JPH0245344B2 - - Google Patents
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- Publication number
- JPH0245344B2 JPH0245344B2 JP58007666A JP766683A JPH0245344B2 JP H0245344 B2 JPH0245344 B2 JP H0245344B2 JP 58007666 A JP58007666 A JP 58007666A JP 766683 A JP766683 A JP 766683A JP H0245344 B2 JPH0245344 B2 JP H0245344B2
- Authority
- JP
- Japan
- Prior art keywords
- amorphous silicon
- transparent electrode
- heat treatment
- reading element
- lower electrode
- 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
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Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F30/00—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors
- H10F30/10—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices being sensitive to infrared radiation, visible or ultraviolet radiation, and having no potential barriers, e.g. photoresistors
- H10F30/15—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices being sensitive to infrared radiation, visible or ultraviolet radiation, and having no potential barriers, e.g. photoresistors comprising amorphous semiconductors
Landscapes
- Solid State Image Pick-Up Elements (AREA)
- Facsimile Heads (AREA)
- Light Receiving Elements (AREA)
Description
本発明は下部電極、光導電体、上部透明電極を
堆積した積層構造からなる長尺薄膜原稿読取素子
の読取性能を向上させるために製造工程中に熱処
理工程を付加した長尺薄膜原稿読取素子の製造方
法に関する。
近年、フアクシミリ等における読取装置の小型
化あるいは機構の簡素化を計るために、下部電
極、光導電体、透明電極を堆積した積層構造を有
する長尺薄膜原稿読取素子が用いられるようにな
つた。第1図は光導電体に水酸化したアモルフア
スシリコン層を適用した従来の一般的な長尺薄膜
原稿読取素子の断面構造を示した略図である。第
1図において1は絶縁性基板、2は下部電極、3
はアモルフアスシリコン層、4は上部透明電極で
ある。従来のこのような積層構造を有する長尺薄
膜原稿読取素子5の製造方法を以下に述べる。
まず絶縁性基板1としてはセラミツク、ガラ
ス、プラスチツク等を用いるのが一般的である
が、機械的強度が強く、製造工程中に行われる熱
処理に対する耐熱性があり、かつ十分な絶縁性を
有するものであればこれらに限定することなく用
いることができる。また下部電極2としては、
Cr、Ni、Pt、Pd、Ti、Mo、Ta等の金属材料あ
るいは高濃度にドープしたアモルフアスシリコン
等の半導体を用いることができる。次にこれら絶
縁性基板1への下部電極2の堆積方法であるが、
前記下部電極2として金属材料を用いる場合には
電子ビーム蒸着法、ポリシリコン層等の半導体を
用いる場合にはプラズマCVD法あるいはCVD法
が好適である。上記いずれの場合においても、下
部電極2の堆積厚さは第1000Å〜5000Å程度に保
たれるのが望ましい。さらに前記下部電極2はフ
オトリソグラフイー法により所定形状(一般的に
はくし形)にパターニングする。次に水素化した
アモルフアスシリコン層3としてはノンドープの
ものまたホウ素Bあるいはその他周期律表族の
元素をドープしたP型層のものを用いることがで
きる。下部電極2の形成された絶縁性基板1上へ
の水酸化アモルフアスシリコン層の堆積方法とし
てはプラズマCVD法を用い、膜厚としては1μm
程度が適当である。さらに上部透明電極4として
はITO膜(In2O3+SnO2)を用いることができ
る。
このとき下部電極2および水酸化アモルフアス
シリコン層3の形成された絶縁性基板1上への堆
積方法としては反応性スパツタリング法を用い、
堆積厚さとしては500Å〜2000Å程度が適当であ
る。以上が一般的な長尺薄膜原稿読取素子5の製
造方法である。次にこの読取素子5における光電
変換原理を簡単に述べる。まず通常このような読
取素子5を動作させる場合には、下部電極2、上
部透明電極4間にバイアス電圧を印加して用いる
がこのとき下部電極2を接地し、上部透明電極4
の負のバイアス電圧を印加するのが一般的であ
る。この状態で前記読取素子5に所定の光を照射
すると該光は上部透明電極4を通過し、アモルフ
アスシリコン層3に照射される。アモルフアスシ
リコン層3内では照射された光のエネルギーによ
り、電子、正孔の対が発生する。
上述したように下部電極2、上部透明電極4間
には逆バイアス電圧が加えられていることから前
記電子は下部電極2側へ、前記正孔は透明電極4
側へそれぞれ流入し、該アモルフアスシリコン層
3内を所定の電流が流れる。したがつてこの電流
を外部へとりだすことによつて該照射光に対する
光電変換電流を得ることができる。一方前記読取
素子5に光が照射されない場合は、上述したよう
な光励起は起きないが前記両電極間に加えられて
いるバイアス電圧によつて前記アモルフアスシリ
コン層3内を微弱な電流すなわち暗電流か流れ
る。
第2図は以上説明した読取素子5の光照射時お
よび非照射時に発生する電流を測定する様子を示
した略図である。
第2図において、下部電極2を接地側とし透明
電極4側にはバイアス電源6から所定のバイアス
電圧が印加されている。この状態でランプ7の発
光を制御し該ランプ7から読取素子5に対して光
の照射あるいは照射停止の動作を行う。
そして前記光照射時の電流計8の指示を光電
流、また前記非照射時の電流計8の指示を暗電流
として測定する。この測定は、バイアス電圧を変
化させ、各点毎に行う。またこの時のランプ7の
発光時の照度(光量)は100xとする。
第3図は上記測定結果の一般的なDCI−V特性
を示したものであり、図中aは光電流、同bは暗
電流をそれぞれ示している。第3図aに示す光電
流の電流密度〔A/cm3〕が低バイアス時から飽和
しているのは下部電極2および透明電極4が光の
照射によつて励起される電子、正孔に対してそれ
ぞれブロツキング接触して働いていることを示し
ている。
なおここで励起された電子正孔の対はすべて外
部に取りだしている。一方、第3図bに示す暗電
流は上記光電流に比べて低い値に抑えられてい
る。この原因としては光の非照射時に下部電極2
からアモルフアスシリコン層3への正孔の注入ま
たは上部透明電極4からアモルフアスシリコン層
3への電子の注入が抑えられているためと推測で
きる。この詳細についてはまだ明らかにされてい
ないのが実状であるが本発明者らは、種々の実験
結果から、後者が有力であると考える。いずれに
しても上記両電極からアモルフアスシリコン層3
への電荷の注入を抑えるものとして、該両電極と
アモルフアスシリコン層3の境界面にある種の電
荷障壁層が形成されておりこの電荷障壁層の高さ
によつて暗電流の増減が変化すると考えられる。
さて周知のように原稿読取素子はフアクシミリ
等に実装される場合照明用光源を原稿に照射し該
原稿からの反射光の有無すなわち明信号と暗信号
から該原稿の情報を読取るものである。
したがつてその読取り性能を向上させるために
は光照射時に得られる光電流と非照射時に得られ
る暗電流の比をできるだけ大きくとれることが望
ましい。しかしながら上述した従来の製造方法に
よつて得られる読取素子では暗電流自体は低い値
にもかかわらず識別の確実性を考慮した場合、前
記光電流と暗電流の比としては決して望ましい大
きさであるとは言いがたかつた。
本発明はかかる実状に鑑みてなされたものであ
り、前記光電流を十分大きな値に保ちつつ暗電流
を極力小さな値に抑えることができ、これによつ
て前記両電流間の比を大きなものとし明信号と暗
信号の識別を確実になすことのできる長尺薄膜原
稿読取素子の製造方法を提供することを目的とす
る。
そこで本発明では、長尺薄膜読取素子の製造に
際し、水酸化アモルフアスシリコン層からなる光
導電体層上にスパツタリング法により上部透明電
極を形成した後、大気または酸素ガスを含む不活
性ガス雰囲気中で200〜300℃の熱処理を施すこと
によつて上記目的を達成している。
以下本発明の実施例を実際の製造工程に即し添
付図面を参照して詳述する。
本発明においては基板1にガラス、下部電極2
にCr、光導電体3に水素化したアモルフアスシ
リコン、上部透明電極4にITO膜(In2O3+
SnO2)をそれぞれ用いている。まず、ガラス基
板上に電子ビーム蒸着法により3000ÅのCrを堆
積し、その後通常のフオトリソグラフイー法によ
り該着膜されたCrをくし形にパターンニングす
る。次にシランガス(SiH4)をグロー放電によ
つて分解することにより水素化したアモルフアス
シリコンをガラス基板、Cr電極上に約1μmの厚
さに堆積する。この時の各堆積条件は基板温度
200〜300℃、放電圧力0.2〜1.0Torr、極板間距離
40mm、RFパワー10〜100W、シランガス流量10〜
50Sccm、堆積時間1時間とした。さらにこの上
にArとO2を混合した反応性ガス雰囲気中でITO
(In2O3+SnO2)をターゲツトとしDCマグネトロ
ンスパツタリング法により約1500ÅのITO膜を堆
積する。この時基板の加熱は行わないが、該基板
温度は50℃以下に保たれている。
次に以上の方法により得た読取素子の明電流と
暗電流を第2図に示したと同様の方法により測定
した。この時バイアス電圧6として−5Vを印加
し、ランプ7に緑色の蛍光灯を用いた。
またこの蛍光灯の照射時の照度は100xとし
た。
この結果光電流9.2×10-10〔A〕、暗電流6.8×
10-13〔A〕を得た。次にこの電流測定後、前記読
取素子5に熱処理を施した。第4図はこの様子を
概念的に示す略図であり大気中で加熱ヒータ9の
加熱により200℃に保たれた加熱炉10内に前記
読取素子5を入れ約30分間放置した。
その後上述したと同様の条件の下でこの読取素
子5の光電流と暗電流を測定したところ光電流
9.8×10-10〔A〕、暗電流7.6×10-14〔A〕をそれぞ
れ得た。第1表は上述した読取素子5の熱処理前
と熱処理後の各光電流、暗電流の測定結果を示し
たものである。
The present invention relates to a long thin film original reading element which has a laminated structure in which a lower electrode, a photoconductor, and an upper transparent electrode are deposited, and which has a heat treatment process added during the manufacturing process in order to improve the reading performance of the long thin film original reading element. Regarding the manufacturing method. In recent years, in order to downsize or simplify the mechanism of reading devices such as facsimile machines, long thin film document reading elements having a laminated structure in which a lower electrode, a photoconductor, and a transparent electrode are deposited have come into use. FIG. 1 is a schematic diagram showing the cross-sectional structure of a conventional long thin film original reading element in which a hydroxylated amorphous silicon layer is applied as a photoconductor. In FIG. 1, 1 is an insulating substrate, 2 is a lower electrode, and 3
4 is an amorphous silicon layer, and 4 is an upper transparent electrode. A conventional method for manufacturing the elongated thin film document reading element 5 having such a laminated structure will be described below. First, as the insulating substrate 1, ceramic, glass, plastic, etc. are generally used, but materials with strong mechanical strength, heat resistance to heat treatment performed during the manufacturing process, and sufficient insulation properties are used. If so, it can be used without being limited to these. Moreover, as the lower electrode 2,
Metal materials such as Cr, Ni, Pt, Pd, Ti, Mo, and Ta, or semiconductors such as highly doped amorphous silicon can be used. Next is the method of depositing the lower electrode 2 on the insulating substrate 1.
When a metal material is used as the lower electrode 2, an electron beam evaporation method is suitable, and when a semiconductor such as a polysilicon layer is used, a plasma CVD method or a CVD method is suitable. In any of the above cases, it is desirable that the deposited thickness of the lower electrode 2 be maintained at about 1000 Å to 5000 Å. Furthermore, the lower electrode 2 is patterned into a predetermined shape (generally a comb shape) by photolithography. Next, as the hydrogenated amorphous silicon layer 3, a non-doped one or a P-type layer doped with boron B or other elements of the periodic table group can be used. The plasma CVD method was used to deposit the amorphous silicon hydroxide layer on the insulating substrate 1 on which the lower electrode 2 was formed, and the film thickness was 1 μm.
The degree is appropriate. Further, as the upper transparent electrode 4, an ITO film (In 2 O 3 +SnO 2 ) can be used. At this time, a reactive sputtering method is used as a deposition method on the insulating substrate 1 on which the lower electrode 2 and the amorphous silicon hydroxide layer 3 are formed.
Appropriate deposition thickness is about 500 Å to 2000 Å. The above is a general method for manufacturing the long thin film document reading element 5. Next, the principle of photoelectric conversion in this reading element 5 will be briefly described. First, when such a reading element 5 is normally operated, a bias voltage is applied between the lower electrode 2 and the upper transparent electrode 4. At this time, the lower electrode 2 is grounded and the upper transparent electrode 4 is
It is common to apply a negative bias voltage of . When the reading element 5 is irradiated with a predetermined light in this state, the light passes through the upper transparent electrode 4 and is irradiated onto the amorphous silicon layer 3. Inside the amorphous silicon layer 3, pairs of electrons and holes are generated by the energy of the irradiated light. As described above, since a reverse bias voltage is applied between the lower electrode 2 and the upper transparent electrode 4, the electrons flow toward the lower electrode 2, and the holes flow toward the transparent electrode 4.
A predetermined current flows through the amorphous silicon layer 3. Therefore, by extracting this current to the outside, a photoelectric conversion current for the irradiated light can be obtained. On the other hand, when the reading element 5 is not irradiated with light, the above-mentioned photoexcitation does not occur, but a weak current, that is, a dark current, flows in the amorphous silicon layer 3 due to the bias voltage applied between the two electrodes. It flows. FIG. 2 is a schematic diagram showing how the current generated by the reading element 5 described above is measured when it is irradiated with light and when it is not irradiated with light. In FIG. 2, a predetermined bias voltage is applied from a bias power supply 6 to the transparent electrode 4 side with the lower electrode 2 being on the ground side. In this state, the light emission of the lamp 7 is controlled, and the lamp 7 irradiates the reading element 5 with light or stops the irradiation. Then, the indication of the ammeter 8 during the light irradiation is measured as a photocurrent, and the indication of the ammeter 8 during the non-irradiation is measured as a dark current. This measurement is performed at each point by changing the bias voltage. Further, the illumination intensity (light amount) when the lamp 7 emits light at this time is 100x. FIG. 3 shows the general DCI-V characteristics of the above measurement results, in which a indicates the photocurrent and b indicates the dark current, respectively. The reason why the current density [A/cm 3 ] of the photocurrent shown in FIG. This shows that they work in blocking contact with each other. Note that all electron-hole pairs excited here are taken out to the outside. On the other hand, the dark current shown in FIG. 3b is suppressed to a lower value than the photocurrent. The cause of this is that the lower electrode 2 when not irradiated with light.
This is presumed to be because the injection of holes from the upper transparent electrode 4 into the amorphous silicon layer 3 or the injection of electrons from the upper transparent electrode 4 into the amorphous silicon layer 3 is suppressed. Although the details of this have not yet been clarified, the present inventors believe that the latter is more likely based on various experimental results. In any case, the amorphous silicon layer 3 is
A charge barrier layer of some kind is formed at the interface between the two electrodes and the amorphous silicon layer 3 to suppress the injection of charge into the amorphous silicon layer 3, and the increase or decrease of the dark current changes depending on the height of this charge barrier layer. It is thought that then. As is well known, when a document reading element is mounted on a facsimile or the like, it illuminates the document with an illumination light source and reads information on the document based on the presence or absence of reflected light from the document, that is, bright and dark signals. Therefore, in order to improve the reading performance, it is desirable that the ratio between the photocurrent obtained during light irradiation and the dark current obtained during non-irradiation be as large as possible. However, in the reading element obtained by the above-mentioned conventional manufacturing method, although the dark current itself is low, when considering the reliability of identification, the ratio of the photocurrent to the dark current is by no means desirable. It was hard to say. The present invention has been made in view of this situation, and it is possible to suppress the dark current to a value as small as possible while keeping the photocurrent at a sufficiently large value, thereby increasing the ratio between the two currents. It is an object of the present invention to provide a method for manufacturing a long thin film document reading element that can reliably distinguish between bright signals and dark signals. Therefore, in the present invention, when manufacturing a long thin film reading element, after forming an upper transparent electrode by a sputtering method on a photoconductor layer made of an amorphous silicon hydroxide layer, the electrode is placed in air or an inert gas atmosphere containing oxygen gas. The above objective is achieved by applying heat treatment at 200 to 300°C. Embodiments of the present invention will be described in detail below in accordance with actual manufacturing processes with reference to the accompanying drawings. In the present invention, the substrate 1 is made of glass, and the lower electrode 2 is made of glass.
Cr, hydrogenated amorphous silicon for the photoconductor 3, ITO film (In 2 O 3 +
SnO 2 ) was used in each case. First, 3000 Å of Cr is deposited on a glass substrate by electron beam evaporation, and then the deposited Cr is patterned into a comb shape by ordinary photolithography. Next, amorphous silicon, which is hydrogenated by decomposing silane gas (SiH 4 ) by glow discharge, is deposited to a thickness of about 1 μm on the glass substrate and Cr electrode. Each deposition condition at this time is the substrate temperature
200~300℃, discharge pressure 0.2~1.0Torr, distance between plates
40mm, RF power 10~100W, silane gas flow rate 10~
The deposition time was 50Sccm and 1 hour. Furthermore, ITO was added on top of this in a reactive gas atmosphere containing a mixture of Ar and O2 .
An ITO film of about 1500 Å is deposited using the DC magnetron sputtering method using (In 2 O 3 + SnO 2 ) as a target. At this time, the substrate is not heated, but the substrate temperature is maintained at 50° C. or lower. Next, the bright current and dark current of the reading element obtained by the above method were measured by the same method as shown in FIG. At this time, -5V was applied as the bias voltage 6, and a green fluorescent lamp was used as the lamp 7. In addition, the illumination intensity during irradiation of this fluorescent lamp was set to 100x. As a result, photocurrent 9.2×10 -10 [A], dark current 6.8×
10 -13 Got [A]. Next, after measuring this current, the reading element 5 was subjected to heat treatment. FIG. 4 is a schematic diagram conceptually showing this situation, and the reading element 5 was placed in a heating furnace 10 kept at 200° C. by heating with a heater 9 in the atmosphere and left for about 30 minutes. Thereafter, the photocurrent and dark current of this reading element 5 were measured under the same conditions as described above.
A dark current of 9.8×10 -10 [A] and a dark current of 7.6×10 -14 [A] were obtained, respectively. Table 1 shows the measurement results of each photocurrent and dark current of the above-mentioned reading element 5 before and after heat treatment.
【表】
第1表において熱処理前から熱処理後にかけて
のそれぞれの電流の変化率を
変化率=(熱処理後の特性値)/(熱処理前の
特性値)
として表わせば、光電流の場合1.07となりあまり
変化がないのに比べ、暗電流の場合は0.11となり
大幅に減少していることがわかる。
また上記熱処理前と熱処理後のそれぞれについ
て光電流と暗電流の比すなわち明暗比を求めると
熱処理前では、9.2×10-10/6.8×10-13≒1400で
あるのに対し熱処理後では9.8×10-10/7.6×
10-14≒13000となりその比が著しく増しているこ
とがわかる。なおこの光電流/暗電流すなわち明
暗比の熱処理前から熱処理後にかけての変化率と
して9.3を得た。
以上の結果は上部透明電極4をアモルフアスシ
リコン3および基板1に堆積後大気中において熱
処理を施した場合の例である。さらに本発明にお
いては前記透明電極4を堆積後、酸素ガスO2を
含む不活性ガス(N2またはAr)からなる雰囲気
中で200〜300℃の熱処理を30〜120分間行つた。
この結果も第1表に示すと同様に熱処理前と熱処
理後での光電流と暗電流の比の著しい増加を確認
することができた。これは、水素化アモルフアス
シリコン層上にスパツタリング法により上部透明
電極としてのITOを堆積した場合、水素化アモル
フアスシリコン層表面にダングリングボンドが発
生し、上部透明電極と水素化アモルフアスシリコ
ン層との界面特性が低下し、暗電流が上昇してい
たのに対し、熱処理によつて、ダングリングボン
ドが減少し上部透明電極と水素化アモルフアスシ
リコン層との界面特性が向上したためと考えられ
る。
さらにまた、酸素雰囲気中で熱処理を行うこと
により、酸素がITO中を拡散し水素化アモルフア
スシリコン層との界面に酸化層を形成し、シヨツ
トキバリアを形成することにより、更に暗電流の
低減をはかることができたものとも考えられる。
また上述したいずれかの熱処理を施した後、さ
らに300℃、120分の真空熱処理を施しその後に第
3図に示した方法でDCI−V特性を測定した所、
その特性値にほとんど変化が認められなかつた。
このことは、前記読取素子5上にパシベーシヨン
膜(外周からの電気的、化学的要件からの該素子
を隔離し電気的安定性を持たせるための酸化膜)
を堆積する場合の熱処理工程にも安定して耐えう
ることを示している。
以上説明したように、本発明の長尺薄膜原稿読
取素子の製造方法によれば、透明電極堆積後、所
定温度の熱処理を施すことによりスパツタリング
で受けた水素化アモルフアスシリコン層表面のダ
メージが回復し、透明電極と水素化アモルフアス
シリコン層との界面特性が向上すると共に、酸素
が透明電極表面に拡散し水素化アモルフアスシリ
コン層との界面に酸化層を形成しシヨツトキバリ
アを形成するため光電流が高い値に保たれ、かつ
暗電流が極めて低い値の読取素子5を得ることが
できる。
このため明電流と前記暗電流との比を十分大き
くとることができ、原稿の読取性能を著しく向上
させることができる。また前記熱処理は大気また
は酸素ガスを含む不活性ガス中で行えるため加圧
装置等の特別の装置も必要とせず製造装置の機構
簡素化、制御の単純化にも寄与できる等種々の優
れた効果を奏する。さらに、上記熱処理によつて
ダングリングボンドが低減され、界面特性が安定
化された素子に、パツシベーシヨン膜の形成工程
で熱処理を加えても特性は安定して維持される。[Table] In Table 1, if the rate of change of each current from before heat treatment to after heat treatment is expressed as rate of change = (characteristic value after heat treatment) / (characteristic value before heat treatment), in the case of photocurrent, it is 1.07, which is too much. It can be seen that while there is no change, the dark current is 0.11, which is a significant decrease. Furthermore, when calculating the ratio of photocurrent to dark current, that is, the brightness ratio, before and after the heat treatment, before the heat treatment, it is 9.2×10 -10 /6.8×10 -13 ≒1400, while after the heat treatment, it is 9.8× 10 -10 /7.6×
10 -14 ≒ 13000, which shows that the ratio has increased significantly. The rate of change in photocurrent/dark current, ie, brightness/darkness ratio, from before to after heat treatment was 9.3. The above results are examples in which the upper transparent electrode 4 was deposited on the amorphous silicon 3 and the substrate 1 and then subjected to heat treatment in the atmosphere. Further, in the present invention, after depositing the transparent electrode 4, heat treatment was performed at 200 to 300° C. for 30 to 120 minutes in an atmosphere consisting of an inert gas (N 2 or Ar) containing oxygen gas O 2 .
As shown in Table 1, this result also confirmed a significant increase in the ratio of photocurrent to dark current before and after heat treatment. This is because when ITO is deposited as the upper transparent electrode on the hydrogenated amorphous silicon layer by sputtering method, dangling bonds are generated on the surface of the hydrogenated amorphous silicon layer, and the upper transparent electrode and the hydrogenated amorphous silicon layer This is thought to be because the interfacial properties between the upper transparent electrode and the hydrogenated amorphous silicon layer decreased and the dark current increased due to heat treatment, while the dangling bonds decreased and the interfacial properties between the upper transparent electrode and the hydrogenated amorphous silicon layer improved. . Furthermore, by performing heat treatment in an oxygen atmosphere, oxygen diffuses through the ITO and forms an oxide layer at the interface with the hydrogenated amorphous silicon layer, forming a shot barrier, thereby further reducing dark current. It is also possible that it was possible. Furthermore, after performing any of the heat treatments described above, vacuum heat treatment was further performed at 300°C for 120 minutes, and then the DCI-V characteristics were measured using the method shown in Figure 3.
Almost no change was observed in the characteristic values.
This means that there is a passivation film (an oxide film for isolating the element from electrical and chemical requirements from the outer periphery and providing electrical stability) on the reading element 5.
This shows that it can stably withstand the heat treatment process when depositing. As explained above, according to the method for manufacturing a long thin film original reading element of the present invention, damage to the surface of the hydrogenated amorphous silicon layer caused by sputtering is recovered by heat treatment at a predetermined temperature after transparent electrode deposition. However, the interfacial properties between the transparent electrode and the hydrogenated amorphous silicon layer are improved, and oxygen diffuses into the surface of the transparent electrode to form an oxide layer at the interface with the hydrogenated amorphous silicon layer, forming a shot barrier. It is possible to obtain a reading element 5 in which the dark current is maintained at a high value and the dark current is extremely low. Therefore, the ratio between the bright current and the dark current can be made sufficiently large, and the document reading performance can be significantly improved. In addition, since the heat treatment can be performed in the atmosphere or in an inert gas containing oxygen gas, special equipment such as a pressurizing device is not required, and it has various excellent effects such as contributing to the simplification of the mechanism and control of the manufacturing equipment. play. Furthermore, even if a heat treatment is applied to the element in which dangling bonds are reduced and the interfacial characteristics are stabilized by the heat treatment, the characteristics are maintained stably even if heat treatment is applied in the step of forming the passivation film.
第1図は一般的な長尺薄膜原稿読取素子の断面
構造を概念的に示した略図、第2図は第1図に示
した読取素子における光電流と暗電流の測定方法
を示した略図、第3図は上記測定を実施して得ら
れる代表的なDCI−V特性を示す図、第4図は本
発明に係る製造装置の一例を示す略図である。
1……絶縁性基板、2……下部電極、3……光
導電体、4……上部透明電極、5……長尺薄膜原
稿読取素子、6……バイアス電源、7……ラン
プ、8……電流計、9……加熱ヒータ、10……
加熱炉。
FIG. 1 is a schematic diagram conceptually showing the cross-sectional structure of a general long thin film document reading element, and FIG. 2 is a schematic diagram showing a method for measuring photocurrent and dark current in the reading element shown in FIG. 1. FIG. 3 is a diagram showing typical DCI-V characteristics obtained by carrying out the above measurements, and FIG. 4 is a schematic diagram showing an example of a manufacturing apparatus according to the present invention. DESCRIPTION OF SYMBOLS 1... Insulating substrate, 2... Lower electrode, 3... Photoconductor, 4... Upper transparent electrode, 5... Long thin film original reading element, 6... Bias power supply, 7... Lamp, 8... ... Ammeter, 9... Heater, 10...
heating furnace.
Claims (1)
極形成工程と、 該下部電極上に水素化アモルフアスシリコン層
からなる光導電体層を積層する光導電体層形成工
程と、 該光導電体層上にスパツタリング法により上部
透明電極を積層する上部透明電極形成工程とから
なり、基板上に複数の光電変換素子を配列してな
る長尺薄膜原稿読取素子の製造方法において、 前記上部透明電極形成後、これらの光電変換素
子に体し、200〜300℃の大気または酸素ガスを含
む不活性ガス雰囲気中で、加熱処理を行う熱処理
工程を含むことを特徴とする長尺薄膜原稿読取素
子の製造方法。[Claims] 1. A lower electrode forming step of forming a lower electrode on an insulating substrate, and a photoconductor layer forming step of laminating a photoconductor layer made of a hydrogenated amorphous silicon layer on the lower electrode. and an upper transparent electrode forming step of laminating an upper transparent electrode on the photoconductor layer by a sputtering method, in a method for manufacturing a long thin film document reading element in which a plurality of photoelectric conversion elements are arranged on a substrate. After forming the upper transparent electrode, the photoelectric conversion element is subjected to a heat treatment step in which the photoelectric conversion element is heated at 200 to 300°C in the atmosphere or an inert gas atmosphere containing oxygen gas. A method for manufacturing a thin film document reading element.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58007666A JPS59132654A (en) | 1983-01-20 | 1983-01-20 | Manufacture of continuous thin film manuscript read-out element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58007666A JPS59132654A (en) | 1983-01-20 | 1983-01-20 | Manufacture of continuous thin film manuscript read-out element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59132654A JPS59132654A (en) | 1984-07-30 |
| JPH0245344B2 true JPH0245344B2 (en) | 1990-10-09 |
Family
ID=11672125
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58007666A Granted JPS59132654A (en) | 1983-01-20 | 1983-01-20 | Manufacture of continuous thin film manuscript read-out element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59132654A (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5635407A (en) * | 1979-08-31 | 1981-04-08 | Fujitsu Ltd | Manufacture of amorphous silicon film |
| JPS5721875A (en) * | 1980-07-14 | 1982-02-04 | Canon Inc | Photosensor |
-
1983
- 1983-01-20 JP JP58007666A patent/JPS59132654A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59132654A (en) | 1984-07-30 |
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