JPH01215014A - Growth of semiconductor crystal - Google Patents

Growth of semiconductor crystal

Info

Publication number
JPH01215014A
JPH01215014A JP3955588A JP3955588A JPH01215014A JP H01215014 A JPH01215014 A JP H01215014A JP 3955588 A JP3955588 A JP 3955588A JP 3955588 A JP3955588 A JP 3955588A JP H01215014 A JPH01215014 A JP H01215014A
Authority
JP
Japan
Prior art keywords
gas
growth
substrate
growth container
semiconductor
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP3955588A
Other languages
Japanese (ja)
Inventor
Yasuto Kawahisa
川久 慶人
Masahiro Sasaki
正洋 佐々木
Masao Mashita
真下 正夫
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Toshiba Corp filed Critical Toshiba Corp
Priority to JP3955588A priority Critical patent/JPH01215014A/en
Publication of JPH01215014A publication Critical patent/JPH01215014A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To realize a high quality epitaxial growth layer at a low temperature by projecting light onto the raw gas or the substrate on which the layer grows in a compound semiconductor or a mixed crystal semiconductor of which composition element is (N). CONSTITUTION:After a substrate 6 is placed in a growth container 1, the interior of the growth container 1 is discharged to high vacuum through an exhaust system 4. Then hydrogen gas is introduced into the growth container 1 from a gas introduction port 3 and the exhaust rate of the exhaust system 4 is adjusted to set the pressure in the growth container 1 to a fixed value. Then the substrate 6 is heated and when a fixed temperature is attained, raw gas of trimethylgallium and carrier gas of hydrogen gas and hydrogen diluted NH gas are introduced into the growth container from the gas introduction port 2. Similar to this gas introduction, a laser beam 10 from an excimer laser 9 is projected vertically onto the substrate 6. Dissociation, surface reaction and surface migration of supplied material of (N) are promoted in this way, thus allowing a high quality semiconductor crystal layer to grow.

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は、窒素を構成元素として有する化合物半導体ま
たは混晶半導体の気相成長法に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a method for vapor phase growth of a compound semiconductor or a mixed crystal semiconductor having nitrogen as a constituent element.

(従来の技術) 窒素を構成元素として有する化合物半導体および混晶半
導体は、光、電子デバイス材料として注目される0例え
ばGaNは直接遷移型でかつ室温において大きなバンド
ギャップを有することから、緑色レーザ等の短波長レー
ザ用材料として期待され、またGaAsやInPのMI
SF[Tデバイスに必要とされる良好な表面制御が可能
な絶縁層材料としても期待されている。 GaNよりも
さらにバンドキャップエネルギーが大きいANNは、前
述のMISFETデバイスの絶縁層材料の他、 SAW
デバイス材料としても期待される。
(Prior Art) Compound semiconductors and mixed crystal semiconductors having nitrogen as a constituent element are attracting attention as optical and electronic device materials.For example, GaN is a direct transition type and has a large band gap at room temperature, so it is used for green lasers, It is expected to be used as a material for short wavelength lasers in
It is also expected to be used as an insulating layer material that allows for the good surface control required for SF[T devices. ANN, which has even higher bandgap energy than GaN, can be used as an insulating layer material for MISFET devices as well as SAW.
It is also expected to be used as a device material.

これらNttW成元素に有する化合物半導体あるいは混
晶半導体のエピタキシャル成長方としては。
As for the epitaxial growth method of compound semiconductors or mixed crystal semiconductors having these NttW constituent elements.

N113(アンモニア)をNtM料に用いた。クロライ
ド気相成長法や、有機金属気相成長が用いられている。
N113 (ammonia) was used as the NtM charge. Chloride vapor phase epitaxy and organometallic vapor phase epitaxy are used.

しかし、Ni13 の原料分解温度が高いために、成長
温度が700℃以上と高く、そのため成分元素による欠
陥1例えば原子空孔等が発生し良質な結晶が得られない
ことや、自己補償効果により1例えばGaNにおいては
p型結晶が得られないという問題があった。成長温度の
低減化を計る方法として電子サイクロトロン共鳴(EC
R)励起による成長法があるが、イオン衝撃による欠陥
が成長結晶内部に誘起され、良好な結晶が得られていな
い。
However, because the raw material decomposition temperature of Ni13 is high, the growth temperature is as high as 700°C or higher, and as a result, defects 1, such as atomic vacancies, occur due to component elements, making it difficult to obtain high-quality crystals. For example, in GaN, there is a problem that a p-type crystal cannot be obtained. Electron cyclotron resonance (EC) is a method to reduce the growth temperature.
R) There is a growth method using excitation, but defects are induced inside the growing crystal due to ion bombardment, and good crystals cannot be obtained.

(発明が解決しようとする課!fi) 以上の様に従来の成長温度の高い気相成長法や。(The problem that the invention tries to solve!fi) As mentioned above, conventional vapor phase growth methods with high growth temperatures.

イオンを用いた成長法では、原子空孔等の結晶欠陥が多
く存在し、Nを構成元素に一有する化合物半導体あるい
は混晶半導体においては、良好なエピタキシャル成長層
を得るのが難しいという問題点があった。
Growth methods using ions have the problem that many crystal defects such as atomic vacancies exist, and it is difficult to obtain good epitaxial growth layers in compound semiconductors or mixed crystal semiconductors that contain N as one of the constituent elements. Ta.

本発明は、この様な問題点を解決し、Nを構成元素とす
る化合物半導体あるいは混晶半導体において、低温で良
質のエビキシャル成長層を得ることを可能とした気相成
長法を提供することを目的とする。
The present invention aims to solve these problems and provide a vapor phase growth method that makes it possible to obtain a high-quality epitaxial growth layer at low temperatures in a compound semiconductor or a mixed crystal semiconductor containing N as a constituent element. purpose.

(発明の構成〕 (課題を解決するための手段) 本発明は、原料ガスあるいは、被成長基板に光を照射し
て気相成長を行なうことを特徴とする。
(Structure of the Invention) (Means for Solving the Problems) The present invention is characterized in that vapor phase growth is performed by irradiating a source gas or a substrate to be grown with light.

(作 用) この様な気相成長法(光励起気相成長法)を用いれば、
Nの供給Jjπ料であるN113やN、I+、あるいは
Nを含む有機化合物の解離が光化学反応により促進され
、かつ被成長基板表面上での成長反応や反応種の表面泳
動が光照射により促進され従来より低温で、良質な半導
体結晶層を得ることができる。
(Function) If such a vapor phase growth method (photoexcited vapor phase growth method) is used,
The dissociation of N113, N, I+, or an organic compound containing N, which is the N supply Jjπ material, is promoted by a photochemical reaction, and the growth reaction and surface migration of reactive species on the surface of the growth substrate are promoted by light irradiation. A high-quality semiconductor crystal layer can be obtained at a lower temperature than before.

(実施例) 以下、本発明の実施例としてGaNを結晶層をAら0.
(サファイヤ)6面基板上に成長した例を図面を参照し
て説明する。
(Example) Hereinafter, as an example of the present invention, a GaN crystal layer is formed from A0.
(Sapphire) An example grown on a six-sided substrate will be described with reference to the drawings.

第1図は、光励起気相成長を行う成長装置である成長容
器1には、 AQ、0.(サファイア)0面基板6がサ
セプタ5上に設置されて収容されている。
FIG. 1 shows that a growth vessel 1, which is a growth apparatus for performing photoexcited vapor phase growth, has AQ, 0. A (sapphire) zero-plane substrate 6 is installed and housed on the susceptor 5.

サセプタ5上の基板6は図示しないヒータにより加熱さ
れ、基板6は所定温度に設定される。成長容器1にはガ
ス導入口2および3が設けられている。ガス導入口2よ
り■族原料および■族〃バ料が、キャリアガス(主とし
て水素ガス)と共に成長容器1内に導入される。基板6
にはエキシマレーザ9からのレーザ光lOが反射ミラー
8と合成石英製光導入窓7を介して照射される。ガス導
入口3からは光導入窓への膜形成を抑制するために、水
素ガスあるいは不活性ガスが成長容器1内へ導入される
様になっている。ガス導入口2および3から容器1に導
入されたガスを排気する排気系4の排気速度を調整する
ことにより、成長容器1内の圧力は所定値に設定される
The substrate 6 on the susceptor 5 is heated by a heater (not shown), and the substrate 6 is set to a predetermined temperature. The growth container 1 is provided with gas inlets 2 and 3. The Group 1 raw material and the Group 2 bar material are introduced into the growth container 1 through the gas inlet 2 together with a carrier gas (mainly hydrogen gas). Board 6
A laser beam lO from an excimer laser 9 is applied via a reflection mirror 8 and a light introduction window 7 made of synthetic quartz. Hydrogen gas or inert gas is introduced into the growth container 1 from the gas inlet 3 in order to suppress film formation on the light introduction window. By adjusting the exhaust speed of the exhaust system 4 that exhausts the gas introduced into the container 1 from the gas introduction ports 2 and 3, the pressure inside the growth container 1 is set to a predetermined value.

この様な成長装置を用いて行なったGaN結晶層のエビ
タキャル成長につき、具体的に次に説明する。at族原
料ガスとしてトリメチルガリウム(Ga(CI+、 )
3 )  を、またそのキャリアガスとして水素を用い
た。■族原料ガスとしてアンモニア(Ni13)を用い
た。基板6を成長容器1内に収容した後、排気系4によ
り、成長容器1内をI X 10−’Torr以下の高
真空に排気した。その後ガス導入口3より水素ガスを成
長容器1内に4008CCM導入し、排気系4の排気速
度を調整して成長して成長容器1内の圧力を10.0T
orrに設定した。その後基板6を加熱し、400℃に
設定した基板6が400℃になった後、ガス導入口2よ
りトリメチルガリウムを0.453CCM、キャリアガ
スである水素ガスをIO3ccM、 10%水素希釈N
H,ガスを4505CCM(NH3流量45SCCM 
)成長容器内に導入した。ガス導入口2より前記原料ガ
スおよび水素ガスを成長容器内に導入すると同様に、エ
キシマレーザ9からのレーザ光10を基板6上に垂直に
照射した。用いたレーザ光10は、波長193n−のA
rFエキシマレーザである、照射エネルギーは基板6表
面上で1パルス当り5+aj/Jとなるように照射した
。パルス照射の繰り返し数は80ppsである。なお、
成長圧力および成長温度は、それぞれ1OTorrおよ
び400℃とした。
Evital growth of a GaN crystal layer using such a growth apparatus will be specifically described below. Trimethylgallium (Ga(CI+, )
3) and hydrogen was used as the carrier gas. Ammonia (Ni13) was used as the Group (2) raw material gas. After the substrate 6 was placed in the growth container 1, the inside of the growth container 1 was evacuated to a high vacuum of I.times.10-' Torr or less by the exhaust system 4. After that, 4008 CCM of hydrogen gas is introduced into the growth container 1 from the gas inlet 3, and the exhaust speed of the exhaust system 4 is adjusted to grow, and the pressure inside the growth container 1 is raised to 10.0T.
It was set to orr. After that, the substrate 6 was heated, and after the temperature of the substrate 6 which was set at 400°C reached 400°C, 0.453 CCM of trimethyl gallium was added from the gas inlet 2, IO3 ccM of hydrogen gas as a carrier gas, and 10% hydrogen diluted N.
H, gas 4505CCM (NH3 flow rate 45SCCM
) was introduced into the growth vessel. In the same way as the source gas and hydrogen gas were introduced into the growth container through the gas inlet 2, the substrate 6 was irradiated with laser light 10 from an excimer laser 9 perpendicularly. The laser beam 10 used was A with a wavelength of 193n-
An rF excimer laser was used to irradiate the surface of the substrate 6 with irradiation energy of 5+aj/J per pulse. The number of repetitions of pulse irradiation was 80 pps. In addition,
The growth pressure and growth temperature were 1OTorr and 400°C, respectively.

このようにして成長させたGaN結晶層の評価を電子線
回折およびX線2結晶法により行なった。
The GaN crystal layer grown in this manner was evaluated by electron beam diffraction and X-ray two-crystal method.

電子線回折パターンはスト−リーク状であり平担で良質
な結晶層が成長していることがわかった。
The electron beam diffraction pattern was streak-like, indicating that a flat, high-quality crystal layer had grown.

またX線2結晶法の回折パターンよりまとまる半値幅は
、従来の光照射を行なわない高温(700℃以上)気相
成長法のものよりも狭かった。
Further, the half-width obtained from the diffraction pattern of the X-ray two-crystal method was narrower than that of the conventional high temperature (700° C. or higher) vapor phase growth method without light irradiation.

上記実施例では、レーザ照射強度を基板表面上で1パル
ス当り5mj/c+Jとしたが、これは基板が溶接しな
いエネルギーであれば良い、また照射する光は他の波長
のエキシマレーザ光1例えばKrF光(波長248nm
)、 XeF (波長350nm)でも良いし低圧、高
圧あるいは超高圧11gランプ、X5−11gランプ。
In the above example, the laser irradiation intensity was set to 5 mj/c+J per pulse on the substrate surface, but this may be sufficient as long as the energy does not cause welding of the substrate.The irradiating light may be an excimer laser beam of other wavelengths, such as KrF. Light (wavelength 248nm
), XeF (wavelength 350 nm), low pressure, high pressure or ultra-high pressure 11g lamp, X5-11g lamp.

重水素ランプなどの光でも良い希ガスマイクロ波放電に
よる輝線を用いることもできる。成長温度も400℃に
限られるものではないが好ましくは700℃以下の成長
温度が良い。成長させる半導体結晶もGaNに限らず、
AQN、 InN、 GaAQN、 InAj!N。
It is also possible to use bright lines produced by rare gas microwave discharge, which may be light from a deuterium lamp or the like. Although the growth temperature is not limited to 400°C, a growth temperature of 700°C or less is preferable. The semiconductor crystal to be grown is not limited to GaN,
AQN, InN, GaAQN, InAj! N.

InGaN、 FaInAQNでも良い、ただしエピタ
キシャル°  成長を行う場合は、結晶層と基板との間
の格子不整が小さくなるよう基板および混晶組成比を選
択する必要がある。
InGaN or FaInAQN may be used, but when epitaxial growth is performed, the substrate and the mixed crystal composition ratio must be selected so that the lattice mismatch between the crystal layer and the substrate is small.

上記実施例で得られたGaN結晶層はn型の電気特性を
示したが、p型層を得る場合には■族あるいは■族元素
を含むガスをドーピング原料として用いれば良い。
Although the GaN crystal layer obtained in the above example exhibited n-type electrical characteristics, in order to obtain a p-type layer, a gas containing a group Ⅰ or group Ⅰ element may be used as a doping material.

さらに上記実施例では単一の光を照射したが。Furthermore, in the above embodiment, a single light beam is irradiated.

複数の波長を有する光を照射しても良い、その他本発明
はその趣旨を逸脱しない範囲で種々変形して実施するこ
とができる。
Light having a plurality of wavelengths may be irradiated, and the present invention can be implemented with various modifications without departing from the spirit thereof.

(発明の効果〕 以上述べた様に本発明によれば、光を照射することによ
りNの供給原料の解難および表面反応、表面泳動が促進
され、Nを構成元素として有する化合物半導体、または
混晶半導体を低温で成長することができ、したがって高
品質な半導体結晶層を成長することができ、したがって
高品質な半導体結晶層を形成することができる。
(Effects of the Invention) As described above, according to the present invention, irradiation with light promotes the disintegration, surface reaction, and surface migration of N as a feedstock, thereby producing a compound semiconductor or mixed crystal containing N as a constituent element. A semiconductor can be grown at a low temperature, and therefore a high quality semiconductor crystal layer can be grown, and therefore a high quality semiconductor crystal layer can be formed.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は1本発明の一実施例を説明するための結晶成長
装置を示す図である。 1・・・成長容器     2.3・・・ガス導入口4
・・・排気系      5・・・サセプタ6・・・基
板       7・・・光導入窓8・・・反射ミラー
    9・・・エキシマレーザlO・・・レーザ光 代理人 弁理士 則 近 憲 佑 同  松山光之
FIG. 1 is a diagram showing a crystal growth apparatus for explaining one embodiment of the present invention. 1...Growth container 2.3...Gas inlet 4
... Exhaust system 5 ... Susceptor 6 ... Substrate 7 ... Light introduction window 8 ... Reflection mirror 9 ... Excimer laser lO ... Laser light agent Patent attorney Nori Chika Ken Yudo Matsuyama Mitsuyuki

Claims (2)

【特許請求の範囲】[Claims] (1)窒素(N)を構成元素として有する化合物半導体
、または混晶半導体の気相成長法において、原料ガスあ
るいは被成長基板に光を照射することを特徴とする半導
体結晶の 成長方法。
(1) A method for growing a semiconductor crystal, which comprises irradiating a source gas or a substrate to be grown with light in a vapor phase growth method for a compound semiconductor or a mixed crystal semiconductor having nitrogen (N) as a constituent element.
(2)前記化合物半導体がGaN、AlN、InN、前
記混晶半導体が、InGaAlN、AlGaN、InG
aNであることを特徴とする請求項1記載の半導体結晶
の気相成長方法。
(2) The compound semiconductor is GaN, AlN, InN, and the mixed crystal semiconductor is InGaAlN, AlGaN, InG.
2. The method for vapor phase growth of a semiconductor crystal according to claim 1, wherein the semiconductor crystal is aN.
JP3955588A 1988-02-24 1988-02-24 Growth of semiconductor crystal Pending JPH01215014A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3955588A JPH01215014A (en) 1988-02-24 1988-02-24 Growth of semiconductor crystal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3955588A JPH01215014A (en) 1988-02-24 1988-02-24 Growth of semiconductor crystal

Publications (1)

Publication Number Publication Date
JPH01215014A true JPH01215014A (en) 1989-08-29

Family

ID=12556314

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3955588A Pending JPH01215014A (en) 1988-02-24 1988-02-24 Growth of semiconductor crystal

Country Status (1)

Country Link
JP (1) JPH01215014A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03112129A (en) * 1989-09-26 1991-05-13 Toyoda Gosei Co Ltd Vapor growth device for compound semiconductor
JP2006303258A (en) * 2005-04-22 2006-11-02 Ishikawajima Harima Heavy Ind Co Ltd Method for growing p-type nitride semiconductor
JP2006303259A (en) * 2005-04-22 2006-11-02 Ishikawajima Harima Heavy Ind Co Ltd Nitride semiconductor light emitting device and method for growing nitride semiconductor
JP2020501345A (en) * 2016-10-28 2020-01-16 ルミレッズ リミテッド ライアビリティ カンパニー Method for growing light emitting device under ultraviolet irradiation

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03112129A (en) * 1989-09-26 1991-05-13 Toyoda Gosei Co Ltd Vapor growth device for compound semiconductor
JP2006303258A (en) * 2005-04-22 2006-11-02 Ishikawajima Harima Heavy Ind Co Ltd Method for growing p-type nitride semiconductor
JP2006303259A (en) * 2005-04-22 2006-11-02 Ishikawajima Harima Heavy Ind Co Ltd Nitride semiconductor light emitting device and method for growing nitride semiconductor
JP2020501345A (en) * 2016-10-28 2020-01-16 ルミレッズ リミテッド ライアビリティ カンパニー Method for growing light emitting device under ultraviolet irradiation

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