Abstract
The first attempt to understand why spectral fluctuations of quantum chaotic systems are faithfully mirrored by random matrices was proposed by Pechukas.
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Notes
- 1.
It seems that in order to exhibit the Hamiltonian character of the dynamics of eigenphases and eigenvectors of the Floquet operator (11.2.2) we had to made two “educated guesses”, one concerning the choice of l mn instead of v mn, m≠n as dynamical variables, cf. (11.2.7), and the second the proper form of the Poisson brackets. In fact, both are easily derived by observing that \(F(\lambda )=\exp (-i\lambda V)F_0\) can be treated as a simple Hamiltonian flow in the space of unitary matrices. The above dynamical equations for ϕ, p, and l are then obtained by changing variables and symmetry reduction; the procedure automatically gives the l as correct variables and determines uniquely all Poisson brackets for ϕ, p, and l as well as the Hamiltonian function itself, for all symmetry classes [12, 13].
- 2.
Ref. [14] relates our issue to Dirac’s theory of constrained Hamiltonian systems.
- 3.
One should keep in mind that the constraint l mm = 0 can be consistently imposed only after all Poisson brackets are evaluated.
- 4.
Note that we have set Planck’s constant equal to unity here such that its role is taken over by 1∕j; in more conventional notation the transition from commutators of quantum observables \(\hat {A},\hat {B},\ldots \) to Poisson brackets of the associated classical observables A, B, … reads \(\frac {\mathrm {i}}{\hbar }[\hat {A},\hat {B}]\to \{A,B\}=\frac {\partial A}{\partial p} \frac {\partial B}{\partial q}-\frac {\partial B}{\partial p}\frac {\partial A}{\partial q}\).
- 5.
More precisely, over all independent real parameters in the Hermitian matrix v.
- 6.
Terms with m − ν pairs plus an unmatched \(\delta (i_{k} \pm 1, i_{{\mathcal {P}} k} )\) are smaller by at least a factor 1∕N; for the sake of brevity, we forego the treatment of that case.
- 7.
To simplify the appearance of T m(S, n, {l i}) we have assumed l 1≠l 2≠ … ≠l n. See the footnote to (5.12.13).
- 8.
Note that the “time” τ of Sect. 11.10 is renamed as λ such that \(g=\cos \lambda \), and now the previous parameter \(\lambda =\tan \tau \) appears as \(\tan \lambda \); moreover, for the reader’s convenience, we rename the perturbation V as H 1.
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Haake, F., Gnutzmann, S., Kuś, M. (2018). Level Dynamics. In: Quantum Signatures of Chaos. Springer Series in Synergetics. Springer, Cham. https://doi.org/10.1007/978-3-319-97580-1_11
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