JPH06230408A - Optical modulation element - Google Patents
Optical modulation elementInfo
- Publication number
- JPH06230408A JPH06230408A JP3270993A JP3270993A JPH06230408A JP H06230408 A JPH06230408 A JP H06230408A JP 3270993 A JP3270993 A JP 3270993A JP 3270993 A JP3270993 A JP 3270993A JP H06230408 A JPH06230408 A JP H06230408A
- Authority
- JP
- Japan
- Prior art keywords
- liquid crystal
- light
- layer
- modulation element
- phase plate
- 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.)
- Granted
Links
- 230000003287 optical effect Effects 0.000 title abstract description 14
- 239000004973 liquid crystal related substance Substances 0.000 claims abstract description 95
- 239000000758 substrate Substances 0.000 claims abstract description 32
- 230000007704 transition Effects 0.000 claims 1
- 230000010287 polarization Effects 0.000 description 17
- 238000010586 diagram Methods 0.000 description 9
- 230000005684 electric field Effects 0.000 description 9
- 238000002834 transmittance Methods 0.000 description 6
- 239000010408 film Substances 0.000 description 5
- 125000006850 spacer group Chemical group 0.000 description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 239000005083 Zinc sulfide Substances 0.000 description 2
- 229910021417 amorphous silicon Inorganic materials 0.000 description 2
- 238000013459 approach Methods 0.000 description 2
- ZUOUZKKEUPVFJK-UHFFFAOYSA-N diphenyl Chemical compound C1=CC=CC=C1C1=CC=CC=C1 ZUOUZKKEUPVFJK-UHFFFAOYSA-N 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 229910003437 indium oxide Inorganic materials 0.000 description 2
- PJXISJQVUVHSOJ-UHFFFAOYSA-N indium(iii) oxide Chemical compound [O-2].[O-2].[O-2].[In+3].[In+3] PJXISJQVUVHSOJ-UHFFFAOYSA-N 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 239000010445 mica Substances 0.000 description 2
- 229910052618 mica group Inorganic materials 0.000 description 2
- 239000010409 thin film Substances 0.000 description 2
- XOLBLPGZBRYERU-UHFFFAOYSA-N tin dioxide Chemical compound O=[Sn]=O XOLBLPGZBRYERU-UHFFFAOYSA-N 0.000 description 2
- 229910001887 tin oxide Inorganic materials 0.000 description 2
- 229910052984 zinc sulfide Inorganic materials 0.000 description 2
- YJTKZCDBKVTVBY-UHFFFAOYSA-N 1,3-Diphenylbenzene Chemical group C1=CC=CC=C1C1=CC=CC(C=2C=CC=CC=2)=C1 YJTKZCDBKVTVBY-UHFFFAOYSA-N 0.000 description 1
- RYHBNJHYFVUHQT-UHFFFAOYSA-N 1,4-Dioxane Chemical compound C1COCCO1 RYHBNJHYFVUHQT-UHFFFAOYSA-N 0.000 description 1
- XDTMQSROBMDMFD-UHFFFAOYSA-N Cyclohexane Chemical compound C1CCCCC1 XDTMQSROBMDMFD-UHFFFAOYSA-N 0.000 description 1
- PXGOKWXKJXAPGV-UHFFFAOYSA-N Fluorine Chemical compound FF PXGOKWXKJXAPGV-UHFFFAOYSA-N 0.000 description 1
- 239000004988 Nematic liquid crystal Substances 0.000 description 1
- 239000004952 Polyamide Substances 0.000 description 1
- 239000004642 Polyimide Substances 0.000 description 1
- CZPWVGJYEJSRLH-UHFFFAOYSA-N Pyrimidine Chemical compound C1=CN=CN=C1 CZPWVGJYEJSRLH-UHFFFAOYSA-N 0.000 description 1
- 229910004298 SiO 2 Inorganic materials 0.000 description 1
- BLRPTPMANUNPDV-UHFFFAOYSA-N Silane Chemical compound [SiH4] BLRPTPMANUNPDV-UHFFFAOYSA-N 0.000 description 1
- 229910006404 SnO 2 Inorganic materials 0.000 description 1
- 125000000751 azo group Chemical group [*]N=N[*] 0.000 description 1
- 125000005337 azoxy group Chemical group [N+]([O-])(=N*)* 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 235000010290 biphenyl Nutrition 0.000 description 1
- 239000004305 biphenyl Substances 0.000 description 1
- AQCDIIAORKRFCD-UHFFFAOYSA-N cadmium selenide Chemical compound [Cd]=[Se] AQCDIIAORKRFCD-UHFFFAOYSA-N 0.000 description 1
- 238000003776 cleavage reaction Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 239000003989 dielectric material Substances 0.000 description 1
- 238000005401 electroluminescence Methods 0.000 description 1
- 150000002148 esters Chemical class 0.000 description 1
- 230000005669 field effect Effects 0.000 description 1
- 229910052731 fluorine Inorganic materials 0.000 description 1
- 239000011737 fluorine Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 239000004615 ingredient Substances 0.000 description 1
- XCAUINMIESBTBL-UHFFFAOYSA-N lead(ii) sulfide Chemical compound [Pb]=S XCAUINMIESBTBL-UHFFFAOYSA-N 0.000 description 1
- ORUIBWPALBXDOA-UHFFFAOYSA-L magnesium fluoride Chemical compound [F-].[F-].[Mg+2] ORUIBWPALBXDOA-UHFFFAOYSA-L 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 229920002647 polyamide Polymers 0.000 description 1
- 229920001721 polyimide Polymers 0.000 description 1
- 229920006254 polymer film Polymers 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 230000007017 scission Effects 0.000 description 1
- 235000012239 silicon dioxide Nutrition 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
- LIVNPJMFVYWSIS-UHFFFAOYSA-N silicon monoxide Chemical compound [Si-]#[O+] LIVNPJMFVYWSIS-UHFFFAOYSA-N 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 229920002554 vinyl polymer Polymers 0.000 description 1
- DRDVZXDWVBGGMH-UHFFFAOYSA-N zinc;sulfide Chemical compound [S-2].[Zn+2] DRDVZXDWVBGGMH-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Liquid Crystal (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、投写型表示装置等に用
いられる電気光学特性の極めて優れた光変調素子に関す
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a light modulation element having extremely excellent electro-optical characteristics used in a projection type display device or the like.
【0002】[0002]
【従来の技術】表示装置には直視型の装置と投写型の装
置とがあり、投写型の装置としては液晶を使った光変調
素子を用いるものが既に実用化されている。図4は光変
調素子を用いた投写型表示装置の原理図である。図4に
おいて、光変調素子10には書込み光学系から発せられ
る書込み光11によって像が書込まれる。一方、光源1
3より発せられた光はコンデンサレンズ14により平行
光とされた後、偏光ビームスプリッタ15に入射し、そ
の入射光の内のS偏光成分は進行方向が接合面で反射し
直角に曲げられることにより、読出し光12として光変
調素子10に入射する。2. Description of the Related Art Display devices include a direct-view type device and a projection type device, and as the projection type device, a device using a light modulation element using liquid crystal has already been put into practical use. FIG. 4 is a principle diagram of a projection display device using a light modulation element. In FIG. 4, an image is written on the light modulation element 10 by the writing light 11 emitted from the writing optical system. On the other hand, light source 1
The light emitted from 3 is collimated by the condenser lens 14 and then incident on the polarization beam splitter 15. The S-polarized component of the incident light is reflected at the joint surface in the traveling direction and bent at a right angle. , And enters the light modulation element 10 as the reading light 12.
【0003】ここで、光変調素子10の液晶層に像が描
かれていると、光変調素子10で反射された反射光中に
は液晶層の像の濃淡に応じて変調を受け、P偏光成分が
含まれるようになる。この反射光中のP偏光成分は偏光
ビームスプリッタ15をそのまま通過し、投写レンズ1
6を介してスクリーン17上に像が投写される。従っ
て、光変調素子10に書込まれている像がスクリーン1
7へ投写されることになる。Here, when an image is drawn on the liquid crystal layer of the light modulation element 10, the reflected light reflected by the light modulation element 10 is modulated in accordance with the light and shade of the image of the liquid crystal layer, and P polarized light is obtained. Ingredients will be included. The P-polarized component in the reflected light passes through the polarization beam splitter 15 as it is, and the projection lens 1
An image is projected on the screen 17 via 6. Therefore, the image written on the light modulation element 10 is displayed on the screen 1
7 will be projected.
【0004】図5はこの投写型表示装置に用いられる従
来の光変調素子10の一例の構造を示す図である。図5
において、液晶層7の周りにはスペーサ8a,8bが配
され、液晶層7の両面には液晶配向層6a,6bが設け
られている。液晶配向層6bの外側には誘電体からなる
光反射層5が積層され、この光反射層5の外側には例え
ば非晶質水素化シリコン(a−Si:H)からなる光導
電層4が積層されている。そして、液晶配向層6a及び
光導電層4の外側には酸化スズ(SnO2 )や酸化イン
ジウム(In2 O3 )からなる透明電極3a,3bが配
され、透明基板2a,2bによって封止された構造とな
っている。FIG. 5 is a view showing the structure of an example of a conventional light modulation element 10 used in this projection type display device. Figure 5
In, the spacers 8a and 8b are arranged around the liquid crystal layer 7, and the liquid crystal alignment layers 6a and 6b are provided on both surfaces of the liquid crystal layer 7. A light reflecting layer 5 made of a dielectric material is laminated on the outer side of the liquid crystal alignment layer 6b, and a photoconductive layer 4 made of, for example, amorphous hydrogenated silicon (a-Si: H) is placed on the outer side of the light reflecting layer 5. It is stacked. Then, transparent electrodes 3a and 3b made of tin oxide (SnO 2 ) or indium oxide (In 2 O 3 ) are arranged outside the liquid crystal alignment layer 6a and the photoconductive layer 4 and sealed by the transparent substrates 2a and 2b. It has a different structure.
【0005】このような構造の光変調素子10におい
て、透明電極3a,3b間には交流駆動電圧が印加さ
れ、書込み側から書込み光11が照射されていない状態
での光導電層4の内部インピーダンスを液晶層7のそれ
よりも十分大きい値に設定しておくことにより、駆動電
圧は主に光導電層4に印加されることになる。そして、
書込み光11が照射され、その書込み光11によって光
導電層4上に像を描くときには、光導電層4の内部イン
ピーダンスが像の濃淡に応じて局部的に低下するため、
その低下部分に隣接する液晶層7には透明電極3a,3
b間の駆動電圧が像の濃淡に応じて空間変調されて印加
されるようになって像が書込まれることになる。In the light modulation element 10 having such a structure, an AC drive voltage is applied between the transparent electrodes 3a and 3b, and the internal impedance of the photoconductive layer 4 in a state where the writing light 11 is not irradiated from the writing side. Is set to a value sufficiently larger than that of the liquid crystal layer 7, the drive voltage is mainly applied to the photoconductive layer 4. And
When the writing light 11 is irradiated and an image is drawn on the photoconductive layer 4 by the writing light 11, the internal impedance of the photoconductive layer 4 locally decreases according to the shading of the image.
The transparent electrodes 3a, 3 are provided on the liquid crystal layer 7 adjacent to the lowered portion.
The drive voltage between points b is spatially modulated according to the density of the image and applied, and the image is written.
【0006】ここで、従来の光変調素子10に用いられ
る液晶層7の液晶分子の配列方向,読出し光の偏光方向
について、45度ツイスト配向の液晶層によるハイブリ
ッド電界効果モードを用いた光変調素子や、ECB(el
ectrically controlled birefringence )効果を利用し
て初期の液晶分子配向を垂直配向あるいは水平配向とし
た光変調素子が知られている。水平配向の液晶層7の液
晶分子はその分子長軸が基板2a,2bにわずかなプレ
ティルト角を有し、略平行になるよう配列している。さ
らに、液晶層7の液晶分子は液晶配向層6a,6b上で
それぞれが平行に配向されている。Here, with respect to the alignment direction of the liquid crystal molecules of the liquid crystal layer 7 used in the conventional light modulation element 10 and the polarization direction of the read-out light, the light modulation element using the hybrid field effect mode by the liquid crystal layer having the twist alignment of 45 degrees. Or ECB (el
An optical modulator is known in which the initial alignment of liquid crystal molecules is made vertical or horizontal by utilizing the effect of electrical controlled birefringence. The liquid crystal molecules of the horizontally aligned liquid crystal layer 7 are arranged so that their long axes have a slight pretilt angle on the substrates 2a and 2b and are substantially parallel to each other. Further, the liquid crystal molecules of the liquid crystal layer 7 are aligned in parallel on the liquid crystal alignment layers 6a and 6b.
【0007】このような水平配向の液晶層7を有する光
変調素子10を図4に示す投写型表示装置に用い、光変
調素子10と読出し光源13との間の偏光ビームスプリ
ッタ15の偏光軸を入射側の液晶層7の液晶分子軸と4
5度をなすように配置すると、直線偏光された入射光は
液晶層7を通過することにより生じる異常光と常光との
間のリタデーション(位相遅れ)Rならびに位相差δ
は、液晶分子の屈折率異方性をΔn、液晶層厚をd、入
射光の波長をλとすると、R=Δn・d、δ=2πR/
λで表され、光反射層5により反射して再び液晶層7を
通過する際に再びリタデーションRならびに位相差δを
生じる。偏光ビームスプリッタ15を透過する透過光強
度Jは、数1で表される。The light modulation element 10 having such a horizontally aligned liquid crystal layer 7 is used in the projection display device shown in FIG. 4, and the polarization axis of the polarization beam splitter 15 between the light modulation element 10 and the reading light source 13 is set. 4 and the liquid crystal molecular axis of the liquid crystal layer 7 on the incident side
When arranged so as to form 5 degrees, the linearly polarized incident light has a retardation (phase lag) R and a phase difference δ between the extraordinary light and the ordinary light generated by passing through the liquid crystal layer 7.
Where R = Δn · d and δ = 2πR /, where Δn is the refractive index anisotropy of the liquid crystal molecules, d is the liquid crystal layer thickness, and λ is the wavelength of the incident light.
It is represented by λ, and when it is reflected by the light reflection layer 5 and again passes through the liquid crystal layer 7, the retardation R and the phase difference δ are generated again. The transmitted light intensity J that passes through the polarization beam splitter 15 is represented by Formula 1.
【0008】[0008]
【数1】 [Equation 1]
【0009】これに対し、光変調素子10の透明電極3
a,3b間に電界を印加していくと、正の誘電率異方性
を持つ液晶分子は基板2a,2bに垂直に近づくような
傾斜した配列になる。このように、液晶分子は基板2
a,2bに対して分子軸方向が変化すると共に実効的な
屈折率異方性は変化するので、リタデーションRが変化
する。このことにより、電界によって液晶層7の複屈折
率が変化し、光のP偏光成分とS偏光成分との比を制御
できるので、電界の印加により偏光ビームスプリッタ1
5を透過する光の強度が変化し、スクリーン17上に像
が投写されることとなる。On the other hand, the transparent electrode 3 of the light modulation element 10
When an electric field is applied between a and 3b, the liquid crystal molecules having a positive dielectric anisotropy are in a tilted array so as to approach the substrates 2a and 2b in a direction perpendicular to them. In this way, the liquid crystal molecules are
Since the effective refractive index anisotropy changes as the molecular axis direction changes with respect to a and 2b, the retardation R changes. As a result, the birefringence of the liquid crystal layer 7 is changed by the electric field, and the ratio of the P-polarized component and the S-polarized component of light can be controlled.
The intensity of the light passing through 5 changes and an image is projected on the screen 17.
【0010】上述した従来の光変調素子10の一例の条
件を表1に示す。Table 1 shows conditions of an example of the above-described conventional light modulation element 10.
【表1】 [Table 1]
【0011】表1に示す条件の従来の光変調素子10に
電界を印加した際の光学特性を図6に、電界を印加しな
いときの波長依存性を図7に示す。図6において、横軸
は印加電圧、縦軸は入射光量(図4中の偏光ビームスプ
リッタ15に入射する光)と出射光量(図4中の偏光ビ
ームスプリッタ15を出射する光)との比である出射光
量/入射光量を、図7において、横軸は波長、縦軸は出
射光量/入射光量を示している。この図6に示す例で
は、下に凸となった部分の前半部分(フロントスロー
プ)における相対光透過率が99%及び1%に対応する
印加電圧V99(=1.18)及びV1 (=1.79)の
範囲で動作させる。なお、この場合、電界を印加しない
ときは白であり、いわゆるノーマリーホワイトモードで
ある。FIG. 6 shows the optical characteristics when an electric field is applied to the conventional optical modulator 10 under the conditions shown in Table 1, and FIG. 7 shows the wavelength dependence when no electric field is applied. In FIG. 6, the horizontal axis is the applied voltage, and the vertical axis is the ratio of the incident light amount (light incident on the polarization beam splitter 15 in FIG. 4) to the emission light amount (light emitted from the polarization beam splitter 15 in FIG. 4). In FIG. 7, the horizontal axis indicates the wavelength, and the vertical axis indicates the output light amount / the input light amount. In the example shown in FIG. 6, applied voltages V99 (= 1.18) and V1 (= 1) corresponding to relative light transmittances of 99% and 1% in the first half (front slope) of the downwardly convex portion. .79). In this case, when no electric field is applied, it is white, which is a so-called normally white mode.
【0012】さらにまた、図6には示していないが、透
過光強度Jが最大となる特異点を使うと、その電圧以上
では印加電圧の大きさに従って透過光強度Jを小さくす
ることができる。このように、上に凸となった部分の後
半部分(バックスロープ)を用い、ノーマリーホワイト
モードとして動作させる方法については、米国特許第4
378955号明細書に開示されている。これによれ
ば、電界を印加しないときに透過光強度Jが最大となる
条件のみならず、ある電圧で透過光強度Jが最大となる
特異点を使うこともできるので、数多くの条件が使用可
能である。Further, although not shown in FIG. 6, by using a singular point at which the transmitted light intensity J becomes maximum, the transmitted light intensity J can be reduced according to the magnitude of the applied voltage above the voltage. As described above, a method of operating in the normally white mode by using the latter half portion (back slope) of the convex portion is described in US Pat.
No. 378,955. According to this, not only the condition that the transmitted light intensity J becomes maximum when the electric field is not applied but also the singular point where the transmitted light intensity J becomes maximum at a certain voltage can be used, so that many conditions can be used. Is.
【0013】[0013]
【発明が解決しようとする課題】前述のように、光変調
素子10に電界を印加すると、液晶層7の液晶分子は基
板2a,2bとのなす角を増大してある傾斜に達する
が、相対光透過率が99%及び1%に対応する印加電圧
V99及びV1 を用いて閾(しきい)値特性の鋭さγは、
γ=V1 /V99のように定義して使用される。図6に示
すように、V1 =1.79、V99=1.18より、γ=
1.52程度であり、入射される書込み光11による光
導電層4の内部インピーダンスの変化量が小さいと、印
加電圧の変化量も小さいために、コントラスト比を大き
くできないという問題点があった。また、図7に示すよ
うに、波長依存性が大きく、ある程度の波長範囲を有す
る光を変調する場合に、波長による光透過率の差が生
じ、色相の変化をもたらすという問題点もあった。As described above, when an electric field is applied to the light modulation element 10, the liquid crystal molecules of the liquid crystal layer 7 increase the angle formed with the substrates 2a and 2b and reach a certain inclination, but Using the applied voltages V99 and V1 corresponding to the light transmittances of 99% and 1%, the sharpness γ of the threshold value characteristic is
It is used by defining it as γ = V1 / V99. As shown in FIG. 6, from V1 = 1.79 and V99 = 1.18, γ =
If the amount of change in the internal impedance of the photoconductive layer 4 due to the incident writing light 11 is small, the amount of change in applied voltage is also small, so that the contrast ratio cannot be increased. Further, as shown in FIG. 7, when light having a large wavelength dependency and a certain wavelength range is modulated, there is a problem that a difference in light transmittance occurs depending on the wavelength, which causes a change in hue.
【0014】さらに、ノーマリーホワイトモードでは例
えば陰極線管のようなパルス光による書込みをすると、
書込み光の照射されない時間には透過光強度Jが増大
し、いわゆる黒浮きの現象が起こり、コントラスト比を
低下させるという問題点もあった。そこで本発明はこの
ような問題点に鑑み、従来の光変調素子とは異なった素
子構成をとることによって閾値特性が鋭く、波長依存性
の小さな極めて優れた電気光学特性を有し、ノーマリー
ホワイトモードとノーマリーブラックモードとの反転が
可能な光変調素子を提供することを目的とする。Further, in the normally white mode, when writing is performed by pulsed light such as a cathode ray tube,
There is also a problem that the transmitted light intensity J increases during the time when the writing light is not irradiated, so-called black floating phenomenon occurs, and the contrast ratio is lowered. Therefore, in view of such a problem, the present invention has a sharp threshold value characteristic by taking an element configuration different from that of the conventional light modulation element, and has extremely excellent electro-optical characteristics with small wavelength dependence, and is normally white. It is an object of the present invention to provide an optical modulator capable of reversing a mode and a normally black mode.
【0015】[0015]
【課題を解決するための手段】本発明は、上述した従来
の技術の課題を解決するため、液晶分子の配向状態を書
込み光によって遷移させることにより画像を書込み、こ
の書込まれた画像を読出し光により投写させる光変調素
子において、第1の透明基板上に第1の透明電極と第1
の液晶配向層とを順次積層し、第2の透明基板上に第2
の透明電極と光導電層と光反射層と第2の液晶配向層と
を順次積層し、前記第1及び第2の液晶配向層間に液晶
層を挟装させると共にこの液晶層の液晶分子を一様に初
期配列させ、前記第1の透明基板の外側に位相板を設け
たことを特徴とする光変調素子を提供するものである。In order to solve the above-mentioned problems of the prior art, the present invention writes an image by transitioning the alignment state of liquid crystal molecules by writing light, and reads the written image. In a light modulation element for projecting with light, a first transparent electrode and a first transparent electrode are provided on a first transparent substrate.
And a liquid crystal alignment layer are sequentially laminated to form a second transparent substrate on the second transparent substrate.
Of the transparent electrode, the photoconductive layer, the light reflecting layer, and the second liquid crystal alignment layer are sequentially laminated, and the liquid crystal layer is sandwiched between the first and second liquid crystal alignment layers, and the liquid crystal molecules of the liquid crystal layer are As described above, the present invention provides an optical modulation element characterized in that a phase plate is provided outside the first transparent substrate in the initial arrangement.
【0016】[0016]
【実施例】以下、本発明の光変調素子について、添付図
面を参照して説明する。図1は本発明の光変調素子の一
実施例の構造を示す図、図2は本発明の光変調素子にお
ける印加電圧と出射光量/入射光量との関係を示す図、
図3は本発明の光変調素子における波長と出射光量/入
射光量との関係を示す図である。なお、図1において、
図5と同一部分には同一符号が付してある。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The light modulator of the present invention will be described below with reference to the accompanying drawings. FIG. 1 is a diagram showing the structure of an embodiment of the light modulation element of the present invention, and FIG. 2 is a diagram showing the relationship between the applied voltage and the emitted light quantity / incident light quantity in the light modulation element of the present invention,
FIG. 3 is a diagram showing the relationship between the wavelength and the emitted light amount / incident light amount in the light modulation element of the present invention. In addition, in FIG.
The same parts as those in FIG. 5 are designated by the same reference numerals.
【0017】本発明の光変調素子1は従来の光変調素子
10と構造が異なり、基板2aの外側、読出し光12の
入射側に位相板9を備えている。本発明の光変調素子1
は、図1に示すように、透明な基板2a,2bが略均等
な間隔で平行に対向しており、この基板2aの基板2b
に対向する側には透明電極3aが、基板2bの基板2a
に対向する側には透明電極3bが設けられている。そし
て、この透明電極3b上には、書込み光11の光強度で
比抵抗が変化する光導電層4が積層形成され、さらに、
光導電層4上には光反射層5が積層形成されている。ま
た、透明電極3a上には液晶配向層6aが、光反射層5
上には液晶配向層6bが積層して設けられている。この
ように、基板2aには透明電極3a,液晶分子配向層6
aが積層して設けられ、基板2bには透明電極3b,光
導電層4,光反射層5,液晶配向層6bが積層して設け
られ、これら基板2a,2bの間には液晶層7が挟装さ
れている。なお、8a及び8bは上記と同様、基板2
a,2bの間に所定間隔を保って液晶を封入させるため
のスペーサである。さらに、基板2aの外側、読出し光
12の入射側に位相板9が積層して、あるいは間隙を有
して設けられている。The optical modulator 1 of the present invention has a structure different from that of the conventional optical modulator 10, and is provided with a phase plate 9 outside the substrate 2a and on the incident side of the readout light 12. Light modulation element 1 of the present invention
As shown in FIG. 1, transparent substrates 2a and 2b face each other in parallel at substantially equal intervals.
The transparent electrode 3a on the side facing the substrate 2a of the substrate 2b.
A transparent electrode 3b is provided on the side opposite to. Then, on the transparent electrode 3b, a photoconductive layer 4 whose specific resistance changes according to the light intensity of the writing light 11 is laminated and further formed.
A light reflection layer 5 is laminated on the photoconductive layer 4. Further, the liquid crystal alignment layer 6a is provided on the transparent electrode 3a, and the light reflection layer 5 is formed on the transparent electrode 3a.
A liquid crystal alignment layer 6b is provided on top of it. Thus, the transparent electrode 3a and the liquid crystal molecule alignment layer 6 are formed on the substrate 2a.
a is laminated and a transparent electrode 3b, a photoconductive layer 4, a light reflection layer 5 and a liquid crystal alignment layer 6b are laminated on the substrate 2b. A liquid crystal layer 7 is provided between the substrates 2a and 2b. It is sandwiched. In addition, 8a and 8b are the same as the above
It is a spacer for enclosing a liquid crystal with a predetermined space between a and 2b. Further, the phase plate 9 is laminated on the outside of the substrate 2a or on the incident side of the readout light 12 or provided with a gap.
【0018】ここで、基板2a,2bは本実施例では例
えば透明なガラス板を用いているが、透明な樹脂板を用
いることもできる。また、透明電極3a,3bは、一般
に酸化インジウム膜または酸化スズ膜等で形成する。透
明電極3b上に形成される光導電層4は、非晶質水素化
シリコン,セレン化カドミウム(CdSe),硫化鉛
(PbS)等の各種の光導電物質を単独に、または複合
化して用いることができる。光導電層4上に積層される
光反射層5は硫化亜鉛(ZnS):フッ化マグネシウム
(MgF2 )多層膜,酸化ケイ素(SiO):二酸化ケ
イ素(SiO2 )多層膜等の誘電体多層膜を用いる。Here, although the substrates 2a and 2b are made of, for example, transparent glass plates in this embodiment, transparent resin plates can also be used. The transparent electrodes 3a and 3b are generally formed of an indium oxide film, a tin oxide film, or the like. For the photoconductive layer 4 formed on the transparent electrode 3b, various photoconductive materials such as amorphous silicon hydride, cadmium selenide (CdSe), and lead sulfide (PbS) are used alone or in combination. You can The light reflection layer 5 laminated on the photoconductive layer 4 is a dielectric multilayer film such as a zinc sulfide (ZnS): magnesium fluoride (MgF 2 ) multilayer film or a silicon oxide (SiO): silicon dioxide (SiO 2 ) multilayer film. To use.
【0019】さらに、液晶配向層6a,6bは、これま
でに知られている液晶表示素子の液晶配向層を用いるこ
とができ、どのような液晶分子をどのように配列させる
かにより適宜選択して用いればよく、本実施例では液晶
分子が水平配列になるポリイミド,ポリアミドやポリビ
ニル等の高分子膜を用いて形成している。液晶層7の液
晶材料は、正の誘電率異方性を有するネマティック液晶
を用いる。これは、フッソ系,シッフ系,アゾ系,アゾ
キシ系,エステル系,ビフェニル系,ターフェニル系,
シクロヘキサン系,ピリミジン系,ジオキサン系等の各
種の液晶物質を単独に、または混合して用いることがで
きる。Further, as the liquid crystal alignment layers 6a and 6b, the liquid crystal alignment layers of the liquid crystal display elements known so far can be used, and the liquid crystal alignment layers are appropriately selected depending on what kind of liquid crystal molecules are arranged and how. It may be used, and in this embodiment, it is formed by using a polymer film such as polyimide, polyamide or polyvinyl in which liquid crystal molecules are horizontally aligned. As the liquid crystal material of the liquid crystal layer 7, nematic liquid crystal having positive dielectric anisotropy is used. This is fluorine, Schiff, azo, azoxy, ester, biphenyl, terphenyl,
Various liquid crystal substances such as cyclohexane type, pyrimidine type and dioxane type can be used alone or in combination.
【0020】また、基板2aの外側に積層して、あるい
は間隙を有して設けられた位相板9は、その回転角が読
出し光12が入射する基板2a側の液晶分子配向層6a
上の液晶分子の軸方向に対して90度程度をなすように
なされている。この位相板9には、例えばπ/2,πの
位相差を与える波長板を用いることができ、本実施例で
はπ/2の位相差を与えるλ/4板(1/4波長板)を
用いている。λ/4板は例えば雲母を所望の位相差に相
当する厚さに劈開(へき開)すればよく、雲母はα軸が
劈開面にほぼ直角なので偏光方向はβ軸,γ軸であり、
屈折率はそれぞれ1.590,1.594であるので、
厚さは36μmにする。Further, the phase plate 9 laminated on the outside of the substrate 2a or provided with a gap has a rotation angle of the liquid crystal molecule alignment layer 6a on the substrate 2a side on which the reading light 12 is incident.
The angle is about 90 degrees with respect to the axial direction of the upper liquid crystal molecules. As the phase plate 9, for example, a wave plate that gives a phase difference of π / 2 or π can be used. In this embodiment, a λ / 4 plate (1/4 wave plate) that gives a phase difference of π / 2 is used. I am using. For the λ / 4 plate, for example, the mica may be cleaved (cleaved) to a thickness corresponding to a desired phase difference. Since the α axis of the mica is almost perpendicular to the cleavage plane, the polarization directions are β axis and γ axis,
Since the refractive indexes are 1.590 and 1.594, respectively,
The thickness is 36 μm.
【0021】このような位相板9を備えた本発明の光変
調素子1は、図4に示すような投写型表示装置の画像作
成要素として利用される。この投写型表示装置において
は、例えばCRT画面から発せられる光を書込み光11
として光変調素子1に入射し画像を書き込む。一方、光
源13より発せられた光はコンデンサレンズ14により
平行光とされた後、偏光ビームスプリッタ15を介して
光変調素子1に照射される。光変調素子1の光反射層5
で反射される空間変調された光は偏光ビームスプリッタ
15を透過し、投写レンズ16を介してスクリーン17
上に結像する。The light modulation element 1 of the present invention provided with such a phase plate 9 is used as an image forming element of a projection type display device as shown in FIG. In this projection display device, for example, the light emitted from the CRT screen is used as the writing light 11
Then, the light enters the light modulation element 1 to write an image. On the other hand, the light emitted from the light source 13 is collimated by the condenser lens 14, and then is irradiated onto the light modulation element 1 via the polarization beam splitter 15. Light reflection layer 5 of light modulation element 1
The spatially-modulated light reflected by is transmitted through the polarization beam splitter 15 and passes through the projection lens 16 and the screen 17
Image on top.
【0022】ここで、光変調素子1と読出し光源13と
の間の偏光ビームスプリッタ15の偏光軸を位相板9の
回転角と45度になるように配置すると、偏光ビームス
プリッタ15で直線偏光された入射光は、位相板9を通
過することにより円偏光に変換され、入射光は液晶層7
を通過し、光反射層5により反射して再び液晶層7を通
過した後、円偏光は位相板9を再び通過することにより
直線偏光に変換され、偏光ビームスプリッタ15で透過
光強度Jが最低になるようになされている。Here, when the polarization axis of the polarization beam splitter 15 between the light modulation element 1 and the reading light source 13 is arranged to be 45 degrees with the rotation angle of the phase plate 9, linear polarization is performed by the polarization beam splitter 15. The incident light is converted into circularly polarized light by passing through the phase plate 9, and the incident light is converted into the liquid crystal layer 7.
After being transmitted through the liquid crystal layer 7, the circularly polarized light is converted into linearly polarized light by passing through the phase plate 9 again, and the transmitted light intensity J is minimum by the polarization beam splitter 15. It is designed to be.
【0023】さらに、本発明の光変調素子1の動作につ
いて説明する。図1において、透明電極3a,3b間に
は図示せぬ外部電源が接続され、最適に設定された交流
駆動電圧が印加される。ここで、書込み側から書込み光
11が照射されていない状態での光導電層4の内部イン
ピーダンスは液晶層7のそれよりも十分大きい値に設定
してあるので、駆動電圧は主に光導電層4に印加される
ことになる。そして、書込み光11が照射され、その書
込み光11によって光導電層4上に像を描くときには、
光導電層4の内部インピーダンスが像の濃淡に応じて局
部的に低下するため、その低下部分に隣接する液晶層7
には透明電極3a,3b間の駆動電圧が像の濃淡に応じ
て空間変調されて印加され、液晶層7における印加され
る電圧が増大した部分の液晶分子は配列状態を変える。Further, the operation of the light modulation element 1 of the present invention will be described. In FIG. 1, an external power supply (not shown) is connected between the transparent electrodes 3a and 3b, and an optimally set AC drive voltage is applied. Here, since the internal impedance of the photoconductive layer 4 in the state where the writing light 11 is not irradiated from the writing side is set to a value sufficiently higher than that of the liquid crystal layer 7, the driving voltage is mainly the photoconductive layer. 4 will be applied. Then, when the writing light 11 is irradiated and an image is drawn on the photoconductive layer 4 by the writing light 11,
Since the internal impedance of the photoconductive layer 4 is locally reduced according to the contrast of the image, the liquid crystal layer 7 adjacent to the lowered portion.
The drive voltage between the transparent electrodes 3a and 3b is spatially modulated and applied according to the contrast of the image, and the liquid crystal molecules in the portion of the liquid crystal layer 7 where the applied voltage is increased change the alignment state.
【0024】印加される電圧が増大すると、正の誘電率
異方性を有する液晶分子の長軸方向は、基板2a,2b
に垂直に近付くような傾斜した配列となる。このような
状態での光変調素子1は、液晶分子の軸方向が変化する
と共に実効的な屈折率異方性は変化するので複屈折率は
変化し、光反射層5で反射して再び液晶層7を透過した
後に出射する光は、円偏光や楕円偏光に変換され、位相
板9を再び通過すると、楕円偏光の主軸の振動方向と位
相板9との回転角が一致する成分のみ直線偏光になり、
偏光ビームスプリッタ15を透過する光が得られるよう
になる。When the applied voltage is increased, the long axis direction of the liquid crystal molecules having positive dielectric anisotropy is changed to the substrates 2a, 2b.
It becomes a slanted array that approaches vertically to. In the light modulation element 1 in such a state, since the effective refractive index anisotropy changes as the axial direction of the liquid crystal molecules changes, the birefringence changes and the light is reflected by the light reflection layer 5 and again the liquid crystal. The light emitted after passing through the layer 7 is converted into circularly polarized light or elliptically polarized light, and when passing through the phase plate 9 again, only the component in which the vibration direction of the principal axis of the elliptically polarized light and the rotation angle of the phase plate 9 are linearly polarized light. become,
The light transmitted through the polarization beam splitter 15 can be obtained.
【0025】そして、この光変調素子1は、入射される
書込み光11による光導電層4の内部インピーダンスの
変化に対応して液晶層7の液晶分子の配列状態が可逆的
に遷移することを利用しているため、書込み光11が照
射されなくなれば自動的に初期の配向状態に戻ることか
ら、蓄積された像は時間遅れを伴って消去される。The light modulation element 1 utilizes that the arrangement state of the liquid crystal molecules of the liquid crystal layer 7 reversibly transits in response to the change of the internal impedance of the photoconductive layer 4 due to the incident writing light 11. Therefore, when the writing light 11 is no longer irradiated, the initial alignment state is automatically restored, and the stored image is erased with a time delay.
【0026】表1には従来の光変調素子10の一例の条
件と併せて、本発明の光変調素子1の一例の条件を示し
ている。そして、表1に示す条件の本発明の光変調素子
1に電界を印加した際の光学特性を図2に、電界を印加
しないときの波長依存性を図3に示す。図2は図6と同
様、横軸は印加電圧、縦軸は縦軸は出射光量/入射光量
であり、図3は図7と同様、横軸は波長、縦軸は出射光
量/入射光量である。この図2より、相対光透過率が1
%及び99%に対応する印加電圧V99及びV1を用いた
閾値特性の鋭さγは、V1 =1.18、V99=1.71
より、γ=1.45程度(この場合、γ=V99/V1 )
であり、本発明の光変調素子1は著しく急峻な閾値特性
を有していることが分かる。さらに、図3に示すよう
に、波長による光透過率の差は小さく、本発明の光変調
素子1は波長依存性が小さい特性を有していることが分
かる。Table 1 shows the conditions of an example of the light modulation element 1 of the present invention together with the conditions of the example of the conventional light modulation element 10. 2 shows the optical characteristics when an electric field is applied to the optical modulator 1 of the present invention under the conditions shown in Table 1, and FIG. 3 shows the wavelength dependence when no electric field is applied. In FIG. 2, as in FIG. 6, the horizontal axis represents applied voltage, the vertical axis represents emission light amount / incident light amount, and in FIG. 3, as in FIG. 7, the horizontal axis represents wavelength and the vertical axis represents emission light amount / incident light amount. is there. From FIG. 2, the relative light transmittance is 1
% And 99%, the sharpness γ of the threshold characteristic using the applied voltages V99 and V1 is V1 = 1.18, V99 = 1.71.
Therefore, γ = 1.45 (in this case, γ = V99 / V1)
Therefore, it can be seen that the light modulation element 1 of the present invention has a remarkably steep threshold characteristic. Furthermore, as shown in FIG. 3, it can be seen that the difference in the light transmittance depending on the wavelength is small, and the light modulation element 1 of the present invention has a characteristic that the wavelength dependence is small.
【0027】そして、本発明の光変調素子1は位相板9
を備えていることにより、ノーマリーホワイトモードと
ノーマリーブラックモードとの反転が実現される。この
ように、ノーマリーホワイトモードをノーマリーブラッ
クモードに反転することにより、黒表示時に透過光強度
Jが増大することはなく、例えば書込み光源に薄膜トラ
ンジスタ(TFT)駆動の液晶パネル等で変調した光が
用いられるのは勿論のこと、特に書込み光源がCRT,
EL(エレクトロルミネセンス素子),LED(発光ダ
イオード),LD(レーザーダイオード)等のパルス光
による書込み光に対して有効である。The optical modulator 1 of the present invention is provided with a phase plate 9
With the provision of, the inversion of the normally white mode and the normally black mode is realized. In this way, by inverting the normally white mode to the normally black mode, the transmitted light intensity J does not increase during black display, and for example, light modulated by a thin film transistor (TFT) driven liquid crystal panel or the like is used as a writing light source. Of course, the writing light source is a CRT,
This is effective for writing light by pulsed light such as EL (electroluminescence element), LED (light emitting diode), and LD (laser diode).
【0028】以上説明した本実施例では、位相板9を備
えることによって、ノーマリーホワイトモードをノーマ
リーブラックモードに反転する場合について述べたが、
これとは逆にノーマリーブラックモードをノーマリーホ
ワイトモードに反転することも同様の手段で実現でき
る。ノーマリーホワイトモードに反転すれば、例えば書
込み光に薄膜トランジスタ駆動の液晶パネル等で変調し
た光を用いる場合、液晶パネルは入力する信号に逆信号
を用いることで容易に白黒反転されて使用される。この
ような一定期間書込み光を保持できる書込み光源に対し
て有効に使用することができ、これによれば読出し光の
波長に依存する光の漏れが少ない黒表示が実現でき、黒
純度を上げることを可能にする。さらに、液晶層7にお
ける初期の液晶分子配向を液晶層7の厚さ方向に水平配
向として説明したが、これに限定されるものではなく、
垂直配向,傾斜配向,ツイスト角を有する配向であって
も全く同じ効果が得られることは勿論であり、本発明の
思想をいささかも変更するものではない。このように、
本発明の光変調素子1は本発明の要旨を逸脱しない範囲
において実施態様を種々適宜に変更可能である。In this embodiment described above, the case where the normally white mode is inverted to the normally black mode by providing the phase plate 9 has been described.
On the contrary, reversing the normally black mode to the normally white mode can be realized by the same means. Inverting to the normally white mode, for example, when the light modulated by a liquid crystal panel driven by a thin film transistor is used as the writing light, the liquid crystal panel is easily inverted in black and white by using a reverse signal as an input signal. It can be effectively used for such a writing light source that can hold writing light for a certain period of time, and this makes it possible to realize black display with less light leakage depending on the wavelength of the reading light and to improve black purity. To enable. Furthermore, although the initial liquid crystal molecule alignment in the liquid crystal layer 7 is described as horizontal alignment in the thickness direction of the liquid crystal layer 7, the present invention is not limited to this.
Of course, the same effect can be obtained even in the vertical alignment, the tilted alignment, and the alignment having the twist angle, and the idea of the present invention is not changed at all. in this way,
The embodiment of the light modulation element 1 of the present invention can be changed in various ways without departing from the scope of the present invention.
【0029】[0029]
【発明の効果】以上詳細に説明したように、本発明の光
変調素子は、第1の透明基板上に第1の透明電極と第1
の液晶配向層とを順次積層し、第2の透明基板上に第2
の透明電極と光導電層と光反射層と第2の液晶配向層と
を順次積層し、前記第1及び第2の液晶配向層間に液晶
層を挟装させると共にこの液晶層の液晶分子を一様に初
期配列させ、前記第1の透明基板の外側に位相板を設け
て構成したので、極めて優れた閾値特性を有し、これに
より光導電層の内部インピーダンスの変化量が小さくて
もよいので、光導電層の形成が容易になり、かつ、コン
トラスト比の大きい表示が可能となる。また、波長依存
性を小さくできるので、波長による光透過率の差による
表示色の色相の変化が小さい安定な表示が可能になる。
さらに、ノーマリーホワイトモードとノーマリーブラッ
クモードとの反転ができるので、書込み光の特性に応じ
て有効なモードの選択が可能になる等の特長を有する。As described in detail above, the light modulation element of the present invention includes the first transparent electrode and the first transparent electrode on the first transparent substrate.
And a liquid crystal alignment layer are sequentially laminated to form a second transparent substrate on the second transparent substrate.
Of the transparent electrode, the photoconductive layer, the light reflecting layer, and the second liquid crystal alignment layer are sequentially laminated, and the liquid crystal layer is sandwiched between the first and second liquid crystal alignment layers, and the liquid crystal molecules of the liquid crystal layer are As described above, since the initial arrangement is performed and the phase plate is provided outside the first transparent substrate, it has an extremely excellent threshold characteristic, and thus the change amount of the internal impedance of the photoconductive layer may be small. The formation of the photoconductive layer is facilitated, and display with a large contrast ratio is possible. In addition, since the wavelength dependence can be reduced, stable display can be achieved in which the hue change of the display color due to the difference in light transmittance depending on the wavelength is small.
Further, since the normally white mode and the normally black mode can be reversed, it is possible to select an effective mode according to the characteristics of the writing light.
【図1】本発明の光変調素子の一実施例の構造を示す図
である。FIG. 1 is a diagram showing a structure of an embodiment of a light modulation element of the present invention.
【図2】本発明の光変調素子における印加電圧と出射光
量/入射光量との関係を示す図である。FIG. 2 is a diagram showing a relationship between an applied voltage and an amount of emitted light / amount of incident light in the light modulation element of the present invention.
【図3】本発明の光変調素子における波長と出射光量/
入射光量との関係を示す図である。FIG. 3 shows the wavelength and the amount of emitted light in the optical modulator of the present invention.
It is a figure which shows the relationship with the amount of incident light.
【図4】光変調素子を用いた投写型表示装置の原理図で
ある。FIG. 4 is a principle view of a projection display device using a light modulation element.
【図5】従来の光変調素子の一例の構造を示す図であ
る。FIG. 5 is a diagram showing a structure of an example of a conventional light modulation element.
【図6】従来の光変調素子における印加電圧と出射光量
/入射光量との関係を示す図である。FIG. 6 is a diagram showing the relationship between the applied voltage and the amount of emitted light / the amount of incident light in a conventional light modulator.
【図7】従来の光変調素子における波長と出射光量/入
射光量との関係を示す図である。FIG. 7 is a diagram showing a relationship between a wavelength and an amount of emitted light / an amount of incident light in a conventional light modulator.
1,10 光変調素子 2a,2b 基板 3a,3b 透明電極 4 光導電層 5 光反射層 6a,6b 液晶配向層 7 液晶層 8a,8b スペーサ 9 位相板 1, 10 Light modulation element 2a, 2b Substrate 3a, 3b Transparent electrode 4 Photoconductive layer 5 Light reflection layer 6a, 6b Liquid crystal alignment layer 7 Liquid crystal layer 8a, 8b Spacer 9 Phase plate
Claims (2)
移させることにより画像を書込み、この書込まれた画像
を読出し光により投写させる光変調素子において、 第1の透明基板上に第1の透明電極と第1の液晶配向層
とを順次積層し、 第2の透明基板上に第2の透明電極と光導電層と光反射
層と第2の液晶配向層とを順次積層し、 前記第1及び第2の液晶配向層間に液晶層を挟装させる
と共にこの液晶層の液晶分子を一様に初期配列させ、 前記第1の透明基板の外側に位相板を設けたことを特徴
とする光変調素子。1. A light modulation element in which an image is written by causing the alignment state of liquid crystal molecules to transition by writing light and the written image is projected by reading light. An electrode and a first liquid crystal alignment layer are sequentially laminated, and a second transparent electrode, a photoconductive layer, a light reflection layer, and a second liquid crystal alignment layer are sequentially laminated on a second transparent substrate, And a liquid crystal layer sandwiched between the second liquid crystal alignment layers, the liquid crystal molecules of the liquid crystal layer are initially aligned uniformly, and a phase plate is provided outside the first transparent substrate. element.
/4波長板であることを特徴とする請求項1記載の光変
調素子。2. The phase plate provides a phase difference of π / 2.
The light modulation element according to claim 1, which is a quarter-wave plate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3270993A JP2828156B2 (en) | 1993-01-28 | 1993-01-28 | Light modulation element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3270993A JP2828156B2 (en) | 1993-01-28 | 1993-01-28 | Light modulation element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH06230408A true JPH06230408A (en) | 1994-08-19 |
| JP2828156B2 JP2828156B2 (en) | 1998-11-25 |
Family
ID=12366374
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3270993A Expired - Fee Related JP2828156B2 (en) | 1993-01-28 | 1993-01-28 | Light modulation element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2828156B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US12429733B2 (en) | 2020-07-24 | 2025-09-30 | Lg Chem, Ltd. | Light modulating device |
-
1993
- 1993-01-28 JP JP3270993A patent/JP2828156B2/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US12429733B2 (en) | 2020-07-24 | 2025-09-30 | Lg Chem, Ltd. | Light modulating device |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2828156B2 (en) | 1998-11-25 |
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