JPH0544195B2 - - Google Patents
Info
- Publication number
- JPH0544195B2 JPH0544195B2 JP5433682A JP5433682A JPH0544195B2 JP H0544195 B2 JPH0544195 B2 JP H0544195B2 JP 5433682 A JP5433682 A JP 5433682A JP 5433682 A JP5433682 A JP 5433682A JP H0544195 B2 JPH0544195 B2 JP H0544195B2
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- current
- drain
- film transistors
- transistor
- 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
Links
- 239000010409 thin film Substances 0.000 claims description 73
- 239000011159 matrix material Substances 0.000 claims description 11
- 239000000758 substrate Substances 0.000 claims description 10
- 239000004973 liquid crystal related substance Substances 0.000 description 19
- 239000004065 semiconductor Substances 0.000 description 14
- 239000003990 capacitor Substances 0.000 description 10
- 239000008186 active pharmaceutical agent Substances 0.000 description 9
- 238000010586 diagram Methods 0.000 description 8
- 230000007423 decrease Effects 0.000 description 5
- 230000005684 electric field Effects 0.000 description 4
- 230000007246 mechanism Effects 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 238000002474 experimental method Methods 0.000 description 3
- 239000011521 glass Substances 0.000 description 3
- 239000010410 layer Substances 0.000 description 3
- 230000008859 change Effects 0.000 description 2
- 239000010408 film Substances 0.000 description 2
- 230000006872 improvement Effects 0.000 description 2
- 230000014759 maintenance of location Effects 0.000 description 2
- 230000000717 retained effect Effects 0.000 description 2
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- 229910052785 arsenic Inorganic materials 0.000 description 1
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical compound [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 238000005094 computer simulation Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000005669 field effect Effects 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 239000011229 interlayer Substances 0.000 description 1
- 230000007257 malfunction Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 229910052698 phosphorus Inorganic materials 0.000 description 1
- 239000011574 phosphorus Substances 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 229910021420 polycrystalline silicon Inorganic materials 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/68—Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/78—Field effect transistors with field effect produced by an insulated gate
-
- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09G—ARRANGEMENTS OR CIRCUITS FOR CONTROL OF INDICATING DEVICES USING STATIC MEANS TO PRESENT VARIABLE INFORMATION
- G09G3/00—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes
- G09G3/20—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes for presentation of an assembly of a number of characters, e.g. a page, by composing the assembly by combination of individual elements arranged in a matrix no fixed position being assigned to or needed to be assigned to the individual characters or partial characters
- G09G3/34—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes for presentation of an assembly of a number of characters, e.g. a page, by composing the assembly by combination of individual elements arranged in a matrix no fixed position being assigned to or needed to be assigned to the individual characters or partial characters by control of light from an independent source
- G09G3/36—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes for presentation of an assembly of a number of characters, e.g. a page, by composing the assembly by combination of individual elements arranged in a matrix no fixed position being assigned to or needed to be assigned to the individual characters or partial characters by control of light from an independent source using liquid crystals
- G09G3/3611—Control of matrices with row and column drivers
- G09G3/3674—Details of drivers for scan electrodes
- G09G3/3677—Details of drivers for scan electrodes suitable for active matrices only
-
- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09G—ARRANGEMENTS OR CIRCUITS FOR CONTROL OF INDICATING DEVICES USING STATIC MEANS TO PRESENT VARIABLE INFORMATION
- G09G3/00—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes
- G09G3/20—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes for presentation of an assembly of a number of characters, e.g. a page, by composing the assembly by combination of individual elements arranged in a matrix no fixed position being assigned to or needed to be assigned to the individual characters or partial characters
- G09G3/34—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes for presentation of an assembly of a number of characters, e.g. a page, by composing the assembly by combination of individual elements arranged in a matrix no fixed position being assigned to or needed to be assigned to the individual characters or partial characters by control of light from an independent source
- G09G3/36—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes for presentation of an assembly of a number of characters, e.g. a page, by composing the assembly by combination of individual elements arranged in a matrix no fixed position being assigned to or needed to be assigned to the individual characters or partial characters by control of light from an independent source using liquid crystals
- G09G3/3611—Control of matrices with row and column drivers
- G09G3/3685—Details of drivers for data electrodes
- G09G3/3688—Details of drivers for data electrodes suitable for active matrices only
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/136—Liquid crystal cells structurally associated with a semi-conducting layer or substrate, e.g. cells forming part of an integrated circuit
- G02F1/1362—Active matrix addressed cells
- G02F1/13624—Active matrix addressed cells having more than one switching element per pixel
-
- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09G—ARRANGEMENTS OR CIRCUITS FOR CONTROL OF INDICATING DEVICES USING STATIC MEANS TO PRESENT VARIABLE INFORMATION
- G09G2300/00—Aspects of the constitution of display devices
- G09G2300/08—Active matrix structure, i.e. with use of active elements, inclusive of non-linear two terminal elements, in the pixels together with light emitting or modulating elements
- G09G2300/0809—Several active elements per pixel in active matrix panels
-
- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09G—ARRANGEMENTS OR CIRCUITS FOR CONTROL OF INDICATING DEVICES USING STATIC MEANS TO PRESENT VARIABLE INFORMATION
- G09G2300/00—Aspects of the constitution of display devices
- G09G2300/08—Active matrix structure, i.e. with use of active elements, inclusive of non-linear two terminal elements, in the pixels together with light emitting or modulating elements
- G09G2300/0809—Several active elements per pixel in active matrix panels
- G09G2300/0823—Several active elements per pixel in active matrix panels used to establish symmetry in driving, e.g. with polarity inversion
-
- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09G—ARRANGEMENTS OR CIRCUITS FOR CONTROL OF INDICATING DEVICES USING STATIC MEANS TO PRESENT VARIABLE INFORMATION
- G09G2320/00—Control of display operating conditions
- G09G2320/02—Improving the quality of display appearance
- G09G2320/0209—Crosstalk reduction, i.e. to reduce direct or indirect influences of signals directed to a certain pixel of the displayed image on other pixels of said image, inclusive of influences affecting pixels in different frames or fields or sub-images which constitute a same image, e.g. left and right images of a stereoscopic display
- G09G2320/0214—Crosstalk reduction, i.e. to reduce direct or indirect influences of signals directed to a certain pixel of the displayed image on other pixels of said image, inclusive of influences affecting pixels in different frames or fields or sub-images which constitute a same image, e.g. left and right images of a stereoscopic display with crosstalk due to leakage current of pixel switch in active matrix panels
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Theoretical Computer Science (AREA)
- Ceramic Engineering (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Liquid Crystal (AREA)
Description
【発明の詳細な説明】
本発明はソース・ドレイン間のリーク電流を低
減させる構造を有する半導体薄膜トランジスタに
関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor thin film transistor having a structure that reduces leakage current between a source and a drain.
近年、絶縁基板上に薄膜トランジスタを形成す
る研究が活発に行なわれている。この技術は、安
価な絶縁基板を用いて薄形デイスプレイを実現す
るアクテイブマトリツクスパネル、あるいは通常
の半導体集積回路上にトランジスタなどの能動素
子を形成する三次元集積回路、あるいは安価で高
性能なイメージセンサ、あるいは高密度のメモリ
など、数多くの応用が期待されるものである。以
下、薄膜トランジスタをアクテイブマトリツクス
パネルに応用した場合を例に取つて説明するが、
本発明は薄膜トランジスタを用いた他の場合にも
全く同様に適用することができる。これは、本発
明の主旨が、リーク電流を減少させるという薄膜
トランジスタの本質的な特性向上に関するものだ
からである。 In recent years, research on forming thin film transistors on insulating substrates has been actively conducted. This technology can be used to create active matrix panels that use inexpensive insulating substrates to create thin displays, three-dimensional integrated circuits that form active elements such as transistors on regular semiconductor integrated circuits, and inexpensive, high-performance images. It is expected to have many applications, including sensors and high-density memory. Below, we will explain the case where thin film transistors are applied to active matrix panels as an example.
The present invention can be similarly applied to other cases using thin film transistors. This is because the gist of the present invention is to reduce leakage current, which is an essential improvement in the characteristics of thin film transistors.
薄膜トランジスタのアクテイブマトリツクスパ
ネルに応用した場合の液晶表示装置は、一般に、
上側のガラス基板と、下側の薄膜トランジスタ基
板と、その間に封入された液晶とから構成されて
おり、前記薄膜トランジスタ基板上にマトリツク
ス状に配置された液晶駆動素子を外部選択回路に
より選択し、前記液晶駆動素子に接続された液晶
駆動電極に電圧を印加することにより、任意の文
字、図形、あるいは画像の表示を行なうものであ
る。前記薄膜トランジスタ基板の一般的な回路図
を第1図に示す。 Liquid crystal display devices when applied to active matrix panels using thin film transistors generally have the following characteristics:
It is composed of an upper glass substrate, a lower thin film transistor substrate, and a liquid crystal sealed between them, and an external selection circuit selects the liquid crystal driving elements arranged in a matrix on the thin film transistor substrate, and selects the liquid crystal driving elements arranged in a matrix on the thin film transistor substrate. By applying a voltage to a liquid crystal drive electrode connected to a drive element, arbitrary characters, figures, or images are displayed. A general circuit diagram of the thin film transistor substrate is shown in FIG.
第1図aは薄膜トランジスタ基板上の液晶駆動
素子のマトリツクス状配置図である。図中の1で
囲まれた領域が表示領域であり、その中に液晶駆
動素子2がマトリツクス状に配置されている。3
は液晶駆動素子2へのデータ信号ラインであり、
4は液晶駆動素子2へのタイミング信号ラインで
ある。液晶駆動素子2の回路図を第1図bに示
す。5は薄膜トランジスタであり、データのスイ
ツチングを行なう。6はコンデンサであり、デー
タ信号の保持用として用いられる。このコンデン
サの容量としては、液晶自体の有する容量と故意
に設けたコンデンサの容量を含むが、場合によつ
ては液晶の容量のみで構成されることもある。7
は液晶パネルであり、7−1は各液晶駆動素子に
対応して形成された液晶駆動電極であり、7−2
は上側ガラスパネルである。 FIG. 1a is a diagram showing a matrix arrangement of liquid crystal driving elements on a thin film transistor substrate. The area surrounded by 1 in the figure is a display area, in which liquid crystal driving elements 2 are arranged in a matrix. 3
is a data signal line to the liquid crystal drive element 2,
4 is a timing signal line to the liquid crystal driving element 2; A circuit diagram of the liquid crystal driving element 2 is shown in FIG. 1b. A thin film transistor 5 performs data switching. 6 is a capacitor, which is used for holding data signals. The capacitance of this capacitor includes the capacitance of the liquid crystal itself and the capacitance of an intentionally provided capacitor, but in some cases, it may be composed only of the capacitance of the liquid crystal. 7
is a liquid crystal panel, 7-1 is a liquid crystal drive electrode formed corresponding to each liquid crystal drive element, and 7-2 is a liquid crystal drive electrode formed corresponding to each liquid crystal drive element.
is the upper glass panel.
以上の説明からわかるように、薄膜トランジス
タは、液晶に印加する電圧のデータをスイツチン
グするために用いられ、このとき薄膜トランジス
タに要求される特性は大きく次の2種類に分類さ
れる。 As can be seen from the above description, thin film transistors are used to switch voltage data applied to liquid crystals, and the characteristics required of thin film transistors at this time can be broadly classified into the following two types.
(1) 薄膜トランジスタをON状態にした時コンデ
ンサを充電させるために充分な電流を流すこと
ができること。(1) Sufficient current must be able to flow to charge the capacitor when the thin film transistor is turned on.
(2) 薄膜トランジスタをOFF状態にした時、極
力、電流が流れないこと。(2) When the thin film transistor is turned off, as little current as possible should flow.
(1)はコンデンサへのデータの書き込み特性に関
するものである。液晶の表示はコンデンサの電位
により決定されるため、短時間にデータを完璧に
書き込むことができるように、薄膜トランジスタ
は充分大きい電流を流すことができなくてはなら
ない。この時の電流(以下、ON電流という)は
コンデンサの容量と、書き込み時間とから定まり
そのON電流をクリアできるように薄膜トランジ
スタを製造しなくてはならない。薄膜トランジス
タの流すことができるON電流は、トランジスタ
のサイズ(チヤネル長とチヤネル幅)、構造、製
造プロセス、ゲート電圧、ドレイン電圧などに大
きく依存する。 (1) relates to the characteristics of writing data to the capacitor. Since the display of a liquid crystal is determined by the potential of a capacitor, thin film transistors must be able to flow a sufficiently large current so that data can be completely written in a short period of time. The current at this time (hereinafter referred to as ON current) is determined by the capacitance of the capacitor and the writing time, and thin film transistors must be manufactured to clear this ON current. The ON current that can flow through a thin film transistor greatly depends on the transistor's size (channel length and channel width), structure, manufacturing process, gate voltage, drain voltage, etc.
(2)は、コンデンサに書き込まれたデータの保持
特性に関するものである。一般に、書き込まれた
データは書き込み時間よりもはるかに長い時間保
持されなくてはならない。コンデンサの容量は、
通常1pF程度の小さい値であるため、薄膜トラン
ジスタがOFF状態の時にわずかでもリーク電流
(以下、OFF電流という)が流れると、ドレイン
の電位(すなわち、コンデンサの電位)は急激に
ソースの電位に近づき、書き込まれたデータは正
しく保持されなくなつてしまう。したがつて、
OFF電流はできる限り、小さくしなくてはなら
ない。OFF電流の機構については、本発明の主
旨に関係するため、後に詳しく述べる。 (2) relates to the retention characteristics of data written to the capacitor. Generally, written data must be retained for a much longer time than the write time. The capacitance of the capacitor is
Since it is usually a small value of about 1 pF, if even a small amount of leakage current (hereinafter referred to as OFF current) flows when the thin film transistor is in the OFF state, the drain potential (that is, the capacitor potential) will rapidly approach the source potential. The written data will no longer be retained correctly. Therefore,
The OFF current must be kept as small as possible. The mechanism of the OFF current will be described in detail later because it is related to the gist of the present invention.
以上述べた内容からわかるように、薄膜トラン
ジスタのOFF電流を低減させることは、非常に
重要な意義を有する。チヤネル長を小さく、チヤ
ネル幅を大きくして充分なON電流を得ようとす
るとOFF電流も増加し、データの保持特性を悪
化させるためである。したがつて、OFF電流を
減少せしめることは、薄膜トランジスタの特性改
善において急務となつている。このことは薄膜ト
ランジスタをアクテイブマトリツクスパネル以外
の用途に応用する場合にも全く同様である。例え
ば、薄膜トランジスタを用いて、通常のロジツク
回路を構成する場合には静止電流が増加し、また
メモリやイメージセンサを構成する場合には誤動
作の原因となる。 As can be seen from the above description, reducing the OFF current of a thin film transistor has very important significance. This is because if an attempt is made to obtain a sufficient ON current by decreasing the channel length and increasing the channel width, the OFF current will also increase, which will deteriorate data retention characteristics. Therefore, reducing the OFF current is an urgent need for improving the characteristics of thin film transistors. This is exactly the same when thin film transistors are applied to uses other than active matrix panels. For example, when a normal logic circuit is constructed using thin film transistors, static current increases, and when a memory or an image sensor is constructed, it causes malfunction.
本発明は、このような従来の薄膜トランジスタ
の欠点を除去するものであり、その目的とすると
ころは、OFF電流を低減させる構造を有する薄
膜トランジスタを提供することである。以下、
OFF電流の機構について詳しく述べた後、それ
に基づいて本発明の内容を説明する。 The present invention aims to eliminate such drawbacks of conventional thin film transistors, and an object thereof is to provide a thin film transistor having a structure that reduces OFF current. below,
After describing the mechanism of the OFF current in detail, the content of the present invention will be explained based thereon.
第2図は半導体薄膜を用いたNチヤネル薄膜ト
ランジスタの一般的な構造を示す断面図である。
8はガラス、石英などの絶縁性透明基板、9は多
結晶シリコンなどの半導体薄膜、10は半導体薄
膜中にリンやヒ素などの不純物をドープして形成
したソース領域、11は同じくドレイン領域、1
2はゲート膜、13はゲート電極、14は層間絶
縁膜、15はソース電極、16はドレイン電極で
ある。この構造を有する薄膜トランジスタの代表
的な特性を第3図及び第4図に示す。 FIG. 2 is a cross-sectional view showing the general structure of an N-channel thin film transistor using a semiconductor thin film.
8 is an insulating transparent substrate such as glass or quartz; 9 is a semiconductor thin film such as polycrystalline silicon; 10 is a source region formed by doping impurities such as phosphorus or arsenic into the semiconductor thin film; 11 is a drain region;
2 is a gate film, 13 is a gate electrode, 14 is an interlayer insulating film, 15 is a source electrode, and 16 is a drain electrode. Typical characteristics of a thin film transistor having this structure are shown in FIGS. 3 and 4.
第3図はチヤネル長L=20μm、チヤネル幅W
=10μmのサイズを有する薄膜トランジスタの特
性を示すグラフである。なお、このデータは本出
願人が実験を行なつて得られた結果である。この
グラフの横軸はソースに対するゲート電圧VGSで
あり、縦軸はドレイン電流IDである。パラメータ
はソースに対するドレイン電圧VDSであり、Aの
曲線がVDS=1Vに、Bの曲線がVDS=4Vに、Cの
曲線がVDS=8Vにそれぞれ対応する。これよりわ
かるように、ドレイン電流IDはVGS=0V近傍で最
小値を取り、VGSの絶対値が増加するにつれてド
レイン電流IDは増加する。VGSが正の領域でドレ
イン電流が増加することは、トランジスタが
OFF状態からON状態へ変化することを意味する
ものであり、電流の増加率はできる限り大きいこ
とが望ましい。一方、VGSが負の領域でドレイン
電流が増加することは、OFF電流がゲート電圧
依存性を有することを意味するものでありトラン
ジスタの特性としては望ましくない。またドレイ
ン電流はドレイン電圧VDSにより大きく変化す
る。特にVGSが負の領域におけるドレイン電流、
すなわちOFF電流は、ON電流以上にドレイン電
圧依存性が大きい。 Figure 3 shows channel length L = 20 μm and channel width W.
1 is a graph showing the characteristics of a thin film transistor having a size of =10 μm. Note that this data is the result obtained through experiments conducted by the applicant. The horizontal axis of this graph is the gate voltage V GS with respect to the source, and the vertical axis is the drain current ID . The parameter is the drain voltage V DS to the source, and the curve A corresponds to V DS =1V, the curve B corresponds to V DS =4V, and the curve C corresponds to V DS =8V. As can be seen from this, the drain current ID takes a minimum value near V GS =0V, and increases as the absolute value of V GS increases. The increase in drain current in the positive V GS region means that the transistor
This means changing from an OFF state to an ON state, and it is desirable that the rate of increase in current is as large as possible. On the other hand, an increase in drain current in a negative V GS region means that the OFF current has gate voltage dependence, which is not desirable as a transistor characteristic. Furthermore, the drain current varies greatly depending on the drain voltage V DS . The drain current, especially in the region where V GS is negative,
That is, the OFF current has a greater drain voltage dependence than the ON current.
第4図はチヤネル幅W=10μmの薄膜トランジ
スタの特性のチヤネル長L依存性を示すグラフで
ある。なお、このデータも出願人が実験を行なつ
て得た結果である。ドレイン電圧はVDS=4Vで一
定であり、パラメータはチヤネル長Lである。D
の曲線がL=10μmに、Eの曲線がL=20μmに、
Fの曲線がL=40μmに、Gの曲線がL=100μm
にそれぞれ対応する。これよりわかるように、
VGSが正の領域ではドレイン電流IDはチヤネル長
Lに反比例し、通常の金属絶縁膜半導体構造電界
効果トランジスタ(MOS FET)の理論と一致
する。しかし、VGSが負の領域では、VGSの絶対
値が大きくなるにつれて、チヤネル長Lの依存性
は小さくなり、ついにはLの依存性が全く無くな
る。すなわち、VGSが約−8V以下のときには、い
かなるLに対してもOFF電流は一定になる。 FIG. 4 is a graph showing the dependence of the characteristics of a thin film transistor with a channel width W=10 μm on the channel length L. Note that this data is also the result of experiments conducted by the applicant. The drain voltage is constant at V DS =4V, and the parameter is the channel length L. D
The curve of E is L = 10 μm, the curve of E is L = 20 μm,
The F curve is L = 40μm, and the G curve is L = 100μm.
correspond to each. As you can see from this,
In the region where V GS is positive, the drain current I D is inversely proportional to the channel length L, which is consistent with the theory of ordinary metal-insulating-film-semiconductor field-effect transistors (MOS FETs). However, in a region where V GS is negative, as the absolute value of V GS increases, the dependence on the channel length L becomes smaller, and finally the dependence on L disappears altogether. That is, when V GS is about -8V or less, the OFF current is constant for any L.
第3図及び第4図に示したデータより、OFF
電流は次のような機構によるものと考えられる。
すなわち、VGS=0VにおけるOFF電流は半導体薄
膜の固有抵抗により決定されるが、VGSを負にバ
イアスした時のOFF電流は、半導体薄膜の表面
に誘起されるP型層と、ソース領域及びドレイン
領域のN型層との間に形成されるPN接合を流れ
る電流により規定される。一般に、半導体薄膜中
には多くのトラツプが存在するため、このPN接
合は不完全であり、したがつて接合リーク電流が
流れやすい。ゲート電圧を負にバイアスするほど
OFF電流が増加するのは、半導体薄膜の表面に
形成されるP型層のキヤリア濃度が増加して、
PN接合のエネルギー障壁の幅が狭くなるため、
電界の集中が起こり、接合リーク電流が増加する
ことによるものである。また、OFF電流のドレ
イン電圧依存性も、同様の理由によるものであ
る。またOFF電流のチヤネル長依存性も、接合
リーク電流により説明できる。すなわち、VGSを
負にバイアスするにつれて、OFF電流はドレイ
ン近傍の接合リーク電流に支配され、半導体薄膜
の固有抵抗により流れる電流は無視できるように
なるためである。 From the data shown in Figures 3 and 4, OFF
The current is thought to be generated by the following mechanism.
In other words, the OFF current at V GS = 0V is determined by the specific resistance of the semiconductor thin film, but the OFF current when V GS is negatively biased is determined by the P-type layer induced on the surface of the semiconductor thin film, the source region and It is defined by the current flowing through the PN junction formed between the drain region and the N-type layer. Generally, since there are many traps in a semiconductor thin film, this PN junction is incomplete, and therefore junction leakage current easily flows. The more negative the gate voltage is biased
The OFF current increases because the carrier concentration of the P-type layer formed on the surface of the semiconductor thin film increases.
Because the width of the energy barrier of the PN junction becomes narrower,
This is because electric field concentration occurs and junction leakage current increases. Furthermore, the drain voltage dependence of the OFF current is also due to the same reason. The channel length dependence of the OFF current can also be explained by the junction leakage current. That is, as V GS is biased more negatively, the OFF current is dominated by the junction leakage current near the drain, and the current flowing due to the resistivity of the semiconductor thin film becomes negligible.
OFF電流の機構は上述した通りのものである
が実際にOFF電流を低減させるための有効な手
段は従来、あまり取られていなかつた。特に、ゲ
ート電圧を負にバイアスした時のOFF電流を低
減させるためには、接合リーク電流を低減させな
くてはならないため、その努力はほとんど払われ
ていなかつた。 Although the mechanism of the OFF current is as described above, few effective measures have been taken to actually reduce the OFF current. In particular, in order to reduce the OFF current when the gate voltage is negatively biased, it is necessary to reduce the junction leakage current, so little effort has been made to this end.
本発明はこのようなOFF電流のゲート電圧依
存性を低減させ、VGSを負の値に増加させても
OFF電流がほとんど増加しない特性を有する画
期的な薄膜トランジスタを提供するものである。
これを実現するために本発明では、半導体薄膜を
用いソース電極とドレイン電極とゲート電極を備
えた薄膜トランジスタにおいて、複数個の前記薄
膜トランジスタを直列に接続し、その両端の電極
をソース電極及びドレイン電極とすると共に、前
記複数個の薄膜トランジスタのゲート電極をすべ
て共通にしたことを特徴とする薄膜トランジスタ
を提供する。以下、図を参照して本発明を詳しく
説明する。 The present invention reduces such dependence of OFF current on gate voltage, and even when V GS increases to a negative value,
The present invention provides an epoch-making thin film transistor having a characteristic that OFF current hardly increases.
In order to achieve this, in the present invention, in a thin film transistor using a semiconductor thin film and having a source electrode, a drain electrode, and a gate electrode, a plurality of the thin film transistors are connected in series, and the electrodes at both ends are connected to the source electrode and the drain electrode. In addition, the present invention provides a thin film transistor characterized in that the plurality of thin film transistors all have a common gate electrode. Hereinafter, the present invention will be explained in detail with reference to the drawings.
第5図は、本発明の回路図を示すものである。
Sはソースを、Dはドレインを、Gはゲートを示
している。またNは直列に接続する薄膜トランジ
スタの個数を表わしている。図からわかるように
N個の薄膜トランジスタを直列に接続し両端の電
極の一方をソースに、他方をドレインとする。ま
た、N個の薄膜トランジスタのゲートはすべて共
通にして、1つのゲートとする。本発明の主旨
は、このように構成された複数個の薄膜トランジ
スタを単一の薄膜トランジスタとして取り扱うこ
とにある。このように構成された薄膜トランジス
タは非常に優れたOFF特性を有する。その理由
は、第6図を参照して説明する。 FIG. 5 shows a circuit diagram of the present invention.
S indicates a source, D indicates a drain, and G indicates a gate. Further, N represents the number of thin film transistors connected in series. As can be seen from the figure, N thin film transistors are connected in series, with one electrode at both ends serving as a source and the other as a drain. Further, the gates of all the N thin film transistors are made common to one gate. The gist of the present invention is to treat a plurality of thin film transistors configured in this manner as a single thin film transistor. The thin film transistor configured in this manner has extremely excellent OFF characteristics. The reason for this will be explained with reference to FIG.
第6図aは、第5図においてN=2とした場合
の回路図である。簡単のため、N=2の場合を例
にとつて本発明を説明する。図中、S,D,Gの
意味する内容は第5図と同じである。S,D,
G,Xにおける電位をそれぞれVS,VD,VG,VX
とする。また、図中の番号は、2つの薄膜トラン
ジスタにつけられた番号であり、それぞれのトラ
ンジスタのチヤネル長をL1,L2とする。また、
第6図bは、aのトランジスタを等価的に1つの
トランジスタに置きかえたものであり、そのチヤ
ネル長はL1+L2である。トランジスタ1のドレ
イン電圧VDS1、ゲート電圧VGS1及びトランジスタ
2のドレイン電圧VDS2,ゲート電圧VGS2は次式で
与えられる。 FIG. 6a is a circuit diagram when N=2 in FIG. 5. For the sake of simplicity, the present invention will be described using the case where N=2 as an example. In the figure, the meanings of S, D, and G are the same as in FIG. 5. S, D,
The potentials at G and X are respectively V S , V D , V G , V X
shall be. Further, the numbers in the figure are numbers assigned to two thin film transistors, and the channel lengths of the respective transistors are assumed to be L 1 and L 2 . Also,
In FIG. 6b, the transistor in a is equivalently replaced with one transistor, and its channel length is L 1 +L 2 . The drain voltage V DS1 and gate voltage V GS1 of transistor 1 and the drain voltage V DS2 and gate voltage V GS2 of transistor 2 are given by the following equations.
VDS1=VX−VS
VGS1=VG−VS
VDS2=VD−VX
VGS2=VG−VX
トランジスタ1を流れる電流I1とトランジスタ
2を流れる電流I2が等しくなるように点Xの電位
VXが定まる。このとき、VS<VX<VDが成立し、
したがつてドレイン電圧VD−VSは2つのトラン
ジスタに分割して印加されることになる。このた
めドレイン電流は減少するはずであるが、ドレイ
ン電流とチヤネル長との間に一定の関係が成立す
る場合には、第6図bに比べてチヤネル長が短い
分だけドレイン電流は増加し、結局、第6図aの
トランジスタと、第6図bのトランジスタとでは
電流値は等しくなる。実際、VG−VS>0の場合
には、この関係が成立し、ON電流は変化しな
い。すなわち、チヤネル長をどのように分割して
も電流値は変わらない。V DS1 = V X −V S V GS1 = V G −V S V DS2 = V D −V X V GS2 = V G −V The potential at point X as
V X is determined. At this time, V S < V X < V D holds, and
Therefore, the drain voltage V D -V S is divided and applied to the two transistors. Therefore, the drain current should decrease, but if a certain relationship holds between the drain current and the channel length, the drain current will increase by the amount of the shorter channel length compared to FIG. 6b, In the end, the current values of the transistor shown in FIG. 6a and the transistor shown in FIG. 6b become equal. In fact, when V G −V S >0, this relationship holds true and the ON current does not change. In other words, the current value does not change no matter how the channel length is divided.
しかし、VG−VS<0の場合には状況が異なる。
これは、第4図に示したように、ゲート電圧を負
にバイアスした場合、ドレイン電流のチヤネル長
依存性がなくなつてくることに起因する。すなわ
ち、ゲート電圧を負の方向に大きくしていくと、
OFF電流はチヤネル長に依存しなくなつてくる
ため、第6図aとbとでチヤネル長の違いによる
効果はなのなつてくる。したがつて、個々のトラ
ンジスタに加わるドレイン電圧が低下する分だ
け、aではOFF電流が減少する。この効果は、
ゲート電圧を負にバイアスするほど顕著になる。 However, the situation is different when V G −V S <0.
This is because, as shown in FIG. 4, when the gate voltage is negatively biased, the dependence of the drain current on the channel length disappears. In other words, as the gate voltage increases in the negative direction,
Since the OFF current becomes independent of the channel length, the effect of the difference in channel length between Figure 6 a and b becomes smaller. Therefore, the OFF current in a decreases by the amount that the drain voltage applied to each transistor decreases. This effect is
The more negative the gate voltage is biased, the more pronounced this becomes.
また、以上の現象は、物性的に次のようにも説
明される。トランジスタがONの状態では、半導
体薄膜の表面にはチヤネルが形成されるため、ソ
ースからドレインに向けて、ほぼ均一な電位勾配
(電界)が生じているために、どのようにチヤネ
ルを分割してもドレイン電流は変化しない。一方
トランジスタがOFFの状態では、前述の通り、
ドレイン近傍のPN接合にほとんどの電界が集中
しているため、トランジスタを分割することによ
り個々のPN接合に加わる電界集中を弱めること
ができ、接合リーク電流、すなわちOFF電流を
減少させることができる。 The above phenomenon can also be explained in terms of physical properties as follows. When a transistor is on, a channel is formed on the surface of the semiconductor thin film, and a nearly uniform potential gradient (electric field) is generated from the source to the drain. However, the drain current remains unchanged. On the other hand, when the transistor is off, as mentioned above,
Most of the electric field is concentrated in the PN junction near the drain, so dividing the transistor can weaken the concentration of electric field applied to each individual PN junction, reducing junction leakage current, or OFF current.
次に、実験データを示して、本発明の効果を実
証する。 Next, experimental data will be shown to demonstrate the effects of the present invention.
第7図は、本発明による薄膜トランジスタの特
性を示すグラフである。第6図aにおいてL1=
L2=10μm、W1=W2=10μmとした場合のトラン
ジスタ特性である。このトランジスタは等価的に
第3図に示したトランジスタに等しいものであ
る。なお、このデータも本出願人が実験を行なつ
て得られた結果である。パラメータはドレイン電
圧であり、Hの曲線がVDS=1Vに、Iの曲線が
VDS=4Vに、Jの曲線がVDS=8Vにそれぞれ対応
している。このグラフからわかるように、VGSが
正の領域、すなわちON電流は第3図のデータと
ほとんど一致するが、VGSが負の領域、すなわち
OFF電流は、第3図と大幅に異なり、低い値で
ほぼ一定の値をとつている。すなわち、従来の薄
膜トランジスタと同じON電流を保ちつつ、OFF
電流を大幅に低減させている。また、本出願人は
従来のトランジスタ特性をもとにしてコンピユー
タシミユレーシヨンを行ない、本発明による薄膜
トランジスタのOFF特性を計算してみたが、そ
の結果は第7図のグラフと非常によく一致した。 FIG. 7 is a graph showing the characteristics of the thin film transistor according to the present invention. In Figure 6a, L 1 =
These are transistor characteristics when L 2 =10 μm and W 1 =W 2 =10 μm. This transistor is equivalently the transistor shown in FIG. Note that this data is also the result obtained through experiments conducted by the applicant. The parameter is the drain voltage, the H curve is V DS = 1V, the I curve is
The curve J corresponds to V DS = 4V, and the curve J corresponds to V DS = 8V. As can be seen from this graph, the region where V GS is positive, that is, the ON current, almost matches the data in Figure 3, but the region where V GS is negative, that is, the ON current almost matches the data in Figure 3.
The OFF current is significantly different from Fig. 3, and is a low and almost constant value. In other words, while maintaining the same ON current as conventional thin film transistors,
The current is significantly reduced. In addition, the applicant performed computer simulation based on conventional transistor characteristics and calculated the OFF characteristics of the thin film transistor according to the present invention, and the results agreed very well with the graph in Figure 7. did.
以上の説明では簡単のため、N=2の場合、す
なわち2つの薄膜トランジスタを直列に接続した
場合について述べたが、3つ以上の場合にも全く
同様の説明をすることができる。直列に接続する
薄膜トランジスタの個数を増加させると、ドレイ
ン電圧が高い場合のOFF電流の改善が顕著にな
つてくる。これは、トランジスタの数が多いほど
個々のトランジスタに印加されるドレイン電圧が
減少するためである。したがつて、薄膜トランジ
スタの用途と、要求されるOFF電流のレベルに
よつて、その個数Nを選択すればよい。アクテイ
ブマトリツクスパネルに応用する場合には、通
常、ドレイン電圧が低いため(約10V以下)、N
=2〜3で充分である。薄膜トランジスタでロジ
ツク回路を構成する場合には、通常、充分なON
電流を得るために高いゲート電圧を印加するが、
ドレイン電圧もそれとほぼ同等の高い値になるた
めNの値は大きくした方がOFF電流の低減には
効果がある。 In the above explanation, for the sake of simplicity, the case where N=2, that is, the case where two thin film transistors are connected in series, has been described, but the same explanation can be given to the case where three or more thin film transistors are connected. When the number of thin film transistors connected in series is increased, the improvement in the OFF current when the drain voltage is high becomes noticeable. This is because the drain voltage applied to each transistor decreases as the number of transistors increases. Therefore, the number N may be selected depending on the purpose of the thin film transistor and the level of required OFF current. When applied to active matrix panels, the drain voltage is usually low (about 10 V or less), so N
=2 to 3 is sufficient. When configuring a logic circuit with thin film transistors, there is usually sufficient ON
Applying a high gate voltage to obtain current,
Since the drain voltage is also almost as high as that, increasing the value of N is more effective in reducing the OFF current.
以上述べたように、本願発明は前述ような構成
をとることにより、オン電流の減少を抑えつつ、
オフ電流を大幅に減少させる。 As described above, by adopting the above-mentioned configuration, the present invention suppresses a decrease in on-current, and
Significantly reduces off-state current.
第1図は薄膜トランジスタをアクテイブマトリ
ツクスパネルに応用した場合の一般的な回路図で
ある。第2図は半導体薄膜を用いたNチヤネル薄
膜トランジスタの一般的な構造を示す断面図であ
る。第3図及び第4図は、従来の薄膜トランジス
タの特性を示すグラフである。第5図は本発明の
一般的な構成を示す回路図である。第6図は本発
明の一例として、2個の薄膜トランジスタを直列
に接続した場合の回路図と、それに等価な単一の
薄膜トランジスタを示すものである。第7図は、
第6図に示した本発明による薄膜トランジスタの
特性を示すグラフである。
FIG. 1 is a general circuit diagram when thin film transistors are applied to an active matrix panel. FIG. 2 is a sectional view showing the general structure of an N-channel thin film transistor using a semiconductor thin film. FIGS. 3 and 4 are graphs showing the characteristics of conventional thin film transistors. FIG. 5 is a circuit diagram showing the general configuration of the present invention. FIG. 6 shows, as an example of the present invention, a circuit diagram in which two thin film transistors are connected in series and a single thin film transistor equivalent thereto. Figure 7 shows
7 is a graph showing the characteristics of the thin film transistor according to the present invention shown in FIG. 6.
Claims (1)
素電極を有し、該画素電極には薄膜トランジスタ
が接続されてなり、一画素内にはN(N≧2)個
の薄膜トランジスタが形成され、該N個の薄膜ト
ランジスタは直列接続され、該直列接続された薄
膜トランジスタの一端は映像信号線に電気的に接
続され、もう一端は画素電極に電気的に接続さ
れ、該直列接続された薄膜トランジスタのゲート
電極は共通化されることを特徴とする薄膜トラン
ジスタ。1 It has a plurality of pixel electrodes arranged in a matrix on a substrate, thin film transistors are connected to the pixel electrodes, N (N≧2) thin film transistors are formed in one pixel, and the N The thin film transistors connected in series are connected in series, one end of the series connected thin film transistors is electrically connected to a video signal line, the other end is electrically connected to a pixel electrode, and the gate electrodes of the series connected thin film transistors are common. A thin film transistor characterized by being
Priority Applications (6)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5433682A JPS58171860A (en) | 1982-04-01 | 1982-04-01 | Thin film transistor |
FR8304924A FR2524714B1 (en) | 1982-04-01 | 1983-03-25 | THIN FILM TRANSISTOR |
GB08308614A GB2117970B (en) | 1982-04-01 | 1983-03-29 | Thin film transistor integrated circuit |
US06/481,087 US4623908A (en) | 1982-04-01 | 1983-03-31 | Thin film transistors |
DE19833311923 DE3311923A1 (en) | 1982-04-01 | 1983-03-31 | THIN FILM TRANSISTOR ARRANGEMENT |
FR8310563A FR2547955B2 (en) | 1982-04-01 | 1983-06-27 | THIN FILM TRANSISTOR |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5433682A JPS58171860A (en) | 1982-04-01 | 1982-04-01 | Thin film transistor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS58171860A JPS58171860A (en) | 1983-10-08 |
JPH0544195B2 true JPH0544195B2 (en) | 1993-07-05 |
Family
ID=12967756
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5433682A Granted JPS58171860A (en) | 1982-04-01 | 1982-04-01 | Thin film transistor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58171860A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE19605634B4 (en) * | 1995-02-15 | 2007-04-19 | Semiconductor Energy Laboratory Co., Ltd., Atsugi | Active matrix display |
DE19605669B4 (en) * | 1995-02-15 | 2007-06-14 | Semiconductor Energy Laboratory Co., Ltd., Atsugi | An active matrix display device |
US8248551B2 (en) | 1997-03-28 | 2012-08-21 | Semiconductor Energy Laboratory Co., Ltd. | Semiconductor device including capacitor line parallel to source line |
Families Citing this family (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH03108766A (en) * | 1989-09-22 | 1991-05-08 | Nippondenso Co Ltd | High breakdown strength transistor |
KR100292767B1 (en) * | 1992-09-25 | 2001-09-17 | 이데이 노부유끼 | LCD Display |
CN1161646C (en) | 1994-06-02 | 2004-08-11 | 株式会社半导体能源研究所 | Active array display device and electro-optic element |
JPH10154816A (en) | 1996-11-21 | 1998-06-09 | Semiconductor Energy Lab Co Ltd | Semiconductor device |
CN101009322B (en) * | 2001-11-09 | 2012-06-27 | 株式会社半导体能源研究所 | Light-emitting device |
JP2005223047A (en) | 2004-02-04 | 2005-08-18 | Casio Comput Co Ltd | Active matrix panel |
-
1982
- 1982-04-01 JP JP5433682A patent/JPS58171860A/en active Granted
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE19605634B4 (en) * | 1995-02-15 | 2007-04-19 | Semiconductor Energy Laboratory Co., Ltd., Atsugi | Active matrix display |
DE19605669B4 (en) * | 1995-02-15 | 2007-06-14 | Semiconductor Energy Laboratory Co., Ltd., Atsugi | An active matrix display device |
DE19605670B4 (en) * | 1995-02-15 | 2007-06-28 | Semiconductor Energy Laboratory Co., Ltd., Atsugi | Active matrix display |
US8248551B2 (en) | 1997-03-28 | 2012-08-21 | Semiconductor Energy Laboratory Co., Ltd. | Semiconductor device including capacitor line parallel to source line |
US8531619B2 (en) | 1997-03-28 | 2013-09-10 | Semiconductor Energy Laboratory Co., Ltd. | Active matrix liquid crystal display device with overlapping conductive film and pixel electrode |
Also Published As
Publication number | Publication date |
---|---|
JPS58171860A (en) | 1983-10-08 |
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