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May 8, 2026Journal of High Energy Physics0 citationsOpen Access

No boundary density matrix in elliptic de Sitter dS/ℤ2

RDRaphaël DulacZWZixia Wei

Key Points

  • The aim is to define a no-boundary density matrix for elliptic de Sitter spacetime and explore its implications.
  • Analyzed the Euclidean elliptic de Sitter spacetime and its path integral.
  • Calculated von Neumann and Rényi entropies for free Dirac fermion CFT in two dimensions.
  • Computed time evolution of entanglement entropy after a crosscap quench.
  • Defined a no-boundary density matrix for elliptic de Sitter spacetime.
  • Calculated von Neumann and Rényi entropies as correlation functions on non-orientable surfaces.
  • Identified that the global Hilbert space is one-dimensional while individual observer spaces are nontrivial Fock spaces.

Abstract

A bstract Elliptic de Sitter (dS) spacetime dS/ ℤ 2 is a non-time-orientable spacetime obtained by imposing an antipodal identification to global dS. Unlike QFT on global dS, whose vacuum state can be prepared by a no-boundary Euclidean path integral, the Euclidean elliptic dS does not define a wavefunction in the usual sense. We propose instead that the path integral on the Euclidean elliptic dS defines a no-boundary density matrix. As an explicit example, we study the free Dirac fermion CFT in two-dimensional elliptic dS and analytically compute the von Neumann and the Rényi entropies of this density matrix. The calculation reduces to correlation functions of vertex operators on non-orientable surfaces. As a by-product, we compute the time evolution of entanglement entropy following a crosscap quench in free Dirac fermion CFT. We also comment on a striking feature of free QFT in elliptic dS: its global Hilbert space is one-dimensional, wheres the Hilbert space associated to each observer is a nontrivial Fock space.

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Cite This Study

Dulac et al. (2026) studied this question.

synapsesocial.com/papers/69fd7e90bfa21ec5bbf06d3ahttps://doi.org/10.1007/jhep05(2026)022
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