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    • 2. 发明授权
    • Arrangement and method relating to analysis of transmission lines
    • 传输线分析的方法和方法
    • US09009017B2
    • 2015-04-14
    • US13504993
    • 2010-01-08
    • Antoni FertnerFredrik LindqvistIoanna PappaKlas EricsonMiguel BergPer Ola BörjessonStefan Höst
    • Antoni FertnerFredrik LindqvistIoanna PappaKlas EricsonMiguel BergPer Ola BörjessonStefan Höst
    • G06F17/50H04M3/26
    • H04B3/466H04M3/26
    • Embodiments of the present invention relate to an arrangement for analyzing transmission line properties. Measurement data providing means provide data of a first frequency dependent line property, line property calculation arrangement with model handling means, a Hubert transform handler and line property determination means calculate said first property based on model parameters, line resistance at 0 frequency, roc, a cut-off frequency, v, a line capacitance C∞ and a line inductance L∞H. The line model handling means calculates the line inductance L(f) via a Hubert transform of a function of Q(f/v), wherein the function Q(f/v) relates the line resistance R(f) to roc as R(f)=roc·Q(f/v). The Hilbert transform values are calculated using a parameterized closed form expression for the Hubert transform or they are tabulated. The line property determination means calculates the first property and criteria function application means uses the measured first property and the calculated first property for model parameters to find optimized numerical model parameter values.
    • 本发明的实施例涉及用于分析传输线特性的装置。 测量数据提供装置提供第一频率相关线性质的数据,具有模型处理装置的线性属性计算装置,休伯特变换处理器和线性属性确定装置基于模型参数计算所述第一属性,0频率处的线电阻,roc,a 截止频率v,线电容C∞和线电感L∞H。 线路模型处理装置通过Q(f / v)函数的休伯特变换来计算线路电感L(f),其中函数Q(f / v)将线路电阻R(f)与roc相关联, f)= roc·Q(f / v)。 希尔伯特变换值使用Hubert变换的参数化闭合表达式计算,或者将它们列表。 行属性确定装置计算第一属性和标准函数应用装置使用测量的第一属性和所计算的模型参数的第一属性来找到优化的数值模型参数值。
    • 3. 发明申请
    • ARRANGEMENT AND METHOD RELATING TO ANALYSIS OF TRANSMISSION LINES
    • 传输线分析方法及方法
    • US20120215503A1
    • 2012-08-23
    • US13504993
    • 2010-01-08
    • Antoni FertnerFredrik LindqvistIoanna PappaKlas EricsonMiguel BergPer Ola BörjessonStefan Höst
    • Antoni FertnerFredrik LindqvistIoanna PappaKlas EricsonMiguel BergPer Ola BörjessonStefan Höst
    • G06F17/10
    • H04B3/466H04M3/26
    • Embodiments of the present invention relate to an arrangement for analyzing transmission line properties. Measurement data providing means provide data of a first frequency dependent line property, line property calculation arrangement with model handling means, a Hubert transform handler and line property determination means calculate said first property based on model parameters, line resistance at 0 frequency, roc r cut-off frequency, v, line capacitance C∞r and line inductance Σ̂. The line model handling means calculates the line inductance L(J) via a Hubert transform of Q(f/v)r relating line resistance R(J) to roc such as formula (I). The Hilbert transform values are calculated using a parameterized closed form expression for the Hubert transform or they are tabulated. The line property determination means calculates the first property and criteria function application means uses the measured first property and the calculated first property for model parameters to find optimized numerical model parameter values.
    • 本发明的实施例涉及用于分析传输线特性的装置。 测量数据提供装置提供第一频率相关线性属性的数据,具有模型处理装置的线性属性计算装置,休伯特变换处理器和线性属性确定装置根据模型参数计算所述第一属性,0频率线路电阻, 截止频率,v,线电容C∞r和线电感&Sgr。 线路模型处理装置通过与线路电阻R(J)相关的Q(f / v)r的休伯特变换到诸如公式(I)的roc来计算线路电感L(J)。 希尔伯特变换值使用Hubert变换的参数化闭合表达式计算,或者将它们列表。 行属性确定装置计算第一属性和标准函数应用装置使用测量的第一属性和所计算的模型参数的第一属性来找到优化的数值模型参数值。
    • 6. 发明授权
    • Multi-carrier method in a measurement device
    • 多载波方法在测量设备中
    • US09191130B2
    • 2015-11-17
    • US14368843
    • 2012-01-05
    • Miguel BergAntoni FertnerDaniel CederholmPer Ola Börjesson
    • Miguel BergAntoni FertnerDaniel CederholmPer Ola Börjesson
    • H04B3/46H04B17/00H04B17/30H04L27/26
    • H04B17/30H04B3/46H04L27/2601H04L27/2627
    • The invention relates to a multi-carrier method in a measurement device for improving reach of a measurement, said method comprising: transmitting a first signal in a sequence, measuring a response to said first signal, calculating a first transfer function for frequency of each modulated subcarrier in the first signal, transmitting a second signal of the sequence, wherein at least one subcarrier in the second signal has modulation different from that of the subcarriers in the first signal, measuring a response to said second signal, calculating a second transfer function for frequency of each modulated subcarrier in the second signal, said second transfer function comprising for each frequency a thereto associated second distortion component, calculating a mean value of all first and second transfer functions. The invention further relates to a measurement device for performing said method.
    • 本发明涉及一种用于提高测量范围的测量装置中的多载波方法,所述方法包括:按顺序发送第一信号,测量对所述第一信号的响应,计算每个调制的频率的第一传递函数 发送所述序列的第二信号,其中所述第二信号中的至少一个子载波具有与所述第一信号中的子载波不同的调制,测量对所述第二信号的响应,计算第二传递函数, 所述第二传递函数包括针对每个频率a与其相关联的第二失真分量,计算所有第一和第二传递函数的平均值。 本发明还涉及一种用于执行所述方法的测量装置。
    • 7. 发明申请
    • MULTI-CARRIER METHOD IN A MEASUREMENT DEVICE
    • 测量装置中的多载波方法
    • US20150180596A1
    • 2015-06-25
    • US14368843
    • 2012-01-05
    • Miguel BergAntoni FertnerDaniel CederholmPer Ola Börjesson
    • Miguel BergAntoni FertnerDaniel CederholmPer Ola Börjesson
    • H04B17/30H04L27/26
    • H04B17/30H04B3/46H04L27/2601H04L27/2627
    • The invention relates to a multi-carrier method in a measurement device for improving reach of a measurement, said method comprising: transmitting a first signal in a sequence, measuring a response to said first signal, calculating a first transfer function for frequency of each modulated subcarrier in the first signal, transmitting a second signal of the sequence, wherein at least one subcarrier in the second signal has modulation different from that of the subcarriers in the first signal, measuring a response to said second signal, calculating a second transfer function for frequency of each modulated subcarrier in the second signal, said second transfer function comprising for each frequency a thereto associated second distortion component, calculating a mean value of all first and second transfer functions. The invention further relates to a measurement device for performing said method.
    • 本发明涉及一种用于提高测量范围的测量装置中的多载波方法,所述方法包括:按顺序发送第一信号,测量对所述第一信号的响应,计算每个调制的频率的第一传递函数 发送所述序列的第二信号,其中所述第二信号中的至少一个子载波具有与所述第一信号中的子载波不同的调制,测量对所述第二信号的响应,计算第二传递函数, 所述第二传递函数包括针对每个频率a与其相关联的第二失真分量,计算所有第一和第二传递函数的平均值。 本发明还涉及一种用于执行所述方法的测量装置。
    • 8. 发明授权
    • Method for transmission line analysis
    • 传输线分析方法
    • US08385510B2
    • 2013-02-26
    • US13129555
    • 2009-11-27
    • Miguel BergDaniel CederholmKlas EricsonPer Ola Börjesson
    • Miguel BergDaniel CederholmKlas EricsonPer Ola Börjesson
    • H04M1/24H04M3/08H04M3/22
    • H04B3/46H04M3/306H04M11/062
    • A FDR SELT measurement is made in a stop band of a DSL band plan, using a PSD allowed by the PSD mask. Further measurements may also be made in an adjacent pass band and further bands, and the results combined to create a wide-band measurement result. When transformed into the time domain (e.g. by inverse Fourier transform to produce the line impulse response) greater resolution in time (and hence greater spatial resolution) is achieved. In order to compensate for AGC calibration errors measurements using different AGC steps may be scaled to fit smoothly to each other. If measurements overlap, measurement results in the region of overlap may be combined in various ways to limit the influence of noise and to create a smooth transition from one measurement to the next.
    • 使用PSD掩模允许的PSD,在DSL频段计划的停止频段进行FDR SELT测量。 还可以在相邻通带和另外的带中进行进一步测量,并且结果组合以产生宽带测量结果。 当变换到时域(例如通过逆傅立叶变换产生线脉冲响应)时,可以获得更高的时间分辨率(因此更大的空间分辨率)。 为了补偿AGC校准误差,使用不同AGC步长的测量可以被缩放以相互平滑地相配合。 如果测量重叠,重叠区域中的测量结果可以以各种方式组合,以限制噪声的影响并创建从一个测量到下一个测量的平滑过渡。
    • 9. 发明申请
    • METHOD FOR TRANSMISSION LINE ANALYSIS
    • 传输线分析方法
    • US20110261932A1
    • 2011-10-27
    • US13129555
    • 2009-11-27
    • Miguel BergDaniel CederholmKlas EricsonPer Ola Börjesson
    • Miguel BergDaniel CederholmKlas EricsonPer Ola Börjesson
    • H04M3/22
    • H04B3/46H04M3/306H04M11/062
    • A FDR SELT measurement is made in a stop band of a DSL band plan, using a PSD allowed by the PSD mask. Further measurements may also be made in an adjacent pass band and further bands, and the results combined to create a wide-band measurement result. When transformed into the time domain (e.g. by inverse Fourier transform to produce the line impulse response) greater resolution in time (and hence greater spatial resolution) is achieved. In order to compensate for AGC calibration errors measurements using different AGC steps may be scaled to fit smoothly to each other. If measurements overlap, measurement results in the region of overlap may be combined in various ways to limit the influence of noise and to create a smooth transition from one measurement to the next.
    • 使用PSD掩模允许的PSD,在DSL频段计划的停止频段进行FDR SELT测量。 还可以在相邻通带和另外的带中进行进一步测量,并且结果组合以产生宽带测量结果。 当变换到时域(例如通过逆傅立叶变换产生线脉冲响应)时,可以获得更高的时间分辨率(因此更大的空间分辨率)。 为了补偿AGC校准误差,使用不同AGC步长的测量可以被缩放以相互平滑地相配合。 如果测量重叠,重叠区域中的测量结果可以以各种方式组合,以限制噪声的影响并创建从一个测量到下一个测量的平滑过渡。