JPS6147031B2 - - Google Patents
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- Publication number
- JPS6147031B2 JPS6147031B2 JP53106472A JP10647278A JPS6147031B2 JP S6147031 B2 JPS6147031 B2 JP S6147031B2 JP 53106472 A JP53106472 A JP 53106472A JP 10647278 A JP10647278 A JP 10647278A JP S6147031 B2 JPS6147031 B2 JP S6147031B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- light receiving
- silicon
- electrode
- image sensor
- 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
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- Solid State Image Pick-Up Elements (AREA)
- Transforming Light Signals Into Electric Signals (AREA)
Description
【発明の詳細な説明】
本発明は、光電変換機能および電荷読出機能を
有するイメージセンサに関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an image sensor having a photoelectric conversion function and a charge readout function.
光学的読取装置等に用いられるイメージセンサ
には、従来第1図に示す如き構造を有するものが
知られている。同図に示すものは、受光部Aの蓄
積電荷を両縁のCCD(電荷転送装置)シフトレ
ジスタ部B1,B2に振り分けて読み出す所謂CCD
ラインセンサである。受光部A、シフトレジスタ
部B1,B2はそれぞれ図面と直交する方向に延
び、受光部Aは蛇行状チヤンネルカツトにより分
割された複数のMOS素子のアレーで線状の受光
面を形成し、またシフトレジスタ部B1,B2は共
通チヤンネルに沿つて配列された複数の基板と逆
型の埋め込み層を有するMOS素子のアレーで構
成されている。 2. Description of the Related Art Image sensors used in optical reading devices and the like are conventionally known to have a structure as shown in FIG. What is shown in the figure is a so-called CCD that distributes the accumulated charge in the light receiving section A to CCD (charge transfer device) shift register sections B 1 and B 2 on both sides and reads it out.
It is a line sensor. The light receiving section A and the shift register sections B 1 and B 2 each extend in a direction perpendicular to the drawing, and the light receiving section A forms a linear light receiving surface with an array of a plurality of MOS elements divided by meandering channel cuts. Furthermore, the shift register sections B 1 and B 2 are composed of a plurality of substrates arranged along a common channel and an array of MOS elements having an inverted buried layer.
上記イメージセンサの主体である受光部Aは、
例えばP型のシリコン(Si)基板1にN型の拡散
層2を形成してこれらの間にPN接合部Jを形成
し、さらに基板1の前記PN接合部上方にシリコ
ン酸化膜(SiO2)3を介して多結晶シリコンのホ
ンゲート電極4を設けこの電極4上もシリコン酸
化膜で覆つている。尚、酸化膜3中の51,52
はトランスフアゲート電極、61,62はシフト
レジスタ部の転送電極であり、また7は受光部A
以外への入射光を遮断するために、ホトゲート電
極4上方のみを除いて酸化膜3上を覆つた光シー
ルド電極であり、例えばアルミニウム(Al)膜
からなる。 The light receiving section A, which is the main body of the image sensor, is
For example, an N-type diffusion layer 2 is formed on a P-type silicon (Si) substrate 1, a PN junction J is formed between them, and a silicon oxide film (SiO 2 ) is further formed above the PN junction of the substrate 1. A Hong gate electrode 4 made of polycrystalline silicon is provided through the electrode 3, and this electrode 4 is also covered with a silicon oxide film. Note that 5 1 , 5 2 in the oxide film 3
is a transfer gate electrode, 6 1 and 6 2 are transfer electrodes of the shift register section, and 7 is a light receiving section A.
This is a light shield electrode that covers the oxide film 3 except for only the upper part of the photogate electrode 4 in order to block incident light to other parts, and is made of, for example, an aluminum (Al) film.
受光部Aは、ホトゲート電極4に電圧を加えて
その下部半導体基板に空乏層を作り、該空乏層に
該電極4上方からの入射光(光像)により発生す
る電荷を溜めるものであるが、ホトゲート電極4
が多結晶シリコンであるために、感度および波長
特性が悪いという欠点を有している。即ち、この
2000〜3000Åの厚みの多結晶シリコン膜は完全な
透明体ではなく、特に短い波長の光を通しにくい
という難点がある。 The light receiving section A applies a voltage to the photogate electrode 4 to create a depletion layer in its lower semiconductor substrate, and stores charges generated by incident light (light image) from above the electrode 4 in the depletion layer. Photogate electrode 4
Since it is made of polycrystalline silicon, it has the disadvantage of poor sensitivity and wavelength characteristics. That is, this
A polycrystalline silicon film with a thickness of 2,000 to 3,000 Å is not completely transparent, and has the disadvantage that it is particularly difficult for light of short wavelengths to pass through.
この点を改善するため、第1図の構成において
ホトゲート電極4を除去して前記PN接合部Jの
上方を酸化膜3のみで構成したイメージセンサが
考えられている。このセンサでは電荷蓄積に当つ
てトランスフアゲート51,52を開き、CCD
シフトレジスタ部の電極61,62に電圧を印加
し、該電圧で受光部AのN型拡散層2を空乏層化
する。即ち、電極61,62および51,52
に、本例ではNチヤンネル素子であるから正電圧
を加えると1aで示すN型領域は基板1より高電
位になる。またこの領域1aはN型拡散層2と連
通しているから該層2を不完全ながら空乏層化し
その電位を上げる。こうしてホトゲート電極4を
設けそれに正電圧を加えて電荷蓄積状態にしたの
とほゞ同様な効果が得られる。その後は電極6
1,62,51,52の電圧を除くが、N型拡散
層2は上記の空乏層化および高電位化された状態
にとどまる。この状態で光像投射すれば該空乏層
およびPN接合部Jに光像に応じた電荷が発生し
かつ蓄積される。この酸化膜3のみの受光部であ
れば波長特性は向上するが、反面CCD電極によ
り作られた空乏層は不完全で電荷蓄積領域は主と
してPN接合部Jとなるので電荷蓄積量が減つて
光入力に対する光電変換出力が低下する欠点があ
る。また、シリコン酸化膜3が光シールド電極7
の開口部から露出しているので電荷付着などのシ
リコン酸化膜の特性不安定性、延いては受光部A
の特性劣化が問題である。 In order to improve this point, an image sensor has been considered in which the photogate electrode 4 is removed from the structure shown in FIG. 1 and the oxide film 3 is formed above the PN junction J only. In this sensor, the transfer gates 5 1 and 5 2 are opened for charge accumulation, and the CCD
A voltage is applied to the electrodes 6 1 and 6 2 of the shift register section, and the N-type diffusion layer 2 of the light receiving section A is turned into a depletion layer by the voltage. That is, the electrodes 6 1 , 6 2 and 5 1 , 5 2
Furthermore, since this example is an N-channel device, when a positive voltage is applied, the N-type region 1a has a higher potential than the substrate 1. Moreover, since this region 1a communicates with the N-type diffusion layer 2, this layer 2 is made into a depletion layer, albeit incompletely, and its potential is increased. In this way, substantially the same effect as when the photogate electrode 4 is provided and a positive voltage is applied to it to create a charge storage state can be obtained. After that, electrode 6
Although the voltages 1 , 62 , 51 , and 52 are removed, the N-type diffusion layer 2 remains in the depleted state and high potential state described above. If a light image is projected in this state, charges corresponding to the light image will be generated and accumulated in the depletion layer and the PN junction J. If the light-receiving part is made up of only this oxide film 3, the wavelength characteristics will improve, but on the other hand, the depletion layer created by the CCD electrode is incomplete and the charge accumulation region is mainly the PN junction J, so the amount of charge accumulation is reduced and the light There is a drawback that the photoelectric conversion output relative to the input decreases. Furthermore, the silicon oxide film 3 is connected to the light shield electrode 7.
Since it is exposed through the opening of the silicon oxide film, it may cause instability of the characteristics of the silicon oxide film such as charge adhesion, and may even cause damage to the light receiving area A.
The problem is the deterioration of the characteristics.
本発明はかかる諸点を一挙に解決したイメージ
センサを提供することを目的としたもので、光を
投射されて発生したキヤリアを蓄積する受光部お
よび該受光部に沿つて配設されて蓄積キヤリアを
転送する電荷転送部を備えるCCDイメージセン
サにおいて、該受光部をPN接合を持つ半導体基
板、該基板上に形成された二酸化シリコン膜、該
二酸化シリコン膜上に形成されそして該二酸化シ
リコン膜より電導度が良くかつ所定電位を加えら
れる窒化シリコン膜で構成したことを特徴として
いる。 The object of the present invention is to provide an image sensor that solves all of these problems at once, and includes a light receiving part that accumulates carriers generated by projecting light, and a light receiving part arranged along the light receiving part to accumulate carriers. In a CCD image sensor equipped with a charge transfer section, the light receiving section is connected to a semiconductor substrate having a PN junction, a silicon dioxide film formed on the substrate, a silicon dioxide film formed on the silicon dioxide film, and a conductivity higher than that of the silicon dioxide film. It is characterized by being made of a silicon nitride film that has good resistance and can be applied with a predetermined potential.
前記二酸化シリコン膜上の窒化シリコン膜は前
記光シールド電極等により適当な電位に保たれる
ことにより擬似ホトゲート電極として機能して半
導体層に広い電荷蓄積領域を形成し、受光部にお
ける蓄積電荷量を増加させる。また窒化シリコン
膜を用いると、屈折率は約2であり、一方、二酸
化シリコンは1.5、周囲の空気は1であるから光
は屈折率1、2、1.5の各層を通つて屈折率4の
シリコン基板に入ることになり、第1図の場合の
屈折率1、1.5、4、1.5の各層を通つて屈折率4
のシリコン基板に入年る場合に比べて入射光の減
衰(反射)率は少なく、イメージセンサとしての
感度が広範囲な波長域において良好になる。そし
て、二酸化シリコン膜上は若干の導電性を持つ窒
化シリコン膜により覆われるので、電荷蓄積など
の問題はなく、酸化膜表面は安定化される。 The silicon nitride film on the silicon dioxide film functions as a pseudo-photogate electrode by being maintained at an appropriate potential by the light shield electrode, etc., and forms a wide charge storage region in the semiconductor layer, reducing the amount of charge stored in the light receiving section. increase. Furthermore, when a silicon nitride film is used, the refractive index is approximately 2, whereas silicon dioxide is 1.5 and the surrounding air is 1. Therefore, light passes through each layer with a refractive index of 1, 2, and 1.5 through the silicon film, which has a refractive index of 4. It enters the substrate, passes through each layer with a refractive index of 1, 1.5, 4, and 1.5 in the case of Fig.
The attenuation (reflection) rate of incident light is lower than that of silicon substrates, and the sensitivity of the image sensor is improved over a wide range of wavelengths. Since the silicon dioxide film is covered with a silicon nitride film having some conductivity, there is no problem of charge accumulation and the surface of the oxide film is stabilized.
以下、第2図を参照して本発明の一実施例を説
明する。第2図はCCDラインセンサに適用した
本発明の一実施例を示す断面図であり、第1図と
同一部分には同一符号を付してある。この実施例
における受光部A′は、半導体層1のPN接合部J
上方に1000〜1500Å程度のシリコン酸化膜
(SiO)3を介して、厚さ1500Å程度のシリコン
窒化膜(Si3N4)8を形成し、さらに窒化膜8の端
縁を導電性の光シールド電極(この例ではアルミ
ニウム)7の開口端縁に接続している。 An embodiment of the present invention will be described below with reference to FIG. FIG. 2 is a sectional view showing an embodiment of the present invention applied to a CCD line sensor, and the same parts as in FIG. 1 are given the same reference numerals. In this embodiment, the light receiving part A' is the PN junction J of the semiconductor layer 1.
A silicon nitride film (Si 3 N 4 ) 8 with a thickness of about 1500 Å is formed above through a silicon oxide film (SiO) 3 with a thickness of about 1000 to 1500 Å, and the edge of the nitride film 8 is further covered with a conductive light shield. It is connected to the opening edge of an electrode (aluminum in this example) 7.
空気に対するSiO2の屈折率は前述したように
約1.5であるのに対し、Si3N4の屈折率は約2であ
つて近似している。従つて、窒化膜8と酸化膜3
との界面における入射光に対する反射率は著しく
小さい。また窒化膜は酸化膜と同様透明度が高い
ので、入射光の減衰は少なく、特に短波長側の感
度が向上する。なお窒化膜8も酸化膜3も共に通
常の導電材料に比べては著しい絶縁性を有する
が、窒化膜8はその気相成長過程でシリコンと窒
素の比、具体的にはシランとアンモニアの混合比
を変えることにより導電性を持たせかつその導電
度をある範囲で調整することができる。そこで、
アースされた光シールド電極7に接続して窒化膜
8を零電位に、または適当な電極を別設して適宜
の正、負直流電位に保持しておくことができ、こ
うして窒化膜8を第1図のホトゲート電極4と同
様に機能させ、半導体層1に入射光により生じた
電荷の広い蓄積領域を形成させ、PN接合部Jの
電荷蓄積領域と併せて、電荷蓄積量を増大させる
ことができる。 The refractive index of SiO 2 with respect to air is about 1.5 as described above, whereas the refractive index of Si 3 N 4 is about 2, which is similar. Therefore, the nitride film 8 and the oxide film 3
The reflectivity of the incident light at the interface with the material is extremely small. Further, since the nitride film has high transparency like the oxide film, the attenuation of incident light is small, and the sensitivity, especially on the short wavelength side, is improved. Both the nitride film 8 and the oxide film 3 have remarkable insulating properties compared to ordinary conductive materials, but the nitride film 8 has a high ratio of silicon to nitrogen, specifically a mixture of silane and ammonia, during its vapor phase growth process. By changing the ratio, conductivity can be imparted and the conductivity can be adjusted within a certain range. Therefore,
The nitride film 8 can be held at zero potential by connecting it to the grounded light shield electrode 7, or at an appropriate positive or negative DC potential by separately providing an appropriate electrode. It functions in the same manner as the photogate electrode 4 in Figure 1, forming a wide accumulation region for charges generated by incident light in the semiconductor layer 1, and increasing the amount of charge accumulation in conjunction with the charge accumulation region of the PN junction J. can.
第3図は通常のCCDラインセンサの平面図で
あり、第3図の×−×での断面が第1、第2図に
相当する。受光部A′は蛇行状チヤンネルカツト
9により分離された複数の受光素子A″(前記の
ダイオード)を線状に配列した所謂ホトダイオー
ドアレイであつて、受光面にはホトゲート電極4
または窒化膜8が設けられ、周囲は光シールド電
極7で覆われている。この受光部A,A′の光電
変換出力(電荷)は、両側のCCDシフトレジス
タ部B1,B2に白矢印イ,ロで示すように1ビツ
ト毎に振り分けられて読み出され、これらシフト
レジスタ部B1,B2内を白矢印ハ方向に転送され
て、出力ゲート101,102を介して増幅器1
11,112に到り、ここで増幅されて出力01,
02として取り出される。尚シフトレジスタ部B1,
B2による電荷転送に先立ちトランスフアゲート
電極51,52に電圧を加え、該ゲートを開けて
受光部A′からCCDレジスタ部へ一斉に電荷を転
送する。CCD電極61,62によるシリアルな
電荷転送は通常のCCD駆動方法と同様であるか
らその詳細は省略する。 FIG. 3 is a plan view of a normal CCD line sensor, and the cross section taken along line x--x in FIG. 3 corresponds to FIGS. 1 and 2. The light-receiving section A' is a so-called photodiode array in which a plurality of light-receiving elements A'' (the above-mentioned diodes) separated by a meandering channel cut 9 are linearly arranged, and a photogate electrode 4 is provided on the light-receiving surface.
Alternatively, a nitride film 8 is provided, and the periphery is covered with a light shield electrode 7. The photoelectric conversion outputs (charges) of the light receiving sections A and A' are distributed and read out bit by bit as shown by white arrows A and B to the CCD shift register sections B 1 and B 2 on both sides. It is transferred in the direction of the white arrow C in the register sections B 1 and B 2 and then sent to the amplifier 1 via the output gates 10 1 and 10 2 .
1 1 , 11 2 , which is amplified and outputs 0 1 ,
Retrieved as 0 2 . Furthermore, the shift register section B 1 ,
Prior to charge transfer by B 2 , a voltage is applied to the transfer gate electrodes 5 1 and 5 2 to open the gates and transfer charges all at once from the light receiving section A' to the CCD register section. Since the serial charge transfer by the CCD electrodes 6 1 and 6 2 is similar to a normal CCD driving method, the details thereof will be omitted.
以上述べたことから明らかなように本発明のイ
メージセンサであれば、波長特性が向上すると共
に蓄積電荷量が大であるから、従来のイメージセ
ンサの有する矛盾した問題点を一挙に解決するこ
とができ、しかも同時にパシベーシヨンが行なわ
れる利点がある。 As is clear from the above, the image sensor of the present invention has improved wavelength characteristics and a large amount of accumulated charge, so it is possible to solve the contradictory problems of conventional image sensors all at once. This has the advantage that passivation can be performed at the same time.
第1図は従来のCCDイメージセンサの一例を
示す断面図、第2図は本発明の一実施列を示す断
面図、第3図はCCDラインセンサの平面図であ
る。
1……P型半導体層、2……N型拡散層、3…
…シリコン酸化膜、51,52……トランフアゲ
ート電極、61,62……CCD電極、7……光
シールド電極、8……シリコン窒化膜(絶縁
膜)、9……チヤネルカツト、101,102…
…出力ゲート、111,112……アンプ、
A′……受光部、B1,B2……CCDシフトレジスタ
部。
FIG. 1 is a sectional view showing an example of a conventional CCD image sensor, FIG. 2 is a sectional view showing one embodiment of the present invention, and FIG. 3 is a plan view of a CCD line sensor. 1... P-type semiconductor layer, 2... N-type diffusion layer, 3...
... silicon oxide film, 5 1 , 5 2 ... transfer gate electrode, 6 1 , 6 2 ... CCD electrode, 7 ... light shield electrode, 8 ... silicon nitride film (insulating film), 9 ... channel cut, 10 1 , 10 2 ...
...output gate, 11 1 , 11 2 ... amplifier,
A′... Light receiving section, B 1 , B 2 ... CCD shift register section.
Claims (1)
受光部および該受光部に沿つて配設されて蓄積キ
ヤリアを転送する電荷転送部を備えるCCDイメ
ージセンサにおいて、該受光部をPN接合を持つ
半導体基板、該基板上に形成された二酸化シリコ
ン膜、該二酸化シリコン膜上に形成されそして該
二酸化シリコン膜より電導度が良くかつ所定電位
を加えられる窒化シリコン膜で構成したことを特
徴とするイメージセンサ。 2 窒化シリコン膜が、電荷転送部等受光部以外
の表面を覆う光シールド電極に接続されたことを
特徴とする特許請求の範囲第1項記載のイメージ
センサ。[Claims] 1. A CCD image sensor comprising a light receiving section that accumulates carriers generated by projecting light and a charge transfer section that is disposed along the light receiving section and transfers the accumulated carriers. A semiconductor substrate having a PN junction, a silicon dioxide film formed on the substrate, and a silicon nitride film formed on the silicon dioxide film, which has better conductivity than the silicon dioxide film and can be applied with a predetermined potential. Featured image sensor. 2. The image sensor according to claim 1, wherein the silicon nitride film is connected to a light shield electrode that covers a surface other than a light receiving part such as a charge transfer part.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10647278A JPS5533385A (en) | 1978-08-31 | 1978-08-31 | Image sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10647278A JPS5533385A (en) | 1978-08-31 | 1978-08-31 | Image sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5533385A JPS5533385A (en) | 1980-03-08 |
| JPS6147031B2 true JPS6147031B2 (en) | 1986-10-17 |
Family
ID=14434458
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10647278A Granted JPS5533385A (en) | 1978-08-31 | 1978-08-31 | Image sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5533385A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0642926U (en) * | 1992-11-24 | 1994-06-07 | 美代子 星野 | Sun avoid baseball cap |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2533371B1 (en) * | 1982-09-21 | 1985-12-13 | Thomson Csf | GRID STRUCTURE FOR AN INTEGRATED CIRCUIT COMPRISING ELEMENTS OF THE GRID-INSULATOR-SEMICONDUCTOR TYPE AND METHOD FOR PRODUCING AN INTEGRATED CIRCUIT USING SUCH A STRUCTURE |
-
1978
- 1978-08-31 JP JP10647278A patent/JPS5533385A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0642926U (en) * | 1992-11-24 | 1994-06-07 | 美代子 星野 | Sun avoid baseball cap |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5533385A (en) | 1980-03-08 |
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