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Entropic Bounds on Semiclassical Measures for Quantized One-Dimensional Maps

机译:量化一维图的半经典测度的熵界

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摘要

Quantum ergodicity asserts that almost all infinite sequences of eigenstates of quantized ergodic Hamiltonian systems are equidistributed in phase space. This, however, does not prohibit existence of exceptional sequences which might converge to different (non-Liouville) classical invariant measures. It has been recently shown by N. Anantharaman and S. Nonnenmacher in [20,21] (with H. Koch) that for Anosov geodesic flows the metric entropy of any semiclassical measure μ must satisfy a certain bound. This remarkable result seems to be optimal for manifolds of constant negative curvature, but not in the general case, where it might become even trivial if the (negative) curvature of the Riemannian manifold varies a lot. It has been conjectured by the same authors, that in fact, a stronger bound (valid in the general case) should hold. In the present work we consider such entropic bounds using the model of quantized piecewise linear one-dimensional maps. For a certain class of maps with non-uniform expansion rates we prove the Anantharaman-Nonnenmacher conjecture. Furthermore, for these maps we are able to construct some explicit sequences of eigenstates which saturate the bound. This demonstrates that the conjectured bound is actually optimal in that case.
机译:量子遍历性断言,量化遍历哈密顿系统的本征态的几乎所有无穷序列都均匀分布在相空间中。但是,这并不禁止存在可能会收敛到不同(非Liouville)经典不变量度的例外序列。 N. Anantharaman和S. Nonnenmacher最近在[20,21](与H. Koch)中表明,对于Anosov测地流,任何半经典量度μ的量度熵必须满足一定的界限。对于非负曲率恒定的流形来说,这一非凡的结果似乎是最佳的,但是在一般情况下,如果黎曼流形的(负)曲率变化很大,则可能变得微不足道。相同作者推测,实际上应该有一个更强的界限(在一般情况下有效)。在当前的工作中,我们使用量化的分段线性一维映射模型来考虑这种熵范围。对于某些具有非均匀扩展速率的地图,我们证明了Anantharaman-Nonnenmacher猜想。此外,对于这些映射,我们能够构造一些明确的本征态序列,从而使边界饱和。这表明在这种情况下,猜想界实际上是最佳的。

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