JP2597550B2 - Photoelectron beam conversion element - Google Patents

Photoelectron beam conversion element

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Publication number
JP2597550B2
JP2597550B2 JP14123486A JP14123486A JP2597550B2 JP 2597550 B2 JP2597550 B2 JP 2597550B2 JP 14123486 A JP14123486 A JP 14123486A JP 14123486 A JP14123486 A JP 14123486A JP 2597550 B2 JP2597550 B2 JP 2597550B2
Authority
JP
Japan
Prior art keywords
type semiconductor
electron beam
junctions
electron emission
emission surface
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 - Fee Related
Application number
JP14123486A
Other languages
Japanese (ja)
Other versions
JPS62299088A (en
Inventor
守 宮脇
幸男 増田
竜一 新井
伸俊 水澤
恭彦 石渡
仁 織田
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP14123486A priority Critical patent/JP2597550B2/en
Publication of JPS62299088A publication Critical patent/JPS62299088A/en
Priority to US07/331,007 priority patent/US4906894A/en
Application granted granted Critical
Publication of JP2597550B2 publication Critical patent/JP2597550B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は光電子ビーム変換素子に関し、特に固体電子
ビーム発生装置を用いた光電子ビーム変換素子に関する
ものである。
Description: TECHNICAL FIELD The present invention relates to a photoelectron beam conversion device, and more particularly to a photoelectron beam conversion device using a solid-state electron beam generator.

〔従来の技術〕[Conventional technology]

固体電子ビーム発生装置として、半導体中に形成され
た異種接合に電界を印加して半導体表面から外部に電子
ビームを放射させる装置が知られている。
2. Description of the Related Art As a solid-state electron beam generator, there has been known an apparatus that applies an electric field to a heterogeneous junction formed in a semiconductor to emit an electron beam from a semiconductor surface to the outside.

例えば特公昭54−30274号公報には、AlPとGaPの混晶
に形成したn−p接合に順方向電圧を印加してP型領域
の表面から電子を放出させる装置が開示されている。特
開昭54−111272号公報には半導体表面の絶縁層に設けた
開口内に少くとも一部を露出させたp−n接合に逆方向
電圧を印加し、かつ開口の縁まで絶縁層に加速電極を設
けている固体電子ビーム発生装置が、また特開昭56−15
529号公報には、半導体表面の絶縁層に設けた開口部の
縁部に加速電極を設け、開口内で半導体表面に平行に伸
長しているp−n接合に逆方向電圧を加えて半導体外部
に電子を放出させる半導体装置が開示され、またこれら
特開昭54−111272号公報、特開昭56−15529号公報には
それぞれ半導体基板上に集積された電子ビーム発生装置
が開示されている。また特開昭57−38528号公報には、
p−n接合に順方向バイアス電圧をかけて半導体表面か
ら電子を放出させる素子を半導体基板上に集積させたマ
ルチ冷電子放出陰極が開示されている。
For example, Japanese Patent Publication No. 54-30274 discloses a device in which a forward voltage is applied to an np junction formed of a mixed crystal of AlP and GaP to emit electrons from the surface of a P-type region. Japanese Patent Application Laid-Open No. 54-111272 discloses that a reverse voltage is applied to a pn junction at least partially exposed in an opening provided in an insulating layer on a semiconductor surface, and the insulating layer is accelerated to the edge of the opening. A solid-state electron beam generator provided with electrodes is disclosed in
No. 529 discloses that an acceleration electrode is provided at an edge of an opening provided in an insulating layer on a semiconductor surface, and a reverse voltage is applied to a pn junction extending parallel to the semiconductor surface in the opening to apply a reverse voltage to the semiconductor. A semiconductor device that emits electrons is disclosed in Japanese Patent Application Laid-Open Nos. 54-111272 and 56-15529, each of which discloses an electron beam generator integrated on a semiconductor substrate. Also, JP-A-57-38528 discloses that
There is disclosed a multi-cold electron emission cathode in which an element for emitting electrons from a semiconductor surface by applying a forward bias voltage to a pn junction is integrated on a semiconductor substrate.

これらの固体電子ビーム発生装置は、小型でかつp−
n接合に印加する電圧により電子放出を変調できる等の
多くの利点を有する。小型化できる利点をいかし、複数
個の電子ビームを配置した装置が考えられるが、その電
子ビーム発生装置を駆動するための配線が複雑になり問
題点となっていた。
These solid-state electron beam generators are compact and have p-
There are many advantages, such as that electron emission can be modulated by the voltage applied to the n-junction. Taking advantage of the advantage of miniaturization, a device in which a plurality of electron beams are arranged is conceivable. However, wiring for driving the electron beam generating device is complicated, which has been a problem.

一方、D.J.Barteling,J.L.Moll,N.I.Meyerらは、Phy
s.Rev.Vol.130 Number 3(1963)972〜985の中で、p−
n接合に逆方向電圧を印加し、電子なだれを起こし、電
子を発生させる場合、P型領域に光を照射し、電子を励
起し、駆動することもできると報告している。しかし、
励起用の光は、電子ビーム放出側から入射しており、光
電子ビーム変換素子として利用する場合この点が大きな
制約となっていた。
On the other hand, DJBarteling, JLMoll, NIMeyer et al.
130. Number 3 (1963) 972-985, p-
It is reported that when a reverse voltage is applied to an n-junction to cause avalanche and generate electrons, the P-type region can be irradiated with light to excite and drive the electrons. But,
Excitation light is incident from the electron beam emission side, and this point has been a great limitation when used as a photoelectron beam conversion element.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

本発明は、上述した従来例の欠点を除去し、光の入射
と、p−n接合への逆電圧の印加によって簡単な構造で
電子ビームを発生しうる光電子ビーム変換素子を提供す
ることを目的とする。
SUMMARY OF THE INVENTION It is an object of the present invention to provide a photoelectron beam conversion element capable of generating an electron beam with a simple structure by eliminating the above-mentioned drawbacks of the conventional example and by applying light and applying a reverse voltage to a pn junction. And

〔問題点を解決するための手段〕[Means for solving the problem]

このような目的を達成するために、本発明の光電子ビ
ーム変換素子は半導体基板と、該基板上に形成された複
数のp型半導体領域と、該複数のp型半導体領域上に設
けられたそれぞれ電子放出面を有するn型半導体領域
と、前記複数のp型半導体領域と複数のn型半導体領域
によって形成される複数のp−n接合と、前記半導体基
板の前記電子放出面とは反対側の表面から、前記複数の
p−n接合のそれぞれに対応する位置に、前記p型半導
体領域に向かって形成された光入射用の開口部と、該開
口部を有する側に設けられ前記p型半導体領域に電気的
に接続する共通の透明電極と、前記電子放出面を有する
側に設けられ前記n型半導体領域に電気的に接続する共
通電極と、前記透明電極および前記共通電極を介して前
記複数のp−n接合に電子なだれによる降伏電圧より低
い逆方向バイアス電圧を印加する手段とを有することを
特徴とする。
In order to achieve such an object, a photoelectron beam conversion element according to the present invention includes a semiconductor substrate, a plurality of p-type semiconductor regions formed on the substrate, and a plurality of p-type semiconductor regions provided on the plurality of p-type semiconductor regions. An n-type semiconductor region having an electron emission surface, a plurality of pn junctions formed by the plurality of p-type semiconductor regions and the plurality of n-type semiconductor regions, and an opposite side of the semiconductor substrate to the electron emission surface. An opening for light incidence formed toward the p-type semiconductor region at a position corresponding to each of the plurality of pn junctions from a surface; and the p-type semiconductor provided on the side having the opening. A common transparent electrode electrically connected to the region, a common electrode provided on the side having the electron emission surface and electrically connected to the n-type semiconductor region, and the plurality of common electrodes via the transparent electrode and the common electrode. Pn junction And having a means for applying a low reverse bias voltage than the breakdown voltage due to the child avalanche.

〔作 用〕(Operation)

本発明においては基板側に設けた開口部から、光を入
射させ、p−n接合に逆方向電圧を印加することにより
電子ビームを発生させることにより、光信号で電子ビー
ムを容易に発生できる。
In the present invention, light is incident from an opening provided on the substrate side, and an electron beam is generated by applying a reverse voltage to the pn junction, whereby an electron beam can be easily generated by an optical signal.

〔実施例〕〔Example〕

以下、図面を参照して本発明の実施例を詳細に説明す
る。
Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.

第1図は、本発明の第1の実施例を構成する単位素子
の構造を模式的に示す断面図である。第1図において、
1はp型Si基板、2は高濃度ドープp型領域、3はn型
領域、4はp−n接合、5は、仕事関数を低下させる材
料でたとえばセシウム(Cs)薄膜等のもの、6は、絶縁
層たとえば酸化シリコン(Sio2)等、7は電子加速用電
極、8は電極、9は高濃度ドープp型領域の基板側に設
けられた開口部、10はSnO2、ITOなどからなる透明電極
である。このような素子は通常の半導体リソグラフィー
技術によって作製できる。
FIG. 1 is a cross-sectional view schematically showing a structure of a unit element constituting a first embodiment of the present invention. In FIG.
1 is a p-type Si substrate, 2 is a heavily doped p-type region, 3 is an n-type region, 4 is a pn junction, 5 is a work function lowering material such as a cesium (Cs) thin film, etc., 6 Is an insulating layer such as silicon oxide (Sio 2 ), etc., 7 is an electron accelerating electrode, 8 is an electrode, 9 is an opening provided on the substrate side of a highly doped p-type region, and 10 is an SnO 2 , ITO, etc. Transparent electrode. Such a device can be manufactured by a usual semiconductor lithography technique.

次に、本発明の素子の動作原理について説明する。本
素子は、駆動回路DCによりp−n接合に逆バイアスが印
加されている。この印加電圧は、電子なだれを生じ始め
るしきい値電界よりやや低くセットされている。第1図
に示す如く、高濃度p型領域2の裏側の開口部9から入
射した光Lは、透明電極10を透過し、高濃度p型領域2
の電子を励起する。励起された電子がトリガとなり電子
なだれが生じ、n型領域3を通りぬけ、さらに加速電極
7により生じる電界により加速され電子ビームEBが放出
される。n型領域3の表面には、セシウム等の仕事関数
を低下させる材料が蒸着されており、低エネルギーの電
子も放出できる。
Next, the operation principle of the device of the present invention will be described. In this element, a reverse bias is applied to the pn junction by the drive circuit DC. This applied voltage is set slightly lower than a threshold electric field at which avalanche starts to occur. As shown in FIG. 1, the light L incident from the opening 9 on the back side of the high-concentration p-type region 2 passes through the transparent electrode 10 and
Excites electrons. The excited electrons serve as a trigger to cause avalanche of electrons, pass through the n-type region 3, and are accelerated by an electric field generated by the acceleration electrode 7 to emit an electron beam EB. A material that lowers the work function such as cesium is deposited on the surface of the n-type region 3 and can also emit low-energy electrons.

次に、本発明の第2実施例について、第2図を用いて
説明する。第2実施例は、第1実施例に比べて、p型Si
基板1が高濃度p型領域2までエッチングされている点
が異なり動作原理は、第1実施例と同様である。第2実
施例の場合、電子ビーム発生のトリガーとなる光Lが直
接、高濃度p型領域2に当り、電子ビーム発生効率が上
がり、さらに、逆バイアス用電極間隔がせまくなるた
め、駆動電圧が小さくて済む等の利点がある。
Next, a second embodiment of the present invention will be described with reference to FIG. The second embodiment is different from the first embodiment in that the p-type Si
The operation principle is the same as that of the first embodiment except that the substrate 1 is etched to the high concentration p-type region 2. In the case of the second embodiment, the light L, which triggers the generation of the electron beam, directly hits the high-concentration p-type region 2 to increase the efficiency of the electron beam generation and further reduce the reverse bias electrode interval. There are advantages such as small size.

基板1の高濃度p型領域までのエッチング方法として
は、マスクを介してフッ酸硝酸の混合材によりウェット
エッチングを行なう方法、Cl2ガスを用い反応性イオン
エッチングを行なう方法がある。基板間が約500μmと
厚いため、1回のマスクでは、エッチングが終了しない
場合は、数回にわけてマスク形成とエッチングをくり返
せば良い。
As a method of etching up to the high-concentration p-type region of the substrate 1, there are a method of performing wet etching with a mixture of hydrofluoric acid and nitric acid through a mask and a method of performing reactive ion etching using Cl 2 gas. Since the distance between the substrates is as thick as about 500 μm, if the etching is not completed with one mask, the mask formation and etching may be repeated several times.

上述した第1、第2の実施例におけるSiにかえて化合
物半導体を用い得ることは明らかである。
It is clear that a compound semiconductor can be used instead of Si in the first and second embodiments described above.

また第1図、第2図に示した素子は構造が簡単であっ
て、単一基板上に複数の素子を集積化できる。
The elements shown in FIGS. 1 and 2 have a simple structure, and a plurality of elements can be integrated on a single substrate.

第1ないし第2実施例として示した単位素子を複数集
積して形成した本発明の実施例について、第3図を用い
て説明する。本実施例は、上述の単位素子を複数配置し
たもの(MEBS)である。従来、この光電子ビーム変換素
子を複数個集積化し、各々を独立に駆動する場合、各素
子への配線が複雑になり、これが高集積化をはばむ原因
となっていた。本素子の場合、複数個の光電子ビーム変
換素子MEBSは光入力側に共通の透明電極10が設けられ、
一方、電子ビーム出射側のn型領域に共通の電極8が設
けられているだけである。911、912…921、922…、955
はそれぞれ電子ビーム源に対応した開口部である。共通
の透明電極10と共通電極8との間に電子なだれを生じる
電圧よりわずかに小さい逆電圧が印加されており、各電
子ビームの放出は、その電子ビーム源に対応した基板側
の開口部に光が入力された時生じるようになっている。
第3図に示す如く、光L11が入射した電子ビーム発生素
子から電子ビームEB11が、同様に光Lmnに対して電子ビ
ームEBmnが放出される。
An embodiment of the present invention in which a plurality of unit elements shown as the first and second embodiments are integrated will be described with reference to FIG. In this embodiment, a plurality of the above-described unit elements are arranged (MEBS). Conventionally, when a plurality of photoelectron beam conversion elements are integrated and each of them is driven independently, wiring to each element becomes complicated, and this has been a cause of the high integration. In the case of this element, a plurality of photoelectron beam conversion elements MEBS are provided with a common transparent electrode 10 on the light input side,
On the other hand, only the common electrode 8 is provided in the n-type region on the electron beam emission side. 911, 912… 921, 922…, 955
Are openings corresponding to the electron beam sources, respectively. A reverse voltage slightly smaller than a voltage causing an avalanche of electrons is applied between the common transparent electrode 10 and the common electrode 8, and each electron beam is emitted to the opening on the substrate side corresponding to the electron beam source. It occurs when light is input.
As shown in FIG. 3, the electron beam EB11 is emitted from the electron beam generating element on which the light L11 is incident, and the electron beam EBmn is emitted similarly to the light Lmn.

[発明の効果] 以上説明したように、電子なだれを起こし、電子ビー
ムを発生させるタイプの装置において、基板側に開口部
を設けて、光を入射させ、p−n接合に逆方向電圧を印
加することにより電子ビームを発生させることにより、
光信号で電子ビームを容易に発生できるという効果があ
る。本発明の光電子ビーム変換素子は光交換器等にも応
用できる。また、本発明の構成をとることにより、電子
ビーム発生装置としての電気的配線を極めて簡略なもの
とすることができる。
[Effects of the Invention] As described above, in an apparatus that generates an electron avalanche and generates an electron beam, an opening is provided on the substrate side, light is incident, and a reverse voltage is applied to the pn junction. By generating an electron beam by doing
There is an effect that an electron beam can be easily generated by an optical signal. The photoelectron beam conversion device of the present invention can be applied to an optical exchanger and the like. Further, by adopting the configuration of the present invention, the electric wiring as the electron beam generator can be extremely simplified.

【図面の簡単な説明】[Brief description of the drawings]

第1図は、本発明を構成する単位素子の第1の実施例の
断面構造を示す模式図、 第2図は、本発明を構成する単位素子の第2の実施例の
断面構造を示す模式図、 第3図は、第1図ないし第2図に示された単位素子を複
数配置して形成した本発明の実施例の構成を示す模式図
である。 L,L1,LN……光、 EB,EB1,EBN……電子ビーム、 1……p型Si基板、 2……高濃度p型領域、 3……n型領域、 4……p−n接合、 5……仕事関数を低下させる膜、 6……絶縁層、 7……電子加速用電極、 8……電極、 9、911、912−−−−9mn……開口部、 10……透明電極、 DC……素子駆動回路、 MEBS……多光電子ビーム変換素子。
FIG. 1 is a schematic view showing a sectional structure of a first embodiment of a unit element constituting the present invention, and FIG. 2 is a schematic view showing a sectional structure of a second embodiment of a unit element constituting the present invention. FIG. 3 is a schematic diagram showing a configuration of an embodiment of the present invention in which a plurality of unit elements shown in FIGS. 1 and 2 are arranged and formed. L, L1, LN: light, EB, EB1, EBN: electron beam, 1: p-type Si substrate, 2: high-concentration p-type region, 3: ... n-type region, 4: pn junction 5, a film that lowers the work function, 6: an insulating layer, 7: an electrode for accelerating electrons, 8: an electrode, 9, 911, 912 --- 9mn ... an opening, 10: a transparent electrode , DC: Element drive circuit, MEBS: Multi-photoelectron beam conversion element.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 水澤 伸俊 東京都大田区下丸子3丁目30番2号 キ ヤノン株式会社内 (72)発明者 石渡 恭彦 東京都大田区下丸子3丁目30番2号 キ ヤノン株式会社内 (72)発明者 織田 仁 東京都大田区下丸子3丁目30番2号 キ ヤノン株式会社内 (56)参考文献 特開 昭50−23168(JP,A) 特開 昭62−299089(JP,A) ──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Nobutoshi Mizusawa 3-30-2 Shimomaruko, Ota-ku, Tokyo Inside Canon Inc. (72) Inventor Yasuhiko Ishiwatari 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Incorporated (72) Inventor Jin Oda 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc. (56) References JP-A-50-23168 (JP, A) JP-A-62-299089 (JP) , A)

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】半導体基板と、該基板上に形成された複数
のp型半導体領域と、該複数のp型半導体領域上に設け
られたそれぞれ電子放出面を有するn型半導体領域と、
前記複数のp型半導体領域と複数のn型半導体領域によ
って形成される複数のp−n接合と、前記半導体基板の
前記電子放出面とは反対側の表面から、前記複数のp−
n接合のそれぞれに対応する位置に、前記p型半導体領
域に向かって形成された光入射用の開口部と、該開口部
を有する側に設けられ前記p型半導体領域に電気的に接
続する共通の透明電極と、前記電子放出面を有する側に
設けられ前記n型半導体領域に電気的に接続する共通電
極と、前記透明電極および前記共通電極を介して前記複
数のp−n接合に電子なだれによる降伏電圧より低い逆
方向バイアス電圧を印加する手段とを有することを特徴
とする光電子ビーム変換素子。
A semiconductor substrate, a plurality of p-type semiconductor regions formed on the substrate, and an n-type semiconductor region provided on the plurality of p-type semiconductor regions, each having an electron emission surface.
A plurality of p-n junctions formed by the plurality of p-type semiconductor regions and a plurality of n-type semiconductor regions; and a plurality of p-n junctions from a surface of the semiconductor substrate opposite to the electron emission surface.
A light incident opening formed toward the p-type semiconductor region at a position corresponding to each of the n-junctions, and a common hole provided on the side having the opening and electrically connected to the p-type semiconductor region. A common electrode provided on the side having the electron emission surface and electrically connected to the n-type semiconductor region, and electron avalanche to the plurality of pn junctions via the transparent electrode and the common electrode. Means for applying a reverse bias voltage lower than the breakdown voltage caused by the photoelectron beam.
【請求項2】前記電子放出面に仕事関数低下材料よりな
る膜を有することを特徴とする特許請求の範囲第1項に
記載の光電子ビーム変換素子。
2. A photoelectron beam conversion device according to claim 1, wherein said electron emission surface has a film made of a work function lowering material.
JP14123486A 1986-06-19 1986-06-19 Photoelectron beam conversion element Expired - Fee Related JP2597550B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP14123486A JP2597550B2 (en) 1986-06-19 1986-06-19 Photoelectron beam conversion element
US07/331,007 US4906894A (en) 1986-06-19 1989-03-28 Photoelectron beam converting device and method of driving the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14123486A JP2597550B2 (en) 1986-06-19 1986-06-19 Photoelectron beam conversion element

Publications (2)

Publication Number Publication Date
JPS62299088A JPS62299088A (en) 1987-12-26
JP2597550B2 true JP2597550B2 (en) 1997-04-09

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JP14123486A Expired - Fee Related JP2597550B2 (en) 1986-06-19 1986-06-19 Photoelectron beam conversion element

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Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4954864A (en) * 1988-12-13 1990-09-04 The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration Millimeter-wave monolithic diode-grid frequency multiplier
JP2752312B2 (en) * 1993-09-10 1998-05-18 浜松ホトニクス株式会社 Photoelectron emission surface, electron tube and photodetector using the same
JP4455996B2 (en) * 2002-08-09 2010-04-21 浜松ホトニクス株式会社 Photodiode array, manufacturing method thereof, and radiation detector
JP4647955B2 (en) * 2004-08-17 2011-03-09 浜松ホトニクス株式会社 Photocathode plate and electron tube

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5220222B2 (en) * 1973-06-28 1977-06-02

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Publication number Publication date
JPS62299088A (en) 1987-12-26

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