラップ加工により板面を平滑化した後に、コロイダルシリカ等を用いた化学機械的研磨(CMP)等により研磨する。こうして、AlN単結晶を作製することができる。
(c) Grinding the seed substrate and polishing the surface of the AlN single crystal layer This process includes a grinding process for grinding the seed substrate to expose the AlN single crystal layer, and a polishing process for removing irregularities and defects on the AlN single crystal surface. Since the AlN single crystal layer produced through the above steps (a) and (b) using a SiC substrate as the seed substrate still has SiC single crystals remaining, the surface of the orientation layer is exposed by grinding. In addition, in order to mirror-finish the surface of the AlN single crystal layer after film formation, the plate surface is smoothed by lapping using diamond abrasive grains, and then polished by chemical mechanical polishing (CMP) using colloidal silica or the like. In this way, the AlN single crystal can be produced.
昇華法以外の方法として、HVPE法を用いてAlN単結晶を作製する手法について、以下に説明する。具体例として、(d)種基板上へのAlN単結晶層の成膜、(e)種基板の研削除去、(f)AlN単結晶層の熱処理、及び(g)AlN単結晶層表面の研磨にて作製される。As a method other than the sublimation method, a method for producing AlN single crystals using the HVPE method is described below. As a specific example, it is produced by (d) forming an AlN single crystal layer on a seed substrate, (e) grinding off the seed substrate, (f) heat treating the AlN single crystal layer, and (g) polishing the surface of the AlN single crystal layer.
(d)種基板上へのAlN単結晶層の成膜
この工程は、種基板上にAlN単結晶層を成膜する工程である。図3にHVPE法を用いた気相成長装置を示す。HVPE法を用いた気相成長装置は、反応炉40と、成膜用下地基板42を載置するサセプタ44と、キャリアガス供給源46と、Al原料供給源48とAl原料供給源48内に配置された金属Al粉末原料50と、ヒーター52と、ガス排出部54を備えている。成膜用下地基板42としてSiC基板を用いるのが好ましい。サセプタ44上に基板42を配置し、加熱したAl原料供給源48にHClガスを供給することで得るAlCl3ガスと、キャリアガス供給源46からのNH3ガスとを、混合して成膜用下地基板42に供給する。このとき、Al原料供給源48の加熱温度は500~700℃が好ましく、より好ましくは550~650℃である。また、AlCl3ガスとNH3ガスとの流量比は1:1~1:500が好ましく、より好ましくは1:10~1:200である。反応炉40内の圧力は1~100Torrが好ましく、より好ましくは10~30Torrである。成長温度は1100~1400℃が好ましく、より好ましくは1150~1250℃である。
(d) Deposition of AlN single crystal layer on seed substrate This step is a step of depositing an AlN single crystal layer on a seed substrate. FIG. 3 shows a vapor phase growth apparatus using the HVPE method. The vapor phase growth apparatus using the HVPE method includes a reactor 40, a susceptor 44 on which a base substrate 42 for film formation is placed, a carrier gas supply source 46, an Al source supply source 48, a metal Al powder source 50 disposed in the Al source supply source 48, a heater 52, and a gas exhaust section 54. It is preferable to use a SiC substrate as the base substrate 42 for film formation. The substrate 42 is placed on the susceptor 44, and AlCl 3 gas obtained by supplying HCl gas to the heated Al source supply source 48 and NH 3 gas from the carrier gas supply source 46 are mixed and supplied to the base substrate 42 for film formation. At this time, the heating temperature of the Al source supply source 48 is preferably 500 to 700°C, more preferably 550 to 650°C. The flow rate ratio of AlCl3 gas to NH3 gas is preferably 1:1 to 1:500, more preferably 1:10 to 1:200. The pressure in the reaction furnace 40 is preferably 1 to 100 Torr, more preferably 10 to 30 Torr. The growth temperature is preferably 1100 to 1400°C, more preferably 1150 to 1250°C.
(e)種基板の研削除去
この工程は、種基板を研削除去しAlN単結晶層を露出させる研削工程である。SiC基板を種基板として用いて上記(d)の工程を経て作製したAlN単結晶層には、SiC単結晶が残留するため、研削加工を施して配向層の表面を露出させる。
(e) Grinding and Removing the Seed Substrate This is a grinding step in which the seed substrate is ground and removed to expose the AlN single crystal layer. Since the AlN single crystal layer produced through the above step (d) using the SiC substrate as the seed substrate still has SiC single crystal remaining, the surface of the orientation layer is exposed by grinding.
(f)AlN単結晶層の熱処理
AlN単結晶を、黒鉛粉末とともにBN製のサヤ内に配置しN2雰囲気で熱処理する。この時、炉内圧力は0.1~10気圧が好ましく、より好ましくは0.5~5気圧である。熱処理温度は2150℃~2300℃が好ましく、より好ましくは2200~2250℃である。
(f) Heat treatment of the AlN single crystal layer The AlN single crystal is placed in a BN sheath together with graphite powder and heat treated in a N2 atmosphere. At this time, the pressure inside the furnace is preferably 0.1 to 10 atm, more preferably 0.5 to 5 atm. The heat treatment temperature is preferably 2150°C to 2300°C, more preferably 2200 to 2250°C.
(g)AlN単結晶層表面の研磨
この工程は、AlN単結晶層表面を鏡面加工する研磨工程である。熱処理後のAlN単結晶層表面を鏡面加工するために、ダイヤモンド砥粒を用いたラップ加工により板面を平滑化した後に、コロイダルシリカ等を用いた化学機械的研磨(CMP)等により研磨する。こうして、AlN単結晶基板を作製することができる。
(g) Polishing the surface of the AlN single crystal layer This is a polishing process for mirror-finishing the surface of the AlN single crystal layer. In order to mirror-finish the surface of the AlN single crystal layer after the heat treatment, the plate surface is smoothed by lapping using diamond abrasive grains, and then polished by chemical mechanical polishing (CMP) using colloidal silica or the like. In this way, the AlN single crystal substrate can be produced.
本発明を以下の例によってさらに具体的に説明する。The present invention will be further illustrated by the following examples.
例1
(1)AlN単結晶の作製
(1a)AlN多結晶粉末の熱処理
図1に示されるように、BNサヤ10内にて、AlN単結晶の原料として用いる市販のAlN粉末12(トクヤマAlN粉末、Fグレード)を配置し、AlN粉末12に直接触れないように市販の黒鉛粉末14(SECカーボン製黒鉛粉末、SGPグレード)を投入したBN坩堝16を配置した。このBN坩堝16はサヤ10内に収納可能な大きさである。このBNサヤ10を黒鉛ヒーター炉内にて、N2雰囲気中で0.1~10気圧で2200℃で熱処理した。この時、黒鉛粉末はAlN粉末100gに対し0.052gの割合で投入した。こうして、AlN多結晶粉末を熱処理してAlN原料粉末を作製した。 Example 1
(1) Preparation of AlN single crystals (1a) Heat treatment of AlN polycrystalline powder As shown in FIG. 1, a commercially available AlN powder 12 (Tokuyama AlN powder, F grade) used as a raw material for AlN single crystals was placed in a BN sheath 10, and a BN crucible 16 containing commercially available graphite powder 14 (graphite powder made by SEC Carbon, SGP grade) was placed so as not to directly touch the AlN powder 12. This BN crucible 16 is large enough to be stored in the sheath 10. This BN sheath 10 was heat treated at 2200° C. in a N 2 atmosphere at 0.1 to 10 atm in a graphite heater furnace. At this time, the graphite powder was added at a ratio of 0.052 g per 100 g of AlN powder. In this way, the AlN polycrystalline powder was heat treated to prepare an AlN raw material powder.
(1b)AlN単結晶層の成膜
図2に示されるように、結晶成長容器として坩堝22を用い、この坩堝内にて、基材(種基板)30としてSiC基板を設置し、これと接触しないように上記(1a)で作製したAlN原料粉末28を入れた。坩堝22をN2雰囲気下で50kPaで加圧し、高周波誘導加熱により坩堝22内のAlN原料粉末28付近の部分を2100℃に加熱する一方で坩堝22内のSiC基板30付近の部分をそれよりも低い温度(温度差が200℃)に加熱して保持することにより、SiC基板30上にAlN単結晶層32を再析出させた。保持時間は10時間とした。
(1b) Formation of AlN single crystal layer As shown in Fig. 2, a crucible 22 was used as a crystal growth container, and a SiC substrate was placed in the crucible as a base material (seed substrate) 30, and the AlN raw material powder 28 prepared in (1a) above was placed in the crucible so as not to come into contact with the SiC substrate. The crucible 22 was pressurized at 50 kPa in a N2 atmosphere, and the portion in the crucible 22 near the AlN raw material powder 28 was heated to 2100°C by high-frequency induction heating, while the portion in the crucible 22 near the SiC substrate 30 was heated to a lower temperature (temperature difference of 200°C) and held at that temperature, thereby re-precipitating an AlN single crystal layer 32 on the SiC substrate 30. The holding time was 10 hours.
(1c)SiC基板の研削除去及びAlN単結晶層表面の研磨
上記(1b)で得られた、AlNが再析出したSiC基板をAlN単結晶が露出するまで、#2000までの番手の砥石を用いて研削した後、ダイヤモンド砥粒を用いたラップ加工により、板面をさらに平滑化した。その後、板面に対してコロイダルシリカを用いた化学機械的研磨(CMP)により鏡面仕上げを施した。こうして、AlN単結晶を作製した。
(1c) Grinding and Removal of SiC Substrate and Polishing of AlN Single Crystal Layer Surface The SiC substrate on which AlN was reprecipitated obtained in (1b) above was ground using a grindstone with a grit size of up to #2000 until the AlN single crystal was exposed, and then the plate surface was further smoothed by lapping using diamond abrasive grains. After that, the plate surface was mirror-finished by chemical mechanical polishing (CMP) using colloidal silica. In this way, an AlN single crystal was produced.
(2)AlN単結晶の評価
(2a)EBSD測定
AlN単結晶の表面及び裏面でEBSD測定を実施したところ、AlN結晶がc軸方向及びa軸方向の両方に配向していることが分かった。
(2) Evaluation of AlN Single Crystal (2a) EBSD Measurement EBSD measurements were performed on the front and back surfaces of the AlN single crystal, and it was found that the AlN crystal was oriented in both the c-axis and a-axis directions.
(2b)透過スペクトル
AlN単結晶について200~800nmの波長域を含む全光線透過率Taを分光光度計(日立ハイテクサイエンス製、UH4150)を用いて測定した。Taの測定値及びAlN単結晶の理論透過率Ttを用いてAlN単結晶の吸収係数αを求めた後に、AlN単結晶の厚さを100μmに換算した場合の透過率T100μmを計算した。α及びT100μmは下記式:
α=-1/t×ln(Ta/Tt)、及び
T100μm=exp(-α/100)
(式中、tはAlN単結晶サンプルの実際の厚さ(cm)を表す)
により求めた。こうして、厚さを100μmに換算した場合の透過率T100μmに基づく透過スペクトルを得た。得られた透過スペクトルに基づき、640~660nmにおける透過率(%)の平均値の540~560nmにおける透過率(%)の平均値に対する差(%pt)(以下、Δ(Tav640-660-Tav540-560)と称する)、及び640~660nmにおける透過率(%)の平均値の780~800nmにおける透過率(%)の平均値に対する差(%pt)(以下、Δ(Tav640-660-Tav540-560)と称する)を算出した。また、540~800nmの波長範囲内において、吸収ピークの半値幅(nm)を求めた。この半値幅は、(i)540~560nmにおける透過率(%)の平均値と780~800nmにおける透過率(%)の平均値のうち小さい方の値をT1と決定し、かつ、640~660nmにおける透過率(%)の平均値をT2と決定した上で、(ii)式:T2+(T1-T2)/2から算出される透過率よりも低い透過率を与える波長範囲の幅を透過スペクトルから読み取ることにより決定した。結果を表1に示す。
(2b) Transmission spectrum The total light transmittance T a of the AlN single crystal, including the wavelength range of 200 to 800 nm, was measured using a spectrophotometer (UH4150, manufactured by Hitachi High-Tech Science). After determining the absorption coefficient α of the AlN single crystal using the measured value of T a and the theoretical transmittance T t of the AlN single crystal, the transmittance T 100 μm was calculated when the thickness of the AlN single crystal was converted to 100 μm. α and T 100 μm are expressed by the following formula:
α=-1/t×ln(T a /T t ), and T 100μm =exp(-α/100)
(where t represents the actual thickness (cm) of the AlN single crystal sample)
It was obtained by. In this way, a transmission spectrum based on the transmittance T 100 μm when the thickness was converted to 100 μm was obtained. Based on the obtained transmission spectrum, the difference (%pt) of the average value of the transmittance (%) at 640 to 660 nm to the average value of the transmittance (%) at 540 to 560 nm (hereinafter referred to as Δ(T av640-660 -T av540-560 )) and the difference (%pt) of the average value of the transmittance (%) at 640 to 660 nm to the average value of the transmittance (%) at 780 to 800 nm (hereinafter referred to as Δ(T av640-660 -T av540-560 )) were calculated. In addition, the half-width (nm) of the absorption peak was obtained in the wavelength range of 540 to 800 nm. This half-width was determined by (i) determining the smaller of the average transmittance (%) from 540 to 560 nm and the average transmittance (%) from 780 to 800 nm as T1 , and determining the average transmittance (%) from 640 to 660 nm as T2 , and then (ii) reading from the transmission spectrum the width of the wavelength range that gives a transmittance lower than the transmittance calculated from the formula: T2 + ( T1 - T2 )/2. The results are shown in Table 1.
(2c)チッピングの確認
上記(1c)にて研削及び研磨した後のAlN単結晶の表面を光学顕微鏡にて観察し、最大の長さが50μm以上の欠け及びクラックをチッピングとみなして、そのチッピングの有無を確認した。上記(1)と同様の方法で合計10個のAlN単結晶を作製し、そのうち何個のAlN単結晶にチッピングが発生するかを確認し、以下に示す評価基準にて格付け評価を行った。結果を表1に示す。
<評価基準>
‐評価A:チッピングが無かったAlN単結晶基板が9~10個
‐評価B:チッピングが無かったAlN単結晶基板が6~8個
‐評価C:チッピングが無かったAlN単結晶基板が3~5個
‐評価D:全てのAlN単結晶基板にチッピングが見られた
(2c) Confirmation of chipping The surface of the AlN single crystal after grinding and polishing in (1c) above was observed with an optical microscope, and the presence or absence of chipping was confirmed, regarding chips and cracks with a maximum length of 50 μm or more as chipping. A total of 10 AlN single crystals were produced in the same manner as in (1) above, and it was confirmed how many of them had chipping, and a rating evaluation was performed according to the evaluation criteria shown below. The results are shown in Table 1.
<Evaluation criteria>
- Evaluation A: 9 to 10 AlN single crystal substrates were free of chipping. - Evaluation B: 6 to 8 AlN single crystal substrates were free of chipping. - Evaluation C: 3 to 5 AlN single crystal substrates were free of chipping. - Evaluation D: Chips were observed on all AlN single crystal substrates.
例2~6
上記(1a)において、AlN多結晶粉末の熱処理時の黒鉛粉末投入量を表1に示される量としたこと以外は、例1と同様にAlN単結晶を作製し、評価した。また、AlN単結晶の表面及び裏面でEBSD測定を実施したところ、AlN結晶がc軸方向及びa軸方向の両方に配向していることが分かった。結果を表1に示す。 Examples 2 to 6
In the above (1a), an AlN single crystal was produced and evaluated in the same manner as in Example 1, except that the amount of graphite powder added during the heat treatment of the AlN polycrystalline powder was the amount shown in Table 1. In addition, when EBSD measurements were performed on the front and back surfaces of the AlN single crystal, it was found that the AlN crystal was oriented in both the c-axis direction and the a-axis direction. The results are shown in Table 1.
例7及び8(比較)
上記(1a)において、AlN多結晶粉末の熱処理時の黒鉛粉末投入量を表1に示される量としたこと以外は、例1と同様にAlN単結晶を作製し、評価した。また、AlN単結晶の表面及び裏面でEBSD測定を実施したところ、AlN結晶がc軸方向及びa軸方向の両方に配向していることが分かった。結果を表1に示す。 Examples 7 and 8 (Comparative)
In the above (1a), an AlN single crystal was produced and evaluated in the same manner as in Example 1, except that the amount of graphite powder added during the heat treatment of the AlN polycrystalline powder was the amount shown in Table 1. In addition, when EBSD measurements were performed on the front and back surfaces of the AlN single crystal, it was found that the AlN crystal was oriented in both the c-axis direction and the a-axis direction. The results are shown in Table 1.
例9(比較)
上記(1a)の工程を経ずに、市販のAlN粉末(トクヤマAlN粉末、Fグレード)をAlN原料粉末として用いたこと以外は、例1と同様にAlN単結晶を作製し、評価した。また、AlN単結晶の表面及び裏面でEBSD測定を実施したところ、AlN結晶がc軸方向及びa軸方向の両方に配向していることが分かった。結果を表1に示す。 Example 9 (Comparison)
An AlN single crystal was produced and evaluated in the same manner as in Example 1, except that the above step (1a) was not carried out and a commercially available AlN powder (Tokuyama AlN powder, F grade) was used as the AlN raw material powder. In addition, EBSD measurements were carried out on the front and back surfaces of the AlN single crystal, and it was found that the AlN crystal was oriented in both the c-axis direction and the a-axis direction. The results are shown in Table 1.
Claims (6)
前記半値幅は、(i)540~560nmにおける透過率の平均値と780~800nmにおける透過率の平均値のうち小さい方の値をT1とし、640~660nmにおける透過率の平均値をT2としたとき、(ii)T2+(T1-T2)/2から算出される透過率よりも低い透過率を与える波長範囲の幅として定義される、請求項1に記載のAlN単結晶。 In the transmission spectrum of the AlN single crystal, there is an absorption peak with a half-width of 50 to 150 nm within a wavelength range of 540 to 800 nm,
The AlN single crystal according to claim 1 , wherein the half-width is defined as (i) the width of a wavelength range that gives a transmittance lower than the transmittance calculated from T2 + ( T1 - T2)/ 2 , where T1 is the smaller of the average transmittance in the range of 540 to 560 nm and the average transmittance in the range of 780 to 800 nm, and T2 is the average transmittance in the range of 640 to 660 nm.
4. The AlN single crystal according to claim 3, wherein in a transmission spectrum of the AlN single crystal, an average value of the transmittance in the range of 640 to 660 nm is lower by 3 to 8% pt than an average value of the transmittance in the range of 540 to 560 nm.
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| LIN, Yung-Hsin et al.,Optical properties of high transmittance aluminum oxynitride thin films for spectral range from near,Optical Review,2009年,Vol.16 No.3,pp. 400-403 |
| 熊谷 義直, 深紫外光透過性発現メカニズム解明による実用的バルク窒化アルミニウム結晶の創出,科学研究費助成事業 研究成果報告書,日本,2015年 |
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