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Phys. Rev. D 51, 1800–1817 (1995)

Spacetime information

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James B. Hartle
Department of Physics, University of California, Santa Barbara, California 93106-9530
Isaac Newton Institute for the Mathematical Sciences, University of Cambridge, Cambridge CB3 0EH, United Kingdom

Received 6 September 1994; published in the issue dated 15 February 1995

In usual quantum theory, the information available about a quantum system is defined in terms of the density matrix describing it on a spacelike surface. This definition must be generalized for extensions of quantum theory which neither require, nor always permit, a notion of state on a spacelike surface. In particular, it must be generalized for the generalized quantum theories appropriate when spacetime geometry fluctuates quantum mechanically or when geometry is fixed but not foliable by spacelike surfaces. This paper introduces a four-dimensional notion of the information available about a quantum system’s boundary conditions in the various sets of decohering, coarse-grained histories it may display. This spacetime notion of information coincides with the familiar one when quantum theory is formulable in terms of states on spacelike surfaces but generalizes this notion when it cannot be so formulated. The idea of spacetime information is applied in several contexts: When spacetime geometry is fixed the information available through alternatives restricted to a fixed spacetime region is defined. The information available through histories of alternatives of general operators is compared to that obtained from the more limited coarse grainings of sum-over-histories quantum mechanics that refer only to coordinates. The definition of information is considered in generalized quantum theories. We consider as specific examples time-neutral quantum mechanics with initial and final conditions, quantum theories with nonunitary evolution, and the generalized quantum frameworks appropriate for quantum spacetime. In such theories complete information about a quantum system is not necessarily available on any spacelike surface but must be searched for throughout spacetime. The information loss commonly associated with the ‘‘evolution of pure states into mixed states’’ in black hole evaporation is thus not in conflict with the principles of generalized quantum mechanics.

© 1995 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.51.1800
DOI:
10.1103/PhysRevD.51.1800
PACS:
03.65.Bz, 04.60.-m, 04.70.Dy, 98.80.Hw

See Also

Comment: Adrian Kent, Comment on “Spacetime information”, Phys. Rev. D 56, 2469 (1997).