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Gravitational dressing: from the crossed product to more general algebraic and mathematical structure

Steven B. Giddings

Abstract

The crossed product, and consequent transition from von Neumann algebras of type III to II, is recovered from a truncation of more general gravitational dressing constructions, about certain spacetimes. This is done by extending "standard dressing" constructions previously used to give a perturbative definition of "gravitational splittings," defining approximate localization of information. This result appears to illustrate that this algebraic transition is a small piece of a more general algebraic, or other mathematical, structure associated with quantum gravity. The leading-order structure involves noncommutativity from separated regions, and at the nonperturbative level connects with a possible explanation of holographic behavior for gravity.

Gravitational dressing: from the crossed product to more general algebraic and mathematical structure

Abstract

The crossed product, and consequent transition from von Neumann algebras of type III to II, is recovered from a truncation of more general gravitational dressing constructions, about certain spacetimes. This is done by extending "standard dressing" constructions previously used to give a perturbative definition of "gravitational splittings," defining approximate localization of information. This result appears to illustrate that this algebraic transition is a small piece of a more general algebraic, or other mathematical, structure associated with quantum gravity. The leading-order structure involves noncommutativity from separated regions, and at the nonperturbative level connects with a possible explanation of holographic behavior for gravity.

Paper Structure

This paper contains 31 equations, 3 figures.

Figures (3)

  • Figure 1: Illustration of a standard dressing construction. The dressing $V_S$ external to the neighborhood $U$ only depends on the neighborhood, e.g. through choice of a fixed point $x_0$ of the neighborhood. The full dressing arises by including an additional piece associated with the dressing of a general point.
  • Figure 2: The spacetime of an eternal black hole, represented via Penrose or Eddington-Finkelstein diagrams, together with different spatial slicings. The top row shows a general slicing of the interior and right exterior. The second row shows one member of a family of stationary slicesBHQIUENVU; other members are found through translation by the Killing vector $\xi_t$. The third row is a member of a family of extremal slices, also related by translation by the Killing vector.
  • Figure 3: The spatial geometry of an extremal slice of Fig. \ref{['slices']}c.