Abstract
In preparation for the asymptotic analysis of the exact Fourier–Laplace integral representation given either in (11.45) as
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Notes
- 1.
From the Greek isotimos, of equal worth.
- 2.
Notice that these approximate expressions for the branch point zero locations are different from those given in an earlier paper [11].
- 3.
- 4.
Notice that this result is somewhat different from (and more accurate than) that given in [11].
- 5.
This result is an extension of that given in [11].
- 6.
Recall that it is assumed here that each of the spectral functions \(\tilde{f}\)(ω) and \(\tilde{u}\)(ω − ω c ) is an analytic function of the complex variable ω, regular in the entire complex ω-plane except at a countable number of isolated points where that function may exhibit poles.
- 7.
Notice that Λ(θ) changes discontinuously with the space–time parameter θ as the path P(θ) crosses over each pole. However, each of these discontinuities is cancelled by a corresponding discontinuous change in I(z, θ).
- 8.
If u(t) is bounded and tends to zero rapidly enough such that the Fourier transform of u(t) converges uniformly for all real ω, then \(\tilde{u}\)(ω − ω c ) is an entire function of complex ω.
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Oughstun, K.E. (2009). Analysis of the Phase Function and Its Saddle Points. In: Electromagnetic and Optical Pulse Propagation 2. Springer Series in Optical Sciences, vol 144. Springer, New York, NY. https://doi.org/10.1007/978-1-4419-0149-1_4
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