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    • 4. 发明授权
    • Transmission line parameter determination
    • 传输线参数确定
    • US09470729B2
    • 2016-10-18
    • US14110215
    • 2011-04-08
    • Fredrik LindqvistPer Ola BörjessonAntoni Fertner
    • Fredrik LindqvistPer Ola BörjessonAntoni Fertner
    • G01R27/02H04B3/466
    • G01R27/02H04B3/466
    • The present disclosure relates to determining parameters in a model of a transmission line. For determining the parameters, reflection coefficient defining data and the total capacitance of the transmission line are obtained. Further, true reflection coefficients obtained through the reflection coefficient defining data are applied in an objective function for the line. The objective function for the line is a sum of error signals and each error signal is the difference between a model value of a reflection coefficient and a corresponding true reflection coefficient. Further, the objective function is minimized by utilizing gradients of the objective function with respect to the transmission line parameters to be determined. A capacitive length is employed and at least two further transmission line parameters are determined as combinations of a basic resistive transmission line parameter, a basic capacitive transmission line parameter and a basic inductive transmission line parameter of the transmission line model.
    • 本公开涉及确定传输线的模型中的参数。 为了确定参数,获得反射系数定义数据和传输线的总电容。 此外,通过反射系数定义数据获得的真实反射系数被应用于该行的目标函数中。 线的目标函数是误差信号的和,每个误差信号是反射系数的模型值和相应的真实反射系数之间的差。 此外,通过利用待确定的传输线参数的目标函数的梯度来最小化目标函数。 使用电容长度,并且将至少两个另外的传输线参数确定为传输线模型的基本电阻传输线参数,基本电容传输线参数和基本感应传输线参数的组合。
    • 5. 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。
    • 7. 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。
    • 8. 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。
    • 10. 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。