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JPS584831B2 - Bipolar negative resistance semiconductor device - Google Patents
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JPS584831B2 - Bipolar negative resistance semiconductor device - Google Patents

Bipolar negative resistance semiconductor device

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Publication number
JPS584831B2
JPS584831B2 JP52005661A JP566177A JPS584831B2 JP S584831 B2 JPS584831 B2 JP S584831B2 JP 52005661 A JP52005661 A JP 52005661A JP 566177 A JP566177 A JP 566177A JP S584831 B2 JPS584831 B2 JP S584831B2
Authority
JP
Japan
Prior art keywords
base layer
semiconductor
layer
layers
negative resistance
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
JP52005661A
Other languages
Japanese (ja)
Other versions
JPS5390883A (en
Inventor
年綱寛史
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.)
Toko Inc
Original Assignee
Toko Inc
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 Toko Inc filed Critical Toko Inc
Priority to JP52005661A priority Critical patent/JPS584831B2/en
Publication of JPS5390883A publication Critical patent/JPS5390883A/en
Publication of JPS584831B2 publication Critical patent/JPS584831B2/en
Expired legal-status Critical Current

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  • Bipolar Transistors (AREA)

Description

【発明の詳細な説明】 本発明は、外部電流搬送率αの改善された二極負性抵抗
半導体素子の内部構造に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an internal structure of a bipolar negative resistance semiconductor device with an improved external current carrying rate α.

従来のこの種半導体素子の動作はNPN(又はPNP)
トランジスタのベースオープン動作涙して説明される。
The operation of conventional semiconductor devices of this type is NPN (or PNP).
The base-open operation of a transistor is explained in detail.

すなわち、NPNトランジスタの外部電流搬送率α、ブ
レークオーバー電圧VB、負性抵抗領域に入ってから電
圧Vcとすると、実験的にVc=VB■1−αの関係が
成立することが知られており、ブレークオーバー電圧V
Bを超えた電圧が素子に印加されると電流が急速に増加
し外部電流搬送率αが1に近ずき、電圧Vcがプレーク
オーバー電圧VBよりも小さくなり負性抵抗特性を示す
That is, it is known experimentally that the relationship of Vc = VB 1 - α holds when the external current carrying rate α of the NPN transistor, the breakover voltage VB, and the voltage Vc after entering the negative resistance region are set. , breakover voltage V
When a voltage exceeding B is applied to the element, the current increases rapidly, the external current carrying rate α approaches 1, the voltage Vc becomes smaller than the breakover voltage VB, and negative resistance characteristics are exhibited.

この原理にもとづき外部電流搬送率αを大きくするため
にエミツタ注入効率γ、ベース伝送効率βを大きくする
ことが従来行われてきた。
Based on this principle, the emitter injection efficiency γ and the base transmission efficiency β have been increased in order to increase the external current carrying rate α.

すなわちエミツタ注入効率γを大きくする為にベース層
よりもエミツタ層の不純物濃度を大きくし、ベース伝送
効率βを大きくする為にベース層の幅をせまくする方法
等が一般的に行われてきた。
That is, in order to increase the emitter injection efficiency γ, the impurity concentration of the emitter layer is made higher than that of the base layer, and in order to increase the base transmission efficiency β, the width of the base layer is made narrower.

このため例えば第1図に示すよりなメサ型に形成された
負性抵抗素子のベース層の幅Wは10〜30ミクロン程
度であり、これを高精度でコントロールすることは容易
ではなかった。
For this reason, for example, the width W of the base layer of the mesa-shaped negative resistance element shown in FIG. 1 is approximately 10 to 30 microns, and it has not been easy to control this with high precision.

又ウエハの工程中における破損を防止するためには最小
150ミクロン程度の厚さは必要であるから接合部J1
,J2の深さは60〜70ミクロンとなり、長時間の高
温での拡散は接合部J1,J2の部分的バラツキ及び結
晶の乱れ等を生じ、少数キャリアのライフタイムの低下
の原因ともなっていた。
Also, in order to prevent damage to the wafer during the process, a minimum thickness of about 150 microns is required, so the bonding part J1
, J2 was 60 to 70 microns deep, and the long-term high-temperature diffusion caused local variations in the junctions J1 and J2, disordered crystals, etc., and also caused a reduction in the lifetime of minority carriers.

一方小数キャリアのライフタイムを長くする方法として
は、ベース層の比抵抗を大きくしてもよいがブレークオ
ーバー電圧VBが大きくなり実際の回路定数からはずれ
てしまうし、ブレークオーバー電圧VBを小さくするた
めには接合部J1,J2の深さを浅くしベース層の幅を
広くせねばならないといった矛盾を生じることとなる。
On the other hand, one way to lengthen the lifetime of minority carriers is to increase the specific resistance of the base layer, but this increases the breakover voltage VB and deviates from the actual circuit constant. This creates a contradiction in that the depth of the joints J1 and J2 must be made shallow and the width of the base layer must be made wide.

また第1図に示すように、従来の二極負性抵抗素子のP
N接合J1,J2露呈部は半導体基体をエッチングする
ことによって傾斜を設けて耐圧破壊によって素子が破壊
されるのを防止するようになされている。
Furthermore, as shown in Figure 1, P of the conventional two-polar negative resistance element
The N-junctions J1 and J2 exposed portions are sloped by etching the semiconductor substrate to prevent the elements from being destroyed due to voltage breakdown.

しかし、長時間のエッチング工程が介在する為に生産コ
ストの上昇等の欠点を生じる。
However, since a long etching process is involved, there are drawbacks such as increased production costs.

本発明は、このような種々の問題点を解決したものであ
り、高比抵抗の半導体ベース層と、このベース層に接し
て両面に設けられた該ベース層とは逆の導電型の高い不
純物濃度をもつ半導体層と該逆の導電型の半導体層のう
ち少くとも一つを囲み底面を該ベース層に接する該ベー
ス層と同じ導電型で高い不純物濃度をもつ低比抵抗ベー
ス層と該逆の導電型の半導体層の外面に設けられた電極
とからなることを特徴とする二極負性抵抗半導体素子に
ある。
The present invention solves these various problems, and consists of a semiconductor base layer with a high specific resistance, and a highly impurity layer having a conductivity type opposite to that of the base layer, which is provided on both sides in contact with the base layer. a low resistivity base layer having the same conductivity type as the base layer and having a high impurity concentration surrounding at least one of the semiconductor layer having a high impurity concentration and a semiconductor layer having a conductivity type opposite to the base layer and having a bottom surface in contact with the base layer; and an electrode provided on the outer surface of a semiconductor layer of conductivity type.

以下本発明の実施例を断面図で示す第2図a1平面図で
示す第2図bによって説明する。
Embodiments of the present invention will be described below with reference to FIG. 2 a, which is a sectional view, and FIG. 2 b, which is a plan view.

第2図a,bにおいて、1は厚さ200ミクロン比抵抗
10〜100Ωcmの高比抵抗P型シリコン半導体から
なるベース層、2と3はベース層10両面に接して設け
られているベース層1とは逆の導電型の高い不純物濃度
をもつN型半導体層、4と5は各々N型半導体層2、N
型半導体層3を囲み底面をベース層1に接し高い不純物
濃度をもつ低比抵抗P型ベース層、6と1は各々N型半
導体層2、N型半導体層3の外面に設けられた電極であ
る。
In FIGS. 2a and 2b, 1 is a base layer made of a high resistivity P-type silicon semiconductor with a thickness of 200 microns and a resistivity of 10 to 100 Ωcm, and 2 and 3 are base layers 1 provided in contact with both sides of the base layer 10. 4 and 5 are N-type semiconductor layers 2 and 5, respectively, which have a high impurity concentration and a conductivity type opposite to
A low resistivity P-type base layer with a high impurity concentration surrounds the type semiconductor layer 3 and has a bottom surface in contact with the base layer 1, and 6 and 1 are electrodes provided on the outer surfaces of the N-type semiconductor layer 2 and the N-type semiconductor layer 3, respectively. be.

N型半導体層2,3の厚さは15ミクロンである。The thickness of the N-type semiconductor layers 2 and 3 is 15 microns.

この実施例に示す本発明の製造方法としては、ベース層
1となる高比抵抗のP型シリコン基板の両面に例えば不
純物として燐をドープしながらN型のエビタキシアル層
を形成し、次にP型不純物例えば硼素なエピタキシアル
層に拡散し底面が該P型シリコン基板に接する低比抵抗
のP型半導体層4,5を形成する。
In the manufacturing method of the present invention shown in this example, an N-type epitaxial layer is formed on both sides of a high-resistivity P-type silicon substrate serving as the base layer 1 while doping, for example, phosphorus as an impurity, and then a P-type Impurities such as boron are diffused into the epitaxial layer to form low resistivity P-type semiconductor layers 4 and 5 whose bottom surfaces are in contact with the P-type silicon substrate.

これによってP型半導体層4,5に囲まれたエビタキシ
アル層でN型半導体層2,3も形成される。
As a result, N-type semiconductor layers 2 and 3 are also formed as an epitaxial layer surrounded by P-type semiconductor layers 4 and 5.

最後に電極6,7を設ける。Finally, electrodes 6 and 7 are provided.

かくのごとぎ本発明の二極負性抵抗半導体素子は、ベー
ス層が幅の広い高比抵抗のベース層1と幅がN型半導体
層2,3と同じで狭い低比抵抗のベース層4,5で構成
されていることを特徴としている。
As described above, the bipolar negative resistance semiconductor device of the present invention has a base layer 1 having a wide base layer 1 having a high specific resistance, and a base layer 4 having a narrow low specific resistance having the same width as the N-type semiconductor layers 2 and 3. , 5.

従ってN型半導体層2,又はN型半導体層3からベース
層へ流れるキャリアの再結合はわずかじか生じないし、
プレークオーバ電圧は高比抵抗ベース層1によってはき
まらず、低比抵抗ベース層4とN型半導体層2との接合
及び低比抵抗ベース層5とN型半導体層3との接合によ
って定まる。
Therefore, recombination of carriers flowing from the N-type semiconductor layer 2 or the N-type semiconductor layer 3 to the base layer occurs only slightly,
The breakover voltage is not determined by the high resistivity base layer 1 but is determined by the junction between the low resistivity base layer 4 and the N-type semiconductor layer 2 and the junction between the low resistivity base layer 5 and the N-type semiconductor layer 3.

従ってN型半導体層2,3、低比抵抗べース層4,5の
デイメンジョンを適当に選択することによりプレークオ
ーバ特性を決めることができる。
Therefore, by appropriately selecting the dimensions of the N-type semiconductor layers 2 and 3 and the low resistivity base layers 4 and 5, the breakover characteristics can be determined.

実施例では高比抵抗のベース層10両面にN型半導体層
2及びN型半導体層3を囲むように低比抵抗ベース層4
及び抵比抵抗ベース層5を夫々設けたが、低比抵抗ベー
ス層を両面に設けることは必ずしも必要ではなく片面だ
けに設け、他の面はN型半導体層だけにしてもよい また、本発明の二極負性抵抗半導体素子P+導電型の低
比抵抗ベース層4,5を設けることにより、プレークオ
ーバ電圧を制御すると共に、高比抵抗ベース層1とN型
半導体層2,3との接合が半導体基体の側面から露呈す
るのを防止している。
In the embodiment, a low resistivity base layer 4 is formed on both sides of the high resistivity base layer 10 so as to surround the N-type semiconductor layer 2 and the N-type semiconductor layer 3.
Although the low resistivity base layer 5 and the low resistivity base layer 5 are respectively provided, it is not necessarily necessary to provide the low resistivity base layer on both sides, and it is also possible to provide the low resistivity base layer on only one side and only the N-type semiconductor layer on the other side. By providing low resistivity base layers 4 and 5 of P+ conductivity type, the breakover voltage can be controlled and the junction between high resistivity base layer 1 and N-type semiconductor layers 2 and 3 can be controlled. is prevented from being exposed from the side surface of the semiconductor substrate.

かくして本発明によれば、ベース層の幅の正確なコント
ロールは必要ではなく、又厚い半導体基板を用いること
が可能であるから工程途中での割れも減少し製造技術上
大きな利点を有する。
Thus, according to the present invention, it is not necessary to accurately control the width of the base layer, and since it is possible to use a thick semiconductor substrate, cracking during the process is reduced, which is a great advantage in terms of manufacturing technology.

さらに又、この素子と共に別の素子を低比抵抗ベース層
4又は低比抵抗ベース層5の外側のベース層10面に合
せ設ける場合には、該低比抵抗ベース層45はアイソレ
ーションの役目をも兼ねることができる。
Furthermore, when another element is provided along with this element on the outer base layer 10 surface of the low resistivity base layer 4 or the low resistivity base layer 5, the low resistivity base layer 45 plays the role of isolation. It can also serve as

また、第1図の二極負性抵抗素子は、周知のように、接
合J1,J2が耐圧破壊を生じるのを防止する為に、ベ
ベル構造を形成しているが、本発明は低比抵抗ベース層
4,5を形成することによって、半導体装置の側面から
接合部が露呈しないように構成されている。
Furthermore, as is well known, the two-pole negative resistance element shown in FIG. By forming the base layers 4 and 5, the structure is such that the bonding portion is not exposed from the side surface of the semiconductor device.

従って、長時間によるエッチング等によってベベル構造
とする必要がない利点を有する。
Therefore, there is an advantage that it is not necessary to form a beveled structure by etching or the like over a long period of time.

なお、本発明は、実施例にとらわれるものではなく、導
電型を反対にしたり、構成する各物分のデイメンジョン
を変化させたり、又全体を絶縁膜で被って保護したりす
ることは本発明の範囲を離脱するものではない。
Note that the present invention is not limited to the embodiments, and it is possible to reverse the conductivity type, change the dimension of each component, or protect the entire structure by covering it with an insulating film. This does not depart from the scope of the invention.

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

第1図は従来のメサ型負性抵抗素子のペレットの断面図
、第2図aは本発明の二極負性抵抗半導体素子のペレッ
ト断面図、第2図bは第2図aの平面図である 1・・・・・・・・・高比抵抗P型ベース層、2,3・
・・・・・・・・N型半導体層、4,5・・・・・・・
・・低比抵抗P型ベース層。
Figure 1 is a sectional view of a pellet of a conventional mesa-type negative resistance element, Figure 2a is a sectional view of a pellet of a bipolar negative resistance semiconductor element of the present invention, and Figure 2b is a plan view of Figure 2a. 1......High resistivity P type base layer, 2,3...
......N-type semiconductor layer, 4,5...
...Low resistivity P type base layer.

Claims (1)

【特許請求の範囲】[Claims] 1 高比抵抗半導体ベース層の両面に該半導体ベース層
の導電型と反対導電型の第1と第2の半導体層ヲエビタ
キンヤル成長法により形成した半導体基体にして、該高
比抵抗半導体ベース層と同一導電型であって高い不純物
濃度をもつ第1と第2の低比抵抗ベース層を該第1と第
2の半導体層の周端縁にその底面が夫々該高比抵抗半導
体ベース層に接する如く拡散形成して、該高比抵抗半i
体ペース層と該第1と第2の半導体層との接合部が半導
体基体側面から露呈するのを防止し、該第1と第2の半
導体層の主表面に電極を形成したことを特徴とする二極
負性抵抗半導体素子。
1 A semiconductor substrate formed by an epitaxial growth method with first and second semiconductor layers of conductivity type opposite to that of the semiconductor base layer on both sides of the high resistivity semiconductor base layer, and having the same conductivity as the high resistivity semiconductor base layer. First and second low resistivity base layers of a conductive type and having a high impurity concentration are placed at the peripheral edges of the first and second semiconductor layers such that their bottom surfaces are in contact with the high resistivity semiconductor base layer, respectively. Diffused to form the high specific resistance half i
The method is characterized in that the joint between the body spacer layer and the first and second semiconductor layers is prevented from being exposed from the side surface of the semiconductor substrate, and electrodes are formed on the main surfaces of the first and second semiconductor layers. A bipolar negative resistance semiconductor device.
JP52005661A 1977-01-21 1977-01-21 Bipolar negative resistance semiconductor device Expired JPS584831B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP52005661A JPS584831B2 (en) 1977-01-21 1977-01-21 Bipolar negative resistance semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP52005661A JPS584831B2 (en) 1977-01-21 1977-01-21 Bipolar negative resistance semiconductor device

Publications (2)

Publication Number Publication Date
JPS5390883A JPS5390883A (en) 1978-08-10
JPS584831B2 true JPS584831B2 (en) 1983-01-27

Family

ID=11617282

Family Applications (1)

Application Number Title Priority Date Filing Date
JP52005661A Expired JPS584831B2 (en) 1977-01-21 1977-01-21 Bipolar negative resistance semiconductor device

Country Status (1)

Country Link
JP (1) JPS584831B2 (en)

Also Published As

Publication number Publication date
JPS5390883A (en) 1978-08-10

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