JPH03203378A - Thin film transistor - Google Patents

Thin film transistor

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Publication number
JPH03203378A
JPH03203378A JP34285889A JP34285889A JPH03203378A JP H03203378 A JPH03203378 A JP H03203378A JP 34285889 A JP34285889 A JP 34285889A JP 34285889 A JP34285889 A JP 34285889A JP H03203378 A JPH03203378 A JP H03203378A
Authority
JP
Japan
Prior art keywords
film
polycrystalline silicon
thickness
thin film
gate
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.)
Granted
Application number
JP34285889A
Other languages
Japanese (ja)
Other versions
JP2629995B2 (en
Inventor
Noriaki Kodama
児玉 典昭
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
NEC Corp
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Priority to JP1342858A priority Critical patent/JP2629995B2/en
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  • Recrystallisation Techniques (AREA)

Abstract

PURPOSE:To restrain hot carrier effect of bias stress, realize high reliability, and reduce irregularity of characteristics, by making the thickness of a polycrystalline silicon film constituting a channel region 10-40nm. CONSTITUTION:On an Si substrate 1, a field oxide film 2 is formed, and thereon a polycrystalline Si film 3 of 10-40nm in thickness is formed. By thermal oxidation, an Si oxide film 4 is formed on the film 3, and the thickness of the film 3 is reduced. The whole part of the film 4 is etched and eliminated, and an element forming region is defined by patterning the film 3. By thermally oxidizing the film 3 surface, a gate oxide film 5 is formed. A gate electrode 6 is selectively formed on the film 5; the electrode 6 is used as a mask, and P-type impurity ions are introduced, thereby forming a source.drain region 7. An interlayer insulating film 8 is deposited on the surface; an extraction electrode 9 connected with the region 7 is formed by selectively forming an aperture; thus a thin film transistor is constituted.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は薄膜トランジスタに関し、特に多結晶シリコン
膜による薄膜トランジスタに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a thin film transistor, and more particularly to a thin film transistor using a polycrystalline silicon film.

〔従来の技術〕[Conventional technology]

活性層を多結晶シリコン膜により構成した多結晶シリコ
ン薄膜トランジスタが知られている。
2. Description of the Related Art A polycrystalline silicon thin film transistor whose active layer is made of a polycrystalline silicon film is known.

第5図は従来の薄膜トランジスタの一例を示す断面図で
ある。
FIG. 5 is a cross-sectional view showing an example of a conventional thin film transistor.

シリコン基板lの上に設けたフィールド酸化膜2の上に
パターンニングされた薄い多結晶シリコン膜3を設け、
多結晶シリコン膜3の上にゲート酸化膜5を介してゲー
ト電極6を設け、ゲート電極6に整合して多結晶シリコ
ン膜3にソース・ドレイン領域7を設け、多結晶シリコ
ン膜3及びゲート電極6を全面に覆うように層間絶縁膜
8を設け、多結晶シリコン膜3のソース・ドレイン領域
7に接続するように層間絶縁膜8に設けたコンタクト用
開孔部のそれぞれに引き出し電極9を設けて構成される
A patterned thin polycrystalline silicon film 3 is provided on a field oxide film 2 provided on a silicon substrate l,
A gate electrode 6 is provided on the polycrystalline silicon film 3 via a gate oxide film 5, a source/drain region 7 is provided in the polycrystalline silicon film 3 in alignment with the gate electrode 6, and the polycrystalline silicon film 3 and the gate electrode are provided. An interlayer insulating film 8 is provided so as to cover the entire surface of the polycrystalline silicon film 3, and an extraction electrode 9 is provided in each of the contact openings provided in the interlayer insulating film 8 so as to be connected to the source/drain regions 7 of the polycrystalline silicon film 3. It consists of

ここで、ゲート電極6下のチャネル領域の多結晶シリコ
ン膜3の膜厚は、例えば2〜10nmのとき実効移動度
が最大になるといわれている(特開昭61−85868
号参照)。
Here, it is said that the effective mobility is maximized when the thickness of the polycrystalline silicon film 3 in the channel region under the gate electrode 6 is, for example, 2 to 10 nm (Japanese Unexamined Patent Publication No. 61-85868).
(see issue).

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上述した従来の薄膜トランジスタは、チャネル領域を形
成する多結晶シリコン膜の膜厚を10nm以下にすると
、以下に示す様に特性のばらつきが大きくなるという欠
点がある。即ち、オン電流のばらつきは多結晶シリコン
膜の膜厚が薄くなる程大きくなる傾向があり、特に10
nm以下ではばらつきは急増する。多結晶シリコン膜の
膜厚が10nm以下では多結晶シリコン膜の結晶粒は、
隣り合せどうし粒界を隔てて、密接に接近しておらず、
粒界での抵抗成分が非常に大きくなる。そのため、チャ
ネル領域における多結晶シリコン膜の粒界の存在、域は
、粒界の数によりオン電流が大きくばらつくことになる
The above-mentioned conventional thin film transistor has a drawback that when the thickness of the polycrystalline silicon film forming the channel region is reduced to 10 nm or less, the characteristics vary widely as shown below. That is, the variation in on-current tends to increase as the thickness of the polycrystalline silicon film becomes thinner.
Below nm, the variation rapidly increases. When the thickness of the polycrystalline silicon film is 10 nm or less, the crystal grains of the polycrystalline silicon film are
Adjacent grain boundaries are separated from each other, and they are not closely approached.
The resistance component at grain boundaries becomes extremely large. Therefore, the presence and area of grain boundaries in the polycrystalline silicon film in the channel region causes on-current to vary greatly depending on the number of grain boundaries.

〔課題を解決するための手段〕[Means to solve the problem]

本発明の薄膜トランジスタは、チャネル領域を形成する
多結晶シリコン膜の膜厚を10〜40nmに構成する。
In the thin film transistor of the present invention, the thickness of the polycrystalline silicon film forming the channel region is 10 to 40 nm.

〔実施例〕〔Example〕

次に、本発明について図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.

第1図(a)〜(e)は本発明の一実施例を説明するた
めの工程順に示した半導体チップの断面図である。
FIGS. 1A to 1E are cross-sectional views of a semiconductor chip shown in order of steps for explaining an embodiment of the present invention.

まず、第1図(a)に示すように、シリコン基板lの上
にフィールド酸化膜2を設け、フィールド酸化膜2の上
に例えば減圧化学気相成長法により、SiH4をソース
ガスとして575℃の温度でP型不純物を含む非晶質シ
リコン薄膜を約15nmの厚さに堆積する。しかる後、
窒素雰囲気中で600℃12時間の熱処理を施し、前記
非晶質シリコン薄膜を多結晶化し、多結晶シリコン膜3
を形成する。ここではじめに非晶質シリコン薄膜を堆積
し、600℃12時間の熱処理を施して、多結晶化する
という手順を踏んだのは、結晶粒の大きな多結晶シリコ
ン膜3を得るためである。多結晶シリコン膜3の粒径を
大きくすることはトランジスタの実効移動度を高める効
果がある。
First, as shown in FIG. 1(a), a field oxide film 2 is provided on a silicon substrate 1, and the field oxide film 2 is grown at 575° C. using SiH4 as a source gas, for example, by low pressure chemical vapor deposition. An amorphous silicon thin film containing P-type impurities is deposited to a thickness of about 15 nm at temperature. After that,
Heat treatment is performed at 600° C. for 12 hours in a nitrogen atmosphere to polycrystallize the amorphous silicon thin film, forming a polycrystalline silicon film 3.
form. The reason why we first deposited an amorphous silicon thin film and subjected it to heat treatment at 600° C. for 12 hours to polycrystallize it was to obtain a polycrystalline silicon film 3 with large crystal grains. Increasing the grain size of the polycrystalline silicon film 3 has the effect of increasing the effective mobility of the transistor.

次に、第1図(b)に示すように、多結晶シリコン膜3
の上表面を熱酸化して酸化シリコン膜4を形成し、多結
晶シリコン膜3の膜厚を薄くする。
Next, as shown in FIG. 1(b), a polycrystalline silicon film 3
The upper surface of the polycrystalline silicon film 3 is thermally oxidized to form a silicon oxide film 4, and the thickness of the polycrystalline silicon film 3 is reduced.

次に、第1図(C)に示すように、酸化シリコン膜4を
全面に亘すエッチングして除去し、薄膜化された多結晶
シリコン膜3を選択的にエツチングしてパターンニング
し、素子形成領域を区画する。
Next, as shown in FIG. 1C, the silicon oxide film 4 is etched and removed over the entire surface, and the thinned polycrystalline silicon film 3 is selectively etched and patterned to form the device. Define the formation area.

次に、多結晶シリコン膜3の表面を熱酸化して、ゲート
酸化膜5を形成する。
Next, the surface of polycrystalline silicon film 3 is thermally oxidized to form gate oxide film 5.

次に、第1図(d)に示すように素子形成領域のゲート
酸化膜5の上に選択的にゲート電極6を形成し、イオン
注入法によりゲート電極6をマスクとして多結晶シリコ
ン膜3にP型不純物イオンを導入し、ソース・ドレイン
領域7を形成する。
Next, as shown in FIG. 1(d), a gate electrode 6 is selectively formed on the gate oxide film 5 in the element formation region, and the polycrystalline silicon film 3 is formed by ion implantation using the gate electrode 6 as a mask. P-type impurity ions are introduced to form source/drain regions 7.

次に、第1図(e)に示すように、多結晶シリコン膜3
及びゲート電極6を含む表面に眉間絶縁膜8を堆積し、
ソース・ドレイン領域7の上の眉間絶縁膜8を選択的に
開孔してコンタクト用開孔部を設ける。次に、コンタク
ト用開孔部のソース・ドレイン領域7と接続する引出電
極9をそれぞれ選択的に設けて薄膜トランジスタを構成
する。
Next, as shown in FIG. 1(e), a polycrystalline silicon film 3
and depositing a glabellar insulating film 8 on the surface including the gate electrode 6,
Contact openings are provided by selectively opening holes in the glabella insulating film 8 above the source/drain regions 7. Next, lead electrodes 9 connected to the source/drain regions 7 of the contact openings are selectively provided to form a thin film transistor.

第2図(a)、 (b)は実施例のPチャネル型多結晶
シリコン薄!+−ランジスタのサブスレツショ/1/ド
特性図である。ここで、ゲート長は0.6μmである。
Figures 2 (a) and (b) show the P-channel type polycrystalline silicon thin film of the example! FIG. 3 is a subthreshold/1/mode characteristic diagram of a +- transistor. Here, the gate length is 0.6 μm.

実線が初期特性であり、破線はトランジスタにゲート・
ソース間電圧−2V、  ドレイン−ソース間電圧−1
0Vを印加して、1000秒保持してストレスを加えた
後の特性である。チャネル領域の多結晶シリコン膜の膜
厚は、第2図(a)が120nm、第2図(b)は40
nmである。第2図(a)に示すように、多結晶シリコ
ン膜の膜厚が120nmの場合には、ストレス後にはバ
ンチスルーの特性を示し劣化が大きいのに対し、第2図
(b)に示すように、多結晶シリコン薄膜の膜厚が40
nmの場合には、ストレス後の特性の劣化はほとんどな
い。
The solid line is the initial characteristic, and the dashed line is the gate and
Source voltage -2V, drain-source voltage -1
This is the characteristic after applying stress by applying 0V and holding it for 1000 seconds. The thickness of the polycrystalline silicon film in the channel region is 120 nm in FIG. 2(a) and 40 nm in FIG. 2(b).
It is nm. As shown in Figure 2(a), when the polycrystalline silicon film has a thickness of 120 nm, it exhibits bunch-through characteristics after stress and exhibits large deterioration, whereas as shown in Figure 2(b), The thickness of the polycrystalline silicon thin film is 40 mm.
In the case of nm, there is almost no deterioration in characteristics after stress.

ストレス後にパンチスルー特性が現れるのは、ストレス
中にドレイン近傍に発生したホットエレクトロンがゲー
ト酸化膜に捕獲され、ドレイン端にチャネルが形成され
る結果、実効的なゲート長が短縮するためである。Pチ
ャネル型トランジスタにおいては、飽和領域動作時に生
ずる。ホットキャリアの量の大小は、動作状態における
ゲート電流の大小で評価できる。
The punch-through characteristic appears after stress because hot electrons generated near the drain during stress are captured in the gate oxide film, forming a channel at the end of the drain, resulting in a shortening of the effective gate length. In a P-channel transistor, this occurs during operation in the saturation region. The amount of hot carriers can be evaluated by the amount of gate current in the operating state.

第3図は、ゲート電流対ゲート電圧特性図である。実線
は、チャネル領域を形成する多結晶シリコン膜の膜厚が
120nmの場合であり、破線は、膜厚が40nmの場
合である。膜厚120nmのものより膜厚40nmのも
のの方がゲート電流が1桁以下低い値を示し、第2図(
a)、 (b)で示した膜厚40nmの方が劣化に強い
という結果に一致する。
FIG. 3 is a characteristic diagram of gate current versus gate voltage. The solid line indicates the case where the thickness of the polycrystalline silicon film forming the channel region is 120 nm, and the broken line indicates the case where the film thickness is 40 nm. The gate current with a film thickness of 40 nm is one order of magnitude lower than that with a film thickness of 120 nm, as shown in Figure 2 (
This agrees with the results shown in a) and (b) that the film thickness of 40 nm is more resistant to deterioration.

第4図に、実線が最大ゲート電流とチャネル領域の多結
晶シリコン薄膜の膜厚の関係を示し、破線がオン電流の
ばらつきとチャネル領域の多結晶シリコン薄膜の膜厚の
関係を示す。最大ゲート電流は、ドレイン・ソース間電
圧を一10Vにして、グーI・・ソース間電圧をO■か
ら一5■まで掃引印加し、この範囲におけるゲート電流
の最大値である。オン電流のばらつきは、ドレイン・ソ
ース間電圧を一5V、ゲート・ソース間電圧を一5■と
した時のドレイン電流をオン電流とし、このオン電流の
最大値と最小値の比を対数で表示した。
In FIG. 4, the solid line shows the relationship between the maximum gate current and the thickness of the polycrystalline silicon thin film in the channel region, and the broken line shows the relationship between the variation in on-current and the film thickness of the polycrystalline silicon thin film in the channel region. The maximum gate current is obtained by setting the drain-source voltage to -10 V and applying the G-I source voltage in a sweeping manner from 0 to -15 V, and is the maximum value of the gate current in this range. The variation in on-current is expressed as the drain current when the drain-source voltage is 15V and the gate-source voltage is 15V, and the ratio of the maximum value and minimum value of this on-current is expressed as a logarithm. did.

最大ゲート電流は、多結晶シリコン薄膜の膜厚を薄くす
るほど小さくなる傾向があるが、膜厚40nm程度以下
で飽和する傾向がある。
The maximum gate current tends to become smaller as the thickness of the polycrystalline silicon thin film becomes thinner, but it tends to be saturated when the film thickness is about 40 nm or less.

従って、バイアスストレスに強い薄膜トランジスタを得
るには、チャネル領域の多結晶シリコン膜の膜厚な40
nm以下にするのが望ましいといえる。
Therefore, in order to obtain a thin film transistor that is resistant to bias stress, it is necessary to increase the thickness of the polycrystalline silicon film in the channel region by 40 mm.
It can be said that it is desirable to make it less than nm.

またばらつきに関しては、チャネル領域の多結晶シリコ
ン膜の膜厚を薄くする程大きくなる傾向がある。特に膜
厚が10nm以下ではばらつきは急増する。故にバイア
スストレスに強くホットキャリア耐性の高い高信頼性を
有して、及び特性のばらつきの小さい薄膜トランジスタ
は、チャネル領域の多結晶シリコン膜の膜厚な10〜4
0nmにすることで得られる。
Furthermore, the variation tends to increase as the thickness of the polycrystalline silicon film in the channel region becomes thinner. In particular, when the film thickness is 10 nm or less, the variation increases rapidly. Therefore, a thin film transistor that is resistant to bias stress, has high reliability with high hot carrier resistance, and has small variations in characteristics is made when the thickness of the polycrystalline silicon film in the channel region is 10 to 4.
This can be obtained by setting the thickness to 0 nm.

以上、Pチャネル型多結晶シリコン薄膜トランジスタの
例を述べたが、Nチャネル型でも同様でチャネル領域を
形成する多結晶シリコン薄膜の膜厚な10〜40nmに
することでホットキャリア耐性の高い高信頼性を有して
、特性のばらつきの小さい薄膜トランジスタを得ること
ができる。
The above describes an example of a P-channel type polycrystalline silicon thin film transistor, but the same applies to an N-channel type as well, and by making the polycrystalline silicon thin film that forms the channel region 10 to 40 nm thick, high reliability with high hot carrier resistance can be achieved. With this, it is possible to obtain a thin film transistor with small variations in characteristics.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、多結晶シリコン薄膜トラ
ンジスタにおいてチャネル領域を形成する多結晶シリコ
ン膜の膜厚を10〜40nmの範囲内にすることで、バ
イアスストレスによるホットキャリア効果を大きく抑制
でき、高い信頼性を実現でき、また特性のばらつきも小
さくできる効果がある。
As explained above, the present invention makes it possible to greatly suppress the hot carrier effect caused by bias stress by setting the thickness of the polycrystalline silicon film forming the channel region in the polycrystalline silicon thin film transistor within the range of 10 to 40 nm. This has the effect of achieving reliability and reducing variation in characteristics.

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

第1図(a)〜(e)は本発明の一実施例を説明するた
めの工程順に示した半導体チ、ブの断面図、第2図(a
)、 (b)は実施例のサブスレッショルド特性図、第
3図はゲート電流対ゲート電圧特性図、第4図は最大ゲ
ート電流対チャネル領域の多結晶シリコン膜の膜厚の関
係と、オン電流のばらつき対チャネル領域の多結晶シリ
コン膜の膜厚の関係を示す図、第5図は従来の薄膜トラ
ンジスタの一例を示す断面図である。 l・・・・・・シリコン基板、2・・・・・・フィール
ド酸化膜、3・・・・・・多結晶シリコン膜、4・・・
・・・酸化シリコン膜、5・・・・・・ゲート酸化膜、
6・・・・・・ゲート電極、7・・・・・・ソース・ド
レイン領域、8・・・・・・層間絶縁膜、9・・・・・
・引出電極。
1(a) to 1(e) are cross-sectional views of semiconductor chips shown in the order of steps for explaining one embodiment of the present invention, and FIG. 2(a)
), (b) is a subthreshold characteristic diagram of the example, FIG. 3 is a gate current vs. gate voltage characteristic diagram, and FIG. 4 is a relationship between maximum gate current vs. film thickness of the polycrystalline silicon film in the channel region, and on-current. FIG. 5 is a cross-sectional view showing an example of a conventional thin film transistor. l...Silicon substrate, 2...Field oxide film, 3...Polycrystalline silicon film, 4...
...Silicon oxide film, 5...Gate oxide film,
6...Gate electrode, 7...Source/drain region, 8...Interlayer insulating film, 9...
・Extraction electrode.

Claims (1)

【特許請求の範囲】[Claims] チャネルが形成される活性層を多結晶シリコン膜により
構成した薄膜トランジスタにおいて、前記多結晶シリコ
ン膜の膜厚が10〜40nmであることを特徴とする薄
膜トランジスタ。
1. A thin film transistor in which an active layer in which a channel is formed is made of a polycrystalline silicon film, wherein the polycrystalline silicon film has a thickness of 10 to 40 nm.
JP1342858A 1989-12-29 1989-12-29 Thin film transistor Expired - Lifetime JP2629995B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1342858A JP2629995B2 (en) 1989-12-29 1989-12-29 Thin film transistor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1342858A JP2629995B2 (en) 1989-12-29 1989-12-29 Thin film transistor

Publications (2)

Publication Number Publication Date
JPH03203378A true JPH03203378A (en) 1991-09-05
JP2629995B2 JP2629995B2 (en) 1997-07-16

Family

ID=18357040

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1342858A Expired - Lifetime JP2629995B2 (en) 1989-12-29 1989-12-29 Thin film transistor

Country Status (1)

Country Link
JP (1) JP2629995B2 (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04301623A (en) * 1991-03-29 1992-10-26 Sharp Corp Production of thin-film transistor
JPH0766424A (en) * 1993-08-20 1995-03-10 Semiconductor Energy Lab Co Ltd Semiconductor device and manufacturing method thereof
US6323069B1 (en) 1992-03-25 2001-11-27 Semiconductor Energy Laboratory Co., Ltd. Method of manufacturing a thin film transistor using light irradiation to form impurity regions
US6331717B1 (en) 1993-08-12 2001-12-18 Semiconductor Energy Laboratory Co. Ltd. Insulated gate semiconductor device and process for fabricating the same
US6500703B1 (en) 1993-08-12 2002-12-31 Semicondcutor Energy Laboratory Co., Ltd. Insulated gate semiconductor device and process for fabricating the same
JP2007173788A (en) * 2005-11-23 2007-07-05 Semiconductor Energy Lab Co Ltd Manufacturing method of semiconductor element and semiconductor element
WO2009123127A1 (en) * 2008-04-02 2009-10-08 Nec液晶テクノロジー株式会社 Semiconductor device, semiconductor device manufacturing method, liquid crystal display device and electronic apparatus
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CN120603270A (en) * 2025-08-11 2025-09-05 华羿微电子股份有限公司 A method for preparing an ultra-low gate charge shielded gate MOSFET device and a device thereof

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