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Eigenvalues λ m of the correlation kernel obtained by numerical method (dots) versus the spectrum (4.21) of a thermal partition function with appropriate temperature (solid lines) for various x → 1. Only the first few eigenvalues are shown. λ m are symmetric across m = 1/2 line. Although not shown in this figure, the discrepancy between analytics and numerics is well resolved by including the second order corrections, see Figure 5.
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We consider the reflected entropy and the associated entanglement spectrum for free fermions reduced to two intervals in 1+1 dimensions. Working directly in the continuum theory the reflected entropy can be extracted from the spectrum of a singular integral equation whose kernel is determined by the known free fermion modular evolved correlation fu...
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... studying perturbative corrections to this later spectrum we give evidence that the reflected density matrix approaches rapidly the thermal density matrix. This agrees well with the eigenvalues obtained from numerical method, see Figure 2. ...
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A bstract
We consider the reflected entropy and the associated entanglement spectrum for free fermions reduced to two intervals in 1 + 1 dimensions. Working directly in the continuum theory the reflected entropy can be extracted from the spectrum of a singular integral equation whose kernel is determined by the known free fermion modular evolved co...
The problem is formulated as a boundary-value problem for a strip in the complex potential plane and converted to a boundary-value problem for a half-plane by conformal mapping. The solution is obtained using a Cauchy type integral for the density of which a nonlinear integral equation is derived. Its solution is found with the Galerkin method and...
We study quantum quenches and subsequent non-equilibrium dynamics of free Dirac fermions in 1 + 1 spacetime dimensions using time dependent mass. The final state is a normalized boundary state which is called generalized Calabrese-Cardy (gCC) state and the system thermalizes to a generalized Gibb’s Ensemble(GGE). We can also tune the initial states...