CN1725042B - Scanning Grating Writing Method Based on Talbot Interferometer and Scanning Talbot Interferometer - Google Patents
Scanning Grating Writing Method Based on Talbot Interferometer and Scanning Talbot Interferometer Download PDFInfo
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Abstract
本发明涉及一种基于Talbot干涉仪的扫描式光栅写入方法及扫描式Talbot干涉仪,属光学技术领域。使用Talbot干涉仪,使入射光束依次经过反射、衍射、反射后,在光纤上形成干涉条纹,同时使形成的干涉条纹沿光纤水平移动,从而在光纤上扫描写入光栅。扫描式Talbot干涉仪由平面镜、水平平移台、相位掩模、零级阻断遮光板,以及垂直平移台及固定在其上的光纤组成。具有可方便地调谐写入的Bragg波长、对写入光源的脉冲能量和相干性要求低,Talbot干涉仪的平面镜的长度小等优点。The invention relates to a scanning grating writing method based on a Talbot interferometer and a scanning Talbot interferometer, belonging to the field of optical technology. Using a Talbot interferometer, the incident beam is reflected, diffracted, and reflected in sequence to form interference fringes on the optical fiber, and at the same time, the formed interference fringes are moved horizontally along the optical fiber to scan and write the grating on the optical fiber. The scanning Talbot interferometer consists of a plane mirror, a horizontal translation stage, a phase mask, a zero-order blocking mask, a vertical translation stage and an optical fiber fixed on it. It has the advantages of conveniently tuning the Bragg wavelength for writing, low requirements on the pulse energy and coherence of the writing light source, and the small length of the plane mirror of the Talbot interferometer.
Description
技术领域:本发明涉及一种基于Talbot干涉仪的扫描式光栅写入方法及扫描式Talbot干涉仪,属光学技术领域。Technical field: The present invention relates to a scanning grating writing method based on a Talbot interferometer and a scanning Talbot interferometer, belonging to the field of optical technology.
技术背景:自从1993年,K.O.Hill等人首次验证了光纤被直接放置于经相位掩模衍射而产生的紫外近场干涉区,该写入方法已广泛应用于制作光纤光栅。但在相位掩模的接触式写入法中,光纤光栅的写入Bragg波长对应于相位掩模的光栅周期,Bragg波长不能够根据需要变化。为使写入的Bragg波长能够改变并大于2nm,有一种Talbot干涉仪,通过调整平面镜的角度实现改变光纤光栅的写入波长;但这种Talbot干涉仪写入的光栅长度受限于平面镜的长度和写入光源的相干性,制作窄带宽的光栅往往需要较长的平面镜(满足紫外干涉的>60mm的平面镜难以制作),写入光栅对紫外光束的脉冲能量密度要求也高(如写制I型光栅,能量密度必须>100mJ/cm2/pulse,累积能量密度必须>500J/cm2);此外,光源的相干性对写入光栅的影响也较大。Technical background: Since 1993, KOHill et al. verified for the first time that the optical fiber was directly placed in the ultraviolet near-field interference region generated by phase mask diffraction, and this writing method has been widely used in the production of fiber gratings. However, in the contact writing method of the phase mask, the writing Bragg wavelength of the fiber grating corresponds to the grating period of the phase mask, and the Bragg wavelength cannot be changed as required. In order to change the written Bragg wavelength and be greater than 2nm, there is a Talbot interferometer, which can change the writing wavelength of the fiber grating by adjusting the angle of the plane mirror; but the length of the grating written by this Talbot interferometer is limited by the length of the plane mirror With the coherence of the writing light source, making a narrow-bandwidth grating often requires a longer plane mirror (it is difficult to make a >60mm plane mirror that satisfies ultraviolet interference), and writing a grating has high requirements for the pulse energy density of the ultraviolet beam (such as writing I type grating, the energy density must be >100mJ/cm 2 /pulse, and the cumulative energy density must be >500J/cm 2 ); in addition, the coherence of the light source also has a great influence on writing the grating.
发明内容:本发明的目的在于克服现有技术之不足,提供一种可方便地调谐写入的Bragg波长、对写入光源的脉冲能量和相干性要求低的基于Talbot干涉仪的扫描式光栅写入方法,以及用于该方法的扫描式Talbot干涉仪。Summary of the invention: The object of the present invention is to overcome the deficiencies of the prior art, to provide a scanning grating writing system based on a Talbot interferometer that can easily tune the written Bragg wavelength and have low requirements on the pulse energy and coherence of the writing light source. input method, and a scanning Talbot interferometer for this method.
本发明的技术方案是:该基于Talbot干涉仪的扫描式光栅写入方法,是使用Talbot干涉仪,使入射光束依次经过反射、衍射、反射后,在光纤上形成干涉条纹,同时使形成的干涉条纹沿光纤水平移动,从而在光纤上扫描写入光栅。The technical solution of the present invention is: the scanning grating writing method based on the Talbot interferometer is to use the Talbot interferometer to make the incident light beam undergo reflection, diffraction and reflection in sequence to form interference fringes on the optical fiber, and at the same time make the formed interference fringes The fringe is moved horizontally along the fiber, thereby scanning and writing the grating across the fiber.
采用具有水平平移台和垂直平移台结构的Talbot干涉仪,使入射光束依次通过水平平移台2上的平面镜1、支架上的相位掩模3、水平平移台2上的衍射反射镜5和6,以及遮光板4阻断相位掩模3所产生零级衍射光,进行反射、衍射、反射,在垂直平移台8上的光纤7上形成干涉条纹,同时水平移动水平平移台2,使干涉条纹沿光纤运动,在光纤上扫描写入光栅;也可使入射光束依次通过支架上的平面镜1、水平平移台2上的相位掩模3、支架上的衍射反射镜5和6,以及遮光板(4)阻断相位掩模(3)所产生零级衍射光,进行反射、衍射、反射,在固定在水平平移台2上的垂直平移台8上的光纤7上形成干涉条纹,同时水平移动水平平移台2,使干涉条纹沿光纤7运动,从而在光纤上扫描写入光栅。Using a Talbot interferometer with a horizontal translation stage and a vertical translation stage structure, the incident light beam passes through the
该扫描式光栅写入法所使用的扫描式Talbot干涉仪,由平面镜1、水平平移台2、相位掩模3、实现零级阻断的遮光板4、衍射反射镜5、衍射反射镜6,以及垂直平移台8及固定在其上的光纤7组成,相位掩模3位于平面镜1与衍射反射镜5、6之间,零级阻断遮光板4位于衍射反射镜5、6之间。根据扫描写入方式的需要,可采用将平面镜1、零级阻断遮光板4、衍射反射镜(平面镜)5、衍射反射镜(平面镜)6固定在水平平移台2上,相位掩模3由支架支撑,垂直平移台8与水平平移台2分离的结构,通过干涉条纹运动实现扫描式写入。也可采用将相位掩模3和垂直平移台8固定在水平平移台2上,平面镜1、衍射反射镜(平面镜)5、衍射反射镜(平面镜)6、零级阻断遮光板4由支架支撑,垂直平移台8放置于水平平移台2上的结构;水平平移台2做水平平移时,会带动垂直平移台8,从而使位于垂直平移台8上的光纤实现水平移动,实现扫描式写入。The scanning Talbot interferometer used in the scanning grating writing method consists of a
在该扫描式Talbot干涉仪中,5、6两个平面镜(衍射反射镜)的转动对改变光纤光栅的写入Bragg波长起着决定作用。根据反射原理,当反射平面镜的角度变化δ时,反射光束的方向变化Δ等于2δ。因此,当两平面镜相向旋转δ时,在给定Bragg条件下,Bragg响应波长为:In the scanning Talbot interferometer, the rotation of the two plane mirrors (diffraction mirrors) 5 and 6 plays a decisive role in changing the Bragg wavelength written in the fiber grating. According to the principle of reflection, when the angle of the reflective plane mirror changes δ, the direction of the reflected beam changes Δ equal to 2δ. Therefore, when the two plane mirrors rotate δ towards each other, under the given Bragg condition, the Bragg response wavelength is:
同时,若5、6两平面镜(衍射反射镜)的旋转轴与入射的±1级衍射光束的重合,则两写入干涉光束的干涉区的菱脊将移动到:At the same time, if the rotation axes of the two plane mirrors (diffraction mirrors) of 5 and 6 coincide with the incident ±1st-order diffracted beams, the ridges of the interference area of the two writing interference beams will move to:
ΔL=(Ws/2)[cot(θ/2+2δ)-cot(θ/2)] (2)ΔL=(W s /2)[cot(θ/2+2δ)-cot(θ/2)] (2)
因此,当扫描式Talbot干涉仪用于调谐写入光栅Bragg波长时,只要放置光纤的平移台8应作相应的平移就能使得待写光纤位于写入干涉区,即在光纤中写入光栅。Therefore, when the scanning Talbot interferometer is used to tune the Bragg wavelength of the writing grating, as long as the
本发明由于采用了可方便调节的运动结构和扫瞄式写入方式,因而较具有如下优点:Since the present invention adopts a conveniently adjustable movement structure and a scanning writing method, it has the following advantages:
1、能够根据需要方便地调节写入光栅Bragg的波长,且写入光栅的长度范围宽;1. The wavelength of the written grating Bragg can be easily adjusted according to the needs, and the length range of the written grating is wide;
2、大大减小了Talbot干涉仪中平面镜的长度,对平面镜的尺寸要求仅需大于激光光斑的大小(>1mm);2. The length of the plane mirror in the Talbot interferometer is greatly reduced, and the size of the plane mirror only needs to be larger than the size of the laser spot (> 1mm);
3、对光源相干长度的要求显著降低,降低了对写入光源相干性的要求;3. The requirements for the coherence length of the light source are significantly reduced, and the requirements for the coherence of the written light source are reduced;
4、显著降低了对激光脉冲能量的要求。4. Significantly reduces the requirement for laser pulse energy.
附图说明:下面结合附图和实施例对本发明作进一步说明。BRIEF DESCRIPTION OF THE DRAWINGS: The present invention will be further described below in conjunction with the accompanying drawings and embodiments.
图1为本发明干涉条纹运动型结构示意图,Fig. 1 is a schematic diagram of the structure of the interference fringe movement of the present invention,
图2为本发明光纤运动型结构示意图,Fig. 2 is a schematic diagram of the optical fiber movement structure of the present invention,
图3为本发明Bragg波长随平面镜旋转的角度变化的曲线图,Fig. 3 is the graph that Bragg wavelength of the present invention changes with the angle of plane mirror rotation,
图4为本发明两写入干涉光束的干涉区的菱脊移动随平面镜旋转的角度变化的曲线图。FIG. 4 is a graph showing the movement of the ridges in the interference region of the two writing interference beams as a function of the rotation angle of the plane mirror according to the present invention.
具体实施方式:Detailed ways:
例1:该基于Talbot干涉仪的扫描式光栅写入方法,是使用Talbot干涉仪,使入射光束依次经过反射、衍射、反射后,在光纤上形成干涉条纹,同时使形成的干涉条纹沿光纤水平移动,从而在光纤上扫描写入光栅。采用具有水平平移台和垂直平移台结构的Talbot干涉仪,使入射光束依次通过水平平移台上的平面镜、支架上的相位掩模、水平平移台上的衍射反射镜,以及插入遮光板4对相位掩模3产生的零级衍射光进行阻断,进行反射、衍射、反射,在垂直平移台上的光纤上形成干涉条纹,同时水平移动水平平移台,使干涉条纹沿光纤运动,在光纤上扫描写入光栅。Example 1: The scanning grating writing method based on the Talbot interferometer is to use the Talbot interferometer to make the incident beam undergo reflection, diffraction and reflection in sequence to form interference fringes on the optical fiber, and at the same time make the formed interference fringes along the horizontal direction of the optical fiber Move to scan and write the grating on the fiber. Using a Talbot interferometer with a horizontal translation stage and a vertical translation stage structure, the incident light beam passes through the plane mirror on the horizontal translation stage, the phase mask on the bracket, the diffraction mirror on the horizontal translation stage, and 4 pairs of phases inserted into the light shield The zero-order diffracted light generated by the
如图1所示,该扫描式光栅写入法所使用的扫描式Talbot干涉仪,由平面镜1、水平平移台2、相位掩模3、零级阻断遮光板4、衍射反射镜5和6,以及垂直平移台8及固定在其上的光纤7组成。平面镜1、零级阻断遮光板4、衍射反射镜(平面镜)5和6固定在水平平移台2上,相位掩模3由支架支撑,相位掩模3位于平面镜1与衍射反射镜5、6之间,零级阻断遮光板4位于衍射反射镜5、6之间,垂直平移台8与水平平移台2分离。As shown in Figure 1, the scanning Talbot interferometer used in the scanning grating writing method consists of a
工作时,通过水平平移台2同时带动其上起反射入射光束作用的平面镜1,和起反射±1级衍射光作用的两个平面镜5、6在水平方向做平移,使干涉条纹沿光纤7运动,从而扫描写入光栅。When working, the
例2:该基于Talbot干涉仪的扫描式光栅写入方法,是使用Talbot干涉仪,使入射光束依次经过反射、衍射、反射后,在光纤上形成干涉条纹,同时使形成的干涉条纹沿光纤水平移动,从而在光纤上扫描写入光栅。采用具有水平平移台和垂直平移台结构的Talbot干涉仪,使入射光束依次通过支架上的平面镜、水平平移台上的相位掩模、支架上的衍射反射镜,以及插入遮光板对相位掩模产生的零级衍射光进行阻断,进行反射、衍射、反射,在固定在水平平移台上的垂直平移台上的光纤上形成干涉条纹,同时水平移动水平平移台,使干涉条纹沿光纤运动,在光纤上扫描写入光栅。Example 2: The scanning grating writing method based on the Talbot interferometer is to use the Talbot interferometer to make the incident light beam undergo reflection, diffraction and reflection in sequence to form interference fringes on the optical fiber, and at the same time make the formed interference fringes along the horizontal direction of the optical fiber Move to scan and write the grating on the fiber. A Talbot interferometer with a horizontal translation stage and a vertical translation stage structure is used to make the incident beam pass through the plane mirror on the support, the phase mask on the horizontal translation stage, the diffraction mirror on the support, and insert the light shield to generate the phase mask. The zero-order diffracted light is blocked, reflected, diffracted, and reflected, and interference fringes are formed on the optical fiber fixed on the vertical translation stage on the horizontal translation stage. At the same time, the horizontal translation stage is moved horizontally to make the interference fringes move along the optical fiber. Scanning write gratings on fiber optics.
如图2所示,该扫描式光栅写入法所使用的扫描式Talbot干涉仪,由平面镜1、水平平移台2、相位掩模3、零级阻断遮光板4、衍射反射镜5和6,以及垂直平移台8及固定在其上的光纤7组成。相位掩模3和垂直平移台8固定在水平平移台2上,平面镜1、衍射反射镜(平面镜)5和6、零级阻断遮光板4由支架支撑,相位掩模3位于平面镜1与衍射反射镜5、6之间,零级阻断遮光板4位于衍射反射镜5、6之间,垂直平移台8放置于水平平移台2上。As shown in Figure 2, the scanning Talbot interferometer used in the scanning grating writing method consists of a
工作时,通过水平平移台2同时带动其上起衍射作用的相位掩模3,和待写入光栅的光纤7在水平方向做平移,使光纤沿干涉条纹运动,从而扫描写入光栅。When working, the
在该改变写入Bragg波长的扫描式Talbot干涉仪中,相位掩模的光栅周期Δpm是1084nm,当若紫外写入光束的波长λuv是248nm时,则±1级衍射光的衍射角θ/2=13.225°;两平面镜之间的间距Ws为10mm,作为公式(2)的结果,相位模板到写入干涉区的距离L为42.6mm;在光纤的纤芯中,有效反射率neff是1.46。In the scanning Talbot interferometer that changes the writing Bragg wavelength, the grating period Δpm of the phase mask is 1084nm, when the wavelength λuv of the ultraviolet writing beam is 248nm, the diffraction angle θ of the ±1st order diffracted light /2=13.225°; the distance W s between the two plane mirrors is 10mm, as a result of formula (2), the distance L from the phase template to the writing interference area is 42.6mm; in the core of the optical fiber, the effective reflectivity n eff is 1.46.
将上述数据代入公式(1),可得表示Bragg波长与5、6两平面镜角度变化关系的图3。与此同时,放置光纤的平移台8应按式(2)的规律进行平移才能使得待写光纤位于写入干涉区,两写入干涉光束的干涉区的菱脊移动随平面镜旋转的角度变化的曲线见图4。Substituting the above data into formula (1), we can get Figure 3, which shows the relationship between the Bragg wavelength and the angle change of the 5 and 6 plane mirrors. At the same time, the
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- 2005-06-30 CN CN200510010888.8A patent/CN1725042B/en not_active Expired - Fee Related
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RU2828253C1 (en) * | 2024-03-21 | 2024-10-08 | Открытое Акционерное Общество "Российские Железные Дороги" | Device for forming fibre bragg grating with possibility of tuning reflection wavelength |
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