CN1678940A - 用于调制光束并具有改进的伽玛响应的方法和装置 - Google Patents

用于调制光束并具有改进的伽玛响应的方法和装置 Download PDF

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CN1678940A
CN1678940A CNA038201615A CN03820161A CN1678940A CN 1678940 A CN1678940 A CN 1678940A CN A038201615 A CNA038201615 A CN A038201615A CN 03820161 A CN03820161 A CN 03820161A CN 1678940 A CN1678940 A CN 1678940A
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CN100380169C (zh
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D·T·阿姆
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ECHELLE Inc
Silicon Light Machines Inc
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    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
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    • G02B26/08Optical devices or arrangements for the control of light using movable or deformable optical elements for controlling the direction of light
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    • GPHYSICS
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Abstract

公开了一种具有改进的可调伽玛响应的装置。所述装置包括:光调制器(20),它具有多个彼此隔开的元件(32),包括位于单一平面(15)的交错的有源和无源元件的;伽玛控制器;以及移位控制器。伽玛控制器将伽玛电压加到衬底(38)上,使多个彼此隔开的元件移动到偏置平面(16),更靠近衬底。在反射方式下,多个彼此隔开的元件对入射光束起镜面作用。在衍射方式下,移位控制器将移位电压加到有源元件上。此时有源元件移动到与偏置平面平行的第二平面,使入射到光调制器上的光束被衍射。检测到的光信号的照度正比于上升至大约1.7 5和3之间的次幂的移位电压,即伽玛响应。

Description

用于调制光束并具有改进 的伽玛响应的方法和装置
发明领域
本发明涉及调制光束的方法和装置。更具体地说,本发明涉及机电偏置的光调制器,通过具有改进的伽玛响应更有效地调制光信号。
发明背景
对于光调制装置,外加信号(通常为电压)和结果输出照度之间的关系称为响应函数或转换函数。许多装置的这种响应函数近似于I=kVγ的函数形式,其中I为输出照度,V为外加电压,k为根据具体装置所选择的任意常数,γ是决定调制器的响应的指数。这样,光调制器可以仅以其伽玛响应来表述。伽玛值为1表示其强度随外加信号呈线性变化的光调制器。在图像显示装置中使用这种装置时,很难提供在图像的最暗部分没有可观察到的颗粒性或可见”台阶”的图像。因此,对于显示器需要有较高的伽玛值。而且,通过使显示装置的伽玛与原来录制图像的方式(称为源伽玛或内容伽玛)相匹配,可以获得最好的图像再现。传统的图像源伽玛值的范围为2到3。
现需要的是一种具有在各种应用情况下可以被优化的可调伽玛响应的光调制器。
发明概述
本发明的实施例包括具有改进的可调伽玛响应的装置。所述装置包括光调制器,所述光调制器具有多个彼此隔开的元件、具有位于第一平面上的交错的有源元件和无源元件并包括伽玛控制器以及移动控制器。伽玛控制器将伽玛电压加到衬底上,形成静电场,所述静电场将彼此隔开的元件拉向与第一平面平行而且最好更靠近衬底的偏置平面。在反射方式下,多个彼此隔开的元件全部位于偏置平面中,照射到多个彼此隔开的元件上的光束基本上被反射,因此所述多个彼此隔开的元件起反射镜的作用。仅接收衍射光的低噪声光接收器(一阶接收器)将检测到具有基本上为零的照度的信号。在衍射方式下,移位控制器将移位电压加到有源元件上。对移位控制器作出响应,把有源元件移位到基本上与偏置平面平行且最好更靠近衬底的第二平面上,使得照射到光调制器上的光束基本上被衍射。此时一阶接收器将检测到具有非零照度的信号。检测到的信号的照度正比于升高到指数幂(称为伽玛响应)的移位电压。最好,伽玛响应在大约1.75和3.0之间。
附图简要说明
图1示意地示出代表性的光调制器。
图2示出图1的光调制器的横截面,在第一平面有细长元件。
图3示出图1的光调制器的横截面,其中,伽玛电压加到衬底上,使得细长元件移位到偏置平面上。
图4示出图1的光调制器的横截面、入射光束和反射光束R。
图5示出图1的光调制器的横截面、入射光束和衍射波前。
图6a是说明图1的光调制器的移位电压和有源元件的偏移之间的关系的曲线图。
图6b是说明图6a所示的偏移和一阶衍射照度I1之间的关系的曲线图。
图6c是说明图6a和图6b二者的卷积的曲线图,并且说明图1的光调制器的移动电压和结果照度之间的关系。
图7是说明当伽玛电压等于0伏、-1伏、-2伏和-3伏时图1的光调制器的移动电压和有源元件相对于偏置平面的偏移之间的关系的曲线图。
图8是上述图7的曲线图,其中图1的光调制器的移动电压和有源元件相对于偏置平面的偏移都是按照对数尺度绘制的。
图9是说明当伽玛电压等于0伏,-1伏,-2伏和-3伏时图1的光调制器的移动电压和归一化一阶衍射强度之间的关系的曲线图。
图10是上述图9的曲线图,其中图1的光调制器的移动电压和归一化一阶衍射强度都是按照对数尺度绘制的。
图11是说明光调制器的伽玛电压和伽玛之间的关系的曲线图。
实施例的详细说明
本发明的实施例包括光调制器,它调制光束并具有可调伽玛响应。在光调制器中,光照射到多个加长的彼此隔开的元件上。通过在交错的彼此隔开的元件上施加输入信号,例如移位电压,使有源元件选择性地变形(弯曲),以致照射光或基本上被反射或基本上被衍射。当光束基本上被衍射时,仅接收一阶衍射光的低噪声光接收器(一阶接收器),例如Schlieren光系统,将检测到具有非零照度I1的光,而当光束基本上被反射时,将检测到具有很小照度或无照度的光。用于在输入信号和照度I1之间转换关系的指数称为伽玛响应。将本发明应用于光调制器上就可提供具有可调伽玛响应的光调制器。这样,就可对移位电压和照度之间的关系作最佳调谐,以适应各种需求。
一阶接收器可以和许多利用调制光的装置或对光进行调制以便以光学方式传送信息的装置耦合。所述装置例如可以用于以下场合:高分辨率图像显示器,它利用调制光束照明投影显示器或计算机到平板(computer-to-plate)产品上的各像素;光开关,它在系统失效时利用调制光束将光数据路由到目的端口或冗余设备上;动态增益均衡器,它利用调制光束校正在光纤上传输的光信号功率的不平衡;以及动态可调滤波器,它利用调制光束滤除可变波长范围内的信号。
图1示意地示出按照本发明实施例的光调制器20。光调制器20最好包括由第一和第二支柱34和36悬挂在衬底38的上方的细长元件32。每个细长元件32包括导电和反射表面40。衬底38包括导体42。工作时,光调制器20起产生从反射方式或衍射方式选择的调制光的作用。
光调制器20包括细长元件32。细长元件32加工成互相平行并基本上位于第一平面上。每个细长元件32包括导电和反射表面40以及弹性材料44。衬底38包括导体42。
工作时,将伽玛电压加到衬底38的导体42上。如下所述,在加伽玛电压前,细长元件32基本上位于第一平面上。伽玛电压产生静电场,静电场使细长元件32弯曲,将细长元件32向衬底38移动。当施加伽玛电压时,细长元件32基本上平行于第一平面略微向衬底38移动,并且移动到偏置平面上方间隙长度G(图3)的位置。如下面更详细描述的,这种移动为光调制器20提供了改进的伽玛响应。
图2示出图1的光调制器20的横截面,此时未加伽玛电压到衬底38(即衬底38的导体42)上。图2显示细长元件32基本上位于第一平面15上。
图3示出图2的光调制器20的横截面,此衬底38上加有伽玛电压,细长元件32上加有零电压。图3示出细长元件32已移动了距离H,更靠近衬底38,移动到基本上与第一平面平行的第二(偏置)平面上。偏置平面16位于衬底38上方距离G处。图3中的距离G和H未按比例画出,而是为了便于说明而以放大的距离示出。实际上,距离H是距离G的一小部分。
图4示出反射方式下的光调制器20。在反射方式下,细长元件32的导电和反射表面40位于偏置平面上,所以入射光I从细长元件32上反射,产生反射光R。在图4中,将伽玛电压加到衬底上,零电压加到细长元件32上。
图5示出衍射方式下的光调制器20。在衍射方式下,移位电压使交错的细长元件32移出偏置平面16,移到更靠近导电38的第二平面17上。对移位电压作出响应移动到第二平面的这部分细长元件称为有源元件,其余的细长元件称为无源元件。将移位电压加到细长元件32的有源元件的反射和导电表面40上。移位电压在细长元件32的交错的有源元件和无源元件之间产生高度差,最好是大约入射光I的四分之一波长λ/4,以获得最大的衍射。四分之一波长的高度差产生的衍射光包括正1和负1衍射级D+1和D-1。这样,加到有源元件上的移位电压将使光调制器20从反射方式移到衍射方式。
应当指出,由于图4和5中入射光和反射光的周期性的缘故,有源元件和无源元件之间大约λ/4的任何奇数倍的高度差产生包括有正1和负1衍射级D+1和D-1的衍射光。在以下的讨论中,任何提到的λ/4高度包括λ/4的奇数倍的高度,任何提到的零高度包括λ/4的偶数倍的高度。
如上所述,图4和5分别示出反射方式和衍射方式的光调制器20。对于有源元件小于四分之一波长λ/4的偏移,入射光I既反射也衍射,产生反射光R和包括有正1和负1衍射级D+1和D-1的衍射光。换句话说,通过使有源元件的偏移小于四分之一波长λ/4,光调制器20就可产生可变的反射率。
对本专业的技术人员来说,显然导电和反射表面40可以用多层的介质反射体和导电元件来代替,其中导电元件埋置在每一个细长元件32之中。
虽然图1-5示出的光调制器20具有六个细长元件32,但光调制器20最好具有更多的细长元件32。通过设置两个以上的细长元件32,细长元件32能够起组的作用,所述组称为像素。最好每个像素是一组两个细长元件32。或者,每个像素是一组多个细长元件32。
本专业的技术人员容易明白,术语”像素”在此用作光调制器的一个元件,而非其更具体显示器的像素的定义。
光调制器在例如1994年5月10日授予Bloom等人的题目为”METHOD AND APPARATUS FOR MODULATING A LIGHT BEAM”的美国专利No.5,311,360中,以及1998年11月24日授予Bloom等人的题目为”FLAT DIFFRACTION GRATIONG LIGHT VALVE”的美国专利No.5,841,579中有进一步的说明,这两份专利均作为参考包括在本文内。
参考图6a-c可以更好地理解在图1的光调制器的细长元件32上加伽玛电压的好处。图6a是说明当衬底加有零电压时,加到有源元件上的电压V(移位电压)和有源元件向衬底38移动的距离d之间的关系的曲线图。图6a示出距离d相对于移位电压V大约为方程d∝V2的关系。图6a示出当移位电压V低于某个中间电压V0时,位移d几乎为零,而当移位电压V高于临界电压V1时位移d不成比例地增大。工作时,光调制器通常工作在小于V1的移位电压。
图6b示出d和相应的照度I1之间的关系图,例如照度I1是由仅接收一阶衍射光的低噪声光接收器(例如Schlieren光系统)检测到的照度。图6b示出照度按照公式I1∝sin2(2πd/λ)而改变,式中λ为入射光束的波长,d为有源元件和无源元件之间的距离。图6b尤其示出,对于等于或几乎等于零的小偏移d,相应的照度I1为零。
图6c示出图6a和图6b的曲线图的卷积,示出移位电压V和照度I1之间的关系。图6c示出对于小移位电压V,相应的照度I1就较小,而对于大移位电压V,相应的照度I1就大。对许多光调制器来说,这个关系可以用公式I1=kVγ来表示,式中γ具有1和4之间的某个数值。图6c还示出对应于足以使有源元件偏离偏置平面而向衬底移动等于入射光束四分之一波长(λ/4)距离的电压的最大强度50。
通过在衬底38的导体42上加伽玛电压Vg=-V0,图1的光调制器20就可在图6a中V=V0右侧的那一部分工作。由于光调制器现在工作在图6c中V=V0右侧的那一部分,即使很小但不同的移位电压将会产生独特的非零照度I1。这样,例如在图像显示装置中,很小但不同的输入信号(即移位电压)将产生独特的照度。这样,即使低照明的像素也将显示一些对比度。输入信号可以是例如二进制权重的电压,但应当指出,任何形式的输入信号都可以使用。
图6a中所示的外加电压V和偏移d之间的关系根据以下事实得出的:对于图1的光调制器,随着细长元件32和衬底38之间的距离减小,衬底38和细长元件32之间的电容增加。所以,当加上移位电压V,使细长元件32向衬底38的方向移动某一距离时,还需要一个更小的附加移位电压ΔV使细长元件32向衬底38移动一附加距离。
应当指出,是细长元件32和衬底38之间的电压差(V-Vg)产生了静电电位(在此为正电压差),将有源元件32拉向第二平面,更靠近衬底38。伽玛电压可以是任何电压(正、负或零),只要伽玛电压Vg和移位电压V之间的电压差(V-Vg)足以在细长元件32和衬底38之间产生静电场就可以。这样,例如在一个实施例中,伽玛电压Vg等于-5伏。加到细长元件上的电压和加到衬底上的电压之间的电压差(0伏-(-5)伏,或+5伏)就足以将细长元件32拉向偏置平面,更靠近衬底38。在此实施例中,移位电压V可以从零伏(将光调制器置于反射方式)到10伏(将光调制器置于衍射方式)。
在另一实施例中,伽玛电压Vg等于-3伏。加到细长元件上的电压和加到衬底上的电压之间的电压差(0伏-(-3)伏,或+3伏)足以将细长元件32拉向偏置平面,更靠近衬底38。所以,移位电压V可以从零伏(将光调制器置于反射方式)到12伏(将光调制器置于衍射方式)。
在又一实施例中,伽玛电压Vg等于0伏。可以将正电压V加到细长元件32上,以使细长元件32和衬底38之间的电压差(V(伏)-0伏,或+V(伏))足以产生能将细长元件32拉向偏置平面的静电电位,使之更靠近衬底38。这时光调制器处于反射方式。加到有源元件上的附加电压将有源元件拉向第二平面,更靠近衬底,将光调制器置于衍射方式。应当指出,在将伽玛电压或者加到衬底上或者加到细长元件上以产生电压差,将有源元件拉向偏置平面,最好更靠近衬底的情况下,本发明的实施例都可起作用。
应当指出,上述实施例中的光调制器起三端装置的作用,在有源元件和衬底之间产生静电电位,在无源元件和衬底之间也产生静电电位。
当衬底38上方第二平面的高度大于偏置平面和衬底38之间的间隙距离G的2/3时,图1所示的光调制器20工作最有效。当衬底38上方第二平面的高度小于(2/3)G时,有源元件会碰撞公共平面38,不可修复地损坏光调制器。使有源元件向第二平面移动大约为衬底38上(2/3)G距离的移位电压称为Vsnap,也称为开关电压。在本发明的一个实施例中,第二平面在衬底上方的高度大约为(3/4)G。应当指出,增加间隙距离G会增加Vsnap,因而可降低损坏的可能性。
按照本发明的实施例还提供一种具有可调伽玛响应的光调制器,方法是在衬底38上加一定范围的伽玛电压。图7-10中图解说明可以轻易地这样做,以下将描述图7-10。复习一下用于产生图7-10中描绘的曲线图的方程会有所帮助。
通常,细长元件32中有源元件的偏移与移位电压V、伽玛电压Vg、间隙长度G以及元件拉向衬底的电压Vsnap有关,经验导出的表达式如方程(1)所示:
d(V)=0.4G[{1-((V-Vg)/Vsnap)2}0.444-1]           (1)
照度I1随移位电压V、方程(1)中描述的函数d(V)、Vg和λ(入射光束的波长)而改变,如方程(2)所示:
I1(V)=[sin{(2π/λ)(d(V-Vg)-d(0-Vg))}2      (2)
在方程(2)中,表达式d(V-Vg)指衍射方式下有源元件的总偏移,即到偏置平面的偏移加上偏移距离λ/4。表达式d(0-Vg)指无源元件从第一平面到偏置平面的偏移,即图3所示的距离H。
图7-10是对于光调制器20、利用方程(1)和(2)而产生的,用于图形说明光调制器的伽玛如何随伽玛电压Vg而变化。图7中有四条曲线,曲线100-103,各自表示移位电压V(伏)和加有移位电压的细长元件距偏置平面的相应位移(以纳米计)之间的关系。
在图7中,曲线100说明当伽玛电压Vg=0伏时移位电压V和有源元件距偏置平面的位移d之间的关系。曲线101说明当伽玛电压Vg=-1伏时移位电压V和有源元件距偏置平面的位移d之间的关系。曲线102说明当伽玛电压Vg=-2伏时移位电压V和有源元件距偏置平面的位移d之间的关系。曲线103说明当伽玛电压Vg=-3伏时移位电压V和有源元件距偏置平面的位移d之间的关系。
曲线100-103说明:通过降低伽玛电压Vg,给定的移位电压将会有相应较大的位移d。例如,当伽玛电压Vg=0时(对应于曲线100),移位电压V=V0产生的偏移等于0。曲线100在此点的斜率为零。当伽玛电压Vg降到-3伏时(对应于曲线103),移位电压V=V0具有非零数值。曲线103在此点的斜率为正。随着伽玛电压进一步降低,偏置平面上的细长元件更靠近衬底,移位电压V与细长元件的位移d的关系曲线的斜率增加。即:小的移位电压可以产生相当大的位移d。如下所述,这又可产生伽玛数值下降的光调制。
图8示出曲线110-113,它们各自表示移位电压V(伏)和有源元件距偏置平面的位移d(以纳米计)之间的关系,如图7所示。曲线110-113分别与图7的曲线100-103的区别在于曲线110-113是以对数尺度绘制各轴线的。曲线110说明当伽玛电压Vg=0伏时移位电压V和有源元件距偏置平面的位移d之间的关系,二者均用对数尺度绘制。曲线111说明当伽玛电压Vg=-1伏时移位电压V和有源元件距偏置平面的位移d之间的关系,二者均用对数尺度绘制。曲线112说明当伽玛电压Vg=-2伏时移位电压V和有源元件距偏置平面的位移d之间的关系,二者均用对数尺度绘制。曲线113说明当伽玛电压Vg=-3伏时移位电压V和有源元件距偏置平面的位移d之间的关系,二者均用对数尺度绘制。
图9示出曲线120-123,它们表示图1的光调制器在各种伽玛电压下移位电压V和相应的归一化一阶衍射强度I1之间的关系。曲线120示出当伽玛电压Vg=0伏时移位电压V和相应的一阶照度I1之间的关系。代表对应于入射光束四分之一波长偏移的最大强度的点,由于处于图9所示的范围之外,故未示出。
曲线121说明当伽玛电压Vg=-1伏时移位电压V和相应的一阶照度I1之间的关系。点121a代表最大强度,对应于入射光束四分之一波长的偏移。
曲线122说明当伽玛电压Vg=-2伏时移位电压V和相应的一阶照度I1之间的关系。点122a代表最大强度,对应于入射光束四分之一波长的偏移。
曲线123说明当伽玛电压Vg=-3伏时移位电压V和相应的一阶照度I1之间的关系。点123a代表最大强度,对应于入射光束四分之一波长的偏移。曲线120-123说明:通过降低伽玛电压Vg(从而将细长元件拉向偏置平面,更靠近衬底),给定的移位电压将会产生较大的照度。图10中进一步说明这种关系。
图10示出曲线130-133,它们图解说明图1的光调制器在各种伽玛电压下移位电压V和相应的归一化一阶衍射强度I1之间的关系。曲线130-133分别与图9的曲线120-123的区别在于曲线130-133是以对数尺度绘制各轴线的。曲线130-133各自的斜率以方程(3)表示:
γ=logI1/logV            (3)
方程(3)定义了移位电压V和相应的归一化一阶衍射强度I1之间的关系,它定义了光调制器的伽玛。
曲线130说明当伽玛电压Vg=0伏时移位电压V的对数和一阶衍射强度I1的对数之间的关系。所述曲线的斜率(因此伽玛响应)大约为4。曲线131说明当伽玛电压Vg=-1伏时移位电压V的对数和一阶衍射强度I1的对数之间的关系。所述曲线的斜率(因此伽玛响应)大约为3.1。曲线132说明当伽玛电压Vg=-2伏时移位电压V的对数和一阶衍射强度I1的对数之间的关系。所述曲线的斜率(因此伽玛响应)大约为2.7。曲线133说明当伽玛电压Vg=-3伏时移位电压V的对数和一阶衍射强度I1的对数之间的关系。所述曲线的斜率(因此伽玛响应)大约为2.5。曲线130-133说明:通过改变光调制器的伽玛电压Vg,可以调谐转换关系以及伽玛响应。
图11描绘把光调制器的伽玛电压Vg和相应的伽玛响应值(γ)绘制成曲线的曲线图。图11的曲线采用正移位电压。但是应当指出,其它电压也可使用,因为光调制器使用电压差而非绝对电压来工作。图11说明可以通过改变图1的光调制器的伽玛电压,将伽玛响应调谐到各种数值。
伽玛响应可调谐的光调制器具有许多应用。例如,为具有第一伽玛响应的第一装置产生的图像可以在调谐成具有第一伽玛响应的第二装置上显示。因此,可以把在第二装置上产生的结果图像调谐成如同在第一装置上显示的一样,或者调谐成具有任何形式的对比度图像。应当指出,伽玛响应可调谐的光调制器在利用调制光的产品中可具有其它用途。
对本专业的技术人员来说,显然可以对实施例作出各种其它的改动,而不背离由所附权利要求书所定义的本发明的精神和范围。

Claims (20)

1.一种用于调制入射光束的调制器,它包括:
多个细长的彼此隔开的元件,它们加工成彼此平行并且基本上位于第一平面内,其中交错的元件处在第一部分,而其余元件处在第二部分;
伽玛控制器,用于将所述多个细长的彼此隔开的元件移动到偏置平面,其中所述偏置平面平行于所述第一平面;以及
移位控制器,用于将所述彼此隔开的元件的所述第一部分移动到所述偏置平面,以反射所述入射光束,以及将所述彼此隔开的元件的所述第一部分移动到与所述偏置平面平行的第二平面,以衍射所述入射光束。
2.如权利要求1所述的调制器,其中所述细长的彼此隔开的元件安装在衬底上方。
3.如权利要求1所述的调制器,其中按照所述入射光束的大约四分之一波长的奇数倍移动所述偏置平面和所述第二平面。
4.如权利要求2所述的调制器,其中所述移位控制器使所述彼此隔开的元件的所述第一部分向所述衬底弯曲。
5.如权利要求2所述的调制器,其中从所述第二平面到所述衬底的距离大于从所述第一平面到所述衬底的距离的大约2/3。
6.如权利要求1所述的调制器,其中激励所述伽玛控制器以便移动所述多个彼此隔开的元件的操作改进了所述调制器的伽玛响应。
7.如权利要求6所述的调制器,其中所述伽玛响应改进到大约1.75到大约3的范围。
8.如权利要求1所述的调制器,其中所述伽玛控制器包括第一电压信号。
9.如权利要求1所述的调制器,其中所述移位控制器包括第二电压信号。
10.一种用于调制入射光束的方法,所述方法包括:
偏置所述多个细长的、彼此隔开的加工成彼此平行的元件,使之基本上位于偏置平面内;以及
将所述彼此隔开的元件的第一部分移动到所述偏置平面,以便反射所述入射光束,并且将所述彼此隔开的元件的第一部分移动到第二平面,以便衍射所述入射光束。
11.如权利要求10所述的方法,其中按照所述入射光束的大约四分之一波长的奇数倍移动所述偏置平面和所述第二平面。
12.如权利要求10所述的方法,其中还包括将所述多个细长的彼此隔开的元件安装在衬底上方的步骤。
13.如权利要求12所述的方法,其中所述偏置步骤包括在所述多个细长的彼此隔开的元件和所述衬底之间加第一电压。
14.如权利要求10所述的方法,其中所述移动步骤包括在所述彼此隔开的元件的所述第一部分和所述衬底之间加第二电压。
15.如权利要求10所述的方法,其中偏置所述多个细长的彼此隔开的元件的操作改进了所述调制器的伽玛响应。
16.如权利要求15所述的方法,其中所述伽玛响应改进到大约1.75到大约3的范围。
17.如权利要求14所述的方法,其中从所述第二平面到所述衬底的距离大于从所述第一平面到所述衬底的距离的大约2/3。
18.一种用于调制入射光束的调制器,它包括:
用于对具有第一转换关系的输入信号作出响应而选择性地反射或衍射所述入射光束的装置,所述第一转换关系是所述输入信号的函数;以及
用于这样偏置所述调制器,使得所述调制器被偏置之后具有第二转换关系的装置。
19.如权利要求18所述的调制器,其中所述入射光束和所述衍射入射光束之间的所述第二转换关系是指数关系,所述指数的幂在大约1.75和3之间。
20.如权利要求19所述的调制器,其中所述第一转换关系和所述第二转换关系是所述调制器的伽玛响应的函数。
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CN107561685B (zh) * 2017-09-30 2020-10-02 Oppo广东移动通信有限公司 滤光片、镜头模组和成像模组

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