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CN112596139A - Grating structure writing method of short-wave range reflection type volume grating - Google Patents

Grating structure writing method of short-wave range reflection type volume grating Download PDF

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CN112596139A
CN112596139A CN202011502556.2A CN202011502556A CN112596139A CN 112596139 A CN112596139 A CN 112596139A CN 202011502556 A CN202011502556 A CN 202011502556A CN 112596139 A CN112596139 A CN 112596139A
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grating
wavelength
ptr glass
exposure
short
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晋云霞
孙静
孔钒宇
何冬兵
邵建达
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Shanghai Institute of Optics and Fine Mechanics of CAS
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    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/18Diffraction gratings
    • G02B5/1847Manufacturing methods
    • G02B5/1857Manufacturing methods using exposure or etching means, e.g. holography, photolithography, exposure to electron or ion beams

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Abstract

The invention provides a grating structure writing method of a short-wave range reflection type volume grating. The method comprises a prism coupling exposure method and a correlation exposure method. The central wavelength of the reflection type volume grating prepared by the grating structure writing method can reach 325nm to 650 nm. The method provided by the invention provides a new idea for the development of the short-wavelength reflective volume grating, and compared with the existing preparation technology, the method widens the technical field of short wavelength, and has great practical application value in the fields of semiconductor laser wave locking, laser beam combination and the like.

Description

Grating structure writing method of short-wave range reflection type volume grating
The technical field is as follows:
the invention relates to a method for preparing a diffraction optical element, in particular to a grating structure writing method of a short-wave reflection type volume grating based on photorefractive glass.
Background art:
the semiconductor laser has the advantages of high efficiency, small volume, long service life, low cost and the like, and is widely applied to the fields of measurement, communication and the like. However, the conventional semiconductor laser has the problems of wide line width, easy drift of wavelength along with the change of temperature and the like, and the narrow-bandwidth frequency stabilization semiconductor laser plays a critical role in the research and development of high-tech products and basic research, so the narrow-bandwidth frequency stabilization semiconductor laser is particularly important for the research and development of the line width voltage and the frequency stabilization technology of the semiconductor laser. In recent years, a reflective volume grating based on PTR glass has the characteristics of excellent reflection efficiency, strong Bragg wavelength selection and angle selection, and is widely applied to line width narrowing and wavelength locking in semiconductor laser as an external cavity technical means.
With the continuous development and breakthrough of semiconductor laser technology, semiconductor lasers are gradually developing towards short wavelengths and high powers. Short wavelength reflective bulk gratings are in great demand, and the current preparation systems: the Luoerio mirror interference system and the double-beam interference system have relatively mature preparation of the reflective gratings of visible and infrared wave bands. There are also difficulties in short wavelength fabrication due to limitations in the exposure wavelength and the absorption line of the PTR. Zhang Xiaofu, Chenyi et al propose "preparation method of multi-wavelength volume Bragg grating", but the shortest used wavelength can only reach 432nm [ patent No CN104133267A ], and preparation method of reflection type volume grating with shorter wavelength is not related in relevant documents and patents. The invention provides a grating writing method of a short-wave reflection type volume grating, which can realize the preparation of the reflection type volume grating with the wavelength of 325nm to 650 nm.
The invention content is as follows:
the invention provides a grating writing method of a short wave reflection type volume grating, namely a prism coupling exposure method and a correlation exposure method. The wavelength of the reflective volume grating prepared by adopting the prism coupling exposure method can be 375nm-650nm, and the preparation of the reflective volume grating with shorter wavelength of 325nm-378nm can be realized by adopting the correlation exposure method.
The technical solution of the invention is as follows:
1. a prism coupled exposure method, the method comprising the steps of:
setting the exposure wavelength lambda of the PTR glass to be exposedExposure methodRefractive index of1Using the wavelength λ at the gratingMake itRefractive index ofavThe exposure angle of two ultraviolet parallel lights in the PTR glass is theta0Exposure to lightWavelength lambdaExposure methodThe wavelength of two beams of ultraviolet parallel light for exposing the PTR glass to be exposed is determined;
polishing the upper surface and the lower surface of the PTR glass to be exposed respectively to form a light-transmitting incident surface and a light-transmitting emergent surface;
making a base angle theta2Isosceles triangular prism of, and theta2=θ0Two isosceles surfaces of the isosceles triangular prisms are respectively plated with an ultraviolet antireflection film, and the isosceles triangular prisms (1) are exposed at an exposure wavelength lambdaExposure methodRefractive index of2And n is2≈n1The bottom surface of the isosceles prism is matched with the size of the upper surface of the PTR glass;
adhering the incident surface of the bottom surface PTR glass of the isosceles prism with matching liquid, and adhering the emergent surface of the PTR glass with the black light absorption sheet; the refractive index n of the matching fluid3And n is3=n1
Two ultraviolet parallel lights vertically enter the two waists of the prism, and generate interference on the entrance surface or inside of the PTR glass.
The exposure angle theta0In the range of 30 DEG to 60 DEG, the grating of said reflective volume grating using a wavelength lambdaMake itIn the range of 375nm to 650 nm.
2. A correlation exposure method, the method comprising the steps of:
let us assume that the grating of the PTR glass to be exposed uses a wavelength lambdaMake itRefractive index n ofavTwo ultraviolet parallel lights at incident angle theta1Obliquely incident on the PTR glass and generating interference in the PTR glass, and the exposure angle is theta0
Polishing two incidence surfaces of the PTR glass to be exposed and plating an ultraviolet anti-reflection film to form a light-passing surface;
the exposure angle theta0In the range of 60 DEG to 90 DEG, the grating of said reflective volume grating using a wavelength lambdaMake itIn the range of 325nm to 378 nm.
The invention has the advantages that:
1. compared with the known reflective bulk grating preparation technology, the method provided by the invention can be used for preparing the reflective bulk grating with shorter wavelength.
2. The method provided by the invention has the advantages of simple structure, easiness in operation and capability of realizing batch production. The prism is easy to process, low in cost, stable in structure and easy to fix, and can ensure the stability of grating writing in the exposure process.
Drawings
FIG. 1 is a schematic view of prism coupling exposure
FIG. 2 is a schematic diagram of a correlation exposure, in which a is a schematic diagram of an exposure method and b is a schematic diagram of an exposure principle
Detailed Description
The following detailed description of the embodiments of the present invention is provided with reference to specific examples and drawings, but the present invention is not limited to the description of the embodiments and the scope of the present invention.
1. A prism coupled exposure method, the method comprising the steps of:
(1) two beams of ultraviolet parallel light 2,3 are provided for exposing the grating write medium PTR glass 9 at an exposure wavelength λExposure method
(2) Polishing the upper surface and the lower surface of PTR glass 9 to be exposed respectively to form a light-transmitting incident surface 8 and a light-transmitting emergent surface 10, wherein the PTR glass 9 is exposed at an exposure wavelength lambdaExposure methodRefractive index of1Using the wavelength λ at the gratingMake itRefractive index ofav
(3) Selecting a base angle of theta2The isosceles prism 1, two equal waist surfaces 4,5 of the isosceles prism 1 are respectively plated with a layer of ultraviolet antireflection film, and the ultraviolet antireflection film is coated at the exposure wavelength lambdaExposure methodThe refractive index of the lower triangular prism is n2Requiring exposure at an exposure wavelength λExposure methodRefractive index n of lower triangular prism 12Refractive index n of PTR glass 91Close to, i.e. n2≈n1The base 6 of the prism 1 is matched in size to the upper surface 8 of the PTR glass 9;
(4) the bottom face 6 of the prism 1 is bonded to the incident face 8 of the PTR glass 9 using a matching fluid 7, the refractive index of the matching fluid 7 being n, the refractive index of the PTR glass 91The same is true. The exit surface 10 of the PTR glass 9 was coated with a black ink using a matching fluid 7A light sheet 11;
(5) two ultraviolet parallel lights 2,3 are emitted at an incident angle theta1The light perpendicularly enters the two waists 4,5 of the prism 1 at 90 DEG, and interferes with the incident surface 8 or the inside of the PTR glass 9 at an exposure angle theta0. According to a geometric relationship, the exposure angle theta0Base angle theta with triangular prism2Equal, i.e. theta0=θ2. According to the fringe period generated by the interference of the two parallel lights 2 and 3 and the relationship between the used wavelength and the period of the volume grating, the following results are obtained:
Figure BDA0002844046840000031
the method is implemented by changing the exposure angle theta0I.e. base angle theta of the prism2And the reflective type volume grating with different wavelengths can be prepared. Taking into account the exposure angle theta0Within a reasonable range, the exposure angle can be between 30 and 60 degrees, and the wavelength of the reflective bulk grating prepared by the method can reach 375 to 650 nm.
2. A correlation exposure method, the method comprising the steps of:
(1) two incident surfaces 8 of the PTR glass 9 are respectively polished and plated with a layer of ultraviolet antireflection film to form a light transmitting surface, and the PTR glass uses the wavelength lambda of the gratingMake itRefractive index n ofav
(2) Two ultraviolet parallel lights 2,3 are set at an incident angle theta1To the light-passing surface 8 of the PTR glass 9 and to generate interference inside the PTR glass with an exposure angle theta0From the refractive index formula, θ0=90°-arcsin(sinθ1/nav);
(3) According to the fringe period generated by the interference of the two parallel lights 2 and 3 and the relationship between the used wavelength and the period of the volume grating, the following results are obtained:
Figure BDA0002844046840000041
the wavelength of the reflective volume grating that can be produced by this method can be 325nm to 378nm, taking into account that the exposure angle is within a reasonable range.
Example 1: the prism coupling exposure method for preparing the reflection type volume grating with the wavelength of 450 +/-0.5 nm comprises the following specific steps:
(1) providing parallel ultraviolet light 2,3 with an exposure wavelength lambdaExposure method=325nm。
(2) Polishing the incident surface 8 and the exit surface 10 of the PTR glass 9 to be exposed, the refractive index of the PTR glass 9 at an exposure wavelength of 325nm being n11.528, refractive index n at a grating use wavelength of 450nmav=1.512
(3) Calculating an exposure angle θ0Is 45.6 degrees. Selecting base angle theta2An isosceles prism 1 of 45.6 DEG and having a refractive index n21.528, two equal waist surfaces 4 and 5 of the triangular prism 1 are plated with a 325nm ultraviolet antireflection film, and the 325nm transmittance is increased.
(3) The bottom edge 6 of the triangular prism is bonded with the PTR glass incidence surface 8 by using matching fluid 7, so that light reflection at the interface is prevented, and meanwhile, the PTR glass emergence surface 10 is pasted with a black light absorbing sheet 11, so that Fresnel diffraction is prevented.
(4) Two beams of 325nm parallel ultraviolet light 2,3 are respectively emitted at an incidence angle theta1When the light enters the two equi- waisted surfaces 4,5 of the prism perpendicularly at 90 °, interference occurs between the incident surface 8 of the PTR glass 9 and the inside of the body, and the PTR glass is exposed to a certain dose of ultraviolet light and then the exposure is stopped.
(5) And (3) preparing a reflective type body grating initial sample through subsequent heat treatment and cutting, testing the central wavelength of the reflective type body grating initial sample, and continuously performing operation adjustment on the steps (3) to (5) to test the exposure angle and the central wavelength so as to enable the central wavelength to fall in a required range.
Example 2: and preparing the reflective volume grating with the central wavelength of 376 +/-0.5 nm by using a correlation exposure mode.
(1) Both incident faces 8 of the PTR glass 9 to be exposed are polished.
(2) Refractive index n of PTR glass 9 at a use wavelength of 376nmavCalculate exposure angle θ as 1.520Is 59.8 degrees, and the incident angle theta is obtained according to the refraction fixed rate1=49.85°。
(3) Make itUsing two beams of ultraviolet parallel light 2,3 in theta1This was made incident on the PTR glass 9 at an angle of 49.85 °, and after exposure to a dose of uv light, the exposure was stopped.
(4) And (3) preparing a reflective type body grating initial sample through subsequent heat treatment and cutting, testing the central wavelength of the reflective type body grating initial sample, and continuously performing operation adjustment on the steps (2) to (4) to test the exposure angle and the central wavelength so as to enable the central wavelength to fall in a required range.
The method of the invention changes the exposure angle theta0The method provided by the invention can relate to the preparation of 325nm short-wave reflective body gratings, widens the technical field of short-wave reflective body gratings, has the advantages of simple structure, easy operation, contribution to mass production and good practical prospect in the fields of laser beam combination, spatial filtering, laser wave locking and the like.

Claims (4)

1.一种短波范围反射式体光栅的光栅结构写入方法,其特征在于,该方法包括步骤如下:1. a grating structure writing method of short-wave range reflective volume grating, is characterized in that, this method comprises the steps as follows: ①设待曝光的PTR玻璃(9)在曝光波长λ下的折射率为n1,在光栅使用波长λ使下的折射率为nav,两束紫外平行光(2,3)在PTR玻璃(9)内的曝光角度为θ0,曝光波长λ为两束对待曝光的PTR玻璃(9)进行曝光的紫外平行光(2,3)的波长;① Let the refractive index of the PTR glass (9) to be exposed at the exposure wavelength λ be n 1 , and the refractive index at the wavelength λ of the grating be n av , and the two beams of ultraviolet parallel light (2, 3) are exposed to the PTR glass. The exposure angle in (9) is θ 0 , and the exposure wavelength λ is the wavelength of the ultraviolet parallel light (2, 3) for exposing the PTR glass (9) to be exposed; ②将待曝光的PTR玻璃(9)的上表面与下表面分别进行抛光处理,形成通光的入射面(8)与出射面(10);② The upper surface and the lower surface of the PTR glass (9) to be exposed are polished respectively to form a light-transmitting incident surface (8) and an exit surface (10); ③制作一底角为θ2的等腰三棱镜(1),且θ2=θ0,该等腰三棱镜(1)的两等腰面(4,5)分别镀制有紫外增透膜,该等腰三棱镜(1)在曝光波长λ下的折射率为n2,且n2≈n1,所述等腰三棱镜(1)的底面(6)与PTR玻璃(9)的上表面(8)尺寸匹配;③ Make an isosceles prism (1) with a base angle of θ 2 , and θ 20 , the two isosceles surfaces (4, 5) of the isosceles prism (1) are respectively coated with an ultraviolet antireflection coating, the The refractive index of the isosceles prism (1) under the exposure wavelength λ is n 2 , and n 2 ≈ n 1 , the bottom surface (6) of the isosceles prism (1) and the upper surface (8) of the PTR glass (9) ) size matching; ④利用匹配液(7)使所述的等腰三棱镜(1)的底面(6)与PTR玻璃(9)的入射面(8)粘合,PTR玻璃(9)的出射面(10)与黑色吸光片(11)粘合;所述的匹配液(7)的折射率n3,且n3=n1④ Use the matching liquid (7) to bond the bottom surface (6) of the isosceles prism (1) with the incident surface (8) of the PTR glass (9), and the exit surface (10) of the PTR glass (9) with black The light-absorbing sheet (11) is bonded; the refractive index of the matching liquid (7) is n 3 , and n 3 =n 1 ; ⑤两束紫外平行光(2,3)垂直入射到三棱镜(1)的两等腰面(4,5)上,在PTR玻璃(9)入射面(8)或者内部产生干涉。⑤ The two beams of ultraviolet parallel light (2, 3) are vertically incident on the two isosceles surfaces (4, 5) of the triangular prism (1), and interference occurs on the incident surface (8) or the interior of the PTR glass (9). 2.根据权利要求1所述的短波范围反射式体光栅的光栅结构写入方法,其特征在于,所述的曝光角度θ0的范围为30°-60°,所述的反射式体光栅的光栅使用波长λ使的范围为375nm-650nm。2. The grating structure writing method of the short-wave range reflective volume grating according to claim 1, wherein the range of the exposure angle θ 0 is 30°-60°, and the The grating uses wavelength λ in the range of 375nm-650nm. 3.一种短波范围反射式体光栅的光栅结构写入方法,其特征在于,该方法包括步骤如下:3. A method for writing a grating structure of a short-wave range reflective volume grating, characterized in that the method comprises the following steps: ①设待曝光的PTR玻璃(9)的光栅使用波长λ使处的折射率nav,两束紫外平行光(2,3)以入射角θ1斜入射到所述的PTR玻璃(9)上,并在PTR玻璃内部产生干涉,曝光角度为θ0① Assume that the grating of the PTR glass (9) to be exposed uses the refractive index n av at the wavelength λ, and the two beams of ultraviolet parallel light (2, 3) are obliquely incident on the PTR glass (9) at the incident angle θ 1 , and interference occurs inside the PTR glass, and the exposure angle is θ 0 ; ②将待曝光的PTR玻璃(9)的两入射面(8)进行抛光并镀制紫外增透膜,形成通光面。② Polishing and coating the two incident surfaces (8) of the PTR glass (9) to be exposed with an ultraviolet anti-reflection film to form a light-transmitting surface. 4.根据权利要求3所述的短波范围反射式体光栅的光栅结构写入方法,其特征在于,所述的曝光角度θ0的范围为60°-90°,所述的反射式体光栅的光栅使用波长λ使的范围为325nm-378nm。4. The grating structure writing method of the short-wave range reflective volume grating according to claim 3, wherein the range of the exposure angle θ 0 is 60°-90°, and the reflective volume grating has a The grating uses wavelength λ in the range of 325nm-378nm.
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113904213A (en) * 2021-12-08 2022-01-07 杭州拓致光电科技有限公司 Multi-wavelength wave locker based on photo-thermal conversion glass and preparation method thereof
CN114089469A (en) * 2022-01-20 2022-02-25 深圳珑璟光电科技有限公司 Volume holographic optical waveguide, manufacturing method thereof and color volume holographic optical waveguide

Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1147096A (en) * 1995-09-01 1997-04-09 清华大学 Method for making fibre-optic Bragg raster prism
JPH09153446A (en) * 1995-11-30 1997-06-10 Sharp Corp Method and apparatus for interference exposure
US20020045104A1 (en) * 2000-01-04 2002-04-18 Efimov Oleg M. High efficiency volume diffractive elements in photo-thermo-refractive glass
CN1424829A (en) * 2002-12-13 2003-06-18 北京工业大学 Stage linked body holographic grating intensive WDM implement manufacture and system thereof
CN1564400A (en) * 2004-04-09 2005-01-12 浙江大学 Pump method of realizing feedback pregue first class laser output of gain raster distribution
CN101963761A (en) * 2009-07-22 2011-02-02 电子科技大学 Surface plasmon (SPP)-based large-area interference lithography technology
CN104483725A (en) * 2014-12-29 2015-04-01 中国科学院长春光学精密机械与物理研究所 Grating exposure system adopting aspherical single lens as collimation structure
CN206400263U (en) * 2017-01-19 2017-08-11 兰州理工大学 Sub-wavelength structure preparation device for surface plasmon multiple interference exposure
US10509327B1 (en) * 2018-07-24 2019-12-17 Facebook Technologies, Llc Variable neutral density filter for multi-beam interference lithography exposure
CN110879433A (en) * 2019-11-25 2020-03-13 中国科学院上海光学精密机械研究所 A method for fabricating reflective volume grating based on photothermal refractive glass
CN110967785A (en) * 2019-12-13 2020-04-07 厦门大学 A method for preparing holographic grating with small duty ratio by means of holographic interference recording

Patent Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1147096A (en) * 1995-09-01 1997-04-09 清华大学 Method for making fibre-optic Bragg raster prism
JPH09153446A (en) * 1995-11-30 1997-06-10 Sharp Corp Method and apparatus for interference exposure
US20020045104A1 (en) * 2000-01-04 2002-04-18 Efimov Oleg M. High efficiency volume diffractive elements in photo-thermo-refractive glass
CN1424829A (en) * 2002-12-13 2003-06-18 北京工业大学 Stage linked body holographic grating intensive WDM implement manufacture and system thereof
CN1564400A (en) * 2004-04-09 2005-01-12 浙江大学 Pump method of realizing feedback pregue first class laser output of gain raster distribution
CN101963761A (en) * 2009-07-22 2011-02-02 电子科技大学 Surface plasmon (SPP)-based large-area interference lithography technology
CN104483725A (en) * 2014-12-29 2015-04-01 中国科学院长春光学精密机械与物理研究所 Grating exposure system adopting aspherical single lens as collimation structure
CN206400263U (en) * 2017-01-19 2017-08-11 兰州理工大学 Sub-wavelength structure preparation device for surface plasmon multiple interference exposure
US10509327B1 (en) * 2018-07-24 2019-12-17 Facebook Technologies, Llc Variable neutral density filter for multi-beam interference lithography exposure
CN110879433A (en) * 2019-11-25 2020-03-13 中国科学院上海光学精密机械研究所 A method for fabricating reflective volume grating based on photothermal refractive glass
CN110967785A (en) * 2019-12-13 2020-04-07 厦门大学 A method for preparing holographic grating with small duty ratio by means of holographic interference recording

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113904213A (en) * 2021-12-08 2022-01-07 杭州拓致光电科技有限公司 Multi-wavelength wave locker based on photo-thermal conversion glass and preparation method thereof
CN114089469A (en) * 2022-01-20 2022-02-25 深圳珑璟光电科技有限公司 Volume holographic optical waveguide, manufacturing method thereof and color volume holographic optical waveguide
CN114089469B (en) * 2022-01-20 2022-05-06 深圳珑璟光电科技有限公司 Volume holographic optical waveguide, manufacturing method thereof and color volume holographic optical waveguide

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