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    • 2. 发明授权
    • All solid state optical cryocooler using intracavity optically pumped semiconductor lasers and a method of making the same
    • 所有使用腔内光泵浦半导体激光器的固态光学低温冷却器及其制造方法
    • US08720219B1
    • 2014-05-13
    • US12984780
    • 2011-01-05
    • Mansoor Sheik-Bahae
    • Mansoor Sheik-Bahae
    • F25D23/00F25B21/00H01S3/04
    • F25B23/00H01S3/0007H01S3/025H01S3/0408H01S3/042H01S3/0604H01S3/061H01S3/0615H01S3/09415H01S5/141H01S5/183
    • A device and corresponding method for cooling electronics is disclosed. The device is an all-solid-state optical cryocooler and can include an optically pumped semiconductor laser (OPSL); a cavity configured to receive and control absorption of the optically pumped semiconductor laser, the cavity having a high reflection (HR) surface and an anti-reflection (AR) surface; and a doped crystal housed within the cavity, the doped crystal configured to cool in response to input of the optically pumped semiconductor laser. The method can include supplying an intracavity optically pumped semiconductor lasers to a doped crystal within a cavity; and configuring the cavity to include a high reflection (HR) surface and an anti-reflection (AR) surface, the HR surface and AR surface formed on or in connection with the doped crystal to increase pump light absorption at the crystal within the cavity.
    • 公开了一种用于冷却电子设备的装置和相应的方法。 该器件是全固态光学低温冷却器,并且可以包括光泵浦半导体激光器(OPSL); 被配置为接收和控制所述光泵浦半导体激光器的吸收的空腔,所述空腔具有高反射(HR)表面和抗反射(AR)表面; 并且掺杂晶体容纳在腔内,掺杂晶体被配置为响应于光泵浦半导体激光器的输入而冷却。 该方法可以包括向空腔内的掺杂晶体提供腔内光泵浦半导体激光器; 并且将所述空腔配置为包括高反射(HR)表面和抗反射(AR)表面,所述HR表面和AR表面形成在所述掺杂晶体上或与所述掺杂晶体结合,以增加在所述腔内的晶体处的泵浦光吸收。
    • 5. 发明授权
    • Non-exothermic quasi-two level laser
    • 非放热准二级激光器
    • US06370172B1
    • 2002-04-09
    • US09472012
    • 1999-12-27
    • Steven R. Bowman
    • Steven R. Bowman
    • H01S304
    • H01S3/091H01S3/0408H01S3/16H01S3/1601
    • A method for selecting laser and pump frequencies for a quasi-two level solid state laser with a selected laser host and operating the laser with the selected laser and pump frequencies, the host having a fluorescence probablility P(&ngr;) over a frequency range from &ngr;i to &ngr;f, has the steps: (a) determining for the laser host, a power weighted average fluorescence frequency given by ⟨ v F ⟩ = 1 ( v f - v i ) ⁢ ∫ v i v f ⁢ v · P ⁡ ( v ) ⁢   ⁢ ⅆ v ; (b) selecting an output frequency &ngr;L for the quasi-two level solid state laser to satisfy the expression &ngr;L , and tuning the laser for laser emission at the &ngr;L; and (c) selecting a pump frequency &ngr;P for the quasi-two level solid state laser to satisfy the expression &ngr;L , and optically pumping the laser host with a laser pump to produce laser emission at the &ngr;L. This invention will provide athermal laser operation.
    • 一种用于选择具有所选择的激光主机的准二级固态激光器的激光和泵浦频率的方法,并且以选定的激光和泵浦频率操作激光器,该主机在频率范围内具有荧光可能性P(&ngr) &ngr; i to&ngr; f,具有以下步骤:(a)确定激光主机,由(b)选择输出频率&ngr; L为准二级给出的功率加权平均荧光频率< 固态激光器满足表达式“L <<&ngr; F>,并调谐激光器的激光发射在” 和(c)为准二级固态激光器选择泵浦频率&ngr; P,以满足表达式&ngr; L <&ngr; P <<&ngr; F>,并用激光泵光学泵浦激光主机以产生 激光发射。 本发明将提供无热激光操作。
    • 9. 发明授权
    • Optical refrigerator using reflectivity tuned dielectric mirrors
    • 使用反射率调谐电介质镜的光学冰箱
    • US6041610A
    • 2000-03-28
    • US289419
    • 1999-04-09
    • Bradley C. EdwardsMelvin I. BuchwaldRichard I. Epstein
    • Bradley C. EdwardsMelvin I. BuchwaldRichard I. Epstein
    • F25B23/00G02B7/18H01S3/00H01S3/04F25D23/00
    • F25B23/003F25B23/00G02B7/1815H01S3/0007H01S3/04H01S3/0408
    • Optical refrigerator using reflectivity-tuned dielectric mirrors. Selected working materials can be optically pumped using monochromatic radiation such that the resulting fluorescence has an average photon energy higher than that of the pumping radiation; that is, net anti-Stokes fluorescence. If the quantum efficiency is sufficiently high, the working material will cool and optical refrigeration can be achieved. Parallel mirrored faces are employed to increase the optical path of the incident pumping radiation within the working material by multiple reflections. Reflectivity-tuned dielectric mirrors which allow higher-energy fluorescence photons to readily escape from the working material while inhibiting the escape of the lower-energy photons which are consequently partially trapped in the working material and ultimately reabsorbed and refluoresced at higher energies are employed. This increases the optical refrigerator efficiency. An efficient geometry for the cooling material is a disk having a large diameter and a small height, since the fluorescence can predominantly escape through the tuned mirror on one end face of the working material. An alternative cooling element could be approximately cubic with tuned mirrors on the sides as well as on one end. In another embodiment of the invention, photocells are used to convert escaping fluorescence energy into electricity, thereby reducing the power requirements of the optical refrigerator and reducing the amount of waste that must be removed from the vicinity of the working material.
    • 使用反射率调谐电介质镜的光学冰箱。 所选择的工作材料可以使用单色辐射进行光泵浦,使得所得荧光的平均光子能量高于泵浦辐射的平均光子能量; 那就是净反斯托克斯荧光。 如果量子效率足够高,则工作材料将冷却并且可以实现光学制冷。 采用平行镜面以通过多次反射来增加工作材料内的入射泵浦辐射的光路。 反射率调谐的电介质反射镜允许更高能量的荧光光子容易地从工作材料逸出,同时抑制低能量光子的逸出,因此部分地被捕获在工作材料中并且最终在较高能量下被再吸收和反射。 这提高了光学冰箱的效率。 用于冷却材料的有效几何形状是具有大直径和小高度的盘,因为荧光可以主要通过工作材料的一个端面上的调谐反射镜逃逸。 替代的冷却元件可以是近似立方体,在侧面以及一端具有调整的反射镜。 在本发明的另一个实施例中,光电池用于将荧光能量转换成电能,从而降低光学冰箱的功率需求并减少必须从工作材料附近去除的废物量。