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When left and right disagree: entropy and von Neumann algebras in quantum gravity with general AlAdS boundary conditions

  • Donald Marolf,
  • Daiming Zhang

摘要

Euclidean path integrals for UV-completions of d-dimensional bulk quantum gravity were recently studied in [1] by assuming that they satisfy axioms of finiteness, reality, continuity, reflection-positivity, and factorization. Sectors H B \( {\mathcal{H}}_{\mathcal{B}} \) of the resulting Hilbert space were then defined for any (d − 2)-dimensional surface B \( \mathcal{B} \) , where B \( \mathcal{B} \) may be thought of as the boundary ∂Σ of a bulk Cauchy surface in a corresponding Lorentzian description, and where B \( \mathcal{B} \) includes the specification of appropriate boundary conditions for bulk fields. Cases where B \( \mathcal{B} \) was the disjoint union BB of two identical (d − 2)-dimensional surfaces B were studied in detail and, after the inclusion of finite-dimensional ‘hidden sectors,’ were shown to provide a Hilbert space interpretation of the associated Ryu-Takayanagi entropy. The analysis was performed by constructing type-I von Neumann algebras A L B \( {\mathcal{A}}_L^B \) , A R B \( {\mathcal{A}}_R^B \) that act respectively at the left and right copy of B in BB.

Below, we consider the case of general B \( \mathcal{B} \) , and in particular for B \( \mathcal{B} \) = BLBR with BL, BR distinct. For any BR, we find that the von Neumann algebra at BL acting on the off-diagonal Hilbert space sector H B L B R \( {\mathcal{H}}_{B_L\bigsqcup {B}_R} \) is a central projection of the corresponding type-I von Neumann algebra on the ‘diagonal’ Hilbert space H B L B L \( {\mathcal{H}}_{B_L\bigsqcup {B}_L} \) . As a result, the von Neumann algebras A L B L \( {\mathcal{A}}_L^{B_L} \) , A R B L \( {\mathcal{A}}_R^{B_L} \) defined in [1] using the diagonal Hilbert space H B L B L \( {\mathcal{H}}_{B_L\bigsqcup {B}_L} \) turn out to coincide precisely with the analogous algebras defined using the full Hilbert space of the theory (including all sectors H B \( {\mathcal{H}}_{\mathcal{B}} \) ). A second implication is that, for any H B L B R \( {\mathcal{H}}_{B_L\bigsqcup {B}_R} \) , including the same hidden sectors as in the diagonal case again provides a Hilbert space interpretation of the Ryu-Takayanagi entropy. We also show the above central projections to satisfy consistency conditions that lead to a universal central algebra relevant to all choices of BL and BR.