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Published January 2023 | Published
Journal Article Open

Entanglement structures in quantum field theories: Negativity cores and bound entanglement in the vacuum

Abstract

The many-body entanglement between two finite (size-d) disjoint vacuum regions of noninteracting lattice scalar field theory in one spatial dimension, i.e., a (d_A × d_B)_mixed Gaussian continuous variable system, is locally transformed into a tensor-product core of (1_A × 1_B)_mixed entangled pairs. Accessible entanglement within these core pairs exhibits an exponential hierarchy and as such identifies the structure of dominant region modes from which vacuum entanglement could be extracted into a spatially separated pair of quantum detectors. Beyond the core, the remaining modes of the halo are determined to be AB separable in isolation, as well as separable from the core. However, state preparation protocols that distribute entanglement in the form of (1_A × 1_B)_mixed core pairs are found to require additional entanglement in the halo that is obscured by classical correlations. This inaccessible (bound) halo entanglement is found to mirror the accessible entanglement, but with a step behavior as the continuum is approached. It remains possible that alternate initialization protocols that do not utilize the exponential hierarchy of core-pair entanglement may require less inaccessible entanglement. Entanglement consolidation is expected to persist in higher dimensions and may aid classical and quantum simulations of asymptotically free gauge field theories, such as quantum chromodynamics.

Additional Information

©2023 American Physical Society. We would like to thank Silas Beane, Roland Farrell, Neda Hosseinidehaj, Aidan Murran, and John Preskill for valuable discussions. We would also like to thank the Center for Experimental Nuclear Physics and Astrophysics for providing a creative environment for developmental periods of this work. We have made extensive use of Wolfram Mathematica [165]. D.H.B. was supported in part by NSF Nuclear Physics Grant No. PHY-2111046. N.K. was supported in part by the Walter Burke Institute for Theoretical Physics and by the U.S. Department of Energy Office of Science, Office of Advanced Scientific Computing Research (Grant No. DE-SC0020290), and Office of High Energy Physics (Grant No. DE-ACO2-07CH11359). M.J.S. was supported in part by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics, InQubator for Quantum Simulation through Award No. DE-SC0020970 and in part by the Institute for Nuclear Theory with DOE Grant No. DE-FG02-00ER41132.

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Additional details

Created:
August 20, 2023
Modified:
October 23, 2023