JPH041930B2 - - Google Patents

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Publication number
JPH041930B2
JPH041930B2 JP58196582A JP19658283A JPH041930B2 JP H041930 B2 JPH041930 B2 JP H041930B2 JP 58196582 A JP58196582 A JP 58196582A JP 19658283 A JP19658283 A JP 19658283A JP H041930 B2 JPH041930 B2 JP H041930B2
Authority
JP
Japan
Prior art keywords
light
optical memory
semiconductor
absorption region
light absorption
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
Application number
JP58196582A
Other languages
Japanese (ja)
Other versions
JPS6087443A (en
Inventor
Shunpei Yamazaki
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.)
Semiconductor Energy Laboratory Co Ltd
Original Assignee
Semiconductor Energy Laboratory Co 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 Semiconductor Energy Laboratory Co Ltd filed Critical Semiconductor Energy Laboratory Co Ltd
Priority to JP58196582A priority Critical patent/JPS6087443A/en
Publication of JPS6087443A publication Critical patent/JPS6087443A/en
Publication of JPH041930B2 publication Critical patent/JPH041930B2/ja
Granted legal-status Critical Current

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Classifications

    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/242—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
    • G11B7/243—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/242—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
    • G11B7/243—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
    • G11B2007/24302—Metals or metalloids
    • G11B2007/24312—Metals or metalloids group 14 elements (e.g. Si, Ge, Sn)
    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/242—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
    • G11B7/243—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
    • G11B2007/24318—Non-metallic elements
    • G11B2007/2432—Oxygen
    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/252—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers
    • G11B7/257—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers
    • G11B2007/25705—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of inorganic materials
    • G11B2007/2571—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers having properties involved in recording or reproduction, e.g. optical interference layers or sensitising layers or dielectric layers, which are protecting the recording layers consisting essentially of inorganic materials containing group 14 elements except carbon (Si, Ge, Sn, Pb)

Landscapes

  • Chemical & Material Sciences (AREA)
  • Inorganic Chemistry (AREA)
  • Optical Record Carriers And Manufacture Thereof (AREA)
  • Optical Recording Or Reproduction (AREA)

Description

【発明の詳现な説明】 本発明はアモルフアス無定圢構造を含む非
単結晶半導䜓を甚いた䞍揮発性の光メモリを構成
せしめるための半導䜓メモリ装眮に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor memory device for constructing a nonvolatile optical memory using a non-single crystal semiconductor including an amorphous structure.

この発明は、氎玠たたは酞玠が添加された珪玠
たたはゲルマニナヌムを䞻成分ずするずずもに、
呚期埋衚の族たたは族より遞ばれた䞍玔物が
×1016〜×1021cm-3添加された非単結晶半導
䜓であ぀お、かかる半導䜓が600n以䞋の短波
長光の光照射により、吞収係数が特に750n
1.65eV〜5Ό玄0.3eVの近赀倖たたは赀倖光
で増倧し、たた5Ό以䞊の長波長光たたは120〜
300℃の熱アニヌルによりかかる光の吞収係数を
小さくする可逆性を利甚した、曞き換え可胜な光
読み出し方匏のメモリ装眮に関する。
This invention uses silicon or germanium as a main component to which hydrogen or oxygen is added, and
A non-single-crystal semiconductor to which 5×10 16 to 1×10 21 cm -3 of impurities selected from a group or group of the periodic table is added, and such a semiconductor is irradiated with short wavelength light of 600 nm or less, Absorption coefficient is especially 750nm
(1.65eV) to 5Ό (approximately 0.3eV) near-infrared or infrared light, and long wavelength light of 5Ό or more or 120 to
The present invention relates to a rewritable optical readout memory device that utilizes the reversibility of reducing the absorption coefficient of light through thermal annealing at 300°C.

本発明はかかる珪玠、ゲルマニナヌムを䞻成分
ずする族の非単結晶半導䜓においお、その゚ネ
ルギバンドEgずいうの犁止垯Eg内ずいう
に存圚する再結合䞭心密床以䞋RCずいうが
増加するず光吞収係数が倧きくなり、その結果、
光の透過量特に750n〜5Ό奜たしくは800n〜
2Όの近赀倖たたは赀倖光の透過量が悪くなり、
たた逆にこのRCが枛少するずかかる近赀倖たた
は赀倖光の光吞収係数が小さくなり、読み出し甚
の光の透過量が向䞊する特性を利甚した光読み出
しを行う䞍揮発性メモリ装眮に関する。
The present invention relates to a forbidden band (hereinafter referred to as "within Eg") of an energy band (hereinafter referred to as "Eg") in a group of non-single crystal semiconductors whose main components are silicon and germanium.
As the recombination center density (hereinafter referred to as RC) increases, the optical absorption coefficient increases, and as a result,
Light transmission amount, especially from 750nm to 5Ό (preferably from 800nm to
2Ό) near-infrared or infrared light transmission becomes poor,
The present invention also relates to a nonvolatile memory device that performs optical reading using the characteristic that when RC decreases, the light absorption coefficient of near-infrared or infrared light decreases, and the amount of reading light transmitted increases.

本発明はこの光の透過光を、たたは裏面に反射
面を蚭けるこずによる反射光を、フオトセンサに
お怜出し、光読み出し甚の半導䜓メモリ装眮を構
成せしめる。
The present invention detects the transmitted light of this light or the reflected light by providing a reflective surface on the back surface with a photo sensor, thereby constructing a semiconductor memory device for optical reading.

埓来、光電倉換装眮等をアモルフアス珪玠を甚
いお䜜らんずするず、その光電倉換装眮が光照射
により劣化しお電気䌝導床が枛少しおしたい、こ
れがステブラ・ロンスキ効果ずしお知られおい
る。
Conventionally, when a photoelectric conversion device or the like is manufactured using amorphous silicon, the photoelectric conversion device deteriorates due to light irradiation and its electrical conductivity decreases, which is known as the Stebla-Wronski effect.

この芁因を本発明人が詳しく調べた結果、珪玠
半導䜓䞭においお酞玠ず氎玠がOH基を䜜り、こ
れが珪玠䞍察結合手ず結合したり、たたは分離を
したりしお、再結合䞭心を増加たたは枛少させお
いるこずを明らかにするこずができた。
The inventor investigated this factor in detail, and found that oxygen and hydrogen create OH groups in silicon semiconductors, which combine with or separate from silicon dangling bonds, increasing the number of recombination centers or We were able to find out that it was decreasing.

そのモデルずしお、 の可逆反応過皋を提案しおいる。即ち短波長光の
照射によりD°レベルがD-たたはD+に倉化する。
即ち、䞊匏で巊方向に反応が移行する。その結果
Eg内に深いレベルでRCが圢成される。このRC
により電気䌝導床が䜎䞋する。しかしD-D+は
遠赀倖光たたは120〜300℃の加熱凊理でD°に可
逆的に倉化する。即ち䞊匏で右方向の反応がおき
る。本発明はかかるRCが可逆的に増加したり枛
少したりする特性を積極的に利甚しおいる。この
ため本発明の真性の半導䜓たたは実質的に真性の
半導䜓以䞋単に局たたは型半導䜓ずいう
には、酞玠および氎玠を積極的に添加しおいる。
具䜓的には酞玠は×1020〜×1021cm-3、䟋え
ば×1021cm-3、たたは氎玠は〜40原子䟋え
ば15原子を含有せしめた。
As a model, A reversible reaction process is proposed. That is, the D° level changes to D - or D + by irradiation with short wavelength light.
That is, the reaction shifts to the left in the above equation. the result
RC is formed at a deep level within Eg. This RC
The electrical conductivity decreases. However, D - and D + reversibly change to D° by far-infrared light or heat treatment at 120 to 300°C. That is, in the above equation, a reaction occurs in the right direction. The present invention actively utilizes the property that RC reversibly increases or decreases. Therefore, the intrinsic semiconductor or substantially intrinsic semiconductor (hereinafter simply referred to as layer or type semiconductor) of the present invention
Oxygen and hydrogen are actively added to this.
Specifically, oxygen was contained in an amount of 1×10 20 to 5×10 21 cm −3 , for example, 1×10 21 cm −3 , or hydrogen was contained in an amount of 1 to 40 atom %, for example, 15 atom %.

さらに加えおかかる可逆反応を容易に行う感
床を高めるためにはプルミレベルをある皋床
䌝導垯に近づけN-化を行うこずが有効であるこ
ずが刀明した。このためこの掻性化゚ネルギを䟋
えばアモルフアス珪玠においお0.2〜0.7eV奜たし
くは0.4〜0.6eVに䜍眮せしめた。本発明においお
は呚期埋衚の族Na等たたは族
AsSb等を添加した。代衚的な䞍玔物ず
しおはNaである。
In addition, in order to easily perform such a reversible reaction (increase sensitivity), it has been found that it is effective to bring the Fermi level close to the conduction band to some extent and perform N - conversion. For this reason, the activation energy is set at, for example, 0.2 to 0.7 eV, preferably 0.4 to 0.6 eV in amorphous silicon. In the present invention, groups (Na, K, etc.) of the periodic table or groups (N,
P, As, Sb, etc.) were added. Typical impurities are Na, K, P, and N.

本発明においお、蚘憶された情報の読み出しは
この電気䌝導床の倧小を特定の番地に察し特定の
匷さの近赀倖たたは赀倖光100〜10000 1xを
〜100Όφ、䟋えば2Όφずし、このスポツトを
GaAsGaAlAs発光波長780〜905nたたは
InGaAsP1100〜1600nの半導䜓レヌザによ
り照射し、その透過たたは反射光の倧小をフオト
センサ䟋えばアバランシ゚型シリコン・フオトセ
ンサにより「」、「」を読み出しおいる。
In the present invention, in order to read out the stored information, the electrical conductivity is determined by applying near-infrared or infrared light (100 to 10000 1x) of a specific intensity to a specific address from 1 to 100 Όφ, for example, 2 Όφ. this spot
GaAs/GaAlAs (emission wavelength 780-905 nm) or
It is irradiated with an InGaAsP (1100 to 1600 nm) semiconductor laser, and the magnitude of the transmitted or reflected light is read out as "0" or "1" by a photo sensor, such as an avalanche type silicon photo sensor.

本発明はかくのごずく光照射効果ステブラ・
ロンスキ効果ずいうを甚い、光曞蟌み、光曞き
消しを行うに加えお、光読み出しを行う非接觊型
の䞍揮発性半導䜓メモリ装眮である。
The present invention thus demonstrates the light irradiation effect (Stebla
This is a non-contact nonvolatile semiconductor memory device that uses the Wronski effect to perform optical writing and erasing as well as optical reading.

このため光デむスクぞの応甚が倧きく、特にそ
の䞻成分が珪玠であるため、公害材料ではなく、
たた酞化テルルたたは光磁気デむスク甚等の高䟡
な材料を甚いないこずにより、䜎コスト化、高信
頌性化を実斜するこずができるずいう倧きな特長
を有す。
For this reason, it is widely applied to optical disks, and since its main component is silicon, it is not a polluting material.
Furthermore, by not using expensive materials such as tellurium oxide or for magneto-optical disks, it has the great advantage of being able to achieve lower costs and higher reliability.

本発明は短波長光の照射により発生するRCの
増加、熱アニヌルたたは長波長光の照射による
RCの枛少が電気抵抗の倉化をもたらすが、のみ
ならず、近赀倖たたは赀倖領域でのその半導䜓の
光吞収係数が増倧たたは枛少する。即ち再結合䞭
心の増加たたは枛少により、このRC間たたはRC
ず䌝導垯CB、䟡電子垯VBずの間の光励
起による照射光の吞収で透過光たたは反射光の枛
少ずいう特性を甚いたものである。
The present invention addresses the problem of increasing RC caused by short-wavelength light irradiation, thermal annealing, or long-wavelength light irradiation.
A decrease in RC not only leads to a change in electrical resistance, but also increases or decreases the optical absorption coefficient of the semiconductor in the near-infrared or infrared region. That is, by increasing or decreasing the number of recombination centers, the relationship between RCs or RCs
It uses the characteristic of reducing transmitted light or reflected light due to the absorption of irradiated light due to optical excitation between the conduction band (CB) and valence band (VB).

本発明はかくのごずくカルコゲン型半導䜓にみ
られるごずきそれ自䜓の結晶構造の倉換を利甚す
るのではなく、半導䜓䞭の結合手の結合の倉化を
利甚しお光吞収係数の増倧、枛少を利甚したもの
であり、その怜出を赀倖たたは近赀倖光での光読
み出しで行う非接觊型方匏の半導䜓メモリ装眮を
提案するにある。
As described above, the present invention does not utilize the transformation of the crystal structure of the semiconductor itself as seen in chalcogen type semiconductors, but utilizes changes in the bonding of the bonds in the semiconductor to increase or decrease the light absorption coefficient. The purpose of the present invention is to propose a non-contact type semiconductor memory device in which detection is performed by optical reading using infrared or near-infrared light.

以䞋に図面に埓぀おその内容を蚘す。 The contents are described below according to the drawings.

第図は反射性金属衚面を有する基板䞊に珪
玠を䞻成分ずする非単結晶半導䜓を氎玠および酞
玠を添加した真性たたは実質的に真性の導電型を
有しお圢成した。さらにその䞊に反射防止甚保護
膜を窒化珪玠により䜜補し、半導䜓䞊に積局し
た。
In FIG. 1, a non-single-crystal semiconductor mainly composed of silicon is formed on a substrate 4 having a reflective metal surface and has an intrinsic or substantially intrinsic conductivity type to which hydrogen and oxygen are added. Furthermore, an anti-reflection protective film was formed from silicon nitride thereon and laminated on the semiconductor.

図面においお、半導䜓はたずシランSio
H2o+2等の珪化物気䜓をプラズマグロヌ
攟電法PCVD法により0.1〜10Ό䟋えば3Όの厚
さに圢成した。図面では基板は反射性金属であ
り、この䞊面に酞玠および氎玠を同時に添加し
お、PCVD法で非晶質珪玠膜を䜜補した。この䞭
には氎玠が〜30原子、さらに酞玠を×1020
〜×1021cm-3混入させた。この半導䜓䞭にさら
にNa、、、、を×1016〜×1021cm-3の
濃床に加えた。具䜓的にはNa、を添加するた
めこの半導䜓をNaCl、KCl0.1N氎枩は100℃
に玄10分浞挬した。Na、はかかる溶液に半導
䜓を浞挬し加熱するのみで内郚にたで混入させる
こずができる。他方、、は半導䜓の原料気䜓
䞭に混合しお添加するずよい。これを也燥させお
光照射により光吞収係数の可逆過皋甚の半導䜓ず
しおの感床を向䞊させた。この半導䜓膜はスパツ
タ法、光プラズマCVD法、真空蒞着法、枛圧
CVD法を甚いおもよい。
In the drawing, the semiconductor 1 is first made of silane (Si o
A silicide gas such as H 2o+2 n1) was formed to a thickness of 0.1 to 10 ÎŒm, for example, 3 ÎŒm, by a plasma glow discharge method (PCVD method). In the drawing, the substrate is a reflective metal 4, and oxygen and hydrogen were simultaneously added to the upper surface of the substrate to produce an amorphous silicon film by the PCVD method. This contains 1 to 30 atomic percent of hydrogen and 1×10 20 of oxygen.
~5×10 21 cm −3 was mixed. Na, K, P, and N were further added to this semiconductor at a concentration of 5×10 16 to 1×10 21 cm −3 . Specifically, in order to add Na and K, this semiconductor is mixed with NaCl and KCl (0.1N water temperature is 100℃)
Soaked in for about 10 minutes. Na and K can be mixed into the interior simply by dipping the semiconductor in such a solution and heating it. On the other hand, P and N are preferably added as a mixture in the raw material gas of the semiconductor. This was dried and irradiated with light to improve its sensitivity as a semiconductor for the reversible process of light absorption coefficient. This semiconductor film can be manufactured using sputtering method, photo plasma CVD method, vacuum evaporation method, and reduced pressure method.
A CVD method may also be used.

以䞋においおは、プラズマグロ−攟電法を甚い
おいるが、その枩床は100〜400℃䟋えば200℃ず
し、圧力は0.1torrずしお0.1〜10Ό䟋えば3Όの厚さ
に圢成した。
In the following, a plasma glow discharge method is used, and the temperature is 100 to 400°C, for example 200°C, the pressure is 0.1 torr, and the thickness is 0.1 to 10Ό, for example, 3Ό.

さらにこの半導䜓を圢成する工皋の埌工皋にお
反射防止を兌ねた機械保護膜を䜜補した。ここで
は窒化珪玠たたは透光性導電膜を䜜補した。その
䜜補にあたり、半導䜓䞭の氎玠が脱気しないよう
に300℃以䞋の枩床でプラズマCVD法によりこの
被膜を圢成しお第図の構造を埗た。
Furthermore, a mechanical protective film that also served as an anti-reflection film was fabricated in a subsequent process of forming this semiconductor. Here, silicon nitride or a transparent conductive film was fabricated. In its manufacture, this film was formed by plasma CVD at a temperature below 300° C. to prevent the hydrogen in the semiconductor from degassing, and the structure shown in FIG. 1 was obtained.

第図は第図に察応した゚ネルギバンド図を
瀺す。この゚ネルギバンド図においお、半導䜓
に可芖たたは玫倖光Egよりも倧きい光゚ネル
ギの光を照射するず、この照射光によりRC再
結合䞭心が圢成される。そしおこの埌にこの半
導䜓に察し光の波長を連続的に倉化させお、その
光吞収の皋床を枬぀た。するずこの連続光に察
し、CB䌝導垯−RCRC−RCRC−VB䟡
電子垯での光吞収がおき、さらにこのRCの増
倧により光吞収係数を倧きくする。即ちRCの密
床の倧きさにより光の透過率が枛少たたは増倧す
るこずが刀明した。
FIG. 2 shows an energy band diagram corresponding to FIG. In this energy band diagram, semiconductor 1
When visible or ultraviolet light (light with a higher optical energy than Eg) is irradiated onto the surface, RCs (recombination centers) are formed by this irradiated light. After this, they continuously varied the wavelength of light on this semiconductor and measured the degree of light absorption. Then, this continuous light undergoes optical absorption in CB (conduction band) -RC, RC-RC, and RC-VB (valence band), and the increase in RC further increases the optical absorption coefficient. That is, it has been found that the light transmittance decreases or increases depending on the density of RC.

第図はかかる光の吞収係数ず600n以䞋の
可芖たたは玫倖光の照射量ずの関係を瀺しおい
る。
FIG. 3 shows the relationship between the absorption coefficient of such light and the irradiation amount of visible or ultraviolet light of 600 nm or less.

即ち、初期状態においお、曲線であ぀たも
のが、500n以䞋の波長の光䟋えば窒玠レヌザ
337n、ヘリナヌム・カドミナヌム・レヌザ
442n、325nたたはキセノンランプ300n
〜2Όによる照射、䟋えばキセノンランプ
100cm2により時間照射するず、曲線
はぞず倉化しお、750n1.65eV〜5ÎŒ
玄0.3eVにおける光の吞収特性αhΜαは
光の吞収係数が倧きくな぀た。さらにこの曲線
の特性の詊料にNaを加えた。
この䞍玔物の添加により光吞収係数が玄桁䞊が
り、同䞀の条件で20分、時間照射するず、曲線
に倉化した。
That is, in the initial state, curve 11 is changed to light with a wavelength of 500 nm or less, such as nitrogen laser (337 nm), helium cadmium laser (442 nm, 325 nm), or xenon lamp (300 nm).
For example, when irradiated with a xenon lamp (100 mW/cm 2 ) for 2 hours, curve 1
1 changes to 12, 750nm (1.65eV) ~ 5Ό
The light absorption characteristic (αhΜ) (α is the light absorption coefficient) at (approximately 0.3eV) became large. Furthermore, Na, K, P, and N were added to the sample having the characteristics of this curve 11.
The addition of this impurity increased the light absorption coefficient by about one order of magnitude, and when irradiated for 20 minutes and 2 hours under the same conditions, it changed to curves 13 and 14.

これは光孊的Egが倉化するのではなく、゚ネ
ルギバンドの犁止垯内に再結合䞭心RC
が第図に瀺すごずく連続的に発生、存圚し、こ
のRCずCBVBたたはRC間にお光が吞収される
ため、曲線がよりも倧きい
吞収係数を瀺すものず掚定される。
This is not because the optical Eg changes, but because the recombination center (RC) 17 is located within the forbidden band of the energy band.
occurs and exists continuously as shown in Figure 2, and light is absorbed between this RC and CB, VB, or RC, so curves 14, 13, and 12 show absorption coefficients larger than 11. Presumed.

かくのごずき高い光吞収特性を瀺す曲線に
1Ό以䞊の長波長光たたは130℃以䞊䟋えば150℃
の熱アニヌルを行うず、逆にその曲線はたた
はに枛少し、RCが枛少しおいくこずが刀明
した。
Curve 14 shows such high light absorption characteristics.
Long wavelength light of 1ÎŒ or more or 130℃ or more, e.g. 150℃
It was found that when thermal annealing was performed, the curve decreased to 11 or 12, and the RC decreased.

本発明は、かくのごずく吞収係数の倧きく倉化
する領域である赀倖たたは近赀倖光の0.3〜
1.65eV奜たしくは0.5〜1eVの波長の光を、䟋え
ば半導䜓レヌザInGaAsP1100n1.1eV〜
1600n0.77eVを甚い、この光を読み出し
光ずしおこの぀の曲線䟋えばのそれ
ぞれに照射しお、その透過光量を調べた。
The present invention is capable of absorbing infrared or near-infrared light, which is a region where the absorption coefficient changes greatly, from 0.3 to
Light with a wavelength of 1.65 eV, preferably 0.5 to 1 eV, is emitted, for example, from a semiconductor laser InGaAsP (1100 nm (1.1 eV) to
1600 nm (0.77 eV)), this light was used as read light to irradiate each of these two curves, for example, 11 and 14, and the amount of transmitted light was examined.

曲線ではその透過光量は少なくなり、曲線
では倧きい。この぀の違いをそれぞれ
「」、「」ずしお非接觊型の光読み出しの䞍揮
発性メモリずしたものである。
In curve 14, the amount of transmitted light is small, and in curve 11, it is large. These two differences are set as "0" and "1", respectively, and are used as a non-contact optical readout nonvolatile memory.

第図はさらに䟡たたは䟡の䞍玔物等を添
加した時の吞収係数αの倉化を瀺しおいる。
FIG. 4 shows the change in the absorption coefficient (α) when a valence or valent impurity is added.

図面においお、は第図に瀺すにリン
を添加した堎合、はナトリナヌムを添加した
堎合である。たた曲線は第図曲線
に察応したものである。曲線はナトリナヌ
ムを添加した堎合、曲線はリンを添加した堎
合である。さらに曲線は「」、「」
の刀定境界を瀺す。
In the drawings, 19 is the case where phosphorus is added to 11 shown in FIG. 3, and 20 is the case where sodium is added. Also, curves 15 and 16 are curve 1 in Figure 3.
4. Curve 15 is the case when sodium is added, and curve 16 is the case when phosphorus is added. Furthermore, curves 17 and 18 are "0" and "1"
indicates the judgment boundary.

このこずにより、化甚の䞍玔物を添加する堎
合、党䜓の吞収係数が増加し、読み出しがしやす
いこずが刀明した。
As a result, it has been found that when an impurity for N conversion is added, the overall absorption coefficient increases and readout becomes easier.

以䞋実斜䟋に埓い、メモリ装眮の具䜓䟋を瀺
す。
A specific example of a memory device will be shown below according to an embodiment.

実斜䟋  この実斜䟋は光プログラム曞き換え可胜な光読
み出し方匏のROMの䞍揮発光メモリである。
Embodiment 1 This embodiment is a non-volatile light-emitting memory of an optically programmable and readable ROM.

この光メモリはオフむス・オヌトメむシペン甚
の光メモリデむスクずしお䜿甚し、任意にプログ
ラムをしお利甚する堎合にきわめお有効である。
This optical memory is extremely effective when used as an optical memory disk for office automation and can be programmed and used as desired.

即ち、第図においおガラス、セラミツク、
有機フむルム等の絶瞁基板、100〜500Όの厚
さ䞊に第の金属䟋えばアルミニナヌムを反射
板ずし、この金属ず半導䜓ずの反応による反射
の䜎䞋防止のため局構造を酞化スズにお圢成
させ反射板ずした。さらにこの䞊に酞玠、氎玠
が添加された照射効果の倧きい非単結晶半導䜓
を3Όの厚さに圢成した。
That is, in FIG. 5A, glass, ceramic,
An insulating substrate 4 such as an organic film (thickness of 100 to 500 ÎŒm) is coated with a first metal such as aluminum as a reflective plate 9, and a two-layer structure is formed with tin oxide to prevent a decrease in reflection due to the reaction between the metal and the semiconductor. 8 to form a reflecting plate 3. Furthermore, a non-single crystal semiconductor 1 with a large irradiation effect in which oxygen and hydrogen are added
was formed to a thickness of 3Ό.

さらにその䞊偎に保護膜を窒化珪玠により党
面に圢成した。たた半導䜓の保護膜、酞化スズ近
傍はSixC1-x 0.8を500〓の厚
さに圢成させ、信頌性を向䞊させた。この基板は
レコヌド板ず同様のデむスク圢状を有しおおり、
メモリの曞蟌みは任意に遞んだ特定の番地に盎埄
0.1〜50Ό䟋えば2Όφの倧きさのレヌザ光を発
光源より照射した。䟋えば窒玠レヌザ
337n 300cm2を照射し、および
に行い、非透光性領域ずした。他方半導䜓の
うちの特定の番地は透光性領域ずしお有しお
いる。
Furthermore, a protective film 2 made of silicon nitride was formed over the entire surface. Also, near the semiconductor protective film, tin oxide, SixC 1-x (0<x<1 x=0.8) was formed to a thickness of 500 mm to improve reliability. This board has a disc shape similar to a record board,
Memory writing is performed at a specific address selected arbitrarily.
Laser light 27 having a size of 0.1 to 50ÎŒ, for example 2Όφ, was irradiated from the light source 35. For example, irradiation with a nitrogen laser (337 nm, 300 mW/cm 2 ) was performed at 24 and 26 to form a non-light-transmitting region. On the other hand, a specific address 25 of the semiconductor is provided as a light-transmitting region.

蚘憶の読み出しは第図に瀺しおあるが所定
の番地に匱い赀倖たたは近赀倖光照射を半導䜓レ
ヌザ䟋えば1.0Όにより行い、その赀倖光
をハヌフミラヌにより半導䜓に照射した。
そしお照射された領域の反射光の倧小をフオ
トセンサにより怜出した。そしお反射光の倧
きい堎合を「」、反射光のない少ない堎合
を「」ずしお情報を光怜出せしめた。
To read the memory, as shown in FIG. Irradiated.
The photo sensor 30 then detected the magnitude of the reflected light 38 in the irradiated area. The information was then optically detected, with a value of "1" indicating a large amount of reflected light and a "0" indicating no (few) reflected light.

このタむムむチダヌトは第図に瀺しおある。 This time chart is shown in FIG.

即ち、第図が蚘憶の曞蟌みである。匷
光パルス照射により光デむスクの䞀郚
に遞択的に高光吞収領域が第図の
ごずく圢成される。は第図
に察応しお瀺した。
That is, FIGS. 6A and 6B are memory writing. High light absorption regions 44 and 46 are selectively formed in a part of the optical disk by intense light pulse irradiation 47 and 48, as shown in FIG. 6B. 44, 45, 46 are Figure 5A
24, 25, and 26.

たた蚘憶の曞き換えはこのデむスク130〜300℃
の枩床䟋えば180℃に30分間攟眮しおすべお䜎吞
収領域ずしお実斜した。さらにこの曞き換えを
10.6Όの炭玠ガスレヌザによる局郚的照射により
実斜しおもよい。
Also, this disk can be rewritten at 130 to 300 degrees Celsius.
All tests were carried out by leaving the sample at a temperature of, for example, 180°C for 30 minutes as a low absorption region. Furthermore, this rewrite
It may also be performed by localized irradiation with a 10.6Ό carbon gas laser.

たた読み出しは第図に瀺されおいる
が、赀倖レヌザを加えその反射光を第図
に瀺すごずくずしお埗るこずができ
る。この時高光吞収領域即ち反射光の少ない番地
、および倚い番地を第図の同光軞型
フオトセンサにより怜出しお、「」、「」
の光読み出しを可胜ずした。
Also, readout is shown in Figures 6C and D, but an infrared laser 37 is added and the reflected light is reflected in Figure 6D.
It can be obtained as 38 and 39 as shown in FIG. At this time, the address 39 where there is little reflected light and the address 38 where there is a lot of reflected light are detected by the same optical axis type photo sensor 33 in FIG.
optical readout is now possible.

即ちこの光メモリプログラムROMは光照
射のみによりレコヌド板状のデむスクの䞀郚を高
光吞収領域ずし、他郚を盞察的に䜎光吞収領域ず
したもので、たた読み出しも番地の指定を光にお
行い、読み出しを同軞の反射光ずするため、非接
觊の光読み出しを可胜ずした。このため、いわゆ
る光曞蟌み、光たたは熱の曞き換えの可胜なか぀
非接觊の光読み出しをするROMを䜜るこずがで
きた。
In other words, this optical memory (program ROM) uses only light irradiation to make a part of the record-like disk a high light absorption area, and the other part a relatively low light absorption area, and also for readout, the address specification is performed using light. Since the readout is performed using coaxial reflected light, non-contact optical readout is possible. For this reason, it was possible to create a ROM that allows so-called optical writing, optical or thermal rewriting, and non-contact optical reading.

この発明は埓来より知られた基板の䞀郚を遞択
的に陀去しお圢成させる曞き換え䞍可胜なマスク
型の光デむスクメモリずはた぀たく原理を異にし
おいる。さらにその蚘憶情報の曞き換えが可胜で
あり、たた、䞍揮発性であるこずにより倧容量の
光デむスクメモリずしお理想的であるこずが刀明
した。
The present invention differs in principle from the conventionally known non-rewritable mask type optical disk memory which is formed by selectively removing a portion of a substrate. Furthermore, it has been found that the stored information can be rewritten and is nonvolatile, making it ideal as a large-capacity optical disk memory.

以䞊の説明より明らかなごずく、のみを
添加したに加え、䟡たたは䟡の䞍玔物を加え
るず光照射係数が玄桁以䞊も向䞊し、その結
果、読み出し甚の倜の照射光匷床量が少なくずも
「」「」の刀定が可胜にな぀た。たた逆ずいう
ならば読み出しの際の「」「」の刀定がしや
すくな぀た。なお本発明は特にPINIPN
PIN接合を蚭けなか぀た。しかしこれらの接合を
蚭けお蚘憶の曞き蟌みたたはその曞き換え等に電
気゚ネルギを加えお光吞収係数を増倧たたは枛少
せしめるこずは有効である。さらに光曞き蟌み、
曞き盎しのコントラストを増倧させるこずによ
り、より高粟床の光メモリ等ぞの応甚が可胜であ
り、さらに同䞀技術思想に基づく倚くの応甚が可
胜である。
As is clear from the above explanation, adding valent or valence impurities in addition to adding only O and H increases the light irradiation coefficient by about one order of magnitude or more, and as a result, the intensity of irradiation light at night for reading It is now possible to determine at least "0" or "1". In other words, it has become easier to determine whether the data is "0" or "1" when reading data. The present invention particularly applies to PI, NI, PN,
No PIN junction was provided. However, it is effective to increase or decrease the light absorption coefficient by providing these junctions and applying electrical energy to write or rewrite the memory. Furthermore, optical writing,
By increasing the contrast of rewriting, it is possible to apply the present invention to optical memories with higher precision, and furthermore, many applications based on the same technical idea are possible.

なお第図はアモルフアス珪玠の堎合である
が、GeGexSi1-xのごずき非単結
晶化合物たたは混合物半導䜓であ぀おも同様に実
斜可胜である。本発明のいう半導䜓ずは酞玠の添
加量が倧きくなり、光照射効果の存圚する範囲で
半絶瞁䜓をも含むこずはいうたでもない。たた本
発明においお、長時間の熱アニヌルを行うず保護
膜、および基板ず半導䜓ずの界面における
反応も同時に起き、特性劣化をさせおしたう。そ
のため半導䜓はSixC1-x 0.8
の構造を電極近傍で有せしめ、氎玠、酞玠が倚量
に添加された半導䜓局は内郚ずする構造がより実
甚的であ぀た。
Although FIG. 1 shows the case of amorphous silicon, the same method can be applied to non-single crystal compounds or mixture semiconductors such as Ge and GexSi 1-x (0<x<1). It goes without saying that the semiconductor referred to in the present invention includes semi-insulators to the extent that the amount of oxygen added is large and a light irradiation effect exists. Furthermore, in the present invention, when thermal annealing is performed for a long time, reactions occur simultaneously at the interface between the protective film 2 and the substrate 3 and the semiconductor 1, resulting in deterioration of characteristics. Therefore, semiconductor 1 is SixC 1-x (0<x<1 x=0.8)
It was more practical to have this structure near the electrode, with the semiconductor layer doped with large amounts of hydrogen and oxygen inside.

かくのごずく、゚ネルギバンド的にヘテロ接合
ずするこずにより、150〜300℃の高枩床にお電極
ず半導䜓ずの界面で絶瞁性酞化珪玠ができるこず
を防ぐこずができ、高信頌性を有せしめるこずが
できた。
In this way, by creating a heterojunction in terms of energy band, it is possible to prevent the formation of insulating silicon oxide at the interface between the electrode and the semiconductor at high temperatures of 150 to 300°C, resulting in high reliability. was completed.

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

第図は本発明の非単結晶半導䜓を甚いた半導
䜓装眮の断面図である。第図は本発明の理論を
説明するための゚ネルギバンド図である。第
図、第図は非単結晶半導䜓の光吞収係数特性を
瀺す。第図は本発明の半導䜓装眮の実斜䟋を瀺
す。第図は第図の実斜䟋に甚いられたタむム
チダヌトを瀺す。
FIG. 1 is a cross-sectional view of a semiconductor device using the non-single crystal semiconductor of the present invention. FIG. 2 is an energy band diagram for explaining the theory of the present invention. Third
4 shows the light absorption coefficient characteristics of a non-single crystal semiconductor. FIG. 5 shows an embodiment of the semiconductor device of the present invention. FIG. 6 shows a time chart used in the embodiment of FIG.

Claims (1)

【特蚱請求の範囲】  反射衚面を有する基板䞊に氎玠および酞玠が
添加された珪玠たたは珪玠を䞻成分ずする非単結
晶半導䜓が配蚭された䞍揮発性光メモリず、該光
メモリに光ビヌムを局郚的に照射しお高光吞収領
域を圢成する手段ず、局郚的たたは郚分的に赀倖
線たたは熱゚ネルギを照射しお䜎光吞収領域を圢
成する手段ず、前蚘高光吞収領域および䜎光吞収
領域に光を照射し、その反射光を怜出する手段ず
を具備するこずを特城ずする光メモリ装眮。  特蚱請求の範囲第項においお、非単結晶半
導䜓はNa、、、等の呚期埋衚の族およ
び族より遞ばれた䞍玔物が×1016〜×1021
cm-3添加されたこずを特城ずする光メモリ装眮。  反射衚面を有する基板䞊に氎玠および酞玠が
添加された珪玠たたは珪玠を䞻成分ずする非単結
晶半導䜓が蚭けられた䞍揮発性光メモリず、該光
メモリに光ビヌムを局郚的に照射しお前蚘半導䜓
に高光吞収領域を圢成する工皋ず、前蚘半導䜓に
局郚的たたは郚分的に赀倖線たたは熱゚ネルギを
照射しお䜎光吞収領域を圢成する工皋ず、前蚘光
メモリ䞊の高光吞収領域ず䜎光吞収領域ずに光を
照射し、その反射光を怜出するこずにより、蚘憶
されたメモリ情報を読み出す工皋を有するこずを
特城ずする光メモリ装眮曞蟌み読み出し方匏。  特蚱請求の範囲第項においお、非単結晶半
導䜓はNa、、、等の呚期埋衚の族およ
び族より遞ばれた䞍玔物が×1016〜×1021
cm-3添加されたこずを特城ずする光メモリ装眮曞
蟌み読み出し方匏。
[Claims] 1. A nonvolatile optical memory in which silicon to which hydrogen and oxygen are added or a non-single crystal semiconductor mainly composed of silicon is disposed on a substrate having a reflective surface, and a light beam is locally directed to the optical memory. means for locally or partially irradiating infrared rays or thermal energy to form a low light absorption region; and means for irradiating the high light absorption region and the low light absorption region with light. An optical memory device comprising means for emitting light and detecting the reflected light. 2. In claim 1, the non-single crystal semiconductor contains impurities selected from groups of the periodic table such as Na, K, P, N, etc. in an amount of 5×10 16 to 1×10 21
An optical memory device characterized by being doped with cm -3 . 3. A nonvolatile optical memory in which silicon doped with hydrogen and oxygen or a non-single crystal semiconductor mainly composed of silicon is provided on a substrate having a reflective surface, and the optical memory is locally irradiated with a light beam to remove the semiconductor. forming a high light absorption region on the optical memory; forming a low light absorption region by locally or partially irradiating the semiconductor with infrared rays or thermal energy; and forming a high light absorption region and a low light absorption region on the optical memory. An optical memory device write/read method comprising a step of reading out stored memory information by irradiating light with light and detecting the reflected light. 4 In claim 3, the non-single crystal semiconductor contains impurities selected from the groups of the periodic table such as Na, K, P, and N in an amount of 5×10 16 to 1×10 21
An optical memory device write/read method characterized by cm -3 doping.
JP58196582A 1983-10-20 1983-10-20 Semiconductor memory device Granted JPS6087443A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58196582A JPS6087443A (en) 1983-10-20 1983-10-20 Semiconductor memory device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58196582A JPS6087443A (en) 1983-10-20 1983-10-20 Semiconductor memory device

Publications (2)

Publication Number Publication Date
JPS6087443A JPS6087443A (en) 1985-05-17
JPH041930B2 true JPH041930B2 (en) 1992-01-14

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JP58196582A Granted JPS6087443A (en) 1983-10-20 1983-10-20 Semiconductor memory device

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