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JPH0738448B2 - Method for manufacturing SOI MOSFET - Google Patents
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JPH0738448B2 - Method for manufacturing SOI MOSFET - Google Patents

Method for manufacturing SOI MOSFET

Info

Publication number
JPH0738448B2
JPH0738448B2 JP61033752A JP3375286A JPH0738448B2 JP H0738448 B2 JPH0738448 B2 JP H0738448B2 JP 61033752 A JP61033752 A JP 61033752A JP 3375286 A JP3375286 A JP 3375286A JP H0738448 B2 JPH0738448 B2 JP H0738448B2
Authority
JP
Japan
Prior art keywords
region
layer
heat conduction
silicon layer
crystal grain
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
JP61033752A
Other languages
Japanese (ja)
Other versions
JPS62193178A (en
Inventor
良一 向井
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP61033752A priority Critical patent/JPH0738448B2/en
Publication of JPS62193178A publication Critical patent/JPS62193178A/en
Publication of JPH0738448B2 publication Critical patent/JPH0738448B2/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
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/60Insulated-gate field-effect transistors [IGFET]
    • H10D30/67Thin-film transistors [TFT]

Landscapes

  • Recrystallisation Techniques (AREA)

Description

【発明の詳細な説明】 〔概 要〕 SOI型MOSFETの製造方法であって、再結晶化の過程で結
晶粒のない領域を形成すると共にこの領域に自己整合に
よりチャネル部とLDD部を形成するようにしたものであ
る。
DETAILED DESCRIPTION [Overview] A method for manufacturing an SOI MOSFET, in which a region without crystal grains is formed in the process of recrystallization, and a channel portion and an LDD portion are formed in this region by self-alignment. It was done like this.

〔産業上の利用分野〕[Industrial application field]

本発明はSOI型MOSFETの製造方法に関する。 The present invention relates to a method for manufacturing an SOI type MOSFET.

SOI型MOSFETは、絶縁体の基板の上にシリコン層を形成
しそこにソース電極(S)とドレイン電極(D)を配置
すると共にSとD間にゲート電極(G)を設けたもので
ある。
The SOI type MOSFET has a silicon layer formed on an insulating substrate, a source electrode (S) and a drain electrode (D) arranged thereon, and a gate electrode (G) provided between S and D. .

このSOI型MOSFETは、高集積化、高耐圧化、高速化、三
次元化等が可能であるという種々の利点を有するもので
ある。
This SOI type MOSFET has various advantages that it can be highly integrated, have high breakdown voltage, high speed, and three-dimensional.

しかし、このFETのシリコン層でキャリア輸送が行われ
る領域に、結晶粒(Grain)の境界(Boundary)である
結晶粒界(Grain Boundary)が生成するとこの結晶粒界
でキャリヤが散乱したり、深い準位が生じ、SOI型MOSFE
Tの電気的特性が低下する。
However, when a grain boundary (Grain Boundary), which is a boundary (Boundary) of crystal grains (Grain), is generated in a region where carrier transport is performed in the silicon layer of the FET, carriers are scattered or deep in the crystal grain boundary. A level is generated and SOI type MOSFE
The electrical characteristics of T deteriorate.

従って、キャリア輸送領域には結晶粒界が存在しないよ
うこれを排除する必要がある。
Therefore, it is necessary to eliminate the crystal grain boundaries so that they do not exist in the carrier transport region.

〔従来の技術〕[Conventional technology]

従来、再結晶化法によって結晶粒界が存在しない領域の
大きさとその位置の制御は行なわれていなかった。
Conventionally, the size and the position of the region where the crystal grain boundaries do not exist have not been controlled by the recrystallization method.

即ち、第4図(A)に示すように、矢印方向にエネルギ
線例えばレーザ光をスキャニング照射し、一旦結晶粒を
液化し再び固化する無数の結晶粒界gbが形成されたシリ
コン層が得られる。この再結晶の過程で結晶粒の拡大化
が図られている。図中Rはトランジスタ領域を示す。
That is, as shown in FIG. 4 (A), an energy beam such as a laser beam is scanning-irradiated in the direction of the arrow to obtain a silicon layer in which numerous crystal grain boundaries gb are formed in which crystal grains are once liquefied and solidified again. . The crystal grains are enlarged in the process of this recrystallization. In the figure, R indicates a transistor region.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

ところが、上述した従来の製造方法ではチャネル領域に
結晶粒界が位置することがある。
However, in the above-described conventional manufacturing method, the crystal grain boundary may be located in the channel region.

例えば、第4図(B)の左方の図に示すように結晶粒界
gb1が長手方向に平行となる場合と、同図の右方の図に
示すようにgb2が横手方向に存在する場合である。
For example, as shown in the diagram on the left side of FIG.
There are cases in which gb 1 is parallel to the longitudinal direction, and cases in which gb 2 exists in the lateral direction as shown in the diagram on the right side of the figure.

前者の場合は、gb1に沿ってソース又はドレイン層のド
ーパントの増速拡散が生じ極端なときはショートする。
また後者の場合はgb2の存在によりキャリアの散乱が起
こり移動量が低下する。
In the former case, accelerated diffusion of the dopant of the source or drain layer occurs along gb 1 to cause a short in an extreme case.
In the latter case, the presence of gb 2 causes carrier scattering to reduce the amount of movement.

即ち、従来は、電気的特性に悪影響を及ぼすという問題
点があった。
That is, conventionally, there has been a problem that the electrical characteristics are adversely affected.

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

本発明の目的は、上記問題点を解決し電気的特性に悪影
響を及ぼさないSOI型MOSFETの製造方法を提供すること
にある。
An object of the present invention is to provide a method for manufacturing an SOI type MOSFET that solves the above problems and does not adversely affect the electrical characteristics.

そのための手段は、結晶粒界のない領域に相当する範囲
が突出した熱伝導を制御する層をシリコン層上に形成
し、さらにその上にエネルギ線吸収層を形成し、該エネ
ルギ線吸収層の上方から、エネルギー線を照射すること
により再結晶過程で上記突起部分に対応したシリコン層
領域に結晶粒界が形成されないようにし、この内部に自
己整合によりチャネル部とLDD部を形成するようにした
ものである。
A means for that is to form a layer for controlling heat conduction, in which a region corresponding to a region having no grain boundary is protruding, on the silicon layer, and further, an energy ray absorbing layer is formed thereon, and the energy ray absorbing layer is formed. By irradiating an energy beam from above, crystal grain boundaries are prevented from being formed in the silicon layer region corresponding to the above-mentioned protruding portion in the recrystallization process, and the channel portion and the LDD portion are formed inside this by self-alignment. It is a thing.

〔作 用〕[Work]

上記のとおり、本発明によれば再結晶化の過程で結晶粒
界の発生が阻止された領域をシリコン層中に形成でき
る。
As described above, according to the present invention, it is possible to form a region in the silicon layer in which the generation of grain boundaries is prevented during the recrystallization process.

従って、SとDの間でGの下に結晶粒界が存在する場合
がなくなって、ドーパントの増速拡散又は散乱が生じな
くなるので、電気的特性に悪影響を及ぼすことがなくな
った。
Therefore, the crystal grain boundary does not exist under G between S and D, and the accelerated diffusion or scattering of the dopant does not occur, so that the electrical characteristics are not adversely affected.

〔実施例〕〔Example〕

以下、本発明を、実施例により添付図面を参照して、説
明する。
Hereinafter, the present invention will be described by way of examples with reference to the accompanying drawings.

第1図は本発明の実施例を示す図である。FIG. 1 is a diagram showing an embodiment of the present invention.

第1図(A)は断面図であり、絶縁体基板1上に形成し
たシリコン層2の上表面に突起部31を有する熱伝導制御
層3が更にその上にエネルギ線吸収層4が積層されてい
る。
FIG. 1 (A) is a cross-sectional view, in which the heat conduction control layer 3 having the protrusions 31 on the upper surface of the silicon layer 2 formed on the insulator substrate 1 is further laminated with the energy ray absorbing layer 4. ing.

このエネルギ線吸収層4の上方から、エネルギ線5をス
キャニング照射する(第3図(A))。
The energy rays 5 are scanned and irradiated from above the energy ray absorption layer 4 (FIG. 3 (A)).

このとき、レーザ光を吸収して発熱したエネルギー線吸
収層4より熱伝導制御層3を通してシリコン層2へヒー
トフローが起こる。2のヒートフローの量は突起部31以
外の方が多くなるので、温度分布は第1図(B)に示す
ようになり、突起部31の下方のシリコン層内部21では結
晶粒界が発生しない(第3図(B))。つまり、この温
度分布を形成することによって、核成長の始まる場所を
定義し、同時に結晶粒の大きさも定義したのである。
At this time, a heat flow occurs from the energy ray absorbing layer 4 which absorbs the laser light and generates heat to the silicon layer 2 through the heat conduction control layer 3. Since the amount of heat flow of No. 2 is larger than that of the portion other than the protrusion 31, the temperature distribution is as shown in FIG. 1 (B), and no grain boundary is generated in the silicon layer inside 21 below the protrusion 31. (FIG. 3 (B)). In other words, by forming this temperature distribution, the place where the nucleus growth starts was defined, and at the same time, the size of the crystal grain was defined.

その後、上記エネルギ線吸収層4をはく離する(第3図
(C))。
Then, the energy ray absorbing layer 4 is peeled off (FIG. 3 (C)).

そして、露出した熱伝導制御層3(第1図(A))をイ
オン注入用マスクとしたドーピングを行い、ソースとド
レイン領域を形成した後(第3図(D))該制御層3を
はく離する。
Then, after the exposed heat conduction control layer 3 (FIG. 1A) is doped with an ion implantation mask to form source and drain regions (FIG. 3D), the control layer 3 is peeled off. To do.

次に素子分離すると共にゲート酸化膜6を形成する(第
3図(E))。
Next, the elements are separated and the gate oxide film 6 is formed (FIG. 3 (E)).

最後に、結晶粒界が存在しない領域21より幅の狭いゲー
ト電極6を形成し、これをマスクとしてLDD部8,9を形成
する(第3図(F)、第2図)。
Finally, the gate electrode 6 having a width narrower than the region 21 where the crystal grain boundaries do not exist is formed, and the LDD portions 8 and 9 are formed using this as a mask (FIG. 3 (F), FIG. 2).

即ち、ゲート電極を用いた自己整合によりLDD部を形成
する。このLDD(Lightly Doped Drain)部は不純物量が
ドレインの約1/100で、電界の集集中を抑えて耐圧を向
上させる働らきがある。
That is, the LDD portion is formed by self-alignment using the gate electrode. In this LDD (Lightly Doped Drain) part, the amount of impurities is about 1/100 of that of the drain.

以後は、通常のMOSFETと同じ工程により製品として完成
する。
After that, it is completed as a product by the same process as a normal MOSFET.

〔発明の効果〕〔The invention's effect〕

上記のとおり、本発明によれば再結晶化の過程で結晶粒
界の発生が阻止された領域をシリコン層中に形成でき
る。
As described above, according to the present invention, it is possible to form a region in the silicon layer in which the generation of grain boundaries is prevented during the recrystallization process.

従って、SとDの間でGの下から結晶粒界を排除でき、
ドーパントの増速拡散又はキャリアの散乱が生じなくな
るので、電気的特性に悪影響を及ぼすことがなくなっ
た。
Therefore, the grain boundary can be eliminated from below G between S and D,
Since the enhanced diffusion of the dopant or the scattering of carriers does not occur, the electrical characteristics are not adversely affected.

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

第1図は本発明の実施例を示す図(その1)、第2図は
本発明の実施例を示す図(その2)、第3図は本発明に
よる工程図、第4図は従来技術の説明図である。 1……絶縁体基板、2……シリコン層、 3……熱伝導制御層、 4……エネルギ線吸収層、 21……結晶粒界の存在しない領域、 31……突起部。
FIG. 1 is a view showing an embodiment of the present invention (No. 1), FIG. 2 is a view showing an embodiment of the present invention (No. 2), FIG. 3 is a process chart according to the present invention, and FIG. FIG. 1 ... Insulator substrate, 2 ... Silicon layer, 3 ... Heat conduction control layer, 4 ... Energy ray absorption layer, 21 ... Region where no grain boundaries exist, 31 ... Protrusion.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】絶縁体基板上に形成したシリコン層の上表
面に、突起部を有する熱伝導制御層を更にその上にエネ
ルギ線吸収層を形成し、 該エネルギ線吸収層の上方からエネルギ線を照射するこ
とにより上記突起部の下方に対応したシリコン層領域に
結晶粒界の存在しない領域を形成した後にエネルギ線吸
収層を除去し、露出した熱伝導制御層をマスクとしてソ
ースとドレイン形成のためにドーピングを行い、ソース
とドレイン領域を形成した後上記熱伝導制御層をはく離
し、ゲート酸化膜を形成し、更に上記結晶粒界の存在し
ない領域の幅より狭いゲート電極を設け、さらにこれを
マスクとしてドーピングを行い自己整合によりLDD部を
形成することを特徴とする、 SOI型MOSFETの製造方法。
1. A heat conduction control layer having a protrusion is further formed on an upper surface of a silicon layer formed on an insulating substrate, and an energy ray absorbing layer is formed thereon. Is applied to form a region where no crystal grain boundary exists in the silicon layer region corresponding to the lower part of the protrusion, and then the energy ray absorbing layer is removed, and the exposed heat conduction control layer is used as a mask to form the source and drain. In order to do so, the source and drain regions are formed, then the heat conduction control layer is peeled off, a gate oxide film is formed, and a gate electrode narrower than the width of the region where no crystal grain boundary exists is provided. A method for manufacturing an SOI-type MOSFET, characterized in that the LDD portion is formed by self-alignment with doping as a mask.
JP61033752A 1986-02-20 1986-02-20 Method for manufacturing SOI MOSFET Expired - Lifetime JPH0738448B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61033752A JPH0738448B2 (en) 1986-02-20 1986-02-20 Method for manufacturing SOI MOSFET

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61033752A JPH0738448B2 (en) 1986-02-20 1986-02-20 Method for manufacturing SOI MOSFET

Publications (2)

Publication Number Publication Date
JPS62193178A JPS62193178A (en) 1987-08-25
JPH0738448B2 true JPH0738448B2 (en) 1995-04-26

Family

ID=12395156

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61033752A Expired - Lifetime JPH0738448B2 (en) 1986-02-20 1986-02-20 Method for manufacturing SOI MOSFET

Country Status (1)

Country Link
JP (1) JPH0738448B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA2031254A1 (en) * 1989-12-01 1991-06-02 Kenji Aoki Doping method of barrier region in semiconductor device
EP0505877A2 (en) * 1991-03-27 1992-09-30 Seiko Instruments Inc. Impurity doping method with adsorbed diffusion source
WO2002009192A1 (en) * 2000-07-24 2002-01-31 Matsushita Electric Industrial Co., Ltd. Semiconductor device, liquid crystal display device, el display device, semiconductor film producing method, and semiconductor device producing method

Also Published As

Publication number Publication date
JPS62193178A (en) 1987-08-25

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