JPS5848454A - Close contact type image sensor - Google Patents

Close contact type image sensor

Info

Publication number
JPS5848454A
JPS5848454A JP56145470A JP14547081A JPS5848454A JP S5848454 A JPS5848454 A JP S5848454A JP 56145470 A JP56145470 A JP 56145470A JP 14547081 A JP14547081 A JP 14547081A JP S5848454 A JPS5848454 A JP S5848454A
Authority
JP
Japan
Prior art keywords
thin film
image sensor
resistor
metal layer
length
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
JP56145470A
Other languages
Japanese (ja)
Other versions
JPS6048908B2 (en
Inventor
Masuji Sato
佐藤 万寿治
Fumiaki Yamada
文明 山田
Toshiaki Naka
中 敏明
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 JP56145470A priority Critical patent/JPS6048908B2/en
Publication of JPS5848454A publication Critical patent/JPS5848454A/en
Publication of JPS6048908B2 publication Critical patent/JPS6048908B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/08Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Electromagnetism (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Computer Hardware Design (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Solid State Image Pick-Up Elements (AREA)

Abstract

PURPOSE:To improve the frequency characteristics and the noise-resisting property of the titled image sensor by a method wherein, in a manuscript reading device such as a facsimile transmitting device, a copying device or the like, the resistance value of a light conductive film is reduced by having the width of the light conductive film coincided with the length in auxiliary scanning direction of longer bit area length. CONSTITUTION:When an image sensor is manufactured, microscopic patterns of thin film resistors or thin film metal layers of 4-1, 4-2, and 5-1-5-4 are formed. To be more precise, these thin film resistor or thin film layer patterns are formed by lifting-off NiCr, Cr-SiO, Al-Cu and the like having the thickness of 100nm or below. The resistor pattern as shown in the diagram can be formed easily if the material to be used sufficiently thin in thickness. Besides, the metal electrodes, to be used for lead wire, 1-1', 1-2', 2-1'-2-4' which will be connected to the resistor or thin film metal layer pattern is formed by NiCr-Au, Au, Al, Al-Cu and the like of 3,000Angstrom or more in thickness, and the resistance value of which is very small when compared with that of the thin film resistor or the thin film metal layer.

Description

【発明の詳細な説明】 本発明はファクタより送信装置、複写装置郷の原稿読取
装置用の密着形イメージセンサに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a contact type image sensor for a transmitting device and a document reading device of a copying device.

最近、ファクシミリ送信装置、複写装置等における原稿
読取は、けい光灯等の光源で原稿を照射し、この反射光
を、多数の°レンズが直線方向(以下、主走査方向とし
1、この方向に垂直な方向−を−Jj走査方向とする)
に配列された導光部を介して、前記各レンズにほぼ密着
して設けられた光電変換素子を有する受光部に導くこと
によって行われる。
Recently, in order to read originals in facsimile transmitters, copying machines, etc., the original is illuminated with a light source such as a fluorescent lamp, and a number of lenses are used to direct this reflected light in a straight direction (hereinafter referred to as the main scanning direction). (vertical direction - is set as -Jj scanning direction)
This is carried out by guiding the light to a light receiving section having a photoelectric conversion element provided in close contact with each of the lenses through light guide sections arranged in a row.

これにより、原稿の1ピツチが1対1すなわち縮小され
ることなく光電的に読込まれるととになる。
As a result, one pitch of the original is read photoelectrically on a one-to-one basis, that is, without being reduced.

このような光電変換素子を主走査方向に配列した受光部
は密着形あ゛るいは大形イメージセンサと呼ばれている
。   ”・ 従来の密着形イメージセンサによれば、主走査方向に配
置された各ビットエリアにおいて、副走査方向の両端に
第1の電極(共通側電極)と第2の電極(個別的電極)
を設け、この2つの電極間に光導電膜を設けである。し
かしながら、一般的には、各ビットエリアにあっては、
主走査方向(横方向)の長さが副走査方向(縦方向)の
長さより小さいという事実があり、シかも各ビ、ドエリ
ア間にはアイソレージ、ンギャップを設けなければなら
ないので、光導電膜の幅はビットエリアの主走査方向の
長さよりもさらに小さくなり、従って、光導電膜の抵抗
値が比較的大きくなり、この結果、イメージセンサの周
波数特性(高速イ()が低下し、また、耐雑音性(S/
N比)が低くなる5という問題点があった。
A light receiving section in which such photoelectric conversion elements are arranged in the main scanning direction is called a contact type or large-sized image sensor. ”- According to a conventional contact image sensor, in each bit area arranged in the main scanning direction, a first electrode (common side electrode) and a second electrode (individual electrode) are placed at both ends in the sub-scanning direction.
A photoconductive film is provided between these two electrodes. However, in general, in each bit area,
Due to the fact that the length in the main scanning direction (horizontal direction) is smaller than the length in the sub-scanning direction (vertical direction), it is necessary to provide an isolation gap between each vibrator and door area. The width becomes even smaller than the length of the bit area in the main scanning direction, and therefore the resistance value of the photoconductive film becomes relatively large. Noise (S/
There was a problem that the N ratio) was low.

本発明の目的は、各ビットエリアにおいて、主走査方向
の両端に第1.第2の電極を薄膜抵抗体として形成し、
これら2つの電極間に光導電膜を形成するという構想に
もとづき、光導電膜の幅をビットエリアの長残副走査方
向の長さに一致せ1めて光導電膜の抵抗値を低竺させ、
これによ、9、イメージセンサの周波数特性および耐雑
音性を向上せしめ、前述の従来形における問題点4を解
決することにある。
An object of the present invention is to provide first . forming the second electrode as a thin film resistor;
Based on the concept of forming a photoconductive film between these two electrodes, the width of the photoconductive film is made to match the length of the bit area in the long remaining sub-scanning direction, thereby reducing the resistance value of the photoconductive film. ,
Thereby, 9. The purpose is to improve the frequency characteristics and noise resistance of the image sensor, and to solve problem 4 in the conventional type described above.

以下、図面により本発明を従来形と比較して説明する。Hereinafter, the present invention will be explained with reference to the drawings in comparison with a conventional type.

第1図は′従来の密着形イメージセンサの平面図である
。第1図において、A1−A4は主走査方向Xに配列さ
れたピットエリアであって、通常、その主走査方向Xの
長さLxは副走査方向の長さLYより小さい。たとえば
、ム4°判(216−幅)で1726ピツトの場合にB
 s Lz ” 125 #+ Ly =130μであ
る。1〜1〜1−4.2−1〜2−4はNlCr7Au
のような金属電極であって、電極1−1〜1−4は共通
側電極、他方、電極2−1〜2−4は個別的電極と呼ば
れる。3−1〜3−4は光導電膜であって、その幅Wは
ビットエリアの主走査方向Xの長さしxよりアイソレー
ジ、ンギャップ長し、だけ小さい。すなわち、 W == Lx−Lg であり、たとえば、アイソレージ、ンギャップ長Llr
を最小−幅の25μとすれば、W=125−25=10
0tenである。他方、光導電膜の長さしをビ、トエリ
アの副走査方向Yの長さLYの1/2とすれは、L=L
Y/2=65μであり、この場合、光電変換面積(1ビ
ツト当9)は100In′IL×651rrrLであり
、各光導電膜の抵抗値に比例する値しWは065と大き
くなる。このように、光導電膜の幅Wはビットエリアの
主走査方向長さLxよリアイソレージ、ンギャップ長り
2分だけ小さくなり、光導電膜の抵抗値は比較的大きく
なる。
FIG. 1 is a plan view of a conventional contact type image sensor. In FIG. 1, A1-A4 are pit areas arranged in the main scanning direction X, and the length Lx in the main scanning direction is usually smaller than the length LY in the sub-scanning direction. For example, if the size is 4° (216-width) and the pitch is 1726,
s Lz ” 125 #+Ly = 130 μ. 1 to 1 to 1-4. 2-1 to 2-4 are NlCr7Au
The electrodes 1-1 to 1-4 are called common electrodes, and the electrodes 2-1 to 2-4 are called individual electrodes. 3-1 to 3-4 are photoconductive films, the width W of which is smaller than the length x of the bit area in the main scanning direction X by the isolation gap length. That is, W == Lx - Lg, for example, isolation, gap length Llr
If the minimum width is 25μ, then W=125-25=10
It is 0ten. On the other hand, if the length of the photoconductive film is set to 1/2 of the length LY of the bit area in the sub-scanning direction, then L=L.
Y/2=65μ, and in this case, the photoelectric conversion area (9 per bit) is 100In'IL×651rrrL, which is a value proportional to the resistance value of each photoconductive film, and W becomes as large as 065. In this way, the width W of the photoconductive film becomes smaller than the length Lx of the bit area in the main scanning direction by two times the rear isolation gap length, and the resistance value of the photoconductive film becomes relatively large.

第2図は本発明の一実施例としての密着形イメージセン
サの平面図である。嬉2図においては、たとえば、Nt
Cr、 Cr−810,、Cr−81等の薄膜抵抗体ま
たは微細パターン形成が容易な厚み100 nm以下の
薄膜金属層4−1.4−2および5−1〜5−4を各ビ
ットエリアA1〜A4の主走査方向の両端に配置し、こ
れらの薄膜抵抗体間に光導電膜3−1′〜3−4′を接
続して形成する。すなわち、光導電膜3−1′〜3−4
′は第1図の光導電膜3−1〜3−4と縦横の関係が逆
になっている。を九、金属電極1−1′および薄膜抵抗
体または薄膜金属層4−1はビットエリアA1 、A、
に共通であり、金属電極1−2′および薄膜抵抗体また
は薄膜金属層4−2はビットエリアA、、A4に共通で
ある。
FIG. 2 is a plan view of a contact type image sensor as an embodiment of the present invention. For example, Nt
A thin film resistor such as Cr, Cr-810, Cr-81 or a thin film metal layer 4-1, 4-2 and 5-1 to 5-4 with a thickness of 100 nm or less that is easy to form a fine pattern is placed in each bit area A1. -A4 are arranged at both ends in the main scanning direction, and photoconductive films 3-1' to 3-4' are connected between these thin film resistors. That is, photoconductive films 3-1' to 3-4
The photoconductive films 3-1 to 3-4 in FIG. 1 are reversed in terms of length and width. 9. The metal electrode 1-1' and the thin film resistor or thin film metal layer 4-1 are connected to the bit areas A1, A,
The metal electrode 1-2' and the thin film resistor or thin film metal layer 4-2 are common to the bit areas A, . . . A4.

すなわち、アイソレージ、/ギャップは2つのピ、トエ
リア毎にのみ設ければよい。また、薄膜抵抗体または薄
膜金属層5−1〜5−4は各金属電極2−1′〜2−4
′に接続されている。
That is, the isolation/gap need only be provided for every two pit areas. Moreover, the thin film resistor or thin film metal layer 5-1 to 5-4 is connected to each metal electrode 2-1' to 2-2.
'It is connected to the.

第2図に示すように1.光導電M3−1’〜3−4′の
幅W′はビットエリアの副走査方向長さLYに一致して
いる。すなわち、 w−LY(=t3o4)       □であり、他方
、光導電膜3−1′〜3−4′の長さL′は第1図の光
導電膜3−1〜3−4の長さLと同じであるとすれば、
L=L’=65μmであり、この場合・、光電費換面積
(1ピツト轟り)は130$×65μmと大きくなり、
また、各光導電膜3−1′〜3−4′の抵抗値に比例す
る値L7wも0.50と小さくなる。すなわち、光導電
膜3−1′〜3−4′の幅Wが大きくなった分、その抵
抗値は第1図の場合に比べて23チも小さくなる。
As shown in Figure 2, 1. The width W' of the photoconductors M3-1' to M3-4' matches the length LY of the bit area in the sub-scanning direction. That is, w-LY(=t3o4) □, and on the other hand, the length L' of the photoconductive films 3-1' to 3-4' is the length of the photoconductive films 3-1 to 3-4 in FIG. If it is the same as L,
L = L' = 65 μm, and in this case, the photoelectric conversion area (1 pit roar) is as large as 130 $ x 65 μm,
Further, the value L7w proportional to the resistance value of each photoconductive film 3-1' to 3-4' is also reduced to 0.50. That is, since the width W of the photoconductive films 3-1' to 3-4' is increased, the resistance value thereof becomes 23 inches smaller than that in the case of FIG.

第2図においては、最小線幅25tWnを薄膜抵抗体ま
たは薄膜金属層4−1.4−2.5−1 、・・・、5
−49最小幅Wに適用する。この場合、アイソレージ1
ンギヤツプ長Lgは4511yILとなり、第1図のア
イソレーションギヤ、f長Lgに比べて大幅に大匙くな
り、これは各ピット間の短絡防止に役立つものである。
In FIG. 2, the minimum line width of 25tWn is defined as the thin film resistor or thin film metal layer 4-1.4-2.5-1,...,5
-49 Applies to minimum width W. In this case, isolation 1
The gap length Lg is 4511yIL, which is significantly larger than the f length Lg of the isolation gear shown in FIG. 1, which is useful for preventing short circuits between the pits.

次に、第2図のイメージセンサを製造する場合、最小線
幅W1とする薄膜抵抗体または薄膜金属層4−1.4−
2.5−1〜5−4の微細/母ターンを形成する。すな
わち、この薄膜抵抗体または薄膜金属層ノ母ターンは厚
さ1100n以下のNiCr+ Cr−810゜Cr−
81,kl、 At−Cu等をリフトオフすることによ
って形成される。このように厚さが小さいと、第2図の
ような抵抗体14ターンは容易に形成することができる
。なお、この抵抗体または薄膜金属層ノ4ターンに接続
される引出線用金属電極1−1’ 。
Next, when manufacturing the image sensor shown in FIG. 2, the thin film resistor or thin film metal layer 4-1.4-
2. Form fine/major turns of 5-1 to 5-4. That is, the main turn of this thin film resistor or thin film metal layer is NiCr+ Cr-810°Cr- with a thickness of 1100 nm or less.
It is formed by lifting off 81,kl, At-Cu, etc. With such a small thickness, 14 turns of the resistor as shown in FIG. 2 can be easily formed. Incidentally, a metal electrode 1-1' for a lead wire is connected to this resistor or the fourth turn of the thin film metal layer.

1−2’ 、 2−1’〜2−4′線厚さ3000X以
上のNiCr−Au、 Au、 At、 Aj−Cu等
によって形成されており、その抵抗値は薄膜抵抗体また
は薄膜金属層の抵抗値に比べて著しく小さい。
1-2', 2-1' to 2-4' are made of NiCr-Au, Au, At, Aj-Cu, etc. with a line thickness of 3000X or more, and the resistance value is the same as that of the thin film resistor or thin film metal layer. It is significantly smaller than the resistance value.

次に、上述の薄膜抵抗体ノ譬ターンによる電位低下につ
いて考察する。たとえば、第2図のr、)エリアAIに
おいては、素子入力抵抗R,(Kα)は、ただし、Kα
=〆西Vち d K3=− R。
Next, the potential drop due to the above-mentioned thin film resistor analogy will be considered. For example, in area AI (r, ) in FIG. 2, the element input resistance R, (Kα) is, however, Kα
=〆West Vchid K3=-R.

−W/ R8=r1G Rp ” rp正 Rd= rd− W/ r、:光導電膜3−1′の明抵抗(Ω/口)rd:光導
電膜3−1′の暗抵抗(Ω/口)で表わせる゛。第3図
において、薄膜抵抗体または薄膜金輌層4−1.5−1
の抵抗値R,と光導電膜3−IIの明抵抗値R1との比
R,/R,を横軸に、(R,(Kα)−a、)、ipを
縦軸に示す。たとえば、R1/R,=10−  (1%
)のときには、R9に比して入力抵抗R,(K(1) 
O増加は1.15%、また、Rv/R。
-W/ R8=r1G Rp ” rpPositive Rd=rd- W/ r,: Bright resistance of photoconductive film 3-1' (Ω/port) rd: Dark resistance of photoconductive film 3-1' (Ω/port) ). In FIG. 3, the thin film resistor or thin film gold layer 4-1.5-1
The ratio R,/R, between the resistance value R, and the bright resistance value R1 of the photoconductive film 3-II is shown on the horizontal axis, and (R, (Kα)-a,), ip is shown on the vertical axis. For example, R1/R,=10- (1%
), the input resistance R, (K(1)
O increase is 1.15% and Rv/R.

=10”(10%)のときには、R9に比して入力抵抗
Ri(Kα)の増加は11.7%’である。また、第5
図において、R,/R,を横軸に、実効明暗抵抗比(R
d/R,)。および明状態における抵抗増加率を縦軸に
示す。第5図における直線AはR,=0のときにRd/
Rp= 10であり、直線BはR1=0のときRd/R
pm 15である。従って、引出線用金属電極1−1’
 、 2−1’による電位降下も考慮してR,/R。
= 10'' (10%), the increase in input resistance Ri (Kα) is 11.7%' compared to R9.
In the figure, the horizontal axis is R, /R, and the effective light-dark resistance ratio (R
d/R,). and the resistance increase rate in the bright state is shown on the vertical axis. The straight line A in Fig. 5 is Rd/ when R, = 0.
Rp=10, and the straight line B is Rd/R when R1=0
It's pm 15. Therefore, the metal electrode 1-1' for the lead wire
, R, /R considering the potential drop due to 2-1'.

を2×10−2以下にすれば、入力抵抗の増加、実効明
暗抵抗比の減少、および明状態における抵抗増加率を無
視することができる。その理由は、薄膜抵抗体または薄
膜金属層は上述の条件R,/R,< 2X 10”を満
足させることが可能であるからである。
If it is set to 2×10 −2 or less, the increase in input resistance, the decrease in the effective bright-dark resistance ratio, and the rate of increase in resistance in the bright state can be ignored. The reason is that a thin film resistor or a thin film metal layer can satisfy the above-mentioned condition R, /R, < 2X 10''.

以上説明したように本発明によれば、薄膜抵抗体または
薄膜金属層の微細/4ターンの容易性を利用して光導電
膜の抵抗値を低減させることができ、゛これによりイメ
ージセンナの周波数特性および耐雑音性を向上させるこ
とができる。
As explained above, according to the present invention, the resistance value of the photoconductive film can be reduced by utilizing the ease of fine/four turns of the thin film resistor or thin film metal layer. Characteristics and noise resistance can be improved.

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

第1図線従来の密着形イメージセンサの平面図1、第2
図は本発明の一実施例としての密着形イメージセンサの
平面図、第3図および第4図は本発明に係る密着形イメ
ージセンサの特性を示す図である。 1−1〜1−4 、1−1’ 、 1−2’ 、 2−
1〜2−4 、2−1’ 。 2−2’:金属電極、3−1〜3−4 、3−1’〜3
−4’:光導電膜、4−1 、4−2 :第1の薄膜紙
′抗体tたは薄膜金属層、5−1〜5−4:第2の薄膜
抵抗体また社薄膜金属層。 特許出願人 富士通株式会社 特許出願代理人 弁理士  青 木   朗 弁理士 西舘和之 弁理士  内 1)幸 男 弁理士  山 口 昭 之
Figure 1: Planar views of a conventional contact type image sensor 1 and 2
The figure is a plan view of a contact type image sensor as an embodiment of the present invention, and FIGS. 3 and 4 are diagrams showing characteristics of the contact type image sensor according to the present invention. 1-1 to 1-4, 1-1', 1-2', 2-
1-2-4, 2-1'. 2-2': metal electrode, 3-1 to 3-4, 3-1' to 3
-4': Photoconductive film, 4-1, 4-2: First thin film paper antibody or thin film metal layer, 5-1 to 5-4: Second thin film resistor or thin film metal layer. Patent applicant Fujitsu Limited Patent agent Akira Aoki Patent attorney Kazuyuki Nishidate Patent attorney 1) Yukio Patent attorney Akira Yamaguchi

Claims (1)

【特許請求の範囲】 1、複数のビットエリアを主走査方向に配列した密着形
イメージセンサにおいて、前記各vy )エリアの前記
主走査方向の両端に位置する第1゜第2の薄膜抵抗体ま
たは薄膜金属層と、該第1゜第2の薄膜抵抗体または薄
膜金属層に接続されて形成された光導電膜とを具備する
ことを特徴とする密着形イメージセンサ。 2、隣接する2つの前記ビットエリアの第1の薄膜抵抗
体または薄膜金属層を共通にした特許請求の範囲第1項
に記載の密着形イメージセンサ。
[Scope of Claims] 1. In a contact image sensor in which a plurality of bit areas are arranged in the main scanning direction, the first and second thin film resistors or A contact type image sensor comprising a thin film metal layer and a photoconductive film connected to the first and second thin film resistors or the thin film metal layer. 2. The contact type image sensor according to claim 1, wherein the first thin film resistor or thin film metal layer of two adjacent bit areas is shared.
JP56145470A 1981-09-17 1981-09-17 Close-contact image sensor Expired JPS6048908B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56145470A JPS6048908B2 (en) 1981-09-17 1981-09-17 Close-contact image sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56145470A JPS6048908B2 (en) 1981-09-17 1981-09-17 Close-contact image sensor

Publications (2)

Publication Number Publication Date
JPS5848454A true JPS5848454A (en) 1983-03-22
JPS6048908B2 JPS6048908B2 (en) 1985-10-30

Family

ID=15385981

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56145470A Expired JPS6048908B2 (en) 1981-09-17 1981-09-17 Close-contact image sensor

Country Status (1)

Country Link
JP (1) JPS6048908B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GR861797B (en) * 1985-07-09 1986-11-11 Agri Shield Inc Plant microbiocidal compound and method

Also Published As

Publication number Publication date
JPS6048908B2 (en) 1985-10-30

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