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JPH0738453B2 - Stacked semiconductor device - Google Patents
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JPH0738453B2 - Stacked semiconductor device - Google Patents

Stacked semiconductor device

Info

Publication number
JPH0738453B2
JPH0738453B2 JP59237073A JP23707384A JPH0738453B2 JP H0738453 B2 JPH0738453 B2 JP H0738453B2 JP 59237073 A JP59237073 A JP 59237073A JP 23707384 A JP23707384 A JP 23707384A JP H0738453 B2 JPH0738453 B2 JP H0738453B2
Authority
JP
Japan
Prior art keywords
layer
type
semiconductor device
laminated
thickness
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 - Lifetime
Application number
JP59237073A
Other languages
Japanese (ja)
Other versions
JPS61115319A (en
Inventor
圭弘 浜川
博明 岡本
順彦 藤田
Original Assignee
社団法人生産技術振興協会
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 社団法人生産技術振興協会 filed Critical 社団法人生産技術振興協会
Priority to JP59237073A priority Critical patent/JPH0738453B2/en
Publication of JPS61115319A publication Critical patent/JPS61115319A/en
Publication of JPH0738453B2 publication Critical patent/JPH0738453B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F10/00Individual photovoltaic cells, e.g. solar cells
    • H10F10/10Individual photovoltaic cells, e.g. solar cells having potential barriers
    • H10F10/17Photovoltaic cells having only PIN junction potential barriers
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/546Polycrystalline silicon PV cells
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/548Amorphous silicon PV cells

Landscapes

  • Recrystallisation Techniques (AREA)
  • Photovoltaic Devices (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は非晶質半導体と微結晶質半導体の積層体から
なる積層半導体素子に関するものである。
TECHNICAL FIELD The present invention relates to a laminated semiconductor device including a laminated body of an amorphous semiconductor and a microcrystalline semiconductor.

〔従来の技術とその問題点〕[Conventional technology and its problems]

半導体素子の材料として、非晶質シリコン(以下、a−
Siと称する)は、次のような長所と欠点を有する材料と
して知られている。
Amorphous silicon (hereinafter a-
Si) is known as a material having the following advantages and disadvantages.

(長所) (1)低温(250℃以下)で形成できる (2)低コスト基板(合成樹脂、ガラス、金属、セラミ
ックス)が使用できる。
(Advantages) (1) Can be formed at low temperature (250 ° C or lower) (2) Low cost substrate (synthetic resin, glass, metal, ceramics) can be used.

(3)大面積化が容易である。(3) It is easy to increase the area.

(4)光の吸収係数が大であるため、薄膜で光電変換素
子などが構成できる。
(4) Since the absorption coefficient of light is large, a photoelectric conversion element or the like can be formed with a thin film.

(5)光電導度が大である。(5) The photoconductivity is high.

(欠点) (1)キャリアの移動度が小さい。(Disadvantage) (1) The mobility of carriers is small.

(2)光電変換効率が低い。(2) The photoelectric conversion efficiency is low.

一方、微結晶シリコン(以下、μc−Siと称する)は、
次のような長所と欠点を有する材料として知られてい
る。
On the other hand, microcrystalline silicon (hereinafter referred to as μc-Si) is
It is known as a material having the following advantages and disadvantages.

(長所) (1)a−Siに比べて、キャリア移動度、不純物ドーピ
ング効率が良い。
(Advantages) (1) Carrier mobility and impurity doping efficiency are better than those of a-Si.

(2)n型層は、電気伝導度が良く、電導度の活性化エ
ネルギが小さいので、pin構造やショットキー構造の半
導体装置に利用されている。
(2) The n-type layer has a good electric conductivity and a small activation energy of the electric conductivity, and therefore is used for a semiconductor device having a pin structure or a Schottky structure.

(欠点) (1)光電導度、キャリアの寿命が小さく、かつ欠陥密
度が大であるため、真正層あるいはノンドープ層として
は利用されていない。
(Defects) (1) It is not used as a genuine layer or a non-doped layer because it has a small photoconductivity, a short carrier life, and a large defect density.

なお、結晶シリコン(以下、c−Siと称する)は、次の
ような長所と欠点を有する。
Crystalline silicon (hereinafter referred to as c-Si) has the following advantages and disadvantages.

(長所) (1)欠陥が少なく、キャリアの移動度が大である。(Advantages) (1) Fewer defects and higher carrier mobility.

(2)光電変換素子に応用した場合、大きい光電変換効
率を得ることができる。
(2) When applied to a photoelectric conversion element, a large photoelectric conversion efficiency can be obtained.

(欠点) (1)溶融する必要があるため、製造工程に高温工程が
含まれ、また大面積化が困難である。
(Disadvantages) (1) Since it needs to be melted, the manufacturing process includes a high temperature process, and it is difficult to increase the area.

(2) 光の吸収係数が小さい。(2) The absorption coefficient of light is small.

この発明は、a−Si、μc−Si、c−Siの上記のごとき
諸特性にかんがみ、a−Siおよびμc−Siを用いて好ま
しい特性、特にμτ積(キャリアの移動度μと寿命τの
積)の大きい半導体素子を提供することを目的とするも
のである。
In view of the various characteristics of a-Si, μc-Si, and c-Si, the present invention uses a-Si and μc-Si to obtain preferable characteristics, particularly the μτ product (carrier mobility μ and lifetime τ. It is intended to provide a semiconductor device having a large product).

〔問題点を解決するための手段〕[Means for solving problems]

この発明は、上記の目的を達成するために、図1に示す
ように、基板1上に順にp型a−Siまたはp型a−SiC
(非晶質炭化シリコン)でなるp型層2、i型a−Si層
3、μc−Si層4とa−Si層5からなる単位積層体6を
繰返し数が2〜10回の範囲で積層したi型多層積層体、
i型μc−Si最終層4、i型a−Si層7、およびn型μ
c−Si層8を順次積層した構造を採用したものである。
In order to achieve the above-mentioned object, the present invention is, as shown in FIG.
The p-type layer 2 made of (amorphous silicon carbide), the i-type a-Si layer 3, the unit laminate body 6 made up of the μc-Si layer 4 and the a-Si layer 5 is repeated in the range of 2 to 10 times. A laminated i-type multilayer laminate,
i-type μc-Si final layer 4, i-type a-Si layer 7, and n-type μ
This is a structure in which the c-Si layer 8 is sequentially laminated.

また、上記単位積層体6の繰返し数をm(mは2〜10の
間の整数)、μc−Si層の厚さをμd、a−Si層の厚さ
をadとしたとき、 m(μd+ad)=2000Å − の関係にある。
When the number of repetitions of the unit laminate body 6 is m (m is an integer between 2 and 10), the thickness of the μc-Si layer is μd, and the thickness of the a-Si layer is ad, m (μd + ad ) = 2000Å-

なお、第1図において符号9で示した範囲の各層はi型
層を形成する。
In addition, each layer in the range indicated by reference numeral 9 in FIG. 1 forms an i-type layer.

上記のa−Si層およびμc−Si層は、例えば次のごとき
方法によって作られる。
The above-mentioned a-Si layer and μc-Si layer are formed by the following method, for example.

(1)プラズマCVD法 少なくともSiH4、SiH6、SiF4などのSi化合物ガスを含む
ガスをグロー放電分解させることによりa−Siが得ら
れ、このときSi化合物ガスを水素などで希釈し、或いは
グロー放電分解の際の投入パワーを大きくすることより
μc−Siが得られる。
(1) Plasma CVD method a-Si is obtained by glow discharge decomposition of a gas containing at least Si compound gas such as SiH 4 , SiH 6 , and SiF 4 , and at this time, the Si compound gas is diluted with hydrogen or the like, or By increasing the input power during glow discharge decomposition, μc-Si can be obtained.

(2)スパッタ法 Siターゲットを水素、フッ素などを含むガスでスパッタ
ーすることによりa−Siが得られ、このときスパッター
のパワーを大きくすることによりμc−Siが得られる。
(2) Sputtering method A-Si is obtained by sputtering a Si target with a gas containing hydrogen, fluorine, etc. At this time, μc-Si is obtained by increasing the sputtering power.

〔実施例〕〔Example〕

図1の構造において、i型層9の全体の厚さを6000Åと
することができる。このときμdは50Å、adは前記式
からmが2〜10の範囲で950Å(m=2)〜150Å(m=
10)となる。
In the structure of FIG. 1, the total thickness of the i-type layer 9 can be set to 6000Å. At this time, μd is 50Å and ad is 950Å (m = 2) to 150Å (m =
10).

第2図は実験結果を示すものであり、本発明の場合の繰
返し数mに対するキャリア(正孔と電子)のμτ積の総
和を黒丸で示している。また、比較のために、単層のa
−Si、μc−Siの場合を白丸で示している。
FIG. 2 shows the experimental results, and the total sum of μτ products of carriers (holes and electrons) with respect to the number of repetitions m in the present invention is shown by black circles. For comparison, a single layer a
In the case of -Si and μc-Si, white circles are shown.

このグラフからわかるように、2≦m≦10(但し、mは
整数)の範囲で単層のものより高μτ積が得られること
がわかった。
As can be seen from this graph, it was found that a higher μτ product can be obtained in the range of 2 ≦ m ≦ 10 (where m is an integer) than that of the monolayer.

なお、i型層9の両端のa−Si層3、7の厚さをそれぞ
れ100〜5000Åとすることができ、また、μdを20〜500
Åとし、前記式よりmが2〜10の範囲でadを50Å(m
=10、μd=150Å)〜980Å(m=2、μd=20Å)と
することができる。
The thickness of each of the a-Si layers 3 and 7 at both ends of the i-type layer 9 can be set to 100 to 5000Å, and μd can be set to 20 to 500.
From the above formula, ad is 50Å (m
= 10, μd = 150Å) to 980Å (m = 2, μd = 20Å).

〔発明の効果〕〔The invention's effect〕

この発明は、上記のごときのものであるから、キャリア
のμτ積を大きくすることができ、その結果、光起電力
素子や発光素子に使用した場合に、光電変換効率の高い
素子を得ることができる。また、キャリアの移動速度が
大であるため、薄膜トランジスタや光電導素子に使用し
た場合応答速度の速い素子を得ることができる。
Since the present invention is as described above, it is possible to increase the μτ product of carriers, and as a result, it is possible to obtain an element with high photoelectric conversion efficiency when used in a photovoltaic element or a light emitting element. it can. Further, since the moving speed of carriers is high, it is possible to obtain an element having a high response speed when used in a thin film transistor or a photoconductive element.

【図面の簡単な説明】[Brief description of drawings]

第1図は実施例の積層半導体素子の積層構造を拡大して
示した説明図、第2図は実験結果のグラフである。 1……基板、2……p型層、3……a−Si層、4……μ
c−Si層、5……a−Si層、6……単位積層体、7……
a−Si層、8……n型層、9……i型層
FIG. 1 is an explanatory view showing an enlarged laminated structure of a laminated semiconductor element of an example, and FIG. 2 is a graph of experimental results. 1 ... Substrate, 2 ... p-type layer, 3 ... a-Si layer, 4 ... μ
c-Si layer, 5 ... a-Si layer, 6 ... Unit laminated body, 7 ...
a-Si layer, 8 ... n type layer, 9 ... i type layer

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 電子材料 1982年9月号 第35〜40頁 電気学会雑誌 第102巻 第12号、第 1117〜1122頁(1982、12) ─────────────────────────────────────────────────── ─── Continuation of the front page (56) Bibliography Electronic materials September 1982, pages 35-40, The Institute of Electrical Engineers of Japan Volume 102, No. 12, 1117-1122 (1982, 12)

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】基板上に順にp型a−Siまたはp型a−Si
Cでなるp型層、i型a−Si層、μc−Si層とa−Si層
からなる単位積層体を繰返し数が2〜10回の範囲で積層
したi型多層積層体、i型μc−Si最終層、i型a−Si
層、およびn型μc−Si層を順次積層した構造であり、
上記単位積層体の繰返し数をm(mは2〜10の間の整
数)、μc−Si層の厚さをμd、a−Si層の厚さをadと
したとき、m(μd+ad)=2000Åの関係にある積層半
導体素子。
1. A p-type a-Si or a p-type a-Si on a substrate in order.
An i-type multilayer laminate in which a unit laminate composed of a p-type layer made of C, an i-type a-Si layer, a μc-Si layer and an a-Si layer is laminated in the range of 2 to 10 times, i-type μc -Si final layer, i-type a-Si
A layer and an n-type μc-Si layer are sequentially laminated,
When the number of repetitions of the unit laminate is m (m is an integer between 2 and 10), the thickness of the μc-Si layer is μd, and the thickness of the a-Si layer is ad, m (μd + ad) = 2000Å Laminated semiconductor device having a relationship of.
【請求項2】単位積層体を構成するμc−Si層のみμd
が20〜500Å、a−Siの厚みがadが50〜980Åである特許
請求の範囲第1項に記載の積層半導体素子。
2. Only the μc-Si layer constituting the unit laminate is μd.
Is 20 to 500Å, and the thickness of a-Si is ad is 50 to 980Å, The laminated semiconductor element according to claim 1.
【請求項3】i型多層積層体の両端に設けたi型a−Si
層の厚みが100〜5000Åである特許請求の範囲第1項又
は第2項に記載の積層半導体素子。
3. An i-type a-Si provided on both ends of an i-type multilayer laminate.
The laminated semiconductor device according to claim 1 or 2, wherein the layer has a thickness of 100 to 5000 Å.
JP59237073A 1984-11-10 1984-11-10 Stacked semiconductor device Expired - Lifetime JPH0738453B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59237073A JPH0738453B2 (en) 1984-11-10 1984-11-10 Stacked semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59237073A JPH0738453B2 (en) 1984-11-10 1984-11-10 Stacked semiconductor device

Publications (2)

Publication Number Publication Date
JPS61115319A JPS61115319A (en) 1986-06-02
JPH0738453B2 true JPH0738453B2 (en) 1995-04-26

Family

ID=17010012

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59237073A Expired - Lifetime JPH0738453B2 (en) 1984-11-10 1984-11-10 Stacked semiconductor device

Country Status (1)

Country Link
JP (1) JPH0738453B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5131249B2 (en) * 2008-06-25 2013-01-30 富士電機株式会社 Thin film solar cell
KR101106480B1 (en) * 2009-06-12 2012-01-20 한국철강 주식회사 Method of manufacturing photovoltaic device

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
電子材料1982年9月号第35〜40頁
電気学会雑誌第102巻第12号、第1117〜1122頁(1982、12)

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Publication number Publication date
JPS61115319A (en) 1986-06-02

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