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    • 91. 发明授权
    • Wavelength selectable laser oscillator in wavelength tunable laser
    • 波长可选激光振荡器在波长可调激光器中
    • US5923685A
    • 1999-07-13
    • US848162
    • 1997-04-29
    • Kazuyuki AkagawaSatoshi WadaHideo Tashiro
    • Kazuyuki AkagawaSatoshi WadaHideo Tashiro
    • H01S3/10G02F1/11H01S3/081H01S3/094H01S3/106H01S3/108H01S3/16H01S3/117
    • H01S3/1068G02F1/116H01S3/081H01S3/094
    • An object of the present invention is to provide a wavelength selectable laser oscillator in wavelength tunable laser by which high-speed tuning of wavelength can be achieved while utilizing continuous-wave laser beam as the excited laser beam. The wavelength selectable laser oscillator in wavelength tunable laser comprises a laser resonator composed of opposed mirrors each having a prescribed reflectivity on the outgoing side and a total reflection mirror which does not transmit light, but reflects the light; a wavelength tunable laser medium disposed in the laser resonator and capable of laser oscillation in a wavelength zone of a prescribed range; an acousto-optical crystal disposed in the laser oscillator and to which is inputted the outgoing light from the wavelength tunable laser medium; an acoustic wave inputting means mounted on the acousto-optical crystal and for inputting an acoustic wave to the acousto-optical crystal; and a continuous-wave laser for inputting excited laser beam into the laser resonator; the laser beam outputted from the mirrors on the outgoing side being utilized as the outgoing laser beam from the laser resonator.
    • 本发明的目的是提供一种波长可调激光器中的波长可选激光振荡器,通过该波长可调激光器可以在利用连续波激光束作为激发激光束的同时实现波长的高速调谐。 波长可调激光器中的波长可选择激光振荡器包括由对置的反射镜组成的激光谐振器,每个反射镜在出射侧具有规定的反射率,而全反射镜不透光但反射光; 设置在所述激光谐振器中并能够在规定范围的波长区域内进行激光振荡的波长可调激光介质; 设置在激光振荡器中的声光晶体,并从波长可调激光介质输入出射光; 声波输入装置,安装在声光晶体上,并将声波输入声光晶体; 以及用于将激发的激光束输入激光谐振器的连续波激光器; 从出射侧的反射镜输出的激光束被用作来自激光谐振器的输出激光束。
    • 92. 发明授权
    • External resonator type wavelength- tunable light source
    • 外部谐振器型波长可调光源
    • US5862162A
    • 1999-01-19
    • US825713
    • 1997-03-19
    • Minoru Maeda
    • Minoru Maeda
    • H01S3/08H01S3/06H01S3/106H01S5/00H01S5/026H01S5/10H01S5/14H01S3/10
    • H01S5/141H01S5/026H01S5/1032H01S5/142
    • A wavelength-tunable light source is provided, by which an output beam of a stable wavelength can be obtained even if a driving condition of the optical amplifier is changed, and in which stable wavelength tuning without mode hopping can be performed. The light source comprises: an optical amplifier, both end faces thereof being antireflection-processed, for generating a natural emission beam from one end face of the amplifier, and for amplifying a beam input into the one end face and outputting the amplified beam from the other end face of the amplifier; an optical amplifier drive circuit for driving the optical amplifier; an optical resonance reflector for resonating the natural emission beam output from the optical amplifier at an optical resonance wavelength, and reflecting the resonated beam to the one end face of the optical amplifier; a wavelength controller for controlling the optical resonance wavelength of the optical resonance reflector; a resonance length controller for controlling a resonance length of the optical resonance reflector; and a beam outputter for extracting a beam, which was reflected by the optical resonance reflector, amplified by the optical amplifier, and output from the other end face of the optical amplifier, and outputting the extracted beam.
    • 提供了一种波长可调光源,即使在光放大器的驱动条件改变的情况下也可以获得稳定波长的输出光束,并且可以执行不进行模式跳变的稳定波长调谐。 光源包括:光放大器,其两个端面经过防反射处理,用于从放大器的一个端面产生自然发射光束,并且用于放大输入到一个端面的光束,并将放大的光束从 放大器的另一端面; 用于驱动光放大器的光放大器驱动电路; 光谐振反射器,用于以光学共振波长谐振从光放大器输出的自然发射光束,并将谐振光束反射到光放大器的一个端面; 波长控制器,用于控制光学谐振反射器的光学谐振波长; 谐振长度控制器,用于控制光学谐振反射器的谐振长度; 以及光束输出器,用于提取由光学共振反射器反射的光束,由光放大器放大,并从光放大器的另一端面输出,并输出提取的光束。
    • 95. 发明授权
    • Microphotonic acousto-optic tunable laser
    • 微波声光可调激光器
    • US5724373A
    • 1998-03-03
    • US751137
    • 1996-11-15
    • Kok-Wai Chang
    • Kok-Wai Chang
    • G02F1/125H01S3/106H01S3/117H01S3/10
    • G02F1/125H01S3/1068
    • A tunable laser that includes a laser amplifier and an acousto-optic filter (AOTF). The AOTF includes a waveguide having first and second ports. A first polarization filter passes light of a first polarization state, the first polarization filter being located between the laser amplifier and the first port of the AOTF. The laser also includes a first asymmetrical polarization rotator located between the first port of the AOTF and the first polarization filter. The first asymmetrical polarization rotator rotates the polarization of light traveling from the first port of the AOTF to the first polarization filter by 90.degree. while leaving unchanged the polarization of light traveling from the first polarization filter to the first port of the AOTF. A mirror reflects light leaving the second port of the AOTF back into the second port of the AOTF. A second polarization filter located between the mirror assembly and the second port of the AOTF passes light of a second polarization state which is orthogonal to the first polarization. A second asymmetrical polarization rotator is located between the second port of the AOTF and the second polarization filter. The second asymmetrical polarization rotator rotates the polarization of light traveling from the second polarization filter to second port of the AOTF by 90.degree. while leaving unchanged the polarization of light traveling from the second port of the AOTF to the second polarization filter.
    • 包括激光放大器和声光滤波器(AOTF)的可调谐激光器。 AOTF包括具有第一和第二端口的波导。 第一偏振滤光器通过第一偏振状态的光,第一偏振滤光器位于激光放大器和AOTF的第一端口之间。 激光器还包括位于AOTF的第一端口和第一偏振滤光器之间的第一不对称偏振旋转器。 第一不对称偏振旋转器将从AOTF的第一端口传播到第一偏振滤光器的光的偏振旋转90度,同时保持从第一偏振滤光器传播到AOTF的第一端口的光的偏振。 镜子反射离开AOTF的第二个端口的光返回到AOTF的第二个端口。 位于反射镜组件和AOTF的第二端口之间的第二偏振滤光器通过与第一偏振正交的第二偏振状态的光。 第二不对称偏振旋转器位于AOTF的第二端口和第二偏振滤光器之间。 第二不对称偏振旋转器将从第二偏振滤光器传播的光的偏振旋转90°的第二端口,同时保持从AOTF的第二端行进到第二偏振滤光器的光的偏振。
    • 96. 发明授权
    • Solid state system for frequency conversion using raman-active media and
non-linear media
    • 使用拉曼活动介质和非线性介质进行变频的固态系统
    • US5673281A
    • 1997-09-30
    • US646983
    • 1996-04-20
    • Robert L. Byer
    • Robert L. Byer
    • H01S3/098H01S3/106H01S3/108H01S3/11H01S3/30
    • H01S3/1086H01S3/08036H01S3/106H01S3/115
    • A solid state system for converting the frequency of light emitted in the form of a laser beam using Stimulated Raman Scattering (SRS) and non-linear conversion. A solid Raman-active medium disposed inside the laser resonator shifts the frequency of the laser beam by a characteristic frequency of the medium to generate a Raman beam in accordance with the SRS effect. Another solid non-linear medium is disposed in the laser resonator for shifting the frequency of the Raman beam to generate an output beam at the desired frequency. The solid non-linear medium is a Second Harmonic Generator (SHG), a Sum Frequency Generator (SFG) or a Difference Frequency Generator (DFG) and can also generate an output beam corresponding to the sum output of the laser beam and the Raman beam. The solid Raman-active medium and the solid-non linear medium can be positioned inside a separate secondary resonator to achieve high conversion efficiency. The system is compatible with Q-switching and frequency tuning for ensuring suitable output beam parameters, and is well-suited for guide star applications.
    • 一种固态系统,用于使用激励拉曼散射(SRS)和非线性转换来转换以激光束形式发射的光的频率。 设置在激光谐振器内部的固体拉曼活性介质通过介质的特征频率移动激光束的频率,以根据SRS效应产生拉曼光束。 在激光谐振器中设置另一固体非线性介质,用于移动拉曼光束的频率以产生所需频率的输出光束。 固体非线性介质是第二谐波发生器(SHG),和频发生器(SFG)或差分频率发生器(DFG),并且还可以产生对应于激光束和拉曼光束的和输出的输出光束 。 固体拉曼活性介质和固体非线性介质可以位于单独的次级谐振器内部,以实现高转换效率。 该系统兼容Q开关和频率调谐,以确保合适的输出光束参数,非常适合导星应用。
    • 98. 发明授权
    • Laser amplifying system
    • 激光放大系统
    • US5553088A
    • 1996-09-03
    • US172126
    • 1993-12-22
    • Uwe BrauchAdolf GiesenAndreas VossKlaus Wittig
    • Uwe BrauchAdolf GiesenAndreas VossKlaus Wittig
    • H01S3/04H01S3/042H01S3/06H01S3/07H01S3/081H01S3/0941H01S3/106H01S3/109H01S3/23
    • H01S3/109H01S3/042H01S3/0604H01S3/07H01S3/081H01S3/0941H01S3/1062H01S3/025H01S3/0405H01S3/08H01S3/083H01S3/094053H01S3/094057H01S3/09408H01S3/2333
    • A laser amplifying system is provided having a solid body arranged in a laser radiation field and including a laser active material that is pumped with a pumping light source. The solid body has a cooling surface and transfers heat created therein to a solid cooling element via the cooling surface. In this manner, a temperature gradient results in the solid body in a direction towards the cooling surface. The solid cooling element forms a carrier for the solid body. The laser radiation field propagates approximately parallel to the temperature gradient in the solid body. By enabling heat to be transferred to the solid cooling element via the cooling surface, this structure enables the solid body to be pumped at a high pumping power. Further, since the laser radiation field propagates approximately parallel to the temperature gradient in the solid body, the radiation field sees the same temperature gradient in all cross-sectional areas. Thus, the temperature gradient does not lead to an adverse effect on the beam quality of the laser radiation field at high pumping power.
    • 提供一种激光放大系统,其具有布置在激光辐射场中的实体,并且包括用泵浦光源泵浦的激光活性材料。 固体具有冷却表面,并通过冷却表面将产生的热量传递给固体冷却元件。 以这种方式,温度梯度导致固体在朝向冷却表面的方向上。 固体冷却元件形成用于固体的载体。 激光辐射场大致平行于固体中的温度梯度传播。 通过使得热能够经由冷却表面传递到固体冷却元件,这种结构使得能够以高泵送功率泵送固体。 此外,由于激光辐射场大致平行于固体中的温度梯度传播,因此辐射场在所有横截面积中看到相同的温度梯度。 因此,在高泵浦功率下,温度梯度不会对激光辐射场的光束质量造成不利影响。