JPH06167732A - Optical logic gate - Google Patents
Optical logic gateInfo
- Publication number
- JPH06167732A JPH06167732A JP31899192A JP31899192A JPH06167732A JP H06167732 A JPH06167732 A JP H06167732A JP 31899192 A JP31899192 A JP 31899192A JP 31899192 A JP31899192 A JP 31899192A JP H06167732 A JPH06167732 A JP H06167732A
- Authority
- JP
- Japan
- Prior art keywords
- laser beam
- saturable
- level
- logic gate
- absorption layer
- 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
Links
- 230000003287 optical effect Effects 0.000 title abstract description 11
- 230000002194 synthesizing effect Effects 0.000 claims abstract description 9
- 238000010521 absorption reaction Methods 0.000 abstract description 7
- 230000004044 response Effects 0.000 abstract description 4
- 239000000975 dye Substances 0.000 abstract 4
- 239000004973 liquid crystal related substance Substances 0.000 description 4
- 239000006096 absorbing agent Substances 0.000 description 3
- 230000005540 biological transmission Effects 0.000 description 2
- 239000004020 conductor Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000001747 exhibiting effect Effects 0.000 description 1
- RBTKNAXYKSUFRK-UHFFFAOYSA-N heliogen blue Chemical compound [Cu].[N-]1C2=C(C=CC=C3)C3=C1N=C([N-]1)C3=CC=CC=C3C1=NC([N-]1)=C(C=CC=C3)C3=C1N=C([N-]1)C3=CC=CC=C3C1=N2 RBTKNAXYKSUFRK-UHFFFAOYSA-N 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000004043 responsiveness Effects 0.000 description 1
- PYWVYCXTNDRMGF-UHFFFAOYSA-N rhodamine B Chemical compound [Cl-].C=12C=CC(=[N+](CC)CC)C=C2OC2=CC(N(CC)CC)=CC=C2C=1C1=CC=CC=C1C(O)=O PYWVYCXTNDRMGF-UHFFFAOYSA-N 0.000 description 1
- 229940043267 rhodamine b Drugs 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は光学論理ゲートに関する
ものである。FIELD OF THE INVENTION The present invention relates to optical logic gates.
【0002】[0002]
【従来の技術】従来、この種の工学論理ゲートには、本
願発明者の考案による液晶ライトバルブ論理ゲートのよ
うに光導体と液晶を用いた空間変調記器を用いる方法
や、NASAのOptical Computer,N
OVAシステムなどが知られているが、いずれもNAN
Dゲートの実現による光学論理演算の実現性を検討して
きたものである。2. Description of the Related Art Conventionally, a method of using a spatial modulation recorder using a light guide and a liquid crystal, such as a liquid crystal light valve logic gate devised by the present inventor, has been used for an engineering logic gate of this type, or a NASA optical computer. , N
OVA system is known, but all are NAN
The feasibility of optical logic operation by realizing the D gate has been examined.
【0003】[0003]
【発明が解決しようとする課題】上述した従来の光学論
理ゲートは、光に対してアクティブな光導電導体と液晶
のようなパッシブな光学素子とを組み合わせており、現
在のところ応答性の遅い光学素子しか実用化していな
い。この応答性及び入力読み出しタイミングに図2に示
すようなずれがあると、必要な論理出力α以外にβ、γ
のような不要の演算出力が発生し、その弁別が困難であ
った。The above-mentioned conventional optical logic gates combine a photoconductive conductor active with respect to light and a passive optical element such as a liquid crystal. Only the element has been put to practical use. If the response and the input read timing are deviated as shown in FIG. 2, β and γ are obtained in addition to the required logical output α.
However, it is difficult to discriminate them.
【0004】従って本発明はナノ秒オーダの高速応答の
可能で而も明確に動作する論理ゲートを提供しようとす
るものである。Accordingly, the present invention seeks to provide a logic gate which is capable of high speed response on the order of nanoseconds and which operates in a very clear manner.
【0005】[0005]
【課題を解決するための手段】本発明は、レーザのQス
イッチ素子として知られる銅−フタロシアニンやローダ
ミンBなど可飽和色素吸収体を用いて、閾値以下の入力
レベルでは出力されず明確な2値化が行える物質を論理
ゲートに適用するっ事によって、上記の欠点のない光学
論理ゲートを提供しようとするものである。The present invention uses a saturable dye absorber, such as copper-phthalocyanine or rhodamine B, which is known as a Q-switch element of a laser, and does not output at an input level below a threshold value and has a clear binary value. The object of the present invention is to provide an optical logic gate that does not have the above-mentioned drawbacks by applying a material that can be converted into a logic gate.
【0006】すなわち本発明によれば、飽和点以上のレ
ベルのレーザビームで動作しそれ以下のレベルで非動作
の可飽和色素吸収層と、2つの方向からのレーザビーム
を合成して前記可飽和色素吸収層に向けるように配設さ
れたレーザビーム合成手段と、このレーザビーム合成手
段の前記2つの方向に面して設けられた、レーザビーム
を空間変調する2つの空間変調手段と、該2つの空間変
調手段に、前記レーザビーム合成手段で合成され前記可
飽和色素吸収層に入射するときのレベルが少なくとも6
5kWの尖頭出力を有し且つ前記飽和色素吸収層に対し
て飽和点以下であるような2つのレーザビームを入射す
る入力手段とを備えた光学論理ゲートが得られる。That is, according to the present invention, the saturable dye absorbing layer that operates with a laser beam at a level above the saturation point and does not operate at a level below that and a laser beam from two directions are combined to form the saturable dye absorption layer. Laser beam synthesizing means arranged so as to face the dye absorbing layer, two spatial modulation means for spatially modulating the laser beam, which are provided so as to face the two directions of the laser beam synthesizing means, and 2 The level when the light is synthesized by the laser beam synthesizing means and is incident on the saturable dye absorbing layer is at least 6 in one spatial modulating means.
An optical logic gate having a peak power of 5 kW and an input means for injecting two laser beams which are below the saturation point with respect to the saturated dye absorbing layer is obtained.
【0007】この本発明の光学論理ゲートにおいて、可
飽和色素吸収体に対する閾値を論理上の負のレベルと
し、閾値を越えるレベルを正のレベルと解釈すれば、該
色素吸収体に対し、負のレベルで活性なレーザビームを
論理遂行のためのアクティブキャリア(即ち論理実現可
能なレベルの光)として定義される。このアクティブキ
ャリアは該論理実現のためのゲートを開くトリガビーム
である。なおレーザビームの種類は実用上波長特性は問
わないが、入力ビームは可飽和特性を呈し得る高出力の
レーザビームが必要である。ただし読み出しの場合には
必ずしもこの条件を満足する必要は無い。In the optical logic gate of the present invention, if the threshold value for the saturable dye absorber is a logically negative level, and the level exceeding the threshold value is interpreted as a positive level, the negative value is obtained for the dye absorber. A laser beam active at a level is defined as an active carrier (that is, a light at a logic-realizable level) for performing logic. This active carrier is a trigger beam that opens the gate for implementing the logic. Although the type of laser beam may be practically any wavelength characteristic, a high-output laser beam capable of exhibiting saturable characteristics is required as an input beam. However, it is not always necessary to satisfy this condition when reading.
【0008】[0008]
【実施例】図1は本発明の一実施例の断面図で有り、1
は第1の入力情報としてのレーザビーム(第1の入力ビ
ームと言う)、2は同じく第2の入力情報としてのレー
ザビーム(第2の入力ビーム)である。3と4はいずれ
も液晶ライトバルブ、PLZT、BSOなどの第1及び
第2の空間変調素子であり、第1及び第2の入力ビーム
がそれぞれ通過する。5はレーザビーム合成部で、第1
及び第2の入力ビームを同一時点で同一空間で合成す
る。6は可飽和色素吸収層であり、閾値以下で尖頭出力
が65kW以上の合成入力レベルでは負の論理“0”を
持ち、閾値を越えての合成入力レベルでは正の論理
“1”を持つ出力ビーム7が得られる。1 is a sectional view of an embodiment of the present invention, in which 1
Is a laser beam as the first input information (referred to as a first input beam), and 2 is a laser beam (second input beam) as the second input information. Reference numerals 3 and 4 are first and second spatial modulation elements such as a liquid crystal light valve, PLZT, BSO, etc., through which the first and second input beams pass, respectively. 5 is a laser beam synthesizing unit, which is the first
And the second input beam are combined in the same space at the same time. Reference numeral 6 denotes a saturable dye absorption layer, which has a negative logic "0" at a synthetic input level below a threshold value and a peak output of 65 kW or more, and has a positive logic "1" at a synthetic input level above the threshold value. An output beam 7 is obtained.
【0009】この図1の論理ゲートはANDゲートとし
て作用でき、ゲート自身がアクティブであるところか
ら、第1及び第2の入力ビームにタイミングのずれがあ
っても不要な論理出力は発生しない。The logic gate of FIG. 1 can act as an AND gate, and since the gate itself is active, no unnecessary logic output is generated even if there is a timing difference between the first and second input beams.
【0010】[0010]
【発明の効果】以上に詳述したように、本発明は可飽和
色素吸収層の2値を論理的に透明、不透明のレベルに2
値化することによって実現し、かつ色素に対し反転レベ
ルでの光透過及び光不透過を容易に得られる,いわゆる
第2高調波レベルでの読み出しを行うことにより、即
ち、閾値以下の入力レベルでは不活性で閾値を越えると
論理“1”を読みだしてビームに与えるいわゆるAND
ゲートを得ることにより、可飽和色素吸収層の持つナノ
秒オーダの高速応答を有する論理ゲートを構成すること
が可能と成った。As described above in detail, according to the present invention, the binary value of the saturable dye absorbing layer is set to the level of logically transparent and opaque.
By reading at the so-called second harmonic level, which is realized by digitizing and easily obtains the light transmission and the light non-transmission at the inversion level with respect to the dye, that is, at the input level below the threshold value. When it is inactive and exceeds the threshold value, a logical "1" is read and given to the beam.
By obtaining the gate, it became possible to construct a logic gate with a nanosecond-order fast response of the saturable dye absorbing layer.
【図1】本発明の第1の実施例の断面図である。FIG. 1 is a cross-sectional view of a first embodiment of the present invention.
【図2】従来装置における応答性と入力読み出しのタイ
ミングのずれがあるきに不要な演算出力が発生すること
を示す図である。FIG. 2 is a diagram showing that an unnecessary calculation output is generated when there is a difference in responsiveness and input read timing in the conventional device.
1 第1の入力ビーム 2 第2の入力ビーム 3 第1の空間変調素子 4 第2の空間変調素子 5 レーザビーム合成部 6 可飽和色素吸収層 7 出力ビーム 1 First Input Beam 2 Second Input Beam 3 First Spatial Modulator 4 Second Spatial Modulator 5 Laser Beam Synthesizer 6 Saturable Dye Absorption Layer 7 Output Beam
Claims (1)
作しそれ以下のレベルで非動作の可飽和色素吸収層と、
2つの方向からのレーザビームを合成して前記可飽和色
素吸収層に向けるように配設されたレーザビーム合成手
段と、このレーザビーム合成手段の前記2つの方向に面
して設けられた、レーザビームを空間変調する2つの空
間変調手段と、該2つの空間変調手段に、前記レーザビ
ーム合成手段で合成され、前記可飽和色素吸収層に入射
するときのレベルが少なくとも65kWの尖頭出力を有
し且つ前記可飽和色素吸収層に対して飽和点以下である
ような2つのレーザビームを入射する入力手段とを備え
た光学論ゲート。1. A saturable dye absorbing layer that operates with a laser beam at a level above the saturation point and does not operate at a level below that,
Laser beam synthesizing means arranged so as to synthesize laser beams from two directions to face the saturable dye absorbing layer, and a laser provided to face the two directions of the laser beam synthesizing means. Two spatial modulation means for spatially modulating the beam and a peak output of at least 65 kW when combined with the two spatial modulation means by the laser beam combining means and incident on the saturable dye absorbing layer. And an input means for injecting two laser beams having a saturation point or less with respect to the saturable dye absorbing layer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31899192A JPH06167732A (en) | 1992-11-27 | 1992-11-27 | Optical logic gate |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31899192A JPH06167732A (en) | 1992-11-27 | 1992-11-27 | Optical logic gate |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH06167732A true JPH06167732A (en) | 1994-06-14 |
Family
ID=18105278
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP31899192A Pending JPH06167732A (en) | 1992-11-27 | 1992-11-27 | Optical logic gate |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH06167732A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6124966A (en) * | 1997-01-13 | 2000-09-26 | Nec Corporation | Optical functional amplifying method and optical functional amplifying device |
-
1992
- 1992-11-27 JP JP31899192A patent/JPH06167732A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6124966A (en) * | 1997-01-13 | 2000-09-26 | Nec Corporation | Optical functional amplifying method and optical functional amplifying device |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| A02 | Decision of refusal |
Free format text: JAPANESE INTERMEDIATE CODE: A02 Effective date: 19981224 |