JPH01228180A - Infrared ray detecting element - Google Patents
Infrared ray detecting elementInfo
- Publication number
- JPH01228180A JPH01228180A JP63055799A JP5579988A JPH01228180A JP H01228180 A JPH01228180 A JP H01228180A JP 63055799 A JP63055799 A JP 63055799A JP 5579988 A JP5579988 A JP 5579988A JP H01228180 A JPH01228180 A JP H01228180A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- junction
- super lattice
- substrate
- cdte
- 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.)
- Pending
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- Light Receiving Elements (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
- Solid State Image Pick-Up Elements (AREA)
- Element Separation (AREA)
Abstract
Description
【発明の詳細な説明】
〔概 要〕
多素子型の光起電力型の赤外線検知素子に藺し、検知素
子で処理された信号がクロストークを生じるのを防止す
るのを目的とし、
基板上に設けた水銀・テルルとカドミウム・テルルの超
格子層に島状の前記超格子層の相互拡散層を形成し、該
超格子層上に化合物半導体層を設け、該化合物半導体層
の前記相互拡散層に対応する領域にP−N接合部を設け
て素子を形成したことで構成する。[Detailed Description of the Invention] [Summary] The present invention is applied to a multi-element type photovoltaic infrared sensing element, and is intended to prevent crosstalk from occurring in signals processed by the sensing element. An island-shaped interdiffusion layer of the superlattice layer is formed in the superlattice layer of mercury/tellurium and cadmium/tellurium, a compound semiconductor layer is provided on the superlattice layer, and the interdiffusion layer of the compound semiconductor layer is formed. It is constructed by forming an element by providing a P-N junction in a region corresponding to the layer.
本発明は赤外線検知素子に係り、特に多素子型の光起電
力型の赤外線検知素子に関する。The present invention relates to an infrared sensing element, and particularly to a multi-element photovoltaic infrared sensing element.
エネルギーバンドギャップの狭い水銀・カドミウム・テ
ルル(Hg+−xcdx Te)の結晶を用いて赤外線
検知素子が形成されており、この検知素子で得られる画
像を高解像度の状態で得るために、前記結晶に赤外線検
知素子を多数アレイ状に配設した多素子型赤外線検知素
子が開発されている。An infrared sensing element is formed using a mercury-cadmium-tellurium (Hg+-xcdx Te) crystal with a narrow energy band gap, and in order to obtain a high-resolution image with this sensing element, the crystal is A multi-element type infrared sensing element in which a large number of infrared sensing elements are arranged in an array has been developed.
ところで素子を高密度に配設するにつれて、光電変換さ
れた少数キャリアの拡散長の寸法より素子間の寸法が短
くなると素子で処理された画像信号にクロストークを発
生する問題が生じ、このクロストークの問題を解消する
素子の開発が望まれている。However, as elements are arranged at a higher density, the problem arises that crosstalk occurs in image signals processed by the elements when the distance between the elements becomes shorter than the diffusion length of photoelectrically converted minority carriers. It is desired to develop a device that solves this problem.
〔従来の技術]
従来の多素子型の光起電力型の赤外線検知素子の構造を
第3図に示す。[Prior Art] The structure of a conventional multi-element photovoltaic infrared sensing element is shown in FIG.
図示するように、従来の赤外線検知素子は、カドミウム
・亜鉛・テルル(CdZnTe)のような化合物半導体
基板1上に水銀空孔子をアクセプタとするP型のHgl
□Cdx Teの結晶層2が液相エピタキシャル成長法
等を用いて形成され、該結晶層2内には所定のパターン
にボロン(B゛)原子がイオン注入されてN型層3が形
成され、該結晶層2の表面には硫化亜鉛(ZnS)より
なる保護膜4が形成され、前記N型層3上が窓開きされ
、該N型層3上に電極5が形成されて多素子型の光起電
力型の赤外線検知素子が形成され、前記P−N接合部6
が1画素に対応している。As shown in the figure, the conventional infrared sensing element has P-type Hgl having mercury vacancies as acceptors on a compound semiconductor substrate 1 such as cadmium-zinc-tellurium (CdZnTe).
□Cdx A crystal layer 2 of Te is formed using a liquid phase epitaxial growth method or the like, and boron (B) atoms are ion-implanted into the crystal layer 2 in a predetermined pattern to form an N-type layer 3. A protective film 4 made of zinc sulfide (ZnS) is formed on the surface of the crystal layer 2, a window is opened on the N-type layer 3, and an electrode 5 is formed on the N-type layer 3 to form a multi-element type light. An electromotive force type infrared sensing element is formed at the P-N junction 6.
corresponds to one pixel.
このような検知素子を用いて赤外線を信号処理する場合
、第3図に示すように基板1の背面側より赤外線を矢印
Aに示すように入射させるが、この赤外線が”gl−X
CdXTeの結晶層2で光電変換された光励起キャリ
ア7はP−N接合部6、或いは該P−N接合部6に隣接
するP−N接合部8の両方の方向に矢印BおよびC方向
に移動できるため、画素間のクロストークが発生し、高
解像度の撮像ができない問題がある。When signal processing of infrared rays is performed using such a detection element, as shown in FIG.
The photoexcited carriers 7 photoelectrically converted in the CdXTe crystal layer 2 move in the directions of arrows B and C in both directions of the P-N junction 6 or the P-N junction 8 adjacent to the P-N junction 6. As a result, crosstalk between pixels occurs, making it impossible to capture high-resolution images.
このクロストークが発生する傾向は損保された画像の高
解像度化を図るために、素子を高密度に配設し、キャリ
アの拡散長に対して素子間の距離CP−N接合部間の水
平方向の距離りが短くなるにつれて大きくなる。The tendency for this crosstalk to occur is that in order to increase the resolution of non-life insurance images, the elements are arranged in a high density, and the distance between the elements is relative to the carrier diffusion length in the horizontal direction between the CP-N junctions. becomes larger as the distance becomes shorter.
本発明は上記した問題点を除去し、クロストークを発生
しない高品位の赤外線検知素子の提供を目的とする。The present invention aims to eliminate the above-mentioned problems and provide a high-quality infrared sensing element that does not generate crosstalk.
本発明の赤外線検知素子は第1図に示すように、基板1
1上に設けた水銀・テルルとカドミウム・テルルの超格
子層12に島状の前記超格子層の相互拡散層13を形成
し、該超格子層上に化合物半導体層14を設け、該化合
物半導体層14の前記相互拡散層13に対応する6g域
にP−N接合部15を設けて素子を形成して構成する。As shown in FIG. 1, the infrared sensing element of the present invention has a substrate 1
An island-shaped mutual diffusion layer 13 of the superlattice layer is formed on the superlattice layer 12 of mercury/tellurium and cadmium/tellurium provided on the superlattice layer 1, and a compound semiconductor layer 14 is provided on the superlattice layer. A device is constructed by providing a PN junction 15 in a 6g region of the layer 14 corresponding to the interdiffusion layer 13.
(作 用〕
7kS艮・テルル
Te)の結晶を数100人程S0厚さに分子線エピタキ
シャル成長法や、有機金属CVD法(MOCVD法)等
を用いて周期的に積層した超格子層12のエネルギーバ
ンドギャップは、この両者の結晶、即ちl1gTeとC
dTeの結晶を相互拡散して形成したHg+−x Cd
、 Teの相互拡散層13のエネルギーバンドギャップ
に比して小さく、この超格子層領域12では短波長の光
を透過しないとともにキャリアが再結合されやすい。(Function) The energy of the superlattice layer 12 is made by periodically laminating several 100 7 kS tellurium (Te) crystals to a thickness of SO using molecular beam epitaxial growth, metal organic CVD (MOCVD), etc. The bandgap of both crystals, namely l1gTe and C
Hg+-x Cd formed by mutual diffusion of dTe crystals
, is smaller than the energy bandgap of the Te interdiffusion layer 13, and this superlattice layer region 12 does not transmit short wavelength light and carriers are easily recombined.
そのため、基板上にHgTeとCdTeの超格子層12
を形成し、この超格子層12を熱処理して島状のl(g
TeとCdTeの相互拡散層13のHg+−x CdX
Teの結晶層を形成し、この超格子層12の上に更に素
子形成用のngl□Cd++ Teの結晶層14を設け
、前記相互拡散層13に対応した素子形成用のHg+−
x Cdx Teの結晶層14内に素子形成用のP−N
接合部15を設けることで、基板の背面側より入射した
光で水平方向の素子の間の位置に入射する光を吸収する
とともに、その位置で光電変換されたキャリアが、前記
エネルギーバンドギャップの狭い超格子層12の部分で
再結合されるため、P−N接合部15の素子に到達せず
、そのためクロストークの発生が無くなる。Therefore, a superlattice layer 12 of HgTe and CdTe is formed on the substrate.
is formed, and this superlattice layer 12 is heat-treated to form island-like l(g
Hg+-x CdX of Te and CdTe mutual diffusion layer 13
A crystal layer of Te is formed, and on this superlattice layer 12, a crystal layer 14 of ngl□Cd++ Te is further provided for forming an element.
x Cdx P-N for element formation in the Te crystal layer 14
By providing the bonding portion 15, light incident from the back side of the substrate is absorbed at a position between the elements in the horizontal direction, and carriers photoelectrically converted at that position are transferred to the narrow energy bandgap. Since they are recombined at the superlattice layer 12, they do not reach the elements at the PN junction 15, thereby eliminating crosstalk.
以下、図面を用いながら本発明の一実施例につき詳細に
説明する。Hereinafter, one embodiment of the present invention will be described in detail with reference to the drawings.
第1図に示すように本発明の赤外線検知素子はCdTe
基板、或いはCdZnTe基板11の表面に、HgTe
−CdTeよりなる超格子層12が5μmの厚さに分子
線エピタキシャル成長法、或いは有機金属CVD法(M
OCVD)を用いて形成され、該超格子層12には所定
のパターンにレーザアニール等の手法を用いてHgTe
とCdTeの島状の相互拡散層のHg+−++ Cd.
Teの結晶層13が形成されている。更にこの超格子
層12上には水銀空孔子をアクセプタとしたP型の素子
形成用のl1g+−x Cdx Teの結晶層14が形
成され、この素子形成用のHgl−0CdえTeの結晶
層14の前記相互拡散層13に対応した領域にB°原子
がイオン注入されてN型層16が形成され、P−N接合
部15が形成されている。As shown in FIG. 1, the infrared sensing element of the present invention is made of CdTe.
HgTe on the surface of the substrate or CdZnTe substrate 11
- The superlattice layer 12 made of CdTe is grown to a thickness of 5 μm by molecular beam epitaxial growth method or metal organic CVD method (M
The superlattice layer 12 is formed using a method such as laser annealing in a predetermined pattern to form HgTe.
and CdTe island-like interdiffused layer of Hg+-++ Cd.
A crystal layer 13 of Te is formed. Further, on this superlattice layer 12, a crystal layer 14 of l1g+-x Cdx Te for forming a P-type element using mercury vacancies as acceptors is formed, and a crystal layer 14 of Hgl-0CdTe for forming this element. B° atoms are ion-implanted into a region corresponding to the interdiffusion layer 13 to form an N-type layer 16, and a PN junction 15 is formed.
更に基板トにZnSよりなる表面保護膜17が形成され
、N型層16上が開口されてInよりなる電極18が設
けられている。Further, a surface protection film 17 made of ZnS is formed on the substrate, and an electrode 18 made of In is provided with an opening on the N-type layer 16.
このような赤外線検知素子を形成するには、第2図(a
)に示すようにCdTe基板、或いはCdZnTe基板
11の表面に、11gTe層12Aを126人の厚さで
、CdTeの結晶層12Bを54人の厚さに交互に周期
的に分子線エピタキシ、ヤル成長法、或いはMOCVD
法を用いて形成し、これ等の結晶層12A、12Bの和
が総計で5μm程度の厚さになるようにしてHgTe−
CdTeの超格子層12を形成する。In order to form such an infrared sensing element, the steps shown in FIG.
), on the surface of a CdTe substrate or a CdZnTe substrate 11, an 11 g Te layer 12A with a thickness of 126 g and a CdTe crystal layer 12B with a thickness of 54 g were alternately and periodically subjected to molecular beam epitaxy and yellow growth. law or MOCVD
HgTe-
A CdTe superlattice layer 12 is formed.
次いで第2図[有])に示すように、該基板上にへ〇等
の金属マスク21を設置し、該金属マスクを用いて静ガ
スレーザ等を用いて矢印り方向に沿ってレーザ光を照射
し、レーザアニールしてHgTeとCdTeの相互拡散
を行って30μmのピッチでかつ20μmX 20 u
m程度のHg6.7 Cd5.3 Teの相互拡散層
13を島状に形成する。Next, as shown in FIG. 2 [ex.], a metal mask 21 such as 〇 is placed on the substrate, and a static gas laser or the like is used to irradiate laser light along the direction of the arrow using the metal mask. Then, laser annealing was performed to mutually diffuse HgTe and CdTe, and the pitch was 30 μm and 20 μm x 20 μm.
A mutual diffusion layer 13 of Hg6.7 Cd5.3 Te with a thickness of about 1.5 m is formed in an island shape.
次いで第2図(C)に示すように、前記形成した相互拡
散層13を設けた超格子層12上に水銀空孔子をアクセ
プタとしたP型の素子形成用のHgo、z Cdo、z
Teの化合物半導体結晶層14を形成する。Next, as shown in FIG. 2(C), Hgo,z Cdo,z for forming a P-type element using mercury vacancies as acceptors is placed on the superlattice layer 12 provided with the formed interdiffusion layer 13.
A Te compound semiconductor crystal layer 14 is formed.
次いで素子形成用結晶層14で前記相互拡散層13に対
応した領域に、B“原子を加速電圧120KeV、ドー
ズM1×1014/CT113の条件でイオン注入して
N型層16を形成してP−N接合部15を形成した後、
前記した第1図に示すようにZnSより保護膜17を蒸
着により形成後、N型層16上を開口してInよりなる
電極18を蒸着により形成して多素子型の赤外線検知素
子を形成する。Next, B" atoms are ion-implanted into the region corresponding to the interdiffusion layer 13 in the element forming crystal layer 14 under the conditions of an acceleration voltage of 120 KeV and a dose of M1 x 1014/CT113 to form an N-type layer 16. After forming the N-junction 15,
As shown in FIG. 1, a protective film 17 made of ZnS is formed by vapor deposition, and then an electrode 18 made of In is formed by vapor deposition with an opening on the N-type layer 16 to form a multi-element type infrared sensing element. .
このようにすれば、77°にの温度で相互拡散により形
成したHga、 t Cdo、 3 Teの結晶層13
のエネルギーバンドギャップは約0.25eVで、前記
HgTe −CdTe1格子層12はエネルギーバンド
ギャップが、約0.1eVであるのでエネルギーバンド
ギャップの狭いl1gTe−CdTe超格子層12の方
が、相互拡散層のHg。、7 Cdo、3 Teの結晶
層13よりキャリアが再結合されやすいため、基板11
の裏面より入射した赤外線のうち、多数形成されている
P−N接合部15の水平方向の間に位置する領域に入射
する光を吸収すると同時にその領域で発生したキャリア
はエネルギーバンドギャップの狭い超格子層12で容易
に再結合されて消滅するため、クロストークの発生を見
ない高信顛度の赤外線検知素子が得られる。In this way, the crystal layer 13 of Hga, tCdo, 3Te formed by interdiffusion at a temperature of 77°
The energy bandgap of is about 0.25 eV, and the energy bandgap of the HgTe-CdTe1 lattice layer 12 is about 0.1eV. Therefore, the I1gTe-CdTe superlattice layer 12 with a narrower energy bandgap is better than the interdiffusion layer. of Hg. , 7 Cdo, 3 Te crystal layer 13 because carriers are more easily recombined in the substrate 11.
Among the infrared rays incident from the back surface of the PN junction 15, the light incident on the region located between the horizontal direction of the many formed P-N junctions 15 is absorbed, and at the same time, the carriers generated in that region are Since they are easily recombined and disappear in the grating layer 12, a highly reliable infrared sensing element with no crosstalk can be obtained.
以上の説明から明らかなように本発明によれば、クロス
トークの発生を見ない高信頬度の多素子型赤外線検知素
子が容易に得られる効果がある。As is clear from the above description, according to the present invention, a highly reliable multi-element infrared sensing element that does not cause crosstalk can be easily obtained.
第1図は本発明の素子の構成図、
第2図(a)より第2図(C)迄は本発明の素子の製造
方法を示す断面図、
第3図は従来の赤外線検知素子の断面図である。
図において、
11は基板(CdTe基板、ZnCdTe基板)、12
は)IgTe−CdTe超格子層、12八はIIgTe
の結晶層、12BはCdTeの結晶層、13は相互拡散
層(llgo、 7cdo、 3Te結晶層)、14は
化合物半導体結晶層、15はP−N接合部、16はN型
層、17は保護膜、18は電極、21は金属マスクを示
す。
苓光朗4し構へ?
第1図
+(1
4仝谷口J■−1知(遺ガJ5末T跡拍yfガま/lt
、、’l−,’幻鮭ワ1知斯介必第3図Fig. 1 is a block diagram of the element of the present invention, Fig. 2(a) to Fig. 2(C) are cross-sectional views showing the method of manufacturing the element of the present invention, and Fig. 3 is a cross-section of a conventional infrared sensing element. It is a diagram. In the figure, 11 is a substrate (CdTe substrate, ZnCdTe substrate), 12
) IgTe-CdTe superlattice layer, 128 is IIgTe
12B is a CdTe crystal layer, 13 is an interdiffusion layer (LLGO, 7CDO, 3Te crystal layer), 14 is a compound semiconductor crystal layer, 15 is a P-N junction, 16 is an N-type layer, 17 is a protection layer. 18 is an electrode, and 21 is a metal mask. Reikoro goes to 4th place? Fig.1
,,'l-,'Phantom Salmon Wa 1 Chisisuke Must Figure 3
Claims (1)
テルルの超格子層(12)に島状の前記超格子層の相互
拡散層(13)を形成し、該超格子層上に化合物半導体
層(14)を設け、該化合物半導体層(14)の前記相
互拡散層(13)に対応する領域にP−N接合部(15
)を設けて素子を形成したことを特徴とする赤外線検知
素子。Mercury, tellurium and cadmium provided on the substrate (11)
An island-shaped interdiffusion layer (13) of the superlattice layer is formed on the tellurium superlattice layer (12), a compound semiconductor layer (14) is provided on the superlattice layer, and a compound semiconductor layer (14) is formed on the superlattice layer (12). A P-N junction (15) is provided in a region corresponding to the interdiffusion layer (13).
) is provided to form an element.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63055799A JPH01228180A (en) | 1988-03-08 | 1988-03-08 | Infrared ray detecting element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63055799A JPH01228180A (en) | 1988-03-08 | 1988-03-08 | Infrared ray detecting element |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH01228180A true JPH01228180A (en) | 1989-09-12 |
Family
ID=13008961
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63055799A Pending JPH01228180A (en) | 1988-03-08 | 1988-03-08 | Infrared ray detecting element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01228180A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0870113A (en) * | 1994-08-29 | 1996-03-12 | Nec Corp | Fabrication of infrared detector array |
| JP2009206175A (en) * | 2008-02-26 | 2009-09-10 | Hamamatsu Photonics Kk | Semiconductor light receiving element |
-
1988
- 1988-03-08 JP JP63055799A patent/JPH01228180A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0870113A (en) * | 1994-08-29 | 1996-03-12 | Nec Corp | Fabrication of infrared detector array |
| JP2009206175A (en) * | 2008-02-26 | 2009-09-10 | Hamamatsu Photonics Kk | Semiconductor light receiving element |
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