JPS58147172A - Manufacture of semiconductor device - Google Patents

Manufacture of semiconductor device

Info

Publication number
JPS58147172A
JPS58147172A JP3013982A JP3013982A JPS58147172A JP S58147172 A JPS58147172 A JP S58147172A JP 3013982 A JP3013982 A JP 3013982A JP 3013982 A JP3013982 A JP 3013982A JP S58147172 A JPS58147172 A JP S58147172A
Authority
JP
Japan
Prior art keywords
layer
ions
distribution
semiconductor device
doped
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.)
Granted
Application number
JP3013982A
Other languages
Japanese (ja)
Other versions
JPH07111976B2 (en
Inventor
Takashi Mimura
高志 三村
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP3013982A priority Critical patent/JPH07111976B2/en
Publication of JPS58147172A publication Critical patent/JPS58147172A/en
Publication of JPH07111976B2 publication Critical patent/JPH07111976B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
    • H01L29/76Unipolar devices, e.g. field effect transistors
    • H01L29/772Field effect transistors
    • H01L29/80Field effect transistors with field effect produced by a PN or other rectifying junction gate, i.e. potential-jump barrier

Landscapes

  • Engineering & Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Physics & Mathematics (AREA)
  • Ceramic Engineering (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Computer Hardware Design (AREA)
  • Junction Field-Effect Transistors (AREA)

Abstract

PURPOSE:To improve the rise and fall switching charateristics of a semiconductor device by heat treating at the temperature which sufficiently produces a distribution that carrier density between AlGaAs layers stepwisely varies in the carrier density from the result that ions in the GaAs layer are sufficiently activated. CONSTITUTION:A non-doped GaAs layer 2 and a non-doped AlGaAs layer 3 are grown on a non-doped AlGaAs layer 1, and when Si ions are implanted to the layer, a distribution characteristic curve PF in which solid line and broken lines exist is obtained. The curve PF is energy and dosage at ion implanting time, which is decited unitarily. When an annealing is performed at a temperature of 700 deg.C in case of activating it after implanting Si ions, the carrier distribution is presented only in the layer 2 as seen by the solid line of the curve PF, thereby providing an ideal profile.

Description

【発明の詳細な説明】 発明の技術分野 本発明は、急峻な立上り或いは立下り或いはその両方の
特性を備えた半導体装置の製造方法に関する。
DETAILED DESCRIPTION OF THE INVENTION Technical Field of the Invention The present invention relates to a method of manufacturing a semiconductor device having characteristics of steep rise and/or fall.

従来技術と問題点 従来、成る種の半導体装置では、イオン注入法(;て半
導体基板(或いは層)に不純物を導入してチャネル領域
を形成することが行なわれている。
Prior Art and Problems Conventionally, in some types of semiconductor devices, a channel region is formed by introducing impurities into a semiconductor substrate (or layer) using an ion implantation method.

一般に、前記のようにしてチャネル領域を形成すると、
そのキャリヤ分布は第1図(=見られるように所謂ガウ
シャン分布となることが知られている。このようなキャ
リヤ分布のチャネル領域を有する半導体装置に於いては
、閾値電圧Vtル近傍に於けるゲート電圧に対するドレ
イン1流変化は緩徐であって、立上り或いは立下りが極
めて鈍いものとなる。この理由は、第1図から判るよう
C二、キャリヤ分布がなだらかな尾を引いていることi
二基因している。即ち、矢印Aの部分に於けるfyaは
高いが、矢印Bの部分(=於けるfigは低い。
Generally, when a channel region is formed as described above,
It is known that the carrier distribution is a so-called Gaussian distribution as shown in Fig. 1. In a semiconductor device having a channel region with such a carrier distribution, the The drain current changes slowly with respect to the gate voltage, and the rise or fall is extremely slow.The reason for this is that the carrier distribution has a gentle tail, as can be seen from Figure 1.
There are two reasons. That is, fya is high in the part indicated by arrow A, but fig in the part indicated by arrow B (=) is low.

発明の目的 本発明は、イオン注入法に依りチャネル領域を形成した
場合C二、キャリヤ分布が急峻な段差を持つよう(二し
、半導体装置の立上り及び立下りスイッチング特性を改
善しようとするものである。
Purpose of the Invention The present invention aims to improve the rise and fall switching characteristics of a semiconductor device so that the carrier distribution has a steep step difference when a channel region is formed by ion implantation. be.

発明の実施例 第2図は本発明一実施例を説明するためのキャリヤ分布
を表わす線図である。
Embodiment of the Invention FIG. 2 is a diagram showing carrier distribution for explaining an embodiment of the invention.

図に見られる様Cニノン・ドープA IG a A J
F層1上1:ノy−ドープG a A 7層2.ノy’
ドープA I G a A z113を成長させ、これ
ζ;Siイオンを注入すると実線及び破線が混在する分
布特性線PFが得られる。この特性線PFはイオン注入
時のエネルギ及びドーズ量で一義的(=決ってしまう。
As seen in the figure C ninone dope A IG a A J
F layer 1 top 1: Noy-doped Ga A 7 layer 2. noy'
When doped A I G a A z113 is grown and Si ions are implanted, a distribution characteristic line PF including solid lines and broken lines is obtained. This characteristic line PF is uniquely determined by the energy and dose during ion implantation.

さて、前記のよう4:Siイオンを注入しても、それを
熱処理して活性化しなければキャリヤとして振舞うこと
はできない。そこで、イオン注入後、アニールを行なう
ことになるが、AIGcAs中のイーオンは温度800
 (’C)程度以上の熱を加えないとドナーにはならな
い。これ(二対し、GaAs中のイオンは700(”C
)程度以上の温度でドナーC:なる。
Now, even if 4:Si ions are implanted as described above, they cannot act as carriers unless they are activated by heat treatment. Therefore, after ion implantation, annealing is performed, and the ions in AIGcAs are heated to a temperature of 800
It will not become a donor unless it is heated to a level above ('C). This (2), whereas the ion in GaAs is 700 ("C
) At a temperature above about 100%, donor C becomes.

そこで、前記のよう(二、A I G aA zとG 
a A pの、テロ接合を形成しくヘテロ接合を一つに
するか二つにするかは任意)、これ(=例えばSiイオ
ンなどを注入してから活性化する(:際し、アニールを
温度700(’C)程度≦二して行なうと、キャリヤ分
布はw12図C二於ける特性線PFの実線(二見られる
よう感二GaAz層2にのみ現われ、理想的なプロファ
イルとなる。そして、アニール温度が700(’C)を
越えた場合であっても、A I G gA JF中で発
生するキャリヤーは僅かであるから、例えば第2図(二
特性線−PF’に見られるような分布となる。却も、8
00(’C)でアニールしても、A I G gA J
中のドナ一単位が深いため(Siで60〔准−V))、
キャリヤ濃度は300〔@K〕でも1/10.77(’
K)では完全(=凍結する。
Therefore, as mentioned above (2. A I G aA z and G
To form a heterojunction of a A p, it is optional whether to make one or two heterojunctions), and then activate it after implanting (for example, Si ions). 700 ('C) ≦ 2, the carrier distribution appears only in the GaAz layer 2, as can be seen from the solid line of the characteristic line PF in Figure C2, and becomes an ideal profile. Even if the temperature exceeds 700 ('C), only a small amount of carriers are generated in A I G g A JF. It will be. No way, 8
Even if annealed at 00('C), A I G g A J
Because the inner donor unit is deep (60 [semi-V] for Si),
Even at 300 [@K], the carrier concentration is 1/10.77 ('
K) completely (=freezes).

前記した本発明の原理を適用して良好なスイツデング特
性を有する半導体装置を製造することができる。
By applying the principles of the present invention described above, a semiconductor device having good switching characteristics can be manufactured.

第5図は本発明を適用して得たショットキ・ゲート電極
形電界効果半導体装jii (MESFET)の要部断
面図である。
FIG. 5 is a sectional view of a main part of a Schottky gate electrode type field effect semiconductor device jii (MESFET) obtained by applying the present invention.

図1=於いて、1は半絶縁性G a A J基板、2は
バッファ層、SはA I G a A 7層、4は電型
G11A#層、5はA I G g A a層、6はソ
ース電極、7はドレイン電極、8はゲート電極をそれぞ
れ示す。
In Figure 1, 1 is a semi-insulating G a A J substrate, 2 is a buffer layer, S is an A I G a A 7 layer, 4 is an electric type G11A# layer, 5 is an A I G g A a layer, Reference numeral 6 indicates a source electrode, 7 indicates a drain electrode, and 8 indicates a gate electrode.

この実施例で94.GaAz層4を電型化するの(二本
発明を適用するものであって、ル型G a A 7層4
はチャネルとして動作し、ゲート電極8(二対する印加
電圧で発生する空乏層(二て制御されるものである。
In this example, 94. The GaAz layer 4 is electrically typed (to which the present invention is applied).
operates as a channel, and is controlled by a depletion layer (which is generated by applying voltage to the gate electrode 8).

第4図は高電子移動度半導体装置(HEMT :雑誌「
電子技術」第224第12号第85頁乃至第90頁参N
)に本発明を適用したものの要部断面図であり、第3図
シニ関して説明した部分と同部分を同記号で指示してあ
る。
Figure 4 shows high electron mobility semiconductor device (HEMT: magazine
Electronic Technology” No. 224 No. 12, pages 85 to 90 N
) is a sectional view of a main part of a device to which the present invention is applied, and the same parts as those described in connection with FIG. 3 are indicated by the same symbols.

図に於いて、9はノン拳ドープAlGmAg層、10は
%fJIG @A #チャネル層、11はs fji 
AIGtAz電子供給層をそれぞれ示す。
In the figure, 9 is the non-doped AlGmAg layer, 10 is the %fJIG@A # channel layer, and 11 is the s fji
AIGtAz electron supply layers are shown respectively.

純粋なHEMTではチャネル層10がノン・ドープであ
って、電子供給層11から遷移してくる電子で高移動度
電子層が形成されるのであるが、近年、デャネル層10
C;%型不純物を導入し、ディプリーション型とする技
術が開発され、このトランジスタとチャネル・ドープさ
れていない本来のHEMTとを組合わせてE/Dインバ
ータとすることが行なわれているので、このII(=は
チャネル層10を算型化するのに本発明を適用すると有
効で°ある。
In a pure HEMT, the channel layer 10 is non-doped, and a high-mobility electron layer is formed by electrons transitioning from the electron supply layer 11. However, in recent years, the channel layer 10 is
C: A technology to introduce depletion type impurities has been developed, and this transistor is combined with an original HEMT whose channel is not doped to form an E/D inverter. , this II (= is effective when the present invention is applied to shape the channel layer 10.

尚、電子供給層11はエピタキシャル成長時(ニドープ
しておけば良い。
Note that the electron supply layer 11 may be doped during epitaxial growth.

発明の効果 本発明(=依れば、A I G a A を層とG g
 A z層とを隣接して形成し、それ等層中(ニドナー
不純物イオンを注入し、両物質中に於けるイオンの活性
化率の差、ドナー・レベルのエネルギ差を利用し、Gt
tAz層のみに充分なキャリヤを発生させ、G g A
 a層とAIGcAI層との間(二階段的に変化するキ
ャリヤ分布な曳出させることができるので、この技術を
適用してMPJFET 、 HEMTなどの半導体装置
を製造するとスイッチング特性良好なものが得られる。
Effects of the Invention According to the present invention (=according to the invention, A I G a A is a layer and G g
The Gt layer is formed adjacent to the Az layer, and the Gt
Generate sufficient carriers only in the tAz layer and G g A
Since it is possible to extract carrier distribution between the a layer and the AIGcAI layer (which changes in two steps), if this technology is applied to manufacture semiconductor devices such as MPJFETs and HEMTs, good switching characteristics can be obtained. .

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

第1図はキャリヤ分布を説明する線図、第2図は本発明
を実施した場合のキャリヤを説明する線図、第6図及び
第4図は本発明を実施して得た半導体装置の要部断面図
である。 図に於いて、1は半絶縁性GlIA#基板、2はバッフ
ァ層、5はA IG a A 1層、4は算型GgAz
@。 5はA IG a A #噛、6はソース電極、7はド
レイン電極、8はゲート電橋、9はノン・ドープAIG
gAz層、10はs tJI GgAzチャネル層、1
1は滲型AlGaル電子供給層である。 特許出願人  富士通株式会社 代理人 弁理士 玉蟲久五部(外3名)表面からの距駿 369− 第3図 第4図
FIG. 1 is a diagram illustrating carrier distribution, FIG. 2 is a diagram illustrating carriers when the present invention is implemented, and FIGS. 6 and 4 are outline diagrams of a semiconductor device obtained by implementing the present invention. FIG. In the figure, 1 is a semi-insulating GlIA# substrate, 2 is a buffer layer, 5 is an A IG a A 1 layer, and 4 is a calculation type GgAz
@. 5 is A IG a A # bit, 6 is source electrode, 7 is drain electrode, 8 is gate bridge, 9 is non-doped AIG
gAz layer, 10 is s tJI GgAz channel layer, 1
1 is a permeable AlGa electron supply layer. Patent applicant Fujitsu Ltd. agent Patent attorney Gobe Tamamushi (3 others) Distance from the surface 369- Figure 3 Figure 4

Claims (1)

【特許請求の範囲】[Claims] A I G g A 7層とG g A 7層とを隣接
させて形成し、次C二、それ等の層中(:ドナー不純物
イオンを注入し、次に、GIIA#暑中のイオンが充分
(;活性化してA I G g A z層との間のキャ
リヤ濃度が階段的に変化する分布を現出させる温度で熱
処理する工程が含まれてなることを特徴とする半導体装
置の製造方法。
The A I G g A 7 layer and the G g A 7 layer are formed adjacent to each other, and then donor impurity ions are implanted into those layers. A method for manufacturing a semiconductor device, comprising the step of performing heat treatment at a temperature that activates and reveals a distribution in which the carrier concentration between the A I G g A z layer changes in a stepwise manner.
JP3013982A 1982-02-26 1982-02-26 Method for manufacturing semiconductor device Expired - Lifetime JPH07111976B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3013982A JPH07111976B2 (en) 1982-02-26 1982-02-26 Method for manufacturing semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3013982A JPH07111976B2 (en) 1982-02-26 1982-02-26 Method for manufacturing semiconductor device

Publications (2)

Publication Number Publication Date
JPS58147172A true JPS58147172A (en) 1983-09-01
JPH07111976B2 JPH07111976B2 (en) 1995-11-29

Family

ID=12295429

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3013982A Expired - Lifetime JPH07111976B2 (en) 1982-02-26 1982-02-26 Method for manufacturing semiconductor device

Country Status (1)

Country Link
JP (1) JPH07111976B2 (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60160670A (en) * 1984-01-31 1985-08-22 Fujitsu Ltd Semiconductor device
JPS60263476A (en) * 1984-06-12 1985-12-26 Sony Corp Manufacture of semiconductor device
JPS6154673A (en) * 1984-08-25 1986-03-18 Fujitsu Ltd Field-effect type semiconductor device
JPS61131565A (en) * 1984-11-30 1986-06-19 Fujitsu Ltd Field effect type semiconductor device
JPS61131564A (en) * 1984-11-30 1986-06-19 Fujitsu Ltd Field effect type semiconductor device
JPS62209866A (en) * 1986-03-10 1987-09-16 Nec Corp Semiconductor device
JPS6337670A (en) * 1986-08-01 1988-02-18 Oki Electric Ind Co Ltd Semiconductor element and manufacture thereof
JPS6337671A (en) * 1986-08-01 1988-02-18 Oki Electric Ind Co Ltd Manufacture of semiconductor element

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60160670A (en) * 1984-01-31 1985-08-22 Fujitsu Ltd Semiconductor device
JPS60263476A (en) * 1984-06-12 1985-12-26 Sony Corp Manufacture of semiconductor device
JPS6154673A (en) * 1984-08-25 1986-03-18 Fujitsu Ltd Field-effect type semiconductor device
JPS61131565A (en) * 1984-11-30 1986-06-19 Fujitsu Ltd Field effect type semiconductor device
JPS61131564A (en) * 1984-11-30 1986-06-19 Fujitsu Ltd Field effect type semiconductor device
JPS62209866A (en) * 1986-03-10 1987-09-16 Nec Corp Semiconductor device
JPS6337670A (en) * 1986-08-01 1988-02-18 Oki Electric Ind Co Ltd Semiconductor element and manufacture thereof
JPS6337671A (en) * 1986-08-01 1988-02-18 Oki Electric Ind Co Ltd Manufacture of semiconductor element

Also Published As

Publication number Publication date
JPH07111976B2 (en) 1995-11-29

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