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Saddle-Point Method for a Complex Function of Several Arguments

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Dissipative Quantum Chaos and Decoherence

Part of the book series: Springer Tracts in Modern Physics ((STMP,volume 172))

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Abstract

Let x represent M real variables x 1,..., x m, and let F(x) and G(x) be complex-valued functions of x with Re F ≤ 0 in the volume V in \( \mathcal{R}^M \) over which we are going to integrate. Suppose that V contains a single nondegenerate stationary point x 0 with xi F(x 0) = 0, i = 1,..., M. Let us denote by Q m×m the matrix of the negative second derivatives, i.e. (Q m×m) ik = - xi xk F(x) taken at x = x 0. The condition of nondegeneracy means detQ m × m ≠ 0. We then have, for J → ∞ [190],

$$ \int_V {d^M xe^{JF(x)} G(x)} = G(x_0 )\sqrt {\frac{{(2\pi )^M }} {{J^M |\det Q_{M \times M} |}}} e^{JF(x_0 ) - (i/2)IndQ_{M \times M} } [1 + \mathcal{O}(1/J)]. $$
((A.1))

Here IndQ m × m is the index of the complex quadratic form χ of M real variables,

$$ \chi = \sum\limits_{i,j = 1}^M {(Q_{M \times M} )_{ij} x_i x_j .} $$
((A.2))

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© 2001 Springer-Verlag Berlin Heidelberg

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(2001). Saddle-Point Method for a Complex Function of Several Arguments. In: Dissipative Quantum Chaos and Decoherence. Springer Tracts in Modern Physics, vol 172. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-40916-5_8

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  • DOI: https://doi.org/10.1007/3-540-40916-5_8

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  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-540-41197-0

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