Dynamical Signatures of Chaos to Integrability Crossover in $2\times 2$
Generalized Random Matrix Ensembles
- URL: http://arxiv.org/abs/2010.16394v2
- Date: Mon, 13 Nov 2023 23:59:15 GMT
- Title: Dynamical Signatures of Chaos to Integrability Crossover in $2\times 2$
Generalized Random Matrix Ensembles
- Authors: Adway Kumar Das, Anandamohan Ghosh
- Abstract summary: We study the energy correlations by calculating the density and 2nd moment of the Nearest Neighbor Spacing (NNS)
We observe that for large $N$ the 2nd moment of NNS and the relative depth of the correlation hole exhibit a second order phase transition at $gamma=2$.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: We introduce a two-parameter ensemble of generalized $2\times 2$ real
symmetric random matrices called the $\beta$-Rosenzweig-Porter ensemble
(\brpe), parameterized by $\beta$, a fictitious inverse temperature of the
analogous Coulomb gas model, and $\gamma$, controlling the relative strength of
disorder. \brpe\ encompasses RPE from all of the Dyson's threefold symmetry
classes: orthogonal, unitary and symplectic for $\beta=1,2,4$. Firstly, we
study the energy correlations by calculating the density and 2nd moment of the
Nearest Neighbor Spacing (NNS) and robustly quantify the crossover among
various degrees of level repulsions. Secondly, the dynamical properties are
determined from an exact calculation of the temporal evolution of the fidelity
enabling an identification of the characteristic Thouless and the equilibration
timescales. The relative depth of the correlation hole in the average fidelity
serves as a dynamical signature of the crossover from chaos to integrability
and enables us to construct the phase diagram of \brpe\ in the $\gamma$-$\beta$
plane. Our results are in qualitative agreement with numerically computed
fidelity for $N\gg2$ matrix ensembles. Furthermore, we observe that for large
$N$ the 2nd moment of NNS and the relative depth of the correlation hole
exhibit a second order phase transition at $\gamma=2$.
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