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    • 2. 发明授权
    • Quantum switch
    • US06628453B2
    • 2003-09-30
    • US09846794
    • 2001-05-01
    • Byoung-Seung Ham
    • Byoung-Seung Ham
    • G02F1355
    • G02F1/3536G02F1/3515
    • A system, method, and apparatus for optical switches based on dark resonance in which three-color lasers interact with a four-level nonlinear optical medium composing three ground states and an excited state through nondegenerate four-wave mixing processes. The switching mechanism is based on dark resonance induced two-photon coherence swapping among the three closely spaced ground states through optical transitions via an excited state. The two-photon coherence induced on the ground states is optically detected via nondegenerate four-wave mixing processes. The nondegenerate four-wave mixing generation is enhanced owing to dark resonance or electromagnetically induced transparency. The switching time and bandwidth of the present optical switching method is not limited by population relaxation time or carrier's lifetime. More advantage is given by signal amplifications owing to the dark-resonance enhanced nondegenerate four-wave mixing processes.
    • 4. 发明授权
    • Polarization inversion method of ferroelectrics and fabrication method of optical wavelength conversion device
    • 铁电极化反演方法及光波长转换装置的制作方法
    • US06762874B2
    • 2004-07-13
    • US09987131
    • 2001-11-13
    • Yasukazu Nihei
    • Yasukazu Nihei
    • G02F1355
    • G02F1/3558G02F1/3775G02F2201/122
    • A method for forming a polarization inversion portion, in which electrodes with a predetermined pattern are formed on one surface of a ferroelectric crystal that has been subjected to a single polarization, and a local polarization inversion portion corresponding to the pattern of the electrodes is formed in the ferroelectric crystal by applying electric field to both front and back surfaces of the ferroelectric crystal via the electrodes, makes it possible to accurately form a polarization inversion pattern. In this method, portions of the ferroelectric crystal corresponding to the respective electrodes and portions between these portions are subjected to a polarization inversion, and one polarization inversion portion is formed.
    • 一种形成极化反转部分的方法,其中具有预定图案的电极形成在已经经受单极化的铁电晶体的一个表面上,并且形成与电极图案对应的局部极化反转部分 通过经由电极向强电介质晶体的前表面和后表面施加电场的铁电晶体使得可以精确地形成极化反转图案。 在该方法中,对应于各个电极的铁电晶体的部分和这些部分之间的部分进行极化反转,并且形成一个极化反转部分。
    • 7. 发明授权
    • Technique for quasi-phase matching
    • 准相位匹配技术
    • US06710912B1
    • 2004-03-23
    • US10326124
    • 2002-12-23
    • Robert John FilkinsPeter William Lorraine
    • Robert John FilkinsPeter William Lorraine
    • G02F1355
    • G02F1/3775G02F2001/3548G02F2202/32
    • A technique for achieving quasi phase matching in a photonic band gap structure comprising a first material and a second material is disclosed. In one particular exemplary embodiment, the technique may be realized by calculating a coherence length of an optical interaction of interest involving at least a first frequency and a second frequency; calculating a first lattice constant of the first material to achieve a predetermined first group velocity for a fundamental optical frequency; calculating a second lattice constant of the second material so that a second group velocity of a second optical frequency is substantially the same as the first group velocity associated with the fundamental optical frequency of the first material; determining a photonic band gap arrangement for achieving quasi phase matching in the photonic band gap structure; and implementing the first lattice constant of the first material and the second lattice constant of the second material in accordance with the photonic band gap arrangement to achieve quasi phase matching in the photonic band gap structure.
    • 公开了一种在包括第一材料和第二材料的光子带隙结构中实现准相位匹配的技术。 在一个特定示例性实施例中,可以通过计算涉及至少第一频率和第二频率的感兴趣的光学相互作用的相干长度来实现该技术; 计算第一材料的第一晶格常数以实现基本光频率的预定的第一组速度; 计算第二材料的第二晶格常数,使得第二光频率的第二组速度与与第一材料的基本光频率相关联的第一组速度基本相同; 确定用于实现光子带隙结构中的准相位匹配的光子带隙布置; 并且根据光子带隙布置实现第一材料的第一晶格常数和第二材料的第二晶格常数,以实现光子带隙结构中的准相位匹配。
    • 8. 发明授权
    • Optical module
    • 光模块
    • US06633428B2
    • 2003-10-14
    • US09859387
    • 2001-05-18
    • Kenichi AbeYuji Hozumi
    • Kenichi AbeYuji Hozumi
    • G02F1355
    • G02F1/0305G02F2001/3505G02F2202/22
    • A pyroelectric crystal, e.g. a LN crystal (1), is coated with conductive films (8). When polarization charges (4) are generated on the surface of the LN crystal (1) due to its pyroelectric effect upon accumulation of stress, the presence of the conductive films (8) induces on themselves reverse electric charges (9) matching the polarization charges (4) generated on the surface of the LN crystal (1). Therefore an electric field created by the polarization charges (4) is canceled by an electric field created by the reverse charges (9) induced on the conductive films (8). The conductive film (8b) formed on a face through which signal light is transmitted is formed from a medium transparent with respect to the signal light. Therefore the light path of the signal light is not blocked by the conductive film (8b), and the polarization charges (4) generated on the signal transmissive face can be neutralized.
    • 热电晶体,例如 将LN晶体( 1 )涂覆有导电膜( 8 )。 由于其热电效应,在LN晶体表面( 1 )上产生极化电荷( 4 ) 应力的累积,导电膜( 8 )的存在本身会引起与之相匹配的反电荷( 9 ) 在LN晶体的表面( 1 )上产生的极化电荷( 4 )。 因此,由反向电荷产生的电场( 9 )消除由极化电荷( 4 )产生的电场 >)导电膜( 8 )。 形成在透射信号光的面上的导电膜( 8 b )由相对于 信号灯。 因此,信号光的光路不被导电膜( 8 b )阻挡,极化电荷( 4 )可以被中和。