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    • 1. 发明授权
    • Ultrashort-pulse source with controllable wavelength output
    • 具有可控波长输出的超短脉冲源
    • US06744555B2
    • 2004-06-01
    • US09042666
    • 1998-03-17
    • Almantas GalvanauskasMark A. ArboreMartin M. FejerDonald J. Harter
    • Almantas GalvanauskasMark A. ArboreMartin M. FejerDonald J. Harter
    • G02F1365
    • G02F1/3132G01B9/02007G01B9/02014G01B9/02091G02F1/3137G02F1/335G02F1/3532G02F1/395G02F2001/3548G02F2201/124G02F2203/26
    • A multiple-wavelength ultrashort-pulse laser system includes a laser generator producing ultrashort pulses at a fixed wavelength, and at least one and preferably a plurality of wavelength-conversion channels. Preferably, a fiber laser system is used for generating single-wavelength, ultrashort pulses. An optical split switch matrix directs the pulses from the laser generator into at least one of the wavelength conversion channels. An optical combining switch matrix is disposed downstream of the wavelength-conversion channels and combines outputs from separate wavelength-conversion channels into a single output channel. Preferably, waveguides formed in a ferroelectric substrate by titanium indiffusion (TI) and/or proton exchange (PE) form the wavelength-conversion channels and the splitting and combining matrices. Use of the waveguide allows efficient optical parametric generation to occur in the wavelength-conversion channels at pulse energies achievable with a mode-locked laser source. The multiple-wavelength laser system can replace a plurality of different, single-wavelength laser systems. In its simplest form, the system can be used to convert the laser wavelength to a more favorable wavelength. For example, pulses generated at 1.55 &mgr;m by a mode-locked erbium fiber laser can be converted to 1.3 &mgr;m for use in optical coherence tomography or to wavelengths suitable for use in a display, printing or machining system.
    • 多波长超短脉冲激光系统包括产生固定波长的超短脉冲的激光发生器和至少一个,优选多个波长转换通道。 优选地,光纤激光系统用于产生单波长超短脉冲。 光分路开关矩阵将来自激光发生器的脉冲引导到至少一个波长转换通道。 光学组合开关矩阵设置在波长转换通道的下游,并将来自分离的波长转换通道的输出组合成单个输出通道。 优选地,通过钛扩散(TI)和/或质子交换(PE)在铁电衬底中形成的波导形成波长转换通道和分离和组合矩阵。 波导的使用允许在波长转换通道中以在锁模激光源可实现的脉冲能量下发生有效的光参量产生。 多波长激光系统可以代替多个不同的单波长激光系统。 在其最简单的形式中,该系统可用于将激光波长转换成更有利的波长。 例如,通过模式锁定铒光纤激光器在1.55μm生成的脉冲可以转换为1.3μm,用于光学相干断层摄影或适用于显示,印刷或加工系统的波长。
    • 3. 发明授权
    • Aperiodic quasi-phasematching gratings for chirp adjustments and
frequency conversion of ultra-short pulses
    • 用于啁啾调节和超短脉冲频率转换的非周期准准同步光栅
    • US5815307A
    • 1998-09-29
    • US824032
    • 1997-03-26
    • Mark A. ArboreMartin M. Fejer
    • Mark A. ArboreMartin M. Fejer
    • G02F1/35G02F1/37H01S3/00G02B5/18
    • G02F1/3544H01S3/0057G02F1/37G02F2001/3548G02F2203/25G02F2203/26
    • An apparatus and method for simultaneous chirp adjustment and frequency conversion of an ultra-short input optical pulse A.sub.1 characterized by a center angular frequency .omega..sub.1,0 in a non-linear optical material with a quasi-phasematching (QPM) grating exhibiting an aperiodic pattern of regions D.sub.j constituting a grating. Passing the ultra-short input optical pulse A.sub.1 through the grating gives rise to a chirp-adjusted and frequency-converted output optical pulse A.sub.2. In the preferred embodiment the non-linear optical material is a Second Harmonic Generator (SHG) such that the output optical pulse A.sub.2 generated from the input optical pulse A.sub.1 is a chirp-adjusted second harmonic of said ultra-short input optical pulse A.sub.1. In the general case the method and apparatus use a transfer function D(.OMEGA.) derived from the equation: A.sub.2 (.OMEGA.)=D(.OMEGA.).multidot.A.sub.1.sup.2 (.OMEGA.), where A.sub.1.sup.2 (.OMEGA.) is the Fourier transform of the square of input optical pulse A.sub.1 and A.sub.2 (.OMEGA.) is the Fourier transform of output optical pulse A.sub.2, to engineer gratings for frequency-conversion and chirp-adjustment.
    • 一种在非线性光学材料中具有中心角频率ω1,0的特征的超短输入光脉冲A1的同步啁啾调节和频率转换的装置和方法,其具有呈非周期性模式的准正交匹配(QPM)光栅 的区域Dj构成光栅。 通过光栅传递超短输入光脉冲A1产生啁啾调节和频率转换的输出光脉冲A2。 在优选实施例中,非线性光学材料是第二谐波发生器(SHG),使得从输入光脉冲A1产生的输出光脉冲A2是所述超短输入光脉冲A1的啁啾调节二次谐波。 在一般情况下,方法和装置使用从以下等式导出的传递函数+ E,Cir D + EE(OMEGA):+ E,cir A + EE 2(OMEGA)= + E,cir D + EE(OMEGA)xA + E,cir 12 + EE(OMEGA),其中A + E,cir 12 + EE(OMEGA)是输入光脉冲A1和+ E的平方的傅里叶变换,cir A + EE 2(OMEGA)是傅立叶 转换输出光脉冲A2,工程光栅进行变频和啁啾调节。
    • 4. 发明授权
    • Generation of terahertz radiation in orientation-patterned semiconductors
    • 在定向图案化的半导体中产生太赫兹辐射
    • US07339718B1
    • 2008-03-04
    • US11357722
    • 2006-02-17
    • Konstantin L. VodopyanovYun-Shik LeeVladimir G. KozlovMartin M. Fejer
    • Konstantin L. VodopyanovYun-Shik LeeVladimir G. KozlovMartin M. Fejer
    • G02F1/35G02F2/02
    • G02F1/39G02F1/3558G02F2203/13
    • A method for generating THz radiation comprises illuminating a semiconductor crystal with an optical pulse train. The semiconductor crystal comprises alternating parallel crystal domains, with each domain having a crystal orientation inverted with respect to adjacent domains. The optical pulse train propagates substantially perpendicularly relative to domain boundaries in the semiconductor crystal. The THz radiation is generated from the optical pulse train by optical down-conversion mediated by the semiconductor crystal. Optical path lengths through the crystal domains at least in part determine a frequency of the generated THz radiation. THz generation efficiency may be enhanced by placing the semiconductor crystal within an external resonant cavity, by placing the semiconductor crystal within a laser cavity, or by placing the semiconductor crystal within an OPO cavity. The semiconductor crystal may comprise zinc-blende, III-V, or II-VI semiconductor.
    • 用于产生太赫兹辐射的方法包括用光脉冲串照射半导体晶体。 半导体晶体包括交替的平行晶体畴,每个畴具有相对于相邻畴反转的晶体取向。 光脉冲串相对于半导体晶体中的畴边界基本垂直地传播。 通过由半导体晶体介导的光学下变频从光脉冲串产生太赫兹辐射。 通过晶体域的光路长度至少部分地确定所产生的太赫兹辐射的频率。 通过将半导体晶体放置在激光腔内,或通过将半导体晶体放置在OPO腔内,可以将半导体晶体放置在外部谐振腔内来提高太赫兹发生效率。 半导体晶体可以包括闪锌矿,III-V或II-VI半导体。
    • 5. 发明授权
    • Nonlinear frequency mixer using quasi-phase-matching gratings having beam-modifying patterns
    • 使用具有光束修改图案的准相位匹配光栅的非线性混频器
    • US06930821B2
    • 2005-08-16
    • US10440490
    • 2003-05-16
    • Jonathan R. KurzMartin M. Fejer
    • Jonathan R. KurzMartin M. Fejer
    • G02F1/37G02F1/377G02F1/39
    • G02F1/3775G02F2001/372
    • A method and a nonlinear frequency mixer employing the method to generate at least one output light from at least one input light with the aid of a quasi-phase-matching (QPM) grating for quasi-phase-matching the input and output light involved in a nonlinear frequency mixing operation such as three-wave mixing, four-wave mixing or other nonlinear operation mediated by a susceptibility of the nonlinear optical material. The QPM grating has a beam-modifying pattern with features for wave front shaping. More specifically, the features shape the wave fronts of the output light by diffraction or phase front shaping to thereby modify its propagation. This modification of propagation can be used to steer, focus, defocusing, split and/or collimate the output light. The features themselves can have various geometric shapes and sizes, even on the order of the wavelength of the output light, and they can include domains exhibiting a nonlinear optical susceptibility χ, such as the second-order susceptibility χ(2), domain edges, and/or spacings between such domains.
    • 一种采用该方法的方法和非线性频率混合器,用于借助于准相位匹配(QPM)光栅从至少一个输入光产生至少一个输出光,以准相相匹配参与的输入和输出光 由非线性光学材料的磁化率介导的三波混频,四波混频或其他非线性运算的非线性频率混合操作。 QPM光栅具有波束修正图案,具有用于波前成形的特征。 更具体地,这些特征通过衍射或相位前置成形来形成输出光的波前,从而改变其传播。 传播的这种修改可用于引导,聚焦,散焦,分离和/或校准输出光。 特征本身可以具有各种几何形状和尺寸,即使在输出光的波长的数量级上,它们也可以包括显示出非线性光学敏感性chi的畴,例如二次磁化率chi(2) / SUP>,域边缘和/或这些域之间的间隔。
    • 7. 发明授权
    • Electric field domain patterning
    • 电场域图案化
    • US5800767A
    • 1998-09-01
    • US307867
    • 1994-09-16
    • Robert L. ByerMartin M. FejerGregory D. MillerLawrence E. Myers
    • Robert L. ByerMartin M. FejerGregory D. MillerLawrence E. Myers
    • G02F1/355B29C71/00
    • G02F1/3558
    • A method of domain patterning a body of ferroelectric material. The method includes the steps of adhering spaced conducting strips to a surface of said body; covering portions of said surface of said body between said strips with material which is insulative relative to electric current produced when an electric field configuration is created in said body and which controls the formation of fringe electric field components in said material; and applying potentials simultaneously to said conducting strips and to a surface of said insulative material to create an electric field configuration in said body whereby said strips define said electric field configuration within said body and wherein said insulating material between said strips defines a potential within said body which is generally the same as the potential applied to said conducting strips.
    • 铁电材料体的域图案化方法。 该方法包括将间隔开的导电条粘合到所述主体的表面上的步骤; 在所述条带之间覆盖所述主体的所述表面的部分,所述材料相对于在所述主体中产生电场结构而产生的电流是绝缘的,并且控制所述材料中的边缘电场分量的形成; 以及将电位同时施加到所述导电条和所述绝缘材料的表面以在所述主体中产生电场结构,由此所述条限定所述主体内的所述电场结构,并且其中所述条之间的所述绝缘材料限定所述主体内的电位 其通常与施加到所述导电条上的电位相同。