Bohigas–Giannoni–Schmit conjecture for quantum spectra of classically chaotic systems
Prove the Bohigas–Giannoni–Schmit conjecture by establishing that, in the semiclassical limit, the unfolded spectral statistics (including the nearest-neighbour spacing distribution) of quantum Hamiltonians whose classical dynamics are fully chaotic coincide with those of Gaussian random matrix ensembles, with the appropriate symmetry class determined by the presence or absence of time-reversal invariance.
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The Bohigas-Giannoni-Schmit (BGS) conjecture, originating from the pioneering work of Bohigas, Giannoni, and Schmit in $ 1984 $, is a fundamental discovery in the field of quantum chaos. It states that the energy spectra of quantum systems, which exhibit complete classical chaos (governed by autonomous Hamiltonians and ergodic behaviour), display statistical properties that can be described using Gaussian Random Matrix Theory (RMT) when examined in the semi-classical limit.
Thus, we propose a reformulation of the GHS conjecture originally conceived in the 80s: random-matrix spectral statistics emerge in the spectral region of the Liouvillian superoperator close to the steady state when the classical analogue displays observable consequences of chaos, either in the transient or in the long-term dynamics.
The chaotic half is due to Bohigas, Giannoni and Schmit, advanced as a conjecture on numerical evidence and since given a semiclassical derivation for uniformly hyperbolic systems by summing correlated pairs of periodic orbits, which is the orbit sum of Sec.~\ref{sec:L4_trace_formula} evaluated beyond its diagonal terms.
The Bohigas--Giannoni--Schmit conjecture (BGS) predicts that generically, the spectra of such systems display the same fluctuation properties at small energy scales as those predicted by random matrix theory.
However, the validity of this approximation remains speculative, and is even known to fail dramatically for certain systems exhibiting exceptional symmetries, such as arithmetic hyperbolic surfaces , for which the length spectrum exhibits exponential degeneracies.
The precise meaning of \say{generic} in the BGS conjecture is unclear, but it is necessary in order to discard exceptional systems for which BGS is known to fail.
According to the Bohigas--Giannoni--Schmit (BGS) conjecture, the statistical properties of the energy levels of a quantum system are determined by the dynamics of the corresponding classical system.