Abstract
This chapter will focus mainly on the kicked rotator that displays global classical chaos in its cylindrical phase space for sufficiently strong kicking. The chaotic behavior takes the form of “rapid” quasi-random jumps of the phase variable around the cylinder and “slow” diffusion of the conjugate angular momentum p along the cylinder.
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Notes
- 1.
We are indebted to H.J. Sommers for showing this proof to us.
- 2.
Here and in the following 0+ denotes an arbitrarily small positive number.
- 3.
While ħτ∕I for the kicked rotator naturally arises as a dimensionless measure of Planck’s constant, that role will be played by 1∕j for the kicked top. Therefore, it is convenient to set ħ = 1 in this section.
- 4.
The reader will pardon the sloppiness of denoting the coherent state by |Θϕ〉 rather than |jΘϕ〉.
- 5.
The top does not, in general, display the phenomenon of quantum localization under conditions of classical chaos; from this fact it may be understood that the localization length is larger than 2j + 1; see, however, the subsequent section.
- 6.
- 7.
The “global” spectral average possible here as it was in Sect. 7.2 saves us from having to use the superanalytic Hubbard-Stratonovich transformation.
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Haake, F., Gnutzmann, S., Kuś, M. (2018). Quantum Localization. In: Quantum Signatures of Chaos. Springer Series in Synergetics. Springer, Cham. https://doi.org/10.1007/978-3-319-97580-1_8
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