JPS59228633A - Optical modulating element - Google Patents
Optical modulating elementInfo
- Publication number
- JPS59228633A JPS59228633A JP10373083A JP10373083A JPS59228633A JP S59228633 A JPS59228633 A JP S59228633A JP 10373083 A JP10373083 A JP 10373083A JP 10373083 A JP10373083 A JP 10373083A JP S59228633 A JPS59228633 A JP S59228633A
- Authority
- JP
- Japan
- Prior art keywords
- light
- light modulation
- switch
- inputted
- parallel
- 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
Classifications
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06K—GRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
- G06K15/00—Arrangements for producing a permanent visual presentation of the output data, e.g. computer output printers
- G06K15/02—Arrangements for producing a permanent visual presentation of the output data, e.g. computer output printers using printers
- G06K15/12—Arrangements for producing a permanent visual presentation of the output data, e.g. computer output printers using printers by photographic printing, e.g. by laser printers
- G06K15/1238—Arrangements for producing a permanent visual presentation of the output data, e.g. computer output printers using printers by photographic printing, e.g. by laser printers simultaneously exposing more than one point
- G06K15/1257—Arrangements for producing a permanent visual presentation of the output data, e.g. computer output printers using printers by photographic printing, e.g. by laser printers simultaneously exposing more than one point on more than one main scanning line
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/0147—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on thermo-optic effects
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06K—GRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
- G06K15/00—Arrangements for producing a permanent visual presentation of the output data, e.g. computer output printers
- G06K15/02—Arrangements for producing a permanent visual presentation of the output data, e.g. computer output printers using printers
- G06K15/12—Arrangements for producing a permanent visual presentation of the output data, e.g. computer output printers using printers by photographic printing, e.g. by laser printers
- G06K15/129—Colour printing
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Optics & Photonics (AREA)
- General Physics & Mathematics (AREA)
- General Engineering & Computer Science (AREA)
- Theoretical Computer Science (AREA)
- Nonlinear Science (AREA)
- Electrochromic Elements, Electrophoresis, Or Variable Reflection Or Absorption Elements (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は、表示装置、記録装置、スイッチング装置等に
利用可能な光変調素子に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a light modulation element that can be used in display devices, recording devices, switching devices, and the like.
従来の電気光学効果あるいは音響光学効果を利用した光
変調素子は光学結晶を使用したものが多く、それ等に入
力した電気信号に対する元の変調の応答速度は速く、減
衰時間に関しても短かい。Conventional light modulation elements that utilize the electro-optic effect or the acousto-optic effect often use optical crystals, and the response speed of the original modulation to the electrical signal input thereto is fast and the decay time is short.
例えば電気光学効果、あるいは音響光学効果を利用した
光変調素子の減衰時間は1μsec以下のものが多い。For example, the decay time of a light modulation element using an electro-optic effect or an acousto-optic effect is often 1 μsec or less.
従って、電気光学効果や音響光学効果を利用した光変調
素子は、フライングスポットスキャン型の変調素子とし
ては高速応答性の利点を発揮できるが、例えば米国特許
第4,281,904 号に示される様にシャッターア
レーとして使用する場合には、上述した如く素子として
応答が高速である為に、入射光束を変調することが出来
る時間が短かく、従って充分な光量を得る為には光源に
高輝度のものを使用しなければならない。又、光源の輝
度をそれ程高く出来ない場合に線、光変調素子を駆動す
る為の入力信号の幅を長くして入力時間を長くする必要
がある。Therefore, an optical modulation element that utilizes the electro-optic effect or acousto-optic effect can exhibit the advantage of high-speed response as a flying spot scan type modulation element. When used as a shutter array, as mentioned above, since the element has a fast response, the time during which the incident light beam can be modulated is short, so in order to obtain a sufficient amount of light, a high-intensity light source is required. have to use something. Furthermore, if the brightness of the light source cannot be made that high, it is necessary to increase the input time by increasing the width of the input signal for driving the line and light modulation elements.
これに対して、本件出願人が特願昭57−179265
゜特願昭58−35077で示した光変調素子は、熱に
よって屈折率が変化しやすい熱効果媒体に局所的に熱を
加えることにより屈折率分布を発生し、光束を変調する
ものである。この熱光学効果光変調素子の変調特性は上
述した電気光学、音響光学型の光変調素子のそれとは異
なっており、特に顕著な相違点は減衰時間が数十μse
(〜数十m5ecと長いことである。On the other hand, the present applicant filed a patent application No. 57-179265.
The light modulation element disclosed in Japanese Patent Application No. 58-35077 generates a refractive index distribution by locally applying heat to a thermal effect medium whose refractive index is easily changed by heat, thereby modulating the luminous flux. The modulation characteristics of this thermo-optic effect light modulator are different from those of the electro-optic and acousto-optic light modulators mentioned above, and the most notable difference is that the decay time is several tens of microseconds.
(It is a long time, about several tens of meters5ec.
上述した様な光変調素子を用いて画像形成又は表示を行
う場合には、独立して光変調が行える1つの光変調部が
投影面上では1ドツトの光変調忙対応し、例えばA4の
短手方向は約210Oドツトであるので、A4の短手方
向を一度に変調させる為には、2100個の光変調部を
一列に並べなければならない。そして、これ等の光変調
部をドライブさせる為には、それと同数のドライブ回路
が必要となり、光変調素子の大型化、複雑化を招く。When forming or displaying an image using a light modulation element such as the one described above, one light modulation section that can independently perform light modulation corresponds to one dot of light modulation on the projection surface. Since there are approximately 210 dots in the width direction, in order to modulate the width direction of an A4 sheet at once, 2100 light modulation sections must be arranged in a row. In order to drive these optical modulators, the same number of drive circuits are required, leading to an increase in size and complexity of the optical modulator.
本発明の目的は、複数の変調部を備えた光変調素子にお
いて、駆動機構が簡素化された光変調素子を提供するこ
とを目的とする。SUMMARY OF THE INVENTION An object of the present invention is to provide a light modulation element with a simplified driving mechanism in a light modulation element including a plurality of modulation sections.
本発明に係る光変調素子においては、上述した熱光学効
果光変調素子の減衰時間が長いことに着目し、この現象
を積極的に利用することにょシ上記目的を達成したもの
である。即ち、熱光学効果光変調素子では減衰時間が長
い為に、光変調素子を駆動する入力信号の巾が短かくて
も、光変調部では長い時間に渡って光変調の作用をする
ことができ、変調される全光量は充分な量に達する。従
って光変調素子の一つの変調部を駆動する駆動時間は短
かいので、換言すれば駆動パルスのパルス中が短かいの
で、一つの駆動回路で、時分割的に複数の光変調部を駆
動させることが出来る。故に光変調部の数に対して駆動
回路の数を少なくすることが出来、駆動手段を簡素化す
ることができたのである。以下、図面を用いて本発明を
詳述する。In the light modulation device according to the present invention, the above object is achieved by paying attention to the long decay time of the above-mentioned thermo-optic effect light modulation device and actively utilizing this phenomenon. In other words, since a thermo-optic effect light modulation element has a long decay time, even if the width of the input signal that drives the light modulation element is short, the light modulation section can perform light modulation over a long period of time. , the total amount of light modulated reaches a sufficient amount. Therefore, since the driving time for driving one modulation part of the light modulation element is short, in other words, the duration of the drive pulse is short, so one drive circuit can drive multiple light modulation parts in a time-sharing manner. I can do it. Therefore, the number of drive circuits can be reduced relative to the number of light modulation sections, and the drive means can be simplified. Hereinafter, the present invention will be explained in detail using the drawings.
第1図は本発明に用いる熱光学効果光変調素子の入力電
圧信号と光出力応答特性の関係を説明する図で、(a)
は入力信号である電圧パルス、(b)はその電圧パルス
によって媒体内に発生した屈折率分布によシ変調された
光の出力応答特性である。横軸はいずれも時間である。FIG. 1 is a diagram illustrating the relationship between the input voltage signal and the optical output response characteristic of the thermo-optic effect light modulator used in the present invention, (a)
is a voltage pulse that is an input signal, and (b) is the output response characteristic of light modulated by the refractive index distribution generated in the medium by the voltage pulse. Both horizontal axes are time.
第1図(a)において、(a)−1〜(a) −5は、
各々の電圧パルス中に応じて電圧値を変えて入力した場
合を示す。第1図(b)において、(b)−1〜(b)
−!lは、上記各電圧式カバ〃スに応じた光出力の応答
を示す模式図である。ここで、入力の電圧値を一定のま
までその電圧パルス中を短かくすると、熱光学効果光変
調素子の変調光と非変調光の光量比が低下するので、第
1図においてはそれをできるだけ避ける為に、入力の電
圧パルス中を短かくするにつれて電圧値を高くした様子
を図示している。第1図(b)において、tDiCi=
1,2.・・・・)は光出力の減衰時間を示し、熱光学
効果光変調素子の場合使用する媒体、構造等によって特
性は種々異なるが、一般的に減衰時間iDiは数十μs
ecから数十m5ec の範囲のものが多い。これに
対して入力信号である電圧パルスのパルス中τ1(z=
1.2.・−・りは短かい程効果が大きい。以下にその
詳細について記述する。In FIG. 1(a), (a)-1 to (a)-5 are
The case where the voltage value is changed and inputted according to each voltage pulse is shown. In FIG. 1(b), (b)-1 to (b)
-! 1 is a schematic diagram showing the response of light output according to each of the above-mentioned voltage type covers. Here, if the input voltage value is kept constant and the duration of the voltage pulse is shortened, the light intensity ratio between the modulated light and the unmodulated light of the thermo-optic effect light modulation element will decrease, so in Fig. 1, this is done as much as possible. In order to avoid this problem, the voltage value is increased as the duration of the input voltage pulse is shortened. In FIG. 1(b), tDiCi=
1, 2. ...) indicates the decay time of the optical output, and in the case of a thermo-optic effect light modulation element, the characteristics vary depending on the medium and structure used, but generally the decay time iDi is several tens of μs.
Many range from ec to several tens of m5ec. On the other hand, during the pulse of the voltage pulse that is the input signal, τ1 (z=
1.2.・The shorter the length, the greater the effect. The details are described below.
第2図は、本発明に使用する熱光学効果光変調素子の変
調原理を説明する図で、1は透明保饅板、2は温度変化
に対して屈折率変化を発生する熱効果媒体、6は光反射
層、4及び7は絶縁体、5は導電体で、発熱抵抗体6及
び導電線9と接続さね、電圧印加手段10によって発熱
抵抗体6に電圧が印加されるようになっている。FIG. 2 is a diagram explaining the modulation principle of the thermo-optic effect light modulation element used in the present invention, in which 1 is a transparent retaining plate, 2 is a thermal effect medium that generates a change in refractive index in response to temperature change, and 6 is a light reflecting layer, 4 and 7 are insulators, and 5 is a conductor, which are connected to a heating resistor 6 and a conductive wire 9, and a voltage is applied to the heating resistor 6 by a voltage applying means 10. There is.
8は支持板である。以上の様な構成の熱光学効果光変調
素子に電圧印加手段10によって電圧が印加されると前
記発熱抵抗体乙に熱が発生し、その熱が熱効果媒体2の
中に伝播して屈折率分布21が形成される。その分布2
/部分に光束11が入射すると、その波面が変換されて
第2図に示した破線の光束12として光変調素子から光
が出射する。8 is a support plate. When a voltage is applied by the voltage applying means 10 to the thermo-optic effect light modulation element having the above configuration, heat is generated in the heat generating resistor B, and the heat propagates into the heat effect medium 2 to change the refractive index. A distribution 21 is formed. Its distribution 2
When the light beam 11 is incident on the / portion, its wavefront is converted and the light is emitted from the light modulation element as a light beam 12 indicated by the broken line in FIG.
前記の電圧印加手段10によって発熱抵抗体6に電圧が
印加されない場合は、媒体2中に屈折率分布が発生せず
、従って入射光束は波面の変換をされないで第2図に示
した16の光束として出射する。出射した光束に対して
結像レンズ14にて結像させ、前記の波面が変換されな
い光束の結像スポットを、その位置に設置した遮光板1
5によって遮光する。一方前記の波面が変換された光束
は、上記遮光板位置と異なった位置に結像され、その位
置に受光媒体(感光媒体、スクリーン、あるいは元セン
サー)を配置し、前記遮光板を所定の大きさに選ぶこと
によって、前記受光媒体上に前記波面の変換された光束
を到達せしめ得る。When no voltage is applied to the heating resistor 6 by the voltage applying means 10, no refractive index distribution is generated in the medium 2, and therefore the incident light beam is not wavefront-converted and becomes the 16 light beams shown in FIG. It emits as. A light-shielding plate 1 that forms an image of the emitted light beam with an imaging lens 14 and sets an imaging spot of the light beam whose wavefront is not converted at that position.
5 to block light. On the other hand, the light beam whose wavefront has been converted is imaged at a position different from the position of the light shielding plate, a light receiving medium (photosensitive medium, screen, or original sensor) is placed at that position, and the light shielding plate is set to a predetermined size. By selecting the desired wavelength, the light flux having the converted wavefront can be caused to reach the light-receiving medium.
以上の構成及び方法によシミ圧印加手段10から印加さ
れる電圧信号に応じて、受光媒体16上にて光変調が確
認できる。With the above configuration and method, light modulation can be confirmed on the light receiving medium 16 according to the voltage signal applied from the stain pressure applying means 10.
第6図は、第2図に示した熱光学効果光変調素子の平面
図と、本発明で用いた発熱抵抗体に印加する電圧信号の
駆動方法を示す図である。第6図において、17−1.
17−2.―・−・、17−Nは導電体であり、18−
1.18−2.・・e・。FIG. 6 is a plan view of the thermo-optic effect light modulation element shown in FIG. 2, and a diagram showing a method of driving a voltage signal applied to the heating resistor used in the present invention. In FIG. 6, 17-1.
17-2. ---, 17-N is a conductor, and 18-
1.18-2.・・e・.
18−Nで示されるN個の発熱抵抗体の電極として接続
されている。It is connected as an electrode of N heating resistors indicated by 18-N.
各電極には、導電線19−1.19−2.・・・・。Each electrode has a conductive wire 19-1, 19-2. ....
19−Nが接続されており、その途中に整流素子20−
1.20−2、−−−−.20−Nが接続サレ、それら
の整流素子は3個づつ(以下この数を同時駆動数と呼び
この数は任意であるが、ここでは6個とした)並列にな
るように導電線21−1゜21−2.−・拳、21−n
に接続されている。さらに、導電線21−1.21−2
.・・・・、21−nはそれぞれスイッチ素子22−1
.22−2 。19-N is connected, and a rectifying element 20-N is connected in the middle.
1.20-2, -----. Connect conductive wires 21-1 so that 20-N is connected, and three rectifying elements are connected in parallel (hereinafter, this number is referred to as the number of simultaneous drives, and this number is arbitrary, but here it is set to six).゜21-2. -・Fist, 21-n
It is connected to the. Furthermore, conductive wire 21-1.21-2
.. ..., 21-n are switch elements 22-1, respectively.
.. 22-2.
・・・・、22−nに接続され、且つそれぞれはスイッ
チ駆動信号発生系24に接続されており、スイッチ駆動
信号発生系によって発生した信号が、前記のスイッチ素
子22−1.22−2、−−−−。..., 22-n, and each of them is connected to the switch drive signal generation system 24, and the signal generated by the switch drive signal generation system is transmitted to the switch elements 22-1, 22-2, 22-n, and 22-n. -----.
22−nのいずれかに入力されたときのみそのスイッチ
は接地あるいは一定電位に接続された導線26と導通状
態になる。一方スイッチ駆動信号発生系24から直−並
列変換素子25にも信号を入力するようにし、ビデオ信
号発生装置26からのビデオ信号を前記の同時駆動数(
この場合は前述の如く6とした)だけ同時に並列に出力
するように設計されである。その同時駆動数の並列信号
は前記発熱抵抗体18−1.、18−2 、・・・・罠
並列に入力される。前記のスイッチ駆動信号発生系24
からスイッチ素子22−1.22−2 、・−・・に入
力される信号は時系列信号とする場合には、スイッチ素
子が順次導通状態になり、その場合前記の並列入力信号
は導通状態のスイッチ素子に対応した発熱抵抗体に入力
される結果となる。並列入力信号の一つは第1図に示し
たパルス巾τiの電圧信号であり、任意の時刻において
、同時駆動数の並列信号はその数に対応した発熱抵抗体
にのみ印加され、順次n回の印加が行われることによっ
て、発熱抵抗体の数N個に各ビデオ信号が分配されるこ
とになる。22-n, the switch becomes conductive with the conductor 26 connected to ground or a constant potential. On the other hand, a signal is also inputted from the switch drive signal generation system 24 to the serial-parallel conversion element 25, and the video signal from the video signal generation device 26 is converted into the number of simultaneous drives (
In this case, as mentioned above, the design is such that 6) are simultaneously output in parallel. The parallel signals of the number of simultaneous drives are the heating resistors 18-1. , 18-2, . . . traps are input in parallel. The switch drive signal generation system 24
When the signals inputted from to switch elements 22-1, 22-2, . This results in input to the heating resistor corresponding to the switch element. One of the parallel input signals is a voltage signal with a pulse width τi shown in Fig. 1. At any given time, the parallel signals of the number of simultaneous drives are applied only to the heating resistors corresponding to that number, and are sequentially applied n times. By applying , each video signal is distributed to N heating resistors.
以上の様に、前記減衰時間が長いことを利用して、発熱
抵抗体のN個のすべてに同時に信号を印加する必要がな
(、n (< N )回に分割して駆動することが可能
である。As described above, by utilizing the long decay time, it is not necessary to apply a signal to all N heating resistors at the same time (it is possible to drive the signal divided into n (< N ) times). It is.
同時に駆動すべき発熱抵抗体の数はVn個でよい。The number of heating resistors to be driven simultaneously may be Vn.
第4図は、本発明の光変調素子を用いた一実施例として
光プリンター装置を示す図で、22,24゜25.26
は各々第6図に示した回付号の部材と同じ機能を有する
スイッチ素子系、スイッチ駆動系、直−並列変換系、ビ
デオ信号発生装置であり、27は第3図に示した整流素
子20−1〜20−nを含む光変調素子で、第2図に示
した原理によって光が変調される。28はレーザーある
いは発光ダイオードあるいはハロゲンの如き光源を有す
る光源装置で、照明光学系29によって、光源装置28
から出射した光束を前記光変調素子27を照明する。5
0は上記照明光のうち変調されない光束をできる限り多
く遮光するS元板であり、破線で示した変調光束をでき
る限り多く通過せしめる様に配置する。上記の変調光束
は結像レンズ61によって電子写真感光体が設けられた
円筒体62に結像スポットを形成する。この時、光変調
素子27は、紙面に垂直な方向に前記発熱抵抗体の一次
元プレイを有し、上記円筒体32の母線と平行にそのア
レイからの変調光を一次元配列スポットとして形成せし
めるよう設計したものである。FIG. 4 is a diagram showing an optical printer device as an example using the light modulation element of the present invention.
2 are a switch element system, a switch drive system, a serial-to-parallel conversion system, and a video signal generator, each having the same functions as the members shown in FIG. 6, and 27 is a rectifier element 20 shown in FIG. -1 to 20-n, light is modulated according to the principle shown in FIG. Reference numeral 28 denotes a light source device having a light source such as a laser, a light emitting diode, or a halogen.
The light modulation element 27 is illuminated with the light beam emitted from the light modulation element 27. 5
Reference numeral 0 denotes an S source plate that blocks as much of the unmodulated light beam as possible out of the illumination light, and is arranged so as to allow as much of the modulated light beam indicated by the broken line as possible to pass through. The above-mentioned modulated light beam forms an imaging spot by an imaging lens 61 on a cylindrical body 62 provided with an electrophotographic photoreceptor. At this time, the light modulation element 27 has a one-dimensional play of the heating resistor in a direction perpendicular to the plane of the paper, and forms modulated light from the array as a one-dimensional array spot parallel to the generatrix of the cylindrical body 32. It was designed that way.
第4図において、光源装置は、線状のフィラメントを有
するハロゲンランプあるいはスリット開口を有するハロ
ゲンランプを用いた光源装置としてもよく、照明光学系
29はシリンドリカルレンズあるいはマルチレンズアレ
イでもよい。In FIG. 4, the light source device may be a light source device using a halogen lamp having a linear filament or a halogen lamp having a slit opening, and the illumination optical system 29 may be a cylindrical lens or a multi-lens array.
光変調素子270発熱抵抗体の数は2,000〜5,0
00個を配列し、結像レンズ61によって電子写真感光
体32上に長さ200〜300 ff1mに投影される
。The number of heating resistors in the light modulation element 270 is 2,000 to 5,000.
00 pieces are arranged and projected onto the electrophotographic photoreceptor 32 with a length of 200 to 300 ff1m by the imaging lens 61.
このとき、結像レンズは拡大倍率をもって投影するもの
でもあるいは等倍投影するものでもよい。At this time, the imaging lens may be one that projects with magnification or one that projects at the same magnification.
特に等倍投影の場合には、装置全体が小屋化できる利点
がある。またこの場合、前記の様に線状のフィラメント
を有するハロゲンランプあるいはスリット状の開口を有
する光源装置を用いるとその効果が大きい。すなわち、
レーザーの如きコヒーレント光を用いて前記のように2
00mm〜300 mmの長さを有した発熱抵抗体部を
照明しようとすると、照明系が複雑化あるいは大型化の
ものになってしまうが、上記の様な光源装置を使用すれ
ば照明系はシリンドリカルレンズあるいはマルチレンズ
アレーの如き一般的なものでよい。Particularly in the case of full-scale projection, there is an advantage that the entire apparatus can be made into a shed. Further, in this case, it is highly effective to use a halogen lamp having a linear filament or a light source device having a slit-like opening as described above. That is,
2 as described above using coherent light such as a laser.
If you try to illuminate a heating resistor section with a length of 00 mm to 300 mm, the illumination system will become complicated or large, but if you use a light source device like the one above, the illumination system will be a cylindrical one. It may be a general lens or a multi-lens array.
この実施例に使用する光変調素子は第2図に示したもの
で、熱効果媒体として蒸留水あるいはエチルアルコール
を例として挙げるが、プラスチック、高分子材料、液晶
等でも良い。各発熱抵抗体に印加する電圧パルス中は1
0μsec〜50μsecであり、変調光の減衰時間は
100 μsec 〜500 ll5ecである。従っ
て、駆動の分割数は50程度迄可能である。The light modulation element used in this embodiment is shown in FIG. 2, and although distilled water or ethyl alcohol is used as the thermal effect medium, plastic, polymeric material, liquid crystal, etc. may also be used. 1 during the voltage pulse applied to each heating resistor.
It is 0 μsec to 50 μsec, and the decay time of the modulated light is 100 μsec to 500 μsec. Therefore, the number of driving divisions can be up to about 50.
また、本発明の光変調素子による変調光は)熱効果媒体
内の屈折率分布による光の屈折によるもので、回折によ
るものよりも波面の変換度が大きい。Further, the modulated light by the light modulation element of the present invention is due to refraction of light due to the refractive index distribution within the thermal effect medium, and the degree of wavefront conversion is greater than that due to diffraction.
この作用によっても露光量を低下せしめずに、上記の分
割駆動を実現し得る効果を有する。This action also has the effect of realizing the above-mentioned divided drive without reducing the exposure amount.
これに対して、 U S P 4,281,904 の
光変調素子を使用する場合は、使用する入射光束に偏光
特性を持たせる必要があり、変調光の減衰時間も短かく
、従って分割駆動を実現するためKは本発明のような光
源を使用することは困難である。On the other hand, when using the optical modulation element of USP 4,281,904, the incident light beam used needs to have polarization characteristics, and the decay time of the modulated light is also short, so split drive is not necessary. In order to realize K, it is difficult to use a light source like the one of the present invention.
以上、本発明に係る光変調素子では、熱光学効果光変調
素子の変調特性を有効に利用することにより駆動系を簡
素化したもので、優れた効果を有するものである。As described above, in the light modulation element according to the present invention, the drive system is simplified by effectively utilizing the modulation characteristics of the thermo-optic effect light modulation element, and it has excellent effects.
第1図(a) 、 (b)は本発明に用いる熱光学効果
光変調素子の、信号パルスと変調特性との関係を示す図
、第2図は本発明に用いる熱光学効果光変調素子の作動
を説明する為の図、第6図は本発明の光変調素子の駆動
回路の一実施例を示す図、第4図は本発明の光変調素子
を用いた光プリンター装置の一実施例を示す図。
1・・・・透明保護板、2・・・・熱効果媒体、3・・
・・光反射層、4,7・・・・絶縁体、5壷・・・導電
体、6・・・・発熱抵抗体、8−・・・支持板、10・
・・・電圧印加手段、11・・・・入射光、12−・・
・変調光、16・・・・非変調光、14・・・・結像レ
ンズ、15・・・−遮光板、16・−・受光媒体、17
・・・拳導電体、18・・・・発熱抵抗体、20・・・
拳整流素子、2211@@11スイツチ素子、24・・
・・スイッチ駆動系、25・・・−直重並列変換系、2
6・・・・ビデオ信号発生装置、28・・・ψ光源装置
、27・・・・光変調素子、32−・Φ・電子写真感光
体を有する円筒体。
出願人 キャノン株式会社
第1頁の続き
0発 明 者 望月祐子
東京都大田区下丸子3丁目30番
2号キャノン株式会社内FIGS. 1(a) and (b) are diagrams showing the relationship between signal pulses and modulation characteristics of the thermo-optic effect light modulator used in the present invention, and FIG. 2 is a diagram showing the relationship between the signal pulse and modulation characteristics of the thermo-optic effect light modulator used in the present invention. A diagram for explaining the operation, FIG. 6 is a diagram showing an embodiment of the drive circuit of the light modulation element of the present invention, and FIG. 4 is a diagram showing an embodiment of the optical printer device using the light modulation element of the present invention. Figure shown. 1... Transparent protection plate, 2... Thermal effect medium, 3...
...Light reflecting layer, 4, 7... Insulator, 5 Pot... Conductor, 6... Heat generating resistor, 8-... Support plate, 10...
... Voltage application means, 11... Incident light, 12-...
-Modulated light, 16...Unmodulated light, 14...Imaging lens, 15...-light shielding plate, 16...-light receiving medium, 17
...Fist conductor, 18...Heating resistor, 20...
Fist rectifier element, 2211@@11 switch element, 24...
...Switch drive system, 25... - Direct/load/parallel conversion system, 2
6...Video signal generator, 28...ψ light source device, 27...Light modulation element, 32--Cylindrical body having Φ-electrophotographic photoreceptor. Applicant: Canon Co., Ltd. Page 1 continued 0 Inventor: Yuko Mochizuki, Canon Co., Ltd., 3-30-2 Shimomaruko, Ota-ku, Tokyo
Claims (1)
体に熱を与える複数個の独立した光変調部、該光変調部
を所定の複数個のグループに分け、各々のグループには
該グループに含まれる光変調部を駆動する一個の駆動手
段を配し、各駆動手段は一つのグループに含まれる光変
調部を経時的に順次駆動してゆくことを特徴とする光変
調素子。(1) A thermal effect medium whose refractive index changes with heat, a plurality of independent light modulation sections that apply heat to the medium, the light modulation sections are divided into a plurality of predetermined groups, and each group has a 1. A light modulation element comprising a single drive means for driving light modulation sections included in a group, each drive means sequentially driving the light modulation sections included in one group over time.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10373083A JPS59228633A (en) | 1983-06-10 | 1983-06-10 | Optical modulating element |
US07/063,788 US4848879A (en) | 1982-10-09 | 1987-06-22 | Light modulating device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10373083A JPS59228633A (en) | 1983-06-10 | 1983-06-10 | Optical modulating element |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59228633A true JPS59228633A (en) | 1984-12-22 |
Family
ID=14361758
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP10373083A Pending JPS59228633A (en) | 1982-10-09 | 1983-06-10 | Optical modulating element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59228633A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63161427A (en) * | 1986-12-24 | 1988-07-05 | Minolta Camera Co Ltd | Driving device for optical shutter array |
-
1983
- 1983-06-10 JP JP10373083A patent/JPS59228633A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63161427A (en) * | 1986-12-24 | 1988-07-05 | Minolta Camera Co Ltd | Driving device for optical shutter array |
JP2569516B2 (en) * | 1986-12-24 | 1997-01-08 | ミノルタ株式会社 | Driving device for optical shutter array |
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