Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6232608B2 - - Google Patents
[go: Go Back, main page]

JPS6232608B2 - - Google Patents

Info

Publication number
JPS6232608B2
JPS6232608B2 JP12854280A JP12854280A JPS6232608B2 JP S6232608 B2 JPS6232608 B2 JP S6232608B2 JP 12854280 A JP12854280 A JP 12854280A JP 12854280 A JP12854280 A JP 12854280A JP S6232608 B2 JPS6232608 B2 JP S6232608B2
Authority
JP
Japan
Prior art keywords
transition layer
layer
gaas
transition
compound 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.)
Expired
Application number
JP12854280A
Other languages
Japanese (ja)
Other versions
JPS5753927A (en
Inventor
Yasuhiro Ishii
Noryuki Shimano
Yoshimoto Fujita
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.)
Oki Electric Industry Co Ltd
Original Assignee
Oki Electric Industry Co Ltd
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 Oki Electric Industry Co Ltd filed Critical Oki Electric Industry Co Ltd
Priority to JP12854280A priority Critical patent/JPS5753927A/en
Publication of JPS5753927A publication Critical patent/JPS5753927A/en
Publication of JPS6232608B2 publication Critical patent/JPS6232608B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/20Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
    • H10P14/34Deposited materials, e.g. layers
    • H10P14/3402Deposited materials, e.g. layers characterised by the chemical composition
    • H10P14/3414Deposited materials, e.g. layers characterised by the chemical composition being group IIIA-VIA materials
    • H10P14/3418Phosphides
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/20Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
    • H10P14/29Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by the substrates
    • H10P14/2901Materials
    • H10P14/2902Materials being Group IVA materials
    • H10P14/2905Silicon, silicon germanium or germanium
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/20Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
    • H10P14/32Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by intermediate layers between substrates and deposited layers
    • H10P14/3202Materials thereof
    • H10P14/3204Materials thereof being Group IVA semiconducting materials
    • H10P14/3211Silicon, silicon germanium or germanium
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/20Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
    • H10P14/32Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by intermediate layers between substrates and deposited layers
    • H10P14/3242Structure
    • H10P14/3244Layer structure
    • H10P14/3254Graded layers
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/20Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
    • H10P14/34Deposited materials, e.g. layers
    • H10P14/3438Doping during depositing
    • H10P14/3441Conductivity type
    • H10P14/3446Transition metal elements; Rare earth elements

Landscapes

  • Semiconductor Lasers (AREA)
  • Led Devices (AREA)
  • Light Receiving Elements (AREA)
  • Solid State Image Pick-Up Elements (AREA)
  • Junction Field-Effect Transistors (AREA)
  • Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)
  • Recrystallisation Techniques (AREA)

Description

【発明の詳細な説明】 本発明は、シリコン単結晶(以下Siという)を
基板結晶材料として化合物半導体GaAs系結晶を
能動層とする半導体装置において、基板結晶と化
合物半導体能動層との間に、組成比xおよびyが
テーパ状またはステツプ状に変化するSi1-xGex
よびIn1-yGayPの二種類の遷移層からなる遷移域
を設けることにより格子定数の完全整合を実現し
た化合物半導体装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides a semiconductor device in which a silicon single crystal (hereinafter referred to as Si) is used as a substrate crystal material and a compound semiconductor GaAs-based crystal is used as an active layer, between the substrate crystal and the compound semiconductor active layer. Perfect matching of lattice constants was achieved by creating a transition region consisting of two types of transition layers, Si 1-x Ge x and In 1-y Ga y P, in which the composition ratios x and y change in a tapered or step-like manner. The present invention relates to compound semiconductor devices.

化合物半導体は、そのバンド構造の特徴や高い
電子移動度等の優れた性能を最大限に活用して、
近年種々の多機能、高性能な新しい電子部品を提
供しつつある。しかし、化合物半導体結晶は、一
般的に高価であり、また、大面積の欠陥の少ない
良質な基板結晶を得る工業化は未だ不満足な現状
にある。そこで、より安価でかつ大量生産の工業
化技術がすでに完成しているSi基板を基板結晶材
料に使用しようとする試みが従来からなされてい
るが、未だ研究段階であり実用化されたものは全
くない。
Compound semiconductors take full advantage of their excellent performance, such as their band structure characteristics and high electron mobility.
In recent years, a variety of new multi-functional, high-performance electronic components have been provided. However, compound semiconductor crystals are generally expensive, and the industrialization of obtaining high-quality substrate crystals with large areas and few defects is still unsatisfactory. Therefore, attempts have been made to use Si substrates as substrate crystal materials, which are cheaper and for which industrial technology for mass production has already been completed, but they are still at the research stage and nothing has been put to practical use. .

第1図は、シリコン単結晶を基板とする化合物
半導体結晶のエピタキシヤル成長の従来の構造例
を示すものである。異種物質間のエピタキシヤル
結晶成長は、主として結晶学的興味および結晶界
面(ヘテロ接合)の電気的特性研究を目的に種々
試みられている。Si基板1表面にGaAs層2をエ
ピタキシヤル成長させる場合、SiとGaAsとの格
子定数が夫々5.431Åと5.654Åであり、相当の相
異があるために良質な成長層を得ることは全く不
可能である。Siの格子定数に最も近い格子定数を
持つている化合物半導体としてはGaP(格子定数
=5.451Å)があるが、この場合でも詳細に観測
すると成長厚さの増大と共に微細なクラツクが数
多く発生しており、欠陥の多い成長層しか得られ
ず、多機能高性能半導体装置の構成に不適当であ
る。
FIG. 1 shows a conventional structural example of epitaxial growth of a compound semiconductor crystal using a silicon single crystal as a substrate. Various attempts have been made to grow epitaxial crystals between different materials, mainly for the purpose of crystallographic interest and the study of electrical properties of crystal interfaces (heterojunctions). When a GaAs layer 2 is epitaxially grown on the surface of a Si substrate 1, the lattice constants of Si and GaAs are 5.431 Å and 5.654 Å, respectively, and it is difficult to obtain a high-quality growth layer due to the considerable difference. It is possible. The compound semiconductor with a lattice constant closest to that of Si is GaP (lattice constant = 5.451 Å), but even in this case, detailed observation reveals that many minute cracks occur as the growth thickness increases. However, only a grown layer with many defects can be obtained, making it unsuitable for the construction of multi-functional, high-performance semiconductor devices.

本発明は、シリコン基板を使用する場合の上述
のような従来の欠点を克服するために、新しい遷
移域を設けた構成になる化合物半導体装置に関す
るものであり、以下実施例によりその基本原理を
説明する。
The present invention relates to a compound semiconductor device having a structure in which a new transition region is provided in order to overcome the above-mentioned conventional drawbacks when using a silicon substrate, and the basic principle thereof will be explained below with reference to examples. do.

第2図は本発明の一実施例を示す構造図であ
る。同図において、シリコン基板3の表面には第
1の遷移層4が設けられる。該遷移層の組成は
Si1-xGexとし、成分比xはシリコン基板表面でx
=0として遷移層の厚さの増加と共にxが増大す
るようなテーパ状の成分構成になるように設定す
る。共に族元素であるSiとGeは同種の結晶構
造を持つており、Si基板上にSi1-xGex層をエピタ
キシヤル成長した場合x〓35%の範囲内で単結晶
Si1-xGexの成長が可能であり、Si基板と成長層の
界面で特有の性質を有するヘテロ接合特性を示す
ことが知られている。本発明での第1の遷移層を
形成するSi1-xGex層4は、Si基板3との界面でx
=0になるようなテーパ状の成分構成とすること
により、界面での格子定数の完全整合を実現する
ものであり、界面でxが不連続的に変ることによ
るヘテロ接合特性を利用しようとするものではな
い。Si1-xGexの格子定数は、x=0でSiの格子定
数(=5.431Å)と一致しまたx=1でGeの格子
定数(=5.658Å)と一致し、その中間では第1
近似としてxに比例して増加する。
FIG. 2 is a structural diagram showing an embodiment of the present invention. In the figure, a first transition layer 4 is provided on the surface of a silicon substrate 3. The composition of the transition layer is
Si 1-x Ge x , and the component ratio x is x on the silicon substrate surface.
= 0, and a tapered component configuration is set in which x increases as the thickness of the transition layer increases. Si and Ge, both group elements, have the same type of crystal structure, and when a Si 1-x Ge x layer is epitaxially grown on a Si substrate, a single crystal is formed within the range of x = 35%.
It is possible to grow Si 1-x Ge x and is known to exhibit unique heterojunction characteristics at the interface between the Si substrate and the grown layer. The Si 1-x Ge x layer 4 forming the first transition layer in the present invention has x
By creating a tapered component configuration so that It's not a thing. The lattice constant of Si 1-x Ge x matches the lattice constant of Si (=5.431 Å) at x = 0, and that of Ge (= 5.658 Å) at x = 1, and the
As an approximation, it increases in proportion to x.

第2図の本発明の一実施例においては、さらに
In1-yGayP層からなる第2の遷移層5が設けられ
る。In1-yGayPは族―族の化合物半導体GaP
とInPとの混晶であり、その格子定数はy=1か
らy=0の範囲内で5.451Åから5.869Åの範囲内
の数値を持つ。第2の遷移層の組成比yがテーパ
状に変化し最外表面でy=0.515、すなわち、
GaAsの格子定数に等しくなるように構成され
る。
In one embodiment of the present invention shown in FIG.
A second transition layer 5 consisting of an In 1-y Ga y P layer is provided. In 1-y Ga y P is a group-group compound semiconductor GaP
It is a mixed crystal of and InP, and its lattice constant has a value within the range of 5.451 Å to 5.869 Å within the range of y = 1 to y = 0. The composition ratio y of the second transition layer changes in a tapered manner to y=0.515 at the outermost surface, that is,
It is configured to have a lattice constant equal to that of GaAs.

第3図は、本発明における第1の遷移層4と第
2の遷移層5の界面で格子定数の完全連続条件の
原理を説明するための説明図である。Si1-xGex
よびIn1-yGayPの常温における格子定数は、第1
近似として5.431+0.227x(Å)および5.869−
0.418y(Å)であり、従つて両遷移層の界面での
常温における格子定数の連続条件を与えるx〜y
の関係式は、x=1.93−1.84yとなり、第3図の
曲線1のようになる。一方、第2の遷移層のエピ
タキシヤル成長時を考えると、エピタキシヤル成
長温度での格子定数の熱膨脹現象があり、
Si1-xGexとIn1-yGayPの格子定数の温度係数の差
を2.97×10-6/℃とし、常温との温度差ΔTのエ
ピタキシヤル成長時において両遷移層の界面での
格子定数の連続条件を与えるx〜yの関係式は、
x=1.93−1.84y+7.678×10-5ΔTとなり、後述
のような本発明の一実施例におけるエピタキシヤ
ル成長温度の上限としてΔT=700℃とした場合
の整合条件を第3図の曲線2に示す。
FIG. 3 is an explanatory diagram for explaining the principle of the perfect continuity condition of the lattice constant at the interface between the first transition layer 4 and the second transition layer 5 in the present invention. The lattice constants of Si 1-x Ge x and In 1-y Ga y P at room temperature are the first
5.431+0.227x (Å) and 5.869− as approximations
0.418y (Å), thus giving the continuity condition of the lattice constant at room temperature at the interface of both transition layers
The relational expression is x=1.93-1.84y, which is like curve 1 in FIG. On the other hand, considering the epitaxial growth of the second transition layer, there is a thermal expansion phenomenon of the lattice constant at the epitaxial growth temperature.
The difference in the temperature coefficients of the lattice constants of Si 1-x Ge x and In 1-y Ga y P is assumed to be 2.97×10 -6 /℃, and at the interface of both transition layers during epitaxial growth with a temperature difference ΔT from room temperature. The relational expression between x and y that gives the continuity condition of the lattice constant is:
x=1.93−1.84y+7.678×10 -5 ΔT, and the matching condition when ΔT=700°C is the upper limit of the epitaxial growth temperature in an embodiment of the present invention as described later is shown in curve 2 in FIG. Shown below.

上述の本発明の格子定数の完全連続条件の検討
結果をみると、y=1すなわちGaPと整合すべき
第1の遷移層は、第3図の曲線1および曲線2か
ら明らかなように界面において約9〜15%の原子
がSi原子に代つて結晶構造に組入れられた結晶界
面を必要とすることを意味し、このGe原子の量
は通常の不純物といわれる添加量と比較して105
〜106倍も多いものである。従来SiとGaPとは格
子定数が接近していると見倣して遷移層を介さず
に直接ヘテロ接合を構成しようとする試みがなさ
れ、好ましくない結果を得ているが、一見微かな
格子定数の差(0.02Å)を克服するためには、
上述のようなGe原子の効果を強力に作用せしめ
るような本発明の遷移層が必要であることが明確
に説明される。
Looking at the results of the study on the perfectly continuous lattice constant condition of the present invention described above, the first transition layer that should match y=1, that is, GaP, is formed at the interface, as is clear from curves 1 and 2 in Figure 3. This means that approximately 9 to 15% of the atoms require crystal interfaces to be incorporated into the crystal structure in place of Si atoms, and this amount of Ge atoms is 10 5 compared to the amount added as a normal impurity.
~ 106 times more. Conventionally, attempts have been made to directly construct a heterojunction without using a transition layer, assuming that Si and GaP have close lattice constants, and have obtained unfavorable results. To overcome the difference (0.02Å),
It is clearly explained that the transition layer of the present invention is required to strongly exert the effect of Ge atoms as described above.

本発明の遷移域を構成するためのSi1-xGexおよ
びIn1-yGayP層のエピタキシヤル成長技術に関し
ては、従来から種々の方法が試みられている。
Si1-xGexのエピタキシヤル成長法としては、
SiCl4とGeCl4による気相成長法が一般的である
が、最近半導体薄膜の成長技術として急速に研究
開発が進められている分子線ビームエピタキシ
(MBE)、イオンビームエピタキシ(IBE)、クラ
スタイオンビームエピタキシ(ICBE)等の新技
術があり、これらの方法は成分元素の供給の制御
が高精度に可能であり、本発明の遷移層のように
テーパ状の組成構造を正確に実現させる場合には
全く好都合である。またこれらの成長法は従来の
通常の気相成長法と比較して非常に低い基板温度
(MBE法では750〜900℃、ICBE法では650〜800
℃)で良好な単結晶の成長が可能であり、基板と
成長層との熱膨脹係数の差により冷却過程で結晶
内に残留する熱応力の軽減に役立つ。In1-yGayP
層のエピタキシヤル成長に対しても、VPE、
LPE、CVDやPlaner Reactive Deposition等の技
術が効果的に応用される。第1と第2の遷移層の
界面での格子定数の連続条件に関する第3図の説
明において、第2の遷移層すなわちIn1-yGayPの
成長温度とx〜yの関係を述べたがIn1-yGayPの
エピタキシヤル成長温度はVPEでは650〜750
℃、LPEでは、500〜700℃、CVDでは500〜600
℃さらにPlaner Reactive Depositionでは300〜
400℃程度である。
Various methods have been tried in the past regarding epitaxial growth techniques for the Si 1-x G x and In 1-y Ga y P layers to constitute the transition region of the present invention.
The epitaxial growth method for Si 1-x Ge x is as follows:
Vapor phase growth using SiCl 4 and GeCl 4 is common, but molecular beam epitaxy (MBE), ion beam epitaxy (IBE), and cluster ion growth techniques, which have recently been rapidly researched and developed as semiconductor thin film growth techniques, are commonly used. There are new technologies such as beam epitaxy (ICBE), and these methods allow the supply of component elements to be controlled with high precision, and are useful when accurately realizing a tapered compositional structure like the transition layer of the present invention. is completely convenient. In addition, these growth methods require extremely low substrate temperatures (750 to 900 degrees Celsius for the MBE method and 650 to 800 degrees Celsius for the ICBE method) compared to conventional normal vapor phase growth methods.
℃), and the difference in thermal expansion coefficient between the substrate and the growth layer helps reduce thermal stress remaining in the crystal during the cooling process. In 1-y Ga y P
For epitaxial growth of layers, VPE,
Technologies such as LPE, CVD and Planer Reactive Deposition are effectively applied. In the explanation of Figure 3 regarding the lattice constant continuity conditions at the interface between the first and second transition layers, we described the relationship between the growth temperature of the second transition layer, that is, In 1-y Ga y P, and x~y. However, the epitaxial growth temperature of In 1-y Ga y P is 650 to 750 in VPE.
℃, for LPE, 500-700℃, for CVD, 500-600
℃ and 300~ for Planer Reactive Deposition
The temperature is around 400℃.

第4図は本発明の他の一実施例図であり、同図
の実施例ではシリコン基板6、Si1-xGexの第1の
遷移層7、In1-yGayPの第2の遷移層8が構成さ
れることは第2図の本発明の一実施例の場合と同
様であるが、第2の遷移層8の表面にCr、Fe等
の不純物を添加した半絶縁性GaAsからなる第3
の遷移層9を設ける。第2の遷移層8と第3の遷
移層9との界面はy=0.515すなわち
In0.485Ga0.515PとGaAsとの接続であり、格子定数
の完全連続性が実現される。半絶縁性GaAsの第
3の遷移層9は、その上に構成されるGaAs活性
層10と基板との電気的な絶縁層としてデバイス
構成上極めて有効な役割りを果たし、同図の一実
施例のようにGaAs―FETを構成する場合のよう
に、ゲート電極11により効率的にソース電極1
2とドレイン電極13間の電流を制御するための
チヤネル設定に活用される。また、GaAs―
FET、発光―受光素子等のモノリシツク集積化
デバイス構成の場合の素子間分離絶縁層として効
果的に活用される。
FIG. 4 shows another embodiment of the present invention, in which a silicon substrate 6, a first transition layer 7 of Si 1-x Ge x , and a second transition layer 7 of In 1-y Ga y P are used. The structure of the transition layer 8 is the same as in the embodiment of the present invention shown in FIG. The third consisting of
A transition layer 9 is provided. The interface between the second transition layer 8 and the third transition layer 9 is y=0.515, i.e.
This is a connection between In 0 . 485 Ga 0 . 515 P and GaAs, and complete continuity of the lattice constant is achieved. The third transition layer 9 of semi-insulating GaAs plays an extremely effective role in device construction as an electrically insulating layer between the substrate and the GaAs active layer 10 formed thereon. As in the case of configuring a GaAs-FET as shown in FIG.
It is utilized for channel setting to control the current between the drain electrode 13 and the drain electrode 13. Also, GaAs—
It is effectively used as an insulating layer for separating elements in monolithic integrated device configurations such as FETs and light-emitting/light-receiving elements.

なお、本発明の第2の遷移層のIn1-yGayP層に
Cr、Fe等の不純物添加を行ない、該層を半絶縁
層化することができる。すなわちCr等の不純物
はInPのみならずCaPに対しても1010Ωcm程度
の良好な半絶縁性を与え、従つて本発明の第2図
の一実施例において第2の遷移層の全域にわたつ
てCr添加を行ない、該層の格子定数の完全連続
性の役割りに加えて、本発明の他の一実施例で説
明した電気的な絶縁層としての役割りを持せるこ
とができる。また、第4図の実施例においても、
第2の遷移層8にCr添加を行なうことにより絶
縁層の厚さは、第2の遷移層8および第3の遷移
層9の、各々の厚さの和となり、漂遊容量の減少
せしめ素子性能の向上に貢献する。
Note that the In 1-y Ga y P layer of the second transition layer of the present invention
By adding impurities such as Cr and Fe, the layer can be made into a semi-insulating layer. That is, impurities such as Cr provide good semi-insulating properties of about 10 10 Ω - cm not only to InP but also to CaP, and therefore, in the embodiment of FIG. 2 of the present invention, the entire area of the second transition layer is By adding Cr over a period of time, in addition to the role of complete continuity of the lattice constant of the layer, it can also serve as an electrically insulating layer as explained in another embodiment of the present invention. . Also, in the embodiment shown in FIG.
By adding Cr to the second transition layer 8, the thickness of the insulating layer becomes the sum of the thicknesses of the second transition layer 8 and the third transition layer 9, which reduces stray capacitance and improves device performance. Contribute to the improvement of

また、本発明の第1および第2の遷移層は、第
2図の一実施例ではxおよびyが最も代表的にテ
ーパ状に変化するような組成構成で説明したが、
各層内のxおよびyの厚さ方向の分布を複数ステ
ツプで近似せしめるように設定することがエピタ
キシヤル成長の装置の状況によつては生産性が向
上する場合があり、本発明の基本原理はかかる手
法においてもすべて成立するものである。
Further, the first and second transition layers of the present invention have been described with a composition composition in which x and y most typically change in a tapered shape in the embodiment shown in FIG.
Depending on the conditions of the epitaxial growth equipment, productivity may be improved by setting the distribution of x and y in the thickness direction in each layer to be approximated by multiple steps, and the basic principle of the present invention is All of the above methods also hold true.

以上本発明の実施例で詳述したように、本発明
はSi基板にSi1-xGexおよびIn1-yGayPの二種類の
遷移層からなる遷移域を設けることを特徴とする
ものであり、かかる遷移域はSi基板とGaAsとの
間の完全な格子定数の整合を実現し、従来化合物
半導体装置の構成においてSi基板結晶を適用する
ことの最大の困難性を根本的に解決するものであ
り、より安価でかつ大面積大量生産技術の確立し
ているSi基板を最大限に活用して、化合物半導体
装置の低価格化、大規模集積化に直接貢献する効
果を有する。また、In1-yGayPからなる第2の遷
移層は、該層にCr、Fe等の不純物添加を行なう
ことにより、格子定数の整合としての役割りに加
えて素子間分離等の電気的な絶縁層としての役割
りを同時に持たせることが可能であり、このこと
はGaAs―FETあるいは光素子の構成さらにはそ
れらの集積化装置構成に全く効果的である。さら
に、Si基板の適用を可能にしたことの効果とし
て、Si系の素子と化合物半導体系素子をモノリシ
ツクに共存させることが可能となり、種々の新し
い多機能集積化装置の構成を可能とする。
As described above in detail in the embodiments of the present invention, the present invention is characterized in that a transition region consisting of two types of transition layers, Si 1-x Ge x and In 1-y Ga y P, is provided on the Si substrate. This transition region realizes perfect lattice constant matching between the Si substrate and GaAs, fundamentally solving the greatest difficulty in applying Si substrate crystals in the construction of conventional compound semiconductor devices. This makes full use of Si substrates, which are cheaper and have established large-area mass production technology, and has the effect of directly contributing to lower prices and large-scale integration of compound semiconductor devices. In addition, the second transition layer made of In 1-y Ga y P is doped with impurities such as Cr and Fe, so that in addition to serving as a lattice constant matching, the second transition layer is made of In 1-y Ga y P and serves as an electrical conductor for isolation between elements. It is possible to simultaneously serve as an insulating layer, and this is completely effective in the construction of GaAs-FETs or optical devices, as well as in the construction of integrated devices thereof. Furthermore, as a result of making it possible to apply a Si substrate, it becomes possible to monolithically coexist Si-based elements and compound semiconductor-based elements, making it possible to construct various new multifunctional integrated devices.

以上の本発明効果を総合して、本発明は化合物
半導体装置の低価格・高性能化に直接貢献するこ
とは勿論のこと、新しい多機能集積化装置の実現
の重大な基盤を与えるものであり、エレクトロニ
クス全般に与える本発明の効果は極めて大きい。
Combining the above-mentioned effects of the present invention, the present invention not only directly contributes to lower cost and higher performance of compound semiconductor devices, but also provides an important basis for realizing new multifunctional integrated devices. , the effects of the present invention on electronics in general are extremely large.

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

第1図はシリコン単結晶を基板とする化合物半
導体結晶のエピタキシヤル成長の従来の構造例、
第2図は本発明の一実施例を示す構造図、第3図
は本発明におけける第1の遷移層と第2の遷移層
との界面で格子定数の完全連続条件を説明するた
めの図、第4図は本発明の他の実施例を示す構造
図である。 3…Si基板、4…第1の遷移層(Si1-xGex)、
5…第2の遷移層(In1-yGayP)、6…Si基板、7
…第1の遷移層(Si1-xGex)、8…第2の遷移層
(In1-yGayP)、9…第3の遷移層(GaAs;Cr添
加)、10…活性層(GaAs)、11…ゲート電
極、12…ソース電極、13…ドレイン電極。
Figure 1 shows a conventional structural example of epitaxial growth of a compound semiconductor crystal using a silicon single crystal as a substrate.
FIG. 2 is a structural diagram showing one embodiment of the present invention, and FIG. 3 is a structural diagram for explaining the perfect continuity condition of the lattice constant at the interface between the first transition layer and the second transition layer in the present invention. 4 are structural diagrams showing other embodiments of the present invention. 3... Si substrate, 4... First transition layer (Si 1-x Ge x ),
5... Second transition layer (In 1-y Ga y P), 6... Si substrate, 7
...First transition layer (Si 1-x Ge x ), 8... Second transition layer (In 1-y Ga y P), 9... Third transition layer (GaAs; Cr added), 10... Active layer (GaAs), 11...gate electrode, 12...source electrode, 13...drain electrode.

Claims (1)

【特許請求の範囲】 1 シリコン結晶基板と、当該シリコン結晶基板
上にエピタキシヤル成長されたものであつて組成
比xがシリコン結晶基板との界面からテーパ状ま
たはステツプ状に増加変化するSi1-xGexの第1の
遷移層と、当該第1の遷移層上にエピタキシヤル
成長されたものであつて組成比yが第1の遷移層
との界面からテーパ状またはステツプ状に減少変
化するIn1-yGayPの第2の遷移層とを備え、当該
第2の遷移層上にGaAs系の素子またはGaAs系の
集積回路を構成することを特徴とする化合物半導
体装置。 2 In1-yGayPの第2の遷移層がCr、Fe等の不純
物添加により半絶縁性化されたものであることを
特徴とする特許請求の範囲第1項記載の化合物半
導体装置。 3 シリコン結晶基板と、当該シリコン結晶基板
上にエピタキシヤル成長されたものであつて組成
比xがシリコン結晶基板との界面からテーパ状ま
たはステツプ状に増加変化するSi1-xGexの第1の
遷移層と、当該第1の遷移層上にエピタキシヤル
成長されたものであつて組成比yが第1の遷移層
との界面からテーパ状またはステツプ状に減少変
化するIn1-yGayPの第2の遷移層と、当該第2の
遷移層上に形成されたものであつてCr、Fe等の
不純物を添加した半絶縁性GaAsの第3の遷移層
とを備え、当該第3の遷移層上にGaAs系の素子
またはGaAs系の集積回路を構成することを特徴
とする化合物半導体装置。 4 In1-yGayPの第2の遷移層がCr、Fe等の不純
物添加により半絶縁性化されたものであることを
特徴とする特許請求の範囲第3項記載の化合物半
導体装置。
[Scope of Claims] 1. A silicon crystal substrate, and Si 1- which is epitaxially grown on the silicon crystal substrate and whose composition ratio x increases in a tapered or step-like manner from the interface with the silicon crystal substrate. A first transition layer of x Ge A compound semiconductor device comprising a second transition layer of In 1-y Ga y P, and a GaAs-based element or a GaAs-based integrated circuit is configured on the second transition layer. 2. The compound semiconductor device according to claim 1, wherein the second transition layer of 2 In 1-y Ga y P is made semi-insulating by adding impurities such as Cr and Fe. 3. A silicon crystal substrate and a first layer of Si 1-x Ge x which is epitaxially grown on the silicon crystal substrate and whose composition ratio In 1-y Ga y which is epitaxially grown on the first transition layer and whose composition ratio y decreases in a tapered or step-like manner from the interface with the first transition layer. A second transition layer made of P, and a third transition layer made of semi-insulating GaAs doped with impurities such as Cr and Fe, which is formed on the second transition layer. 1. A compound semiconductor device comprising a GaAs-based element or a GaAs-based integrated circuit on a transition layer. 4. The compound semiconductor device according to claim 3, wherein the second transition layer of In 1-y Ga y P is made semi-insulating by adding impurities such as Cr and Fe.
JP12854280A 1980-09-18 1980-09-18 Compound semiconductor device Granted JPS5753927A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12854280A JPS5753927A (en) 1980-09-18 1980-09-18 Compound semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12854280A JPS5753927A (en) 1980-09-18 1980-09-18 Compound semiconductor device

Publications (2)

Publication Number Publication Date
JPS5753927A JPS5753927A (en) 1982-03-31
JPS6232608B2 true JPS6232608B2 (en) 1987-07-15

Family

ID=14987327

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12854280A Granted JPS5753927A (en) 1980-09-18 1980-09-18 Compound semiconductor device

Country Status (1)

Country Link
JP (1) JPS5753927A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20220112012A (en) * 2021-02-03 2022-08-10 충북대학교 산학협력단 Downward pressure type hip joint dislocation prevention clothing
KR20220112011A (en) * 2021-02-03 2022-08-10 충북대학교 산학협력단 Upward pressure type hip joint dislocation prevention clothing

Families Citing this family (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4529455A (en) * 1983-10-28 1985-07-16 At&T Bell Laboratories Method for epitaxially growing Gex Si1-x layers on Si utilizing molecular beam epitaxy
US4514748A (en) * 1983-11-21 1985-04-30 At&T Bell Laboratories Germanium p-i-n photodetector on silicon substrate
JPS60231333A (en) * 1984-04-27 1985-11-16 Sanyo Electric Co Ltd Semiconductor structure
JPS61107719A (en) * 1984-10-31 1986-05-26 Matsushita Electric Ind Co Ltd Si substrate provided with iii-v compound single crystal thin film and manufacture thereof
JPS61107721A (en) * 1984-10-31 1986-05-26 Matsushita Electric Ind Co Ltd Si substrate provided with iii-v compound single crystal thin film and manufacture thereof
JPH0669113B2 (en) * 1986-04-23 1994-08-31 株式会社日立製作所 Semiconductor laser device
US5011550A (en) * 1987-05-13 1991-04-30 Sharp Kabushiki Kaisha Laminated structure of compound semiconductors
JPS63310111A (en) * 1987-06-12 1988-12-19 Hitachi Cable Ltd Compound semiconductor wafer and its manufacture
US5221413A (en) * 1991-04-24 1993-06-22 At&T Bell Laboratories Method for making low defect density semiconductor heterostructure and devices made thereby
JPH0567769A (en) * 1991-09-05 1993-03-19 Sony Corp Three-dimensional photoelectronic integrated circuit device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20220112012A (en) * 2021-02-03 2022-08-10 충북대학교 산학협력단 Downward pressure type hip joint dislocation prevention clothing
KR20220112011A (en) * 2021-02-03 2022-08-10 충북대학교 산학협력단 Upward pressure type hip joint dislocation prevention clothing

Also Published As

Publication number Publication date
JPS5753927A (en) 1982-03-31

Similar Documents

Publication Publication Date Title
US4500388A (en) Method for forming monocrystalline semiconductor film on insulating film
JP2516604B2 (en) Method for manufacturing complementary MOS integrated circuit device
JPS6232608B2 (en)
US4292374A (en) Sapphire single crystal substrate for semiconductor devices
US4568905A (en) Magnetoelectric transducer
JPS5946414B2 (en) compound semiconductor device
JPH01722A (en) Manufacturing method of semiconductor base material
JPS58158967A (en) Silicon thin film transistor
JPS6232609B2 (en)
JPS61189621A (en) Compound semiconductor device
JPS5856322A (en) Manufacture of semiconductor substrate
JPH11233440A (en) Semiconductor device
JPH0475649B2 (en)
JPS6353711B2 (en)
US5254211A (en) Method for forming crystals
EP0284434A2 (en) Method of forming crystals
JPH04373121A (en) Method for manufacturing crystalline base material
JPH0435019A (en) Thin film transistor
JPS62158314A (en) Compound semiconductor single crystal thin film substrate
JPH0113210B2 (en)
JP3246067B2 (en) Field effect transistor wafer and transistor
JP2592929B2 (en) Optoelectronic integrated circuit manufacturing method
JPH01194315A (en) Silicon carbide semiconductor element
JPH0344937A (en) Bipolar transistor and manufacture thereof
JPS59191393A (en) Semiconductor device