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JPH01201971A - Infra-red ray detector - Google Patents

Infra-red ray detector

Info

Publication number
JPH01201971A
JPH01201971A JP63025908A JP2590888A JPH01201971A JP H01201971 A JPH01201971 A JP H01201971A JP 63025908 A JP63025908 A JP 63025908A JP 2590888 A JP2590888 A JP 2590888A JP H01201971 A JPH01201971 A JP H01201971A
Authority
JP
Japan
Prior art keywords
crystal layer
forming
layer
compound semiconductor
semiconductor crystal
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
Application number
JP63025908A
Other languages
Japanese (ja)
Inventor
Soichiro Hikita
匹田 聡一郎
Yoshihiro Miyamoto
義博 宮本
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 JP63025908A priority Critical patent/JPH01201971A/en
Publication of JPH01201971A publication Critical patent/JPH01201971A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To reduce crosstalks by forming a crystal layer having an energy band gap greater than that of a crystal layer for forming an element as a buffer layer between a compound semiconductor crystal layer for forming an element and a substrate, and further by providing a light absorber in the bottom of a grove where elements are separated. CONSTITUTION:A compound semiconductor crystal having a higher energy band gap than that of a compound semiconductor crystal layer 13 for forming an element is provided as a buffer layer 12 between an insulating or semi-insulating substrate 11 and a compound semiconductor crystal layer 13 for forming an element. The compound semiconductor crystal layer 13 provided with a PN junction 17 for forming an element is provided with a groove 19 that reaches the buffer layer 12 from the surface of the crystal layer 13 or reaches the substrate 11 from the surface of the crystal layer 13 for forming an element. An infra-red ray detector is arranged by forming the crystal layer 13 for forming an element, or the crystal layer 13 for forming an element laminated in the buffer layer 12 to a mesa form and by providing a light absorber 20. This enables a detecting array having a high pixel density and causing a small number of crosstalks to be arranged. A high-quality detecting array which applies a uniform bias voltage to each photodiode can also be obtained.

Description

【発明の詳細な説明】 〔概 要〕 赤外線検知装置に関し、 検知素子間のクロストークの発生を少なくし、かつ各検
知素子に印加するバイアス電圧が変動しないようにする
ことを目的とし、 絶縁性、或いは半絶縁性基板上に形成した化合物半導体
結晶層の所定の位置にP−N接合を設けてホトダイオー
ドアレイを形成した装置であって、前記基板と素子形成
用の化合物半導体結晶層の間に、該素子形成用化合物半
導体結晶よりエネルギーハンドギャップの大きい化合物
半導体結晶をバッファ層として設け、前記P−N接合部
を設けた素子形成用の化合物半導体結晶層を、該結晶層
表面よりバッファ層に、或いは素子形成用結晶層表面よ
り基板に到達する溝を設けることにより、前記素子形成
用結晶層、或いはバッファ層に積層された素子形成用結
晶層をメリー状に形成するとともに前記溝の底部に光吸
収体を設けて構成する。
[Detailed Description of the Invention] [Summary] Regarding an infrared detection device, the purpose is to reduce the occurrence of crosstalk between detection elements and to prevent fluctuations in the bias voltage applied to each detection element. , or a device in which a photodiode array is formed by providing a P-N junction at a predetermined position of a compound semiconductor crystal layer formed on a semi-insulating substrate, wherein the photodiode array is formed between the substrate and the compound semiconductor crystal layer for element formation. , a compound semiconductor crystal having a larger energy hand gap than the element-forming compound semiconductor crystal is provided as a buffer layer, and the element-forming compound semiconductor crystal layer provided with the P-N junction is disposed in the buffer layer from the surface of the crystal layer. Alternatively, by providing a groove that reaches the substrate from the surface of the crystal layer for element formation, the crystal layer for element formation or the crystal layer for element formation laminated on the buffer layer is formed in a merry shape, and at the bottom of the groove. It is configured by providing a light absorber.

[産業上の利用分野] 本発明は赤外線検知装置に係り、特にアレイ状に形成し
た検知素子間に於けるクロストークの発生を少なくした
赤外線検知装置に関する。
[Industrial Field of Application] The present invention relates to an infrared detection device, and more particularly to an infrared detection device that reduces the occurrence of crosstalk between detection elements formed in an array.

カドミウムテルル(CdTe)のような半絶縁性基板、
或いはリーファイアのような絶縁性基板上に、エネルギ
ーハンドギャップの狭い水銀・カドミラJ、 テルル(
lLg+−1Cd、、Te)のような化合物半導体をエ
ピタキシャル法等を用いて薄層状態に形成し、該化合物
半導体結晶層に所定のパターンのP−N接合を形成して
ポI・ダイオードをアレイ状に形成し、ごのボI−タイ
オードアレイを有する赤外線検知装置と、ソリコン(S
i)基板に形成したマルチプレクリ等の伝号処理装置と
をインジウム(In)金属柱を用いて接続形成して一体
化して赤外線撮像装置を形成している。
Semi-insulating substrates such as cadmium tellurium (CdTe),
Alternatively, on an insulating substrate such as Leefire, mercury, cadmira J, tellurium (with a narrow energy hand gap)
A compound semiconductor such as 1Lg+-1Cd, Te) is formed into a thin layer using an epitaxial method, and a predetermined pattern of PN junctions is formed in the compound semiconductor crystal layer to form an array of PoI diodes. An infrared detection device formed in the shape of
i) An infrared imaging device is formed by connecting and forming a signal processing device such as a multiplexer formed on a substrate using an indium (In) metal pillar.

〔従来の技術〕 従来の赤外線検知装置の構造を第6図に示す。[Conventional technology] The structure of a conventional infrared detection device is shown in FIG.

第6図に示すように、従来の赤外線検知装置はCd T
eよりなる半絶縁性基板1−[−に1〕型のl+1−8
Cd。
As shown in FIG. 6, the conventional infrared detection device uses Cd T
Semi-insulating substrate 1-[-1] type l+1-8 consisting of e
Cd.

Te結晶2か気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の所定位置にはレジストvをマスクと
して用いてイオン注入法を用いてボロン(Bo)原子か
導入され、N゛層3形成されて1)−N接合4が形成さ
れている。更に該結晶層2の表面には、該結晶の陽極酸
化膜、或いは陽極硫化l模か保8W膜5として形成され
てホトダイード6が形成されている。更にこのホトクイ
オート6上の保護膜5は窓開きされ、前記形成されたN
″層3上にはInの金属柱7か茂着により形成されてい
る。
A Te crystal 2 is formed using a vapor phase epitaxial growth method, etc., boron (Bo) atoms are introduced into a predetermined position of the crystal layer 2 using an ion implantation method using a resist v as a mask, and a N layer 3 is formed. 1)-N junction 4 is formed. Further, on the surface of the crystal layer 2, a photodiode 6 is formed as an anodic oxidation film of the crystal or an anodic sulfide 8W film 5. Further, the protective film 5 on the photoquat 6 is opened to allow the formed N
On the ``layer 3, a metal column 7 of In is formed by adhesion.

そしてこの基板1の裏面側より赤外線を入射して、この
入射された赤外線が基板1および化合物半導体結晶層2
を通過し、該結晶層2内で光電変換されてキャリアよな
り、このキャリアを光起電力として検知している。
Then, infrared rays are incident on the back surface side of the substrate 1, and the incident infrared rays are directed to the substrate 1 and the compound semiconductor crystal layer.
The light passes through the crystal layer 2 and is photoelectrically converted into carriers, which are detected as photovoltaic force.

〔発明が解決しよう々ずろ課題〕[Problems that inventions are unlikely to solve]

ところで従来の装置に於いて、第7図(a)に示すよう
に、各タイオート間の距離Sか、CdTe 1の基板の
裏面より化合物半導体結晶2内に導入された赤外線によ
り、光電変換されて形成された少数キャリアの拡散長d
に比して充分大きい場合、各ダイオ−1”6A、5B間
で発生した少数キャリア8は、結晶層2内の例えば×印
の位置で再結合して消滅し、隨接ずろダ・イオード6A
、6Bに到達することがないのてりlニアストークを発
生することは無い。
By the way, in the conventional device, as shown in FIG. 7(a), photoelectric conversion is performed either by the distance S between the tie-outs or by the infrared rays introduced into the compound semiconductor crystal 2 from the back surface of the CdTe 1 substrate. Diffusion length d of minority carriers formed by
, the minority carriers 8 generated between the diodes 1" 6A and 5B recombine and disappear at the position marked with an "X" in the crystal layer 2, and
, 6B will never be reached, and no near-stoke will occur.

然しなから、近年ごの裏面入射型のホトダイオードアレ
イは益々大規模化、高密度に形成することが要求されて
おり、これに伴ってダイオード間の距離Sか少数キャリ
アの拡散長dより小さくなり、この場合は第7図(b)
に示すように、ホトダイオード6A、61’tの間に発
生した少数キャリア8は、随接するホI・ダイオード6
A、6Bに到達してクロストークの現象が生じる問題が
ある。
However, in recent years, back-illuminated photodiode arrays have been required to be larger and more densely formed, and as a result, the distance S between diodes has become smaller than the minority carrier diffusion length d. , in this case Fig. 7(b)
As shown in FIG.
There is a problem that a crosstalk phenomenon occurs when A and 6B are reached.

本発明はト記した問題点を除去し、クロストークの発生
を少なくした赤外線検知装置の提供を目的とする。
It is an object of the present invention to provide an infrared detection device that eliminates the above-mentioned problems and reduces the occurrence of crosstalk.

(課題を解決するだめの手段] 上記した「1的を達成する本発明の赤外線検知装置は、
第1図に示すように絶縁性、或いは半絶縁性基板11と
素子形成用の化合物半導体結晶層13の間に、該素子形
成用化合物半導体結晶層13よりエネルギーハンドギャ
ップの大きい化合物半導体結晶をバッファ層12として
設け、P−N接合部17を設けた素子形成用の化合物半
導体結晶層13を、該結晶層13表面よりバッファ層1
2に、或いは素子形成用結晶層13表面より基板11に
到達する溝19を設けることにより、01■記素子形成
用結晶層13、或いはバッファ層12に積層された素子
形成用結晶層13をメザ状に形成するとともに、前記溝
19の底部に光吸収体20を設けて構成する。
(Means for Solving the Problems) The infrared detection device of the present invention that achieves the above-mentioned “Objective 1” has the following features:
As shown in FIG. 1, a compound semiconductor crystal having a larger energy hand gap than the compound semiconductor crystal layer 13 for forming an element is buffered between an insulating or semi-insulating substrate 11 and a compound semiconductor crystal layer 13 for forming an element. A compound semiconductor crystal layer 13 for forming an element provided as a layer 12 and provided with a P-N junction 17 is layered from the surface of the crystal layer 13 to the buffer layer 1.
2, or by providing a groove 19 reaching the substrate 11 from the surface of the element forming crystal layer 13, the element forming crystal layer 13 laminated on the element forming crystal layer 13 or the buffer layer 12 described in 01. A light absorber 20 is provided at the bottom of the groove 19.

〔作 用〕[For production]

本発明の赤外線検知装置は、該検知装置を構成するホト
ダイオードを形成する素子形成用化合物半導体結晶層1
3と基板11との間に該素子形成用結晶層13よりエネ
ルギーハンドギャップの大きい結品Jj’iをバッファ
ー層12として形成し、また上記ホI・タイオードをメ
゛り型に形成することで、該ダイオード間か確実に素子
分離されるようにする。
The infrared detection device of the present invention includes a compound semiconductor crystal layer 1 for forming an element forming a photodiode constituting the detection device.
By forming a crystal Jj'i having a larger energy hand gap than the element-forming crystal layer 13 between the buffer layer 12 and the substrate 11, and forming the above-mentioned hole diode in a diagonal shape, , ensure element isolation between the diodes.

そして素子分離した溝19の底部に更に光吸収体20を
設りる。このようにすれば第5図に示すように、検知す
べき赤外線が素子形成用の結晶層13で吸収され、−1
−ヤリアとなっても、そのうちの成る少数キャリー7(
電子)aは、該バッファ層12のエネル昌−−バンドギ
ャップ21が広いために伝導帯22の壁Q、二当たって
矢印B方向に移動してバッファ層12側にキャリアが到
達しない。また他の成る少数キャリアbは、価電子帯2
4と伝導帯22との間のハンドギャップ21の狭い素子
形成用結晶層13の領域側に到達してP−N接合部23
を通過して光電流として検知される。
A light absorber 20 is further provided at the bottom of the trench 19 where the elements are separated. In this way, as shown in FIG. 5, the infrared rays to be detected are absorbed by the crystal layer 13 for forming the element, and -1
-Even if it becomes Yaria, the minority carry 7 (
Since the energy band gap 21 of the buffer layer 12 is wide, the electrons a hit the wall Q of the conduction band 22 and move in the direction of arrow B, so that the carriers do not reach the buffer layer 12 side. The other minority carrier b is the valence band 2
4 and the conduction band 22 reaches the narrow region side of the element forming crystal layer 13 and the P-N junction 23
is detected as a photocurrent.

またこの素子形成用結晶層13はメサ環に分離されてい
るのでキャリアは隣接画素にも流れ込まないため、クロ
スl−−りの発生を見なくなる。
Further, since the crystal layer 13 for forming the element is separated into mesa rings, carriers do not flow into adjacent pixels, so that no cross-reflection occurs.

更に本発明では、素子間を分離する溝19の底部乙こ硫
化亜鉛(ZnS)とクロム(Cr)とを積層した光吸収
体20を設けているので、CdTe1板の底部より入射
してP、−N接合部を有するメリ°状の検知素子間に入
射した光は、+’+ii記光吸収体20にて吸収され、
そのため、このような素子間に入射した迷光がマルチプ
レクサに到達し、該マルチプレクサの表面で反射されて
再びP−N接合部へ導入されることがなくなるので更に
クロストーク現象か確実に除去できる。
Furthermore, in the present invention, a light absorber 20 made of a layered layer of zinc sulfide (ZnS) and chromium (Cr) is provided at the bottom of the groove 19 separating the elements, so that light incident on the bottom of the CdTe plate 1, P, The light incident between the meridian-shaped detection elements having the -N junction is absorbed by the light absorber 20 described in +'+ii,
Therefore, such stray light that has entered between the elements will not reach the multiplexer, be reflected on the surface of the multiplexer, and be reintroduced into the PN junction, so that the crosstalk phenomenon can be further reliably eliminated.

更に検知すべき波長の赤外線が透過するバッファ層12
を素子形成用の結晶層13と積層した状態で形成してい
るので結晶層全体の厚さが厚くなり、その厚さの厚く成
ることで結晶層全体のシート抵抗か低くなり、各ホトダ
イオードのそれぞれに印加するバイアス電圧は、各ホト
ダイオードの結晶層の長手方向の位置に対応させて変動
させる必要がなくなり、各ダイオードに印加するバイア
ス電圧は均一な値て良い。
Furthermore, a buffer layer 12 through which infrared rays having a wavelength to be detected is transmitted.
Since it is formed in a laminated state with the crystal layer 13 for element formation, the thickness of the entire crystal layer becomes thick, and the sheet resistance of the entire crystal layer decreases as the thickness increases. It is no longer necessary to vary the bias voltage applied to each photodiode in accordance with the position in the longitudinal direction of the crystal layer of each photodiode, and the bias voltage applied to each diode may have a uniform value.

〔実施例] 以下、図面を用いて本発明の一実施例につき詳細に説明
する。
[Example] Hereinafter, an example of the present invention will be described in detail using the drawings.

第2関は本発明の赤外線検知装置の一実施例の断面図で
10μm ’jl)の波長に感度を有する検知装置であ
る。図示するように本発明の装置は、半絶縁性のCd 
Te4%板11上にエネルキーハンドギャップが0.2
5eVのl1g、−yCdyTe(y=0.3)の結晶
層が30μmの厚さてバッファ層12として形成され、
その上にはエネルキーハンドキャンプか、0.11eV
のHg+−xCd、 Te(x”0.2)の素子形成用
の結晶層13が形成され、該結晶層13の所定位置には
、B゛原子イオン注入されてN゛層14が形成され、該
P−N接合が形成された結晶層13がメサ環にエツチン
グ形成されている。そしてこのメサ構造を形成する溝1
9の底部にはZn3層20A とCr層20Bとを蒸着
により積層形成した光吸収体層20が被着形成され、メ
サの側壁部表面には該結晶層の陽極硫化膜が保護膜15
として形成されている。またメリーの頂部にはInの金
属栓16か茄着により形成されている。
The second section is a cross-sectional view of an embodiment of the infrared detection device of the present invention, and is a detection device sensitive to a wavelength of 10 μm'jl). As shown in the figure, the device of the present invention uses a semi-insulating Cd
Energy key hand gap on Te4% plate 11 is 0.2
A crystal layer of l1g of 5 eV, -yCdyTe (y=0.3) with a thickness of 30 μm is formed as the buffer layer 12,
Above that is the energy hand camp, 0.11eV
A crystal layer 13 for element formation of Hg+-xCd, Te (x"0.2) is formed, and a N layer 14 is formed by implanting B' atomic ions into predetermined positions of the crystal layer 13. The crystal layer 13 in which the P-N junction is formed is etched into a mesa ring.The groove 1 forming this mesa structure is
A light absorber layer 20 formed by laminating a Zn3 layer 20A and a Cr layer 20B by vapor deposition is formed on the bottom of the mesa, and the anodic sulfide film of the crystal layer is formed on the surface of the side wall of the mesa as a protective film 15.
It is formed as. Further, an In metal plug 16 is formed on the top of the merry.

このような本発明の装置の基板11の底部より赤外線を
導入すると、結晶層12は5μm帯以下の波長の光は吸
収するが、5μm帯以上の波長の光は透過するので、5
μm以下の波長の光は結晶層12に吸収され、光電変換
されてキャリアとなる。
When infrared rays are introduced from the bottom of the substrate 11 of the device of the present invention, the crystal layer 12 absorbs light with a wavelength of 5 μm or less, but transmits light with a wavelength of 5 μm or more.
Light with a wavelength of μm or less is absorbed by the crystal layer 12 and photoelectrically converted into carriers.

一方、5μm以上の光は、結晶層12を透過して結晶層
13に到達する。結晶層13は10μm帯より短い光を
吸収するので、5μm〜10μmの波長の光が結晶層1
3て光電変換されてキャリアとなり、p−N接合部17
へ到達して、ホトダイオード18にて検知される。そし
てこの結晶層13で光電変換されたキャリアは、ホトダ
イオ−1・がメサ状に確実に素子分離されているので、
クロストークを発生ずることはない。またバッファ層と
の間にはハント障壁が形成されているので、該結晶層1
3で発生した少数キャリアがバッファ層を介して隣接画
素に流入することもない。
On the other hand, light of 5 μm or more passes through the crystal layer 12 and reaches the crystal layer 13. Since the crystal layer 13 absorbs light shorter than the 10 μm band, light with a wavelength of 5 μm to 10 μm is absorbed by the crystal layer 1.
3, photoelectrically converted into carriers, and p-N junction 17
and is detected by the photodiode 18. The carriers photoelectrically converted in this crystal layer 13 are reliably separated into elements in the photodiode 1 in a mesa shape.
No crosstalk will occur. In addition, since a hunt barrier is formed between the crystal layer 1 and the buffer layer,
Minority carriers generated in step 3 do not flow into adjacent pixels via the buffer layer.

更に溝19の底部に&J光吸収体20か形成されている
ので、CdTeの基板の裏面側より入射し、P−N接合
部17を有するメ・り状の赤外線検知素子に到達しない
迷光は、前記光吸収体20にて吸収されるので、その迷
光か該検知素子の一ヒ部に設置されているマルチプレク
リ′に当たって反射し、その光がP−N接合部に到達し
てクロストークを発生する事故が防止される。
Furthermore, since the &J light absorber 20 is formed at the bottom of the groove 19, stray light that enters from the back side of the CdTe substrate and does not reach the square infrared sensing element having the P-N junction 17 is Since it is absorbed by the light absorber 20, the stray light hits the multiplex filter installed in a part of the detection element and is reflected, and the light reaches the P-N junction and generates crosstalk. Accidents caused by accidents are prevented.

また結晶層12を厚く形成しても、10μm帯の波長の
光は結晶層12を透過するので、検知装置の感度が低下
することがなく、またこのように結晶層12をh゛くす
ることで、化合物半導体結晶層12.13の厚さが厚く
なるので、結晶層12.13のシート抵抗が増加するこ
とがなくなり、従って結晶層13の長手方向の位置によ
って、シート抵抗の増加によってホトダイオードに印加
するバイアス電圧を変動さゼる必要もなくなる。
Furthermore, even if the crystal layer 12 is formed thick, light with a wavelength in the 10 μm band will pass through the crystal layer 12, so the sensitivity of the detection device will not decrease. Since the thickness of the compound semiconductor crystal layer 12.13 becomes thicker, the sheet resistance of the crystal layer 12.13 does not increase. Therefore, depending on the position of the crystal layer 13 in the longitudinal direction, the increase in sheet resistance causes a change in the photodiode. There is no need to vary the applied bias voltage.

また本実施例の他の実施例として第4図に示すように、
素子形成用結晶層12よりバッファ層13を口通して基
板11に到達する溝25を形成し、この溝25上に前記
した光吸収体20を設け、線溝25で分割されたへソフ
ァ層13上に素子形成用結晶層12を積層した状態で、
バッファ層と共に素子形成用結晶層12をメサ状に形成
しても良い。
In addition, as shown in FIG. 4 as another example of this example,
A groove 25 is formed that passes through the buffer layer 13 from the crystal layer 12 for element formation and reaches the substrate 11, and the above-mentioned light absorber 20 is provided on this groove 25, and the bottom layer 13 divided by the linear groove 25 is formed. With the element forming crystal layer 12 laminated thereon,
The element-forming crystal layer 12 may be formed in a mesa shape together with the buffer layer.

このような赤外線検知装置の第1実施例の製造方法に付
いて述へると、第3図(a)に示すようにCdTe基+
F1.11上にエネルギーハンドギャップが0.25e
VのIlg l −y Cdy Te (y−O,J)
のバッファ層12を30μmの厚さて気相エピタキシャ
ル成長にて形成する。
Regarding the manufacturing method of the first embodiment of such an infrared detection device, as shown in FIG. 3(a), CdTe base +
Energy hand gap is 0.25e on F1.11
V's Ilg l -y Cdy Te (y-O, J)
A buffer layer 12 having a thickness of 30 μm is formed by vapor phase epitaxial growth.

次いてその上に、第2図(b)に示すように、エネルギ
ーハンドギャップか0.11eVのHg、−1Cd、 
Te(x−0,2)の素子形成用結晶層13を気相エピ
タキシャル成長により形成する。
Next, as shown in FIG. 2(b), the energy hand gap is 0.11 eV of Hg, -1Cd,
A crystal layer 13 for element formation of Te(x-0,2) is formed by vapor phase epitaxial growth.

次いで第31F(C)に示すように該素子形成用結晶層
13にB゛原子イオン注入してN+層14を形成する。
Next, as shown in 31F (C), B atoms are ion-implanted into the element-forming crystal layer 13 to form an N+ layer 14.

更に第3図(d)に示すように、該11’−N接合が形
成された素子形成用結晶層13を、ホトレジスト膜をマ
スクとして用いてバッファ層12に到達するまでメサ型
にエツチング形成後、前記第1図に示したように、i苗
19の底部にZnS膜2〇八とCr層20Bが積層形成
された光吸収体20を設け、素子形成用結晶層12のメ
サの1!]lI壁部に該結晶層12.13の陽極硫化膜
を陽極硫化膜液を用いて、また第4図に示すように基板
11に到達するまて溝25を形成するとともに、その上
に光吸収体20を設け、素子形成用結晶層13とハンフ
ァ1i12か工、チングされたメサの側壁部に該結晶層
12.13の陽極硫化膜15を前記第2図(a)に示し
たようにして形成しても良い。
Further, as shown in FIG. 3(d), the element forming crystal layer 13 in which the 11'-N junction is formed is etched into a mesa shape using a photoresist film as a mask until it reaches the buffer layer 12. As shown in FIG. 1, a light absorber 20 in which a ZnS film 208 and a Cr layer 20B are laminated is provided at the bottom of the i-sapling 19, and one of the mesas of the element-forming crystal layer 12 is provided. ] The anode sulfide film of the crystal layer 12.13 is formed on the II wall using an anode sulfide film solution, and as shown in FIG. The absorber 20 is provided, the crystal layer 13 for element formation and the Hanwha 1i12 are processed, and the anodic sulfide film 15 of the crystal layer 12.13 is formed on the side wall of the chimed mesa as shown in FIG. 2(a). It may be formed by

〔発明の効果〕〔Effect of the invention〕

以上の説明から明らかなように本発明によれば、クロス
1−一りの発生の少ない、高画素密度の検知アレイを構
成でき、また各ホトダイオードに印加するバイアス電圧
が均一となる高品質な赤外線検知装置が得られる効果が
ある。
As is clear from the above description, according to the present invention, it is possible to construct a detection array with high pixel density and less occurrence of cross 1-1, and also to provide high-quality infrared rays with uniform bias voltage applied to each photodiode. This has the effect of providing a detection device.

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

第1図は本発明の赤外線検知装置の原理構成回、第2図
は本発明の赤外線検知装置の第1実施例の断面図、 第3図(a)より第3図(d)迄は第1実施例の装置の
製造方法を示す断面図、 第4図は本発明の第2実施例の赤外線検知装置の断面図
、 第5図は本発明の装置に於りる−)−ヤリアの状態の説
明図、 第6図は従来の赤外線検知装置の断面図、第7図(a)
および第7図(b)は従来の装置の不都合な状態の説明
図である。 図において、 11ばCdTe基板、12はバッファ層(Hgl−yC
dyTeの結晶層)、13は素子形成用結晶層(tlg
l−8CdXT(!の結晶層)、14はN゛層、15は
保護膜、16はIn金属柱、17.23はP−N接合部
、18はボI・ダイオード、19.25は溝、20は光
吸収体、20AはZnS膜、20BはCr層、21はエ
ネルギーハンドギャップ、22は伝導帯、24は価電子
帯を示す。 代理人 弁理士  井 桁 貞 −
FIG. 1 is a diagram showing the basic structure of the infrared detection device of the present invention, FIG. 2 is a sectional view of the first embodiment of the infrared detection device of the present invention, and FIG. Fig. 4 is a cross-sectional view of an infrared detection device according to a second embodiment of the present invention, and Fig. 5 is a cross-sectional view showing a method of manufacturing the device of the first embodiment. Fig. 6 is a cross-sectional view of a conventional infrared detection device, Fig. 7(a)
FIG. 7(b) is an explanatory diagram of an inconvenient state of the conventional device. In the figure, 11 is a CdTe substrate, 12 is a buffer layer (Hgl-yC
dyTe crystal layer), 13 is a crystal layer for element formation (tlg
l-8CdXT (crystal layer of !), 14 is N layer, 15 is protective film, 16 is In metal column, 17.23 is P-N junction, 18 is BoI/diode, 19.25 is groove, 20 is a light absorber, 20A is a ZnS film, 20B is a Cr layer, 21 is an energy hand gap, 22 is a conduction band, and 24 is a valence band. Agent Patent Attorney Sada Igata −

Claims (1)

【特許請求の範囲】  絶縁性、或いは半絶縁性基板(11)上に形成した化
合物半導体結晶層(13)の所定の位置にP−N接合を
設けてホトダイオードアレイを形成した装置であって、 前記基板(11)と素子形成用の化合物半導体結晶層(
13)の間に、該素子形成用化合物半導体結晶よりエネ
ルギーハンドギャップの大きい化合物半導体結晶層(1
2)をバッファ層として設け、前記P−N接合部を設け
た素子形成用の化合物半導体結晶層(13)を、該結晶
層(13)表面よりバッファ層(12)に、或いは素子
形成用結晶層(13)表面より基板(11)に到達する
溝(19)を設けることにより、前記素子形成用結晶層
(13)、或いはバッファ層(12)に積層された素子
形成用結晶層(13)をメサ状に形成するとともに、前
記溝の底部に光吸収体(20)を設けたことを特徴とす
る赤外線検知装置。
[Claims] A device in which a photodiode array is formed by providing a P-N junction at a predetermined position of a compound semiconductor crystal layer (13) formed on an insulating or semi-insulating substrate (11), The substrate (11) and a compound semiconductor crystal layer for element formation (
13), a compound semiconductor crystal layer (1
2) is provided as a buffer layer, and the compound semiconductor crystal layer (13) for forming an element provided with the P-N junction is transferred from the surface of the crystal layer (13) to the buffer layer (12), or the crystal for forming an element. By providing a groove (19) reaching the substrate (11) from the surface of the layer (13), the crystal layer (13) for forming an element is laminated on the crystal layer (13) for forming an element or the buffer layer (12). An infrared detection device characterized in that the groove is formed into a mesa shape, and a light absorber (20) is provided at the bottom of the groove.
JP63025908A 1988-02-05 1988-02-05 Infra-red ray detector Pending JPH01201971A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63025908A JPH01201971A (en) 1988-02-05 1988-02-05 Infra-red ray detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63025908A JPH01201971A (en) 1988-02-05 1988-02-05 Infra-red ray detector

Publications (1)

Publication Number Publication Date
JPH01201971A true JPH01201971A (en) 1989-08-14

Family

ID=12178879

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63025908A Pending JPH01201971A (en) 1988-02-05 1988-02-05 Infra-red ray detector

Country Status (1)

Country Link
JP (1) JPH01201971A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04217363A (en) * 1990-03-07 1992-08-07 Santa Barbara Res Center Control of optical crosstalk between adjacent photodetection areas
US5177580A (en) * 1991-01-22 1993-01-05 Santa Barbara Research Center Implant guarded mesa having improved detector uniformity
WO2002007226A1 (en) * 2000-07-18 2002-01-24 Nippon Sheet Glass Co., Ltd. Photodetector array

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04217363A (en) * 1990-03-07 1992-08-07 Santa Barbara Res Center Control of optical crosstalk between adjacent photodetection areas
US5177580A (en) * 1991-01-22 1993-01-05 Santa Barbara Research Center Implant guarded mesa having improved detector uniformity
WO2002007226A1 (en) * 2000-07-18 2002-01-24 Nippon Sheet Glass Co., Ltd. Photodetector array
US6828541B2 (en) 2000-07-18 2004-12-07 Nippon Sheet Glass Co., Ltd. Light receiving element array having isolated pin photodiodes

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