JPH05196960A - Space optical modulator and driving method thereof - Google Patents
Space optical modulator and driving method thereofInfo
- Publication number
- JPH05196960A JPH05196960A JP2884692A JP2884692A JPH05196960A JP H05196960 A JPH05196960 A JP H05196960A JP 2884692 A JP2884692 A JP 2884692A JP 2884692 A JP2884692 A JP 2884692A JP H05196960 A JPH05196960 A JP H05196960A
- Authority
- JP
- Japan
- Prior art keywords
- writing
- light
- liquid crystal
- reading
- ferroelectric liquid
- 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 claims abstract description 18
- 238000000034 method Methods 0.000 title claims description 14
- 239000005262 ferroelectric liquid crystals (FLCs) Substances 0.000 claims abstract description 26
- 229910021417 amorphous silicon Inorganic materials 0.000 claims abstract description 7
- 239000004973 liquid crystal related substance Substances 0.000 claims description 10
- 239000000758 substrate Substances 0.000 claims description 9
- 230000001678 irradiating effect Effects 0.000 claims description 6
- 239000011521 glass Substances 0.000 claims description 4
- 239000000203 mixture Substances 0.000 claims description 2
- 238000000926 separation method Methods 0.000 claims 1
- 230000010365 information processing Effects 0.000 abstract description 6
- 230000007704 transition Effects 0.000 abstract description 4
- 230000000694 effects Effects 0.000 abstract description 2
- 238000010586 diagram Methods 0.000 description 4
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 230000006870 function Effects 0.000 description 2
- 229910052736 halogen Inorganic materials 0.000 description 2
- 150000002367 halogens Chemical class 0.000 description 2
- 230000002093 peripheral effect Effects 0.000 description 2
- 239000003566 sealing material Substances 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- LIVNPJMFVYWSIS-UHFFFAOYSA-N silicon monoxide Chemical compound [Si-]#[O+] LIVNPJMFVYWSIS-UHFFFAOYSA-N 0.000 description 2
- 239000004990 Smectic liquid crystal Substances 0.000 description 1
- 238000002347 injection Methods 0.000 description 1
- 239000007924 injection Substances 0.000 description 1
- 238000007644 letterpress printing Methods 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 238000007639 printing Methods 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
Landscapes
- Liquid Crystal (AREA)
Abstract
Description
【発明の詳細な説明】Detailed Description of the Invention
【0001】[0001]
【産業上の利用分野】本発明は画像処理装置、光情報処
理用空間光変調器等に応用される光書き込み型強誘電性
液晶空間光変調器及びその駆動方法に関するものであ
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a photo-writing type ferroelectric liquid crystal spatial light modulator applied to an image processing device, a spatial light modulator for optical information processing and the like, and a driving method thereof.
【0002】[0002]
【従来の技術】従来、強誘電性液晶を用いた空間光変調
器は入力された画像情報を、リアルタイムで強度変調出
力する素子として用いられている。また、発明者らは、
特願平02−239594号によって、上記素子におい
て連続階調を有する出力を得る駆動方法をも示した。2. Description of the Related Art Conventionally, a spatial light modulator using a ferroelectric liquid crystal has been used as an element for intensity-modulating and outputting input image information in real time. In addition, the inventors
Japanese Patent Application No. 02-239594 also showed a driving method for obtaining an output having continuous gradation in the above device.
【0003】[0003]
【発明が解決しようとする課題】しかし、従来の強誘電
性液晶を用いた空間光変調器及びその駆動方法によって
は、いずれも書き込み光強度に対して一つの閾値を持つ
のみであり、例えば2入力光(書き込み光)に対して1
出力光(読み出し光)のデジタルなロジックを考えた場
合、閾値に対する入力光強度の設定によってANDまた
はORを得ることはできても、NANDやEORを得る
ことはできず、素子を幾つもカスケードに接続して、同
期させて用いる等の方法を用いなければならず、光コン
ピューティング等への応用を妨げていた。また、アナロ
グのフーリエ光情報処理系においては、0次光の処理、
ダイナミックレンジの点で高次領域は利用不可能であっ
た。However, depending on the conventional spatial light modulator using the ferroelectric liquid crystal and its driving method, each has only one threshold value for the writing light intensity, for example, 2 1 for input light (writing light)
Considering the digital logic of output light (reading light), it is not possible to obtain NAND or EOR even if AND or OR can be obtained by setting the input light intensity with respect to the threshold value, and several elements are cascaded. It was necessary to use a method such as connecting and synchronizing and using, which hindered application to optical computing and the like. Further, in the analog Fourier light information processing system, processing of the 0th order light,
Higher areas were not available in terms of dynamic range.
【0004】そこで、この発明の目的は、従来のこのよ
うな課題を解決するため、強誘電性液晶を用いた空間光
変調器及びその駆動方法において、特殊な素子構造を用
いることなく光情報処理において、有用な機能を示すこ
とが可能な、第二の閾値を発現させることを可能とし、
これを応用する事によってデジタル系、アナログ系いず
れに関してもその応用範囲を飛躍的に増大せしめるもの
である。SUMMARY OF THE INVENTION Therefore, an object of the present invention is to solve the above-mentioned conventional problems, and in a spatial light modulator using a ferroelectric liquid crystal and a driving method thereof, optical information processing without using a special element structure. In, it is possible to express a second threshold, which can show a useful function,
By applying this, the range of application will be dramatically increased for both digital and analog systems.
【0005】[0005]
【課題を解決するための手段】上記問題を解決するため
に、本発明では水素化アモルファスシリコン光導電層と
強誘電性液晶光変調層を組み合わせた光変調器におい
て、該光導電膜は0.1〜5μmの厚みを有するイント
リンシックな水素化アモルファスシリコンであり、該強
誘電性液晶層は0.5〜5μmの厚みを有し、書き込み
光として強度の書き込み面での最大値が0.01mW/
cm2 以上の光を用い、読み出し光を常時照射しなが
ら、書き込みを行ない、書き込まれた像をメモリー状態
で読み出しを行う場合に、書き込み光が照射されていな
い状態で強誘電性液晶分子が安定化されている一方の安
定状態から他方の安定状態へ遷移する場合の書き込み光
強度の第一の閾値よりも書き込み光が強い領域に、より
強い書き込み光が照射された領域の強誘電性液晶分子
が、逆に前記一方の安定状態に遷移する第二の閾値を発
現させ、さらに駆動パルス幅、電圧、バイアス光の照射
によって第一及び第二の閾値を制御可能とした。In order to solve the above problems, according to the present invention, in a light modulator in which a hydrogenated amorphous silicon photoconductive layer and a ferroelectric liquid crystal light modulating layer are combined, the photoconductive film has a thickness of 0. Intrinsic hydrogenated amorphous silicon having a thickness of 1 to 5 μm, the ferroelectric liquid crystal layer has a thickness of 0.5 to 5 μm, and the maximum intensity of writing light is 0.01 mW on the writing surface. /
When writing is performed by constantly irradiating the reading light with light of cm 2 or more, and the written image is read in the memory state, the ferroelectric liquid crystal molecules are stable in the state where the writing light is not radiated. Liquid crystal molecules in a region irradiated with stronger writing light in a region where the writing light is stronger than the first threshold of the writing light intensity when transitioning from one stable state to the other stable state However, on the contrary, the second threshold value that transits to the one stable state is expressed, and the first and second threshold values can be controlled by the drive pulse width, the voltage, and the irradiation of the bias light.
【0006】[0006]
【作用】前記の方法を用いる事により、書き込み光強度
に対して2つの閾値が得られ、しかもその値が制御可能
となり、これを利用することによって、デジタル光情報
処理においては1つの素子を用いるのみで、実用的なロ
ジックを全て実現することが可能である。また、アナロ
グ系においても0次光の除去等が簡単に行える。これに
よってデジタル系、アナログ系いずれに関しても、強誘
電性液晶空間光変調器の応用範囲を飛躍的に増大させる
事ができる。By using the above method, two threshold values for the writing light intensity can be obtained and the values can be controlled. By using this, one element is used in digital optical information processing. Only by doing so, it is possible to realize all practical logic. Further, even in an analog system, removal of 0th order light can be easily performed. As a result, the application range of the ferroelectric liquid crystal spatial light modulator can be dramatically increased in both digital and analog systems.
【0007】[0007]
【実施例】以下に図面を用いて本発明を詳細に説明す
る。図3は、本発明に係る光書き込み型強誘電性液晶空
間光変調器の構造を示す模式図である。液晶分子を挟持
するための基板31a、31bとして、両面をHe−Neレ
ーザー波長において、平行平面度λ/5以下に研磨した
厚さ5mmの透明ガラス基板を用いた。両基板の表面には
ITO透明電極層32a、32bを設けた。光による書き込
み側の透明電極層32a上には2.5μmの厚さの水素化
アモルファスシリコン(a−Si:H)光導電層35を形
成した。さらに両基板の表面には基板の法線方向から85
゜の入射角で、且つ組み合わせた状態で書き込み側及び
読み出し側の基板上の入射方向が一致するように一酸化
珪素を斜方蒸着した配向膜層33a、33bを設けた。The present invention will be described in detail below with reference to the drawings. FIG. 3 is a schematic diagram showing the structure of an optical writing type ferroelectric liquid crystal spatial light modulator according to the present invention. As the substrates 31a and 31b for sandwiching liquid crystal molecules, transparent glass substrates with a thickness of 5 mm whose both surfaces were polished to a parallel flatness of λ / 5 or less at a He-Ne laser wavelength were used. ITO transparent electrode layers 32a and 32b were provided on the surfaces of both substrates. A 2.5 μm thick hydrogenated amorphous silicon (a-Si: H) photoconductive layer 35 was formed on the transparent electrode layer 32a on the light writing side. Furthermore, the surface of both boards is 85 degrees from the normal direction of the boards.
Orientation film layers 33a and 33b in which silicon monoxide was obliquely vapor-deposited were provided so that the incident directions on the write-side and read-side substrates coincided with each other at an incident angle of ° and combined.
【0008】次に、1.0 μmの平均粒径を持つシリカ球
を外周シール材に混合分散し、凸版印刷法を用いて前記
シール材を印刷塗布した後2枚の基板を接着し、強誘電
性液晶を狭持する間隙を形成した。強誘電性液晶組成物
34としては、SCE−13(BDH社製)等を用い、ア
イソトロピック相迄昇温したのち、真空注入しスメクチ
ックC相迄徐冷して均一な配向を得た。Next, silica spheres having an average particle diameter of 1.0 μm are mixed and dispersed in the outer peripheral sealing material, the sealing material is applied by printing using a letterpress printing method, and then two substrates are adhered to each other to obtain a ferroelectric property. A gap for holding the liquid crystal was formed. Ferroelectric liquid crystal composition
As 34, SCE-13 (manufactured by BDH) was used. After the temperature was raised to the isotropic phase, vacuum injection was performed and the smectic C phase was gradually cooled to obtain a uniform orientation.
【0009】図4は書き込み、読み出し実験を行った光
学系のシステム図である。書き込み光源41はNEC製の
He−Neレーザー(最大出力150mW)を用い、偏
光板42を通して強度を制御した。書き込み光はミラー43
a、43bで反射され、本発明に係る強誘電性液晶空間光
変調器44へ斜めに照射される。(書き込み光の光路には
10倍のビームエキスパンダ45aが挿入される場合もあ
る)読み出し光源46は、メレスグリオ製のHe−Neレ
ーザー(出力10mW)を用い、光量を調節するための
NDフィルター47、10倍のビームエキスパンダ45b 、
ビームスプリッタ48を通って本発明に係る強誘電性液晶
空間光変調器44へ照射され、強誘電性液晶層で変調され
つつ強誘電性液晶層と水素化アモルファスシリコン光導
電層の界面で反射され、再びビームスプリッタ48に入射
する。FIG. 4 is a system diagram of an optical system in which writing and reading experiments were conducted. A He-Ne laser (maximum output 150 mW) manufactured by NEC was used as the writing light source 41, and the intensity was controlled through the polarizing plate 42. Writing light is mirror 43
The light is reflected by a and 43b, and is obliquely applied to the ferroelectric liquid crystal spatial light modulator 44 according to the present invention. (The beam expander 45a of 10 times may be inserted in the optical path of the writing light.) The reading light source 46 uses a Heles-Ne laser (output 10 mW) made by Melles Griot, and the ND filter 47 for adjusting the light amount. 10x beam expander 45b,
It is irradiated to the ferroelectric liquid crystal spatial light modulator 44 according to the present invention through the beam splitter 48, and is reflected by the interface between the ferroelectric liquid crystal layer and the hydrogenated amorphous silicon photoconductive layer while being modulated by the ferroelectric liquid crystal layer. , Enters the beam splitter 48 again.
【0010】ここで、ビームスプリッタ面で反射された
光が偏光板49で検光され、CCDカメラ50で観測され
る。読み出し光源46は書き込み光が照射されていない場
合の強誘電性液晶層の安定状態に対して偏波面が変調を
受けない方位に配置され、偏光板49は上記の状態での反
射光に対しクロスに配置されている。即ち、書き込み光
の無い状態では読み出しは暗状態となる。観察はCCD
カメラ50で取り込んだ画像をCRT51に表示し、撮影し
た。また、CCDカメラ50の代わりにフォトディテクタ
ー52を置いて光学応答をも測定した。駆動は、自作のド
ライバー53を用いて行った。Here, the light reflected by the beam splitter surface is detected by the polarizing plate 49 and observed by the CCD camera 50. The reading light source 46 is arranged in a direction in which the polarization plane is not modulated with respect to the stable state of the ferroelectric liquid crystal layer when the writing light is not irradiated, and the polarizing plate 49 crosses the reflected light in the above state. It is located in. That is, the reading is in the dark state in the absence of the writing light. CCD observation
The image captured by the camera 50 was displayed on the CRT 51 and photographed. Further, the photodetector 52 was placed instead of the CCD camera 50, and the optical response was also measured. The driving was performed using a self-made driver 53.
【0011】なお、書き込みに用いられる光源はHe−
Neレーザー、Arレーザー、半導体レーザー、ハロゲ
ンランプのいずれかであり、読み出し光に用いられる光
源はHe−Neレーザー、Arレーザー、半導体レーザ
ー、ハロゲンランプのいづれかであればよい。上記のシ
ステムを用いて、以下の書き込み実験を行った。The light source used for writing is He-
It is any one of a Ne laser, an Ar laser, a semiconductor laser, and a halogen lamp, and the light source used for the reading light may be any one of a He—Ne laser, an Ar laser, a semiconductor laser, and a halogen lamp. The following writing experiment was conducted using the above system.
【0012】図1は、本発明による空間光変調器に、
4.63μW/cm2 の書き込み光を照射し続けながら
書き込み光強度を変化させて、メモリー状態で読み出し
た場合の読み出し光強度を示したグラフである。強誘電
性液晶を用いた光変調層は双安定性を有しており、メモ
リ状態での読み出し光強度であるため、読み出し光は明
状態、暗状態の二値で得られており、且つ、書き込み光
強度が大きくなるに従って暗状態から明状態に遷移する
第一の閾値11と、明状態から暗状態に遷移する第二の閾
値12が得られている。なお、この実施例ではバイアス光
は照射されておらず、駆動波形は消去パルス+9.15
V2.5ms、書き込みパルス−9.15V2ms、フ
レーム周波数100Hzである。第一の閾値は書き込み
光強度0.2mW/cm2 付近に、第二の閾値は書き込
み光強度2mW/cm2 付近に現れている。FIG. 1 shows a spatial light modulator according to the present invention.
6 is a graph showing the read light intensity in the case of reading in a memory state by changing the write light intensity while continuously irradiating the write light of 4.63 μW / cm 2 . Since the light modulation layer using the ferroelectric liquid crystal has bistability and has the read light intensity in the memory state, the read light is obtained in the binary state of the bright state and the dark state, and A first threshold value 11 that transitions from a dark state to a bright state and a second threshold value 12 that transitions from a bright state to a dark state are obtained as the writing light intensity increases. In this embodiment, the bias light is not emitted, and the drive waveform is the erase pulse +9.15.
V2.5 ms, write pulse −9.15 V2 ms, frame frequency 100 Hz. The first threshold appears near the writing light intensity of 0.2 mW / cm 2 , and the second threshold appears near the writing light intensity of 2 mW / cm 2 .
【0013】図2は、本発明による空間光変調器に、
4.63μW/cm2 の書き込み光を照射し続けなが
ら、He−Neレーザービーム(NEC製75mW)
を、中心200μmピンホール内の強度3.14μW迄
弱めた状態で書き込み光として照射し、メモリ状態で読
み出した場合の読み出し像の写真である。バイアス光は
照射されておらず、駆動波形は消去パルス+9.15
V,2.5ms、書き込みパルス−9.15V,2m
s、フレーム周波数100Hzである。写真はCCDで
取り込んだ画像をCRTに表示し、CRTの画面を撮影
したものである。そのため、写真にはCRTの走査線に
対応する横方向の線が見えている。写真から、第一の閾
値以上で第二の閾値以下のリング状の部分21のみが明状
態に反転、メモリされていることが分かる。第二の閾値
以上の書き込み光強度を有する中央の部分22は、第一の
閾値以下である周辺の暗状態の部分23と全く同じ反射率
であった。なお、写真でリング上の部分の輪郭が乱れて
いるのは、書き込み光の強度分布によるものであり、実
際のシステムにおいては問題は生じない。FIG. 2 shows a spatial light modulator according to the present invention.
He-Ne laser beam (75 mW made by NEC) while continuously irradiating the writing light of 4.63 μW / cm 2.
Is a photograph of a read image in the case of irradiating as a writing light in a state where the intensity is weakened to 3.14 μW in the center 200 μm pinhole, and reading is performed in a memory state. Bias light is not emitted and the drive waveform is erase pulse +9.15
V, 2.5 ms, write pulse-9.15 V, 2 m
s, the frame frequency is 100 Hz. The photograph is an image captured by the CCD, displayed on the CRT, and the screen of the CRT is taken. Therefore, a horizontal line corresponding to the scanning line of the CRT is visible in the photograph. From the photograph, it can be seen that only the ring-shaped portion 21 that is equal to or greater than the first threshold value and equal to or less than the second threshold value is inverted and stored in the bright state. The central portion 22 having the writing light intensity equal to or higher than the second threshold had exactly the same reflectance as the peripheral dark-state portion 23 equal to or lower than the first threshold. It should be noted that the fact that the contour of the portion on the ring is disturbed in the photograph is due to the intensity distribution of the writing light, and no problem occurs in an actual system.
【0014】これにより、第一及び第二の閾値の発現が
明確に実証された。This clearly demonstrated the expression of the first and second thresholds.
【0015】[0015]
【発明の効果】以上述べてきたように本発明の方法によ
れば、強誘電性液晶を用いた光書き込み型液晶空間光変
調器において、特殊な素子構造を用いることなく光情報
処理において有用な機能を示す事が可能な、第二の閾値
を発現させることを可能とし、これを応用する事によっ
てデジタル系、アナログ系いずれに関してもその応用範
囲を飛躍的に増大する効果がある。As described above, according to the method of the present invention, a photo-writing type liquid crystal spatial light modulator using a ferroelectric liquid crystal is useful in optical information processing without using a special element structure. It is possible to express a second threshold value that can exhibit a function, and by applying this, there is an effect of dramatically increasing the range of application in both digital and analog systems.
【図1】本発明による空間光変調器に、書き込み光を照
射し続けながら書き込み光強度を変化させて、メモリー
状態で読み出した場合の読み出し光強度を示したグラフ
である。FIG. 1 is a graph showing the read light intensity when the spatial light modulator according to the present invention is read in a memory state by changing the write light intensity while continuously irradiating the write light.
【図2】本発明による空間光変調器に、書き込み光を照
射し続けながら、He−Neレーザービームを書き込み
光として照射し、メモリー状態で読み出した場合の読み
出し像の図面代用写真である。FIG. 2 is a drawing-substituting photograph of a read-out image when a spatial light modulator according to the present invention is irradiated with a writing light and a He—Ne laser beam is irradiated as the writing light and is read in a memory state.
【図3】本発明に係る光書き込み型強誘電性液晶空間光
変調器の構造を示す模式図である。FIG. 3 is a schematic diagram showing the structure of an optical writing type ferroelectric liquid crystal spatial light modulator according to the present invention.
【図4】書き込み、読み出し実験を行った光学系のシス
テム図である。FIG. 4 is a system diagram of an optical system in which writing and reading experiments are performed.
11 第一の閾値 12 第二の閾値 21 明状態の部分(第一の閾値以上第二の閾値以下の
部分) 22 暗状態の部分1(第二の閾値以上の部分) 23 暗状態の部分2(第一の閾値以下の部分) 31a、31b 透明基板 32a、32b 透明電極 33a、33b 配向膜層 34 強誘電性液晶層 35 光導電膜 41 書き込み光源 42 偏光板 43a、43b ミラー 44 強誘電性液晶空間光変調器 45a、45b ビームエキスパンダ 46 読み出し光源 47 NDフィルター 48 ビームスプリッタ 49 偏光板 50 CCDカメラ 51 CRT 52 フォトディテクター 53 ドライバー11 First Threshold 12 Second Threshold 21 Bright State Part (First Threshold or More and Second Threshold or Less) 22 Dark State Part 1 (Second Threshold or More) 23 Dark State Part 2 (Parts Below First Threshold) 31a, 31b Transparent Substrates 32a, 32b Transparent Electrodes 33a, 33b Alignment Film Layer 34 Ferroelectric Liquid Crystal Layer 35 Photoconductive Film 41 Writing Light Source 42 Polarizing Plates 43a, 43b Mirror 44 Ferroelectric Liquid Crystal Spatial light modulator 45a, 45b Beam expander 46 Readout light source 47 ND filter 48 Beam splitter 49 Polarizing plate 50 CCD camera 51 CRT 52 Photodetector 53 Driver
───────────────────────────────────────────────────── フロントページの続き (72)発明者 海老原 照夫 東京都江東区亀戸6丁目31番1号 セイコ ー電子工業株式会社内 (72)発明者 瀬倉 利江子 東京都江東区亀戸6丁目31番1号 セイコ ー電子工業株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Teruo Ebihara 6-31-1, Kameido, Koto-ku, Tokyo Seiko Electronics Co., Ltd. (72) Rieko Sekura 6-31-1, Kameido, Koto-ku, Tokyo No. Seiko Electronics Industry Co., Ltd.
Claims (7)
し手段及び電圧印加手段を具備し、透明電極上に光導電
膜が形成されたガラス基板と、透明電極の形成されたガ
ラス基板のそれぞれの対向する表面に液晶配向膜が形成
された一組のガラス基板が対向配置され、その間隙に強
誘電性液晶組成物が封入されてなる強誘電性液晶空間光
変調器において、該光導電膜は0.1〜5μmの厚みを
有するイントリンシックな水素化アモルファスシリコン
であり、該強誘電性液晶層は0.5〜5μmの厚みを有
し、書き込み光として強度は書き込み面での最大値が
0.01mW/cm2 以上の光を用い、読み出し光を常
時照射しながら書き込みを行ない、書き込まれた像をメ
モリー状態で読み出しを行う場合に、書き込み光が照射
されていない状態で強誘電性液晶分子が安定化されてい
る一方の安定状態から他方の安定状態へ遷移する場合の
書き込み光強度の第一の閾値よりも書き込み光が強い領
域に、より強い書き込み光が照射された領域の強誘電性
液晶分子が逆に前記一方の安定状態に遷移する第二の閾
値を有することを特徴とする空間光変調器。1. A glass substrate having a photo-conductive film formed on a transparent electrode and a glass substrate having a transparent electrode, which are provided with a light-writing device, a light-reading device, and a voltage applying device, which face each other. In a ferroelectric liquid crystal spatial light modulator in which a pair of glass substrates having a liquid crystal alignment film formed on their surfaces are opposed to each other and a ferroelectric liquid crystal composition is sealed in the gap, the photoconductive film has a thickness of 0. Intrinsic hydrogenated amorphous silicon having a thickness of 1 to 5 μm, the ferroelectric liquid crystal layer has a thickness of 0.5 to 5 μm, and the intensity of writing light is 0.01 mW at the maximum value on the writing surface. / Cm 2 or more of light, writing is performed while irradiating the reading light all the time, and when reading the written image in the memory state, it is urged without the writing light being radiated. A region where the writing light is stronger than the first threshold of the writing light intensity when the electronic liquid crystal molecule is stabilized and transits from one stable state to the other stable state. 2. The spatial light modulator according to claim 1, wherein the ferroelectric liquid crystal molecule has a second threshold value that causes the liquid crystal molecule to transit to the one stable state.
誘電体ミラーが形成されている事を特徴とする請求項1
記載の空間光変調器。2. A dielectric mirror for light separation is formed between the photoconductive film and the liquid crystal alignment layer.
The spatial light modulator described.
一のパルス電圧と、前記第一のパルス電圧と逆の極性を
有する書き込みを行うための第二のパルス電圧、及びメ
モリーの期間からなり、読み出しはメモリーの期間に行
なわれ、前記第一及び第二のパルス電圧のパルス幅また
は波高は、第一及び第二の閾値を制御するため別個に制
御されることを特徴とする請求項1記載の空間光変調器
の駆動方法。3. The applied drive voltage is determined from a first pulse voltage for erasing, a second pulse voltage for writing having a polarity opposite to that of the first pulse voltage, and a memory period. The reading is performed during the memory, and the pulse width or pulse height of the first and second pulse voltages is controlled separately to control the first and second thresholds. 2. The method for driving the spatial light modulator according to 1.
れ、且つ前記第一のパルス電圧により決定される液晶分
子の配列方向が、該クロスニコル下において、明または
暗視野状態となるように配置されることを特徴とする請
求項3記載の空間光変調器の駆動方法。4. A crossed Nicol is arranged in the readout optical system, and the liquid crystal molecules are arranged so that the arrangement direction of the liquid crystal molecules determined by the first pulse voltage is in a bright or dark field state under the crossed Nicols. 4. The method for driving a spatial light modulator according to claim 3, wherein:
源以外に、書き込み側または読み出し側から、バイアス
光が照射され、このバイアス光の強度を制御することに
よって前記第一及び第二の閾値を制御することを特徴と
する請求項1記載の空間光変調器の駆動方法。5. A bias light is irradiated from a writing side or a reading side in addition to a light source used for writing and reading light, and the first and second threshold values are controlled by controlling the intensity of the bias light. The method of driving a spatial light modulator according to claim 1, wherein
ッターを有し、読み出し時には書き込み光が照射されな
いことを特徴とする請求項1記載の空間光変調器の駆動
方法。6. The method for driving a spatial light modulator according to claim 1, wherein the writing optical system used has a shutter in the system, and the writing light is not irradiated at the time of reading.
を制御可能な2つ以上の系からなり、2つ以上の像が同
一の書き込み面に同時に照射されることを特徴とする請
求項1記載の空間光変調器の駆動方法。7. The writing optical system used comprises two or more systems whose intensity can be controlled independently, and two or more images are simultaneously irradiated on the same writing surface. Driving method for spatial light modulators.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2884692A JPH05196960A (en) | 1992-01-20 | 1992-01-20 | Space optical modulator and driving method thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2884692A JPH05196960A (en) | 1992-01-20 | 1992-01-20 | Space optical modulator and driving method thereof |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH05196960A true JPH05196960A (en) | 1993-08-06 |
Family
ID=12259738
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2884692A Pending JPH05196960A (en) | 1992-01-20 | 1992-01-20 | Space optical modulator and driving method thereof |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH05196960A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0634994A (en) * | 1992-07-20 | 1994-02-10 | Seiko Instr Inc | Driving method for space optical modulator |
-
1992
- 1992-01-20 JP JP2884692A patent/JPH05196960A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0634994A (en) * | 1992-07-20 | 1994-02-10 | Seiko Instr Inc | Driving method for space optical modulator |
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