JPS6314871B2 - - Google Patents
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- Publication number
- JPS6314871B2 JPS6314871B2 JP57230091A JP23009182A JPS6314871B2 JP S6314871 B2 JPS6314871 B2 JP S6314871B2 JP 57230091 A JP57230091 A JP 57230091A JP 23009182 A JP23009182 A JP 23009182A JP S6314871 B2 JPS6314871 B2 JP S6314871B2
- Authority
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- Prior art keywords
- implantation
- approximately
- dose
- gaas substrate
- conductivity
- Prior art date
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Classifications
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/80—FETs having rectifying junction gate electrodes
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- Semiconductor Integrated Circuits (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に係り、特にガ
リウム・砒素(GaAs)集積回路装置における抵
抗素子の形成方法に関する。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 forming a resistive element in a gallium arsenide (GaAs) integrated circuit device.
(b) 従来技術と問題点
超高速デイジタル回路或いは超高周波信号処理
の実現のため、シリコン(Si)より易動度が数倍
大きいGaAsを用いた集積回路装置の実用化が進
められている。(b) Prior Art and Problems In order to realize ultra-high-speed digital circuits or ultra-high frequency signal processing, integrated circuit devices using GaAs, which has mobility several times higher than silicon (Si), are being put into practical use.
かかる超高速或いは超高波用GaAs半導体装置
は、GaAs結晶基板表面のごく浅い表層部にトラ
ンジスタや抵抗素子が形成される。ところが
GaAs基板の表層部は、GaAs基板内の残留不純
物等の影響及び基板表面に保護膜を形成するに伴
つて生じた表面準位によつて引き起された表面空
乏層の影響を強く受ける。抵抗素子は半絶縁性
GaAs基板表面に通常n型不純物のシリコン
(Si)イオン等を注入して形成するが、これの抵
抗値制御は上述の問題があるため必ずしも容易と
は言えない。 In such a GaAs semiconductor device for ultra-high speed or ultra-high waves, transistors and resistance elements are formed in a very shallow surface layer of the surface of a GaAs crystal substrate. However
The surface layer of a GaAs substrate is strongly influenced by residual impurities in the GaAs substrate and by a surface depletion layer caused by surface states generated when a protective film is formed on the substrate surface. Resistance element is semi-insulating
It is usually formed by implanting n-type impurity silicon (Si) ions or the like into the surface of a GaAs substrate, but controlling the resistance value thereof is not necessarily easy due to the above-mentioned problems.
第1図は従来のGaAs半導体装置の製造方法を
製造工程の順に示す要部断面図である。以下同図
を参照しながら上述の問題点を説明する。 FIG. 1 is a cross-sectional view of a main part showing a conventional method for manufacturing a GaAs semiconductor device in the order of manufacturing steps. The above-mentioned problems will be explained below with reference to the same figure.
同図aにおいて、1は半絶縁性GaAs基板、2
は第1のフオトレジスト膜である。上記GaAs基
板1はクローム(Cr)を凡そ0.1〔ppm〕の濃度に
ドープして半絶縁性基板としたものを用いる。こ
のGaAs基板1に第1のフオトレジスト膜2をマ
スクとして、注入エネルギ凡そ60〔KeV〕,ドー
ズ量約0.8〔cm-2〕でシリコン(Si)イオンを選択
的に注入する。3はSiイオン注入領域を示す。 In the same figure a, 1 is a semi-insulating GaAs substrate, 2
is the first photoresist film. The GaAs substrate 1 is a semi-insulating substrate doped with chromium (Cr) to a concentration of approximately 0.1 [ppm]. Using the first photoresist film 2 as a mask, silicon (Si) ions are selectively implanted into this GaAs substrate 1 at an implantation energy of about 60 [KeV] and a dose of about 0.8 [cm -2 ]. 3 indicates the Si ion implantation region.
次いで同図bに見られる如く、上記第1のフオ
トレジスト膜2に変えて第2のフオトレジスト膜
4を形成し、これをマスクとして再びSiイオンの
注入を行う。本工程においては、注入エネルギ凡
そ120〔KeV〕,ドーズ量は凡そ3×1012〔cm-2〕と
する。5は本工程におけるSiイオン注入領域を示
す。 Next, as shown in FIG. 1B, a second photoresist film 4 is formed in place of the first photoresist film 2, and using this as a mask, Si ions are implanted again. In this step, the implantation energy is approximately 120 [KeV] and the dose is approximately 3×10 12 [cm -2 ]. 5 shows the Si ion implantation region in this step.
次いで同図cに示すように、Siイオン注入領域
3表面にタングステン・シリサイド(WSi)より
なるシヨツトキゲート電極6を形成し、更に上記
Siイオン注入領域3及び5部と開口部とする二酸
化シリコン(SiO2)膜7を形成し、これと前記
シヨツトキゲート電極6とをマスクとして再度Si
イオン注入を行う。本工程においては、注入エネ
ルギを凡そ200〔KeV〕、ドーズ量凡そ2×1013〔cm
-2〕とする。8は本工程におけるSiイオン注入領
域である。 Next, as shown in Figure c, a shot gate electrode 6 made of tungsten silicide (WSi) is formed on the surface of the Si ion implanted region 3, and then
A silicon dioxide (SiO 2 ) film 7 is formed to form openings in the Si ion implantation regions 3 and 5, and the SiO 2 film is re-injected using this and the shot gate electrode 6 as a mask.
Perform ion implantation. In this process, the implantation energy is approximately 200 [KeV] and the dose is approximately 2×10 13 [cm
-2 ]. 8 is a Si ion implantation region in this step.
次いで同図dに示す如く、上記SiO2膜7を除
去し、窒化アルミニウム(AlN)膜(図示せず)
を形成し、これを保護膜として凡そ800〔℃〕お温
度で約15分間の加熱処理を行い、上記Siイオン注
入領域3,5,及び8内に注入されたSiイオンを
活性化して、n+型のソース及びドレイン領域9,
9′、n型の活性層10、n+型のコンタクト領域
11、n型の抵抗層12を形成する。 Next, as shown in FIG. d, the SiO 2 film 7 is removed and an aluminum nitride (AlN) film (not shown) is removed.
is formed, and this is used as a protective film to perform heat treatment for about 15 minutes at a temperature of about 800 [°C] to activate the Si ions implanted in the Si ion implanted regions 3, 5, and 8. + type source and drain regions 9;
9', an n-type active layer 10, an n + type contact region 11, and an n-type resistance layer 12 are formed.
次いで上記AlN膜を除去した後、n型GaAs結
晶に対してオーミツク接触を形成する金・ゲルマ
ニウム―金(AuGe―Au)よりなるソース,ド
レイン電極13,13′及び抵抗の端子電極14,
14′をリフトオフ法により形成する。さらに上
記各電極上を含むGaAs基板1全面に層間絶縁膜
として例えばSiO2膜15を被着せしめ、これを
選択的に除去してコンタクト窓を開口し、該コン
タクト窓内にて上記各電極に接続するチタン―金
(Ti―Au)よりなる上部配線電極16を選択的
に形成する。 Next, after removing the AlN film, source and drain electrodes 13 and 13' made of gold-germanium-gold (AuGe-Au) and resistor terminal electrodes 14, which form ohmic contact with the n-type GaAs crystal, are formed.
14' is formed by a lift-off method. Furthermore, a SiO 2 film 15, for example, is deposited as an interlayer insulating film on the entire surface of the GaAs substrate 1 including the tops of each of the above electrodes, and this is selectively removed to open a contact window. A connecting upper wiring electrode 16 made of titanium-gold (Ti-Au) is selectively formed.
以上のような方法によりGaAs集積回路装置は
作成されるが、上記従来の製造方法は前述した如
く抵抗層12の制御性が十分ではなかつた。第2
図に上記従来工程により120〔KeV〕のエネルギ
でSiイオンを注入して形成した抵抗層12の抵抗
率と、ドーズ量の関係を示す。同図の横軸はドー
ズ量〔×1012cm-2〕を、また縦軸は左側がシート
導電率〔KΩ□-1〕,右側がシート抵抗率
〔KΩ□〕を示す。 Although a GaAs integrated circuit device is manufactured by the method described above, the conventional manufacturing method described above does not provide sufficient controllability of the resistive layer 12. Second
The figure shows the relationship between the resistivity and the dose of the resistive layer 12 formed by implanting Si ions at an energy of 120 [KeV] using the conventional process described above. The horizontal axis of the figure shows the dose [×10 12 cm -2 ], and the vertical axis shows the sheet conductivity [KΩ□ -1 ] on the left and the sheet resistivity [KΩ□] on the right.
抵抗層12の導電率は本来ならばドーズ量に比
例し、従つて両者の関係は第2図の原点を通る直
線で示されるべきものである。しかしながら実際
には同図の実線Aに見られる如く、両者の関係を
示す直線の延長線は原点をはずれ、抵抗率はドー
ズ量が少ない場合には理論値よりもはるかに高い
値となる。これはGaAs基板内の残留不純物等の
影響により、低ドーズ注入時には見掛け上の不活
性化が起こつていること、及び前記第1図dに示
したSiO2膜15とGaAs基板1との界面に生じた
表面準位によつて表面空乏層が形成されることに
起因するものである。 The electrical conductivity of the resistive layer 12 is originally proportional to the dose, and therefore the relationship between the two should be shown by a straight line passing through the origin in FIG. However, in reality, as shown by the solid line A in the figure, the extension of the straight line showing the relationship between the two deviates from the origin, and the resistivity takes a value much higher than the theoretical value when the dose is small. This is because apparent inactivation occurs during low-dose implantation due to the influence of residual impurities in the GaAs substrate, and because the interface between the SiO 2 film 15 and GaAs substrate 1 shown in FIG. This is due to the formation of a surface depletion layer by the generated surface states.
このような理由により導電率は低ドーズ注入時
に非直線的となり、ある閾値を越えて始めて導電
性を示す〔実線A〕ことになる。また導電率とド
ーズ量とが直線関係からはずれる場合〔一点鎖線
B〕もあり、更に製造ロツトが異なると、比例定
数が異なる(実線AとC〕場合も生じる。 For these reasons, conductivity becomes non-linear during low-dose implantation, and conductivity is exhibited only after a certain threshold value is exceeded [solid line A]. In addition, there are cases where the conductivity and the dose deviate from the linear relationship (dotted chain line B), and there are also cases where the constant of proportionality differs depending on the manufacturing lot (solid lines A and C).
このように従来の製造方法においては、抵抗層
12は抵抗率の制御性、再現性が悪く、このため
所望の電気的特性を有するGaAs集積回路装置を
製作することは必ずしも容易とは言えなかつた。 As described above, in the conventional manufacturing method, the controllability and reproducibility of the resistivity of the resistive layer 12 is poor, and therefore it is not necessarily easy to manufacture a GaAs integrated circuit device having desired electrical characteristics. .
(c) 発明の目的
本発明の目的は上記問題点を解消して、半絶縁
性GaAs基板に所望の抵抗素子を安定且つ容易に
形成し得る半導体装置の製造方法を提供すること
にある。(c) Object of the Invention An object of the present invention is to solve the above-mentioned problems and provide a method for manufacturing a semiconductor device in which a desired resistance element can be stably and easily formed on a semi-insulating GaAs substrate.
(d) 発明の構成
本発明の特徴は、半絶縁性ガリウム・砒素基板
の所望の領域に、当該ガリウム・砒素基板の表面
から凡そ0.05〔μm〕以下の深さに濃度分布のピー
クが位置する如く、シリコン・イオンを0.5〜1.0
×1012〔cm-2〕のドーズ量で注入する工程と、前
記所望の領域に当該ガリウム・砒素基板の表面か
ら凡そ0.05〔μm〕以上の深さに濃度分布のピーク
が位置する如く所定のn型不純物イオンを注入す
る工程と、前記注入されたイオンを活性化する工
程とを有する抵抗素子の形成工程を含むことにあ
る。(d) Structure of the Invention The present invention is characterized in that the peak of the concentration distribution is located in a desired region of a semi-insulating gallium/arsenic substrate at a depth of approximately 0.05 [μm] or less from the surface of the gallium/arsenic substrate. Like, silicon ion 0.5~1.0
A step of implanting at a dose of ×10 12 [cm -2 ] and a predetermined implantation step in which the peak of the concentration distribution is located at a depth of about 0.05 [μm] or more from the surface of the gallium/arsenic substrate in the desired region. The present invention includes a step of forming a resistor element including a step of implanting n-type impurity ions and a step of activating the implanted ions.
(e) 発明の実施列
本発明は上記従来の問題点がGaAs基板表面の
影響に起因することに鑑み、この表面の影響を
種々検討の結果なされたもので、GaAs基板表面
の影響を極力減殺すること、及び表面の影響の及
ばない領域に導電層を形成することにより、
GaAs基板上に抵抗素子を、良好な再現性及び制
御性をもつて形成し得るようにしたものである。(e) Implementation sequence of the invention In view of the fact that the above conventional problems are caused by the influence of the surface of the GaAs substrate, the present invention was made as a result of various studies on the influence of this surface, and the influence of the GaAs substrate surface is reduced as much as possible. and by forming a conductive layer on unaffected areas of the surface.
This allows a resistor element to be formed on a GaAs substrate with good reproducibility and controllability.
以下本発明の一実施列を上述の検討結果ととも
に、図面を参照しながら説明する。 Hereinafter, one embodiment of the present invention will be explained together with the above-mentioned study results with reference to the drawings.
第3図は導電層形成のためのイオン注入を行う
際の、注入エネルギ(即ち導電層の形成深さ)と
得られた導電層の導電率のバラツキとの関係を示
す図である。同図の横軸は注入エネルギ〔KeV〕
を、縦軸は導電率のバラツキで、導電率の平均値
xに対する標準偏差σとの比をもつて示す。なお
同図の試料のイオン注入は、GaAs基板表面が露
出した状態で行なつた。また注入するイオン種は
Siを用い、ドーズ量は凡そ3×1012〔cm-2〕で行
なつた。 FIG. 3 is a diagram showing the relationship between the implantation energy (that is, the formation depth of the conductive layer) and the variation in the conductivity of the obtained conductive layer when performing ion implantation for forming the conductive layer. The horizontal axis in the figure is the implantation energy [KeV]
The vertical axis represents the variation in conductivity, which is expressed as the ratio of the standard deviation σ to the average value x of the conductivity. Note that ion implantation for the sample shown in the figure was performed with the surface of the GaAs substrate exposed. Also, the ion species to be implanted are
Si was used at a dose of approximately 3×10 12 [cm −2 ].
同図に示されるように注入エネルギが凡そ100
〔KeV〕以上となると、バラツキはほぼ〔%〕以
下となる。これは注入されたイオン濃度分布のピ
ーク位置Rpを、GaAs基板表面から凡そ0.1〔μm〕
以上とする必要があることを示す。これは逆に見
れば表面の影響の及ぶ深さは、凡そ0.1〔μm〕以
下であることを示唆する。 As shown in the figure, the implantation energy is approximately 100
When it is more than [KeV], the variation becomes almost [%] or less. This means that the peak position Rp of the implanted ion concentration distribution is approximately 0.1 [μm] from the GaAs substrate surface.
Indicates that it is necessary to meet the above requirements. Conversely, this suggests that the depth at which the surface is affected is approximately 0.1 [μm] or less.
第4図はGaAs基板表面の影響を減殺するた
め、GaAs基板表面に予め浅くSiイオンを注入
(以下これを基底注入と称する)しておき、これ
に更に深くSiを注入(導電率制御のための注入と
いう意味から以下これを制御注入と称する)した
場合の効果を示す図である。同図の横軸は凡そ
120〔KeV〕のエネルギにより上記制御注入を行
なつたときのドーズ量を、縦軸は得られた導電層
のシート導電率〔KΩ□-1〕を示す。 Figure 4 shows that in order to reduce the influence of the GaAs substrate surface, Si ions are implanted shallowly into the GaAs substrate surface (hereinafter referred to as base implantation), and then Si is implanted deeper (to control conductivity). 2 is a diagram showing the effect of injection (hereinafter referred to as controlled injection). The horizontal axis of the figure is approximately
The dose when the above-mentioned controlled implantation was performed with an energy of 120 [KeV] is shown, and the vertical axis shows the sheet conductivity [KΩ□ -1 ] of the obtained conductive layer.
上記基底注入として、前記第3図の結果から凡
そ0.1〔μm〕の深さにわたつてSiイオンを注入す
るため、Rpが凡そ0.05〔μm〕の深さとなる注入
エネルギ、即ち凡そ60〔KeV〕により、ドーズ量
凡そ0.8×10〔cm-2〕の注入を行なつた。この試料
に凡そ120〔KeV〕の注入エネルギにより制御注
入を行つたところ、同図に示すように得られた導
電層のシーナ導電率と制御注入のドーズ量との関
係は、ほぼ原点を通る直線関係となつた。 As for the above-mentioned base implantation, since Si ions are implanted to a depth of approximately 0.1 [μm] from the results shown in Fig. 3, the implantation energy that makes Rp approximately 0.05 [μm] deep, that is, approximately 60 [KeV] Accordingly, implantation was performed at a dose of approximately 0.8×10 [cm −2 ]. Controlled implantation was performed on this sample with an implantation energy of approximately 120 [KeV], and as shown in the figure, the relationship between the Sina conductivity of the conductive layer obtained and the dose of controlled implantation was approximately a straight line passing through the origin. It became a relationship.
このことは、GaAs基板表面に適当な基底注入
を行うことにより、表面の影響はほぼ吸収される
こと、及びこの状態で更に深い位置に制御注入を
行なつて導電層を形成すれば、この導電層の導電
率は制御注入のみに決定し得ることを示唆してい
る。 This means that by performing an appropriate base implantation on the surface of the GaAs substrate, the influence of the surface is almost absorbed, and that if a conductive layer is formed by controlled implantation at a deeper position in this state, this conductive layer can be It is suggested that the conductivity of the layer can be determined only by controlled implantation.
第5図は上記第4図の関係を、更に基底注入の
ドーズ量をパラメータとして示して図で、曲線A
は前記第4図と同一であり、ドーズ量は、0.8×
1012〔cm-2〕である。更に曲線B,C,D,E,
Fはドーズ量がそれぞれ0.1×1012,0.5×1012,
1.0×1012,1.5×1012,2.0×1012〔cm-2〕の場合を
示す。これらの曲線に示されるように、ドーズ量
が0.5〜1.0×1012〔cm-2〕の範囲にあれば、導電率
の変動は小さいが、ドーズ量が上記範囲より少な
い場合は表面の影響に対し補償不足となり、多い
場合は補償過剰となり。即ち、結果として上記範
囲をはずれると導電層の導電率は基底注入のドー
ズ量によつて大きく変動し、制御性を失うことと
なる。 FIG. 5 is a diagram showing the relationship shown in FIG. 4 above with the dose amount of base implantation as a parameter, and curve A
is the same as in Figure 4 above, and the dose is 0.8×
10 12 [cm -2 ]. Furthermore, curves B, C, D, E,
F has a dose of 0.1×10 12 , 0.5×10 12 ,
The cases of 1.0×10 12 , 1.5×10 12 , and 2.0×10 12 [cm -2 ] are shown. As shown in these curves, if the dose is in the range of 0.5 to 1.0×10 12 [cm -2 ], the fluctuation in conductivity is small, but if the dose is less than the above range, the surface effect may occur. On the other hand, if there is too much compensation, it will be under-compensated, and if there is too much, it will be over-compensated. That is, as a result, if the above range is exceeded, the conductivity of the conductive layer will vary greatly depending on the dose of the base implantation, and controllability will be lost.
さらに第6図は基底注入の注入エネルギ(即ち
注入深さ)に対するシート導電率のバラツキの関
係を示す図であつて、横軸は注入エネルギ
〔KeV〕、縦軸はシート導電率のバラツキσ/
〔%〕を示す。同図の試料は基底注入のドーズ量
は総て0.8×1012〔cm-2〕とし、基底注入を行なつ
たのち、注入エネルギ凡そ120〔KeV〕にてドー
ズ量凡そ1×1012〔cm-2〕の制御注入を行なつた
ものである。 Furthermore, FIG. 6 is a diagram showing the relationship between the variation in sheet conductivity and the implantation energy (i.e., implantation depth) of basal implantation, where the horizontal axis is the implantation energy [KeV] and the vertical axis is the variation in sheet conductivity σ/
Indicates [%]. For the sample in the same figure, the base implantation dose was 0.8×10 12 [cm -2 ], and after the base implantation, the implantation energy was approximately 120 [KeV] and the dose was approximately 1×10 12 [cm -2 ]. -2 ] was carried out using a controlled injection.
同図に見られる如く基底注入時の注入エネルギ
が増大するにつれて導電率のバラツキは増大す
る。このバラツキは実用上凡そ5〔%〕以下とす
ると、基底注入の注入エネルギは略60〔KeV〕以
下とすることが必要である。これは基底注入の
Rpを凡そ0.05〔μm〕以下の深さに押さえること
が必要であることを意味する。 As seen in the figure, as the implantation energy during base implantation increases, the variation in conductivity increases. Assuming that this variation is approximately 5% or less in practical terms, the implantation energy of the basal implantation must be approximately 60[KeV] or less. This is the basal injection
This means that it is necessary to suppress Rp to a depth of approximately 0.05 [μm] or less.
以上の検討結果に基づき本発明では、半絶縁性
GaAs基板表面に、濃度分布のピーク位置Rpの深
さが凡そ0.05〔μm〕以下で、ドーズ量が略0.5〜
1.0〔cm-2〕のイオンの注入を行なつた後、濃度分
布のピーク位置Rpが略0.05〔μm〕以上の深さに
所望のn型不純物イオンを注入することにより、
所期の抵抗素子を良好な制御性及び再現性をもつ
て作成し得るとの結論に達した。 Based on the above study results, in the present invention, semi-insulating
On the GaAs substrate surface, the depth of the peak position Rp of the concentration distribution is about 0.05 [μm] or less, and the dose is about 0.5 ~
After implanting ions of 1.0 [cm -2 ], desired n-type impurity ions are implanted to a depth where the peak position Rp of the concentration distribution is approximately 0.05 [μm] or more.
It was concluded that the desired resistance element could be produced with good controllability and reproducibility.
第7図は上記結論に基づいて実施された本発明
の一実施列を、製造工程の順に示す要部断面図で
ある。以下同図を参照して本実施列を説明する。 FIG. 7 is a cross-sectional view of a main part of one embodiment of the present invention implemented based on the above conclusion, showing the manufacturing process in order. The present implementation sequence will be described below with reference to the same figure.
第7図aに示すように、クローム(Cr)が凡
そ0.1〔ppm〕ドーズされた抵抗率凡そ107〔Ωcm〕
の半絶縁性GaAs基板1の表面に、トランジスタ
素子及び抵抗素子を形成すべき領域に所定パター
ンの開口を有するフオトレジスト膜2を形成し、
これをマスクとしてSiイオンを前記GaAs基板表
面に注入して、イオン注入領域2及び5を形成す
る。本工程において注入エネルギは凡そ60
〔KeV〕、Siイオンのドーズ量は凡そ0.8×1012〔cm
-2〕とした。これにより凡そ0.05〔μm〕の深さに
分布のピークRpが位置する濃度分布が得られる。 As shown in Figure 7a, the resistivity is approximately 10 7 [Ωcm] with a dose of approximately 0.1 [ppm] of chromium (Cr).
A photoresist film 2 having a predetermined pattern of openings in areas where transistor elements and resistance elements are to be formed is formed on the surface of a semi-insulating GaAs substrate 1,
Using this as a mask, Si ions are implanted into the surface of the GaAs substrate to form ion implantation regions 2 and 5. In this process, the injection energy is approximately 60
[KeV], the dose of Si ions is approximately 0.8×10 12 [cm
-2 ]. As a result, a concentration distribution in which the peak Rp of the distribution is located at a depth of approximately 0.05 [μm] is obtained.
上記イオン注入はトランジスタ素子に対しては
活性層を形成するために、また抵抗素子に対して
は前述の基底注入を目的として行われるものであ
る。このようにGaAs基板上にFETと抵抗素子と
を具備する集積回路装置を作成する場合、本発明
における抵抗素子形成のための基底注入の条件
は、FETの活性層形成のためのイオン注入条件
と同一で良い場合が多い。従つてこのような場合
には両者のイオン注入は同一工程において実施し
得る。もしFETの活性層形成のためのイオン注
入が、たとえば3×1012〔cm-2〕程度を要し、前
述の基底注入の条件を満足しない場合には、前記
従来の製造方法の如くそれぞれ別の工程において
イオン注入を行えば良い。 The above ion implantation is performed for the purpose of forming an active layer for a transistor element, and for the above-mentioned base implantation for a resistor element. When creating an integrated circuit device having a FET and a resistance element on a GaAs substrate in this way, the conditions for base implantation for forming the resistance element in the present invention are the same as the ion implantation conditions for forming the active layer of the FET. In many cases, they are the same. Therefore, in such a case, both ion implantations can be performed in the same process. If the ion implantation for forming the active layer of the FET requires, for example, about 3×10 12 [cm -2 ] and does not satisfy the above-mentioned conditions for base implantation, the ion implantation for forming the active layer of the FET may be performed separately as in the conventional manufacturing method. Ion implantation may be performed in the step of.
この後は通常の製造工程に従つて進めて良く、
すてわち同図bに示すように、前記フオトレジス
ト膜2を除去したのち、W―Siのような高融点金
属の砒化物層を選択的に形成することにより、前
記イオン注入層3表面とシヨツトキ接触をなすシ
ヨツトキゲート電極6を形成し、更にあらためて
フオトレジスト膜7を形成し、この両者をマスク
としてSiイオンを、注入エネルギ凡そ200〔KeV〕
でSiイオンをGaAs基板表面に選択的に注入し、
イオン注入領域8及び21を形成する。本工程に
おけるドーズ量と得られた導電層のシート導電率
との関係については後述する。 After this, you can proceed according to the normal manufacturing process.
In other words, as shown in Figure b, after removing the photoresist film 2, an arsenide layer of a high melting point metal such as W--Si is selectively formed to improve the surface of the ion implantation layer 3. A shot gate electrode 6 is formed to make shot contact with the photoresist film 7, and a photoresist film 7 is formed again. Using both as a mask, Si ions are implanted at an implantation energy of approximately 200 [KeV].
selectively implant Si ions into the GaAs substrate surface,
Ion implantation regions 8 and 21 are formed. The relationship between the dose in this step and the sheet conductivity of the obtained conductive layer will be described later.
次いで同図cに示す如く、上記SiO2膜7を除
去し、窒化アルミニウム(AlN)膜(図示せず)
を形成し、これを保護膜として凡そ800〔℃〕の温
度で約15分間加熱処理を行い、上記Siイオン注入
領域3,5及び8内に注入されたSiイオンを活性
化して、n+型のソース及びドレイン領域9,
9′、n型の活性層10、n型の基底注入22及
びn+型の導電層23を形成する。 Next, as shown in Figure c, the SiO 2 film 7 is removed and an aluminum nitride (AlN) film (not shown) is removed.
This is used as a protective film and heat-treated at a temperature of about 800 [°C] for about 15 minutes to activate the Si ions implanted in the Si ion implanted regions 3, 5, and 8, and to form n + type source and drain regions 9,
9', an n-type active layer 10, an n-type base implant 22, and an n + -type conductive layer 23 are formed.
次いで上記AlN膜を除去した後、n型GaAs結
晶に対してオーミツク接触を形成する金・ゲルマ
ニウム―金(AuGe―Au)よりなるソース、ド
レイン電極13,13′及び抵抗の端子電極14,
14′をリフトオフ法により形成する。さらに上
記各電極上を含むGaAs基板1全面に層間絶縁膜
として例えばSiO2膜15を被着せしめ、これを
選択的に除去してコンタクト窓を開口し、該コン
タクト窓内にて上記各電極に接触するチタン―金
(Ti―Au)よりなる上部配線電極16を選択的
に形成する。 Next, after removing the AlN film, source and drain electrodes 13 and 13' made of gold-germanium-gold (AuGe-Au) and resistor terminal electrodes 14, which form ohmic contact with the n-type GaAs crystal, are formed.
14' is formed by a lift-off method. Furthermore, a SiO 2 film 15, for example, is deposited as an interlayer insulating film on the entire surface of the GaAs substrate 1 including the tops of each of the above electrodes, and this is selectively removed to open a contact window. A contacting upper wiring electrode 16 made of titanium-gold (Ti-Au) is selectively formed.
図示せる如く本実施列における抵抗素子Rは
GaAs基板1表面の浅い部分に形成された基底注
入層22と、深い部分に形成されたn+型導電層
とが一体化されたものとして形成される。上記基
底注入層22は前述したようにGaAs基板1表面
の影響を吸収するためのもので、この層自身は抵
抗素子Rの導電には寄与しない。従つて本実施列
における抵抗素子Rの抵抗値は実質的に導電層2
3の導電率を制御することによつて決定される。 As shown in the figure, the resistance element R in this implementation row is
The base injection layer 22 formed in the shallow part of the surface of the GaAs substrate 1 and the n + type conductive layer formed in the deep part are formed as an integrated layer. As mentioned above, the base injection layer 22 is for absorbing the influence of the surface of the GaAs substrate 1, and this layer itself does not contribute to the conductivity of the resistive element R. Therefore, the resistance value of the resistance element R in this embodiment is substantially equal to that of the conductive layer 2.
It is determined by controlling the conductivity of 3.
第8図は本実施列の上記抵抗素子Rのシート導
電率(即ちシート抵抗率の逆数)の導電層23の
ドーズ量に対する依存性を示す図であつて、縦軸
は抵抗素子Rのシート導電率〔KΩ□-1〕、横軸は
導電層23のドーズ量〔×1012cm-2〕を示す。同
図に見られる如く本実施列の抵抗素子Rの導電率
は、導電層23形成のためのイオン注入を一定の
エネルギのもとで行えば、このイオン注入のドー
ズ量と綺麗な比例関係を示すとともに、バラツキ
が小さく再現性が良い。従つて制御性も極めて良
く、GaAs集積回路装置の製作が容易となる。 FIG. 8 is a diagram showing the dependence of the sheet conductivity (that is, the reciprocal of the sheet resistivity) of the resistive element R in this embodiment on the dose of the conductive layer 23, where the vertical axis is the sheet conductivity of the resistive element R. The rate [KΩ□ -1 ] and the horizontal axis indicate the dose of the conductive layer 23 [×10 12 cm -2 ]. As can be seen in the figure, the conductivity of the resistive element R in this example row has a neat proportional relationship with the dose of the ion implantation if the ion implantation for forming the conductive layer 23 is performed at a constant energy. In addition, the variation is small and the reproducibility is good. Therefore, the controllability is extremely good, and the production of GaAs integrated circuit devices is facilitated.
なお上記一実施列においては、基底注入及び制
御注入のいずれもSiをイオン種として用いた例を
掲げて説明したが、この両者のうち基底注入に用
いるイオン種はGaAs基板内において拡散しにく
いことからSiが望ましいが、制御注入はSiに限定
する必要はなく、通常用いられるn型不純物例え
ばセレン(Se)等を使用しても良い。 Note that in the above example, an example was given in which Si is used as the ion species for both base implantation and controlled implantation, but of both, the ion species used for base implantation is difficult to diffuse within the GaAs substrate. However, controlled implantation need not be limited to Si, and commonly used n-type impurities such as selenium (Se) may also be used.
また前記一実施列ではイオン注入に際して、注
入領域表面を露出せしめた状態でイオンを注入す
る例を説明したが、注入領域表面にSiO2膜等を
形成し、これを透過してイオン注入を行なつても
良いことは勿論である。この場合には注入エネル
ギに対する注入深さの関係は当然異なり、所定の
深さに注入するには注入エネルギを前記実施列に
比較して増大させる必要がある。 Furthermore, in the above embodiment, an example was explained in which ions are implanted with the surface of the implanted region exposed during ion implantation. Of course, it's okay to grow old. In this case, the relationship between implantation energy and implantation depth is naturally different, and in order to implant to a predetermined depth, it is necessary to increase the implantation energy compared to the above embodiment.
更に上記一実施列では基底注入に次いで制御注
入を行なつた例を示したが、この両者は何れを先
に行なつても良く、この順序関係は特に限定する
必要はない。 Further, in the above embodiment, an example was shown in which the basal injection was followed by the control injection, but either of these may be performed first, and there is no need to particularly limit the order.
(f) 発明の効果
以上説明した如く本発明によれば、半絶縁性
GaAs基板上に所望の抵抗素子を良好な制御性及
び再現性をもつて作成可能となり、従つて所期の
特性を有するGaAs集積回路装置を安定且つ容易
に製造することが出来、且つ製造歩留りも向上す
る。(f) Effects of the invention As explained above, according to the present invention, semi-insulating
It is possible to create a desired resistance element on a GaAs substrate with good controllability and reproducibility, and therefore it is possible to stably and easily manufacture GaAs integrated circuit devices with desired characteristics, and the manufacturing yield is also reduced. improves.
第1図及び第2図は従来の半導体装置の製造方
法の問題点を説明するための図で、第1図は製造
工程を示す要部断面図、第2図は問題点を示す曲
線図、第3図〜第6図は本発明の原理を示す曲線
図、第7図は本発明の一実施列を製造工程の順に
示す要部断面図、第8図は上記一実施列の効果を
示す曲線図である。
図において、1は半絶縁性GaAs基板、3,
5,8,21はイオン注入層、9はn+型のソー
ス及びドレイン領域、22は基底注入層、23は
制御注入層、Rは抵抗素子を示す。
1 and 2 are diagrams for explaining problems in the conventional semiconductor device manufacturing method, in which FIG. 1 is a sectional view of a main part showing the manufacturing process, FIG. 2 is a curve diagram showing the problems, Figures 3 to 6 are curve diagrams showing the principle of the present invention, Figure 7 is a cross-sectional view of essential parts showing one embodiment of the present invention in the order of manufacturing steps, and Figure 8 shows the effect of the above-mentioned embodiment. It is a curve diagram. In the figure, 1 is a semi-insulating GaAs substrate, 3,
5, 8, and 21 are ion implantation layers, 9 is an n + type source and drain region, 22 is a base implantation layer, 23 is a control implantation layer, and R is a resistance element.
Claims (1)
に、当該ガリウム・砒素基板の表面から凡そ0.05
〔μm〕以下の深さに濃度分布のピークが位置する
如く、シリコン・イオンを0.5〜1.0×1012〔cm-2〕
のドーズ量で注入する工程と、前記所望の領域に
当該ガリウム・砒素基板の表面から凡そ0.05
〔μm〕以上の深さに濃度分布のピークが位置する
如くn型不純物イオンを注入する工程と、前記注
入されたイオンを活性化する工程とを有する抵抗
素子の形成工程を含むことを特徴とする半導体装
置の製造方法。[Claims] 1. Approximately 0.05% of the area from the surface of the semi-insulating gallium/arsenic substrate is applied to a desired area of the semi-insulating gallium/arsenic substrate.
Silicon ions are distributed at a depth of 0.5 to 1.0×10 12 [cm -2 ] so that the peak of the concentration distribution is located at a depth of less than [μm].
The step of implanting at a dose of approximately 0.05 m
It is characterized by comprising a step of forming a resistive element, which includes a step of implanting n-type impurity ions so that the peak of the concentration distribution is located at a depth of [μm] or more, and a step of activating the implanted ions. A method for manufacturing a semiconductor device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57230091A JPS59123274A (en) | 1982-12-28 | 1982-12-28 | Manufacture of semicondcutor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57230091A JPS59123274A (en) | 1982-12-28 | 1982-12-28 | Manufacture of semicondcutor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59123274A JPS59123274A (en) | 1984-07-17 |
| JPS6314871B2 true JPS6314871B2 (en) | 1988-04-01 |
Family
ID=16902402
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57230091A Granted JPS59123274A (en) | 1982-12-28 | 1982-12-28 | Manufacture of semicondcutor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59123274A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63124863A (en) * | 1986-11-14 | 1988-05-28 | Komatsu Zenoa Kk | Two-cycle engine |
| JPH0218657U (en) * | 1988-07-18 | 1990-02-07 |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6321864A (en) * | 1986-07-16 | 1988-01-29 | Oki Electric Ind Co Ltd | Manufacture of semiconductor element |
-
1982
- 1982-12-28 JP JP57230091A patent/JPS59123274A/en active Granted
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63124863A (en) * | 1986-11-14 | 1988-05-28 | Komatsu Zenoa Kk | Two-cycle engine |
| JPH0218657U (en) * | 1988-07-18 | 1990-02-07 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59123274A (en) | 1984-07-17 |
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