CN1746721A - Optical bend and higher diffraction beam splitting method - Google Patents
Optical bend and higher diffraction beam splitting method Download PDFInfo
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- CN1746721A CN1746721A CN 200510010385 CN200510010385A CN1746721A CN 1746721 A CN1746721 A CN 1746721A CN 200510010385 CN200510010385 CN 200510010385 CN 200510010385 A CN200510010385 A CN 200510010385A CN 1746721 A CN1746721 A CN 1746721A
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Abstract
A method for splitting beam of photorefractive high order diffraction includes using two light beams to shine photorefractive material after two beams with coherence are crossed for forming interference fringe with light intensity distributed non-uniformly and for utilizing photorefractive effect to prepare beam splitting component, making beam spitting component generate Raman-Nath diffraction for realizing beam splitting, regulating included angle of two said light beams to let diffraction generate at this moment be Raman-Nath diffraction.
Description
Technical field
The present invention relates to photorefractive effect and optical beam splitting technical field.
Background technology
Optical beam splitting equipment is a kind of importing the optical device that light is divided into one dimension or two-dimensional array output beam or hot spot, widespread use in many fields of modern science and technology such as optical interconnection, photometry calculation, optical disc storage, photoelectric technology, Flame Image Process and precision measurement.Traditional optical beam splitting method is to utilize refraction-reflecting system, through repeatedly reflecting and reflecting a kind of beam-splitting method that obtains required optical field distribution.The shortcoming of this method (for example is the divided beam system complex structure, expect tens bundle light, then need to carry out repeatedly beam split), volume is big, energy loss is big, lack of homogeneity, when input optical power is very big, the plated film on the divided beam system element is burnt and damage etc. easily.
The binary optical beam-splitting method is a kind of pure position phase diffraction optical element, and it can convert beam of laser to the uniform laser beam array of intensity, also has functions such as multiple imaging, light interconnection, optically-coupled and light beam be compound.The binary optical beam-splitting method is especially noticeable owing to adopted new technology such as Computer Design and VLSI (very large scale integrated circuit) manufacturing process.At present, people have proposed the various structures and the algorithm of binary optical beam-splitting method, as with the Dammann grating of the method design of finding the solution Nonlinear System of Equations, ceasing grating mutually, have the Talbot beam-splitting optical grating of image effect of one's own and based on the phase-type Fresnel Lenses array of the paraxial diffraction theory of Fresnel zone plate etc. based on Talbot with the design of nonlinear optimization algorithms such as simulated annealing.According to the branch beam request in the practical application, can select the method for designing of various binary optical beam splitting.In today that computer technology develops rapidly, the optical beam-splitter that designs different purposes has not become difficulty, key is the technology making of binary optical beam splitting element, this binary optical beam-splitting method is subject to processing technology is that all right ripe restriction in actual applications, also has the restriction that applicable wavelengths is single, can not be used for the light beam of the information of carrying is carried out shortcomings such as beam splitting, cost height simultaneously.
When light transmission medium tilts to use, because electric field and the magnetic field tangential component on each interface is continuous, therefore the effective refractive index of p component and s component will produce polarization separation so inevitably with different, around this principle can make various polarization beam splitter prisms.Polarization beam splitter prism both had been different from the Nicol prism based on the birefringence principle, its o light and e light have a fixing shooting angle, be different from the polaroid that absorbs based on selectivity again, it has the characteristics of low-loss and design of Optical System dirigibility, thereby polarization beam splitter prism is widely used in the optoisolator and systems such as optical circulator, silicon liquid crystal light valve and fiber-Optic Voltage Sensors of TV projection system, Fiber Optical Communication System.But this polarization beam splitting method once can only be divided into two bundles to incident light, and has polarizability, can not realize multichannel output, and require oblique incidence, with many restrictions are arranged on Time Bandwidth and the angle.
Summary of the invention
In order to solve existing beam-splitting method or complex structure, the cost height, fragile beam splitting element, processing technology is immature, shortage is carried out the ability of beam splitting to the light beam that has information, the light beam of telling has the problem of polarizability, and then provide a kind of optical bend and higher diffraction beam splitting method, it mainly is to solve the beam splitting problem that runs in the optical information processing process, make the volume of beam splitting element reduce greatly, cost also reduces greatly, beam splitting quantity is improved, and the wavelength coverage that beam splitting element is suitable for increases, and installation process is simple when the equipment of needs that beam splitting element is packed into.
Optical bend and higher diffraction beam splitting method of the present invention carries out according to the following steps: one, preparation beam splitting element: the light beam that makes two bundles have the coherence intersects and is input to the light input end of Anaclasis variant, so in Anaclasis variant, form the uneven interference fringe of light distribution and utilize photorefractive effect in Anaclasis variant, to note volume hologram, wait for that the stable back of grating Anaclasis variant has just become beam splitting element, the angle of light beam when intersecting that described two bundles have a coherence should make at this moment take place be diffracted to Raman-Nath diffraction (Raman-Na Si diffraction); Two, beam splitting process: the beam splitting element of step 1 preparation is placed in the light path that needs beam splitting, makes the light beam that needs beam splitting be input to the light input end of beam splitting element, utilize the Raman-Nath diffraction can obtain the multi beam outgoing beam at the light output end of beam splitting element.In the present invention, described two restraint the coherent length of the optical path difference of the light beam with coherence less than described light beam, and above-mentioned coherent length can measure by interferometric method, and the purpose of doing like this is in order to make above-mentioned two light beams have the coherence.
In the present invention, in order to obtain high order diffraction grating as much as possible, the angle of crossing two-beam is as far as possible little, normally within the several years; When angle was excessive, what the refractive-index grating that two crossing bundle coherent lights produce in Anaclasis variant took place was Bragg diffraction (Bragg diffraction), and this Bragg diffraction can only be divided into two bundles to incident light, can not be used for the beam splitting of multi beam emergent light.Usually by computing formula Q=2 π λ L/n Λ
2Determine whether the parameter of selecting satisfies the condition that produces the Raman-Nath diffraction when implementing: when Q＜1, be the Raman-Nath diffraction; When Q＞1, be the Bragg diffraction; The wavelength of the crossing light beam of λ-incident wherein, the thickness of L-Anaclasis variant, the refractive index of n-Anaclasis variant, Λ-grating space.
When being used for beam splitting, penetrate the approximately equalised multi beam outgoing beam of angle with the made beam splitting element of the present invention, and each outgoing beam has same wavefront form on the position that distance outgoing place equates from beam splitting element.In dividing intrafascicular a kind of new beam splitting element that designed, the preparation method of this beam splitting element is simple relatively, cost is lower, simple in structure photorefractive effect application in the present invention.Compare with the beam-splitting method that utilizes polarization beam splitter prism with the binary optical beam-splitting method, the present invention utilizes the photorefractive effect of photorefractive material to realize the light beam splitting, not only can carry out beam splitting to the light beam of the breath of not taking a message, and can be beamed into multi beam output to the incident light that has information of different wave length, the present invention also has an advantage in addition in addition, promptly loose to the beam splitting conditional request when beam splitting: 1) for the not strict requirement of the incident angle of the light beam irradiates beam splitting element that needs beam splitting, 2) beam splitting element spectral bandwidth broad applicatory.The optical wavelength that uses during the preparation beam splitting element can be inconsistent with the optical wavelength that needs beam splitting, therefore can carry out beam splitting to the light wave in certain wavelength coverage, and is very flexible in the application.
Description of drawings
Fig. 1 prepares the light transmission process flow diagram of beam splitting element 10 for the step 1 of beam-splitting method of the present invention, Fig. 2 is the light transmission process flow diagram of embodiment six, Fig. 3 is the experimental result picture of embodiment seven, Fig. 4 is the experimental result picture of embodiment eight, Fig. 5 is the experimental result picture of embodiment ten, and Fig. 6 is the experimental result picture of embodiment 11.
Embodiment
Embodiment one: this embodiment is described in conjunction with Fig. 1, in this embodiment, optical bend and higher diffraction beam splitting method carries out according to the following steps: one, preparation beam splitting element 10: the light beam that makes two bundles have the coherence intersects and is input to the light input end of Anaclasis variant 5, so in Anaclasis variant 5, form the uneven interference fringe of light distribution and utilize photorefractive effect in Anaclasis variant 5, to note volume hologram, wait for that the stable back of grating Anaclasis variant 5 has just become beam splitting element 10, the angle theta of light beam when intersecting that described two bundles have a coherence should make at this moment take place be diffracted to Raman-Nath diffraction (Raman-Na Si diffraction); Two, beam splitting process: the beam splitting element 10 of step 1 preparation is placed in the light path that needs beam splitting, make the light beam that needs beam splitting be input to the light input end of beam splitting element 10, utilize the Raman-Nath diffraction can obtain the multi beam outgoing beam at the light output end of beam splitting element 10.In this embodiment, two restraint the coherent length of the optical path difference of the light beam with coherence less than described light beam described in the step 1.
Embodiment two: this embodiment is described in conjunction with Fig. 1, in embodiment one, Anaclasis variant described in the step 15 is selected any materials that can produce photorefractive effect for use, and it comprises organic material or inorganic material, and its size requires to decide according to specific product.Behind the material of having selected Anaclasis variant 5, the refractive index n of Anaclasis variant can be determined, can judge according to other conditions whether Anaclasis variant 5 can produce the Raman-Nath diffraction then.
Embodiment three: in conjunction with Fig. 1 this embodiment is described, in embodiment one, needs the wavelength of the light beam of beam splitting to be decided by that the bundle of two described in the step 1 has the wavelength of coherence's light beam described in the step 2.The wavelength of light beam that two bundles have a coherence equal in the wavelength or near the certain limit the wavelength of the described light beam that needs beam splitting of the described light beam that needs beam splitting.
Embodiment four: in conjunction with Fig. 1 this embodiment is described, this embodiment with the difference of embodiment one is: the device that produces the crossing light beam with coherence of two bundles in the step 1 is made up of first laser instrument 1, semi-transparent semi-reflecting lens 2, first catoptron 3 and second catoptron 4; The method that produces the crossing light beam with coherence of two bundles in the step 1 is: the light beam of output is input to the light input end of semi-transparent semi-reflecting lens 2 from first laser instrument 1, semi-transparent semi-reflecting lens 2 is divided into transmitted light and reflected light with the light beam of input, described reflected light is input to the light input end of first catoptron 3 and utilizes first catoptron 3 to make described reflected light change direction, described transmitted light is input to the light input end of second catoptron 4 and utilizes second catoptron 4 to make described transmitted light change direction, the reflected light that has made from the change of first catoptron 3 output direction with from the change of second catoptron, 4 outputs the transmitted light of direction intersect and be in the same place, promptly obtained the light beam with coherence that two bundles intersect, the optical path difference of described reflected light and transmitted light is less than the coherent length of the laser of first laser instrument, 1 output; Described first laser instrument 1 can produce the laser of any wavelength with photorefractive effect, and the light intensity of described laser is by the material decision of Anaclasis variant 5.Other steps are identical with embodiment one.High-intensity luminous energy produces refractive-index grating faster.The method of the coherent light beam that this embodiment generation two bundles can intersect is simple, easy to operate, and the optical device consumption is few.
Embodiment five: in conjunction with Fig. 2 this embodiment is described, this embodiment with the difference of embodiment one is: the light beam that needs beam splitting described in the step 2 is the laser of directly exporting from laser instrument.Other steps are identical with embodiment one.Utilize the beam splitting element 10 of method preparation of the present invention directly to carry out beam splitting to the light beam that does not contain information, usage is simple.
Embodiment six: this embodiment is described in conjunction with Fig. 2, this embodiment with the difference of embodiment four is: need the generation device of the light beam of beam splitting to be made of second laser instrument 11, spatial light wave filter 6, first fourier lense 7, spatial light modulator 8, second fourier lense 9 described in the step 2, spatial light modulator 8 is between first fourier lense 7 and second fourier lense 9, and the distance of spatial light modulator 8 to second fourier lenses 9 is focal lengths of second fourier lense 9; The described production method of the light beam of beam splitting that needs is: be input to the light input end of first fourier lense 7 by spatial light wave filter 6 and through 7 transmission of first fourier lense from the light beam of second laser instrument 11 output, light output end at first fourier lense 7 obtains parallel beam, after transmitting through spatial light modulator 8, described parallel beam is input to the light input end of second fourier lense 9, described parallel beam is loaded information in the process through spatial light modulator 8 transmission, the described directional light that is loaded information is finished Fourier transform through second fourier lense, 9 transmission backs at the light output end of second fourier lense 9, and the light beam that Fourier transform is finished in described light output end output from second fourier lense 9 promptly is the light beam that needs beam splitting.Other steps are identical with embodiment four.In this embodiment, input light forms the Fourier transform frequency spectrum in beam splitting element 10, because the beam splitting effect of beam splitting element 10, diffraction goes out the identical Fourier transform frequency spectrum of spectrum distribution, but the direction difference of each Fourier transform frequency spectrum, thereby incident light is divided into multi beam.In this embodiment, beam splitting element 10 is placed near the Fourier focal plane of second fourier lense 9 usually, can reduce the volume of branch beam device like this.This embodiment has only provided the method and apparatus that a kind of generation has the light beam of information, if the output terminal that runs into method and apparatus that other generations have the light beam of information and only need beam splitting element 10 with the present invention's preparation be placed on this device can be realized beam splitting.
Embodiment seven: in conjunction with Fig. 1 and Fig. 2 this embodiment is described, this embodiment with the difference of embodiment six is: in step 1, described first laser instrument 1 adopts Ar
+Laser instrument, its output light wavelength is 488.0 nanometers, and described Anaclasis variant 5 is selected the lithium columbate crystal of doping zinc and iron for use, and wherein the volumetric molar concentration of zinc is 3%, and the weight concentration of iron is 0.03%, crystalline size is 20.60 * 15.03 * 3.02mm
3(cubic millimeter), described catoptrical light intensity is 10.22mWcm
-2(every square centimeter of milliwatt), the light intensity of described transmitted light are 10.16mWcm
-2, the reflected light that intersects and the angle theta of transmitted light are 1.56 ° (degree), the C direction of principal axis of the reflected light that intersects and the polarization direction of transmitted light and lithium columbate crystal in plane of incidence, described Anaclasis variant 5 by crossing light beam irradiates after five minutes grating reach stable; In step 2, described second laser instrument 11 adopts Ar
+Laser instrument, its output light wavelength is 488.0 nanometers, and the focal length of described second fourier lense 9 is 505 millimeters, and optical bend and higher diffraction beam splitting element 10 is placed on preceding 5 millimeters places, Fourier focal plane of second fourier lense 9.Can see that at the output terminal of optical bend and higher diffraction beam splitting element 10 5 diffracted signal light that corner dimension equates occur, and the spectrum distribution situation of each diffraction light is identical on the identical distance of distance outgoing place, as shown in Figure 3.Other steps are identical with embodiment six.In this embodiment, " the C direction of principal axis of the reflected light that intersects and the polarization direction of transmitted light and lithium columbate crystal is in plane of incidence " this condition is in order to obtain best refractive-index grating in lithium columbate crystal, thereby reach the optimum condition of Raman-Nath diffraction, the best incident direction of incident light of irradiation Anaclasis variant 5 is by the material character decision of Anaclasis variant 5.
Embodiment eight: in conjunction with Fig. 1 and Fig. 2 this embodiment is described, this embodiment with the difference of embodiment seven is: in step 2, described second laser instrument, 11 output light wavelengths are 632.8 nanometers.Other steps are identical with embodiment seven.Can see that at the output terminal of optical bend and higher diffraction beam splitting element 10 4 diffracted signal light that corner dimension equates occur, and the spectrum distribution situation of each diffraction light is identical on the identical distance of distance outgoing place, as shown in Figure 4.
Embodiment nine: in conjunction with Fig. 1 and Fig. 2 this embodiment is described, this embodiment with the difference of embodiment seven is: in step 2, described second laser instrument, 11 output light wavelengths are 532.0 nanometers.Other steps are identical with embodiment seven.
Embodiment ten: this embodiment is described in conjunction with Fig. 1 and Fig. 2, this embodiment with the difference of embodiment seven is: in step 1, described Anaclasis variant 5 is selected the lithium columbate crystal of doping praseodymium and iron for use, wherein the volumetric molar concentration of praseodymium is 1%, the weight concentration of iron is 0.03%, and crystalline size is 1.20 * 10.01 * 0.52mm
3, described Anaclasis variant 5 intersected light beam irradiates after ten minutes grating reach stable.Other steps are identical with embodiment seven.Can see that at the output terminal of optical bend and higher diffraction beam splitting element 10 6 diffracted signal light that corner dimension equates occur, and the spectrum distribution situation of each diffraction light is identical on the identical distance of distance outgoing place, as shown in Figure 5.
Embodiment 11: this embodiment is described in conjunction with Fig. 1 and Fig. 2, this embodiment with the difference of embodiment ten is: in step 2, described second laser instrument 11 adopts He-Ne (helium-neon) laser instrument, and its output light wavelength is 632.8 nanometers.Other steps are identical with embodiment ten.Can see that at the output terminal of optical bend and higher diffraction beam splitting element 10 6 diffracted signal light that corner dimension equates occur, and the spectrum distribution situation of each diffraction light is identical on the identical distance of distance outgoing place, as shown in Figure 6.
Embodiment 12: this embodiment is described in conjunction with Fig. 1 and Fig. 2, this embodiment with the difference of embodiment seven is: in step 1, described Anaclasis variant 5 is selected the organic photorefractive material of PQ-PMMA (phenanthrenequione-polymethylmethacrylate) for use.Other steps are identical with embodiment seven.
Except that above-mentioned embodiment, utilize photorefractive effect in photorefractive material, to form refractive-index grating and reach beam splitting purpose technical scheme all in the protection domain of this instructions.
Claims (10)
1, optical bend and higher diffraction beam splitting method, it is characterized in that it carries out according to the following steps: one, preparation beam splitting element (10): the light beam that makes two bundles have the coherence intersects and is input to the light input end of Anaclasis variant (5), so in Anaclasis variant (5), form the uneven interference fringe of light distribution and utilize photorefractive effect in Anaclasis variant (5), to note volume hologram, wait for that grating stable back Anaclasis variant (5) has just become beam splitting element (10), the angle (θ) of light beam when intersecting that described two bundles have a coherence should make at this moment take place be diffracted to the Raman-Nath diffraction; Two, beam splitting process: the beam splitting element (10) of step 1 preparation is placed in the light path that needs beam splitting, make the light beam that needs beam splitting be input to the light input end of beam splitting element (10), utilize the Raman-Nath diffraction can obtain the multi beam outgoing beam at the light output end of beam splitting element (10).
2, optical bend and higher diffraction beam splitting method according to claim 1 is characterized in that described in the step 1 that two bundles have coherence's the optical path difference of light beam less than the coherent length of described light beam.
3, optical bend and higher diffraction beam splitting method according to claim 1, it is characterized in that Anaclasis variant described in the step 1 (5) selects any materials that can produce photorefractive effect for use, it comprises organic material or inorganic material, and its size requires to decide according to specific product.
4, optical bend and higher diffraction beam splitting method according to claim 1 needing described in the step 2 to is characterized in that the wavelength of the light beam of beam splitting to be decided by that the bundle of two described in the step 1 has the wavelength of coherence's light beam.
5, optical bend and higher diffraction beam splitting method according to claim 1 is characterized in that producing in the step 1 two devices of restrainting the light beam with coherence that intersects and is made up of first laser instrument (1), semi-transparent semi-reflecting lens (2), first catoptron (3) and second catoptron (4); The method that produces the crossing light beam with coherence of two bundles in the step 1 is: the light beam of output is input to the light input end of semi-transparent semi-reflecting lens (2) from first laser instrument (1), semi-transparent semi-reflecting lens (2) is divided into transmitted light and reflected light with the light beam of input, described reflected light is input to the light input end of first catoptron (3) and utilizes first catoptron (3) to make described reflected light change direction, described transmitted light is input to the light input end of second catoptron (4) and utilizes second catoptron (4) to make described transmitted light change direction, the reflected light that has made from the change of first catoptron (3) output direction with from the change of second catoptron (4) output the transmitted light of direction intersect and be in the same place, promptly obtained the light beam with coherence that two bundles intersect, the optical path difference of described reflected light and transmitted light is less than the coherent length of the laser of first laser instrument (1) output; Described first laser instrument (1) can produce the laser of any wavelength with photorefractive effect, and the light intensity of described laser is by the material decision of Anaclasis variant (5).
6, optical bend and higher diffraction beam splitting method according to claim 1 is characterized in that needing the light beam of beam splitting described in the step 2 is the laser of directly exporting from laser instrument.
7, optical bend and higher diffraction beam splitting method according to claim 1, needing described in the step 2 to it is characterized in that the generation device of the light beam of beam splitting to constitute by second laser instrument (11), spatial light wave filter (6), first fourier lense (7), spatial light modulator (8), second fourier lense (9), spatial light modulator (8) is positioned between first fourier lense (7) and second fourier lense (9), and spatial light modulator (8) is the focal length of second fourier lense (9) to the distance of second fourier lense (9); The described production method of the light beam of beam splitting that needs is: be input to the light input end of first fourier lense (7) by spatial light wave filter (6) and transmit through first fourier lense (7) from the light beam of second laser instrument (11) output, light output end at first fourier lense (7) obtains parallel beam, after transmitting through spatial light modulator (8), described parallel beam is input to the light input end of second fourier lense (9), described parallel beam is loaded information in the process through spatial light modulator (8) transmission, the described directional light that is loaded information is finished Fourier transform through second fourier lense (9) transmission back at the light output end of second fourier lense (9), and the light beam that Fourier transform is finished in described light output end output from second fourier lense (9) promptly is the light beam that needs beam splitting.
According to claim 1,3,5 or 7 described optical bend and higher diffraction beam splitting methods, it is characterized in that in step 1 that 8, described first laser instrument (1) adopts Ar
+Laser instrument, its output light wavelength is 488.0 nanometers, and described Anaclasis variant (5) is selected the lithium columbate crystal of doping zinc and iron for use, and wherein the volumetric molar concentration of zinc is 3%, and the weight concentration of iron is 0.03%, crystalline size is 20.60 * 15.03 * 3.02mm
3, described catoptrical light intensity is 10.22mWcm
-2, the light intensity of described transmitted light is 10.16mWcm
-2, the reflected light that intersects and the angle of transmitted light are 1.56 °, the C direction of principal axis of the reflected light that intersects and the polarization direction of transmitted light and lithium columbate crystal in plane of incidence, described Anaclasis variant (5) intersected light beam irradiates after five minutes grating reach stable; In step 2, described second laser instrument (11) adopts Ar
+Laser instrument, its output light wavelength is 488.0 nanometers, and the focal length of described second fourier lense (9) is 505 millimeters, and optical bend and higher diffraction beam splitting element (10) is placed on preceding 5 millimeters places, Fourier focal plane of second fourier lense 9.
According to claim 1 or 3 described optical bend and higher diffraction beam splitting methods, it is characterized in that in step 1 that 9, described Anaclasis variant (5) is selected the lithium columbate crystal of doping praseodymium and iron for use, wherein the volumetric molar concentration of praseodymium is 1%, and the weight concentration of iron is 0.03%; Or the organic photorefractive material of PQ-PMMA.
According to claim 1 or 7 described optical bend and higher diffraction beam splitting methods, it is characterized in that in step 2 that 10, described second laser instrument (11) adopts the He-Ne laser instrument, its output light wavelength is 632.8 nanometers.
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Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101799593A (en) * | 2010-04-23 | 2010-08-11 | 哈尔滨工业大学 | High-speed electric control holographic crystal diffraction beam splitter, preparation method thereof and beam splitting method realized based on beam splitter |
| CN101943805A (en) * | 2010-08-27 | 2011-01-12 | 哈尔滨工业大学 | Manufacturing method of electronically-controlled quadratic electro-optical effect Prague diffraction beam splitter and beam splitting method by using beam splitter |
| CN109581789A (en) * | 2019-01-10 | 2019-04-05 | 浙江理工大学 | A kind of diffraction projecting method and system |
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2005
- 2005-09-28 CN CNB2005100103850A patent/CN100504504C/en not_active Expired - Fee Related
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101799593A (en) * | 2010-04-23 | 2010-08-11 | 哈尔滨工业大学 | High-speed electric control holographic crystal diffraction beam splitter, preparation method thereof and beam splitting method realized based on beam splitter |
| CN101943805A (en) * | 2010-08-27 | 2011-01-12 | 哈尔滨工业大学 | Manufacturing method of electronically-controlled quadratic electro-optical effect Prague diffraction beam splitter and beam splitting method by using beam splitter |
| CN109581789A (en) * | 2019-01-10 | 2019-04-05 | 浙江理工大学 | A kind of diffraction projecting method and system |
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