JPH0458177B2 - - Google Patents
Info
- Publication number
- JPH0458177B2 JPH0458177B2 JP58096221A JP9622183A JPH0458177B2 JP H0458177 B2 JPH0458177 B2 JP H0458177B2 JP 58096221 A JP58096221 A JP 58096221A JP 9622183 A JP9622183 A JP 9622183A JP H0458177 B2 JPH0458177 B2 JP H0458177B2
- Authority
- JP
- Japan
- Prior art keywords
- etching
- plasma
- gas
- semiconductor
- gaas
- 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 - Lifetime
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Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/01—Manufacture or treatment
- H10D84/02—Manufacture or treatment characterised by using material-based technologies
- H10D84/05—Manufacture or treatment characterised by using material-based technologies using Group III-V technology
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/01—Manufacture or treatment
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/80—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers characterised by the integration of at least one component covered by groups H10D12/00 or H10D30/00, e.g. integration of IGFETs
- H10D84/82—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers characterised by the integration of at least one component covered by groups H10D12/00 or H10D30/00, e.g. integration of IGFETs of only field-effect components
- H10D84/83—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers characterised by the integration of at least one component covered by groups H10D12/00 or H10D30/00, e.g. integration of IGFETs of only field-effect components of only insulated-gate FETs [IGFET]
- H10D84/84—Combinations of enhancement-mode IGFETs and depletion-mode IGFETs
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/80—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers characterised by the integration of at least one component covered by groups H10D12/00 or H10D30/00, e.g. integration of IGFETs
- H10D84/86—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers characterised by the integration of at least one component covered by groups H10D12/00 or H10D30/00, e.g. integration of IGFETs of Schottky-barrier gate FETs
Landscapes
- Semiconductor Lasers (AREA)
- Drying Of Semiconductors (AREA)
- Junction Field-Effect Transistors (AREA)
Description
【発明の詳細な説明】
(a) 発明の技術分野
本発明は半導体装置の製造方法、特にガリウム
又は砒素を含む化合物半導体層の極めて高精度な
エツチング方法に関する。DETAILED DESCRIPTION OF THE INVENTION (a) Technical Field of the Invention The present invention relates to a method for manufacturing a semiconductor device, and particularly to a method for etching a compound semiconductor layer containing gallium or arsenic with extremely high precision.
(b) 技術の背景
情報処理装置などの能力及びコストパフオーマ
ンスの一層の向上を志向して、半導体装置の高速
化及び低消費電力化が推進されている現在、キヤ
リアの移動度がシリコン(Si)より遥に大きい砒
化ガリウム(GaAs)などの化合物半導体を用い
るトランジスタが多数提案されている。これら化
合物半導体トランジスタのうちに、変調ドーピン
グを行ない不純物から空間的に分離された電子に
よつてキヤリア移動度の増大を実現しているヘテ
ロ接合型電界効果トランジスタ(以下ヘテロ接合
FETと略称する)がある。(b) Background of the technology At present, with the aim of further improving the performance and cost performance of information processing equipment, semiconductor devices are becoming faster and lower in power consumption. Many transistors using much larger compound semiconductors such as gallium arsenide (GaAs) have been proposed. Among these compound semiconductor transistors, heterojunction field effect transistors (hereinafter referred to as heterojunction field effect transistors) achieve an increase in carrier mobility through modulation doping and electrons spatially separated from impurities.
(abbreviated as FET).
また光フアイバ通信など、光を情報信号媒体に
用いるシステムにおいて、半導体レーザ及びフオ
トダイオード等の光半導体装置は最も重要で基本
的な構成要素である。これらの光半導体装置にお
いても、ダブルヘテロ構造の活性層等を量子論的
寸法とする超格子構造によりその特性向上が推進
されている。 Furthermore, in systems that use light as an information signal medium, such as optical fiber communications, optical semiconductor devices such as semiconductor lasers and photodiodes are the most important and fundamental components. In these optical semiconductor devices as well, improvements in their characteristics are being promoted by using a superlattice structure in which the double heterostructure active layer and the like have quantum theoretical dimensions.
以上の例の如く、半導体装置の超微細化は半導
体基体面上のパターンの例えばサブミクロン化の
みならず、半導体基体の厚さ方向についても例え
ば10〔nm〕程度の厚さの制御が必要とされる。 As shown in the above example, the ultra-fine design of semiconductor devices requires not only submicronization of the pattern on the semiconductor substrate surface, but also control of the thickness of the semiconductor substrate to about 10 [nm] in the thickness direction. be done.
(c) 従来技術と問題点
半導体装置の製造工程において半導体基体面上
にパターンを形成するためには、マスク等を用い
て選択的にエツチングが行なわれるが、前記ヘテ
ロ接合FET等においては、一つの半導体層の厚
さ方向の中間の位置までエツチングし、その精度
を例えば10〔nm〕以下に制御することが必要とさ
れることがある。(c) Prior art and problems In order to form a pattern on a semiconductor substrate surface in the manufacturing process of a semiconductor device, selective etching is performed using a mask or the like. It is sometimes necessary to perform etching to a midpoint in the thickness direction of two semiconductor layers and control the etching accuracy to, for example, 10 [nm] or less.
半導体装置の製造工程におけるエツチング方法
として従来より、例えば、GaAS基板に対しては
燐酸(H3PO4)又は弗酸(HF)系溶液等を用い
るウエツトエツチング法が行なわれている。しか
しながらウエツトエツチング法では、エツチング
方向の選択性が通常は少なくサイドエツチングが
大きく進行してパター精度が大幅に低下しまたエ
ツチング深さを均一にかつ精密に制御することは
極めて困難である。 Conventionally, as an etching method in the manufacturing process of semiconductor devices, for example, a wet etching method using a phosphoric acid (H 3 PO 4 ) or hydrofluoric acid (HF) based solution has been performed on GaAS substrates. However, in the wet etching method, selectivity in the etching direction is usually low, and side etching progresses to a large extent, resulting in a significant drop in putter accuracy, and it is extremely difficult to uniformly and precisely control the etching depth.
半導体基体面上のパターン精度を向上し、かつ
工程を合理化する目的からウエツトエツチング法
に代るドライエツチング法への転換が進められて
いる。 For the purpose of improving pattern accuracy on the surface of a semiconductor substrate and streamlining the process, the wet etching method is being replaced by a dry etching method.
ドライエツチング法の技術には、そのエツチン
グ機構が化学的作用によるもの、物理的作用によ
るもの並びに化学及び物理的作用によるものが含
まれる。 Dry etching techniques include those in which the etching mechanism is based on chemical action, physical action, and chemical and physical action.
化学的ドライエツチング方法の例にはプラズマ
エツチング方法があげられる。通常プラズマエツ
チングで用いられる低温ガスプラズマは、反応管
中に適当な反応性ガスを0.1及至10〔Torr〕程度
に導入し、これに高周波電力を印加することによ
つて得られている。このガスプラズマの電離度は
通常小さいが、各種の衝突過程によつて励起状態
となつた原子や分子が多く含まれる。この励起状
態にある原子や分子は化学的な活性が高く、ガス
プラズマが接する試料表面では原子との間に化学
反応が起こり、この結果揮発性の反応物が生成さ
れると、試料表面から原子が取り去られてエツチ
ングされる。 An example of a chemical dry etching method is a plasma etching method. The low-temperature gas plasma normally used in plasma etching is obtained by introducing a suitable reactive gas into a reaction tube at a pressure of about 0.1 to 10 [Torr] and applying high-frequency power to it. Although the degree of ionization of this gas plasma is usually low, it contains many atoms and molecules that have become excited through various collision processes. Atoms and molecules in this excited state have high chemical activity, and a chemical reaction occurs between them on the sample surface that comes into contact with the gas plasma. As a result, volatile reactants are generated, and the atoms and molecules are removed from the sample surface. is removed and etched.
このプラズマエツチング方法は通常被処理材料
に対する選択性に富み、そのエツチング方向は等
方的である。 This plasma etching method is usually highly selective to the material to be processed, and the etching direction is isotropic.
一方、物理的ドライエツチング方法とは大きな
運動エネルギーをもつた粒子、通常はイオンを固
体表面に衝突させたときに生ずるスパツタリング
現象を利用するエツチング法である。この方法は
方向の揃つた一様な入射イオンビームを用いるこ
とによつてマスク下のアンダーカツトを抑制する
ことができるが、被処理材料についての選択性に
乏しく、またイオンの衝撃による半導体基体への
ダメージに留意する必要がある。 On the other hand, the physical dry etching method is an etching method that utilizes the sputtering phenomenon that occurs when particles with large kinetic energy, usually ions, collide with a solid surface. This method can suppress undercuts under the mask by using a uniform incident ion beam with a uniform direction, but it has poor selectivity with respect to the material to be processed, and the ion bombardment may cause damage to the semiconductor substrate. It is necessary to pay attention to the damage caused by
前記スパツタエツチング方法においては不活性
ガスが用いられるが、これを反応性ガスとするこ
とによつて化学反応及びスパツタリング効果が共
存して、被処理材料及びエツチング方向に関する
選択性が得られる。このエツチング方法はリアク
テイブイオンエツチング又はリアクテイブスパツ
タエツチングなどと呼ばれる。 Although an inert gas is used in the sputter etching method, by using this as a reactive gas, a chemical reaction and a sputtering effect coexist, and selectivity with respect to the material to be processed and the etching direction can be obtained. This etching method is called reactive ion etching or reactive sputter etching.
以上説明した各種のドライエツチング法のうち
GaAs化学物半導体に適用された例としては、塩
素系又は弗素系ガスを用いたリアクテイブイオン
エツチング法及び水素(H2)ガスを用いたプラ
ズマエツチング法などが知られている。 Among the various dry etching methods explained above,
As examples applied to GaAs chemical semiconductors, there are known reactive ion etching methods using chlorine-based or fluorine-based gases, and plasma etching methods using hydrogen (H 2 ) gas.
塩素系又は弗素系ガスを用いるリアクテイブイ
オンエツチング法はそのエツチング速度が通常大
きいため(一般的に数100〔nm/min〕乃至数
〔μm/min〕)、エツチング深さを層の中間で10
〔nm〕程度以下に制御することは一般的に不可能
である。又、この様なガス系では、塩素物又は弗
化物による半導体基体表面の汚染が問題になる場
合が多い。一方、H2ガスによるプラズマエツチ
ング法は表面汚染の影響が少ないと考えられる
が、前記程度にエツチング深さを制御することは
極めて困難である。かつこの方法は先に述べた如
く等方的であつて、パターン形状の制御性も良好
ではない。 Since the reactive ion etching method using chlorine-based or fluorine-based gas usually has a high etching rate (generally from several 100 [nm/min] to several [μm/min]), the etching depth is set to 10% in the middle of the layer.
It is generally impossible to control it to below [nm] level. Furthermore, in such a gas system, contamination of the semiconductor substrate surface by chlorine or fluoride often becomes a problem. On the other hand, although the plasma etching method using H 2 gas is considered to have less influence of surface contamination, it is extremely difficult to control the etching depth to the above degree. Moreover, as mentioned above, this method is isotropic, and the controllability of the pattern shape is not good.
(d) 発明の目的
本発明は前記問題点に対処すべく、ガリウム
(Ga)又は砒素(As)を含む化合物半導体につ
いて、エツチング深さ及び精度を10〔nm〕程度以
下に制御することが可能なエツチング方法を提供
することを目的とする。(d) Purpose of the Invention In order to address the above-mentioned problems, the present invention makes it possible to control the etching depth and accuracy to about 10 [nm] or less for compound semiconductors containing gallium (Ga) or arsenic (As). The purpose of this invention is to provide an etching method.
(e) 発明の構成
本発明の前記目的は、少なくともガリウム又は
砒素を含む化合物半導体層を、イオン化した水素
原子によるリアクテイブイオンエツチング法によ
つてエツチングすることにより達成される。(e) Structure of the Invention The above object of the present invention is achieved by etching a compound semiconductor layer containing at least gallium or arsenic by a reactive ion etching method using ionized hydrogen atoms.
すなわち先に述べたH2ガスを用いるプラズマ
エツチング法においては、エツチング種であるプ
ラズマ中の励起状態の中性水素原子が高濃度であ
るため、本発明の目的に対してはエツチング速度
が過大であるのに対して、本発明のリアクテイブ
イオンエツチング法においては、プラズマ中の中
性水素原子より非常に低濃度であるイオン化した
水素原子を電極上に置れた被処理半導体基体に入
射せしめて、この入射方向のスパツタリング効果
と水素イオンによる化学反応とを利用してエツチ
ングが行なわれるために、エツチング速度は緩徐
であつてエツチング深さの精密な制御が可能とな
りかつパターン形状の精度も極めて良好となる。 In other words, in the plasma etching method using H 2 gas mentioned above, the etching rate is too high for the purpose of the present invention because of the high concentration of excited neutral hydrogen atoms in the plasma as the etching species. On the other hand, in the reactive ion etching method of the present invention, ionized hydrogen atoms, which have a much lower concentration than neutral hydrogen atoms in plasma, are made to enter a semiconductor substrate to be processed placed on an electrode. Since etching is performed using the sputtering effect in the direction of incidence and the chemical reaction caused by hydrogen ions, the etching speed is slow, making it possible to precisely control the etching depth and achieving extremely high precision in pattern shape. becomes.
本発明は第1図に例示する如き通常のリアクテ
イブイオンエツチング装置を使用して実施するこ
とができる。エツチング処理室1内には電極2及
び3が上下に対向して設けられ、ガスが送気管4
及び排気管5によつて導入、排出される。下方の
電極2が絶縁物6によつて支持され、上方の対向
電極3との間に高周波電力が印加されることによ
つて両電極間に、電極2の近傍を除いて、プラズ
マ7が形成される。被処理半導体基体8を電極2
上に置くことによつて先に述べたリアクテイブイ
オンエツチングが行なわれる。 The present invention can be practiced using a conventional reactive ion etching apparatus such as that illustrated in FIG. Electrodes 2 and 3 are provided vertically facing each other in the etching chamber 1, and gas is supplied to the air pipe 4.
and is introduced and discharged through the exhaust pipe 5. The lower electrode 2 is supported by an insulator 6, and high frequency power is applied between it and the upper counter electrode 3, whereby plasma 7 is formed between both electrodes except in the vicinity of the electrode 2. be done. The semiconductor substrate 8 to be processed is connected to the electrode 2
The above-mentioned reactive ion etching is performed by placing it on top.
第2図は本発明のエツチング方法によつて
GaAs半導体層及び砒化アルミニウム・ガリウ
ム・(AlxGa1−xAs)半導体層にエツチング処理
を行なつた場合の、エツチング速度の水素ガス圧
力に対する相関の例を示す図である。ただし本例
のプラズマ周波数13.56〔MHZ〕、電力密度5×
10-2〔W/cm-3〕電磁界によつて生成している。
図において曲線AはGaAs半導体層、曲線Bは
AlxGa1−xAs(x=0.3)半導体層の場合を示す。 Figure 2 shows the etching method of the present invention.
FIG. 3 is a diagram showing an example of the correlation between etching rate and hydrogen gas pressure when etching is performed on a GaAs semiconductor layer and an aluminum arsenide/gallium/(AlxGa1-xAs) semiconductor layer. However, in this example, the plasma frequency is 13.56 [MHZ], and the power density is 5×
10 -2 [W/cm -3 ] Generated by an electromagnetic field.
In the figure, curve A is a GaAs semiconductor layer, and curve B is a GaAs semiconductor layer.
The case of an AlxGa1−xAs (x=0.3) semiconductor layer is shown.
第2図において曲線A及びBはともに水素ガス
圧力5〔Pa〕近傍において極大値を示し、そのと
きのエツチング速度は4〔nm/min〕及び3
〔nm/min〕程度である。この極大値を示す水素
ガス圧力においてプラズマ中のイオン化した水素
原子の比率が極大となり、エツチング処理系は最
も安定する。なお水素ガス圧力が1〔Pa〕程度以
下もしくは50〔Pa〕程度以上であるときにはプラ
ズマ状態が生成されなくなる。 In Fig. 2, curves A and B both show maximum values near the hydrogen gas pressure of 5 [Pa], and the etching rates at that time are 4 [nm/min] and 3 [nm/min].
It is about [nm/min]. At this maximum hydrogen gas pressure, the ratio of ionized hydrogen atoms in the plasma becomes maximum, and the etching system becomes most stable. Note that when the hydrogen gas pressure is about 1 [Pa] or less or about 50 [Pa] or more, no plasma state is generated.
この様に例えば4〔nm/min〕程度のエツチン
グ速度が高い安定性をもつて実現されることによ
り、10〔nm〕以下の精度をもつエツチング深さの
制御を容易に行なうことが可能となる。 In this way, for example, by achieving an etching rate of about 4 [nm/min] with high stability, it becomes possible to easily control the etching depth with an accuracy of 10 [nm] or less. .
(f) 発明の実施例
以下本発明の実施例を図面を参照して具体的に
説明する。(f) Embodiments of the invention Examples of the invention will be specifically described below with reference to the drawings.
第3図a乃至cはヘテロ操合FETの製造工程
に本発明を実施した例を示す断面図である。第3
図a参照
半絶縁性GaAs基板11上に、ノンドープの
GaAs12を厚さ例えば300〔nm〕程度に、
シリコン(Si)を例えば1×1013〔cm-3〕程度に
ドープしたn型Al0.3Ga0.7As13を例えば厚さ
20〔nm〕程度に、Alの組成比xが0.3から0まで
次第に減少するn型AlxGa1−xAs層14を例え
ば厚さ20〔nm〕程度に、n型GaAs層15を例え
ば厚さ40〔nm〕程度に順次分子線エピタキシヤル
成長法等によつて成長させる。16はノンドープ
のGaAs層2のn型Al0.3Ga0.7As層13とのヘテ
ロ接合界面近傍に形成される2次元電子ガスであ
る。 FIGS. 3a to 3c are cross-sectional views showing an example in which the present invention is implemented in the manufacturing process of a hetero-operated FET. Third
See figure a. On the semi-insulating GaAs substrate 11, a non-doped
GaAs12 to a thickness of about 300 [nm], for example,
N-type Al0.3Ga0.7As13 doped with silicon (Si) to, for example, about 1×10 13 [cm -3 ] is
The n-type AlxGa1-xAs layer 14, in which the Al composition ratio x gradually decreases from 0.3 to 0, has a thickness of about 20 [nm], and the n-type GaAs layer 15 has a thickness of, for example, 40 [nm]. ] by molecular beam epitaxial growth method or the like. A two-dimensional electron gas 16 is formed near the heterojunction interface between the non-doped GaAs layer 2 and the n-type Al0.3Ga0.7As layer 13.
次いでソース電極17及び17′、並びにドレ
イン電極18及び18′を例えば金・ゲルマニウ
ム/金(AuGe/Au)を用いて形成し、加熱処
理を行なつてn型GaAs層15などと合金化する
ことによつて、低抵抗のオーミツク接続領域19
が形成される。また素子間分離領域20を例えば
酸素(O2)のイオン注入によつて形成する。第
3図b参照
ゲート閾値電圧の制御を目的として、n型
GaAs層15のゲート領域にマスクを用いて選択
的なエツチングを行なう。本実施例においては、
例えば二酸化シリコン(SiO2)膜によつてマス
ク21を設けて、デイプリーシヨンモードFET
のゲート領域22については深さ約10〔nm〕、エ
ンハンスメントモードFETのゲート領域23に
ついては深さ約30〔nm〕のエツチングを本発明に
より、H2ガス圧力約5〔Pa〕、高周波電力密度約
4×10-2〔W/cm3〕の条件で実施している。 Next, source electrodes 17 and 17' and drain electrodes 18 and 18' are formed using, for example, gold-germanium/gold (AuGe/Au), and heat-treated to alloy with the n-type GaAs layer 15 and the like. The low resistance ohmic connection region 19
is formed. Further, the element isolation region 20 is formed by, for example, ion implantation of oxygen (O 2 ). See Figure 3b. For the purpose of controlling the gate threshold voltage,
Selective etching is performed on the gate region of GaAs layer 15 using a mask. In this example,
For example, by providing a mask 21 with a silicon dioxide (SiO 2 ) film, the depletion mode FET
According to the present invention, the gate region 22 of the enhancement mode FET is etched to a depth of about 10 [nm], and the gate region 23 of the enhancement mode FET is etched to a depth of about 30 [nm]. The test was carried out under conditions of approximately 4×10 -2 [W/cm 3 ].
高周波電力を例えば2倍にすればエツチング速
度が大略1.5倍程度となるなどエツチング速度は
高周波電力にも支配されるが、電力が過少となれ
ばプラズマが安定して形成されずまた過大となれ
ば被処理半導体基体に強いダメージを与えるため
に、高周波電力密度が1×10-2乃至4×10-1
〔W/cm- 3〕程度の範囲内で上記の要因などを考
慮して最適値を選択する。またH2ガスに不活性
ガスを添加することによつてプラズマ形成及びエ
ツチング速度などの制御の自由度が拡大される
が、本実施例のヘテロ接合型FETの如く極めて
薄い半導体層によつて構成される半導体基体を主
たる対象とする本発明においては、スパツタリン
グ効果によつて被処理半導体基体にダメージを与
えないことが特に重要である。第3図c参照
グート電極24及び24′をゲート領域の前記
エツチング面上に例えばアルミニウム(Al)に
よつて形成する。 For example, if the high frequency power is doubled, the etching speed will be approximately 1.5 times. Etching speed is also controlled by the high frequency power, but if the power is too low, plasma will not be formed stably, and if the power is too high, the etching speed will be approximately 1.5 times. In order to cause strong damage to the semiconductor substrate to be processed, the high frequency power density is 1×10 -2 to 4×10 -1.
The optimum value is selected within a range of approximately [W/cm - 3 ], taking into consideration the above factors. Furthermore, by adding an inert gas to the H 2 gas, the degree of freedom in controlling plasma formation, etching rate, etc. is expanded. In the present invention, whose main object is a semiconductor substrate to be processed, it is particularly important not to damage the semiconductor substrate to be processed by the sputtering effect. Referring to FIG. 3c, gate electrodes 24 and 24' are formed of, for example, aluminum (Al) on the etched surface of the gate region.
本実施例のゲート閾値電圧は、デイプリーシヨ
ンモードFETについて約−0.5〔V〕、エンハンス
メントモードFETについてほぼ0〔V〕であつ
て、素子相互間及び面内の分布は従来に比較して
大幅に改善されている。 The gate threshold voltage of this example is approximately -0.5 [V] for the depletion mode FET and approximately 0 [V] for the enhancement mode FET, and the distribution between elements and within the plane is significantly larger than that of the conventional one. has been improved.
以上の説明並びに実施例は半導体材料として
GaAs及びAlGaAsを引例しているが、本発明に
よつて、例えばガリウム・アンチモン(GaSb)
ガリウム・燐(GaP)、インジウム・砒素
(InAs)或いはガリウム・インジウム・砒素
(GaInAs)等のガリウムもしくは砒素を含む化
合物半導体についても同様の効果が得られる。 The above explanation and examples are used as semiconductor materials.
Although reference is made to GaAs and AlGaAs, the present invention provides for example gallium antimony (GaSb).
Similar effects can be obtained with compound semiconductors containing gallium or arsenic, such as gallium-phosphorus (GaP), indium-arsenic (InAs), or gallium-indium-arsenic (GaInAs).
(g) の効果
以上説明した如く本発明によれば、ガリウム又
は砒素を含む化合物半導体層のエツチングに際し
て、その深さを10〔nm〕程度以下の精度に容易に
制御することができ、かつその均一性は良好であ
り、更にパターン精度も優れていて、例えばヘテ
ロ接合FET等について要求される量子論的寸法
の工業的実施に大きく寄与する。Effect (g) As explained above, according to the present invention, when etching a compound semiconductor layer containing gallium or arsenic, the depth can be easily controlled to an accuracy of about 10 [nm] or less, and the etching depth can be easily controlled to an accuracy of about 10 [nm] or less. The uniformity is good, and the pattern accuracy is also excellent, which greatly contributes to the industrial implementation of quantum-theoretical dimensions required for, for example, heterojunction FETs.
第1図は本発明の実施に用いるエツチング装置
の例を示す断面図、第2図はエツチング速度と水
素ガス圧力との相関の例を示す図、第3図a乃至
cは本発明の実施例を示す断面図である。
図において、11はGaAs基板、12はノンド
ープのGaAs層、13はn型AlGaAs層、14は
n型グレーデツドAlGaAs層、15はn型GaAs
層、16は2次元電子ガス、17及び17′はソ
ース電極、18及び18′はドレイン電極、19
はオーミツク接続領域、20は素子間分離領域、
21はマスク、22及び23はゲート領域、24
及び24′はゲート電極を示す。
FIG. 1 is a cross-sectional view showing an example of an etching apparatus used to carry out the present invention, FIG. 2 is a diagram showing an example of the correlation between etching rate and hydrogen gas pressure, and FIGS. 3 a to 3 c are examples of the present invention. FIG. In the figure, 11 is a GaAs substrate, 12 is a non-doped GaAs layer, 13 is an n-type AlGaAs layer, 14 is an n-type graded AlGaAs layer, and 15 is an n-type GaAs layer.
layer, 16 is a two-dimensional electron gas, 17 and 17' are source electrodes, 18 and 18' are drain electrodes, 19
20 is an ohmic connection region, 20 is an inter-element isolation region,
21 is a mask, 22 and 23 are gate regions, 24
and 24' indicate a gate electrode.
Claims (1)
導体層を、イオン化した水素原子によるリアクテ
イブイオンエツチング法によつてエツチングする
工程を含んでなることを特徴とする半導体装置の
製造方法。 2 前記化合物半導体が砒化ガリウム及び砒化ア
ルミニウムの少なくとも一つであることを特徴と
する特許請求の範囲第1項記載の半導体装置の製
造方法。Claims: 1. A method for manufacturing a semiconductor device, comprising the step of etching a compound semiconductor layer containing at least gallium or arsenic by a reactive ion etching method using ionized hydrogen atoms. 2. The method of manufacturing a semiconductor device according to claim 1, wherein the compound semiconductor is at least one of gallium arsenide and aluminum arsenide.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58096221A JPS59220927A (en) | 1983-05-31 | 1983-05-31 | Manufacture of semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58096221A JPS59220927A (en) | 1983-05-31 | 1983-05-31 | Manufacture of semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59220927A JPS59220927A (en) | 1984-12-12 |
| JPH0458177B2 true JPH0458177B2 (en) | 1992-09-16 |
Family
ID=14159176
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58096221A Granted JPS59220927A (en) | 1983-05-31 | 1983-05-31 | Manufacture of semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59220927A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0690506B1 (en) * | 1994-06-29 | 1999-09-08 | Laboratoires D'electronique Philips S.A.S. | Method of fabrication of a semiconductor device comprising at least two field-effect transistors having a different pinch-off voltage |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5845174B2 (en) * | 1979-03-05 | 1983-10-07 | 日本電信電話株式会社 | 3↓-Method for forming an insulating film on a Group 5 compound semiconductor |
| US4361461A (en) * | 1981-03-13 | 1982-11-30 | Bell Telephone Laboratories, Incorporated | Hydrogen etching of semiconductors and oxides |
-
1983
- 1983-05-31 JP JP58096221A patent/JPS59220927A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59220927A (en) | 1984-12-12 |
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