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JPH0652353B2 - Light modulator - Google Patents
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JPH0652353B2 - Light modulator - Google Patents

Light modulator

Info

Publication number
JPH0652353B2
JPH0652353B2 JP61082922A JP8292286A JPH0652353B2 JP H0652353 B2 JPH0652353 B2 JP H0652353B2 JP 61082922 A JP61082922 A JP 61082922A JP 8292286 A JP8292286 A JP 8292286A JP H0652353 B2 JPH0652353 B2 JP H0652353B2
Authority
JP
Japan
Prior art keywords
liquid crystal
diffraction grating
light
transparent
state
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
JP61082922A
Other languages
Japanese (ja)
Other versions
JPS62238529A (en
Inventor
知幸 梅沢
千織 望月
和也 石渡
石井  隆之
幸俊 大久保
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 JP61082922A priority Critical patent/JPH0652353B2/en
Priority to US07/033,773 priority patent/US4850681A/en
Publication of JPS62238529A publication Critical patent/JPS62238529A/en
Publication of JPH0652353B2 publication Critical patent/JPH0652353B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Liquid Crystal (AREA)

Description

【発明の詳細な説明】 <技術分野> 本発明は、光変調素子、特に回折格子と液晶とを組み合
わせて液晶の屈折率を制御することにより入射光に所望
の回折現象を生じせしめる光変調素子に関する。
Description: TECHNICAL FIELD The present invention relates to a light modulation element, and more particularly to a light modulation element that causes a desired diffraction phenomenon in incident light by controlling the refractive index of liquid crystal by combining a diffraction grating and liquid crystal. Regarding

<従来技術> 従来から良く知られている光変調素子としては、互いに
偏光方向が直交する様に配した一対の偏光板と、この一
対の偏光板間に配され一対の透明基板の相対する基板面
に互いに直交する配向処理を施して液晶を封入した素子
とから成り、この液晶の配向状態をねじれた状態と基板
面に垂直に向いた状態との間でスイツチングを行ない入
射光の変調をする所謂TN(ツウイストネマチツク)型
の液晶表示素子がある。この種の表示素子は構成が簡便
で駆動が容易なことから多岐に亘り利用されているが、
2枚の偏光板を利用して光束の透過及び遮断を行なう為
に消色時、即ち光透過時の透過率が悪く光束利用効率の
面からは好ましい光変調素子とは言えなかった。
<Prior Art> Conventionally well-known light modulation elements include a pair of polarizing plates arranged so that polarization directions thereof are orthogonal to each other, and a pair of transparent substrates arranged between the pair of polarizing plates and facing each other. It is composed of a device in which liquid crystal is enclosed by subjecting the surfaces to mutually orthogonal alignment processing, and the incident light is modulated by switching the alignment state of this liquid crystal between a twisted state and a state oriented perpendicular to the substrate surface. There is a so-called TN (twist nematic) liquid crystal display element. This type of display element is widely used because of its simple structure and easy driving.
Since the light beams are transmitted and blocked by using two polarizing plates, the transmittance at the time of erasing, that is, at the time of transmitting light is poor, and it cannot be said to be a preferable light modulator in terms of light beam utilization efficiency.

又、液晶を利用した同種の表示素子として、液晶分子に
色素を混入させて用いる所謂ゲスト・ホストモードの液
晶素子があるが、この表示素子に於ても色素が介在する
為に消色時の透過率は良くても70%程度であった。
Further, as a display element of the same type using liquid crystal, there is a so-called guest-host mode liquid crystal element in which a dye is mixed in liquid crystal molecules. The transmittance was about 70% at best.

一方、特公昭53−3928号公報やUSP4,25
1,137等に於て反射型や透過型の位相回折格子と液
晶とを組合せた表示素子や色フイルター素子が開示され
ている。これらで開示されている素子は確かに光束利用
効率は優れているが、特公昭53−3928号公報に開
示されている素子は単なる装飾効果を示すのみであり、
文字や画像を表示する表示素子や光束の透過、遮断を行
なう交変調素子としては満足出来るものではなかった。
又、USP4,251,137に開示されている色フイ
ルター素子は一対の対向する基板面に互いに配列方向が
直交する様に回折格子を形成し、この基板間に液晶を充
填して液晶分子の配向状態を制御することにより屈折率
を変え、回折格子を成す物質と液晶との屈折率差を変え
ることで分光透過率特性を可変にするものであり、光束
利用効率に優れ且つ可変色フイルターとして高性能を有
する。しかしながら、この種の従来の回折格子を用いた
光変調素子は一般に静的状態に於ても入射光を回折して
しまっていた為、実際に表示素子として用いる際は無表
示状態即ち入射光束が全て透過する状態を維持する為に
常時電圧等を印加しておく必要があった。従って、電力
を多く消費する、液晶の配向状態等に依存する為に無表
示状態に於る素子の透過特性が不安定である等、表示素
子としては好ましくない問題をかかえていた。
Meanwhile, Japanese Patent Publication No. 53-3928 and USP 4,25
No. 1,137, etc., a display element and a color filter element in which a reflection type or transmission type phase diffraction grating and a liquid crystal are combined are disclosed. The elements disclosed in these are certainly excellent in luminous flux utilization efficiency, but the element disclosed in Japanese Patent Publication No. 53-3928 shows only a decorative effect.
It was not satisfactory as a display element for displaying characters or images or an intermodulation element for transmitting or blocking a light beam.
In the color filter device disclosed in USP 4,251,137, diffraction gratings are formed on a pair of opposed substrate surfaces so that their arrangement directions are orthogonal to each other, and liquid crystals are filled between the substrates to align liquid crystal molecules. The refractive index is changed by controlling the state, and the spectral transmittance characteristics are made variable by changing the difference in refractive index between the substance forming the diffraction grating and the liquid crystal, which is excellent in luminous flux utilization efficiency and high as a variable color filter. Have performance. However, since the light modulation element using the conventional diffraction grating of this kind generally diffracts the incident light even in the static state, when it is actually used as a display element, the non-display state, that is, the incident light flux is It was necessary to constantly apply a voltage or the like in order to maintain the state of being completely transparent. Therefore, there are problems that are unfavorable for a display device, such as a large amount of power being consumed and the transmission characteristics of the device in the non-display state being unstable due to the alignment state of the liquid crystal and the like.

<発明の概要> 本発明の目的は、上記従来の問題点に鑑み、安定した無
表示状態が得られ、表示素子として用いるのに好適な光
変調素子を提供することにある。
<Summary of Invention> An object of the present invention is to provide a light modulation element suitable for use as a display element, in which a stable non-display state is obtained in view of the above-mentioned conventional problems.

上記目的を達成する為に、本発明に係る光変調素子は、
所定の部材から成る位相型回折格子と該回折格子の溝部
に存する液晶と該液晶の配向状態を変化せしめる制御手
段とを有する素子であって、前記制御手段が前記回折格
子の側面に設けた電極を有することを特徴とする。
In order to achieve the above object, the light modulation element according to the present invention,
An element having a phase type diffraction grating composed of a predetermined member, a liquid crystal existing in a groove portion of the diffraction grating, and a control means for changing an alignment state of the liquid crystal, wherein the control means is an electrode provided on a side surface of the diffraction grating. It is characterized by having.

尚、本発明の更なる特徴は以下に示す実施例より明らか
になるであろう。
Further features of the present invention will be apparent from the examples shown below.

<実施例> 第1図(A),(B)は本発明に係る光変調素子の一実
施例を示す模式図で、1は透明基板、2は透明電極、3
は透明絶縁膜、4は液晶、5は回折格子を成す透明絶縁
体、6は透明保護膜で絶縁膜を兼ねる。7はスイツチ、
8は駆動電源、9は入射光、10は零次回折光、10′
は高次回折光を示す。
<Example> FIGS. 1A and 1B are schematic views showing an example of an optical modulator according to the present invention, in which 1 is a transparent substrate, 2 is a transparent electrode, and 3 is a transparent substrate.
Is a transparent insulating film, 4 is a liquid crystal, 5 is a transparent insulator forming a diffraction grating, and 6 is a transparent protective film which also serves as an insulating film. 7 is a switch,
8 is a driving power source, 9 is incident light, 10 is zero-order diffracted light, and 10 '.
Indicates high-order diffracted light.

ここで、第1図(A)はスイツチ7がOFF状態の電界
無印加の状態、第1図(B)はスイツチ7がON状態の
電界印加状態を示しており、又、本実施例に於ては液晶
1として正誘電性ネマチツク液晶を用いるものとする。
Here, FIG. 1A shows a state in which the switch 7 is OFF and no electric field is applied, and FIG. 1B shows a state in which the switch 7 is ON and an electric field is applied, and in the present embodiment. As the liquid crystal 1, a positive dielectric nematic liquid crystal is used.

本実施例に於る光変調素子は、一対の透明基板1の夫々
の片面に透明絶縁膜を形成し、一方の透明基板1の透明
絶縁膜3上に透明絶縁体5からなる矩形状の回折格子を
形成して、該回折格子の側面及び透明絶縁膜3と該回折
格子との界面に透明電極2を設け、該回折格子を透明保
護膜6で被って、回折格子を有する透明基板1と他方の
透明基板1とを透明保護膜3が対向する様に貼り合わせ
て、間隙部に液晶4を封入して構成されている。尚、隣
り合う凸部の透明電極2はリード線を介して駆動電源8
及びスイツチ7と接続されている。更に透明絶縁膜3に
は垂直配向処理が施されており、液晶4の分子は垂直配
向、所謂ホメオトロピツク配向をしている。
In the light modulation element of this embodiment, a transparent insulating film is formed on one surface of each of a pair of transparent substrates 1, and a rectangular diffraction pattern is formed on the transparent insulating film 3 of one transparent substrate 1 by a transparent insulator 5. A grating is formed, a transparent electrode 2 is provided on a side surface of the diffraction grating and an interface between the transparent insulating film 3 and the diffraction grating, and the diffraction grating is covered with a transparent protective film 6 to form a transparent substrate 1 having the diffraction grating. The other transparent substrate 1 is bonded so that the transparent protective film 3 faces it, and the liquid crystal 4 is sealed in the gap. In addition, the transparent electrodes 2 of the adjacent convex portions are connected to the driving power source 8 via the lead wire.
And the switch 7. Further, the transparent insulating film 3 is subjected to vertical alignment treatment, and the molecules of the liquid crystal 4 are vertically aligned, that is, so-called homeotropic alignment.

以下、本光変調素子の機能に関して述べる。The function of the present light modulation element will be described below.

第1図(A)に示す状態、即ちスイツチ7がOFFで透
明電極2間に電圧が印加されていない状態では、前述の
如く液晶4はホメオトロピツク配向をしており、基板1
に対して垂直な方向へ長軸が向いている。この時、入射
光9はその偏光状態に係わりなく液晶4の常屈折率n
を感じる為、透明電極2と透明保護膜6の膜厚が回折格
子のライン幅(凸部の幅)に比べ十分小さいとすれば、
透明絶縁体5の屈折率nを液晶4の常屈折率nと等
しく設定しておくことにより、入射光9は回折作用を受
けることなく本素子を素通りし、零次の出射光10とし
て出射する。
In the state shown in FIG. 1A, that is, in the state where the switch 7 is OFF and no voltage is applied between the transparent electrodes 2, the liquid crystal 4 is homeotropically aligned as described above, and the substrate 1
The long axis is oriented in a direction perpendicular to. At this time, the incident light 9 is normal refractive index n o of the liquid crystal 4 regardless of its polarization state
Therefore, if the film thickness of the transparent electrode 2 and the transparent protective film 6 is sufficiently smaller than the line width of the diffraction grating (width of the convex portion),
By keeping the refractive index n g of the transparent insulator 5 is set equal to the ordinary refractive index n o of the liquid crystal 4, the incident light 9 is passed through the present device without receiving the diffraction action, as the zero-order output light 10 Emit.

一方、第1図(B)に示す状態、即ちスイツチ7がON
で透明電極2間に所定電圧が印加されている状態では、
液晶4の分子の長軸は電界方向に揃い、図示する様に基
板1の面に対して平行な方向へ配向される(ホモジニア
ス配向)。この時、入射光9の偏光成分の内、液晶4の
配向方向と同方向の偏光成分は液晶4の異常屈折率n
を感じる。従って、この偏光成分の光が液晶4の通過す
る際の光路長と透明絶縁体5を通過する際の光路長との
間の光路長差が丁度λ/2(λは入射光の波長)になる
様に液晶4の異常屈折率nと透明絶縁体5の屈折率n
と回折格子の高さTとを設定することにより、入射光
9は零次の出射光10となることはなく全て高次回折光
10′となり出射する。尚、高次回折光10′の回折角
(出射角)は波長λと回折格子のピツチに依存するもの
である。
On the other hand, the state shown in FIG. 1 (B), that is, the switch 7 is turned on.
With a predetermined voltage applied between the transparent electrodes 2,
The major axes of the molecules of the liquid crystal 4 are aligned with the direction of the electric field, and are aligned in a direction parallel to the surface of the substrate 1 (homogeneous alignment) as shown in the figure. At this time, among the polarization components of the incident light 9, the polarization component in the same direction as the alignment direction of the liquid crystal 4 has an extraordinary refractive index n e of the liquid crystal 4.
Feel Therefore, the optical path length difference between the optical path length when the light of the polarization component passes through the liquid crystal 4 and the optical path length when passing through the transparent insulator 5 is just λ / 2 (λ is the wavelength of the incident light). Therefore, the extraordinary refractive index n e of the liquid crystal 4 and the refractive index n e of the transparent insulator 5
By setting g and the height T of the diffraction grating, the incident light 9 does not become the zero-order emitted light 10 but all becomes the higher-order diffracted light 10 '. The diffraction angle (emission angle) of the high-order diffracted light 10 'depends on the wavelength λ and the pitch of the diffraction grating.

即ち、第1図(A),(B)に示す様な矩形状回折格子
に於る零次透過回折光(図中、出射光10)の回折効率
ηは次の(1)式で近似的に表わすことが出来る為、
所定波長λの光の回折効率ηをη≒0とするには
(2)式の条件を満足させれば良いものである。
That is, the diffraction efficiency η o of the zero-order transmitted diffracted light (emitted light 10 in the figure) in the rectangular diffraction grating as shown in FIGS. 1 (A) and (B) is approximated by the following equation (1). Can be expressed as
In order to set the diffraction efficiency η o of the light of the predetermined wavelength λ to η o ≈0, it is sufficient to satisfy the condition of the expression (2).

但し、Δn=|n−n|である。 However, Δn = | n e -n g | it is.

尚、第1図(B)に於て、入射光9の偏光成分の内、液
晶4の配向方向と垂交する方向、即ち回折格子の溝方向
に偏光した偏光成分はスイツチ7がONの電界印加状態
であっても、液晶4の常屈折率nを感じる。従って、
入射光9のこの偏光成分は本実施例に於る光変調素子で
は変調し得ない。従って、任意の偏光特性の入射光を変
調する為には、例えば第1図に示す如き素子を2個用い
て互いに回折格子の配列方向が直交する様に重畳させて
構成すれば良く、重畳した夫々の素子が独立して互いに
直交する偏光成分を変調することが可能である。
In FIG. 1 (B), among the polarization components of the incident light 9, the polarization component polarized in the direction perpendicular to the alignment direction of the liquid crystal 4, that is, the groove direction of the diffraction grating is the electric field in which the switch 7 is ON. even applied state, feel ordinary refractive index n o of the liquid crystal 4. Therefore,
This polarization component of the incident light 9 cannot be modulated by the light modulator of this embodiment. Therefore, in order to modulate the incident light having an arbitrary polarization characteristic, for example, two elements as shown in FIG. 1 may be used so that they are superposed so that the arrangement directions of the diffraction gratings are orthogonal to each other. It is possible for each element to independently modulate polarization components that are orthogonal to each other.

以上説明した様に、本実施例に係る光変調素子に於て
は、電界無印加時に、“明”状態、即ち全透過状態で、
電界印加時には“暗”、即ち変調状態(表示状態)が得
られる為、通常状態(“明”状態)での電流消費がな
く、素子を駆動する為に用いられる駆動回路の設計自由
度も増す。
As described above, in the light modulation element according to the present embodiment, when no electric field is applied, the "bright" state, that is, the total transmission state,
Since "dark", that is, a modulation state (display state) is obtained when an electric field is applied, current consumption in the normal state ("bright" state) is eliminated, and the degree of freedom in designing the drive circuit used to drive the element is increased. .

又、透明電極の電蝕速度も遅くなり、素子としての信頼
性が著しく向上する。従って、表示素子や色フイルタ
ー、光スイツチ等、本光変調素子の適用範囲は大きく拡
がっている。
Also, the electrolytic corrosion rate of the transparent electrode is slowed down, and the reliability as an element is significantly improved. Therefore, the applicable range of the present light modulation element such as a display element, a color filter, an optical switch, etc. is greatly expanded.

更に、当然の事ながら、従来の液晶を利用した表示素子
の様に偏光板や光吸収性物質(例えば色素)を用いない
為に光束利用効率に優れる。
Further, as a matter of course, unlike the display element using the conventional liquid crystal, the polarizing plate and the light absorbing substance (for example, dye) are not used, so that the luminous flux utilization efficiency is excellent.

本発明に係る光変調素子を成す回折格子は第1図から解
る様に、凹凸のレリーフパターンから成る所謂位相型の
回折格子であり、この種のレリーフパターンの形成する
方法としては、例えばフオトリングラフィーとドライエ
ツチングを組み合わせた方法、熱硬化性樹脂あるいは紫
外線硬化性樹脂等を用いたレプリカ法、ルーリングエン
ジンを用いた切削法あるいはエンボス法等の各種方法が
挙げられる。
As can be seen from FIG. 1, the diffraction grating forming the light modulation element according to the present invention is a so-called phase type diffraction grating consisting of a relief pattern of concavities and convexities. As a method of forming this kind of relief pattern, for example, a photolin There are various methods such as a method combining a graphic and dry etching, a replica method using a thermosetting resin or an ultraviolet curable resin, a cutting method using a ruling engine or an embossing method.

又、本実施例に於ては回折格子の形状として矩形状のも
のを有する素子を示しているが、この形状が如何なる形
であっても光の変調は可能である。例えば、三角波状や
正弦波状、及び非対称形状等各種形状の回折格子を用い
ることが出来、回折光間の分離角は回折格子のピツチと
入射光の波長に依存し、例えば零次透過回折光の分光透
過率特性は回折格子の形状(波形プロフイール)と高さ
T、及び屈折率差Δnに主として依存する。即ち、矩形
状回折格子に於る零次透過回折光の回折効率ηを表わ
す前記(1)式は、三角波状や正弦波状の回折格子に於
る回折効率に対しては適用出来ず、設計の際は夫々の回
折格子形状に対応する式を用いる。
Further, in the present embodiment, an element having a rectangular shape as a diffraction grating is shown, but light can be modulated even if this shape has any shape. For example, a diffraction grating of various shapes such as a triangular wave shape, a sine wave shape, and an asymmetrical shape can be used, and the separation angle between the diffracted lights depends on the pitch of the diffraction grating and the wavelength of the incident light. The spectral transmittance characteristics mainly depend on the shape (waveform profile) and height T of the diffraction grating and the refractive index difference Δn. That is, the equation (1) representing the diffraction efficiency η o of the zero-order transmitted diffracted light in the rectangular diffraction grating cannot be applied to the diffraction efficiency in the triangular wave-shaped or sinusoidal-shaped diffraction grating, and In this case, the equations corresponding to the respective diffraction grating shapes are used.

又、本実施例では所謂透過型の光変調素子を示している
が、反射型の光変調素子として用いることも可能であ
る。この場合、第1図に於る一対の透明電極3の内一方
を使用波長(域)に於て反射特性を備えた部材で構成し
たり、又は基板1と透明電極3の界面に反射膜を施す
か、回折格子を成す凹凸のレリーフパターン全面に反射
膜を形成すれば良い。
Further, although a so-called transmissive light modulation element is shown in this embodiment, it can be used as a reflective light modulation element. In this case, one of the pair of transparent electrodes 3 shown in FIG. 1 is composed of a member having a reflection characteristic in the used wavelength (band), or a reflective film is provided on the interface between the substrate 1 and the transparent electrode 3. It may be applied or a reflection film may be formed on the entire surface of the relief pattern having concaves and convexes forming a diffraction grating.

更に、第1図に示す素子に於ては透明電極2が透明保護
膜3との界面にも形成してあるが、この界面には必ずし
も透明電極2を形成する必要はなく、第1図の素子の如
く所謂正誘電性ネマチツク液晶に対して横電界(基板1
の面に平行な電界)を印加出来れば良い。従って、通
常、回折格子を形成している透明絶縁体の側壁に形成さ
れていれば良い。又、液晶の配向状態を制御する手段と
しては電界に限られるものではなく、熱や磁界等を発す
る制御手段を用いることも可能であるが、素子構成や制
御方法の簡便さや応答特性等を鑑みると電界による制御
が最も好ましい。
Further, in the element shown in FIG. 1, the transparent electrode 2 is also formed on the interface with the transparent protective film 3, but it is not always necessary to form the transparent electrode 2 on this interface. A so-called positive dielectric nematic liquid crystal such as an element is applied to a lateral electric field (substrate 1
It is only necessary to apply an electric field parallel to the plane. Therefore, it is usually sufficient that it is formed on the side wall of the transparent insulator forming the diffraction grating. Further, the means for controlling the alignment state of the liquid crystal is not limited to the electric field, and it is possible to use a control means for generating heat or a magnetic field, but in view of the element structure, the simplicity of the control method, the response characteristics, etc. And the control by the electric field is most preferable.

<発明の効果> 以上、本発明に係る光変調素子は、静的状態に於て全透
過状態を得て、無表示状態の安定化を可能にした表示素
子や色フイルター等に好適な素子である。
<Effects of the Invention> As described above, the light modulation element according to the present invention is an element suitable for a display element, a color filter, or the like that can obtain a total transmission state in a static state and can stabilize a non-display state. is there.

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

第1図(A),(B)は本発明に係る光変調素子の一実
施例を示す模式図で、第1図(A)は静的状態、第1図
(B)は駆動状態を示す。 1……透明基板 2……透明電極 3……透明絶縁膜 4……液晶 5……透明絶縁体(回折格子) 6……透明保護膜 7……スイツチ 8……駆動電源 9……入射光 10……零次回折光 10′……高次回折光
1 (A) and 1 (B) are schematic views showing an embodiment of the light modulation element according to the present invention. FIG. 1 (A) shows a static state and FIG. 1 (B) shows a driving state. . 1 ... Transparent substrate 2 ... Transparent electrode 3 ... Transparent insulating film 4 ... Liquid crystal 5 ... Transparent insulator (diffraction grating) 6 ... Transparent protective film 7 ... Switch 8 ... Drive power supply 9 ... Incoming light 10 ... Zero-order diffracted light 10 '... High-order diffracted light

───────────────────────────────────────────────────── フロントページの続き (72)発明者 石井 隆之 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 大久保 幸俊 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 ─────────────────────────────────────────────────── ─── Continued front page (72) Inventor Takayuki Ishii 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc. (72) Inventor Yukitoshi Okubo 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Within the corporation

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】所定の部材から成る回折格子と該回折格子
の溝部に存する液晶と該液晶の配向状態を変化せしめる
制御手段とを有する素子であって、前記制御手段が前記
回折格子の側面に設けた電極を有する光変調素子。
1. An element having a diffraction grating made of a predetermined member, a liquid crystal existing in a groove portion of the diffraction grating, and a control means for changing an alignment state of the liquid crystal, wherein the control means is provided on a side surface of the diffraction grating. A light modulation element having an electrode provided.
【請求項2】前記液晶が正の誘電性を有するネマチツク
液晶である特許請求の範囲第(1)項記載の光変調素
子。
2. The light modulation element according to claim 1, wherein the liquid crystal is a nematic liquid crystal having a positive dielectric property.
【請求項3】前記制御手段が電界印加を行なう手段であ
って、前記回折格子の凸部側面に電極を有する特許請求
の範囲第(2)項記載の光変調素子。
3. An optical modulator according to claim 2, wherein said control means is a means for applying an electric field and has an electrode on the side surface of the convex portion of said diffraction grating.
JP61082922A 1986-04-07 1986-04-09 Light modulator Expired - Fee Related JPH0652353B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP61082922A JPH0652353B2 (en) 1986-04-09 1986-04-09 Light modulator
US07/033,773 US4850681A (en) 1986-04-07 1987-04-03 Optical modulation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61082922A JPH0652353B2 (en) 1986-04-09 1986-04-09 Light modulator

Publications (2)

Publication Number Publication Date
JPS62238529A JPS62238529A (en) 1987-10-19
JPH0652353B2 true JPH0652353B2 (en) 1994-07-06

Family

ID=13787731

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61082922A Expired - Fee Related JPH0652353B2 (en) 1986-04-07 1986-04-09 Light modulator

Country Status (1)

Country Link
JP (1) JPH0652353B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4984389B2 (en) * 2004-12-24 2012-07-25 旭硝子株式会社 Horizontal electric field drive liquid crystal cell and wavelength tunable filter using the same
JP7393066B2 (en) * 2022-04-13 2023-12-06 株式会社SteraVision Liquid crystal panels and optical switching elements

Also Published As

Publication number Publication date
JPS62238529A (en) 1987-10-19

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