会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 31. 发明授权
    • Multiple channel optical frequency mixers for all-optical signal processing
    • 用于全光信号处理的多通道光混频器
    • US07009759B2
    • 2006-03-07
    • US09821701
    • 2001-03-28
    • Ming-Hsien ChouKrishnan ParameswaranMartin M. Fejer
    • Ming-Hsien ChouKrishnan ParameswaranMartin M. Fejer
    • G02F1/365
    • G02F1/3544G02F1/365
    • A multi-channel optical frequency mixer for all-optical signal processing and a method for engineering the same. The multi-channel mixer uses a nonlinear optical material exhibiting an effective nonlinearity deff whose spatial distribution is defined by a quasi-phase-matching grating, e.g., a QPM grating. The spatial distribution is defined such that its Fourier transform to the spatial frequency domain defines at least two wavelength channels which are quasi-phase-matched for performing optical frequency mixing. The wavelength channels correspond to dominant Fourier components and the Fourier transform is appropriately adjusted using grating parameters such as grating periods, phase reversal sequences and duty cycles to include an odd or even number of dominant Fourier components. The multi-channel mixer can perform frequency mixing operations such as second harmonic generation (SHG), difference frequency generation (DFG), sum frequency generation (SFG), and parametric amplification.
    • 一种用于全光信号处理的多通道光混频器及其工程方法。 多通道混频器使用表现出有效非线性的非线性光学材料,其空间分布由准相位匹配光栅例如QPM光栅限定。 定义空间分布,使得其对空间频域的傅立叶变换定义了至少两个准相位匹配用于执行光频率混合的波长通道。 波长通道对应于显性傅立叶分量,并且使用诸如光栅周期,相位反转序列和占空比的光栅参数适当地调整傅立叶变换,以包括奇数或偶数数量的显性傅立叶分量。 多通道混频器可以执行诸如二次谐波发生(SHG),差频产生(DFG),和频产生(SFG)和参数放大之类的混频操作。
    • 34. 发明授权
    • Electric field domain patterning
    • 电场域图案化
    • US6156255A
    • 2000-12-05
    • US111058
    • 1998-07-07
    • Robert L. ByerMartin M. FejerGregory D. MillerLawrence E. Myers
    • Robert L. ByerMartin M. FejerGregory D. MillerLawrence E. Myers
    • G02F1/355G01B15/00H05B6/00
    • G02F1/3558
    • A method of patterning domains within a body of a ferroelectric material includes the application of an electric field thereto via spaced conductors. Prior to applying the electric field to the material effects on the patterning of the existence of fringe electric field components which will be created in said body by said application of an electric field, surface treatments, and relative geometries of the body and the conductors are examined. The steps of this examination include:(a) characterizing the ferroelectric material byfirst measuring the breakdown field as a function of pulse width,determining the domain wall velocity as a function of electric field strength while simultaneously measuring the nucleation statistics,determining the hysteresis of the body relative to several candidate frequencies, andmeasuring the spontaneous polarization in the body, and the body's conductivity and permittivity;(b) characterizing various possible surface treatments bymeasuring the ferroelectric properties for the surface treatments, andidentifying a desired surface treatment with the most extreme values of .eta.v.sup.2 (E), wherein .eta. is the nucleation rate, v is the velocity at which the surface is patterned and E is the electric field,(c) selecting said relative geometries to minimize the formation of fringe electric field components formed in said body by the electric field application; and(d) applying the desired surface treatment to the body.
    • 在铁电材料的主体内构图区域的方法包括通过间隔的导体向其施加电场。 在将电场应用于对通过施加电场在所述主体中产生的边缘电场分量的存在的图案化的材料效应之后,检查物体和导体的表面处理和相对几何形状 。 该检查的步骤包括:(a)通过首先测量击穿场作为脉冲宽度的函数来表征铁电材料,确定畴壁速度作为电场强度的函数,同时测量成核统计,确定磁滞 身体相对于几个候选频率,并测量身体的自发极化,以及身体的电导率和介电常数; (b)通过测量表面处理的铁电性能来表征各种可能的表面处理,并用eta v2(E)的最极值来鉴定所需的表面处理,其中η是成核速率,v是 表面被图案化并且E是电场,(c)选择所述相对几何形状以通过电场施加使形成在所述主体中的条纹电场分量的形成最小化; 和(d)对身体施加所需的表面处理。
    • 36. 发明授权
    • Atomic absorption apparatus using a phase-modulated light beam
    • 使用相位调制光束的原子吸收装置
    • US5530541A
    • 1996-06-25
    • US396215
    • 1995-02-28
    • Charles H. AhnMalcolm R. BeasleySteven J. BenerofeMartin M. FejerRobert H. HammondWeizhi Wang
    • Charles H. AhnMalcolm R. BeasleySteven J. BenerofeMartin M. FejerRobert H. HammondWeizhi Wang
    • G01J3/433G01N21/31G01N21/39
    • G01N21/3103G01J3/4338
    • An atomic absorption apparatus using a laser for producing a light beam having a characteristic frequency f, typically ranging from several MHz to several GHz, and a characteristic polarization for measuring the absorption of that light beam by atoms of interest. The apparatus has a modulator to generate a modulating signal to modulate the characteristic frequency f and produce a phase-modulated light beam. The apparatus includes a domain where the specific atoms are located. This domain is positioned in the path of the phase-modulated light beam such that the phase-modulated light beam encounters the specific atoms when passing through the domain and some of the specific atoms absorb a portion of the phase-modulated light beam. Typically, the domains containing the atoms of interest include process chambers for vacuum coating, ion milling, sputtering, mass spectroscopy vapor coating or deposition, and the like. The amount of light absorbed depends on the motion of the atoms relative to the phase-modulated light beam.
    • 一种使用激光产生具有特征频率f(通常为几MHz至几GHz)的光束的原子吸收装置,以及用于测量该光束被感兴趣原子吸收的特征极化。 该装置具有调制器以产生调制信号以调制特征频率f并产生相位调制光束。 该装置包括特定原子所在的区域。 该域位于相位调制光束的路径中,使得相位调制光束在通过畴时遇到特定原子,并且一些特定原子吸收相位调制光束的一部分。 通常,包含感兴趣原子的结构域包括用于真空涂覆,离子研磨,溅射,质谱法蒸镀或沉积的处理室。 吸收的光量取决于原子相对于相位调制光束的运动。