Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6130436B2 - - Google Patents
[go: Go Back, main page]

JPS6130436B2 - - Google Patents

Info

Publication number
JPS6130436B2
JPS6130436B2 JP52081314A JP8131477A JPS6130436B2 JP S6130436 B2 JPS6130436 B2 JP S6130436B2 JP 52081314 A JP52081314 A JP 52081314A JP 8131477 A JP8131477 A JP 8131477A JP S6130436 B2 JPS6130436 B2 JP S6130436B2
Authority
JP
Japan
Prior art keywords
region
impurity concentration
conductivity
semiconductor
diode element
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
JP52081314A
Other languages
Japanese (ja)
Other versions
JPS5416184A (en
Inventor
Hiroshi Sakuma
Toshuki Suzuki
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.)
NEC Corp
Original Assignee
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP8131477A priority Critical patent/JPS5416184A/en
Publication of JPS5416184A publication Critical patent/JPS5416184A/en
Publication of JPS6130436B2 publication Critical patent/JPS6130436B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D8/00Diodes
    • H10D8/411PN diodes having planar bodies

Landscapes

  • Bipolar Integrated Circuits (AREA)

Description

【発明の詳細な説明】 本発明は、誘電体絶縁基板上の半導体薄膜に形
成された半導体ダイオード素子、特に高耐圧ダイ
オード素子に係る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor diode element, particularly a high voltage diode element, formed in a semiconductor thin film on a dielectric insulating substrate.

近年、誘電体絶縁基板上にトランジスタや集積
回路素子を形成できれば、素子分離や寄生容量の
低減に著しい効果が期待されるところからシリコ
ンオンサフアイヤ(Silicon on Sapphire=
SOS)基板の様な誘電体絶縁基板上にシリコン単
結晶膜をエピタキシヤル成長させた高品質半導体
基板が、安価に得られるようになり、このような
基板を用いた半導体装置の研究開発が盛んに行な
われている。
In recent years, silicon on sapphire (Silicon on Sapphire =
High-quality semiconductor substrates made by epitaxially growing silicon single crystal films on dielectric insulating substrates such as SOS (SOS) substrates have become available at low cost, and research and development of semiconductor devices using such substrates is flourishing. It is carried out in

たとえば、シリコンオンサフアイヤ(以下、
SOS基板と略す)基板に半導体集積回路装置を構
成する場合、PN接合ダイオードは、その一構成
素子として重要である。特に、各素子分離の完全
なこの種の半導体装置は、本質的に高耐圧動作回
路向きであり、たとえば、SOS基板上で、他のト
ランジスタ素子と同様の工程により、良好な特性
を持つ高耐圧ダイオード素子が得られることが望
まれている。この場合、用いる基板の導電型に対
応させて、n+pp+型のダイオードを形成する
ことになる。
For example, silicon-on-sapphire (hereinafter referred to as
When configuring a semiconductor integrated circuit device on a substrate (abbreviated as an SOS substrate), a PN junction diode is an important component. In particular, this type of semiconductor device with complete isolation of each element is essentially suitable for high-voltage operation circuits. It is desired to obtain a diode element. In this case, an n+pp+ type diode is formed corresponding to the conductivity type of the substrate used.

又、上述のように、SOS基板上に形成されたダ
イオードは、互いに、完全に素子分離されている
から、同一基板上に形成された複数個のダイオー
ドを直列接続することにより、容易に、より高耐
圧なダイオードを得ることができる。
In addition, as mentioned above, the diodes formed on the SOS substrate are completely isolated from each other, so by connecting multiple diodes formed on the same substrate in series, it is easy to A diode with high breakdown voltage can be obtained.

ところで、一般に、PN接合ダイオードにおけ
る逆方向耐圧は、電圧印加時に拡がる空乏層巾
に、言いかえれば、pおよびn領域の不純物濃度
分布に依存するから、逆方向耐圧を向上させるた
めには、空乏層を容易に拡げ得る低不純物濃度半
導体膜を用いる必要があつた。すなわち、第1図
において、誘電体絶縁基板11上のn型半導体薄
膜12に、p+領域13、およびn+領域14を
形成して電極とし、高電圧ダイオードを構成する
場合、n型半導体膜12の不純物濃度Nsubは、
所望の耐圧に応じて低く選ぶ必要があつた。たと
えば理想的なシリコン平面PN接合を考えた場合
でも、750V以上の逆方向耐圧を得るためには、
シリコンの絶縁破壊耐圧を3×105×V/cmと仮
定して、長さ25μmの以上の低不純物濃度シリコ
ンエピタキシヤル膜領域12が必要であり、その
領域の不純物濃度は7×1014cm-3程度以下である
必要があつた。現実の素子では、局所的電界集中
を考慮し、さらに、余裕を持つた値を選ぶ必要が
あつた。又、特にSOS基板においては、結晶性が
不充分なため、少数キヤリヤの寿命が一般に0.1
〜1nsec程度とバルクシリコンのそれに比して、
非常に小さいことが知られている。従つて、SOS
基板上のダイオードが順方向にバイアスされた場
合、両高不純物濃度電極領域13および14から
の電子および正孔の注入による伝導度変調は期待
できず、この場合、低不純物濃度シリコンエピタ
キシヤル膜領域12は順方向電流の大きいところ
で直列抵抗として、作用することになる。
By the way, in general, the reverse breakdown voltage of a PN junction diode depends on the depletion layer width that expands when voltage is applied, in other words, it depends on the impurity concentration distribution in the p and n regions. It was necessary to use a low impurity concentration semiconductor film that can be easily expanded. That is, in FIG. 1, when a p+ region 13 and an n+ region 14 are formed on an n-type semiconductor thin film 12 on a dielectric insulating substrate 11 to form a high voltage diode, the n-type semiconductor film 12 is The impurity concentration Nsub is
It was necessary to select a lower value depending on the desired withstand voltage. For example, even when considering an ideal silicon planar PN junction, in order to obtain a reverse breakdown voltage of 750V or more,
Assuming that the dielectric breakdown voltage of silicon is 3×10 5 ×V/cm, a low impurity concentration silicon epitaxial film region 12 with a length of 25 μm or more is required, and the impurity concentration in that region is 7×10 14 cm. It needed to be around -3 or less. In actual devices, it is necessary to take local electric field concentration into consideration and to select a value with a margin. In addition, especially in SOS substrates, the lifetime of the minority carrier is generally 0.1 due to insufficient crystallinity.
~1nsec compared to that of bulk silicon,
It is known to be very small. Therefore, SOS
When the diode on the substrate is forward biased, conductivity modulation due to the injection of electrons and holes from both high impurity concentration electrode regions 13 and 14 cannot be expected, and in this case, the low impurity concentration silicon epitaxial film region 12 acts as a series resistance where the forward current is large.

すなわち、ダイオードの逆方向耐圧を上げるべ
く、高不純物濃度電極領域13および14の間隔
を広くとり、シリコンエピタキシヤル膜領域12
の不純物濃度を、より低く設計すれば、ダイオー
ドの順方向特性を、著しく劣化させる結果になつ
た。
That is, in order to increase the reverse breakdown voltage of the diode, the spacing between the high impurity concentration electrode regions 13 and 14 is widened, and the silicon epitaxial film region 12
If the impurity concentration of the diode was designed to be lower, the forward characteristics of the diode would be significantly degraded.

たとえば、前述の例で、長さ25μm、厚さ2μ
mで7×1014cm-3のn型シリコンエピタキシヤル
膜領域12を考えると、同領域は、100μ巾当
り、約25KΩの直列抵抗を構成することになる。
For example, in the example above, the length is 25μm and the thickness is 2μm.
Considering an n-type silicon epitaxial film region 12 of 7×10 14 cm −3 in m, this region constitutes a series resistance of about 25 KΩ per 100 μm width.

本発明の目的は、前記従来の欠点である逆方向
耐圧の半導体薄膜領域12の不純物濃度に対する
依存性を緩和せしめ、設計自由度が大きな、又、
順方向バイアス時に直列抵抗の小さな半導体ダイ
オード素子を提供するところにある。
An object of the present invention is to alleviate the dependence of the reverse breakdown voltage on the impurity concentration of the semiconductor thin film region 12, which is the drawback of the conventional art, and to provide a large degree of freedom in design.
The object of the present invention is to provide a semiconductor diode element with low series resistance when forward biased.

本発明によれば、誘電体絶縁基板上に設けられ
た半導体層に、それぞれ、該半導体層と同じ第1
の導電性を有する高不純物濃度領域と、該半導体
層と異なる第2の導電性を有する高不純物濃度領
域とからなる二つの独立した電極領域および該半
導体層を破り絶縁性保護膜を備え、該第1および
第2の導電性を有する高不純物濃度電極領域の間
の、該絶縁性保護膜下の前記半導体層表面部に、
第2の導電性を有する高不純物濃度電極領域端部
に接して、該半導体層の導電性と異なる第2の導
電性を有する低不純物濃度領域が構成されてな
り、かつ該第2の導電性を有する低濃度領域の不
純物濃度及び深さ方向の分布が、逆方向電圧増加
時に、第2の導電性を有する低温度領域と、同領
域下部の第1の導電性を有する半導体層領域の間
に生ずる空乏層により、前記二つの高不純物濃度
電極領域方向に対して垂直方向の領域全域が空乏
層化せしめられ、第2の導電性を有する高不純物
濃度電極領域から、第1の導電性を有する高不純
物濃度電極に向つて伸びる空乏層領域が、同方向
に最大となるように選択されていることを特徴と
する半導体ダイオード素子が得られる。
According to the present invention, each of the semiconductor layers provided on the dielectric insulating substrate has the same first layer as the semiconductor layer.
and a high impurity concentration region having a second conductivity different from that of the semiconductor layer, and an insulating protective film that breaks through the semiconductor layer. In the surface portion of the semiconductor layer under the insulating protective film between the first and second conductive high impurity concentration electrode regions,
A low impurity concentration region having a second conductivity different from the conductivity of the semiconductor layer is configured in contact with an end of a high impurity concentration electrode region having a second conductivity, and the second conductivity When the reverse voltage increases, the impurity concentration and the distribution in the depth direction of the low concentration region with Due to the depletion layer generated, the entire region in the direction perpendicular to the direction of the two high impurity concentration electrode regions becomes a depletion layer, and the first conductivity is transferred from the high impurity concentration electrode region having the second conductivity. A semiconductor diode element is obtained, in which the depletion layer region extending toward the high impurity concentration electrode is selected to be maximum in the same direction.

以下、本発明について、誘電体絶縁基板上の半
導体薄膜材料としてSOS基板を用いて半導体ダイ
オード素子の実施例を、図面を用いて詳細に説明
する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS In the following, embodiments of a semiconductor diode element using an SOS substrate as a semiconductor thin film material on a dielectric insulating substrate will be described in detail with reference to the drawings.

実施例 1 第2図aは、本発明の一実施例を説明するため
の図である。まず、半導体薄膜として、膜厚1〜
1.5μm、不純物濃度がそれぞれ約2×1015cm-3
よび約7×1015cm-3のn型シリコンエピタキシヤ
ル膜22をサフアイヤ基板21上に形成し、該n
型シリコンエピタキシヤル膜22に、高不純物濃
度p+電極領域23、高不純物濃度n+電極領域
24、絶縁性保護膜としてのシリコン熱酸化膜2
5および金属Al配線26を設けた。これらの工
程は、SOSMOSトランジスタを製造する標準的
工程と同様である。p+電極23から伸びるp型
低不純物濃度領域27は、ホトレジストをイオン
注入のマスクとし、約1300Å厚のシリコン熱酸化
膜25を介して、同部に、加速電圧40KeVでボロ
ンをイオン注入することにより形成した。その
後、打ち込みイオンの活性化および、イオン注入
のアニールを兼ねて、窒素雰囲気中500℃で約30
分の熱処理を行なつた。第4図はイオン注入によ
るp型低不純物濃度領域27の長さを30μm、高
濃度電極領域間の間融を40μmとした場合のシリ
コンエピタキシヤル膜、不純物濃度約2×1015cm
-3のダイオードにおける逆方向耐圧とイオン注入
量の関係を示す一例である。イオン注入を施さな
いダイオードの逆方向耐圧は、約150Vである
が、約3×1012cm-2のボロンイオン注入を施した
ダイオードは、最高800Vの逆方向耐圧を示し、
それ以上のイオン注入量に対しては、再び逆方向
耐圧の低下をきたした。
Embodiment 1 FIG. 2a is a diagram for explaining an embodiment of the present invention. First, as a semiconductor thin film, the film thickness is 1~
An n-type silicon epitaxial film 22 with a thickness of 1.5 μm and impurity concentrations of approximately 2×10 15 cm -3 and approximately 7×10 15 cm -3 is formed on the sapphire substrate 21, and the n-type silicon epitaxial film 22 is formed on the sapphire substrate 21.
type silicon epitaxial film 22, a high impurity concentration p+ electrode region 23, a high impurity concentration n+ electrode region 24, and a silicon thermal oxide film 2 as an insulating protective film.
5 and metal Al wiring 26 were provided. These steps are similar to standard steps for manufacturing SOSMOS transistors. The p-type low impurity concentration region 27 extending from the p+ electrode 23 is formed by using a photoresist as a mask for ion implantation and implanting boron ions into the same area at an acceleration voltage of 40 KeV through the silicon thermal oxide film 25 with a thickness of about 1300 Å. Formed. Afterwards, the implanted ions are activated and the ion implantation is annealed at 500°C for approximately 30 minutes in a nitrogen atmosphere.
Heat treatment was carried out for 30 minutes. Figure 4 shows a silicon epitaxial film with an impurity concentration of approximately 2×10 15 cm when the length of the p-type low impurity concentration region 27 by ion implantation is 30 μm and the interfusion between the high concentration electrode regions is 40 μm.
This is an example showing the relationship between reverse breakdown voltage and ion implantation amount in a -3 diode. The reverse breakdown voltage of a diode without ion implantation is approximately 150V, but a diode with boron ion implantation of approximately 3×10 12 cm -2 exhibits a maximum reverse breakdown voltage of 800V.
For a higher ion implantation amount, the reverse breakdown voltage decreased again.

同じ構造の不純物濃度約7×1015cm-3のシリコ
ンエピタキシヤル膜上に形成したダイオードでは
約6×1012cm-2のボロンイオン注入により、やは
り、最高750〜800Vの逆方向耐圧が得られ、その
前後のイオン注入量では、逆方向耐圧が低下し
た。又、各ダイオードの逆方向耐圧はp型低不純
物濃度領域27の長さに比例して変わり、同長さが
長いほど逆方向耐圧は、増加した。一方、ある一
定長さのp型低不純物濃度領域27に対しては、シ
リコンエピタキシヤル膜不純物濃度が約2×1015
cm-3のダイオードにおいてイオン注入量が約3×
1012cm-2のところで、シリコンエピタキシヤル膜
不純濃度が7×1015cm-3であるダイオードにおい
てはイオン注入量が約6×1012cm-2のところで、
それぞれ最高の逆方向耐圧が得られた。
A diode with the same structure formed on a silicon epitaxial film with an impurity concentration of about 7 x 10 15 cm -3 can also achieve a maximum reverse breakdown voltage of 750 to 800 V by implanting boron ions at about 6 x 10 12 cm -2 . The reverse breakdown voltage decreased at ion implantation doses before and after that. Further, the reverse breakdown voltage of each diode varied in proportion to the length of the p-type low impurity concentration region 27, and the longer the same length, the greater the reverse breakdown voltage. On the other hand, for a certain length of p-type low impurity concentration region 27, the silicon epitaxial film impurity concentration is approximately 2×10 15
In a cm -3 diode, the ion implantation amount is approximately 3×
10 12 cm -2 , and in a diode with a silicon epitaxial film impurity concentration of 7 x 10 15 cm -3 , when the ion implantation amount is about 6 x 10 12 cm -2 ,
The highest reverse breakdown voltage was obtained for each.

実施例 2 第2図bにおいて半導体薄膜として膜厚4〜
1.5μm、不純物濃度が約2×1016cm-3のp型シリ
コンエピタキシヤル膜22′をサフアイヤ基板2
1′上に形成し、該p型シリコンエピタキシヤル
膜22′に、実施例1と同様の方法により、高不
純物濃度n+電極領域23′、高濃度p+電極領
域24′、絶縁性保護膜としてのシリコン熱酸化
膜25′およびAl配線26′を設けた。n+電極
23′から伸びるn型低不純物濃度領域27′は、
実施例1におけると同様に、ホトレジストをマス
クとして、100KeVの加速電圧で、同部にリンを
イオン注入することにより形成し、その後窒素中
500℃で30分の熱処理を行なつた。
Example 2 In FIG. 2b, the thickness of the semiconductor thin film is 4 to 4.
A p-type silicon epitaxial film 22' with a thickness of 1.5 μm and an impurity concentration of approximately 2×10 16 cm -3 is placed on a sapphire substrate 2.
A high impurity concentration n+ electrode region 23', a high concentration p+ electrode region 24', and an insulating protective film are formed on the p-type silicon epitaxial film 22' by the same method as in Example 1. A silicon thermal oxide film 25' and an Al wiring 26' were provided. The n-type low impurity concentration region 27' extending from the n+ electrode 23' is
As in Example 1, phosphorus was ion-implanted into the same area at an acceleration voltage of 100 KeV using a photoresist as a mask, and then ion-implanted in nitrogen.
Heat treatment was performed at 500°C for 30 minutes.

本実施例における長さ30μn型低不純物濃度領
域27′を有するn+pp+型ダイオードにおいて
も、約8×1012cm-2のリンイオン注入により、
700V以上の逆方向耐圧を有するものが得られ
た。
Also in the n+pp+ type diode having a length of 30 μn type low impurity concentration region 27' in this example, by implanting approximately 8×10 12 cm -2 of phosphorus ions,
A device with a reverse breakdown voltage of 700V or more was obtained.

本実施例のn+pp+型ダイオードにおける逆
方向耐圧も、やはり、実施例1のp+nn+型ダ
イオードにおけると同様、最適イオン注入量を有
し、n型低不純物濃度領域27′の長さに対し
て、比例した依存性を示した。
Similarly to the p+nn+ type diode of Example 1, the reverse breakdown voltage of the n+pp+ type diode of this embodiment also has an optimum ion implantation amount and is proportional to the length of the n-type low impurity concentration region 27'. showed a dependence.

実施例 3 第3図は、低不純物濃度領域37が、高濃度p
+および高濃度n+電極領域33,34間にまた
がつて形成された構造を有する半導体ダイオード
の実施例を示すものである。
Example 3 FIG. 3 shows that a low impurity concentration region 37 is a high concentration p
3 shows an example of a semiconductor diode having a structure formed astride between + and high concentration n+ electrode regions 33 and 34.

本実施例においては、半導体薄膜として、膜厚
1〜1.5μm、不純物濃度が約2×1015cm-3のn型
エピタキシヤル膜32をサフアイヤ基板31上に
形成し、まず該n型シリコンエピタキシヤル膜3
2に高濃度p+電極領域33、高濃度n+電極領
域34および絶縁性保護膜としてのシリコン熱酸
化膜35を形成した。
In this example, an n-type epitaxial film 32 having a thickness of 1 to 1.5 μm and an impurity concentration of about 2×10 15 cm -3 is formed on a saphire substrate 31 as a semiconductor thin film, and first the n-type silicon epitaxial film 32 is formed on a sapphire substrate 31. Yaru membrane 3
2, a high concentration p+ electrode region 33, a high concentration n+ electrode region 34, and a silicon thermal oxide film 35 as an insulating protective film were formed.

次に、厚さ約1300Åの該シリコン熱酸化膜35
を介して、シリコンエピタキシヤル膜全域に、加
速電圧40KeVで約1×1012cm-2のドーズ量のボロ
ンのイオン注入を行ない、窒素雰囲気中950℃で
約30分の熱処理を行なつて、p型低不純物濃度領
域27を形成し、最後に、Al配線36を施し
た。
Next, the silicon thermal oxide film 35 with a thickness of about 1300 Å
Boron ions were implanted into the entire silicon epitaxial film at a dose of approximately 1×10 12 cm -2 at an acceleration voltage of 40 KeV, and heat treatment was performed at 950° C. for approximately 30 minutes in a nitrogen atmosphere. A p-type low impurity concentration region 27 was formed, and finally, an Al wiring 36 was formed.

高不純物濃度p+およびn+電極33,34の
間隔が30μmである本実施例の半導体ダイオード
においては、約600Vの逆方向耐圧を得た。
In the semiconductor diode of this example in which the spacing between the high impurity concentration p+ and n+ electrodes 33 and 34 was 30 μm, a reverse breakdown voltage of about 600V was obtained.

本実施例では、イオン注入のためのマスク工程
が不要であり、実施例1および実施例2の素子に
比して製造工程が簡単であるが、第2の導電性を
有する低不純物濃度領域37が第1の導電性を有
する高濃度電極領域34に接しているため、両者
間での局所的な電界集中を防止する必要があり、
たとえば抵不純物濃度領域37の不純物濃度の最
高値を低める等、不純物濃度分布を制御する必要
がある。又、同様の理由から低不純物濃度領域3
7および同領域下部のシリコンエピタキシヤル膜
中の有効不純物イオン総量を、実施例1および2
の場合に比較して、より正確に制御する必要があ
る。
In this example, a mask process for ion implantation is not required, and the manufacturing process is simpler than the elements of Example 1 and Example 2. Since it is in contact with the high concentration electrode region 34 having the first conductivity, it is necessary to prevent local electric field concentration between the two.
For example, it is necessary to control the impurity concentration distribution, such as by lowering the maximum value of the impurity concentration in the resistive impurity concentration region 37. Also, for the same reason, the low impurity concentration region 3
7 and the total amount of effective impurity ions in the silicon epitaxial film at the bottom of the same region in Examples 1 and 2.
It is necessary to control more accurately than in the case of

以上の実施例から明らかなように、本発明にか
かる半導体ダイオード素子においては、逆方向耐
圧は、シリコンエピタキシヤル膜と異なる導電性
を有する高濃度電極領域に隣接して設けられたシ
リコンエピタキシヤル膜と異なる導電性を有する
低不純物濃度領域の効果によつて、素子の基体と
なるシリコンエピタキシヤル膜の不純物濃度に直
接制約されなくなるため、本発明によれば、高逆
方向耐圧を維持したまま、ダイオード素子の基体
となるシリコンエピタキシヤル膜の不純物濃度を
広い範囲にわたつて選択することが可能となる。
As is clear from the above embodiments, in the semiconductor diode device according to the present invention, the reverse breakdown voltage is higher than that of the silicon epitaxial film provided adjacent to the high concentration electrode region, which has a different conductivity than the silicon epitaxial film. Due to the effect of the low impurity concentration region having a conductivity different from that of the silicon epitaxial film that is the base of the device, the present invention allows for high reverse breakdown voltage while maintaining high reverse breakdown voltage. It becomes possible to select the impurity concentration of the silicon epitaxial film serving as the base of the diode element over a wide range.

本発明の基本原理は、低不純物濃度領域と、同
領域下部のシリコンエピタキシヤル膜との間に、
エピ膜厚方向に拡がる空乏層の効果を考慮するこ
とにより、実施例1の第2図aを例に以下の如
く、説明できる。すなわち、絶縁性保護膜との界
面、および誘電体絶縁基板との界面における等価
電荷密度を考慮した低不純物濃度領域27におけ
る有効不純物イオン総量と、同領域下部のシリコ
ンエピタキシヤル膜22中における反対極性の有
効不純物イオンの総量とを、互いに等しくなるよ
う選択することにより、本発明にかかる半導体ダ
イオード素子に逆方向電圧が印加され、pn接合
間に空乏層が拡がる場合、低不純物濃度領域27
の不純物イオンから発した電気力縁を、ほぼすべ
て同領域下部のシリコンエピタキシヤル膜中の反
対極性不純物イオンにより終端させることができ
る。この場合、一定電圧下で低不純物濃度領域2
7および同領域下部のシリコンエピタキシヤル膜
を含む全域が、エピ膜厚方向に拡がる空乏層によ
つて同時に空乏層化した状態が実現される。ここ
で、全シリコンエピタキシヤル膜厚は、エピ膜厚
方向に拡がる空乏層中の電界強度が、シリコンの
絶縁破壊電界強度を越えないようダイオード素子
における膜厚方向の不純物濃度およびその分布を
考慮して選択すべきことは、もちろんである。上
記効果により、一定の逆方向電圧以上の電圧が印
加された高不純物濃度電極領域23,24間に
は、低不純物濃度領域27の長さにほぼ対応した
長さの膜厚方向全域が空乏層化した空乏層領域が
介在することになり、同空乏層領域は、該逆方向
電圧以上において、いわゆるpin構造ダイオード
におけるイントリンジツク領域の如く作用するか
ら、本発明の高逆方向耐圧半導体ダイオード素子
が実現される。すなわち、本発明にかかる半導体
ダイオード素子においては、一定逆方向電圧以上
で、高濃度p+およびn+電極23,24間に、
該一定逆方向電圧以上の電圧増加分を吸収すべき
全空乏層化領域が実現されればよく、実施例で示
されたように該半導体ダイオード素子の逆方向耐
圧は直接、低不純物濃度領域27と、同領域下部
のシリコンエピタキシヤル膜の不純物濃度に依存
せず、むしろ該全空乏層化領域長を決める低不純
物濃度領域27の長さに依存することになる。た
とえば、本実施例における様に、シリコンエピタ
キシヤル膜22の膜厚および不純物濃度が与えら
れた場合、低不純物濃度領域27には、最終的に
空乏層化に寄与する同領域の有効不純物イオン総
量と同領域下部のシリコンエピタキシヤル膜22
中の有効不純物イオン総量とが互いにほぼ等しく
なるよう、然るべき極性および量の不純物イオン
を、たとえばイオン注入等の方法により導入すれ
ばよい。
The basic principle of the present invention is that between the low impurity concentration region and the silicon epitaxial film below the region,
By considering the effect of the depletion layer expanding in the epitaxial film thickness direction, the following explanation can be given using FIG. 2a of Example 1 as an example. That is, the effective total amount of impurity ions in the low impurity concentration region 27 considering the equivalent charge density at the interface with the insulating protective film and the interface with the dielectric insulating substrate, and the opposite polarity in the silicon epitaxial film 22 below the region. By selecting the total amount of effective impurity ions to be equal to each other, when a reverse voltage is applied to the semiconductor diode element according to the present invention and a depletion layer expands between the pn junctions, the low impurity concentration region 27
Almost all of the electric force edges emitted from impurity ions can be terminated by impurity ions of opposite polarity in the silicon epitaxial film below the same region. In this case, under a constant voltage, the low impurity concentration region 2
7 and the entire area including the silicon epitaxial film at the bottom of the same region simultaneously becomes a depletion layer due to the depletion layer expanding in the epitaxial film thickness direction. Here, the total silicon epitaxial film thickness is determined by considering the impurity concentration and its distribution in the film thickness direction in the diode element so that the electric field strength in the depletion layer that spreads in the epitaxial film thickness direction does not exceed the dielectric breakdown field strength of silicon. Of course, you should choose accordingly. Due to the above effect, between the high impurity concentration electrode regions 23 and 24 to which a voltage higher than a certain reverse voltage is applied, the entire region in the film thickness direction with a length approximately corresponding to the length of the low impurity concentration region 27 becomes a depletion layer. Therefore, the depletion layer region acts like an intrinsic region in a so-called pin structure diode at a voltage higher than the reverse voltage, so that the high reverse voltage semiconductor diode element of the present invention is realized. That is, in the semiconductor diode element according to the present invention, at a constant reverse voltage or higher, between the high concentration p+ and n+ electrodes 23 and 24,
It is only necessary to realize a fully depleted region that should absorb the voltage increase above the certain reverse voltage, and as shown in the embodiment, the reverse breakdown voltage of the semiconductor diode element is directly determined by the low impurity concentration region 27. Therefore, it does not depend on the impurity concentration of the silicon epitaxial film below the region, but rather depends on the length of the low impurity concentration region 27 which determines the length of the total depletion layer region. For example, when the film thickness and impurity concentration of the silicon epitaxial film 22 are given as in this embodiment, the low impurity concentration region 27 has a total effective impurity ion amount in the same region that ultimately contributes to the depletion layer. and the silicon epitaxial film 22 at the bottom of the same area.
Impurity ions of appropriate polarity and amount may be introduced by a method such as ion implantation so that the total amount of effective impurity ions therein is approximately equal to each other.

以下、説明したように、本発明によれば、誘電
体絶縁基板上の半導体薄膜にダイオード素子を形
成する場合、該半導体薄膜の膜厚および不純物濃
度(すなわち、膜中の不純物イオン総量)は、前
記膜厚方向の全空乏層化が実現できる範囲で、広
く選択できるから、たとえば、然るべき濃度の
SOS基板上に、p型もしくはn型の電界効果トラ
ンジスタを形成すると同時に、該SOS基板上に、
高耐圧半導体ダイオード素子を形成できる。たと
えば通常、エンハンスメントモードのpMOSトラ
ンジスタでは、1〜5×1015cm-3、同、nMOSト
ランジスタでは、1〜4×1016cm-3程度の基板濃
度がしばしば使用されるが、同一基板上に、本発
明にかかる半導体ダイオード素子を形成する場
合、該ダイオード素子の低不純物濃度領域37,
27′,または37に、然るべき最適不純物イオ
ン量を導入してやれば、該低不純物濃度領域2
7,27′または37の長さに対応した逆方向耐
圧を有する該半導体ダイオード素子が形成でき
る。又、実施例1における約7×1015cm-3の不純
物濃度を有するn型SOS膜の比抵抗は、前述の例
の7×1014cm-3の不純物濃度のn型SOS膜の比抵
抗の約十分の一である。これらの例からも明らか
なように、同程度の逆方向耐圧を有する本発明の
半導体ダイオード素子では、通常のSOS基板上の
pn接合ダイオード素子に比して、順方向の直列
抵抗を大巾に下げることができ、ダイオード順方
向特性の向上を図ることができる。
As described below, according to the present invention, when a diode element is formed in a semiconductor thin film on a dielectric insulating substrate, the film thickness and impurity concentration of the semiconductor thin film (i.e., the total amount of impurity ions in the film) are as follows: As long as the full depletion layer in the film thickness direction can be achieved, a wide range of choices can be made, so for example,
At the same time, a p-type or n-type field effect transistor is formed on the SOS substrate, and at the same time, on the SOS substrate,
A high voltage semiconductor diode element can be formed. For example, enhancement mode pMOS transistors often use a substrate concentration of 1 to 5 x 10 15 cm -3 , while nMOS transistors often use substrate concentrations of about 1 to 4 x 10 16 cm -3 . , when forming a semiconductor diode element according to the present invention, the low impurity concentration region 37 of the diode element,
If an appropriate optimum amount of impurity ions is introduced into 27' or 37, the low impurity concentration region 2
The semiconductor diode element having a reverse breakdown voltage corresponding to the length of 7, 27' or 37 can be formed. Furthermore, the specific resistance of the n-type SOS film having an impurity concentration of about 7×10 15 cm -3 in Example 1 is the same as the specific resistance of the n-type SOS film having an impurity concentration of about 7×10 14 cm -3 in the example described above. This is about one-tenth of the total. As is clear from these examples, in the semiconductor diode element of the present invention having the same reverse breakdown voltage,
Compared to a pn junction diode element, the forward series resistance can be significantly lowered, and the forward direction characteristics of the diode can be improved.

ところで、本実施例では、誘電体絶縁基板上の
半導体薄膜としてSOS基板を用いたが、本発明に
おける基板材料は、もちろんSOS基板である必要
は無く、たとえば、ポリシリコン厚膜上に、シリ
コン酸化膜を介して形成されたシリコン単結晶薄
膜のような誘電体絶縁分離基板であつてよい。さ
らに、半導体薄膜としては、シリコン以外のもの
であつてもかまわない。
By the way, in this example, an SOS substrate was used as a semiconductor thin film on a dielectric insulating substrate, but the substrate material in the present invention does not necessarily have to be an SOS substrate. It may be a dielectric insulating isolation substrate such as a silicon single crystal thin film formed through a film. Furthermore, the semiconductor thin film may be made of something other than silicon.

また、本発明においては、逆方向バイアス時
に、薄いダイオードのPN接合部が、ある長さに
わたつて全域膜厚方向に空乏層化されれば良く、
本発明の構造を実現するためには、本実施例に示
した製造工程を経ることなく、たとえば最初に低
不純物濃度領域27を形成した後、絶縁性保護膜
26を設ける等、種々、製造工程の変形が可能で
あることは言うまでもない。また、本実施例の図
において、各高不純物濃度電極領域が、誘電体絶
縁基板に達している場合を示したが、本発明の実
施に際し、必ずしも、該電極領域が誘電体絶縁基
板に達している必要が無いことは、前述の動作説
明から明らかである。
Further, in the present invention, it is sufficient that the PN junction of the thin diode is depleted in the film thickness direction over a certain length during reverse bias.
In order to realize the structure of the present invention, various manufacturing steps such as first forming the low impurity concentration region 27 and then providing the insulating protective film 26 are required, without going through the manufacturing steps shown in this embodiment. It goes without saying that the following modifications are possible. Furthermore, although the diagrams of this embodiment show the case where each high impurity concentration electrode region reaches the dielectric insulating substrate, when implementing the present invention, the electrode regions do not necessarily reach the dielectric insulating substrate. It is clear from the above description of the operation that there is no need to do so.

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

第1図は従来例を示す断面概略図、第2図a,
b、第3図は本発明の実施例を示す断面概略図、
第4図はダイオードにおける逆方向耐圧とイオン
注入量の関係を説明するための図である。 各図において、11は誘電体絶縁基板、12は
n型半導体膜、13はp+半導体領域、14はn
+半導体領域、15は酸化膜、21,21′,3
1はサフアイヤ基板、22,22′32はエピタ
キシヤル膜、23,23′33は高不純物濃度電
極領域、24,24′,34は反対極性の高不純
物濃度電極領域、25,25′,35はシリコン
熱酸化膜、26,26′,36はAl配線、27,
27′37は低不純物濃度領域をそれぞれ示す。
Fig. 1 is a schematic cross-sectional view showing a conventional example, Fig. 2 a,
b, FIG. 3 is a cross-sectional schematic diagram showing an embodiment of the present invention;
FIG. 4 is a diagram for explaining the relationship between the reverse breakdown voltage and the amount of ion implantation in a diode. In each figure, 11 is a dielectric insulating substrate, 12 is an n-type semiconductor film, 13 is a p+ semiconductor region, and 14 is an n-type semiconductor film.
+ semiconductor region, 15 is oxide film, 21, 21', 3
1 is a sapphire substrate, 22, 22', 32 are epitaxial films, 23, 23', 33 are high impurity concentration electrode regions, 24, 24', 34 are high impurity concentration electrode regions of opposite polarity, 25, 25', 35 are high impurity concentration electrode regions. Silicon thermal oxide film, 26, 26', 36 are Al wiring, 27,
27' and 37 indicate low impurity concentration regions, respectively.

Claims (1)

【特許請求の範囲】 1 誘電体絶縁基板上に設けられた半導体層に、
それぞれ該半導体層と同じ第1の導電性を有する
高不純物濃度領域と、該半導体層と異なる第2の
導電性を有する高不純物濃度領域とからなる二つ
の独立した電極領域および該半導体層を被う絶縁
性保護膜を備え、該第1および第2の導電性を有
する高不純物濃度電極領域の間の、該絶縁性保護
膜下の前記半導体層表面部に、第2の導電性を有
する高不純物濃度電極領域端部に接して、該半導
体層の導電性と異なる第2の導電性を有する低不
純物濃度領域が構成されてなり、かつ該第2の導
電性を有する低濃度領域の不純物濃度及び深さ方
向の分布が、逆方向電圧増加時に、第2の導電性
を有する低濃度領域と、同領域下部の第1の導電
性を有する半導体層領域の間に生ずる空乏層によ
り前記二つの高濃度電極領域方向に対して垂直方
向の領域全域が空乏層化せしめられ、第2の導電
性を有する高濃度電極領域から、第1の導電性を
有する高濃度電極に向つて伸びる空乏層領域が、
同方向に最大となるように選択されていることを
特徴とする半導体ダイオード素子。 2 誘電体絶縁基板上に設けられた半導体層が、
n型半導体である特許請求の範囲第1項記載の半
導体ダイオード素子。 3 誘電体絶縁基板上に設けられた半導体層が、
p型半導体である特許請求の範囲第1項記載の半
導体ダイオード素子。 4 第2の導電性を有する低不純物濃度領域が、
第2および第1の導電性を有する二つの高不純物
濃度電極間にまたがつて、構成されている特許請
求の範囲第1項記載の半導体ダイオード素子。 5 第2の導電性を有する低不純物濃度領域が、
第1の導電性を有する高濃度電極領域に達してい
ない特許請求の範囲第1項記載の半導体ダイオー
ド素子。
[Claims] 1. A semiconductor layer provided on a dielectric insulating substrate,
Two independent electrode regions each consisting of a high impurity concentration region having the same first conductivity as the semiconductor layer and a high impurity concentration region having a second conductivity different from the semiconductor layer and covering the semiconductor layer. a second highly conductive high impurity concentration electrode region between the first and second conductive high impurity concentration electrode regions under the insulating protective film; A low impurity concentration region having a second conductivity different from the conductivity of the semiconductor layer is configured in contact with an end of the impurity concentration electrode region, and the impurity concentration of the low concentration region having the second conductivity is When the reverse voltage increases, the depletion layer formed between the low concentration region with the second conductivity and the semiconductor layer region with the first conductivity below the same region causes the two The entire region in the direction perpendicular to the high concentration electrode region is made into a depletion layer, and the depletion layer region extends from the high concentration electrode region having the second conductivity toward the high concentration electrode having the first conductivity. but,
A semiconductor diode element, characterized in that the semiconductor diode element is selected such that it is maximized in the same direction. 2 The semiconductor layer provided on the dielectric insulating substrate is
The semiconductor diode element according to claim 1, which is an n-type semiconductor. 3 The semiconductor layer provided on the dielectric insulating substrate is
The semiconductor diode element according to claim 1, which is a p-type semiconductor. 4 The low impurity concentration region having second conductivity is
2. The semiconductor diode element according to claim 1, which is constructed astride between two high impurity concentration electrodes having second and first conductivities. 5 The low impurity concentration region having second conductivity is
The semiconductor diode element according to claim 1, which does not reach the high concentration electrode region having the first conductivity.
JP8131477A 1977-07-06 1977-07-06 Semiconductor diode element Granted JPS5416184A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8131477A JPS5416184A (en) 1977-07-06 1977-07-06 Semiconductor diode element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8131477A JPS5416184A (en) 1977-07-06 1977-07-06 Semiconductor diode element

Publications (2)

Publication Number Publication Date
JPS5416184A JPS5416184A (en) 1979-02-06
JPS6130436B2 true JPS6130436B2 (en) 1986-07-14

Family

ID=13742923

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8131477A Granted JPS5416184A (en) 1977-07-06 1977-07-06 Semiconductor diode element

Country Status (1)

Country Link
JP (1) JPS5416184A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56105921U (en) * 1980-01-16 1981-08-18
GB2089119A (en) * 1980-12-10 1982-06-16 Philips Electronic Associated High voltage semiconductor devices
DE4201276C1 (en) * 1992-01-18 1993-06-17 Daimler-Benz Aktiengesellschaft, 7000 Stuttgart, De

Also Published As

Publication number Publication date
JPS5416184A (en) 1979-02-06

Similar Documents

Publication Publication Date Title
US5900652A (en) Apparatus for the localized reduction of the lifetime of charge carriers, particularly in integrated electronic devices
US4620211A (en) Method of reducing the current gain of an inherent bipolar transistor in an insulated-gate semiconductor device and resulting devices
JP3471823B2 (en) Insulated gate semiconductor device and method of manufacturing the same
EP0442144A2 (en) Manufacturing high speed low leakage radiation hardened CMOS/SOI devices
US5444271A (en) Conductivity-modulated semiconductor device with high breakdown voltage
KR20020084685A (en) Method for fabricating forward and reverse blocking devices
US10062681B2 (en) SOI integrated circuit equipped with a device for protecting against electrostatic discharges
JP3958388B2 (en) Semiconductor device
US6649981B2 (en) High breakdown voltage semiconductor device
US4807012A (en) IC which eliminates support bias influence on dielectrically isolated components
JP3472476B2 (en) Semiconductor device and driving method thereof
CA1126875A (en) Dielectrically-isolated integrated circuit complementary transistors for high voltage use
KR100956241B1 (en) Bipolar Methods and Structures with Depletable Collector Columns
JP2022117495A (en) Silicon carbide vertical conduction mosfet device and manufacturing process thereof
JPH0786580A (en) High voltage semiconductor device
US6759303B1 (en) Complementary vertical bipolar junction transistors fabricated of silicon-on-sapphire utilizing wide base PNP transistors
JPH0648691B2 (en) Semiconductor device and manufacturing method thereof
CN100474614C (en) Semiconductor device and manufacturing method thereof
KR20140080741A (en) Asymmetric two-terminal biristor and fabrication method
JPS6130436B2 (en)
US5976942A (en) Method of manufacturing a high-voltage semiconductor device
KR20180065769A (en) SiC MOSPET power semiconductor device and method of fabricating the same
JP2024109061A (en) Silicon carbide power MOSFET device with improved performance and manufacturing process thereof
US6787816B1 (en) Thyristor having one or more doped layers
JP4181322B2 (en) Power semiconductor module structured vertically