JPS6031108B2 - Manufacturing method of semiconductor device - Google Patents
Manufacturing method of semiconductor deviceInfo
- Publication number
- JPS6031108B2 JPS6031108B2 JP50087395A JP8739575A JPS6031108B2 JP S6031108 B2 JPS6031108 B2 JP S6031108B2 JP 50087395 A JP50087395 A JP 50087395A JP 8739575 A JP8739575 A JP 8739575A JP S6031108 B2 JPS6031108 B2 JP S6031108B2
- Authority
- JP
- Japan
- Prior art keywords
- current
- semiconductor substrate
- base
- mos
- circuit
- 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
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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
- H10D84/80—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]
- H10D84/85—Complementary IGFETs, e.g. CMOS
- H10D84/854—Complementary IGFETs, e.g. CMOS comprising arrangements for preventing bipolar actions between the different IGFET regions, e.g. arrangements for latchup prevention
Landscapes
- Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)
- Bipolar Transistors (AREA)
Description
【発明の詳細な説明】
本発明は相補型電界効果トランジスタ(以後C/MOS
と略称する)に寄生するバィポーラTrによる難点を排
除した半導体装置の製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a complementary field effect transistor (hereinafter referred to as C/MOS).
The present invention relates to a method of manufacturing a semiconductor device that eliminates the drawbacks caused by bipolar transistors parasitic on the semiconductor device.
従来からC/MOSで構成した回路は種々知られている
が、その代表例を第1図及び第2図により説明する。Various circuits constructed using C/MOS have been known in the past, and representative examples thereof will be explained with reference to FIGS. 1 and 2.
このインバータ回路はPチャンネルMOSTr8,とN
チャンネルMOSTr82とで構成され、8,のソース
電極は正電源Vooに接続する外、8,のドレィン電極
は82のドレィン電極と共通接続して出力端に、82の
ソース電極は負電源V$に結ぶ。又8,及び82のゲー
ト電極は共に入力端に結んでィンバータを構成する。第
2図はこの回路を半導体ウェハに作成した断側面図であ
る。This inverter circuit consists of P channel MOS Tr8 and N
The source electrode of 8 is connected to the positive power source Voo, the drain electrode of 8 is commonly connected to the drain electrode of 82 to form the output terminal, and the source electrode of 82 is connected to the negative power source V$. tie. Further, the gate electrodes 8 and 82 are both connected to the input terminal to form an inverter. FIG. 2 is a cross-sectional side view of this circuit formed on a semiconductor wafer.
この例では1×1びもtoms/の位の濃度を持つN導
電形基板1に2×1び6atoms/仇程度の濃度を有
するP導電型不純物よりなるいわゆるP−Well層2
を形成し、このP−Well層2外のN導電型基板にP
チャンネルMOSTrとなるP領域3,4を(例えば1
び9a■ms/の)拡散する。一方前記P−Well層
2内にもNチャンネルMOSTrとなるN領域5,6を
N導電形不純物を1ぴoatoms/の程度拡散する。
更にP−Well領域2及びこれ以外の半導体基板1に
は電源に接続するP及びN形の拡散領域7,8を形成す
る。これに続いてMOSTrのゲートとなる位置に約1
500△の薄い珪素酸化物を被着し、必要部分を関孔し
て山等の半導体で回路接続する。必要ならば基板上に保
護膜を設けてC/MOS半導体素子が得られる。この工
程は概略であり一例を示したものである。このような構
造を有するC/MOS回路はPチヤンネルMOSTrと
NチヤンネルMOSTrのしきし・直電圧ythが逆極
性を持つため入力電圧に対して夫々全て逆の動作を行い
その動作/ぐヮは非常に小さい。例えばVoDに5V,
Vssを接地(GND)とした際入力lnに十5Vが供
給されれば02は導通(ON)し、8,は非導通(OF
F)となり、VDo−V$間に直流電流が流れないこと
になる。そのためC/MOS回路は一般に動作消費電力
が殆んどなく入力情報のパルス過渡領域で8,,82
が共にONし、瞬時の過度電流が流れることと、PN接
合に起るリーク電流及び出力にある負荷容量を充放電す
るための電流が流れるに過ぎない。従って一般にC/M
OS回路のPowerは極小と言える。しかしこのよう
なC/MOS回路系にあっては出力或は入力にimpu
lse的にノイズが加わった時Vo。In this example, a so-called P-well layer 2 made of an N conductivity type impurity having a concentration of about 2×1 and 6 atoms/substrate is formed on an N conductivity type substrate 1 having a concentration of about 1×1 atoms/substrate.
is formed on the N conductivity type substrate outside this P-Well layer 2.
The P regions 3 and 4 that will become the channel MOSTr (for example, 1
and 9a ms/). On the other hand, also in the P-well layer 2, N conductivity type impurities are diffused to the extent of 1 poatoms/in the N regions 5 and 6 which will become the N channel MOSTr.
Furthermore, P- and N-type diffusion regions 7 and 8 connected to a power source are formed in the P-well region 2 and the rest of the semiconductor substrate 1. Following this, approximately 1
A thin layer of silicon oxide with a thickness of 500△ is deposited, holes are formed in the necessary areas, and a circuit is connected using a semiconductor such as a mountain. If necessary, a protective film is provided on the substrate to obtain a C/MOS semiconductor device. This process is schematic and is provided as an example. In a C/MOS circuit having such a structure, the threshold/direct voltage yth of the P-channel MOSTr and the N-channel MOSTr have opposite polarities, so they all operate in the opposite direction with respect to the input voltage, and their operation is extremely unstable. small. For example, 5V for VoD,
When Vss is grounded (GND), if 15V is supplied to input ln, 02 will be conductive (ON) and 8, will be non-conductive (OF
F), and no direct current flows between VDo and V$. Therefore, C/MOS circuits generally have almost no operating power consumption, and in the pulse transient region of input information, 8, 82
Both turn on, and only an instantaneous transient current flows, a leakage current occurring in the PN junction, and a current for charging and discharging the load capacitance at the output. Therefore, generally C/M
The power of the OS circuit can be said to be extremely small. However, in such a C/MOS circuit system, there is an impu
Vo when noise is added like lse.
−V$間にDCの大電流(数十mA〜数百mA)が流れ
、そのノイズを取り除いても定常的にその電流を保持し
続ける現象が起った。このImpulseの極性には正
負があり、この現象を解除するにはVoDを或る一定電
圧以下に下げるか回路系の電源を切らねばならなかった
。本発明は上記の欠点を除去した新規な半導体装置の製
造方法を提供するものである。即ちC/MOS構造を有
する半導体装置にあっては特定のサィリスタ回路が構成
されることを見出した事実を基に完成したものである。A phenomenon occurred in which a large DC current (several tens of mA to several hundred mA) flows between -V$ and the current continues to be maintained even after the noise is removed. The polarity of this impulse has positive and negative polarities, and in order to eliminate this phenomenon, it is necessary to lower the VoD below a certain voltage or turn off the power to the circuit system. The present invention provides a novel method for manufacturing a semiconductor device that eliminates the above-mentioned drawbacks. That is, it was completed based on the fact that it was discovered that a specific thyristor circuit is configured in a semiconductor device having a C/MOS structure.
第3図はこのサィリスタ回路がC/MOS回路内に作成
された状態を示した断側面図であり、第4図はその等価
回路図である。FIG. 3 is a cross-sectional side view showing this thyristor circuit created in a C/MOS circuit, and FIG. 4 is an equivalent circuit diagram thereof.
これは複数のバィポーラTrから成りサィリスタ動作が
一旦生じるとパワーが膨大となることが多い。このサィ
リスタ回路を第3図により説明するとN形半導体基板1
川こ形成されたP−Well領域11には半導体基板の
厚さ方向に沿って寄生バイポーラTr2,Tr4が、又
P−Well領域1 1外の半導体基板10には、この
厚方向に交叉する方向に寄生バィポーラTr,,Tr3
が形成される外、P−Well領域1 1及びN形半導
体基板10の保有する抵抗とで前記サィリス夕回路が構
成される。又C/MOSに必要なソース、ドレィンを構
成するN+領域12,13、P+領域14,15とコン
タクト領域となるP十領域16,N十領域17が形成さ
れ更にガードリング層18が形成される。以下の説明で
Qはバィポーラトランジスタ用語として一般こ定義され
る電流増中率、B‘ま三7で定義される電流増中率、1
は電流、1に付属した記号でe:ェミツタ、b:ベース
、c:コレク夕、又数字又は記号は各Tr及び抵抗を意
味する。This is made up of a plurality of bipolar transistors, and once thyristor operation occurs, the power often becomes enormous. To explain this thyristor circuit with reference to FIG. 3, an N-type semiconductor substrate 1
Parasitic bipolar transistors Tr2 and Tr4 are formed along the thickness direction of the semiconductor substrate in the P-Well region 11 formed by the river, and parasitic bipolar transistors Tr2 and Tr4 are formed in the semiconductor substrate 10 outside the P-Well region 11 in a direction crossing this thickness direction. parasitic bipolar Tr,, Tr3
In addition to the above, the resistor circuit is constituted by the P-well region 11 and the resistor held by the N-type semiconductor substrate 10. Further, N+ regions 12, 13 and P+ regions 14, 15 forming the sources and drains necessary for the C/MOS, P+ regions 16 and N+ regions 17 serving as contact regions are formed, and a guard ring layer 18 is further formed. . In the following explanation, Q is a current increase rate generally defined as a bipolar transistor term, a current increase rate defined by B'Masan7, 1
is current, and the symbols attached to 1 are e: emitter, b: base, c: collector, and the numbers or symbols mean each Tr and resistance.
第4図の実線矢印に示すように出力に正のィンパルスノ
ィズが加わるとQ3 ×linの電流がRp−well
をバィパスして流れその電圧降下がV戊2になった時T
r2のベースに電流1ぬ が流れる。As shown by the solid arrow in Fig. 4, when positive impulse noise is added to the output, the current of Q3 × lin flows into the Rp-well.
When the voltage drop becomes V2, T
A current 1 flows through the base of r2.
I蛇ごQ3Iin(Rp−Well>〉rbe2 …
…【lITr2のコレクタ電流を1のとすると・偽 ニ
821b2ニ82 は31in ……■同様に
13がドライブ電流となってRNsub間での電圧降下
がVbe,になった時Tr,のベース電流lb,が流れ
てTr,はON状態となる。Ijago Q3Iin (Rp-Well>>rbe2...
...[If the collector current of lITr2 is 1, False Ni821b2ni82 is 31in...■Similarly, when 13 becomes the drive current and the voltage drop between RNsub becomes Vbe, the base current of Tr, lb , flows, and Tr is in the ON state.
lb,=lc2(RNSub>rq) ・・
・・・・‘3’lc,=6,lq=3,62 Q31i
n ……【41ここで外部からのノイズが取除
かれてもVDo−GND間即ちTr,,Tr2間で電流
が保持されるためにはlb2Sic.
・・・・・・t51の条件が満足されて
いれば良い。lb,=lc2(RNSub>rq)...
...'3'lc,=6,lq=3,62 Q31i
n...[41 Here, in order for the current to be maintained between VDo and GND, that is, between Tr, Tr2 even if external noise is removed, lb2Sic.
...It is sufficient if the condition of t51 is satisfied.
即ちQ31inミ8,P2 Q31in
1=ミ8,62 ……■
1<8,82の条件が成立した時1サイクルのベース電
流IQ(n)より次の1サイクルのベース電流IQ(n
十1)が大となるので、サイクルを繰り返すことによっ
て系を流れる電流が増加すると6maxを境にして8が
減少し始めるので無限に発散する訳でない。That is, Q31in Mi8,P2 Q31in 1=Mi8,62...■ When the condition 1<8,82 is satisfied, the base current IQ(n) of one cycle is changed from the base current IQ(n) of the next one cycle.
11) becomes large, and as the current flowing through the system increases by repeating the cycle, 8 starts to decrease after reaching 6max, so it does not diverge infinitely.
即ち定常状態で前述のような異常電流としては次の2条
件を満たすところで落着くと考えられる。lb2(n−
1):lb2(n),8,(n)・8(n)と・又先の
Trの寸法の大小が前記異常電流が流れる現象の起り易
さについての主要因でないが、上式を基に考察する。That is, in a steady state, the above-mentioned abnormal current is considered to settle down when the following two conditions are satisfied. lb2(n-
1): lb2(n), 8, (n), 8(n), etc.Although the size of the Tr is not the main factor in the likelihood of the abnormal current flowing, based on the above equation, will be considered.
Trの寸法(正確にはドレィン面積)の大小をパラメー
タとした電流増中率を測定したところ異常電流が収数し
た時の電流値とTr寸法の大小とは相関があり大きなド
レィン面積を持ったTr程異常電流が大となり逆に小さ
いTrはその値が小さくなる。又出力に負のノイズが加
わっても正のノイズと同様にlb,ミQ41in(RN
subミr戊,) ・・・・・・【7’lc,=
8,lq=8,Q41inlb2ニに,(Rp−wel
l》r戊2)lc2:B21Q=3,82 Q41in
系の電流が保持するための条件としては
lb,≦に2 1≦8,82 ……■とな
る。When we measured the current increase rate using the size of the Tr dimensions (more precisely, the drain area) as a parameter, we found that there was a correlation between the current value when the abnormal current was collected and the size of the Tr dimensions, and the drain area was large. The higher the Tr, the larger the abnormal current, and conversely, the smaller the Tr, the smaller the value. Also, even if negative noise is added to the output, lb, mi Q41in (RN
submir 戊,) ・・・・・・【7'lc,=
8, lq=8, Q41inlb2, (Rp-wel
l》r戊2) lc2:B21Q=3,82 Q41in
The conditions for maintaining the current in the system are lb,≦2 1≦8,82...■.
このように前記サィリスタ回路の動作によって発生する
異常電流を防止するには半導体基板の厚さ方向にほ)、
沿って形成されるバィポーラTr則ちVertical
Trと半導体基板の主面にはゞ沿って形成されるLaに
raITrのP積を1以下に保持すれば良い事を示した
。次にこの条件を満足する具体的手段としては{ィ}ベ
ース中を拡大する。In order to prevent the abnormal current generated by the operation of the thyristor circuit, it is necessary to
Bipolar Tr formed along the vertical
It has been shown that it is sufficient to keep the P product of raITr to 1 or less for La formed along the main surface of the transistor and the semiconductor substrate. Next, as a concrete means to satisfy this condition, {i} expands the inside of the base.
‘ロー半導体基板のライフタイムを小にするし一半導体
基板の基となるウェハーのライフタイムを小にする〇半
導体基板のライフタイムを小にするために熱処理工程を
挿入する■半導体基板にAuをドープする等の手段が有
効なことが判った。川についてであるが第3図に示した
VemcalTr2及びTr4のベース中則ちN−su
bl oとN+領域12間、更にN−s帆10とN十領
域13間の距離を拡大することと、LateralTr
,及びTr3のベース中則ち、P−Well領域1 1
とP+領域14、P−Wen領域11とP+領域15問
の距離を拡大することである。'Reducing the lifetime of the raw semiconductor substrate and reducing the lifetime of the wafer that is the base of the semiconductor substrate 〇 Inserting a heat treatment process to shorten the lifetime of the semiconductor substrate ■ Adding Au to the semiconductor substrate It has been found that methods such as doping are effective. Regarding the river, the base medium of Vemcal Tr2 and Tr4 shown in Figure 3 is N-su.
By enlarging the distance between blo o and the N+ region 12, and further between the N-s sail 10 and the N+ region 13, and by increasing the distance between the LateralTr
, and the base of Tr3, that is, P-Well region 1 1
and the distance between the P+ area 14, the P-Wen area 11, and the P+ area 15 questions.
第5図及び第6図には、VerticalNPNTr及
びLaにraIPNPTrのベース中Wv(仏),WL
(仏)を又縦軸には電流増中率hfevを探って、ベー
ス中による依存性を示した。縦軸に示した電流増中率は
各ベース中毎の測定によって得られた値の中最大値を採
用している。尚第5図におけるVenjcaITr2T
r4のベース中は、実質的にはP−Well領域11の
深さ(即ち半導体基板の厚さ方向)の距裏珪xiから各
N+領域1 2,1 3の深さ距離を差引し、た値を示
した。尚第5図ではP−Well領域のスランピング時
間を20,40,60時間と変化させその時P−Wel
l領域表示濃度が一定となるようドーズ量を補正した。
一方第7図にはVemcaITrのP−Well領域の
深さ距離L(仏)を機軸には凶teraITrのベース
中WL(一)を探って両Trの電流増中率の積則ち3積
が1より大きい場合には前記異常電流が起り、1より4
・さし、時には起らなかった。In Figures 5 and 6, Wv (France), WL in the base of VerticalNPNTr and La of raIPNPTr are shown.
(France), and the current increase rate hfev was plotted on the vertical axis to show its dependence on the base medium. For the current increase rate shown on the vertical axis, the maximum value among the values obtained by measurements for each base is adopted. In addition, VenjcaITr2T in FIG.
The base of r4 is substantially calculated by subtracting the depth distance of each N+ region 1 2, 1 3 from the backside silicon xi at the depth of the P-Well region 11 (that is, in the thickness direction of the semiconductor substrate). The value was shown. In addition, in FIG. 5, the slumping time of the P-Well area is changed to 20, 40, and 60 hours, and the P-Well area is
The dose amount was corrected so that the displayed concentration in the l area was constant.
On the other hand, Fig. 7 shows the product of the current increase rates of both Tr, which is 3 products, by searching for WL (1) in the base of the teraITr based on the depth distance L (France) of the P-Well region of the VemcaITr. If it is larger than 1, the abnormal current occurs;
・Sometimes it didn't happen.
しかし第5図及び第6図に示した電流増中率はそのC/
MOS回路を作成するPrOCeSSによって、その値
が変化するため、第7図のB積を示す直線の勾配は変化
します。However, the current increase rate shown in Figures 5 and 6 is that C/
Since its value changes depending on the PrOCeSS used to create the MOS circuit, the slope of the straight line showing the B product in Figure 7 changes.
しかしVerticaITrとじteraITrのベー
ス中即ちP一Well領域の深さとLaにraITrの
ベース中を選択して8積を1以下に抑えると異常電流が
防止可能となる。However, by selecting the depth of the VerticaITr and the base of the teraITr, that is, the depth of the P-Well region and the base of the raITr for La, and suppressing the 8 product to 1 or less, abnormal current can be prevented.
P一Well領域11とP+領域14,15間の距離を
広げることはLateralPNPTrの電流増中率を
小さくしようとするものであるが、これはVemcaI
NPNTrのベース中がP−Well領域のxiで規定
されることになる。Increasing the distance between the P-Well region 11 and the P+ regions 14 and 15 is intended to reduce the current increase rate of the LateralPNPTr, but this
The base of the NPNTr is defined by xi of the P-Well region.
しかしいteralPNPTrの輸送効率はあるベース
中値によって0になることも起り得るので際限なく広げ
得ない。このようにLate例TrとVenjcaIT
rのベース中WL,Wvの制御によって8積を1以下は
規正することが可能となる。However, the transport efficiency of teralPNPTr may become 0 depending on a certain base median value, so it cannot be expanded indefinitely. Late example Tr and VenjcaIT like this
By controlling WL and Wv in the base of r, it is possible to regulate the 8 product to 1 or less.
次に半導体基板のライフタイムを小さくするし一・〜片
の手段について説明する。Next, some means for reducing the lifetime of the semiconductor substrate will be explained.
し一の手法の具体的手段は半導体単結晶を引上げる工程
後この単結晶の比抵抗を補正するために実施する熱処理
温度を約1100℃にすることである。A specific means of this method is to set the heat treatment temperature to about 1100° C. after the step of pulling the semiconductor single crystal in order to correct the resistivity of the single crystal.
従来この種の熱処理温度は950oo位で行われていた
が、1100oo附近で行うことによっていteraI
Tr及びVerticalTrの電流増中率をLaにr
aITrでは5×10‐2から1.4×10‐2,Ve
rticalTrでは200→56に下がることが確め
られた。前述の熱処理工程の温度領域は1000oo〜
115000が可能であり1050qo〜1150q0
は可成り有効であり又1100qoが最良である。Conventionally, this type of heat treatment was performed at a temperature of about 950 oo, but by performing it at around 1100 oo,
The current increase rate of Tr and Vertical Tr is set to La.
aITr from 5×10-2 to 1.4×10-2, Ve
It was confirmed that the rtical Tr decreased from 200 to 56. The temperature range of the heat treatment process mentioned above is 1000 oo~
115000 is possible and 1050qo~1150q0
is quite effective and 1100qo is the best.
次に仁}の手段はC/MOS製作工程におけるゲート酸
化工程後に実施する。Next, the method described above is carried out after the gate oxidation step in the C/MOS manufacturing process.
このC/MOS工程は一般的には以下のようにして実施
される。半導体基板に酸化物を被着後所望の位置をPE
P法で除去してから露出した半導体基板内に不純物を拡
散してソース、ドレイン領域を作る。勿論このソース、
ドレィン領域以外にも前述のように拡散領域を作成する
。ソース、ドレィン領域の間にはゲート電極を作成する
為、この領域に相当する部分の酸化物を除去してから露
出した半導体基板に薄い酸化物を被看する。(以下、こ
の工程を酸化工程と略する。)この工程後、半導体基板
を120000で1び分間熱処理した。This C/MOS process is generally carried out as follows. After depositing the oxide on the semiconductor substrate, apply PE to the desired location.
After removal using the P method, impurities are diffused into the exposed semiconductor substrate to form source and drain regions. Of course this sauce,
In addition to the drain region, a diffusion region is created as described above. In order to form a gate electrode between the source and drain regions, the oxide in the portion corresponding to this region is removed and then a thin oxide is deposited on the exposed semiconductor substrate. (Hereinafter, this step will be abbreviated as an oxidation step.) After this step, the semiconductor substrate was heat-treated at 120,000 ℃ for 1 minute.
この工程を実施後従来と同様な工程を行ってから、仏t
eraITrとVenicaITrの電流増中率を測定
したところ、VemcaITr2Tr4では前記熱処理
工程を実施しないものは、200を示したのに対し実施
したものは50LateralTr.Tらでは5×1ぴ
が1.4×10‐2に低下して極めて有効であった。次
に【対の方法について述べる。これはゲート酸化工程後
半導体基板の裏面即ち回路素子が形成されていない部分
に被着している酸化物を除去し、更に、この部分を清浄
にする為食刻工程を行って30仏程度半導体基板を除去
する。After implementing this process, perform the same process as before, and then
When the current increase rate of eraITr and VenicaITr was measured, VemcaITr2Tr4 without the heat treatment showed a value of 200, whereas that of VemcaITr2Tr4 without the heat treatment process showed a value of 50LateralTr. In T. et al., 5×1 pi was reduced to 1.4×10-2, and it was extremely effective. Next, we will discuss the pairing method. After the gate oxidation process, the oxide adhering to the back side of the semiconductor substrate, that is, the area where circuit elements are not formed, is removed, and an etching process is performed to clean this area. Remove the substrate.
次に金を厚さ300A程度蒸着する。この蒸発源として
は直径1側の金線を使用して被蒸着物即ち、半導体基板
温度は室温とする。前記蒸着工程完了後は1100こC
に10分間N2中で保持してから従釆工程に移行する。Next, gold is deposited to a thickness of about 300A. A gold wire with a diameter of 1 is used as the evaporation source, and the temperature of the object to be evaporated, that is, the semiconductor substrate, is set at room temperature. After the vapor deposition process is completed, the temperature is 1100℃.
After holding in N2 for 10 minutes, proceed to the secondary process.
この工程を挿入して得られたC/MOS回路はVert
icalTrの電流増中率は第8図のようになった。こ
の図は横軸に蒸着後行う加熱時間を探り縦軸には金をド
ーブした電流増中率と金拡散がない時のそれとの比を採
ったものである。この図から判るように金が拡散するに
つれて電流増中率が低下しており、有効なことが判る。
この金拡散が寄生Trの中VerticalTrZ玖t
eraITrであり又P岬Tr>npnTrである。The C/MOS circuit obtained by inserting this process is Vert.
The current increase rate of icalTr was as shown in FIG. In this figure, the horizontal axis shows the heating time after vapor deposition, and the vertical axis shows the ratio of the current increase rate when doping with gold to that when there is no gold diffusion. As can be seen from this figure, the current increase rate decreases as the gold diffuses, indicating that it is effective.
This gold diffusion creates a vertical Tr inside the parasitic Tr.
eraITr and P MisakiTr>npnTr.
このように本発明はC/MOSTrに形成される寄生T
rの8積を1より小さく制御することによって、異常電
流の発生が防止可能となったので極めて実用的でありま
す。In this way, the present invention solves the problem of parasitic T formed in C/MOSTr.
By controlling the 8 product of r to be less than 1, it is possible to prevent abnormal current from occurring, which is extremely practical.
【図面の簡単な説明】
第1図は従釆のC/MOS回路図、第2図は第1図回路
を半導体基板に作成した断側面図、第3図は本発明に係
る半導体基板の断側面図、第4図はC/MOS回路素子
に形成されるサィリスタ回路の等価回路図、第5図はV
erticalTrのベース中を機軸に、縦軸に電流増
中率を探り電流増中率hfevのベース中依存性を示し
た図、第6図はいteraITrの電流増中率のベース
中依存性を示した図、第7図は寄生両Trのベース中と
両Trの8積の関係を示した図、第8図は金拡散有無に
よる電流増中率の関係を示した図である。
図において、1 0:半導体基板、1 1:ゥェル領域
、Tr,,Tr3:寄生はteraITr、Tr2,T
r4:寄生Ve九icaITr。第1図
第2図
第3図
第5図
第4図
第6図
第7図
第8図[Brief Description of the Drawings] Fig. 1 is a C/MOS circuit diagram of a subsidiary, Fig. 2 is a cross-sectional side view of the circuit shown in Fig. 1 created on a semiconductor substrate, and Fig. 3 is a cross-sectional view of a semiconductor substrate according to the present invention. The side view, Fig. 4 is an equivalent circuit diagram of a thyristor circuit formed in a C/MOS circuit element, and Fig. 5 is a V
Figure 6 shows the dependence of the current increase rate hfev on the base, with the base of the erticalTr as the axis, and the current increase rate on the vertical axis. 7 is a diagram showing the relationship between the base of both parasitic transistors and the 8 product of both transistors, and FIG. 8 is a diagram showing the relationship between the current increase rate depending on the presence or absence of gold diffusion. In the figure, 10: semiconductor substrate, 11: well region, Tr,, Tr3: parasitics are teraITr, Tr2, T
r4: Parasitic Ve9icaITr. Figure 1 Figure 2 Figure 3 Figure 5 Figure 4 Figure 6 Figure 7 Figure 8
Claims (1)
を形成し、この不純物領域外の前記半導体基板に第2導
電型のチヤンネルを有するMOS型Trを形成し、前記
不純物領域に第1導電型のチヤンネルを有するMOS型
Trを形成する半導体装置の製造方法において、前記半
導体基板の基となる半導体単結晶を引上げる工程後、1
000℃乃至1150℃の熱処理工程を具備することを
特徴とする半導体装置の製造方法。1. An impurity region of a second conductivity type is formed in a semiconductor substrate of a first conductivity type, a MOS type transistor having a channel of a second conductivity type is formed in the semiconductor substrate outside the impurity region, and a first impurity region is formed in the impurity region. In a method for manufacturing a semiconductor device forming a MOS type Tr having a channel of a conductivity type, after the step of pulling a semiconductor single crystal serving as a base of the semiconductor substrate, 1
1. A method for manufacturing a semiconductor device, comprising a heat treatment step at 000°C to 1150°C.
Priority Applications (8)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50087395A JPS6031108B2 (en) | 1975-07-18 | 1975-07-18 | Manufacturing method of semiconductor device |
| GB29283/76A GB1559583A (en) | 1975-07-18 | 1976-07-14 | Complementary mosfet device and method of manufacturing the same |
| DE2632448A DE2632448B2 (en) | 1975-07-18 | 1976-07-19 | CMOS device |
| FR7621991A FR2318500A1 (en) | 1975-07-18 | 1976-07-19 | COMPLEMENTARY METAL-OXIDE-SEMICONDUCTOR FIELD-EFFECT TRANSISTOR CIRCUIT AND ITS MANUFACTURING PROCESS |
| CH923576A CH613071A5 (en) | 1975-07-18 | 1976-07-19 | |
| US05/890,029 US4167747A (en) | 1975-07-18 | 1978-03-24 | Complementary mosfet device and method of manufacturing the same |
| US06/041,764 US4302875A (en) | 1975-07-18 | 1979-05-23 | Complementary MOSFET device and method of manufacturing the same |
| MY313/81A MY8100313A (en) | 1975-07-18 | 1981-12-30 | A complementary mosfet device and method of manufacturing the same |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50087395A JPS6031108B2 (en) | 1975-07-18 | 1975-07-18 | Manufacturing method of semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5211870A JPS5211870A (en) | 1977-01-29 |
| JPS6031108B2 true JPS6031108B2 (en) | 1985-07-20 |
Family
ID=13913681
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP50087395A Expired JPS6031108B2 (en) | 1975-07-18 | 1975-07-18 | Manufacturing method of semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6031108B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4387119B2 (en) | 2003-03-27 | 2009-12-16 | 三菱電機株式会社 | Semiconductor device |
| JP2009231851A (en) * | 2009-07-09 | 2009-10-08 | Mitsubishi Electric Corp | Semiconductor device |
-
1975
- 1975-07-18 JP JP50087395A patent/JPS6031108B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5211870A (en) | 1977-01-29 |
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