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 $Nam_f\sim \mathscr{O}(1)$.

Highlights

  • Quantum correlations play an important role when describing quantum physics as they help us extract relevant information about a system via measurements

  • The theory can be written on a lattice, with the Hilbert space being a product of Hilbert spaces for each lattice point, i.e., H 1⁄4⊗i Hi

  • Let HA be the product of Hilbert spaces at lattice sites within the spatial region A and HB be the product over the remaining lattice sites so that

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Summary

INTRODUCTION

Quantum correlations play an important role when describing quantum physics as they help us extract relevant information about a system via measurements. [5,10] as we analytically obtain a crossover in the leading divergent term of entanglement entropy around Namf ∼ Oð1Þ, from log to log-log We put forth an analytical treatment of the crossover that primarily involves studying the leading order divergent term in the zero-mode limit for entanglement entropy and logarithmic negativity for maximally entangled pure states.

MODEL AND QUANTIFYING TOOLS
ENTANGLEMENT SPECTRUM
COVARIANCE MATRIX APPROACH TO ENTANGLEMENT ENTROPY
Dirichlet boundary condition
Neumann boundary condition
ENTANGLEMENT ENTROPY
Effects on scaling symmetry
LOGARITHMIC NEGATIVITY
Periodic boundary conditions
Neumann boundary conditions
Dirichlet boundary conditions
Large N limit analysis
THE GROUND-STATE OVERLAP FUNCTION
VIII. CONCLUSIONS AND DISCUSSIONS
Eigenvalues for logarithmic negativity
Expression for logarithmic negativity
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