JPS58197770A - Semiconductor device - Google Patents

Semiconductor device

Info

Publication number
JPS58197770A
JPS58197770A JP7965182A JP7965182A JPS58197770A JP S58197770 A JPS58197770 A JP S58197770A JP 7965182 A JP7965182 A JP 7965182A JP 7965182 A JP7965182 A JP 7965182A JP S58197770 A JPS58197770 A JP S58197770A
Authority
JP
Japan
Prior art keywords
region
base
barrier
superposed
collector
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP7965182A
Other languages
Japanese (ja)
Inventor
Yoshifumi Mori
森 芳文
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP7965182A priority Critical patent/JPS58197770A/en
Publication of JPS58197770A publication Critical patent/JPS58197770A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. 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
    • H01L29/7606Transistor-like structures, e.g. hot electron transistor [HET]; metal base transistor [MBT]

Abstract

PURPOSE:To increase the amplification factor of a unipolar transistor as well as to reduce the noise thereof by a method wherein an n-AlyGA1-yAs is superposed on an n-AlxGa1-xAs, and an n-Aly'Ga1-y'As and an n-Alx'Ga1-x'As are superposed through the intermediary of an n type Ga layer, and composition ratio of x-y' are properly selected. CONSTITUTION:The barrier 1 of an n-AlyGa1-yAs is contacted with the emitter layer E of an n-AlxGa1-xAs and an n-Ge base layer B is superposed thereon. Subsequently, the barrier 2 of an n-Aly'Ga1-y'As is contacted with the above, an n-Alx'Ga1-x'As collector layer C is superposed, and they are selected into o>=x, x'>=y and y'. The As can be doped in extreme high density and the base width can also be reduced markedly by using Ge for the base B. Also, as a forbidden band width increases when the composition of Al is increased and the effective barrier when viewed from the base B is increased in height, the possibility of dropping of an electron to the conduction band level of the base region is little, and the possibility of running to a collector C as a hot electron increases. According to this constitution, the characteristics of a supersonic transistor can be improved remarkably.

Description

【発明の詳細な説明】 本発明は、半導体装置特にトランジスタに係わる。[Detailed description of the invention] The present invention relates to semiconductor devices, particularly transistors.

例えばGaAsバイポーラトランジスタはA ’l n
pn構造が採られるが、ペース領域からエミッタ領域へ
の正孔注入による損失電流分を一誠させて層中率の向上
を図る目的で、エミッタ領域にGaAsよりも禁制帯幅
の広いA1GaAs tt設けたものがある。
For example, a GaAs bipolar transistor has A 'l n
Although a pn structure is adopted, A1GaAs tt, which has a wider forbidden band width than GaAs, is provided in the emitter region in order to reduce current loss due to hole injection from the pace region to the emitter region and improve the layer filling ratio. There is something.

この場合AffiGaAsとGaAs f)県制帯暢の
差が大きい程良いが、あまり大きくしすぎるとAffi
QaAs中の電子移動度が急11に低くなるためにエミ
ッタ抵抗の増加をもたらし素子特性を悪化させ【しま5
゜一方篇1図のエネルギーバンド図(図は上側の伝導帯
のみを示す)で示すよ5にn+形GaAsをペース領域
(B)として、その両側のn形QaAaのエミッタ領域
(g)及びコレクタ領域(C)に夫々GaAsより禁制
i−の大きいAlQaム2による障vi!領域11)及
び(2)を設け、工建ツタ領域<m>からの注入電子を
そのまま熱い電子としてコレクタ領域(C) litの
障壁を越えてコレクタ領域(C)に流すように構成した
ユニポーラトランジスタ(通称ホットエレクトロン・ト
ランジスp ; IgDM TechnicalDig
est 、 嬉629 m (1980) #照)が提
案されている。又、障壁層がなくエミッタ領域、ベース
領域及びコレクタ領域を夫々n形GaAs 、 n形G
e及びn形QaAsで構成したトランジスタも特公昭4
0−4181号におい″′C提案されている。しかし、
前記ユニポーラトランジスタにおいてはベース懺If!
 (B)がGJIAIゆえにペース幅に限界があり、こ
のベース輪の限界によつ【増巾率低下、雑音の増大を招
くものであり、さらに特性改善が望まれている。
In this case, the larger the difference between AffiGaAs and GaAs f) Prefectural coverage, the better, but if it is too large, Affi
The electron mobility in QaAs suddenly drops to 11, causing an increase in emitter resistance and deteriorating device characteristics.
゜On the other hand, as shown in the energy band diagram in Figure 1 (the figure shows only the upper conduction band), n+ type GaAs is used as a pace region (B) in 5, and the emitter region (g) and collector of n type QaAa on both sides of the pace region (B). In region (C), there is a disturbance vi! due to AlQa film 2 which has a larger inhibition i- than GaAs, respectively. A unipolar transistor in which regions 11) and (2) are provided, and the electrons injected from the ivy region <m> flow as hot electrons directly to the collector region (C) over the barrier of the collector region (C) lit. (commonly known as hot electron transistors p; IgDM Technical Dig
est, 629 m (1980) has been proposed. In addition, there is no barrier layer, and the emitter region, base region, and collector region are made of n-type GaAs and n-type G, respectively.
Transistors made of e- and n-type QaAs were also
No. 0-4181 proposes ``'C. However,
In the unipolar transistor, the base voltage If!
Since (B) is a GJIAI, there is a limit to the pace width, and this limit of the base ring causes a decrease in the amplification rate and an increase in noise, and further improvement of the characteristics is desired.

本発明は上述の点に、鑑み更に特性向上を図った半導体
装置、%にユニポーラトランジスタを提供するものであ
る。
In view of the above points, the present invention provides a semiconductor device and a unipolar transistor with further improved characteristics.

本発明においては、第2図のエネルギーバンドwA(上
側の伝導帯のみ示す)に示すよ5に、夫々順次に隣接す
るAm zQa 1− XAIのIll導電形のエミッ
タ領域(lit)、ム”Y”1−yA@の第1導電形の
エミッタ側障壁領域(1)、Geの第1導電形のベース
領域(B)、ム1y’Ga1−yAiの第1導電形のコ
レクタ側障壁領域(2)及びAI X’G511− X
’AIの第1導電屡のコレクタ領域(C)を有して成る
(但し、0≦X * X’< Yr Y’に選定する)
。各エミッタ領域(N)、ベース領域(B)及びコレク
タ領域(C)には、夫々電極な設けてエンツタ領域(E
)の多数キャリアをコレクタ領域(C) K送るための
所要の電位を印加するようになす。ここで、エミッタ領
域(K)及びコレクタ領域(C)における各電極側の領
域は夫々^不#@智濃度の第1導電形のAIzGll−
zAm及びAlz(jal−1Aaで構成するを可とす
る。
In the present invention, as shown in the energy band wA (only the upper conduction band is shown) in FIG. Emitter-side barrier region (1) of the first conductivity type of ``1-yA@, base region (B) of the first conductivity type of Ge, collector-side barrier region (2) of the first conductivity type of Ga1-yAi ) and AI X'G511-
'AI's first conductive collector region (C) (selected as 0≦X*X'<Yr Y')
. Each emitter region (N), base region (B) and collector region (C) is provided with an electrode, respectively.
) is applied to send the majority carriers to the collector region (C). Here, the regions on the side of each electrode in the emitter region (K) and collector region (C) are AIzGll- of the first conductivity type with the concentration of
It is possible to configure zAm and Alz (jal-1Aa).

上記各領域の実施例を次に示す。エミッタ領域(M)は
n形QaAs (iA制制御輪14eV)で形成し、そ
の厚さを1〜3μm、不純物濃度を〜10  cm−”
程度とする。エミッタ側障壁領域illはn形AgGa
As(AIが多くなるii*制帯鴫は太き(なり、A1
AsのIII制帯幅は2.2@Vとなる)で形成し、そ
の厚さ100〜1000 X 、不純1i1119濃度
な〜10  Cm−”程度とする。ここで厚さが100
0 !より厚いと抵抗が大きくなり、loo lより薄
いと障壁の実効高さが低(なる。ベース領域(B)はn
+形Ge (禁制帯輸帆66・V)で形成し、その厚さ
を100X以下、不純物濃度を〜IQ  cm−”とす
る。コレクタ側障ma城f2]はエミッタ@障壁領域1
1)と同様にn形AlAsで形成し、その厚さはコレク
タ領域(C)と合せて2〜5fimとなるように選び、
その不純物濃度はキャリア(この場合電子)が飽和速度
で移動する1016cm−3以下にする。コレクタ領域
(C)はn形GaAs (厚さ、不純物濃度は同上)で
形成する。
Examples of each of the above areas are shown below. The emitter region (M) is formed of n-type QaAs (iA control wheel 14 eV), with a thickness of 1 to 3 μm and an impurity concentration of ~10 cm.
degree. The emitter side barrier region ill is n-type AgGa
As (AI increases ii * system obi is thick
The III-limiting width of As is 2.2@V), the thickness is 100 to 1000X, and the impurity concentration is about 10 Cm-''. Here, the thickness is 100
0! If it is thicker, the resistance increases, and if it is thinner than loo l, the effective height of the barrier is low (the base region (B) is n
+ type Ge (forbidden zone 66 V), its thickness is 100X or less, and the impurity concentration is ~IQ cm-''.
Similarly to 1), it is formed of n-type AlAs, and its thickness is selected to be 2 to 5 fim including the collector region (C).
The impurity concentration is set to 1016 cm-3 or less, at which carriers (electrons in this case) move at a saturation speed. The collector region (C) is formed of n-type GaAs (thickness and impurity concentration are the same as above).

なお、障壁領域(1)及び(2)としてはAtGmAg
の他に、Zn8e 、 InQslAIPなどを用いる
ことも出来る。
Note that the barrier regions (1) and (2) are AtGmAg.
Besides, Zn8e, InQslAIP, etc. can also be used.

斯る構成のユニポーラトランジスタによれば、特にベー
ス領域(B) K Geを用いたことKより、コノ種の
トランジスタの特性向上を図ることができる。IKJち
、虫はAs不純物を10  C1n−J!itでドープ
することができるなどGtAsに比べて不純物をより高
濃度にドーグすることができるので、10”Cm−” 
4度のQiAs ヘ−x領域に比ヘテGeヘース領域は
同一ベース抵抗でのベース暢を/100程度まで小さく
できる。一方、同一物質の障−で比ヘルド、Φベースは
G1Asペースに比べ【ペースから見た実効的な障壁の
^さが大きくなるので、エイツタ領域(E)からの電子
がベース領域の伝導帯のレベルにまで落ちる確率が少(
、そのまま熱い電子としてコレクタ側の障壁を越えてコ
レクタ領域(C) K流れる確率が大きくなる。
According to the unipolar transistor having such a configuration, it is possible to improve the characteristics of the type of transistor, especially by using KGe in the base region (B). IKJ, the insect is As impurity 10 C1n-J! Compared to GtAs, impurities can be doped at a higher concentration than GtAs, so it is possible to dope with 10"Cm-"
The 4° QiAs Hex region and the Ge Hess region can reduce the base resistance to about /100 with the same base resistance. On the other hand, due to the barrier of the same material, the specific Held and Φ base has a larger [effective barrier seen from the pace] than the G1As pace, so electrons from the Eitzta region (E) move into the conduction band of the base region. The probability of falling to the level is low (
, there is a high probability that the hot electrons will flow as hot electrons over the barrier on the collector side into the collector region (C).

このように本発明によれば、ベース領域の一−に之より
禁制帯幅の大きい障壁領域をもつユニポーラトランジス
タにおいて、より増巾率が向上し、且つ雑音が低減する
ものであり、特に超高速トランジスタに応用して飛躍的
な特性向上なもたらすものである。
As described above, according to the present invention, in a unipolar transistor having a barrier region with a larger forbidden band width on one side of the base region, the amplification factor is further improved and the noise is reduced. When applied to transistors, it brings about dramatic improvements in characteristics.

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

111図は従来のユニポーラトランジスタ(、t、ット
エレクトロン・トランジスタ)の例を示すエネルギーバ
ンド図、JII2図は本発明によるユニポーラトランジ
スタの例を示すエネルギーバンド図である。 (k!J)はエミッタ領域、(B)はベース領域、(c
)はコレクタ領域、IIJ i21は障壁領域である。
Figure 111 is an energy band diagram showing an example of a conventional unipolar transistor (t, electron transistor), and Figure JII2 is an energy band diagram showing an example of a unipolar transistor according to the present invention. (k!J) is the emitter region, (B) is the base region, (c
) is the collector region, and IIJ i21 is the barrier region.

Claims (1)

【特許請求の範囲】[Claims] 夫々順次K11lI*するAIXGII−XAI f)
菖1導電形の$111領域、ムjiyQ11−yAs 
I)第1導電形の第2領域、伽の第1導電形の第3領域
、At y’Ga 1− y’Asの第1導電形のjl
I4領域及びA藤X’G!l 1− z気の第1導電形
の第5領域(但し、0≦x、x′<y、y′)と、前記
第1 、fl13及び菖5領域に夫々電極を設けて前記
第1領域の多数キャリアを前記第S*域に送る手段を有
して成る半導体装置。
AIXGII-XAI f)
$111 area of iris 1 conductivity type, MujiyQ11-yAs
I) A second region of the first conductivity type, a third region of the first conductivity type of A, and a jl of the first conductivity type of At y'Ga 1- y'As.
I4 area and A Fuji X'G! The fifth region of the first conductivity type (where 0≦x, x'<y, y') and the first, fl13, and irises 5 regions are provided with electrodes, respectively, and the first region A semiconductor device comprising means for sending majority carriers of to the S* region.
JP7965182A 1982-05-12 1982-05-12 Semiconductor device Pending JPS58197770A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7965182A JPS58197770A (en) 1982-05-12 1982-05-12 Semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7965182A JPS58197770A (en) 1982-05-12 1982-05-12 Semiconductor device

Publications (1)

Publication Number Publication Date
JPS58197770A true JPS58197770A (en) 1983-11-17

Family

ID=13696024

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7965182A Pending JPS58197770A (en) 1982-05-12 1982-05-12 Semiconductor device

Country Status (1)

Country Link
JP (1) JPS58197770A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61102774A (en) * 1984-10-26 1986-05-21 Agency Of Ind Science & Technol Semiconductor device
JPS62217658A (en) * 1986-03-18 1987-09-25 Fujitsu Ltd Resonant tunnel semiconductor device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61102774A (en) * 1984-10-26 1986-05-21 Agency Of Ind Science & Technol Semiconductor device
JPS62217658A (en) * 1986-03-18 1987-09-25 Fujitsu Ltd Resonant tunnel semiconductor device
JPH0834213B2 (en) * 1986-03-18 1996-03-29 富士通株式会社 Resonant tunnel semiconductor device

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