Abstract

We examine, in a quantum mechanical setting, the Hilbert space representation of the BRST symmetry associated with Schwinger-Keldysh path integrals. This structure had been postulated to encode important constraints on influence functionals in coarse-grained systems with dissipation, or in open quantum systems. Operationally, this entails uplifting the standard Schwinger-Keldysh two-copy formalism into superspace by appending BRST ghost degrees of freedom. These statements were previously argued at the level of the correlation functions. We provide herein a complementary perspective by working out the Hilbert space structure explicitly. Our analysis clarifies two crucial issues not evident in earlier works: firstly, certain background ghost insertions necessary to reproduce the correct Schwinger-Keldysh correlators arise naturally. Secondly, the Schwinger-Keldysh difference operators are systematically dressed by the ghost bilinears, which turn out to be necessary to give rise to a consistent operator algebra. We also elaborate on the structure of the final state (which is BRST closed) and the future boundary condition of the ghost fields.

Highlights

  • The Schwinger-Keldysh formalism [1,2,3] allows one to compute real-time observables in either closed or open quantum systems prepared initially in a mixed state

  • In a quantum mechanical setting, the Hilbert space representation of the Becchi, Rouet, Stora, and Tyutin (BRST) symmetry associated with Schwinger-Keldysh path integrals

  • We find that there is ample freedom in how one can embed the Schwinger-Keldysh doubled formalism into an enlarged Hilbert space where our BRST symmetries act naturally

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Summary

INTRODUCTION

The Schwinger-Keldysh formalism [1,2,3] allows one to compute real-time observables in either closed or open quantum systems prepared initially in a (without loss of generality) mixed state. We find that there is ample freedom in how one can embed the Schwinger-Keldysh doubled formalism into an enlarged Hilbert space where our BRST symmetries act naturally. The initial state of our quantum system as well as the future boundary condition of the Schwinger-Keldysh construction are uplifted into this extended Hilbert space, albeit with some freedom. Along with this uplift, we demonstrate how to uplift the operator algebra in a fashion consistent with the OPE structure.

BRST SYMMETRY IN SCHWINGER-KELDYSH: A REVIEW
SCHWINGER-KELDYSH IN HILBERT SPACE
States in the doubled Hilbert space
Superspace uplift and constraints
States in the extended Hilbert space
Superoperators and the OPE
QUANTUM HARMONIC OSCILLATOR
Ladder superoperators and Hilbert space
Composite operators
Product multiplet
Difference multiplet
Average multiplet
Superembedding of states
Superspace correlators
One-point functions
Two-point functions
Example
GENERALIZATIONS AND OPEN QUESTIONS
Interacting theories
Lessons for QFTs
Full Text
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