Log to log-log crossover of entanglement in $(1+1)-$ dimensional massive
scalar field
- URL: http://arxiv.org/abs/2103.01772v2
- Date: Wed, 19 May 2021 14:58:09 GMT
- Title: Log to log-log crossover of entanglement in $(1+1)-$ dimensional massive
scalar field
- Abstract summary: We study three measures of quantum correlations -- entanglement spectrum, entanglement entropy, and logarithmic negativity -- for (1+1)-dimensional massive scalar field in flat spacetime.
The entanglement spectrum for the discretized scalar field in the ground state indicates a cross-over in the zero-mode regime.
We show that this cross-over manifests as a change in the behavior of the leading order term for entanglement entropy and logarithmic negativity close to the zero-mode limit.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: We study three different measures of quantum correlations -- entanglement
spectrum, entanglement entropy, and logarithmic negativity -- for
(1+1)-dimensional massive scalar field in flat spacetime. The entanglement
spectrum for the discretized scalar field in the ground state indicates a
cross-over in the zero-mode regime, which is further substantiated by an
analytical treatment of both entanglement entropy and logarithmic negativity.
The exact nature of this cross-over depends on the boundary conditions used --
the leading order term switches from a $\log$ to $\log-\log$ behavior for the
Periodic and Neumann boundary conditions. In contrast, for Dirichlet, it is the
parameters within the leading $\log-\log$ term that are switched. We show that
this cross-over manifests as a change in the behavior of the leading order
divergent term for entanglement entropy and logarithmic negativity close to the
zero-mode limit. We thus show that the two regimes have fundamentally different
information content. Furthermore, an analysis of the ground state fidelity
shows us that the region between critical point $\Lambda=0$ and the crossover
point is dominated by zero-mode effects, featuring an explicit dependence on
the IR cutoff of the system. For the reduced state of a single oscillator, we
show that this cross-over occurs in the region $Nam_f\sim \mathscr{O}(1)$.
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