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    • 161. 发明授权
    • Device and method for doubling the frequency of elecromagnetic radiation
of a given frequency
    • 给定频率的电磁辐射频率加倍的装置和方法
    • US4867510A
    • 1989-09-19
    • US325029
    • 1989-03-16
    • Peter J. Dobson
    • Peter J. Dobson
    • H01S3/109G02F1/377
    • G02F1/377
    • A device and method for doubling the frequency of electromagnetic radiation of a given frequency are described. The device comprises a substrate (1) on which is provided a first layer (2) and a second layer (3). One of the first and second layers (2) has a plasma oscillation frequency equal to the given frequency for causing an electric field at twice the given frequency to be produced across the device in response to electromagentic radiation at the given frequency being incident on the device normally of the first and second layers (2and 3). A thus-produced electric field is converted to electromagnetic radiation at twice the given frequency by the said other of the first and second layers (3) which forms a waveguide for electromagnetic radiation at twice the given frequency. A further layer (2') similar to the said one layer (2) may be provided so that the said other layer (3) is sandwiched between the said one and further layers (2 and 2').
    • 描述了给定频率的电磁辐射频率加倍的装置和方法。 该装置包括一个衬底(1),其上设置有第一层(2)和第二层(3)。 第一和第二层(2)中的一个具有等于给定频率的等离子体振荡频率,用于响应于以给定频率入射到设备上的电磁辐射而在整个装置上产生两倍于给定频率的电场 通常为第一和第二层(2和3)。 这样产生的电场被第一和第二层(3)中的所述另一个转换成给定频率的两倍的电磁辐射,其形成用于以给定频率两倍的电磁辐射的波导。 可以提供类似于所述一层(2)的另一层(2'),使得所述另一层(3)夹在所述一层和另外层(2和2')之间。
    • 162. 发明授权
    • High-efficiency mode-matched solid-state laser with transverse pumping
and cascaded amplifier stages
    • 具有横向泵浦和级联放大器级的高效模式匹配固态激光器
    • US4837771A
    • 1989-06-06
    • US195713
    • 1988-05-18
    • Thomas M. Baer
    • Thomas M. Baer
    • H01S3/08H01S3/0941H01S3/109
    • H01S3/109H01S3/08H01S3/0941
    • A high efficiency pumping scheme mode matches the TEMOO laser mode volume with a plurality of linearly spaced laser diode pumping sources positioned along a lateral side of a block of laser material. The cavity resonator within the block is configured in a tightly folded zig-zag configuration. Pump radiation from the diode pumping sources is collimated by an optical fiber and the fold angle is selected to mode match the pump radiation to the mode volume.A laser oscillator is followed by one or more cascaded amplifier stages including a block of laser material arranged in a tightly folded zig-zag configuration. Pump radiation from the diode pumping sources is collimated by an optical fiber and the fold angle is selected to mode match the pump radiation to the mode volume.
    • 高效泵浦方案模式将TEM00激光模式体积与沿激光材料块的侧面定位的多个线性间隔的激光二极管泵浦源匹配。 块内的空腔谐振器被配置成紧密折叠的之字形配置。 来自二极管泵浦源的泵浦辐射由光纤校准,并且折叠角度被选择为将泵辐射与模式体积匹配。 激光振荡器之后是一个或多个级联放大器级,其包括以紧凑折叠的之字形配置布置的激光材料块。 来自二极管泵浦源的泵浦辐射由光纤校准,并且折叠角度被选择为将泵辐射与模式体积匹配。
    • 163. 发明授权
    • Diode pumped laser and doubling to obtain blue light
    • 二极管泵浦激光和倍增获得蓝光
    • US4809291A
    • 1989-02-28
    • US907495
    • 1986-09-15
    • Robert L. ByerTso Y. Fan
    • Robert L. ByerTso Y. Fan
    • G02F1/35H01S3/0941H01S3/109H01S3/16H01S5/06H01S3/091
    • H01S3/109G02F2001/3542G02F2001/3546H01S2302/00H01S2303/00H01S3/09415H01S3/1611H01S3/1671
    • A source of coherent blue light comprises a diode laser for pumping a Nd.sup.3+ doped member of lasant material disposed within an optical resonator for exciting the .sup.4 F.sub.3/2 -.sup.4 I.sub.9/2 laser transition of a wavelength within the range of 0.870 to 0.960 .mu.m. The laser radiation within the optical resonator is doubled by means of a doubler crystal of a non-linear, electro-optic material to produce blue light which is then extracted from the optical resonator as an output beam. A thermo-electric cooler is coupled in heat-exchanging relation with the Nd.sup.3+ doped laser material to improve the efficiency and the doubler crystal is temperature controlled for phase matching to the laser radiation within the range of 0.870 to 0.960 .mu.m. The diode pump laser is preferably either a GaAlAs or GaAs diode laser producing pumping radiation of a wavelength of approximately 0.810 .mu.m. In the case of Nd:YAG end pumped laser material, the laser material is preferably doped to have a high an absorption coefficient as possible and its length is chosen to be within the range of 0.5 to 3 mm. In one embodiment, the lasant material and the non-linear, electro-optic material are disposed in separate optical resonators with the laser resonator optically decoupled from the doubler resonator for inhibiting reflection of optical power back to the laser resonator.
    • 相干蓝光源包括二极管激光器,用于泵浦设置在光学谐振器内的惰性材料的Nd3 +掺杂元件,用于激发波长在0.870至0.960μm范围内的4F3 / 2-4I9 / 2激光转换。 光学谐振器内的激光辐射借助于非线性电光材料的倍晶晶体加倍,以产生蓝光,然后将其从光谐振器中提取为输出光束。 热电冷却器与Nd3 +掺杂的激光材料以热交换关系耦合,以提高效率,并且倍增晶体受温度控制,用于激光辐射的相位匹配在0.870至0.960μm的范围内。 二极管泵浦激光器优选地是产生大约0.810μm波长的泵浦辐射的GaAlAs或GaAs二极管激光器。 在Nd:YAG端部泵浦激光材料的情况下,激光材料优选被掺杂以具有尽可能高的吸收系数,并且其长度被选择在0.5至3mm的范围内。 在一个实施例中,将惰性材料和非线性电光材料设置在分离的光学谐振器中,激光谐振器与倍频谐振器光学去耦合,以抑制光功率反射回激光谐振器。