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    • 1. 发明授权
    • System for converting optical beams to collimated flat-top beams
    • 将光束转换成准直平顶梁的系统
    • US06801368B2
    • 2004-10-05
    • US10679058
    • 2003-10-02
    • Hans J. CoufalJohn A. HoffnagleCarl M. Jefferson
    • Hans J. CoufalJohn A. HoffnagleCarl M. Jefferson
    • G02B1318
    • G02B19/0057G02B13/18G02B19/0014G02B27/09G02B27/0927G02B27/0944G02B27/0955G03F7/70075
    • An optical beam transformation system includes a first and a second optical element, each of which has a non-reentrant surface. The system transforms a substantially non-uniform optical input beam (such as a Gaussian) to a substantially uniform output beam. The first and second optical elements are arranged in either a Keplerian or Galilean configuration. The aspheric surface of the second optical element is related to the aspheric surface of the first optical element by a ray-tracing function that maps substantially all of an input light beam that is incident on the first optical element to a collimated output light beam that is output from the second optical element. Preferably, the output light beam has a Fermi-Dirac intensity distribution, and the ray-tracing function maps the input light beam to the output beam out to the (1/e)6 intensity radius of the input light beam.
    • 光束转换系统包括第一和第二光学元件,每个光学元件具有非凹入表面。 系统将基本上不均匀的光输入光束(例如高斯)转换成基本均匀的输出光束。 第一和第二光学元件以开普勒或伽利略配置布置。 第二光学元件的非球面通过光线跟踪功能与第一光学元件的非球面相关,该光线跟踪功能将入射在第一光学元件上的输入光束基本上全部映射到准直的输出光束 从第二光学元件输出。 优选地,输出光束具有费米 - 迪拉克强度分布,并且光线跟踪功能将输入光束映射到输入光束的输出光束的(1 / e)6强度半径。
    • 3. 发明授权
    • Optical recording by energy-induced fractionation and homogenization
    • 通过能量分解和均化进行光学记录
    • US4576895A
    • 1986-03-18
    • US621410
    • 1984-06-18
    • Roger W. BartonHans J. CoufalVictor B. JipsonWen Y. Lee
    • Roger W. BartonHans J. CoufalVictor B. JipsonWen Y. Lee
    • B41M5/26G11B7/00G11B7/004G11B7/0045G11B7/243G11B7/257G11B9/00G11B11/00G03C1/94
    • G11B7/257G11B11/00G11B7/0045G11B7/243G11B9/00G11B2007/25706G11B2007/25708G11B2007/2571G11B2007/25715Y10S430/146
    • A method of and structure for optical recording by energy-induced homogenization or fractionation is disclosed. When the method involves fractionation, a film is provided that contains a homogeneous mixture of a matrix material and an incident energy absorbing material. A spot on the film is treated with sufficient energy in the form of electric fields, radiation or heat, or combinations thereof to effect fractionation and/or homogenization of the film which will undergo further physical state transition only under treatment with additional energy. In a preferred embodiment, the fractionation is effected by laser radiation. The laser irradiated spot becomes inhomogeneous and can be detected by the resulting changes in its optical properties. When the method involves homogenization, a film is provided that contains a inhomogeneous mixture. The energy treated spot in this case becomes homogeneous without undergoing a phase transition between the amorphous and crystalline phases. Numerous combinations of fractionation and homogenization can result in the writing and erasing of information in a storage device.
    • 公开了通过能量均化或分馏进行光学记录的方法和结构。 当该方法包括分馏时,提供包含基质材料和入射能量吸收材料的均匀混合物的膜。 以电场,辐射或热的形式或其组合的形式,以足够的能量对薄膜上的斑点进行处理,以实现膜的分级和/或均化,仅在额外的能量处理下进行进一步的物理状态转变。 在优选的实施方案中,分馏通过激光辐射来实现。 激光照射的斑点变得不均匀,并且可以通过其光学性质的变化来检测。 当该方法包括均化时,提供含有不均匀混合物的膜。 在这种情况下,能量处理的斑点变得均匀,而不会在非晶相和晶相之间经历相变。 分馏和均化的许多组合可导致存储设备中信息的写入和擦除。
    • 4. 发明授权
    • System for converting optical beams to collimated flat-top beams
    • 将光束转换成准直平顶梁的系统
    • US06654183B2
    • 2003-11-25
    • US09917370
    • 2001-07-27
    • Hans J. CoufalJohn A. HoffnagleCarl M. Jefferson
    • Hans J. CoufalJohn A. HoffnagleCarl M. Jefferson
    • G02B1318
    • G02B19/0057G02B13/18G02B19/0014G02B27/09G02B27/0927G02B27/0944G02B27/0955G03F7/70075
    • An optical beam transformation system includes a first and a second optical element, each of which has a non-reentrant surface. The system transforms a substantially non-uniform optical input beam (such as a Gaussian) to a substantially uniform output beam. The first and second optical elements are arranged in either a Keplerian or Galilean configuration. The aspheric surface of the second optical element is related to the aspheric surface of the first optical element by a ray-tracing function that maps substantially all of an input light beam that is incident on the first optical element to a collimated output light beam that is output from the second optical element. Preferably, the output light beam has a Fermi-Dirac intensity distribution, and the ray-tracing function maps the input light beam to the output beam out to the (1/e)6 intensity radius of the input light beam.
    • 光束转换系统包括第一和第二光学元件,每个光学元件具有非凹入表面。 系统将基本上不均匀的光输入光束(例如高斯)转换成基本均匀的输出光束。 第一和第二光学元件以开普勒或伽利略配置布置。 第二光学元件的非球面通过光线跟踪功能与第一光学元件的非球面相关,该光线跟踪功能将入射在第一光学元件上的输入光束基本上全部映射到准直的输出光束 从第二光学元件输出。 优选地,输出光束具有费米 - 迪拉克强度分布,并且光线跟踪功能将输入光束映射到输入光束的输出光束的(1 / e)6强度半径。