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    • 3. 发明授权
    • Loop phase-conjugate mirror for depolarized beams
    • 用于去极化光束的环路相位共轭反射镜
    • US5729380A
    • 1998-03-17
    • US741275
    • 1996-10-30
    • Alexander A. BetinMetin S. Mangir
    • Alexander A. BetinMetin S. Mangir
    • G02F1/35H01S3/083H01S3/10H01S3/108G02B26/08
    • G02F1/3538H01S3/083H01S3/10076
    • A loop four-wave mixing phase conjugator that can be used with depolarized signal beams comprises a polarization separator, a polarization mixer, an optical diode, a gain medium and relay optics that together form a unidirectional laser resonator. In operation, the polarization separator separates a signal beam .epsilon..sub.1 into orthogonally polarized signal beam components .epsilon..sub.11 and .epsilon..sub.12 and directs them to a nonlinear medium. The components propagate through the nonlinear medium and emerge as loop beam .epsilon..sub.2, with orthogonally polarized components .epsilon..sub.2 and .epsilon..sub.22. The polarization mixer mixes the energy from the two orthogonally polarized loop beam components, and relay optics direct the loop beam components back to the nonlinear medium at an angle with respect to the input beam. The loop beam components intersect and optically interfere with signal beam components .epsilon..sub.11 and .epsilon..sub.22 in the nonlinear medium to form gratings. The optical diode and gain medium are positioned in the optical loop so that an oscillation beam .epsilon..sub.3 builds up from optical noise in the resonator and oscillates in a direction counter to the propagation direction of loop beam components .epsilon..sub.21 and .epsilon..sub.22. A portion of oscillation beam .epsilon..sub.3 is transmitted by the gratings, and exits the optical loop as an output beam .epsilon..sub.4. .epsilon..sub.3 is phase conjugate to the input beam .epsilon..sub.1 in both the spatial and polarization senses.
    • 可以与去极化信号光束一起使用的环路四波混频相位共轭器包括一起形成单向激光谐振器的偏振分离器,偏振混频器,光二极管,增益介质和中继光学器件。 在操作中,偏振分离器将信号光束ε1分离成正交偏振信号光束分量ε11和ε12,并将它们引导到非线性介质。 这些分量通过非线性介质传播并出现为环形光束ε2,具有正交极化分量ε2和ε22。偏振混频器混合来自两个正交极化环形光束分量的能量,并且中继光学器将环形光束分量反馈回 非线性介质相对于输入光束成一定角度。 环路光束分量与非线性介质中的信号光束分量ε11和ε22相交并光学地干扰以形成光栅。 光二极管和增益介质被定位在光环路中,使得振荡光束ε3从谐振器中的光噪声构成,并且在与环形光束分量ε21和ε22的传播方向相反的方向上振荡。 振荡光束ε3由光栅传输,并作为输出光束ε4离开光环路.ε3在空间和极化感测中都与输入光束epsilon 1相位共轭。
    • 4. 发明授权
    • Compact phase-conjugate mirror utilizing four-wave mixing in a loop
configuration
    • 紧凑型相位共轭反射镜采用四波混频的环形结构
    • US5726795A
    • 1998-03-10
    • US741274
    • 1996-10-30
    • Alexander A. BetinMetin S. MangirDavid A. Rockwell
    • Alexander A. BetinMetin S. MangirDavid A. Rockwell
    • G02F1/35H01S3/083H01S3/10H01S3/108G02B26/08
    • G02F1/3538H01S3/083H01S3/10076
    • A compact loop four-wave mixing phase conjugator that can be used in practical optical applications comprises a reflective nonlinear cell, relay optics, an optical gain medium, and an optical diode that together form a unidirectional ring laser resonator. In operation, a signal beam .epsilon..sub.1 is directed to the nonlinear cell, where it passes through a nonlinear medium contained within the cell and is reflected out of the cell as loop beam .epsilon..sub.2. The relay optics direct loop beam .epsilon..sub.2 through the optical diode, optical gain medium, and back to the nonlinear cell, where it intersects and optically interferes with the signal beam .epsilon..sub.1 to form a refractive index grating in the nonlinear medium. The optical diode and gain medium are positioned in the loop so that an oscillation beam .epsilon..sub.3 builds up from optical noise in the resonator and oscillates in a direction counter to the propagation direction of loop beam .epsilon..sub.2. A portion of oscillation beam .epsilon..sub.3 is transmitted by the refractive index grating, reflects off the reflective portion of the nonlinear cell and emerges from the cell as phase conjugate output beam .epsilon..sub.4.
    • 可用于实际光学应用的紧凑型环路四波混频相位共轭器包括一起形成单向环形激光谐振器的反射非线性单元,中继光学器件,光学增益介质和光二极管。 在操作中,信号束ε1被引导到非线性单元,其中它穿过包含在单元内的非线性介质,并且被作为环形波束ε2从单元反射出来。中继光学器件通过光学器件直接环形光束 二极管,光学增益介质,并且返回到非线性单元,其中它与信号光束ε1相交并光学地干涉以在非线性介质中形成折射率光栅。 光二极管和增益介质定位在环路中,使得振荡光束ε3从谐振器中的光噪声构成,并且在与环形光束ε2的传播方向相反的方向上振荡。振荡光束ε3的一部分是 由折射率光栅透射,反射出非线性单元的反射部分,并从单元中作为相位共轭输出光束ε4出射。
    • 6. 发明授权
    • Integrated laser head and low inductance pulse forming circuit for
pulsed gas lasers
    • 脉冲气体激光器的集成激光头和低电感脉冲形成电路
    • US4876693A
    • 1989-10-24
    • US686339
    • 1984-12-26
    • David J. LuceroClaudio G. ParazzoliMetin S. Mangir
    • David J. LuceroClaudio G. ParazzoliMetin S. Mangir
    • H01S3/03H01S3/038H01S3/0971
    • H01S3/038H01S3/03H01S3/0971
    • Integrated laser head apparatus is disclosed for producing high energy pulses in pulsed gas lasers. The present invention provides high energy pulses over short time durations suitable for laser rangefinder systems due to an improvement in the arrangement of energy storage capacitors (22, 24) which keeps circuit inductance to a minimum. The pair of nested, ceramic capacitors (22, 24) are substantially cylindrical and are coupled through thin conductive layers (23). The capacitors are charged by a spark gap trigger (14), an inductor (18), and a charging resistor (52). The capacitors (22, 24) enclose a pressure vessel (28) which further encloses a laser resonator (12) including a laser output coupler mirror (42), totally reflective mirror (44), discharge electrodes (32, 34) and a central chamber (30) which contains a pressurized gaseous phase laser medium. The high voltage discharge electrode (32) is disposed coaxially with the surrounding capacitors (22, 24).
    • 公开了用于在脉冲气体激光器中产生高能脉冲的集成激光头装置。 本发明由于能够将电路电感保持最小的储能电容器(22,24)的布置改进而在适用于激光测距系统的短时间内提供高能量脉冲。 一对嵌套陶瓷电容器(22,24)基本上是圆柱形的,并且通过薄导电层(23)耦合。 电容器由火花隙触发器(14),电感器(18)和充电电阻器(52)充电。 电容器(22,24)包围压力容器(28),该压力容器进一步包围激光谐振器(12),该激光谐振器包括激光输出耦合镜(42),全反射镜(44),放电电极(32,34) 包含加压气相激光介质的室(30)。 高电压放电电极(32)与周围的电容器(22,24)同轴配置。
    • 8. 发明授权
    • Design for a Yb-doped CP fiber laser for operating near EDFA absorption
band
    • 设计用于在EDFA吸收带附近操作的Yb掺杂CP光纤激光器
    • US5991314A
    • 1999-11-23
    • US58539
    • 1998-04-10
    • Stanislav I. IonovDennis C. JonesMetin S. Mangir
    • Stanislav I. IonovDennis C. JonesMetin S. Mangir
    • H01S3/067H01S3/094H01S3/106H01S3/16H01S3/30
    • H01S3/0675H01S2302/00H01S2303/00H01S3/094003H01S3/1062H01S3/1608H01S3/1618
    • A Yb-doped cladding pumped fiber laser includes a reflective grating located at each distal end of the laser cavity. Each reflective grating can reflect light propagating inside a fiber core and at a desired wavelength range. A plurality of band-rejecting gratings are disposed between the reflective gratings, whereby the band-rejecting gratings can couple light at an undesired wavelength range and out of the fiber core. When the band-rejecting gratings are in an end-to-end relationship, they are separated by a distance of approximately L whereby L=[(.sigma..sub.e.sup.d +.sigma..sub.a.sup.d)ln 1/T]/[n(.sigma..sub.a.sup.d .sigma..sub.e.sup.u -.sigma..sub.e.sup.d .sigma..sub.a.sup.u)], n is a concentration of ions subject to excitation, .sigma..sub.a.sup.d is an absorption cross section at said desired wavelength range, .sigma..sub.e.sup.u is an emission cross section at said undesired wavelength range, .sigma..sub.e.sup.d is an emission cross section at said desired wavelength range, .sigma..sub.a.sup.u is an absorption cross section at said undesired wavelngth range, and T is a band-rejecting grating transmission factor. The number of band-rejecting gratings is given by N whereby N=d/L.gtoreq.dn (.sigma..sub.a.sup.d .sigma..sub.e.sup.u -.sigma..sub.e.sup.d .sigma..sub.a.sup.u)/[.sigma..sub.e.sup.d +.sigma..sub.a.sup.d) ln 1/T] and d is the length of the laser.
    • Yb掺杂包层泵浦光纤激光器包括位于激光腔的每个远端处的反射光栅。 每个反射光栅可以反射在光纤芯内传播并在期望波长范围内的光。 多个带阻光栅设置在反射光栅之间,由此带状光栅可将不期望的波长范围内的光耦合到光纤芯外。 当带状抑制光栅处于端对端关系时,它们被分开大约L的距离,由此L = [(sigma ed + sigma ad)ln 1 / T] / [n(西格玛西格玛 ed sigma au)],n是受激发的离子的浓度,σad是在所述期望波长范围的吸收截面,σeu是在所述不期望波长范围的发射截面,σed是 所述期望的波长范围,σau是在所述不希望的波长范围的吸收截面,T是带阻光栅传播因子。 带隙光栅的数量由N给出,其中N = d / L> / = dn(σσσσσσσσ/σ) 激光。
    • 10. 发明授权
    • Speckle resistant method and apparatus with chirped laser beam
    • 具有啁啾激光束的防斑方法和装置
    • US5434662A
    • 1995-07-18
    • US173302
    • 1993-12-23
    • David A. RockwellMetin S. Mangir
    • David A. RockwellMetin S. Mangir
    • G01S7/484G01S17/10G01S17/66G01C3/08
    • G01S17/66G01S17/102G01S7/484
    • Laser beam speckle effects are mitigated by frequency chirping a single-mode laser beam, reflecting it off a speckling surface, and then integrating the reflected beam over at least one chirp period. The speckle reduction is comparable to the use of a multi-longitudinal mode beam having a bandwidth similar to the chirped frequency excursion, while leaving the beam compatible with nonlinear optical processes that are not compatible with multi-longitudinal mode beams. Where the nonlinear process is stimulated Brillouin scattering (SBS) phase conjugation, the beam can be chirped at a rate up to the order of ##EQU1## where .DELTA..nu..sub.B is the gain bandwidth and L is the effective SBS interaction length of the phase conjugator, and C is the speed of light. Other nonlinear processes with which the beam may be used include harmonic generation and Raman-based beam cleanup or wavelength conversion.
    • 通过频率啁啾单模激光束,将其从斑点表面反射出来,然后在至少一个啁啾周期上积分反射光束来减轻激光束斑点效应。 斑点减少与使用具有类似于啁啾频率偏移的带宽的多纵向模式波束相当,同时使波束与与多纵向模式波束不兼容的非线性光学过程兼容。 在非线性过程被刺激的布里渊散射(SBS)相位共轭的情况下,波束可以以高达“IMAGE”的速率被啁啾,其中DELTA nu B是增益带宽,L是相位共轭器的有效SBS相互作用长度 ,C是光速。 可以使用光束的其他非线性处理包括谐波生成和基于拉曼的束清除或波长转换。