Abstract
Random matrix theory (RMT) serves as a very useful backdrop for the discussion of classical chaos and its effects on quantum mechanics. Two important suggestions began this fruitful association: the conjecture by Bohigas, Giannoni, and Schmit1 associated RMT phenomenology with quantum eigenstates of classically chaotic systems. Berry’s conjecture2 stated that quantum eigenstates of classically chaotic systems should locally look like random superpositions of plane waves of the same (local) wavevector magnitude k, producing Gaussian random fluctuations in position space. These two closely related ideas turn out to be the clay out of which the truth is molded. Much research has centered on modifications to the extreme uniformity of RMT, modifications imposed by known constraints on the quantum dynamics. In fact there is no Hamiltonian system whose eigenstates are known to hold to the rigors of true Gaussian randomness.
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L. Kaplan and E. J. Heller, unpublished.
L. Kaplan, unpublished.
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Kaplan, L., Heller, E.J. (1999). Theory of Eigenfunction Scarring. In: Lerner, I.V., Keating, J.P., Khmelnitskii, D.E. (eds) Supersymmetry and Trace Formulae. NATO ASI Series, vol 370. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-4875-1_6
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