JPS603793B2 - Infrared sensing element - Google Patents
Infrared sensing elementInfo
- Publication number
- JPS603793B2 JPS603793B2 JP53093821A JP9382178A JPS603793B2 JP S603793 B2 JPS603793 B2 JP S603793B2 JP 53093821 A JP53093821 A JP 53093821A JP 9382178 A JP9382178 A JP 9382178A JP S603793 B2 JPS603793 B2 JP S603793B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- sensing element
- electrodes
- infrared sensing
- 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
Links
Landscapes
- Radiation Pyrometers (AREA)
- Light Receiving Elements (AREA)
Description
【発明の詳細な説明】
本発明は赤外線検知素子、特に光伝導型赤外線検知素子
の電極と受光部の構造の改良に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in the structure of an electrode and a light receiving part of an infrared sensing element, particularly a photoconductive infrared sensing element.
半導体赤外線検知素子の構成材料としては一般に狭いバ
ンドキャップを有する多元半導体、たとえば水銀カドミ
ウムテルル(Hg1−xC舷Te)等が用いられている
。As a constituent material of a semiconductor infrared sensing element, a multicomponent semiconductor having a narrow bandgap, such as mercury cadmium telluride (Hg1-xC Te), is generally used.
このような多元半導体からなる赤外線検知素子の一種と
して、光子のエネルギーが素子材料のエネルギーギャッ
プよりも大きい波長の赤外線を照射することによりキャ
リアを発生させ、このキヤリャに基づく素子の電気伝導
度の変化を利用して入射した赤外線を検出する光伝導型
検知素子がある。As a type of infrared sensing element made of such a multi-component semiconductor, carriers are generated by irradiating infrared rays with a wavelength where the photon energy is greater than the energy gap of the element material, and the electrical conductivity of the element changes based on these carriers. There is a photoconductive sensing element that detects incident infrared rays using
従来この種の素子における電極の構成としては、上記の
光による電気伝導度の変化に基づく電気信号をもっとも
効率よく取り出すために第1図に示すごとく、赤外線検
知素子1の受光面2の両端にln等の金属を用し、蒸着
法等により電極3を設け、素子1と電極3はオーム性接
触であるように形成していた。Conventionally, the structure of the electrodes in this type of element is as shown in FIG. The electrode 3 was formed using a metal such as ln by a vapor deposition method or the like, and the element 1 and the electrode 3 were formed so as to be in ohmic contact.
しかし素子の電極間の寸法iが小さくなると光信号によ
って発生した少数キャリアが受光部中で自然に消滅する
寿命時間程度すなわち拡散長程度以下になると、該少数
キャリアが寿命時間以内に前記オーム性接触の領域にほ
とんど達し消滅するというスィープアウト(Sweep
out)と呼ばれる現象が起こるため、電極間のバイア
ス電圧をある程度以上高くすると素子の光信号に対する
感度が飽和してしまう欠点があった。However, when the dimension i between the electrodes of the element becomes smaller, and the minority carriers generated by the optical signal naturally disappear in the light receiving part, which is less than the lifetime time, that is, the diffusion length, the minority carriers will contact the ohmic contact within the lifetime time. Sweep out (Sweep
Since a phenomenon called "out" occurs, if the bias voltage between the electrodes is increased beyond a certain level, the sensitivity of the element to the optical signal will become saturated.
そこでこの欠点を除去するために第2図で示すように素
子21と電極23の界面に赤外光は透過するが電気的に
絶縁体である物質、たとえば硫化亜鉛(ZnS)等を葵
着して絶縁体層24を形成し、受光面積を決定する寸法
1は前記ln等の電極により従釆と同様に定め、オーム
性接触の領域のみを受光面22から遠ざけて電極と絶縁
体層とが一部重なり合う構造にし、キャリアの拡散消滅
長より離れた位置に構成することが提案された。Therefore, in order to eliminate this drawback, a material such as zinc sulfide (ZnS), which transmits infrared light but is an electrical insulator, is deposited on the interface between the element 21 and the electrode 23, as shown in FIG. Dimension 1, which determines the light-receiving area, is determined in the same way as for the slave by the electrodes such as ln, and only the area of ohmic contact is kept away from the light-receiving surface 22, so that the electrode and the insulator layer are separated. It was proposed to have a partially overlapping structure and to configure the structure at a position farther than the carrier diffusion/annihilation length.
しかし従来の検知素子を構成している電極は電気信号を
検出する機能のみでなく、受光面積を決定する役割をも
兼備していた。本発明は従来からの製作工程を大きく変
えることなく、前述のスィープァゥトが起こり難い位置
に電極を配設し、素子の受光面積は上記電極上から被着
された赤外光を遮断する電気的絶縁物層に設けた窓で定
めた新規な赤外線検知素子を提供しようとするものであ
る。However, the electrodes that make up conventional sensing elements not only have the function of detecting electrical signals, but also have the role of determining the light-receiving area. The present invention has been developed by arranging electrodes in positions where the above-mentioned sweep is unlikely to occur, without significantly changing the conventional manufacturing process, and by forming an electrically insulated layer on the electrodes to block infrared light. The present invention aims to provide a novel infrared sensing element defined by a window provided in a material layer.
かかる目的を達成するために本発明は赤外線検知素子の
受光面側の両端に電極を配備してなる構造の赤外線検知
器に関して、前記受光面側赤外線素子上の電極端部に一
部がオーバーラップする遮光絶縁層により所望受光部を
構成したことを特徴とするものであって、以下図面を用
いて本発明の一実施例について詳細に説明する。In order to achieve such an object, the present invention relates to an infrared detector having a structure in which electrodes are provided at both ends of the light-receiving surface side of an infrared detecting element, in which electrodes partially overlap the ends of the electrodes on the infrared element on the light-receiving surface side. The present invention is characterized in that a desired light-receiving portion is formed by a light-shielding insulating layer, and one embodiment of the present invention will be described in detail below with reference to the drawings.
まず第3図に示すごとく支持板31、たとえば高比抵抗
Si等の上にHg1‐丈舷Te等からなる赤外線検知素
子用ウェハを接着剤等により接着後、研磨とエッチング
とにより所要の形状のチップ32とする。First, as shown in FIG. 3, a wafer for an infrared sensing element made of Hg1-Length Te is bonded onto a support plate 31, such as high resistivity Si, etc. with an adhesive, and then polished and etched to form the desired shape. It is assumed that the chip is 32.
ただし支持板31は、絶縁性材料からなるサフアィャを
用いてもよい。次いで上記チップ32にメタルマスク等
を用い、電極33をln等の金属で蒸着形成する。ただ
しこの際、電極間隔Lは予定された受光面Aの幅とは一
致せず該受光面の幅よりも大とする。この理由について
は後に詳述する。さらに上記電極33を形成したチップ
32上に該電極端に一部がオーバラッブするように赤外
光を遮断し電気的に絶縁体となる物質、たとえばSi0
2等34を化学蒸着法により被着し、ホトェッチング等
により所定面積の窓を明けてこれを受光面Aとする。However, the support plate 31 may be made of saphire made of an insulating material. Next, using a metal mask or the like on the chip 32, an electrode 33 is formed by vapor deposition of a metal such as ln. However, at this time, the electrode spacing L does not match the planned width of the light receiving surface A, but is made larger than the width of the light receiving surface. The reason for this will be explained in detail later. Further, on the chip 32 on which the electrode 33 is formed, a material that blocks infrared light and becomes an electrical insulator, such as Si0, is placed so as to partially overlap the electrode end.
A second layer 34 is deposited by chemical vapor deposition, and a window of a predetermined area is opened by photoetching or the like to form a light-receiving surface A.
また電極はチップに対し良好なオーム性接触を形成する
ようにする。光伝導型赤外線検知素子は光によって発生
したキャリアが両電極の中間に存在する間だけチップの
導電度の変化、したがって素子の抵抗値変化が現れ、該
キャリアが消滅すればもはや抵抗変化に寄与しなくなる
。The electrodes also make good ohmic contact with the chip. In a photoconductive infrared sensing element, a change in the conductivity of the chip, and therefore a change in the resistance value of the element, occurs only while carriers generated by light exist between the two electrodes, and once the carriers disappear, they no longer contribute to the change in resistance. It disappears.
また同様にキャリアが前記電極のオーム接触領域に達す
ると消滅するため信号の飽和が起こる。ゆえに検知素子
の電極間隔Lは、入射光によって受光部中に発生したキ
ャリアが寿命時間によって消滅するまでに拡散移動する
距離よりも大きくする必要があるわけである。Similarly, when carriers reach the ohmic contact region of the electrode, they disappear, resulting in signal saturation. Therefore, the electrode spacing L of the sensing element needs to be larger than the distance over which the carriers generated in the light receiving section by the incident light diffuse and move before disappearing over the lifetime.
一般に上記の間隔Lを受光面幅1の3倍から7倍に選ぶ
のが好適である。以上のような電極と受光部の構成によ
り受光面Aより入射した信号によって生ずるキャリアが
スイープアゥトにより消滅することを防止し、検知素子
の赤外線に対する応答能力の改善が可能となる。Generally, it is preferable to select the above-mentioned interval L to be 3 to 7 times the width 1 of the light receiving surface. The configuration of the electrode and light receiving section as described above prevents carriers generated by signals incident from the light receiving surface A from disappearing due to sweep-out, and improves the response ability of the sensing element to infrared rays.
さらに検知素子用チップ32上に形成する電極33の間
隔Lは、受光面積を決定する受光面幅1との関係から所
定の間隔で電極を形成しておけば、あとは遮光絶縁層3
4により受光面積を定めればよい。ゆえに各種の所望の
受光面積を持つ検知素子を、また電極部には従来の製作
工程を適用して極めて容易に製作することが可能となる
利点が得られる。なお本発明は、これまでに説明したH
g1−xCdxTeによる光伝導型素子以外のスィープ
アウト現象を持つ光伝導型素子にも適用できることはい
うまでもないことである。Furthermore, the spacing L between the electrodes 33 formed on the sensing element chip 32 is determined by forming the electrodes at a predetermined spacing from the relationship with the light receiving surface width 1 that determines the light receiving area, and then the light shielding insulating layer 33
4, the light receiving area may be determined. Therefore, there is an advantage that sensing elements having various desired light-receiving areas can be manufactured extremely easily by applying conventional manufacturing processes to the electrode portions. Note that the present invention is based on the H
It goes without saying that the present invention can also be applied to photoconductive devices having a sweep-out phenomenon other than photoconductive devices using g1-xCdxTe.
第1図及び第2図は従来の赤外線検知素子の断面図、第
3図は本発明に係る赤外線検知素子の構造を説明するた
めの断面図である。
1,21,32:赤外線検知素子、2,22,A:受光
面、3,23,33:電極、24:絶縁体層、31:支
持板、34:絶縁層、1:受光面積を決定する寸法、L
:電極間隔。
第1図
第2図
第3図1 and 2 are cross-sectional views of a conventional infrared sensing element, and FIG. 3 is a cross-sectional view for explaining the structure of an infrared sensing element according to the present invention. 1, 21, 32: infrared sensing element, 2, 22, A: light-receiving surface, 3, 23, 33: electrode, 24: insulator layer, 31: support plate, 34: insulating layer, 1: determining light-receiving area Dimensions, L
: Electrode spacing. Figure 1 Figure 2 Figure 3
Claims (1)
る赤外線検知素子用チツプを固定し、該チツプ上面の予
定受光窓の両側に電極を形成し、該電極上に一部がオー
バーラツプするように遮光絶縁層を形成し、該絶縁層の
上記両電極の中間にある部分を除去して所定面積の受光
窓を構成したことを特徴とする赤外線検知素子。1. An infrared sensing element chip made of a multi-component semiconductor is fixed on a support plate made of a high resistivity material, and electrodes are formed on both sides of the expected light receiving window on the top surface of the chip, so that the chips partially overlap on the electrodes. 1. An infrared sensing element, comprising: forming a light-shielding insulating layer; and removing a portion of the insulating layer located between the two electrodes to form a light-receiving window of a predetermined area.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP53093821A JPS603793B2 (en) | 1978-07-31 | 1978-07-31 | Infrared sensing element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP53093821A JPS603793B2 (en) | 1978-07-31 | 1978-07-31 | Infrared sensing element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5521142A JPS5521142A (en) | 1980-02-15 |
| JPS603793B2 true JPS603793B2 (en) | 1985-01-30 |
Family
ID=14093055
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP53093821A Expired JPS603793B2 (en) | 1978-07-31 | 1978-07-31 | Infrared sensing element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS603793B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4684812A (en) * | 1983-08-31 | 1987-08-04 | Texas Instruments Incorporated | Switching circuit for a detector array |
| JPS6221282A (en) * | 1985-07-22 | 1987-01-29 | Nippon Telegr & Teleph Corp <Ntt> | Light conducting type detector |
-
1978
- 1978-07-31 JP JP53093821A patent/JPS603793B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5521142A (en) | 1980-02-15 |
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