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CN101718884B - Zero-level light optical locating method of optical grating substrate in manufacturing of plane holographic grating - Google Patents

Zero-level light optical locating method of optical grating substrate in manufacturing of plane holographic grating Download PDF

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CN101718884B
CN101718884B CN200910217814XA CN200910217814A CN101718884B CN 101718884 B CN101718884 B CN 101718884B CN 200910217814X A CN200910217814X A CN 200910217814XA CN 200910217814 A CN200910217814 A CN 200910217814A CN 101718884 B CN101718884 B CN 101718884B
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mirror
reticle
light
plane
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CN101718884A (en
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孔鹏
李文昊
巴音贺希格
齐向东
唐玉国
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Changchun Institute of Optics Fine Mechanics and Physics of CAS
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Abstract

The invention relates to a zero-level light optical locating method of an optical grating substrate in manufacturing of a plane holographic grating, belonging to a locating method of the optical grating substrate in the spectroscopy field; the solved technical problem is that the zero-level light optical locating method of the optical grating substrate in manufacturing of the plane holographic grating is provided; the technical proposal is that: step I, a set of plane holographic grating exposure unit is allocated, and the unit is completely consistent to a holographic grating exposure unit in the prior art; step II, a monitoring laser and a reticle are additionally arranged in the plane holographic grating exposure unit, and the position of a standard optical grating is recorded on the reticle; step III, another reticle is additionally arranged, the position of a monitoring laser beam is recorded on the two reticles; step IV, the optical grating substrate is installed and regulated to lead the reflected light of the monitoring laser beam to return to the center of the reticles, at the moment, exposure is carried out to manufacture the plane holographic grating with standard grating constant. The method can rapidly and accurately locate the optical grating substrate and improve the manufacturing efficiency.

Description

平面全息光栅制作中光栅基底的零级光定位方法 Zero-order light positioning method for grating substrate in the fabrication of planar holographic gratings

技术领域technical field

本发明属于光谱技术领域中涉及的一种平面全息光栅制作中光栅基底的定位方法。 The invention belongs to the field of spectrum technology and relates to a method for positioning a grating substrate in the production of a plane holographic grating. the

背景技术Background technique

在平面全息光栅的制作中,光栅基底的定位精度会直接影响光栅常数的精确度,利用零级光对光栅基底进行定位能够保证光栅常数的精确度。 In the manufacture of planar holographic gratings, the positioning accuracy of the grating substrate will directly affect the accuracy of the grating constants, and the use of zero-order light to position the grating substrate can ensure the accuracy of the grating constants. the

平面全息光栅是通过光刻胶记录下两相干光束的干涉条纹后经显影制作而成,其光栅常数由干涉条纹周期决定。制作平面全息光栅时的干涉条纹周期非常小,实际中难以对其进行直接的精确测量。常规的检测方法一般都是在完成光栅制作后,通过测量光栅0级与1级衍射光的夹角来计算光栅常数,测量误差较大,光路调整过程没有固定的基准可依,仅凭经验进行调整,往往要经过多个光栅制作回合,并且很难达到要求的精度。与本发明最为接近的已有技术是中国专利号为CN1544994的专利,提出一种平面全息光栅制作中精确控制光栅常数的方法,平面全息光栅曝光装置结构示意图如图1所示。激光光源1发出的光束经第一平面反射镜2和第二平面反射镜3反射,再经空间滤波器4扩束滤波后成为球面波,球面波经准直反射镜5准直后成为平行光,在平行光光路里放置第五平面反射镜8引出一束平行光,再经第六平面反射镜9反射后到达半反半透镜10,调整第六平 面反射镜9使通过半反半透镜10的反射光和透射光均以自准直衍射角入射到标准机刻反射光栅11上,这两束光经标准机刻反射光栅11的±1级自准直衍射后,各自按它们的入射方向原路返回,再经半反半透镜10之后,-1级的反射光和+1级的透射光在半反半透镜10的另一侧重叠,在接收屏12上形成干涉条纹。这时,将第五平面反射镜8和第六平面反射镜9以及标准机刻反射光栅11撤走并保持半反半透镜10和接收屏12位置不变,在平行光束中放置第三平面反射镜6和第四平面反射镜7,调整两束反射光方向使它们在接收屏上形成与原来一样的干涉条纹。这样,在放置标准机刻反射光栅11的区域由第三平面反射镜6和第四平面反射镜7的反射光束交汇形成的干涉场的条纹周期就与标准机刻反射光栅11的光栅常数相同,将涂有光刻胶的光栅基底放置到标准机刻反射光栅11的位置进行曝光、显影就可以制得具有标准光栅常数的平面全息光栅。 The planar holographic grating is made by recording the interference fringes of two coherent light beams through photoresist and then developed. The grating constant is determined by the period of the interference fringes. The period of the interference fringes when making a planar holographic grating is very small, and it is difficult to measure it directly and accurately in practice. The conventional detection method is to calculate the grating constant by measuring the angle between the 0th order and the 1st order diffracted light of the grating after the grating is manufactured. The measurement error is relatively large. There is no fixed benchmark for the optical path adjustment process, and it is only based on experience. Adjustments often have to go through multiple grating production rounds, and it is difficult to achieve the required accuracy. The existing technology closest to the present invention is Chinese Patent No. CN1544994, which proposes a method for precisely controlling the grating constant in the manufacture of a planar holographic grating. The schematic diagram of the planar holographic grating exposure device is shown in Figure 1. The light beam emitted by the laser light source 1 is reflected by the first plane mirror 2 and the second plane mirror 3, and then becomes a spherical wave after being expanded and filtered by the spatial filter 4, and the spherical wave becomes parallel light after being collimated by the collimating mirror 5 , place the fifth flat reflector 8 in the parallel light path to draw a bunch of parallel light, then reach the half mirror 10 after being reflected by the sixth plane reflector 9, adjust the sixth plane reflector 9 to pass through the half mirror Both the reflected light and the transmitted light of 10 are incident on the standard machine-engraved reflective grating 11 at the self-collimation diffraction angle. The direction goes back the same way, and after passing through the half mirror 10, the reflected light of -1 level and the transmitted light of +1 level overlap on the other side of the half mirror 10, forming interference fringes on the receiving screen 12. At this time, the fifth plane reflector 8 and the sixth plane reflector 9 and the standard machine-engraved reflective grating 11 are withdrawn and the positions of the half mirror 10 and the receiving screen 12 are kept unchanged, and the third plane reflector is placed in the parallel light beam. The mirror 6 and the fourth plane reflector 7 adjust the direction of the two beams of reflected light so that they form the same interference fringes on the receiving screen as before. Like this, the fringe period of the interference field formed by the intersection of the reflected light beams of the third plane reflector 6 and the fourth plane reflector 7 in the area where the standard engraved reflective grating 11 is placed is the same as the grating constant of the standard engraved reflective grating 11, A planar holographic grating with a standard grating constant can be produced by placing the grating substrate coated with photoresist at the position of the standard engraved reflective grating 11 for exposure and development. the

该方法存在的主要问题是:实际操作中撤走标准机刻反射光栅11后,很难将待曝光的光栅基底还原到标准机刻反射光栅11原来的位置,如果待曝光的光栅基底法线偏离标准机刻反射光栅11的法线方向,则必然使制作出光栅的光栅常数产生误差。待曝光的光栅基底法线偏离标准机刻反射光栅11的法线方向越多,制作出光栅的光栅常数误差越大。 The main problem of this method is: after removing the standard machine-engraved reflective grating 11 in actual operation, it is difficult to restore the grating substrate to be exposed to the original position of the standard machine-engraved reflective grating 11. If the normal line of the grating substrate to be exposed deviates from The normal direction of the standard machine engraved reflective grating 11 will inevitably cause errors in the grating constant of the fabricated grating. The more the normal line of the grating substrate to be exposed deviates from the normal direction of the standard machine-engraved reflective grating 11, the greater the error of the grating constant of the fabricated grating. the

发明内容Contents of the invention

为了克服已有技术存在的问题,本发明的目的在于建立一种简便可行的在平面全息光栅制作中采用零级光对光栅基底进行精确定位的方法。 In order to overcome the problems existing in the prior art, the object of the present invention is to establish a simple and feasible method for precise positioning of the grating substrate using zero-order light in the manufacture of planar holographic gratings. the

本发明要解决的技术问题是:提供一种平面全息光栅制作中光栅基底的零级光定位方法。解决技术问题的技术方案为:步骤一,配备一套平面全息光栅曝光装置,该装置与背景技术中的全息光栅曝光装置完全一致,如图2所示,包括激光光源1、第一平面反射镜2、第二平面反射镜3、空间滤波器4、准直反射镜5、第三平面反射镜6、第四平面反射镜7、第五平面反射镜8、第六平面反射镜9、半反半透镜10、标准机刻反射光栅11和接收屏12;该光路结构及调整与背景技术中的描述完全一致,在接收屏12上能够观察到铅直并清晰可见的干涉条纹;步骤二,在平面全息光栅曝光装置中,在正对标准机刻反射光栅11的一侧置有监测激光器13,在监测激光器13的出射光路前方置有第一分划板14,如图2所示,监测激光器13的出射光束穿过第一分划板14中心正入射到标准机刻反射光栅11上,零级衍射光原路返回第一分划板14中心;步骤三,如图3所示,取下图2中标准机刻反射光栅11、第五平面反射镜8和第六平面反射镜9,并确保半反半透镜10、接收屏12、监测激光器13和第一分划板14的位置不变,这时调节第三平面反射镜6和第四平面反射镜7的反射光分别经半反半透镜10透射和反射后叠加,使接收屏12上的干涉条纹的方向和数量分别与标准机刻反射光栅11所产生的干涉条纹相同,在监测激光器13的出射光束的传播方向上半反半透镜10的另一侧远处放置第二分划板15,使监测激光器13的出射光束穿过第二分划板15的中心,这时将监测激光器13移到第二分划板15后方并使其出射光束先后通过第二分划板15和第一分划板14的中心;步骤四,如图4所示,取下图3所示的半反半透镜10、接收屏12和第一分划板14,将涂有光刻胶的待制作光栅基底16放置到标准机刻反射光栅11的位置,光栅基底16的装卡具安装在能够调整旋转、俯仰的精密调整台上,调整光栅基底16使监测激光器13的出射光束经光栅基底16的反射光原路返回第二分划板15的中心,此时进行曝光就能制作出具有标准光栅常数的平面全息光栅。 The technical problem to be solved by the present invention is to provide a zero-order light positioning method for the grating substrate in the manufacture of the planar holographic grating. The technical solution to solve the technical problem is: step 1, equip a set of planar holographic grating exposure device, which is completely consistent with the holographic grating exposure device in the background technology, as shown in Figure 2, including laser light source 1, first plane reflector 2. The second plane mirror 3, the spatial filter 4, the collimation mirror 5, the third plane mirror 6, the fourth plane mirror 7, the fifth plane mirror 8, the sixth plane mirror 9, half mirror Semi-mirror 10, standard machine-engraved reflective grating 11 and receiving screen 12; the optical path structure and adjustment are completely consistent with the description in the background technology, and vertical and clearly visible interference fringes can be observed on the receiving screen 12; Step 2, in In the planar holographic grating exposure device, a monitoring laser 13 is placed on the side facing the standard engraved reflective grating 11, and a first reticle 14 is placed in front of the exit light path of the monitoring laser 13, as shown in Figure 2, the monitoring The outgoing beam of the laser 13 passes through the center of the first reticle 14 and is incident on the standard engraved reflective grating 11, and the zero-order diffracted light returns to the center of the first reticle 14 in the original path; Step 3, as shown in Figure 3, takes The standard engraved reflective grating 11, the fifth plane reflector 8 and the sixth plane reflector 9 in the following figure 2, and ensure that the positions of the half mirror 10, the receiving screen 12, the monitoring laser 13 and the first reticle 14 are consistent. At this time, the reflected light of the third plane reflector 6 and the fourth plane reflector 7 is adjusted to be superimposed after being transmitted and reflected by the half mirror 10 respectively, so that the direction and quantity of the interference fringes on the receiving screen 12 are respectively different from those of the standard machine The interference fringes produced by engraved reflective grating 11 are the same, and the second reticle 15 is placed far away on the other side of half mirror 10 in the propagation direction of the outgoing light beam of monitoring laser 13, so that the outgoing light beam of monitoring laser 13 passes through At the center of the second reticle 15, at this moment, the monitoring laser 13 is moved to the second reticle 15 rear and its outgoing light beam passes through the center of the second reticle 15 and the first reticle 14 successively; Step 4, As shown in Figure 4, take off the half mirror 10 shown in Figure 3, the receiving screen 12 and the first reticle 14, the grating substrate 16 to be made that is coated with photoresist is placed on the position of the standard machine engraving reflective grating 11 The mounting fixture of the grating base 16 is installed on a precision adjustment platform capable of adjusting rotation and pitch, and the grating base 16 is adjusted so that the outgoing light beam of the monitoring laser 13 returns to the center of the second reticle 15 through the original path of the reflected light of the grating base 16 , then exposure can produce a planar holographic grating with a standard grating constant. the

本发明工作原理说明:以具有标准光栅常数的机刻光栅做为基准,使干涉条纹周期与具有标准光栅常数的机刻光栅的光栅常数一致,调整待制作光栅基底使其与干涉条纹垂直,从而使制得的平面全息光栅的光栅常数与具有标准光栅常数的机刻光栅相同。步骤一,调整第六平面反射镜9,使它的反射光经半反半透镜10后分为两束光,一束为反射光,另一束为透射光。半反半透镜10的反射光以+1级自准直方向入射到标准机刻反射光栅11上,根据自准直原理,衍射光按其入射方向原路返回至半反半透镜10,其中一半透过半反半透镜10到达接收屏12;半反半透镜10的透射光以-1级自准直方向入射到标准机刻反射光栅11上,衍射光按其入射方向原路返回至半反半透镜10,其中一半经半反半透镜10反射到达接收屏12,到达接收屏12的两束相干光束叠加形成干涉条纹。步骤二,在正对标准机刻反射光栅11的一侧放置监测激光器13,使其出射光通过第一分划板14的中心正入射到标准机刻反射光栅11上,零级衍射光原路返回第一分划板14中心。步骤三,取下标准机刻反射光栅11、第五平面反射 镜8和第六平面反射镜9,用第三平面反射镜6和第四平面反射镜7的反射光代替标准机刻反射光栅11自准直状态下的+1级和-1级衍射光,第三平面反射镜6的反射光透过半反半透镜10到达接收屏12,第四平面反射镜7的反射光经半反半透镜10反射到达接收屏12,两束光干涉形成干涉条纹,由步骤一和步骤三获得的相干光有相同的传播方向和光程差,必然有相同的干涉条纹。在监测激光器13的出射光束传播方向上半反半透镜10的另一侧远处放置第二分划板15,使监测激光器13的出射光束穿过第二分划板15的中心,这样第一分划板14和第二分划板15的中心连线方向就是标准机刻反射光栅11的法线方向,将监测激光器13移到第二分划板15后方,使其出射光束先后穿过第二分划板15和第一分划板14的中心。步骤四,取下半反半透镜10、接收屏12和第一分划板14,将涂有光刻胶的待制作光栅基底16放置到标准机刻反射光栅11的位置,调整光栅基底16的旋转、俯仰使监测激光器13入射在光栅基底16上的激光束的反射光返回第二分划板15的中心,使光栅基底16的法线与标准机刻反射光栅11的法线方向相同,从而制作出的平面全息光栅的光栅常数与标准机刻反射光栅11相同。 Description of the working principle of the present invention: take the machine-engraved grating with standard grating constants as a reference, make the interference fringe period consistent with the grating constant of the machine-engraved grating with standard grating constants, and adjust the grating substrate to be made to be perpendicular to the interference fringes, thereby The grating constant of the prepared planar holographic grating is the same as that of the machine-engraved grating with the standard grating constant. Step 1, adjust the sixth flat reflector 9 so that its reflected light is divided into two beams after passing through the half mirror 10, one beam is reflected light, and the other beam is transmitted light. The reflected light of the half-mirror 10 is incident on the standard machine-engraved reflective grating 11 with the +1-level self-collimation direction, and according to the principle of self-collimation, the diffracted light returns to the half-mirror 10 according to the original path of its incident direction, and half of them Pass through the half-mirror 10 to reach the receiving screen 12; the transmitted light of the half-mirror 10 is incident on the standard engraved reflective grating 11 in the -1st order self-collimation direction, and the diffracted light returns to the half-reflective grating according to its original path of incidence. Half of the lens 10 is reflected by the half mirror 10 to reach the receiving screen 12, and the two beams of coherent light beams arriving at the receiving screen 12 are superimposed to form interference fringes. Step 2: Place the monitoring laser 13 on the side facing the standard machine-engraved reflective grating 11, so that the outgoing light is incident on the standard machine-engraved reflective grating 11 through the center of the first reticle 14, and the zero-order diffracted light passes through the original path Return to the center of the first reticle 14 . Step 3, remove the standard machine-engraved reflective grating 11, the fifth plane reflector 8 and the sixth plane reflector 9, and replace the standard machine-engraved reflective grating 11 with the reflected light of the third plane reflector 6 and the fourth plane reflector 7 +1 order and -1 order diffracted light under the self-collimation state, the reflected light of the 3rd plane reflector 6 reaches the receiving screen 12 through the half mirror 10, the reflected light of the 4th plane reflector 7 passes through the half mirror half mirror 10 is reflected and reaches the receiving screen 12, and the two beams of light interfere to form interference fringes. The coherent light obtained by step 1 and step 3 has the same propagation direction and optical path difference, and must have the same interference fringes. Place the second reticle 15 far away on the other side of the semi-mirror 10 in the outgoing light beam propagation direction of the monitoring laser 13, so that the outgoing light beam of the monitoring laser 13 passes through the center of the second reticle 15, so that the first The direction of the connecting line between the centers of the reticle 14 and the second reticle 15 is the normal direction of the standard machine-engraved reflective grating 11, and the monitoring laser 13 is moved to the rear of the second reticle 15 so that its outgoing light beam passes through the second reticle successively. The center of the second reticle 15 and the first reticle 14. Step 4, remove the half mirror 10, the receiving screen 12 and the first reticle 14, place the grating substrate 16 coated with photoresist to the position of the standard machine-engraved reflective grating 11, adjust the rotation of the grating substrate 16, The pitch makes the reflected light of the laser beam incident on the grating substrate 16 by the monitoring laser 13 return to the center of the second reticle 15, so that the normal of the grating substrate 16 is in the same direction as the normal of the standard machine-engraved reflective grating 11, thereby producing The grating constant of the planar holographic grating is the same as that of the standard machine-engraved reflective grating 11. the

本发明的积极效果:可以快速准确地调整平面全息光栅曝光装置中干涉场的干涉条纹周期,并将干涉条纹周期准确的转移到涂有光刻胶的光栅基底上,从而大大的提高了平面全息光栅的光栅常数的精确度。 The positive effect of the present invention: the interference fringe period of the interference field in the planar holographic grating exposure device can be adjusted quickly and accurately, and the interference fringe period can be accurately transferred to the grating substrate coated with photoresist, thereby greatly improving the performance of the planar holographic grating The precision of the grating constant. the

附图说明Description of drawings

图1是已有技术中平面全息光栅曝光装置光路结构及干涉条纹调整示意图; Figure 1 is a schematic diagram of the optical path structure and interference fringe adjustment of a planar holographic grating exposure device in the prior art;

图2是本发明中平面全息光栅曝光装置光路结构及零级光定位装置示意图; Fig. 2 is a schematic diagram of the optical path structure of the planar holographic grating exposure device and the zero-order light positioning device in the present invention;

图3是从图2所示光路中去掉第五平面反射镜8、第六平面反射镜9和标准机刻反射光栅11后所形成的干涉光路及零级光定位装置示意图; Fig. 3 is from the optical path shown in Fig. 2 and removes the interference optical path and the zero-order light positioning device schematic diagram formed after the fifth plane reflector 8, the sixth plane reflector 9 and the standard machine-engraved reflective grating 11;

图4是在图3所示光路中去掉半反半透镜10、接收屏12和第一分划板14,将待制作光栅基底16置入干涉场并进行零级光定位示意图。 FIG. 4 is a schematic diagram of removing the half-mirror 10, the receiving screen 12 and the first reticle 14 in the optical path shown in FIG. 3, placing the grating substrate 16 to be fabricated into the interference field and performing zero-order light positioning. the

具体实施方式Detailed ways

本发明按图1、2、3、4所示光路结构和按上述步骤一、步骤二、步骤三、步骤四方法步骤实施,激光光源1采用氪离子激光器,波长为413.1nm,第一平面反射镜2、第二平面反射镜3、第三平面反射镜6、第四平面反射镜7、第五平面反射镜8和第六平面反射镜9均为玻璃基底镀铝反射镜,空间滤波器4由显微物镜和针孔组成,准直反射镜5的口径为φ320mm、焦距为1.2m,半反半透镜10为薄的半反射半透射分束镜片,标准机刻反射光栅11的刻线密度及尺寸根据需要选择,接收屏12采用普通白色毛玻璃,监测激光器13采用He-Ne激光器,出射波长为632.8nm,第一分划板14和第二分划板15为透明标有十字刻度的圆板,光栅基底16采用K9光学玻璃,K9光学玻璃上涂敷的光致抗蚀剂为日本产的Shipley 1805型光致抗蚀剂。 The present invention is implemented according to the optical path structure shown in Figures 1, 2, 3, and 4 and by the method steps of the above-mentioned steps 1, 2, 3, and 4. The laser light source 1 adopts a krypton ion laser with a wavelength of 413.1 nm, and the first plane reflection The mirror 2, the second plane mirror 3, the third plane mirror 6, the fourth plane mirror 7, the fifth plane mirror 8 and the sixth plane mirror 9 are all aluminum-plated mirrors on glass substrates, and the spatial filter 4 Composed of a microscopic objective lens and a pinhole, the diameter of the collimating mirror 5 is φ320mm, the focal length is 1.2m, the semi-reflective half-mirror 10 is a thin semi-reflective and semi-transmissive beam-splitting lens, and the standard machine-engraved reflective grating 11 has a groove density The receiving screen 12 is made of ordinary white frosted glass, the monitoring laser 13 is made of He-Ne laser, the output wavelength is 632.8nm, the first reticle 14 and the second reticle 15 are transparent circles marked with a cross Plate, the grating substrate 16 adopts K9 optical glass, and the photoresist coated on the K9 optical glass is Shipley 1805 type photoresist produced in Japan. the

Claims (1)

1.平面全息光栅制作中光栅基底的零级光定位方法,该方法是利用平面全息光栅曝光装置实现的,其特征在于:步骤一,配备一套平面全息光栅曝光装置,包括激光光源(1)、第一平面反射镜(2)、第二平面反射镜(3)、空间滤波器(4)、准直反射镜(5)、第三平面反射镜(6)、第四平面反射镜(7)、第五平面反射镜(8)、第六平面反射镜(9)、半反半透镜(10)、标准机刻反射光栅(11)和接收屏(12);激光光源(1)发出的光束经第一平面反射镜(2)和第二平面反射镜(3)反射,再经空间滤波器(4)扩束滤波后成为球面波,球面波经准直反射镜(5)准直后成为平行光,在平行光光路里放置第五平面反射镜(8)引出一束平行光,再经第六平面反射镜(9)反射后到达半反半透镜(10),调整第六平面反射镜(9)使通过半反半透镜(10)的反射光和透射光均以自准直衍射角入射到标准机刻反射光栅(11)上,这两束光经标准机刻反射光栅(11)的±1级自准直衍射后,各自按它们的入射方向原路返回,再经半反半透镜(10)之后,-1级的反射光和+1级的透射光在半反半透镜(10)的另一侧重叠,在接收屏(12)上能够观察到铅直并清晰可见的干涉条纹;步骤二,在平面全息光栅曝光装置中,在正对标准机刻反射光栅(11)的一侧置有监测激光器(13),在监测激光器(13)的出射光路前方置有第一分划板(14),监测激光器(13)的出射光束穿过第一分划板(14)中心正入射到标准机刻反射光栅(11)上,零级衍射光原路返回第一分划板(14)中心;步骤三,从平面全息光栅曝光装置光路结构及零级光定位装置中取下标准机刻反射光栅(11)、第五平面反射镜(8)和第六平面反射镜(9),并确保半反半透镜(10)、接收屏(12)、监测激光器(13)和第一分划板(14)的位置不变,这时调节放置在平行光光路中的第三平面反射镜(6)和第四平面反射镜(7)的反射光分别经半反半透镜(10)透射和反射后叠加,使接收屏(12)上的干涉条纹的方向和数量分别与标准机刻反射光栅(11)所产生的干涉条纹相同,在监测激光器(13)的出射光束的传播方向上半反半透镜(10)的另一侧远处放置第二分划板(15),使监测激光器(13)的出射光束穿过第二分划板(15)的中心,这时将监测激光器(13)移到第二分划板(15)后方并使其出射光束先后通过第二分划板(15)和第一分划板(14)的中心;步骤四,取下半反半透镜(10)、接收屏(12)和第一分划板(14),将涂有光刻胶的待制作光栅基底(16)放置到标准机刻反射光栅(11)的位置,光栅基底(16)的装卡具安装在能够调整旋转、俯仰的精密调整台上,调整光栅基底(16)使监测激光器(13)的出射光束经光栅基底(16)的反射光原路返回第二分划板(15)的中心,此时进行曝光就能制作出具有标准光栅常数的平面全息光栅。1. The zero-order light positioning method of the grating substrate in the production of a planar holographic grating, which is realized by using a planar holographic grating exposure device, and is characterized in that: step 1, a set of planar holographic grating exposure devices is equipped, including a laser light source (1) , the first plane mirror (2), the second plane mirror (3), the spatial filter (4), the collimating mirror (5), the third plane mirror (6), the fourth plane mirror (7 ), the fifth plane reflector (8), the sixth plane reflector (9), half mirror (10), standard machine-engraved reflective grating (11) and receiving screen (12); the laser light source (1) sends The light beam is reflected by the first plane mirror (2) and the second plane mirror (3), and then beam expanded and filtered by the spatial filter (4) to become a spherical wave, and the spherical wave is collimated by the collimating mirror (5) Become parallel light, place the fifth plane reflector (8) in the parallel light path to draw a bunch of parallel light, then reach the half-mirror half mirror (10) after being reflected by the sixth plane reflector (9), adjust the sixth plane reflection The mirror (9) makes the reflected light and the transmitted light through the half-mirror (10) incident on the standard machine-engraved reflective grating (11) at a self-collimated diffraction angle, and the two beams of light pass through the standard machine-engraved reflective grating (11 ) after the ±1-order self-collimation diffraction, respectively return by their original path of incident direction, and then through the half mirror (10), the reflected light of -1 order and the transmitted light of +1 order are in the half mirror The other side of (10) overlaps, and can observe vertical and clearly visible interference fringes on the receiving screen (12); Step 2, in the planar holographic grating exposure device, engrave the reflective grating (11) on the standard machine One side of the monitoring laser (13) is equipped with a monitoring laser (13), and the first reticle (14) is placed in front of the exit light path of the monitoring laser (13), and the outgoing light beam of the monitoring laser (13) passes through the first reticle (14) ) center is incident on the standard engraved reflective grating (11), and the zero-order diffracted light returns to the center of the first reticle (14) in the original path; Step 3, from the optical path structure of the planar holographic grating exposure device and the zero-order light positioning device Remove the standard machine-engraved reflective grating (11), the fifth flat mirror (8) and the sixth flat mirror (9), and ensure that the half mirror (10), receiving screen (12), monitoring laser (13) And the position of the first reticle (14) is constant, at this moment adjust the reflected light of the 3rd plane reflector (6) and the 4th plane reflector (7) that is placed in the parallel light path through the semi-reflection half mirror respectively (10) superposition after transmission and reflection, so that the direction and quantity of the interference fringes on the receiving screen (12) are identical with the interference fringes produced by the standard machine-engraved reflective grating (11) respectively, and the output beam of the monitoring laser (13) Place the second reticle (15) far away on the other side of the semi-anti-half mirror (10) in the propagation direction, so that the outgoing light beam of the monitoring laser (13) passes through the center of the second reticle (15), at this time Move the monitoring laser (13) to the second reticle (15) rear and make its outgoing light beam pass through the center of the second reticle (15) and the first reticle (14) successively; Step 4, Take off the half mirror (10), receiving screen (12) and the first reticle (14), the grating base (16) to be made that is coated with photoresist is placed on the position of the standard machine engraved reflective grating (11), The mounting fixture of the grating base (16) is installed on a precision adjustment platform capable of adjusting rotation and pitch, and the grating base (16) is adjusted so that the outgoing light beam of the monitoring laser (13) returns to the first path through the reflected light of the grating base (16). The center of the reticle (15) is exposed at this time to produce a planar holographic grating with a standard grating constant.
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