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    • 3. 发明申请
    • Method and Device for Multiplying Optical Frequencies by a Factor 1.5
    • 用于乘以因子1.5的光频率的方法和装置
    • US20080055702A1
    • 2008-03-06
    • US11663705
    • 2005-09-23
    • Gabriele Ferrari
    • Gabriele Ferrari
    • G02F1/35G02F1/01G02F1/37
    • G02F1/3534G02F1/39G02F2001/3507
    • An optical cavity is combined with non-linear optical crystals and a laser source to generate light radiation at a frequency about 1.5 times the frequency of the initial laser source having a wavelength ⅔ that of the initial laser source. The optical cavity comprises mirrors with relatively high reflectivity for optical radiation at a frequency of F/2, superior transmission for radiation at a frequency of 3/2*F for extracting the final radiation and mirrors with relatively immediate or high reflectivity, or generally high transmission for radiation at frequency F. The effective optical length of the cavity is precisely tunable by acting on at least one of the mirrors that form the cavity. The optical cavity contains at least two non-linear optical crystals: at least one of which satisfies the phase-matching-quasi phase-matching-condition for non-linear conversion F 2*F/2, and at least one of which satisfies the phase-matching—or quasi phase-matching-condition for non-linear conversion F+F/2? 3/2*F. The length of the optical cavity, and its resonance modes, are actively stabilized such that the only process of frequency division is that by a factor of 2.
    • 光腔与非线性光学晶体和激光源组合以产生具有初始激光源的波长2/3的初始激光源的频率约1.5倍的频率的光辐射。 光学腔包括对F / 2频率的光辐射具有相对较高反射率的反射镜,用于以3/2 * F频率进行辐射的优异透射率用于提取最终辐射和具有相对立即或高反射率或通常高的反射镜 用于在频率F处的辐射的透射。通过作用于形成腔的至少一个反射镜,可以精确地调节腔的有效光学长度。 光腔包含至少两个非线性光学晶体:其中至少一个满足用于非线性转换F 2 * F / 2的相位匹配准相位匹配条件,并且其中至少一个满足 相位匹配或准相位匹配条件用于非线性转换F + F / 2? 3/2 * F。 光腔的长度及其谐振模式被主动地稳定,使得唯一的分频过程是2倍。
    • 4. 发明授权
    • Device for multiplying optical frequencies
    • 用于倍增光频率的装置
    • US07623556B2
    • 2009-11-24
    • US11663705
    • 2005-09-23
    • Gabriele Ferrari
    • Gabriele Ferrari
    • H01S3/10
    • G02F1/3534G02F1/39G02F2001/3507
    • An optical cavity is combined with non-linear optical crystals and a laser source to generate light radiation at a frequency about 1.5 times the frequency of the initial laser source while having a wavelength 2/3 that of the initial laser source. The optical cavity comprises mirrors of relatively high reflectivity for optical radiation at a frequency of F/2, superior transmission for radiation at a frequency of 3/2*F to extract the final radiation and mirrors with relatively immediate or high reflectivity, or generally high transmission for radiation at a frequency F. The effective optical length of the cavity is precisely tunable by operating at least one of the mirrors that form the cavity. The optical cavity houses at least two non-linear optical crystals: at least one of which satisfies the phase-matching—quasi phase-matching—condition for non-linear conversion F 2*F/2, and at least one of which satisfies the phase-matching—or quasi phase-matching—condition for non-linear conversion F+F/23/2*F The length of the optical cavity, and its resonance modes, are actively stabilized such that the only process of frequency division is that by a factor of around 2.
    • 光学腔与非线性光学晶体和激光源组合,以产生具有初始激光源的频率的初始激光源的频率的约1.5倍的光辐射,同时具有初始激光源的波长的2/3。 光学腔包括用于频率为F / 2的光辐射的相对较高反射率的反射镜,用于以3/2 * F频率的辐射的优异透射以提取最终辐射和具有相对立即或高反射率或通常高的反射镜 以频率F的辐射传输。通过操作形成空腔的至少一个反射镜,可以精确地调节空腔的有效光学长度。 光腔容纳至少两个非线性光学晶体:其中至少一个满足非线性转换F 2 * F / 2的相位匹配准相位匹配条件,并且其中至少一个满足 相位匹配或准相位匹配条件用于非线性转换F + F / 2 3/2 * F光腔的长度及其谐振模式被主动稳定, 分频的唯一过程是约2倍。