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    • 2. 发明申请
    • Method of retrieving phase and magnitude of weak ultra-short optical pulses using a stronger unknown pulse
    • 使用更强的未知脉冲检索弱超短脉冲的相位和幅度的方法
    • US20070055466A1
    • 2007-03-08
    • US11384230
    • 2006-03-17
    • Aydogan OzcanMichel DigonnetGordon Kino
    • Aydogan OzcanMichel DigonnetGordon Kino
    • G01R29/26
    • G04F13/02G01J11/00
    • A method determines a complex electric field temporal profile of an optical pulse. The method includes providing a measured magnitude of the Fourier transform of a complex electric field temporal profile of a pulse sequence comprising the optical pulse and a dummy pulse. The method further includes providing an estimated phase term of the Fourier transform of the complex electric field temporal profile of the pulse sequence. The method further includes multiplying the measured magnitude and the estimated phase term to generate an estimated Fourier transform of the complex electric field temporal profile of the pulse sequence. The method further includes calculating an inverse Fourier transform of the estimated Fourier transform, wherein the inverse Fourier transform is a function of time. The method further includes calculating an estimated complex electric field temporal profile of the pulse sequence by applying at least one constraint to the inverse Fourier transform.
    • 一种方法确定光脉冲的复电场时间曲线。 该方法包括提供包括光脉冲和伪脉冲的脉冲序列的复电场时间分布的傅里叶变换的测量幅度。 该方法还包括提供脉冲序列的复电场时间分布的傅立叶变换的估计相位项。 该方法还包括乘以测量的幅度和估计的相位项以产生脉冲序列的复电场时间曲线的估计傅立叶变换。 该方法还包括计算傅立叶逆变换的傅立叶逆变换,其中逆傅里叶变换是时间的函数。 该方法还包括通过对傅里叶逆变换应用至少一个约束来计算脉冲序列的估计复电场时间分布。
    • 5. 发明申请
    • Mitigation of photodarkening to achieve laser oscillation and amplification with highly doped fibers
    • 减轻光暗化实现激光振荡和高掺杂光纤放大
    • US20070053400A1
    • 2007-03-08
    • US11508550
    • 2006-08-22
    • Supriyo SinhaMichel DigonnetRobert ByerJens Limpert
    • Supriyo SinhaMichel DigonnetRobert ByerJens Limpert
    • H01S3/03
    • H01S3/0675H01S3/06716H01S3/06791H01S3/07H01S3/094003H01S3/094011H01S3/1055
    • Photodarkening in active fiber or waveguide devices (e.g. lasers, amplifiers, and incoherent sources such as ASE sources) can be reduced by altering the dopant concentration along the length of the doped fiber. A fiber or waveguide device includes two or more intentionally doped fiber or waveguide sections having different concentrations of one or more dopants. The dopants provide optical gain responsive to pump radiation provided to the fiber device by a pump source. A first optical intensity in a first of the fiber or waveguide sections is greater than a second optical intensity in a second of the fiber or waveguide sections. A first dopant concentration in the first fiber or waveguide section is lower than a second dopant concentration in the second fiber or waveguide section. Thus the dopant concentration is reduced in sections of the fiber or waveguide device having a higher optical intensity. The optical intensity can be due to pump radiation and/or signal radiation. Reduced dopant concentration in regions of high optical intensity reduces photodarkening.
    • 通过改变沿着掺杂光纤的长度的掺杂剂浓度,可以减少有源光纤或波导器件(例如,激光器,放大器和非相干源,例如ASE源)中的光标。 光纤或波导器件包括具有不同浓度的一种或多种掺杂剂的两个或更多个有意掺杂的光纤或波导部分。 掺杂剂通过泵浦源提供响应于提供给光纤装置的泵浦辐射的光学增益。 第一光纤或波导部分中的第一光强度大于第二光纤或波导部分中的第二光强度。 第一光纤或波导部分中的第一掺杂剂浓度低于第二光纤或波导部分中的第二掺杂剂浓度。 因此,具有较高光强度的光纤或波导器件的部分的掺杂剂浓度降低。 光强度可能是由于泵浦辐射和/或信号辐射。 高光强度区域的掺杂剂浓度降低会降低光暗化。
    • 6. 发明申请
    • Femtosecond spectroscopy using minimum phase functions
    • 飞秒光谱使用最小相位函数
    • US20070027689A1
    • 2007-02-01
    • US11396931
    • 2006-04-03
    • Aydogan OzcanMichel DigonnetGordon Kino
    • Aydogan OzcanMichel DigonnetGordon Kino
    • G10L13/00
    • G01J11/00G04F13/02
    • A method determines a transient response of a sample. The method includes providing a measured magnitude of the Fourier transform of a complex electric field temporal profile of a pulse sequence comprising a probe pulse and a dummy pulse, wherein the probe pulse is indicative of the transient response of the sample. The method further includes providing an estimated phase term of the Fourier transform of the complex electric field temporal profile of the pulse sequence. The method further includes multiplying the measured magnitude and the estimated phase term to generate an estimated Fourier transform of the complex electric field temporal profile of the pulse sequence. The method further includes calculating an inverse Fourier transform of the estimated Fourier transform, wherein the inverse Fourier transform is a function of time. The method further includes calculating an estimated complex electric field temporal profile of the pulse sequence by applying at least one constraint to the inverse Fourier transform.
    • 一种方法确定样品的瞬态响应。 该方法包括提供包括探针脉冲和伪脉冲的脉冲序列的复电场时间分布的傅立叶变换的测量幅度,其中探针脉冲表示样品的瞬态响应。 该方法还包括提供脉冲序列的复电场时间分布的傅立叶变换的估计相位项。 该方法还包括乘以测量的幅度和估计的相位项以产生脉冲序列的复电场时间曲线的估计傅立叶变换。 该方法还包括计算傅立叶逆变换的傅立叶逆变换,其中逆傅里叶变换是时间的函数。 该方法还包括通过对傅里叶逆变换应用至少一个约束来计算脉冲序列的估计复电场时间分布。
    • 7. 发明申请
    • Method of characterizing fiber bragg gratings using iterative processing
    • 使用迭代处理表征光纤布拉格光栅的方法
    • US20070025432A1
    • 2007-02-01
    • US11130418
    • 2005-05-16
    • Aydogan OzcanMichel DigonnetGordon Kino
    • Aydogan OzcanMichel DigonnetGordon Kino
    • H04B17/00
    • G02B6/0208G01M11/3145G01M11/3172G02B2006/02166
    • A method determines a complex reflection impulse response of a fiber Bragg grating. The method includes providing a measured amplitude of a complex reflection spectrum of the fiber Bragg grating. The method further includes providing an estimated phase term of the complex reflection spectrum. The method further includes multiplying the measured amplitude and the estimated phase term to generate an estimated complex reflection spectrum. The method further includes calculating an inverse Fourier transform of the estimated complex reflection spectrum, wherein the inverse Fourier transform is a function of time. The method further includes calculating an estimated complex reflection impulse response by applying at least one constraint to the inverse Fourier transform of the estimated complex reflection spectrum.
    • 一种方法确定光纤布拉格光栅的复反射脉冲响应。 该方法包括提供光纤布拉格光栅的复反射光谱的测量幅度。 该方法还包括提供复反射谱的估计相位项。 该方法还包括将测量的幅度和估计的相位项相乘以产生估计的复反射谱。 该方法还包括计算估计的复反射谱的傅立叶逆变换,其中逆傅立叶变换是时间的函数。 该方法还包括通过对估计的复反射光谱的傅里叶逆变换应用至少一个约束来计算估计的复反射脉冲响应。