JPH0449629A - Compound semiconductor crystal and its manufacturing method - Google Patents
Compound semiconductor crystal and its manufacturing methodInfo
- Publication number
- JPH0449629A JPH0449629A JP16067390A JP16067390A JPH0449629A JP H0449629 A JPH0449629 A JP H0449629A JP 16067390 A JP16067390 A JP 16067390A JP 16067390 A JP16067390 A JP 16067390A JP H0449629 A JPH0449629 A JP H0449629A
- Authority
- JP
- Japan
- Prior art keywords
- compound semiconductor
- substrate
- semiconductor crystal
- crystal
- heating region
- 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
Links
Landscapes
- Recrystallisation Techniques (AREA)
Abstract
Description
【発明の詳細な説明】
〔概 要〕
化合物半導体結晶、および該化合物半導体結晶の製造方
法に関し、
基板上にエピタキシャル成長により形成された化合物半
導体結晶が低転位密度と成る結晶、および該結晶の製造
方法を目的とし、
基板上にエピタキシャル成長された化合物半導体結晶が
、線状の加熱領域で熱サイクル焼鈍されて成ることで構
成する。[Detailed Description of the Invention] [Summary] Regarding a compound semiconductor crystal and a method for manufacturing the compound semiconductor crystal, the compound semiconductor crystal formed by epitaxial growth on a substrate has a low dislocation density, and the method for manufacturing the crystal. It is composed of a compound semiconductor crystal epitaxially grown on a substrate and thermally cycle annealed in a linear heating region.
また基板上に化合物半導体結晶をエピタキシャル成長す
る成長途中、或いは基板上に該結晶をエピタキシャル成
長した後、該結晶に線状の加熱領域を走査させて該結晶
を熱サイクル焼鈍することで構成する。Further, it is constructed by thermally annealing the crystal by scanning a linear heating region on the crystal during epitaxial growth of the compound semiconductor crystal on the substrate, or after epitaxially growing the crystal on the substrate.
本発明は化合物半導体結晶、およびその製造方法に係り
、特に基板上にエピタキシャル成長により形成される化
合物半導体結晶が低転位密度で得られるようにした化合
物半導体結晶、およびその製造方法に関する。The present invention relates to a compound semiconductor crystal and a method for manufacturing the same, and more particularly to a compound semiconductor crystal that can be formed on a substrate by epitaxial growth and has a low dislocation density, and a method for manufacturing the same.
赤外線検知素子形成材料としてはエネルギーバンドギャ
ップの狭い水銀・カドミウム・テルル(Hg、−、Cd
xTe)のような化合物半導体結晶が用いられている。Mercury, cadmium, tellurium (Hg, -, Cd) with narrow energy band gaps are used as materials for forming infrared sensing elements.
A compound semiconductor crystal such as xTe) is used.
このような化合物半導体結晶を素子形成に都合が良いよ
うに大面積でかつ薄層状態に形成する方法として気相、
或いは液相エピタキシャル成長方法が用いられている。Vapor phase,
Alternatively, a liquid phase epitaxial growth method is used.
このような化合物半導体結晶の製造に於いて、従来より
カドミウム・テルル(CdTe) M板が用いられてい
るが、この基板は高価であるので最近、GaAs基板を
用い、その上にCdTe結晶、Hg+−x CdxTe
結晶を順次へテロエピタキシャル成長して複数層に積層
することが行われ□ている。In the production of such compound semiconductor crystals, cadmium-tellurium (CdTe) M plates have traditionally been used, but since this substrate is expensive, recently GaAs substrates have been used, and CdTe crystals, Hg+ -x CdxTe
Crystals are successively grown heteroepitaxially and stacked into multiple layers.
然し、このようにヘテロエピタキシャル成長したHg+
−11Cdx Te結晶は転位密度が大であるので、こ
れを所定の範囲内に収める技術が要望されている。However, Hg+ grown heteroepitaxially in this way
Since the -11Cdx Te crystal has a high dislocation density, there is a need for a technique to keep this within a predetermined range.
従来、例えばシリコン(Si)基板にガリウム砒素(G
aAs)結晶をヘテロエピタキシャル成長する場合、S
i基板にアルミニウム砒素(A/As)層、GaAs層
を交互に数10人の厚さの薄層で多数層積層した歪超格
子層を形成し、この上にGaAs結晶を積層することで
、形成されるGaAs結晶の転位密度を低減させる方法
がある。Conventionally, for example, gallium arsenide (G) was deposited on a silicon (Si) substrate.
aAs) When growing a crystal heteroepitaxially, S
By forming a strained superlattice layer in which aluminum arsenide (A/As) layers and GaAs layers are alternately laminated in multiple thin layers of several tens of layers on an i-substrate, and by laminating a GaAs crystal on top of this, There is a method of reducing the dislocation density of the GaAs crystal that is formed.
然し、この方法では上記歪超格子層を形成するのは困難
で煩雑である。However, with this method, it is difficult and complicated to form the strained superlattice layer.
また特開昭56−61179号に於いて、イオン注入で
不純物原子が導入されて点欠陥を生じた基板を、レーザ
で加熱してイオン注入する以前の状態に戻す方法が開示
されている。Furthermore, Japanese Patent Application Laid-Open No. 56-61179 discloses a method of heating a substrate with point defects due to the introduction of impurity atoms by ion implantation using a laser to restore the state to the state before the ion implantation.
然し、この方法に於いては基板の極く表面層のみの点欠
陥を元の状態に復帰させるに過ぎず、基板上に形成され
た所定の厚さの結晶全体の転位密度を低下させるには不
十分である。However, this method only restores point defects in the very surface layer of the substrate to its original state, and it is difficult to reduce the dislocation density of the entire crystal of a given thickness formed on the substrate. Not enough.
また従来よりSi基板上に多結晶SiをCVD法で形成
した後、これをレーザアニールして単結晶Siとする固
相エピタキシャル成長方法もあるが、この方法であると
基板全体を加熱することになる。There is also a conventional solid-phase epitaxial growth method in which polycrystalline Si is formed on a Si substrate by CVD and then laser annealed to form single-crystal Si, but this method requires heating the entire substrate. .
また特願昭61−226994号、特願昭62−619
69号に於いて基板上に該基板と格子定数の異なる結晶
をヘテロエピタキシャル成長し、この基板全体の温度を
上昇、或いは下降して熱サイクル焼鈍を行って基板上の
結晶の転位密度を低減させた例もあるが、この場合に於
いても基板全体を加熱している。Also, Japanese Patent Application No. 61-226994, Japanese Patent Application No. 62-619
In No. 69, a crystal having a lattice constant different from that of the substrate was heteroepitaxially grown on a substrate, and the temperature of the entire substrate was increased or decreased to perform thermal cycle annealing to reduce the dislocation density of the crystal on the substrate. Although there are some examples, even in this case, the entire substrate is heated.
然し、このように基板全体の温度を上下させる熱サイク
ル焼鈍では、基板とエピタキシャル層との間で熱膨張率
の相違が無い場合、基板とエピタキシャル結晶のへテロ
界面に応力が働がない。そのため、エピタキシャル層内
で横方向に走る正、或いは負の転位の移動がなく、その
ため転位の合体消滅が起こらないため、転位の低減が起
こらないといった問題がある。However, in thermal cycle annealing in which the temperature of the entire substrate is raised and lowered in this manner, if there is no difference in thermal expansion coefficient between the substrate and the epitaxial layer, no stress is applied to the heterointerface between the substrate and the epitaxial crystal. Therefore, there is no movement of positive or negative dislocations running in the lateral direction within the epitaxial layer, and therefore dislocation coalescence and annihilation do not occur, resulting in a problem that dislocations are not reduced.
また転位を移動させるための駆動力は、基板とエピタキ
シャル結晶の境界のへテロ界面からのみエネルギーが与
えられるので、エピタキシャル結晶と基板の両方を加熱
する方法では、転位が移動し難いと言った問題もある。In addition, the driving force for moving dislocations is given energy only from the heterointerface between the substrate and the epitaxial crystal, so methods that heat both the epitaxial crystal and the substrate have the problem that dislocations are difficult to move. There is also.
本発明は上記した問題点を解決し、転位の移動を容易に
して、簡単な方法で容易に転位の消滅した化合物半導体
結晶、および該結晶の製造方法の提供を目的とする。The object of the present invention is to solve the above-mentioned problems and provide a compound semiconductor crystal in which dislocations can be easily moved and dislocations can be easily eliminated by a simple method, and a method for producing the crystal.
上記目的を達成する本発明の化合物半導体結晶は、第1
図(a)および第1図(b)の原理図に示すように、基
板1上にエピタキシャル成長された化合物半導体結晶2
が、線状の加熱領域3で熱サイクル焼鈍されて形成され
ている。The compound semiconductor crystal of the present invention that achieves the above object has a first
As shown in the principle diagrams of FIG. 1(a) and FIG. 1(b), a compound semiconductor crystal 2 is epitaxially grown on a substrate 1.
is formed by thermal cycle annealing in the linear heating region 3.
またその化合物半導体結晶の製造方法は、第1図(a)
および第1図色)の原理図に示すように、基板1上に化
合物半導体結晶2をエピタキシャル成長する成長途中、
或いは基板1上に該結晶2をエピタキシャル成長した後
、該結晶に線状の加熱領域3を走査させて該結晶2を熱
サイクル焼鈍する。The method for manufacturing the compound semiconductor crystal is shown in Figure 1(a).
As shown in the principle diagram of FIG.
Alternatively, after epitaxially growing the crystal 2 on the substrate 1, the crystal 2 is thermally annealed by scanning the linear heating region 3 over the crystal.
更に前記化合物半導体結晶2は基板1上に成長された単
一の結晶、或いは積層された組成の異なる複数のへテロ
結晶とする。Further, the compound semiconductor crystal 2 may be a single crystal grown on the substrate 1, or a plurality of stacked heterocrystals having different compositions.
また前記加熱領域3が、前記基板上の単一の化合物半導
体結晶か、或いは前記複数の化合物半導体結晶のうちの
所定の結晶に選択的に吸収される波長の光を発生する光
源で形成されるものとする。Further, the heating region 3 is formed by a light source that generates light of a wavelength that is selectively absorbed by a single compound semiconductor crystal on the substrate or a predetermined crystal of the plurality of compound semiconductor crystals. shall be taken as a thing.
また前記加熱領域3を基板1上、或いは基板下より交互
に或いは同時に化合物半導体結晶に走査する。Further, the heating region 3 is scanned over the compound semiconductor crystal from above the substrate 1 or from below the substrate alternately or simultaneously.
また前記加熱領域3が化合物半導体結晶2に選択的に形
成されるように、加熱領域形成用光源をオンオフしなが
ら該加熱領域を化合物半導体結晶に走査し、該化合物半
導体結晶に高転位密度領域、或いは低転位密度領域を選
択的に形成し、該化合物半導体結晶の低転位密度領域に
選択的に素子を形成することにある。Further, in order to selectively form the heating region 3 in the compound semiconductor crystal 2, the heating region is scanned over the compound semiconductor crystal while turning on and off the light source for forming the heating region, and the high dislocation density region is formed in the compound semiconductor crystal. Another method is to selectively form low dislocation density regions and selectively form elements in the low dislocation density regions of the compound semiconductor crystal.
第1図(a)の平面図、第1図(a)の断面図の第1図
(b)に示すように、基板1上に化合物半導体結晶2を
形成し、その上より幅が約1ml11のレーザ光源の加
熱による加熱領域3を矢印AおよびB方向に沿って走査
させると、第4図の曲線11に示すように所定の時間毎
に、IIA、 IIBのピーク値に示すように加熱領域
3が化合物半導体結晶上を周期的に通過することになる
。そしてこの加熱領域3を挟んで化合物半導体結晶2に
温度勾配が生じる。そしてこの温度勾配による温度差に
基づく熱膨張に起因して該結晶内に格子定数差が生じる
。As shown in the plan view of FIG. 1(a) and FIG. 1(b) of the cross-sectional view of FIG. 1(a), a compound semiconductor crystal 2 is formed on a substrate 1, and a width of about 1 ml 11 When the heating area 3 caused by heating by the laser light source is scanned along the directions of arrows A and B, the heating area changes at predetermined time intervals as shown by the peak values of IIA and IIB, as shown by the curve 11 in FIG. 3 passes periodically over the compound semiconductor crystal. A temperature gradient is generated in the compound semiconductor crystal 2 across the heating region 3. A difference in lattice constant occurs within the crystal due to thermal expansion based on the temperature difference due to this temperature gradient.
この状態で加熱領域を移動すると基板上の成る定点11
Aでは基板温度T0から加熱領域の最高温度T、まで周
期的に変化する。When the heating area is moved in this state, a fixed point 11 will be formed on the substrate.
At A, the temperature changes periodically from the substrate temperature T0 to the maximum temperature T of the heating region.
これは基板と化合物半導体結晶の境界のへテロ界面だけ
で無く、エピタキシャル成長された化合物半導体結晶2
の全体で起こるために、第1図(alおよび第1図(b
)に示すように矢印A方向に示す正方向の転位の移動、
矢印B方向に示す負方向の転位の移動が生じ、これら正
負の両方向に移動する転位の合体消滅が促進される。This occurs not only at the hetero interface between the substrate and the compound semiconductor crystal, but also at the epitaxially grown compound semiconductor crystal 2.
Figure 1 (al) and Figure 1 (b) occur throughout the
), the movement of dislocations in the positive direction shown in the direction of arrow A,
Dislocations move in the negative direction shown in the direction of arrow B, and the coalescence and annihilation of these dislocations moving in both positive and negative directions is promoted.
更に第3図に図示するように、基板1上に3〜5μmの
波長の光を吸収するHgTeの光吸収片の化合物半導体
結晶21と、上記波長の光を透過するCdTeの光透過
用の化合物半導体結晶22をヘテロエピタキシャル成長
し、光吸収用の化合物半導体結晶のみに吸収される波長
のレーザ光をレーザ光源34より基板上に照射する。す
ると前記加熱領域3を基板の横方向に沿って移動する際
に形成される温度勾配と共に更に積層されたエピタキシ
ャル結晶の相互の熱膨張率差に起因する転位の移動のた
めの駆動力が加わることになり、より一層の転位の合体
消滅が図れるようになる。Further, as shown in FIG. 3, a compound semiconductor crystal 21 made of a light-absorbing piece of HgTe that absorbs light with a wavelength of 3 to 5 μm and a light-transmitting compound of CdTe that transmits light with a wavelength of 3 to 5 μm are disposed on the substrate 1. A semiconductor crystal 22 is grown heteroepitaxially, and a laser light source 34 irradiates the substrate with laser light having a wavelength that is absorbed only by the light-absorbing compound semiconductor crystal. Then, along with the temperature gradient formed when the heating region 3 is moved along the lateral direction of the substrate, a driving force for the movement of dislocations due to the mutual thermal expansion coefficient difference of the laminated epitaxial crystals is added. This makes it possible to further coalesce and eliminate dislocations.
また基板上に前記した光吸収用の化合物半導体結晶と光
透過用の化合物半導体結晶の複数のへテロエピタキシャ
ル結晶を形成後、基板の表面と裏面の両側に設けた光源
を、それぞれ独立に、または同一方向に走査することで
エピタキシャル結晶層の表面と裏面側に加熱領域が形成
されることになり、より一層転位の低下が図れる。Further, after forming a plurality of heteroepitaxial crystals of the above-mentioned light-absorbing compound semiconductor crystal and light-transmitting compound semiconductor crystal on the substrate, light sources provided on both sides of the front and back surfaces of the substrate can be used independently or By scanning in the same direction, heated regions are formed on the front and back sides of the epitaxial crystal layer, thereby further reducing dislocations.
以下、図面を用いて本発明の実施例につき詳細に説明す
る。Embodiments of the present invention will be described in detail below with reference to the drawings.
第2図に示すようにGaAs基板1上にCdTe結晶3
1をホントウオールエピタキシャル成長方法、分子線エ
ピタキシャル成長方法、或いはMOCVD法を用いて約
1μmの厚さに形成する。As shown in FIG. 2, a CdTe crystal 3 is placed on a GaAs substrate 1.
1 is formed to a thickness of about 1 μm using a real wall epitaxial growth method, a molecular beam epitaxial growth method, or an MOCVD method.
このGaAs基板1を石英ガラス製の容器32内に導入
し、次いでGaAs基板1を200℃(To)に容器の
周囲に設けたヒータ33にて加熱し、Arガスレーザ光
源34を用いて111℃m程度の線状の加熱領域3を形
成し、この加熱領域3の温度が700℃に成るように調
整する。This GaAs substrate 1 is introduced into a container 32 made of quartz glass, and then the GaAs substrate 1 is heated to 200° C. (To) with a heater 33 provided around the container, and heated to 111° C. using an Ar gas laser light source 34. A linear heating region 3 of about 100° C. is formed, and the temperature of this heating region 3 is adjusted to 700° C.
次いでこの線状の加熱領域3を走査ミラー(図示せず)
を用いて1mm /minの速度で基板の横方向に矢印
A方向、またはB方向に沿って移動し、この走査を10
回程度繰り返す。Next, this linear heating area 3 is scanned by a scanning mirror (not shown).
was used to move laterally across the substrate at a speed of 1 mm/min in the direction of arrow A or direction B, and this scanning was repeated for 10 minutes.
Repeat several times.
ここでGaAs基板1上にエピタキシャル成長したCd
Te結晶31よりCdが蒸発するのを防止するために、
容器32内に図示しないがCdのソース結晶を封入して
Cdの蒸気を容器内に充満して容器32内をCdの雰囲
気とする。Here, Cd epitaxially grown on the GaAs substrate 1
In order to prevent Cd from evaporating from the Te crystal 31,
Although not shown, a source crystal of Cd is sealed in the container 32, and the container is filled with Cd vapor to create a Cd atmosphere inside the container 32.
このようにすることで、GaAs基板1上に転位密度が
106まで減少したCdTe結晶31が得られた。By doing so, a CdTe crystal 31 with a dislocation density reduced to 106 was obtained on the GaAs substrate 1.
このような方法を用いないで従来の方法により形成した
CdTe結晶は10?程度の転位密度を有する。CdTe crystals formed by conventional methods without using such methods are 10? It has a dislocation density of approximately
なお、本実施例ではエピタキシャル成長後に加熱処理を
行ったが、エピタキシャル結晶を所定の厚さで形成後、
この加熱処理を行って、更にエピタキシャル結晶を形成
するようにしても良い。Note that in this example, heat treatment was performed after epitaxial growth, but after forming epitaxial crystals to a predetermined thickness,
This heat treatment may be performed to further form epitaxial crystals.
次いで本発明の第2実施例を第3図に示す。Next, a second embodiment of the present invention is shown in FIG.
図示するようにGaAs基板1上に前記ホットウォール
エピタキシャル成長法、分子線エピタキシャル成長法、
MOCVD法を用いてHgTeよりなる光吸収用の化合
物半導体結晶21を約1μmの厚さに形成し、その上に
CdTeより成る光透過層としての化合物半導体結晶2
2を1μmの厚さに形成する。As shown in the figure, the hot wall epitaxial growth method, molecular beam epitaxial growth method,
A light-absorbing compound semiconductor crystal 21 made of HgTe is formed to a thickness of about 1 μm using the MOCVD method, and a compound semiconductor crystal 2 made of CdTe as a light-transmitting layer is formed thereon.
2 to a thickness of 1 μm.
そしてこの基板を透明な石英製の容器32内に封入し、
該基板上よりレーザ光源34を用いて2〜3μmの波長
のレーザ光を照射する。Then, this substrate is enclosed in a transparent quartz container 32,
A laser beam having a wavelength of 2 to 3 μm is irradiated onto the substrate using a laser light source 34.
このレーザ光源は光吸収用の化合物半導体結晶21に吸
収され、光透過用の化合物半導体結晶22を透過する波
長の光を照射する光源とする。This laser light source is a light source that emits light of a wavelength that is absorbed by a compound semiconductor crystal 21 for light absorption and transmitted through a compound semiconductor crystal 22 for light transmission.
そしてこの波長の光は光透過用の化合物半導体結晶22
を透過して光吸収用の化合物半導体結晶21にて吸収さ
れ、1mm程度の幅の加熱領域3が化合物半導体結晶2
1に形成されるように、図示しないがレンズ、ミラー等
の光学系、およびレーザ光源の出射光を調整する。そし
てこのレーザ光を図示しないがミラー等を用いて1mm
/min程度の速度で矢印AまたはB方向に10往復程
度走査する。The light of this wavelength is transmitted through a compound semiconductor crystal 22 for light transmission.
The light is transmitted through the compound semiconductor crystal 21 and absorbed by the compound semiconductor crystal 21, and a heated region 3 with a width of about 1 mm is formed by the compound semiconductor crystal 2.
1, optical systems such as lenses and mirrors (not shown) and the emitted light of the laser light source are adjusted. Although this laser beam is not shown, a mirror or the like is used to
Scanning is performed about 10 times in the direction of arrow A or B at a speed of about /min.
するとこの加熱領域3が格子定数の異なる基板とへテロ
エピタキシャル成長した光透過用の化合物半導体結晶2
2の間に囲まれて移動することになり、この加熱領域の
左右の方向の温度勾配による熱膨張の差に起因する転位
の駆動力とあいまって光吸収用の化合物半導体結晶21
の縦方向のへテロ界面21A、21Bにも温度勾配が生
じてより一層転位の移動が生じ易くなる。Then, this heating region 3 forms a light-transmitting compound semiconductor crystal 2 which is grown heteroepitaxially with a substrate having a different lattice constant.
The compound semiconductor crystal 21 for light absorption
A temperature gradient also occurs at the vertical hetero interfaces 21A and 21B, making it easier for dislocations to move.
またその他の実施例としてGaAs基板上にCdTe結
晶とHgI−x Cdx Te結晶とを積層し、上記レ
ーザ光を走査する際にレーザ光の照射をオンオフするよ
うにしておき、光吸収層のHg、−、Cdx T6結晶
内部にレーザ光で加熱された領域、或いは加熱されない
領域を選択的に形成して、高転位密度領域と低転位密度
領域とを選択的に形成し、この低転位密度領域に素子形
成用不純物を導入して赤外線検知素子を形成すると、高
転位密度領域が素子骨M jJI域となって、素子分離
されたアレイ状の赤外線検知素子が容易に得られる。As another example, a CdTe crystal and a HgI-x Cdx Te crystal are stacked on a GaAs substrate, and the laser beam irradiation is turned on and off when scanning with the laser beam, and the Hg of the light absorption layer, -, Cdx A region heated by a laser beam or a region not heated is selectively formed inside the T6 crystal to selectively form a high dislocation density region and a low dislocation density region, and the low dislocation density region is When element-forming impurities are introduced to form an infrared sensing element, the high dislocation density region becomes an element bone MjJI region, and an array-shaped infrared sensing element in which elements are separated can be easily obtained.
また基板の裏面側にも光源を配置し、基板の表裏両面側
より交互に、或いは同時に加熱領域となるレーザ光を照
射するようにしても良い。Further, a light source may also be arranged on the back side of the substrate, and laser light may be irradiated from both the front and back sides of the substrate alternately or simultaneously, which will serve as the heating area.
以上の説明から明らかなように本発明によれば転位密度
の少ない高品質の化合物半導体結晶が容易に得られる効
果がある。As is clear from the above description, the present invention has the effect of easily obtaining a high quality compound semiconductor crystal with a low dislocation density.
【図面の簡単な説明】
第1図(a)および第1図(b)は本発明の化合物半導
体結晶およびその製造方法の原理図、
第2図は本発明の第1実施例の説明図、第3図は本発明
の第2実施例の説明図、第4図は本発明の方法に於ける
結晶の定点の温度分布図である。
図において、
1は基板(GaAs基板)、2は化合物半導体結晶、3
は加熱領域、11は加熱温度分布曲線、IIA、 II
Bは加熱温度分布曲線のピーク値、21は化合物半導体
結晶(HgTe)、21A、21Bはへテロ界面、22
は化合物半導体結晶(CdTe) 、31はCdTe結
晶、32は容器、33はヒータ、34はレーザ光源を示
す。[BRIEF DESCRIPTION OF THE DRAWINGS] FIGS. 1(a) and 1(b) are principle diagrams of the compound semiconductor crystal of the present invention and its manufacturing method, FIG. 2 is an explanatory diagram of the first embodiment of the present invention, FIG. 3 is an explanatory diagram of the second embodiment of the present invention, and FIG. 4 is a temperature distribution diagram at a fixed point of the crystal in the method of the present invention. In the figure, 1 is a substrate (GaAs substrate), 2 is a compound semiconductor crystal, and 3 is a substrate (GaAs substrate).
is the heating region, 11 is the heating temperature distribution curve, IIA, II
B is the peak value of the heating temperature distribution curve, 21 is a compound semiconductor crystal (HgTe), 21A and 21B are hetero interfaces, 22
31 is a CdTe crystal, 32 is a container, 33 is a heater, and 34 is a laser light source.
Claims (6)
半導体結晶(2)が、走査可能の線状の加熱領域(3)
にて熱サイクル焼鈍されて成ることを特徴とする化合物
半導体結晶。(1) A compound semiconductor crystal (2) epitaxially grown on a substrate (1) is formed into a scannable linear heating area (3)
1. A compound semiconductor crystal characterized by being thermally cycle annealed.
キシャル成長する成長途中、或いはエピタキシャル成長
した後、該化合物半導体結晶(2)に線状の加熱領域(
3)を走査させて該結晶を熱サイクル焼鈍することを特
徴とする化合物半導体結晶の製造方法。(2) During the epitaxial growth of the compound semiconductor crystal (2) on the substrate (1), or after the epitaxial growth, a linear heating region (
3) A method for manufacturing a compound semiconductor crystal, which comprises scanning the crystal and subjecting the crystal to thermal cycle annealing.
(2)が単一の結晶(31)か、或いは組成の異なる複
数の化合物半導体結晶(21、22)が積層されている
ことを特徴とする請求項(2)記載の化合物半導体結晶
の製造方法。(3) The compound semiconductor crystal (2) grown on the substrate (1) is a single crystal (31) or a stack of multiple compound semiconductor crystals (21, 22) having different compositions. The method for producing a compound semiconductor crystal according to claim (2).
)か、前記複数の化合物半導体結晶(21、22)のう
ちの所定の結晶(21)に、選択的に吸収される波長を
有する光源(34)で形成されていることを特徴とする
請求項(2)、或いは(3)記載の化合物半導体結晶の
製造方法。(4) The heating region (3) is a single crystal (31) on the substrate.
) or a light source (34) having a wavelength that is selectively absorbed by a predetermined crystal (21) of the plurality of compound semiconductor crystals (21, 22). The method for producing a compound semiconductor crystal according to (2) or (3).
交互に、或いは同時に化合物半導体結晶(2)に走査す
ることを特徴とする請求項(2)、(3)或いは(4)
記載の化合物半導体結晶の製造方法。(5) Claim (2), (3) or (4) characterized in that the heating region (3) is scanned over the compound semiconductor crystal (2) alternately or simultaneously from above the substrate or from below the substrate.
A method for manufacturing the compound semiconductor crystal described above.
選択的に形成されるように、加熱領域形成用光源をオン
オフしながら走査し、該化合物半導体結晶に高転位密度
領域、或いは低転位密度領域を選択的に形成し、該化合
物半導体結晶の低転位密度領域に選択的に素子を形成す
ることを特徴とする請求項(2)、(3)、(4)或い
は(5)に記載の化合物半導体結晶の製造方法。(6) Scanning the heating region forming light source while turning on and off so that the heating region (3) is selectively formed in the compound semiconductor crystal (2), and forming a high dislocation density region or a low dislocation density region in the compound semiconductor crystal. According to claim (2), (3), (4) or (5), wherein dislocation density regions are selectively formed and elements are selectively formed in low dislocation density regions of the compound semiconductor crystal. A method for manufacturing the compound semiconductor crystal described above.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16067390A JPH0449629A (en) | 1990-06-18 | 1990-06-18 | Compound semiconductor crystal and its manufacturing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16067390A JPH0449629A (en) | 1990-06-18 | 1990-06-18 | Compound semiconductor crystal and its manufacturing method |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0449629A true JPH0449629A (en) | 1992-02-19 |
Family
ID=15720007
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16067390A Pending JPH0449629A (en) | 1990-06-18 | 1990-06-18 | Compound semiconductor crystal and its manufacturing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0449629A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2012504857A (en) * | 2008-10-01 | 2012-02-23 | インターナショナル・ビジネス・マシーンズ・コーポレーション | Method and system for eliminating dislocations in an active region of a semiconductor body |
-
1990
- 1990-06-18 JP JP16067390A patent/JPH0449629A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2012504857A (en) * | 2008-10-01 | 2012-02-23 | インターナショナル・ビジネス・マシーンズ・コーポレーション | Method and system for eliminating dislocations in an active region of a semiconductor body |
| KR101475992B1 (en) * | 2008-10-01 | 2014-12-30 | 인터내셔널 비지네스 머신즈 코포레이션 | Dislocation engineering using a scanned laser |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US4444620A (en) | Growth of oriented single crystal semiconductor on insulator | |
| US4835116A (en) | Annealing method for III-V deposition | |
| US5107317A (en) | Semiconductor device with first and second buffer layers | |
| US4345967A (en) | Method of producing thin single-crystal sheets | |
| US4900372A (en) | III-V on Si heterostructure using a thermal strain layer | |
| US6299680B1 (en) | CdTe crystal or CdZnTe crystal and method for preparing the same | |
| JPH0449629A (en) | Compound semiconductor crystal and its manufacturing method | |
| JPH01315127A (en) | Formation of gallium arsenide layer | |
| US12203191B2 (en) | Method of producing large GaAs and GaP infrared windows | |
| JPS62172715A (en) | Manufacture of semiconductor epitaxial thin film | |
| US5451552A (en) | Method for improvement of optical quality and reduction of background doping in gainSB/INAS superlattices | |
| JPH04298020A (en) | Manufacture of silicon thin film crystal | |
| JP2651146B2 (en) | Crystal manufacturing method | |
| JP3364696B2 (en) | Method for producing group III-V compound thin film | |
| JP2006253414A (en) | Method for forming semiconductor thin film on Si substrate and structure thereof | |
| JPH0645249A (en) | Growth method of gaas layer | |
| JP2737152B2 (en) | SOI forming method | |
| JPS63291897A (en) | Method for growing single crystal membrane | |
| JP2771635B2 (en) | Ca lower 1-lower x Sr lower x F lower 2 | |
| JP2695462B2 (en) | Crystalline semiconductor film and method for forming the same | |
| JPS63192227A (en) | Epitaxial growth method of compound semiconductor | |
| JP2759298B2 (en) | Thin film formation method | |
| WO1990003659A1 (en) | Fabrication of semiconductor nanostructures | |
| JPH05243148A (en) | Formation of delta-doped multilayered film semiconductor single crystal | |
| JPS6272109A (en) | Manufacture of compound semiconductor device |