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This is derived from the definition of the argument of the coupling coefficient, arg(q(z, 4ηπ/γ) ∫0 z δndc(z′)dz′, where δndc is the DC component of the index change and δndc(z, ∂n/∂TδTz
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This can also be used as an alternative means of characterizing strong gratings [13, however, in this case the temperature perturbation must be large (> 100 K) to separate the spectrum of the locally perturbed region from the main grating spectrum and phase information is generally lost
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This can also be used as an alternative means of characterizing strong gratings [13]; however, in this case the temperature perturbation must be large (> 100 K) to separate the spectrum of the locally perturbed region from the main grating spectrum and phase information is generally lost.
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