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    • 1. 发明授权
    • Method and apparatus for testing transmission lines normally propagating optical signals
    • 测试传输线正常传播光信号的方法和装置
    • US08861953B2
    • 2014-10-14
    • US13204350
    • 2011-08-05
    • Bernard RuchetNormand Cyr
    • Bernard RuchetNormand Cyr
    • H04B10/08H04B10/079
    • H04B10/07955H04B3/46H04B10/079H04B10/0793H04B10/0795H04B10/07953H04Q11/0067H04Q2011/0083
    • Portable apparatus for measuring parameters of optical signals propagating concurrently in opposite directions in an optical transmission path between two elements, at least one of the elements being operative to transmit a first optical signal (S1) only if it continues to receive a second optical signal (S2) from the other (10) of said elements, comprises first and second connectors for connecting the apparatus into the optical transmission path in series therewith, and a device connected between the first and second connectors for propagating at least the second optical signal (S2) towards the one of the elements, and measuring the parameters of the concurrently propagating optical signals (S1, S2). The measurement results may be displayed by a suitable display unit. Where one element transmits signals at two different wavelengths, the apparatus may separate parts of the corresponding optical signal portion according to wavelength and process them separately.
    • 用于测量在两个元件之间的光传输路径中沿相反方向同时传播的光信号的参数的便携式设备,所述元件中的至少一个仅在其继续接收第二光信号(S1)时才发送第一光信号(S1) S2)从所述元件的另一个(10)中包括用于将设备串联连接到光传输路径中的第一和第二连接器以及连接在第一和第二连接器之间的装置,用于至少传播第二光信号(S2 ),并测量同时传播的光信号(S1,S2)的参数。 测量结果可以由合适的显示单元显示。 当一个元件以两个不同的波长发射信号时,该装置可以根据波长分离对应的光信号部分的部分并分别处理它们。
    • 2. 发明申请
    • IN-BAND OPTICAL NOISE MEASUREMENT USING DIFFERENTIAL POLARIZATION RESPONSE
    • 使用差分偏振响应的带内光噪声测量
    • US20110091206A1
    • 2011-04-21
    • US12859648
    • 2010-08-19
    • Gang HENormand CYRDaniel GARIEPY
    • Gang HENormand CYRDaniel GARIEPY
    • H04B10/08
    • H04B10/07953
    • A method comprises: acquiring, for a number nSOP of varied State-Of-Polarization analysis conditions of the input optical signal, nSOP polarization-analyzed optical spectrum traces; mathematically discriminating said signal contribution from said noise contribution within said optical signal bandwidth using said polarization-analyzed optical spectrum traces, said mathematically discriminating comprising: obtaining a differential polarization response that is related to the optical spectrum of said signal contribution by a constant of proportionality; estimating the constant of proportionality of a differential polarization response to the optical spectrum of said signal contribution; estimating the optical spectrum of said noise contribution from said input optical signal, within said optical signal bandwidth using said constant of proportionality and said differential polarization response; and determining said in-band noise parameter on said input optical signal from the mathematically discriminated noise contribution.
    • 一种方法包括:对于输入光信号的nSOP极化分析条件的nSOP数值,获取nSOP偏振分析光谱图; 使用所述经偏振分析的光谱轨迹,在所述光信号带宽内从所述噪声贡献中数学地识别所述信号贡献,所述数学鉴别包括:获得与所述信号贡献的光谱相关比例常数的差分偏振响应; 估计差分极化响应与所述信号贡献的光谱的比例常数; 使用所述比例常数和所述微分极化响应在所述光信号带宽内估计来自所述输入光信号的所述噪声贡献的光谱; 以及从所述数学鉴别的噪声贡献中确定所述输入光信号上的所述带内噪声参数。
    • 3. 发明授权
    • In-band optical noise measurement using differential polarization response
    • 使用差分极化响应的带内光学噪声测量
    • US08364034B2
    • 2013-01-29
    • US12859648
    • 2010-08-19
    • Gang HeNormand CyrDaniel Gariepy
    • Gang HeNormand CyrDaniel Gariepy
    • H04B10/08
    • H04B10/07953
    • A method comprises: acquiring, for a number nSOP of varied State-Of-Polarization analysis conditions of the input optical signal, nSOP polarization-analyzed optical spectrum traces; mathematically discriminating said signal contribution from said noise contribution within said optical signal bandwidth using said polarization-analyzed optical spectrum traces, said mathematically discriminating comprising: obtaining a differential polarization response that is related to the optical spectrum of said signal contribution by a constant of proportionality; estimating the constant of proportionality of a differential polarization response to the optical spectrum of said signal contribution; estimating the optical spectrum of said noise contribution from said input optical signal, within said optical signal bandwidth using said constant of proportionality and said differential polarization response; and determining said in-band noise parameter on said input optical signal from the mathematically discriminated noise contribution.
    • 一种方法包括:对于输入光信号的nSOP极化分析条件的nSOP数值,获取nSOP偏振分析光谱图; 使用所述经偏振分析的光谱轨迹,在所述光信号带宽内从所述噪声贡献中数学地识别所述信号贡献,所述数学鉴别包括:获得与所述信号贡献的光谱相关比例常数的差分偏振响应; 估计差分极化响应与所述信号贡献的光谱的比例常数; 使用所述比例常数和所述微分极化响应在所述光信号带宽内估计来自所述输入光信号的所述噪声贡献的光谱; 以及从所述数学鉴别的噪声贡献中确定所述输入光信号上的所述带内噪声参数。
    • 4. 发明申请
    • METHOD AND APPARATUS FOR TESTING TRANSMISSION LINES NORMALLY PROPAGATING OPTICAL SIGNALS
    • 用于测试传输线正常传播光信号的方法和装置
    • US20110293267A1
    • 2011-12-01
    • US13204350
    • 2011-08-05
    • Bernard RuchetNormand Cyr
    • Bernard RuchetNormand Cyr
    • H04B10/08
    • H04B10/07955H04B3/46H04B10/079H04B10/0793H04B10/0795H04B10/07953H04Q11/0067H04Q2011/0083
    • Portable apparatus for measuring parameters of optical signals propagating concurrently in opposite directions in an optical transmission path between two elements, at least one of the elements being operative to transmit a first optical signal (S1) only if it continues to receive a second optical signal (S2) from the other (10) of said elements, comprises first and second connectors for connecting the apparatus into the optical transmission path in series therewith, and a device connected between the first and second connectors for propagating at least the second optical signal (S2) towards the one of the elements, and measuring the parameters of the concurrently propagating optical signals (S1, S2). The measurement results may be displayed by a suitable display unit. Where one element transmits signals at two different wavelengths, the apparatus may separate parts of the corresponding optical signal portion according to wavelength and process them separately.
    • 用于测量在两个元件之间的光传输路径中沿相反方向同时传播的光信号的参数的便携式设备,所述元件中的至少一个仅在其继续接收第二光信号(S1)时才发送第一光信号(S1) S2)从所述元件的另一个(10)中包括用于将设备串联连接到光传输路径中的第一和第二连接器以及连接在第一和第二连接器之间的装置,用于至少传播第二光信号(S2 ),并测量同时传播的光信号(S1,S2)的参数。 测量结果可以由合适的显示单元显示。 当一个元件以两个不同的波长发射信号时,该装置可以根据波长分离对应的光信号部分的部分并分别处理它们。
    • 6. 发明授权
    • Method and apparatus for testing transmission lines normally propagating optical signals
    • 测试传输线正常传播光信号的方法和装置
    • US07995915B2
    • 2011-08-09
    • US11713735
    • 2007-03-05
    • Bernard RuchetNormand Cyr
    • Bernard RuchetNormand Cyr
    • H04B10/08
    • H04B10/07955H04B3/46H04B10/079H04B10/0793H04B10/0795H04B10/07953H04Q11/0067H04Q2011/0083
    • Portable apparatus for measuring parameters of optical signals propagating concurrently in opposite directions in an optical transmission path between two elements, at least one of the elements being operative to transmit a first optical signal (S1) only if it continues to receive a second optical signal (S2) from the other (10) of said elements, comprises first and second connectors for connecting the apparatus into the optical transmission path in series therewith, and a device connected between the first and second connectors for propagating at least the second optical signal (S2) towards the one of the elements, and measuring the parameters of the concurrently propagating optical signals (S1, S2). The measurement results may be displayed by a suitable display unit. Where one element transmits signals at two different wavelengths, the apparatus may separate parts of the corresponding optical signal portion according to wavelength and process them separately.
    • 用于测量在两个元件之间的光传输路径中沿相反方向同时传播的光信号的参数的便携式设备,所述元件中的至少一个仅在其继续接收第二光信号(S1)时才发送第一光信号(S1) S2)从所述元件的另一个(10)中包括用于将设备串联连接到光传输路径中的第一和第二连接器以及连接在第一和第二连接器之间的装置,用于至少传播第二光信号(S2 ),并测量同时传播的光信号(S1,S2)的参数。 测量结果可以由合适的显示单元显示。 当一个元件以两个不同的波长发射信号时,该装置可以根据波长分离对应的光信号部分的部分并分别处理它们。
    • 7. 发明授权
    • Polarization optical time domain reflectometer and method of determining PMD
    • 偏振光学时域反射计和PMD的测定方法
    • US07920253B2
    • 2011-04-05
    • US11992797
    • 2006-09-29
    • Normand CyrHongxin Chen
    • Normand CyrHongxin Chen
    • G01N21/00G01J4/00
    • G01M11/3181
    • In a method of measuring cumulative polarization mode dispersion (PMD) along the length of a fiber-under-test (FUT), a polarization-sensitive optical time domain reflectometer (POTDR) is used to inject into the FUT plural series of light pulses arranged in several groups. Each group comprises at least two series having closely-spaced wavelengths and the same state of polarization (SOP). At least two of such groups are injected and corresponding OTDR traces obtained for each series by averaging the impulse-response signals of the several series in the group. The process is repeated for a number of groups. The PMD is obtained by normalizing the OTDR traces of all of the groups, then computing the difference between each normalized OTDR trace in one group and the corresponding normalized OTDR trace in another group, followed by the mean-square value of the differences. Finally, the PMD is computed as a predetermined function of the mean-square difference.
    • 在沿着被测光纤(FUT)的长度测量累积偏振模色散(PMD)的方法中,使用极化敏感光时域反射计(POTDR)将FUT多个系列的光脉冲 在几个组。 每个组包括具有紧密间隔的波长和相同的极化状态(SOP)的至少两个系列。 通过平均组中几个系列的脉冲响应信号,为每个系列注入至少两个这样的组以及相应的OTDR迹线。 对于多个组重复该过程。 通过归一化所有组的OTDR轨迹,然后计算一组中的每个归一化OTDR轨迹与另一组中相应的归一化OTDR轨迹之间的差异,然后是差值的均方根值,获得PMD。 最后,将PMD计算为均方差的预定函数。
    • 8. 发明授权
    • Method and apparatus for measuring polarization mode dispersion
    • 用于测量偏振模色散的方法和装置
    • US07227645B2
    • 2007-06-05
    • US10544638
    • 2003-02-06
    • Normand Cyr
    • Normand Cyr
    • G01B9/02
    • G01J4/04G01M11/331G01M11/336
    • Apparatus for measuring polarization mode dispersion (PMD) of a device, e.g. a waveguide, comprises a broadband light source (10,12) for passing polarized broadband light through the device (14), an interferometer (20) for dividing and recombining light that has passed through the device to form interferograms, a polarization separator (30) for receiving the light from the interferometer and separating such received light along first and second orthogonal Feb. 25, 2003 Feb. 25, 2003 polarization states, detectors (32x,32y) for converting the first and second orthogonal polarization states, respectively, into corresponding first and second electrical signals (Px(τ),Py(τ)), and a processor (36) for computing the modulus of the difference and such, respectively, of the first and second electrical signals to produce a cross-correlation envelope (EC(τ)) and an auto-correlation envelope (Ec(τ)), and determining the polarization mode dispersion according to the expression PMD=where and τ is the delay difference between the paths of the interferometer.
    • 用于测量装置的偏振模色散(PMD)的装置,例如, 波导,包括用于使偏振宽带光通过装置(14)的宽带光源(10,12),用于分割和重新组合通过该装置的光以形成干涉图的干涉仪(20);偏振分离器(30) ),用于接收来自干涉仪的光并且在2003年2月25日的第一和第二正交方向上分离这样的接收光,2003年2月25日,偏振态,检测器(32×32, 分别将第一和第二正交极化状态转换成对应的第一和第二电信号(P SUB)(τ),P SUB(τ)), 以及用于分别计算第一和第二电信号的差的模数和处理器(36)以产生互相关包络(E SUB)(τ) 相关包络(τ)(τ)),以及根据表达式PMD =其中确定偏振模色散 并且τT是干涉仪的路径之间的延迟差。
    • 9. 发明申请
    • In-Band Optical Noise Measurement Using Differential Polarization Response
    • 使用差分极化响应的带内光噪声测量
    • US20120093501A1
    • 2012-04-19
    • US13378557
    • 2010-08-19
    • Gang HeNormand Cyr
    • Gang HeNormand Cyr
    • H04B10/08
    • H04B10/07953
    • A method comprises: acquiring, for a number nSOP of varied State-Of-Polarization analysis conditions of the input optical signal, nSOP polarization-analyzed optical spectrum traces, the distribution of the input optical signal of said SOP analysis conditions being approximately known; mathematically discriminating said signal contribution from said noise contribution within said optical signal bandwidth using said polarization-analyzed optical spectrum traces, said mathematically discriminating comprising: obtaining a differential polarization response that is related to the optical spectrum of said signal contribution by a constant of proportionality; estimating the constant of proportionality of a differential polarization response to the optical spectrum of said signal contribution as a function of said number nSOP; estimating the optical spectrum of said noise contribution from said input optical signal, within said optical signal bandwidth using said constant of proportionality and said differential polarization response; and determining said in-band noise parameter on said input optical signal from the mathematically discriminated noise contribution.
    • 一种方法包括:对于输入光信号,nSOP偏振分析的光谱轨迹的不同状态的极化分析条件的数量nSOP,获取所述SOP分析条件的输入光信号的分布近似已知; 使用所述经偏振分析的光谱轨迹,在所述光信号带宽内从所述噪声贡献中数学地识别所述信号贡献,所述数学鉴别包括:获得与所述信号贡献的光谱相关比例常数的差分偏振响应; 估计作为所述数量nSOP的函数的所述信号贡献的光谱的差分偏振响应的比例常数; 使用所述比例常数和所述微分极化响应在所述光信号带宽内估计来自所述输入光信号的所述噪声贡献的光谱; 以及从所述数学鉴别的噪声贡献中确定所述输入光信号上的所述带内噪声参数。
    • 10. 发明授权
    • Measurement of optical properties of passive optical devices using the matrix method
    • 使用矩阵法测量无源光学器件的光学特性
    • US06762829B2
    • 2004-07-13
    • US10373736
    • 2003-02-27
    • François BabinNormand Cyr
    • François BabinNormand Cyr
    • G01N2100
    • G01N21/21G01J4/04G01M11/337
    • A property of a device that is dependent upon both wavelength and state of polarization is measured by; passing through the device an optical signal having its wavelength and SOP varied, the wavelength over a spectral range of the device and the SOP between four Mueller SOPs; measuring the insertion loss of the device for each of the four SOPS and at each wavelength; using the four insertion loss measurements for each of the four different states of polarization for each wavelength to compute the four elements of the first line of the Mueller matrix for each wavelength; and using the Mueller matrix elements, computing insertion loss variations for the device for a multiplicity of input states of polarization in addition to the four states of polarization for which the actual attenuation measurements were made and using the insertion loss variations to compute the polarization and wavelength dependent property.
    • 取决于波长和极化状态的器件的性质是通过测量的; 通过该器件具有其波长和SOP的光信号变化,器件的光谱范围上的波长和四个Mueller SOP之间的SOP; 测量四个SOPS中每一个和每个波长的器件的插入损耗; 对于每个波长使用四种不同极化状态中的每一种的四次插入损耗测量来计算每个波长的Mueller矩阵的第一行的四个元素; 并且使用Mueller矩阵元素,除了进行实际衰减测量的四个极化状态之外,还计算多个输入极化状态的装置的插入损耗变化,并且使用插入损耗变化来计算极化和波长 依赖财产。