WO2012100642A1 - Speckle removal device based on mie scattering and motion of magnetically controlled particles - Google Patents

Speckle removal device based on mie scattering and motion of magnetically controlled particles Download PDF

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Publication number
WO2012100642A1
WO2012100642A1 PCT/CN2012/000041 CN2012000041W WO2012100642A1 WO 2012100642 A1 WO2012100642 A1 WO 2012100642A1 CN 2012000041 W CN2012000041 W CN 2012000041W WO 2012100642 A1 WO2012100642 A1 WO 2012100642A1
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Prior art keywords
closed optical
speckle
sol
solution
mie scattering
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PCT/CN2012/000041
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French (fr)
Chinese (zh)
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陈旭远
高文宏
石云波
张文栋
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中北大学
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Publication of WO2012100642A1 publication Critical patent/WO2012100642A1/en

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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/10Beam splitting or combining systems
    • G02B27/1006Beam splitting or combining systems for splitting or combining different wavelengths
    • G02B27/102Beam splitting or combining systems for splitting or combining different wavelengths for generating a colour image from monochromatic image signal sources
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/48Laser speckle optics
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/09Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on magneto-optical elements, e.g. exhibiting Faraday effect
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/09Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on magneto-optical elements, e.g. exhibiting Faraday effect
    • G02F1/094Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on magneto-optical elements, e.g. exhibiting Faraday effect based on magnetophoretic effect
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F2203/00Function characteristic
    • G02F2203/03Function characteristic scattering

Definitions

  • the invention relates to the field of display technology using coherent light as a light source, in particular to a speckle elimination device based on Mie scattering and magnetron particle motion, which mainly relates to optical speckle phenomenon existing in laser display technology and optical instrument.
  • the technical solution for successfully eliminating the spot by controlling the laser time coherence to achieve practical requirements is basically based on multi-light source superposition; 2.
  • Eliminating speckle by controlling the spatial coherence of the laser beam is currently eliminated.
  • the main method of speckle the basic principle is to adjust the phase distribution of the elementary light wave in the laser beam, thereby changing the spatial distribution of the speckle, and superimposing the plurality of speckle images in the integration time of the human eye to obtain a uniform distribution of light energy.
  • the image in turn, achieves the purpose of eliminating speckle.
  • the specific methods are: using a rotating scatterer, a vibrating screen, and vibration
  • the patent discloses "a scattering-based dephasing shimming device" that requires the use of a scattering medium having particles having a diameter that must be less than one tenth of the wavelength of the incident light to effect Rayleigh scattering of the incident laser.
  • an inorganic salt or an aqueous solution of an organic alcohol such as NaCl, KC1, KN0 3 or ZnS0 4 aqueous solution
  • the inorganic salt or organic alcohol aqueous solution is present in the form of hydrated ions or macromolecules, which is much smaller than the laser wavelength.
  • the speckle was removed by a light pipe filled with a saturated NaCl aqueous solution at a temperature of 50 mm at room temperature. As a result, as shown in Fig. 1, the speckle contrast was 70%, which hardly played. Reduce the effect of speckle.
  • the present invention provides a speckle reduction device based on Mie scattering and magnetron particle motion in order to solve the problems of poor speckle removal, complex structure, easy damage, and high cost in the existing speckle elimination method.
  • a speckle elimination device based on Mie scattering and magnetron particle motion comprising a closed optical reflection cavity provided with an incident light coupling device and a transmission exit surface, and a closed optical reflection cavity
  • the inner wall except the inner wall of the transmission exit surface is a "mirror" inner wall (ie, the inner wall has a high reflectivity characteristic, and can "fully reflect” the laser beam incident on the optical reflection cavity), and the closed optical reflection cavity is filled with the entire a solution or sol of the closed optical reflection cavity, and the solution or sol is dispersed with magnetic medium particles whose linearity can cause Mie scattering of the incident laser
  • the closed optical reflection cavity is provided with a magnetic field generating device for generating a magnetic field, and The electromagnet of the magnetic field generator is disposed outside the enclosed optical reflection cavity.
  • the laser beam emitted by the laser source is incident through the incident light coupling device. Mist scattering occurs in a solution or sol in a closed optical reflection chamber, and a magnetic medium particle dispersed in a solution or a sol (as shown in FIG.
  • the incident laser 101 irradiates the magnetic medium particle 402 to Mie scattering
  • the intensity of the scattered light scattered by the incident laser 101 is distributed over a wide range of angles, mainly concentrated on the forward scattered light 104, 105, 106, which generally accounts for more than 90% of the total scattering; the backscattered light 102 only occupies a small The portion is usually less than 10%; the scattered light 105 along the direction of the incident laser light is the strongest, and the scattered light 103, 107 in the vertical direction is the weakest. Therefore, the incident laser light is scattered by the magnetic medium particles 402, and is split into a plurality of strengths.
  • the scattered light, etc., while the scattering angle of the scattered light is enlarged, is split into a plurality of scattered light of different intensities, or reflected by the inner wall of the closed optical reflecting cavity, or again with the medium particles dispersed in the solution or sol.
  • Mie scattering the scattered light beam is more scattered light, after multiple Mie scattering, is emitted from the transmission exit surface of the closed optical reflection cavity;
  • the electromagnet is excited to form a constant magnetic field, or a pulsed magnetic field, or an alternating magnetic field outside the closed optical reflection cavity.
  • the magnetic medium particles in the solution or sol are subjected to a magnetic field force to counteract the effect of gravity, and are made in solution or sol.
  • the incident laser will randomly move with the magnetic medium particles moving in the solution or sol to cause Mie scattering, so that the scattered light of the incident laser at each moment will randomly change in the solution or The direction and path of propagation in the sol, and finally the phase distribution and scattering angle distribution of the scattered light emitted from the exit surface of the optical reflection cavity are randomly changed.
  • the scattered light at different times has different phase distribution and scattering angle distribution.
  • a speckle image is generated correspondingly; in the eye integration time (50ms), multiple speckle images are superimposed, and An image with uniform light energy distribution achieves the purpose of eliminating speckle. '
  • the present invention provides a closed optical reflection cavity filled with a solution or a sol, and the magnetic medium particles dispersed in the solution or the sol in the closed optical reflection cavity cause Mich scattering of the incident laser to perform scattering and splitting. And applying a magnetic field outside the closed optical reflection chamber to control the magnetic medium particles Irregular motion in a solution or sol, or counteracting gravity by magnetic force, causing irregular thermal motion of magnetic media particles, thereby randomly changing the propagation direction and path of the scattered beam in the closed optical reflection cavity, resulting in closed optical reflection
  • the cavity exit surface distributes the scattered light of the incident laser with different phase distributions and scattering angles at different times; thereby changing the spatial distribution of the speckle after the projection, so that the plurality of speckle images are superimposed in the integration time of the human eye to obtain a The light energy is evenly distributed, which effectively eliminates speckle.
  • the speckle contrast of the image can be less than 4%, as shown in FIG. 5, the speckle contrast of the image is as low as 3.8%, and the speckle elimination effect is excellent;
  • the speckle elimination effect is improved by increasing the temperature of the solution or sol, the concentration of the magnetic medium particles in the solution or the sol, controlling the variation of the field strength of the applied magnetic field, etc.;
  • the present invention performs the incident laser in the closed optical reflection cavity. Total reflection", the total light energy loss of the incident laser is very small, which ensures the high utilization of the laser, and achieves the purpose of uniformity in the "total reflection”process; in addition, the closed optical reflection cavity structure used in the present invention is very common.
  • the solution and the sol do not need to select a special material, and have the advantage of low cost.
  • the invention has the advantages of reasonable structure, compactness, easy realization, low cost, good speckle elimination effect, high laser utilization rate, stable performance, safety and reliability, and uniform light function.
  • Figure 3 is a diagram showing the angular distribution of light intensity of Mie scattering
  • FIG. 4 is a schematic view showing a transmission state of a light beam in the device of the present invention.
  • Figure 5 is a graph showing test results obtained by using the apparatus of the present invention to eliminate speckle
  • FIG. 6 is a schematic diagram of application of the device of the present invention in a point scan display system
  • FIG. 7 is a schematic diagram of application of the device of the present invention in a full frame display system; In the figure: 101 - incident laser; 102, 103, 104, 105, 106, 107 - scattered light;
  • 300-speckle elimination device 301-incident optical coupling device; 302-closed optical reflection cavity; 303- transmission exit surface; 304-incident optical aperture; 305, 306, 307-speckle elimination device; 308-electromagnet ( Not for the intentional table);
  • the speckle elimination device based on Mie scattering and magnetron particle motion includes a closed optical reflection cavity 302 on which an incident light coupling device 301 and a transmission surface 303 are disposed, and closed optical reflection.
  • the inner wall of the cavity 302 except the inner wall of the transmission exit surface 303 is a "mirror surface” inner wall (ie, the inner wall has a high reflectivity characteristic, and can "fully reflect” the laser beam incident on the optical reflection cavity), and the closed optical reflection ⁇ 302 Filled with a solution or sol 401 filled with the entire closed optical reflection cavity 302, and the solution or sol 401 is dispersed with magnetic medium particles 402 whose linearity can cause Mie scattering of the incident laser light;
  • the closed optical reflection cavity 302 is provided with A magnetic field generating device that generates a magnetic field, and an electromagnet 308 of the magnetic field generator is disposed outside the closed optical reflecting chamber 302.
  • the solution is an organic solution or an inorganic solution
  • the sol is an aerosol or a sol
  • the magnetic medium particles 402 may be polystyrene magnetic microspheres, silica magnetic microspheres, The ferroferric oxide magnetic microspheres, the ferric oxide magnetic microspheres, and the like
  • the closed optical reflection cavity 302 is mostly made of metal, plane mirror, transparent plastic or glass, and the shape thereof is not particularly limited, and generally adopts a tubular shape.
  • the surface of the transmission exit surface 303 of the closed optical reflection cavity 302 is mostly made of transparent plastic or glass, and is mostly a rectangular plane or a circular plane, and the surface is provided with an antireflection film matched with the incident laser band;
  • the incident light coupling device 301 on the closed optical reflection cavity 302 can be realized as follows: a transmission incident surface is adopted, and an antireflection film matching the incident laser band is provided on the surface; or an incident aperture structure is adopted, and An optical coupling element such as a lens is disposed on the incident aperture 304.
  • the speckle elimination device of the present invention can be applied to a laser projection display technology, for example, as shown in FIG. 6, applied to a Raster-Scanned Displays system, and the signal sources 601, 602, 603 are based on a two-dimensional image.
  • the information of each pixel modulates the output power of the three primary color lasers 501, 502, 503 respectively; the three incident lasers are coupled to the speckle elimination device 300 of the present invention through the mirrors 504, 505, 506, modulated, and then exported through the exit surface.
  • the lens 700 and the micro-scanning mirror (Scan Mirror 701 project to the screen 800.
  • the micro-scanning mirror 701 scans the screen on a pixel-by-pixel basis according to the two-dimensional image driven by the electric signal.
  • This application example is suitable for point scanning laser projectors and lasers TV display.
  • the system is applied to a Full-Frame Displays system, and the three primary color lasers 501, 502, and 503 output a constant power laser beam, and are respectively introduced into the speckle elimination device 305, 306 of the present invention.
  • the relay lenses 701, 704, 707, the plane mirror 708, and the TIR prisms 703, 705, 709 are condensed to the optical modulators DLP 702, 706, 710; the optical modulators DLP 702, 706, 710 are based on each frame.
  • the 2-dimensional image information is modulated to produce a monochrome image; the three primary color images are blended by prism 711 and projected by lens 700 onto screen 800.
  • This application example is suitable for laser projectors and laser TV displays based on optical modulators such as DMD and LCOS.

Abstract

A speckle removal device relating to the technical field of display having a coherent light as a light source, based on Mie scattering and motion of magnetically controlled particles, solves the problems in the prior art of bad speckle removal effect, complex structure, high cost, and being easily damaged. The speckle removal device (300) comprises a closed optical reflective chamber (302) disposed with an incident optical coupler device (301) and a projection emergent surface (303). The inner walls of the closed optical reflective chamber (302) are all mirrors except the inner wall of the projection emergent surface (303). The inside of the closed optical reflective chamber (302) is filled with a solution or a sol (401). Dispersed inside of the solution or sol (401) are magnetic medium particles (402) having a linear dimension that triggers Mie scattering on an incident laser. Disposed for the closed optical reflective chamber (302) is a magnetic field generation device for generating a magnetic field. The electromagnet (308) of the magnetic field generation device is disposed outside of the closed optical reflective chamber. The speckle removal device has a logical, compact structure, high speckle removal effect, and is safe, reliable, and easy to implement at a low cost. The device has high laser utilization rate and stability, and makes illumination even.

Description

基于米氏散射及磁控粒子运动的散斑消除装置 技术领域  Speckle elimination device based on Mie scattering and magnetron particle motion
本发明涉及以相干光为光源的显示技术领域,具体是一种基于米氏散射及 磁控粒子运动的散斑消除装置,主要针对激光显示技术及光学仪器中存在的光 学散斑现象。  The invention relates to the field of display technology using coherent light as a light source, in particular to a speckle elimination device based on Mie scattering and magnetron particle motion, which mainly relates to optical speckle phenomenon existing in laser display technology and optical instrument.
背景技术  Background technique
以激光为光源照射屏幕时, 由于激光的相干性及屏幕的粗糙, 导致人眼看 到被散斑覆盖的图像, 严重影响图像显示质量, 阻碍观察者从图像中提取有用 信息。 因此, 如何消除散斑一直是以激光为光源的光学仪器领域和显示技术领 域中的研发热点。而就目前的研究结果来看, 为消除散斑所用的方法大致可以 分为两大类: 一、通过控制激光光源的时间相干性来降低散斑, 其原理是通过 调整激光波长 (或者频率)及多波长光源产生沸腾散斑, 目前通过控制激光时间 相干性成功消除光斑达到实用要求的技术方案基本上以多光源叠加为主; 二、 通过控制激光光束空间相干性消除散斑, 是目前消除散斑的主要方法, 基本原 理是调整激光光束中基元光波的相位分布, 从而改变散斑的空间分布, 将多个 散斑图像在人眼积分时间内相叠加, 得到一个光能分布均匀的图像, 进而实现 消除散斑的目的。 具体的方法有: 采用旋转散射体、 振动屏幕、 振动具有 When the laser is used as the light source to illuminate the screen, the coherence of the laser and the roughness of the screen cause the human eye to see the image covered by the speckle, which seriously affects the image display quality and hinders the observer from extracting useful information from the image. Therefore, how to eliminate speckle has always been a research and development hotspot in the field of optical instruments and display technology with laser as the light source. As far as the current research results are concerned, the methods used to eliminate speckle can be roughly divided into two categories: 1. Control the temporal coherence of the laser source to reduce speckle. The principle is to adjust the laser wavelength (or frequency). And the multi-wavelength light source generates boiling speckle. At present, the technical solution for successfully eliminating the spot by controlling the laser time coherence to achieve practical requirements is basically based on multi-light source superposition; 2. Eliminating speckle by controlling the spatial coherence of the laser beam is currently eliminated. The main method of speckle, the basic principle is to adjust the phase distribution of the elementary light wave in the laser beam, thereby changing the spatial distribution of the speckle, and superimposing the plurality of speckle images in the integration time of the human eye to obtain a uniform distribution of light energy. The image, in turn, achieves the purpose of eliminating speckle. The specific methods are: using a rotating scatterer, a vibrating screen, and vibration
Hadamard 图形散射体、 高频振动光纤等。 上述方法, 或要借助机械振动, 甚 至需要高频或大幅振动, 或要集成多光源, 实现结构复杂、 易损坏、 成本高, 更主要的是散斑消除效果不佳。 Hadamard graphic scatterers, high frequency vibrating fibers, etc. The above method, or mechanical vibration, even requires high frequency or large vibration, or integrated multiple light sources, to achieve a complex structure, easy to damage, high cost, and more importantly, the speckle removal effect is not good.
也有未借助机械振动的技术方案,例如:专利号为 200820122639.7的中国 专利公开了"一种基于散射的消相干匀场装置", 要求使用含有直径必须小于入 射光波长十分之一的颗粒的散射介质, 以实现对入射激光形成瑞利散射。专利. 中利用无机盐或有机醇水溶液 (如 NaCl、 KC1、 KN03或 ZnS04水溶液)作为散 射介质, 基于无机盐或有机醇水溶液的存在形式是水合离子或大分子, 相对于 激光波长小很多, 会对入射激光形成瑞利散射, 以此实现入射激光分束, 并在 光导管内传导, 以期降低入射激光的相干性来消除散斑, 同时利用光导管的混 光作用, 将上述分束光进行匀化来匀场消相干。但按该申请所述技术方法进行 试验, 在室温下, 利用长度为 50mm、 充满饱和 NaCl水溶液的光导管消除散 斑, 结果如图 1所示, 其散斑对比度为 70%, 几乎没有起到降低散斑的作用。 There are also technical solutions that do not rely on mechanical vibration, for example: China with patent number 200820122639.7 The patent discloses "a scattering-based dephasing shimming device" that requires the use of a scattering medium having particles having a diameter that must be less than one tenth of the wavelength of the incident light to effect Rayleigh scattering of the incident laser. In the patent, an inorganic salt or an aqueous solution of an organic alcohol (such as NaCl, KC1, KN0 3 or ZnS0 4 aqueous solution) is used as a scattering medium. The inorganic salt or organic alcohol aqueous solution is present in the form of hydrated ions or macromolecules, which is much smaller than the laser wavelength. Rayleigh scattering is formed on the incident laser to split the incident laser and conduct it in the light pipe, in order to reduce the coherence of the incident laser to eliminate the speckle, and at the same time, use the light mixing effect of the light pipe to split the beam Homogenize to homogenize the coherence. However, according to the technical method described in the application, the speckle was removed by a light pipe filled with a saturated NaCl aqueous solution at a temperature of 50 mm at room temperature. As a result, as shown in Fig. 1, the speckle contrast was 70%, which hardly played. Reduce the effect of speckle.
发明内容  Summary of the invention
本发明为了解决现有散斑消除方法存在的消除散斑效果不佳、实现结构复 杂、 易损坏、 成本高等问题, 提供了一种基于米氏散射及磁控粒子运动的散斑 消除装置。  The present invention provides a speckle reduction device based on Mie scattering and magnetron particle motion in order to solve the problems of poor speckle removal, complex structure, easy damage, and high cost in the existing speckle elimination method.
本发明是采用如下技术方案实现的:基于米氏散射及磁控粒子运动的散斑 消除装置, 包括其上设有入射光耦合装置和透射出射面的封闭式光学反射腔, 封闭式光学反射腔除透射出射面内壁之外的内壁皆为"镜面"内壁(即内壁具有 高反射率特性, 能"全反射"入射于光学反射腔内的激光光束) , 封闭式光学反 射腔内填有充满整个封闭式光学反射腔的溶液或溶胶,且溶液或溶胶内散布有 其线度能引起入射激光发生米氏散射的磁性介质粒子;封闭式光学反射腔配设 有用以产生磁场的磁场发生装置,且磁场发生器的电磁铁设置于封闭式光学反 射腔外。  The invention is realized by the following technical solutions: a speckle elimination device based on Mie scattering and magnetron particle motion, comprising a closed optical reflection cavity provided with an incident light coupling device and a transmission exit surface, and a closed optical reflection cavity The inner wall except the inner wall of the transmission exit surface is a "mirror" inner wall (ie, the inner wall has a high reflectivity characteristic, and can "fully reflect" the laser beam incident on the optical reflection cavity), and the closed optical reflection cavity is filled with the entire a solution or sol of the closed optical reflection cavity, and the solution or sol is dispersed with magnetic medium particles whose linearity can cause Mie scattering of the incident laser; the closed optical reflection cavity is provided with a magnetic field generating device for generating a magnetic field, and The electromagnet of the magnetic field generator is disposed outside the enclosed optical reflection cavity.
应用时, 如图 4所示, 由激光光源发射的激光光束经入射光耦合装置入射 到封闭式光学反射腔内的溶液或溶胶中,与溶液或溶胶中散布的磁性介质粒子 作用发生米氏散射 (如图 3所示, 当入射激光 101照射磁性介质粒子 402发生米 氏散射时, 入射激光 101散射后的散射光光强分布于一个很宽的角度范围内, 主要集中于前向散射光 104、 105、 106, 一般占总散射 90%以上; 后向散射光 102只占很小部分,通常小于 10%;沿入射激光前进方向的散射光 105光强最强, 垂直方向的散射光 103、 107最弱, 因此入射激光经磁性介质粒子 402散射后, 分束成多个强度不等的散射光, 同时散射光的散射角分布扩大) , 分束成多个 强度不等的散射光, 或经封闭式光学反射腔内壁反射, 或再次与溶液或溶胶中 散布的介质粒子作用发生米氏散射, 散射光分束为更多的散射光, 经多次米氏 散射后, 由封闭式光学反射腔的透射出射面出射; 在磁场发生器的控制下, 电 磁铁励磁, 在封闭式光学反射腔外形成恒定磁场、 或脉冲磁场、 或交变磁场, 溶液或溶胶中磁性介质粒子受到磁场力作用, 抵消自身重力作用, 于溶液或溶 胶中做无规则热运动, 或者, 在磁场力作用下受控运动, 入射激光会与溶液或 溶胶中运动的磁性介质粒子随机作用发生米氏散射,使得各时刻入射激光的散 射光会随机改变在溶液或溶胶中传播方向和路径,最终在光学反射腔出射面出 射的散射光的相位分布、 散射角分布随机变化。而不同时刻的出射散射光具有 不同的相位分布、 散射角分布, 经投影后, 分别会对应产生一个散斑图像; 在 人眼积分时间(50ms) 内, 多个散斑图像相叠加, 会得到一个光能分布均匀的 图像, 进而实现了消除散斑现象的目的。 ' When applied, as shown in Figure 4, the laser beam emitted by the laser source is incident through the incident light coupling device. Mist scattering occurs in a solution or sol in a closed optical reflection chamber, and a magnetic medium particle dispersed in a solution or a sol (as shown in FIG. 3, when the incident laser 101 irradiates the magnetic medium particle 402 to Mie scattering) The intensity of the scattered light scattered by the incident laser 101 is distributed over a wide range of angles, mainly concentrated on the forward scattered light 104, 105, 106, which generally accounts for more than 90% of the total scattering; the backscattered light 102 only occupies a small The portion is usually less than 10%; the scattered light 105 along the direction of the incident laser light is the strongest, and the scattered light 103, 107 in the vertical direction is the weakest. Therefore, the incident laser light is scattered by the magnetic medium particles 402, and is split into a plurality of strengths. The scattered light, etc., while the scattering angle of the scattered light is enlarged, is split into a plurality of scattered light of different intensities, or reflected by the inner wall of the closed optical reflecting cavity, or again with the medium particles dispersed in the solution or sol. Mie scattering, the scattered light beam is more scattered light, after multiple Mie scattering, is emitted from the transmission exit surface of the closed optical reflection cavity; Under the system, the electromagnet is excited to form a constant magnetic field, or a pulsed magnetic field, or an alternating magnetic field outside the closed optical reflection cavity. The magnetic medium particles in the solution or sol are subjected to a magnetic field force to counteract the effect of gravity, and are made in solution or sol. Irregular thermal motion, or controlled motion under the action of a magnetic field, the incident laser will randomly move with the magnetic medium particles moving in the solution or sol to cause Mie scattering, so that the scattered light of the incident laser at each moment will randomly change in the solution or The direction and path of propagation in the sol, and finally the phase distribution and scattering angle distribution of the scattered light emitted from the exit surface of the optical reflection cavity are randomly changed. The scattered light at different times has different phase distribution and scattering angle distribution. After projection, a speckle image is generated correspondingly; in the eye integration time (50ms), multiple speckle images are superimposed, and An image with uniform light energy distribution achieves the purpose of eliminating speckle. '
与现有技术相比, 本发明设置充满溶液或溶胶的封闭式光学反射腔, 在封 闭式光学反射腔内以溶液或溶胶中散布的磁性介质粒子引起入射激光发生米 氏散射, 进行散射分束, 并于封闭式光学反射腔外施加磁场, 控制磁性介质粒 子在溶液或溶胶内的无规则运动, 或以磁场力抵消重力, 使磁性介质粒子无规 则热运动, 进而随机改变散射光束在封闭式光学反射腔中的传播方向和路径, 使得封闭式光学反射腔出射面在不同时间以不同的相位分布和散射角分布出 射入射激光的散射光; 从而改变投影后产生散斑的空间分布, 使多个散斑图像 在人眼积分时间内相叠加,得到一个光能分布均匀的图像,进而有效消除散斑。 且经试验测试, 应用本发明所述装置后, 图像的散斑对比度可低于 4%, 如图 5 所示, 图像的散斑对比度已低至 3.8%, 散斑消除效果极好; 并可以通过提高溶 液或溶胶的温度、溶液或溶胶中的磁性介质粒子浓度、控制外加磁场场强的变 化规律等等措施来提高散斑消除效果;本发明于封闭式光学反射腔中对入射激 光进行 "全反射", 入射激光的总体光能损失甚微, 保证了激光的高利用率, 并 在"全反射 "过程中实现了匀光目的; 此外, 本发明所用封闭式光学反射腔结构 极为普通, 且溶液、 溶胶也无须选择特殊材料, 具有低造价的优势。 Compared with the prior art, the present invention provides a closed optical reflection cavity filled with a solution or a sol, and the magnetic medium particles dispersed in the solution or the sol in the closed optical reflection cavity cause Mich scattering of the incident laser to perform scattering and splitting. And applying a magnetic field outside the closed optical reflection chamber to control the magnetic medium particles Irregular motion in a solution or sol, or counteracting gravity by magnetic force, causing irregular thermal motion of magnetic media particles, thereby randomly changing the propagation direction and path of the scattered beam in the closed optical reflection cavity, resulting in closed optical reflection The cavity exit surface distributes the scattered light of the incident laser with different phase distributions and scattering angles at different times; thereby changing the spatial distribution of the speckle after the projection, so that the plurality of speckle images are superimposed in the integration time of the human eye to obtain a The light energy is evenly distributed, which effectively eliminates speckle. And after testing, after applying the device of the invention, the speckle contrast of the image can be less than 4%, as shown in FIG. 5, the speckle contrast of the image is as low as 3.8%, and the speckle elimination effect is excellent; The speckle elimination effect is improved by increasing the temperature of the solution or sol, the concentration of the magnetic medium particles in the solution or the sol, controlling the variation of the field strength of the applied magnetic field, etc.; the present invention performs the incident laser in the closed optical reflection cavity. Total reflection", the total light energy loss of the incident laser is very small, which ensures the high utilization of the laser, and achieves the purpose of uniformity in the "total reflection"process; in addition, the closed optical reflection cavity structure used in the present invention is very common. Moreover, the solution and the sol do not need to select a special material, and have the advantage of low cost.
本发明结构合理、 紧凑, 易实现, 造价低, 散斑消除效果好, 激光利用率 高, 性能稳定, 安全可靠, 并具有匀光功能。  The invention has the advantages of reasonable structure, compactness, easy realization, low cost, good speckle elimination effect, high laser utilization rate, stable performance, safety and reliability, and uniform light function.
附图说明  DRAWINGS
图 1为利用一现有技术消除散斑获得的测试结果图;  1 is a graph showing test results obtained by eliminating speckle using a prior art;
图 2为本发明的结构示意图;  2 is a schematic structural view of the present invention;
图 3为米氏散射的光强角分布图;  Figure 3 is a diagram showing the angular distribution of light intensity of Mie scattering;
图 4为本发明所述装置内光束的传输状态示意图;  4 is a schematic view showing a transmission state of a light beam in the device of the present invention;
图 5为利用本发明所述装置消除散斑获得的测试结果图;  Figure 5 is a graph showing test results obtained by using the apparatus of the present invention to eliminate speckle;
图 6为本发明所述装置在点扫描显示系统中的应用示意图;  6 is a schematic diagram of application of the device of the present invention in a point scan display system;
图 7为本发明所述装置在全帧显示系统中的应用示意图; 图中: 101-入射激光; 102、 103、 104、 105、 106、 107-散射光;7 is a schematic diagram of application of the device of the present invention in a full frame display system; In the figure: 101 - incident laser; 102, 103, 104, 105, 106, 107 - scattered light;
300-散斑消除装置; 301-入射光耦合装置; 302-封闭式光学反射腔; 303- 透射出射面; 304-入射光孔; 305、 306、 307-散斑消除装置; 308-电磁铁 (为 不意式表不) ; 300-speckle elimination device; 301-incident optical coupling device; 302-closed optical reflection cavity; 303- transmission exit surface; 304-incident optical aperture; 305, 306, 307-speckle elimination device; 308-electromagnet ( Not for the intentional table);
401-溶液或溶胶; 402-磁性介质粒子;  401-solution or sol; 402-magnetic medium particles;
501、 502、 503-激光器;  501, 502, 503-laser;
601 602 > 603-信号源;  601 602 > 603-signal source;
700-透镜; 701-中继透镜; 702-光调制器 DLP; 703-TIR棱镜; 704-中继透 镜; 705-TIR棱镜; 706-光调制器 DLP; 707-中继透镜; 708-平面镜; 709-TIR 棱镜; 710-光调制器 DLP; 711-棱镜; 712-微扫描镜;  700-lens; 701-relay lens; 702-light modulator DLP; 703-TIR prism; 704-relay lens; 705-TIR prism; 706-light modulator DLP; 707-relay lens; 708-plane mirror; 709-TIR prism; 710-light modulator DLP; 711-prism; 712-micro-scanning mirror;
800-屏幕。  800-screen.
具体实施方式  detailed description
如图 2所示, 基于米氏散射及磁控粒子运动的散斑消除装置, 包括其上设 有入射光耦合装置 301和透射出^ f面 303的封闭式光学反射腔 302, 封闭式光学 反射腔 302除透射出射面 303内壁之外的内壁皆为 "镜面 "内壁(即内壁具有高反 射率特性, 能"全反射 "入射于光学反射腔内的激光光束) , 封闭式光学反射脍 302内填有充满整个封闭式光学反射腔 302的溶液或溶胶 401,且溶液或溶胶 401 内散布有其线度能引起入射激光发生米氏散射的磁性介质粒子 402; 封闭式光 学反射腔 302配设有用以产生磁场的磁场发生装置,且磁场发生器的电磁铁 308 设置于封闭式光学反射腔 302外。  As shown in FIG. 2, the speckle elimination device based on Mie scattering and magnetron particle motion includes a closed optical reflection cavity 302 on which an incident light coupling device 301 and a transmission surface 303 are disposed, and closed optical reflection. The inner wall of the cavity 302 except the inner wall of the transmission exit surface 303 is a "mirror surface" inner wall (ie, the inner wall has a high reflectivity characteristic, and can "fully reflect" the laser beam incident on the optical reflection cavity), and the closed optical reflection 脍 302 Filled with a solution or sol 401 filled with the entire closed optical reflection cavity 302, and the solution or sol 401 is dispersed with magnetic medium particles 402 whose linearity can cause Mie scattering of the incident laser light; the closed optical reflection cavity 302 is provided with A magnetic field generating device that generates a magnetic field, and an electromagnet 308 of the magnetic field generator is disposed outside the closed optical reflecting chamber 302.
具体实施时, 所述溶液为有机溶液或无机溶液; 所述溶胶为气溶胶或液溶 胶; 所述磁性介质粒子 402可以采用聚苯乙烯磁性微球、 二氧化硅磁性微球、 四氧化三铁磁性微球、 三氧化二铁磁性微球等等; 所述封闭式光学反射腔 302 多选用金属、 平面镜、 透明塑料或玻璃加工制作, 且其形状无需特别限定, 一 般多采用管状腔体;封闭式光学反射腔 302的透射出射面 303表面多选用透明塑 料或玻璃加工制作, 且多为矩形平面或圆形平面, 且表面设有与入射激光波段 匹配的增透膜; In a specific implementation, the solution is an organic solution or an inorganic solution; the sol is an aerosol or a sol; the magnetic medium particles 402 may be polystyrene magnetic microspheres, silica magnetic microspheres, The ferroferric oxide magnetic microspheres, the ferric oxide magnetic microspheres, and the like; the closed optical reflection cavity 302 is mostly made of metal, plane mirror, transparent plastic or glass, and the shape thereof is not particularly limited, and generally adopts a tubular shape. The surface of the transmission exit surface 303 of the closed optical reflection cavity 302 is mostly made of transparent plastic or glass, and is mostly a rectangular plane or a circular plane, and the surface is provided with an antireflection film matched with the incident laser band;
所述封闭式光学反射腔 302上的入射光耦合装置 301可以按如下结构实现- 采用透射入射面, 并在表面设有与入射激光波段匹配的增透膜;.或者采用入射 光孔结构, 并在入射光孔 304上配设有光学耦合元件, 如: 透镜。  The incident light coupling device 301 on the closed optical reflection cavity 302 can be realized as follows: a transmission incident surface is adopted, and an antireflection film matching the incident laser band is provided on the surface; or an incident aperture structure is adopted, and An optical coupling element such as a lens is disposed on the incident aperture 304.
本发明所述散斑消除装置能应用于激光投影显示技术中, 例如: 如图 6所 示, 应用于点扫描投影 (Raster-Scanned Displays)系统, 信号源 601、 602、 603 根据二维图像上每个像素的信息分别调制三基色激光器 501、 502、 503输出功 率; 三个入射激光通过镜子 504、 505、 506耦合入射本发明所述散斑消除装置 300, 经调制后于出射面导出, 通过透镜 700和微扫描镜 (Scan Mirror 701投影到 屏幕 800。在电信号的驱动下,微扫描镜 701根据二维图像逐像素扫描到屏幕上。 本应用实例适用于点扫描的激光投影仪和激光电视显示。  The speckle elimination device of the present invention can be applied to a laser projection display technology, for example, as shown in FIG. 6, applied to a Raster-Scanned Displays system, and the signal sources 601, 602, 603 are based on a two-dimensional image. The information of each pixel modulates the output power of the three primary color lasers 501, 502, 503 respectively; the three incident lasers are coupled to the speckle elimination device 300 of the present invention through the mirrors 504, 505, 506, modulated, and then exported through the exit surface. The lens 700 and the micro-scanning mirror (Scan Mirror 701 project to the screen 800. The micro-scanning mirror 701 scans the screen on a pixel-by-pixel basis according to the two-dimensional image driven by the electric signal. This application example is suitable for point scanning laser projectors and lasers TV display.
如图 7所示, 应用于全帧显示投影 (Full-Frame Displays)系统, 三基色激光 器 501、 502、 503输出恒定功率激光光束, 分别稱合导入本发明所述散斑消除 装置 305、 306、 307; 经调制后, 由中继透镜 701、 704、 707, 平面镜 708及 TIR 棱镜 703、 705、 709汇聚到光调制器 DLP 702、 706、 710; 光调制器 DLP 702、 706、 710根据每帧 2维图像信息调制生成单色图像;三基色图像经棱镜 711融和, 由透镜 700投影至屏幕 800。 本应用实例适用于基于 DMD、 LCOS 等光调制器 件的激光投影仪和激光电视显示。  As shown in FIG. 7, the system is applied to a Full-Frame Displays system, and the three primary color lasers 501, 502, and 503 output a constant power laser beam, and are respectively introduced into the speckle elimination device 305, 306 of the present invention. After being modulated, the relay lenses 701, 704, 707, the plane mirror 708, and the TIR prisms 703, 705, 709 are condensed to the optical modulators DLP 702, 706, 710; the optical modulators DLP 702, 706, 710 are based on each frame. The 2-dimensional image information is modulated to produce a monochrome image; the three primary color images are blended by prism 711 and projected by lens 700 onto screen 800. This application example is suitable for laser projectors and laser TV displays based on optical modulators such as DMD and LCOS.

Claims

权利要求书 Claim
1、 一种基于米氏散射及磁控粒子运动的散斑消除装亶, 其特征在于: 包 括其上设有入射光耦合装置(301 )和透射出射面(303 ) 的封闭式光学反射腔 A speckle removal device based on Mie scattering and magnetron particle motion, comprising: a closed optical reflection cavity having an incident light coupling device (301) and a transmission exit surface (303);
(302) , 封闭式光学反射腔 (302) 除透射出射面 (303 ) 内壁之外的内壁皆 为"镜面"内壁, 封闭式光学反射腔 (302) 内填有充满整个封闭式光学反射腔(302), the closed optical reflection cavity (302) except for the inner wall of the transmission exit surface (303) is a "mirror" inner wall, and the closed optical reflection cavity (302) is filled with the entire closed optical reflection cavity.
(302) 的溶液或溶胶 (401 ) , 且溶液或溶胶 (401 ) 内散布有其线度能引起 入射激光发生米氏散射的磁性介质粒子(402) ; 封闭式光学反射腔 (302)配 设有用以产生磁场的磁场发生装置, 且磁场发生器的电磁铁 (308) 设置于封 闭式光学反射腔 (302) 夕卜。 a solution or sol (401) of (302), and a magnetic medium particle (402) whose linearity can cause Mie scattering of the incident laser is dispersed in the solution or sol (401); the closed optical reflection cavity (302) is disposed There is a magnetic field generating means for generating a magnetic field, and the electromagnet (308) of the magnetic field generator is disposed in the closed optical reflecting chamber (302).
2、 根据权利要求 1所述的基于米氏散射及磁控粒子运动的散斑消除装置. 其特征在于: 所述溶液为有机溶液或无机溶液; 所述溶胶为气溶胶或液溶胶。  2. The speckle reduction device based on Mie scattering and magnetron particle motion according to claim 1. The solution is an organic solution or an inorganic solution; and the sol is an aerosol or a sol.
3、 根据权利要求 1所述的基于米氏散射及磁控粒子运动的散斑消除装置, 其特征在于: 磁性介质粒子 (402) 采用聚苯乙烯磁性微球、 或者二氧化硅磁 性微球、 或者四氧化三铁磁性微球、 或者三氧化二铁磁性微球。  3. The speckle reduction device based on Mie scattering and magnetron particle motion according to claim 1, wherein: the magnetic medium particles (402) are made of polystyrene magnetic microspheres or silica magnetic microspheres. Or ferroferric oxide magnetic microspheres, or ferric oxide magnetic microspheres.
4、 根据权利要求 1所述的基于米氏散射及磁控粒子运动的散斑消除装置, 其特征在于: 封闭式光学反射腔(302) 的透射出射面(303 )表面设有与入射 光束波段匹配的增透膜。  4. The speckle reduction device based on Mie scattering and magnetron particle motion according to claim 1, wherein: the surface of the transmission exit surface (303) of the closed optical reflection cavity (302) is provided with an incident beam band Matching AR coating.
PCT/CN2012/000041 2011-01-29 2012-01-10 Speckle removal device based on mie scattering and motion of magnetically controlled particles WO2012100642A1 (en)

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