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Entangled de Sitter from Stringy Axionic Bell pair I: An analysis using Bunch Davies vacuum

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arxiv 1708.02265 v3 pith:SSW36S5O submitted 2017-08-07 hep-th astro-ph.COgr-qchep-phquant-ph

classification hep-thastro-ph.COgr-qchep-phquant-ph
keywords entanglemententropybellbunchdaviesquantumsitteranalysis
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

In this work, we study the quantum entanglement and compute entanglement entropy in de Sitter space for a bipartite quantum field theory driven by axion originating from ${\bf Type~ IIB}$ string compactification on a Calabi Yau three fold (${\bf CY^3}$) and in presence of ${\bf NS5}$ brane. For this compuation, we consider a spherical surface ${\bf S}^2$, which divide the spatial slice of de Sitter (${\bf dS_4}$) into exterior and interior sub regions. We also consider the initial choice of vaccum to be Bunch Davies state. First we derive the solution of the wave function of axion in a hyperbolic open chart by constructing a suitable basis for Bunch Davies vacuum state using Bogoliubov transformation. We then, derive the expression for density matrix by tracing over the exterior region. This allows us to compute entanglement entropy and R$\acute{e}$nyi entropy in $3+1$ dimension. Further we quantify the UV finite contribution of entanglement entropy which contain the physics of long range quantum correlations of our expanding universe. Finally, our analysis compliments the necessary condition for the violation of Bell's inequality in primordial cosmology due to the non vanishing entanglement entropy for axionic Bell pair.

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Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Open Quantum Entanglement: A study of two atomic system in static patch of de Sitter space

    hep-th 2019-08 reject novelty 5.0 of 10

    Using a two-atom open quantum system in de Sitter space, the authors claim to derive analytic entanglement dynamics and Bell inequality violation, but the derivation rests on an ad hoc imaginary-frequency condition.

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