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A simple method to identify the spatial location complication due to the transient phonon relaxation on the Brillouin loss spectrum

机译:一种简单的方法来确定由于布里渊损耗谱上的瞬时声子弛豫而引起的空间位置复杂化

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For the pump-probe stimulated Brillouin scattering with probe pulse of a few nanoseconds duration and with a finite DC level, the acoustic wave relaxation time varies with the pump power and DC level. For the pump power of 1-6mW, the acoustic wave relaxation changes between 9 to 90 ns for polarization maintained fiber (PMF) at temperature of -45℃ for 2 ns pulse width. When pulse to DC ratio of the probe varies from 10 to 20dB, the acoustic relaxation time changes between 24 to 45ns for single mode fiber (SMF) at 25℃. This induced a power increment spectral feature in detected AC pump signal in the Brillouin loss spectrum of two temperature or strain sections, where both spectral components appeared at the positions much longer than natural phonon relaxation time (~10ns) equivalent length. This can cause problem for the distributed sensor in determining the strain/temperature boundary, and central Brillouin peak fitting due to the multiple peak convolution, and it affects temperature and strain accuracy. We propose the 2nd order partial derivative of Stokes signal with respect to frequency and position giving a maximum or minimum at the boundary between two different strained sections. This allows finding the true stress or temperature corresponded section.
机译:对于具有几纳秒持续时间的探测脉冲和有限直流电平的泵浦探针激发的布里渊散射,声波弛豫时间随泵浦功率和直流电平而变化。对于1-6mW的泵浦功率,对于偏振保持光纤(PMF),在-45℃的温度下2 ns的脉冲宽度,声波弛豫在9到90 ns之间变化。当探头的脉冲直流比在10至20dB之间变化时,单模光纤(SMF)在25℃时的声弛豫时间在24至45ns之间变化。这在两个温度或应变部分的布里渊损耗谱中的检测到的交流泵浦信号中引入了功率增量谱特征,其中两个谱分量出现在比自然声子弛豫时间(〜10ns)等效长度更长的位置。这可能会导致分布式传感器在确定应变/温度边界以及由于多个峰卷积而导致中心布里渊峰拟合时出现问题,并且会影响温度和应变精度。我们提出了斯托克斯信号相对于频率和位置的二阶偏导数,在两个不同应变部分之间的边界处给出了最大值或最小值。这允许找到真实的应力或温度对应的部分。

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