1996
DOI: 10.1007/bf02099363
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Quantization of a class of piecewise affine transformations on the torus

Abstract: We present a unified framework for the quantization of a family of discrete dynamical systems of varying degrees of "chaoticity". The systems to be quantized are piecewise affine maps on the two-torus, viewed as phase space, and include the automorphisms, translations and skew translations. We then treat some discontinuous transformations such as the Baker map and the sawtooth-like maps. Our approach extends some ideas from geometric quantization and it is both conceptually and calculationally simple.

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Cited by 28 publications
(26 citation statements)
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“…To obtain the Hilbert space we take the subspace of the wave functions on a line whose probability densities, |Ψ(x)| 2 , |Ψ(p)| 2 are periodic in both position and momentum representations, respectively: Ψ(x+1) = exp(i2πϕ q )Ψ(x), Ψ(p + 1) = exp(i2πϕ p )Ψ(p), where ϕ q , ϕ p ∈ [0, 1) are phases parameterizing quantization. The quantization of the baker map requires the phase space volume to be an integer multiple of the quantum of action [8,9,18,19,20,21]. Therefore the effective Planck constant is h = 1/N, for a baker map on a unit torus, where N, an integer, is the dimension of the Hilbert space.…”
Section: The Quantum Multi-baker Mapmentioning
confidence: 99%
“…To obtain the Hilbert space we take the subspace of the wave functions on a line whose probability densities, |Ψ(x)| 2 , |Ψ(p)| 2 are periodic in both position and momentum representations, respectively: Ψ(x+1) = exp(i2πϕ q )Ψ(x), Ψ(p + 1) = exp(i2πϕ p )Ψ(p), where ϕ q , ϕ p ∈ [0, 1) are phases parameterizing quantization. The quantization of the baker map requires the phase space volume to be an integer multiple of the quantum of action [8,9,18,19,20,21]. Therefore the effective Planck constant is h = 1/N, for a baker map on a unit torus, where N, an integer, is the dimension of the Hilbert space.…”
Section: The Quantum Multi-baker Mapmentioning
confidence: 99%
“…There are other quantization schemes of skew translations in the literature[3,2]. However, they do not satisfy Theorem 3.1 and so their relevance to the classical dynamics is unclear.…”
mentioning
confidence: 99%
“…[8]). The basic problem comes from the fact that the projection operators L and E p (for example) do not commute as Ä 0 (even weakly).…”
Section: The Classical Limitmentioning
confidence: 93%