Abstract

Relativistic invariance of the vacuum is (or follows from) one of the Wightman axioms which is commonly believed to be true. Without these axioms, here we present a direct and general proof of continuous relativistic invariance of all real-time vacuum correlations of fields, not only scattering (forward in time), based on closed time path formalism. The only assumptions are basic principles of relativistic quantum field theories: the relativistic invariance of the Lagrangian, of the form including known interactions (electromagnetic, weak and strong), and standard rules of quantization. The proof is in principle perturbative leaving a possibility of spontaneous violation of invariance. Time symmetry is however manifestly violated.

Highlights

  • In this paper, we confirm the common intuition by a direct proof, not relying on Wightman axioms

  • We show that zero-temperature vacuum correlations of fields at real spacetime points are invariant under continuous transformations of a reference frame

  • We shall use the framework of the closed time path formalism (CTP) [14,15,16] where correlations are defined on the complex path

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Summary

Introduction

We confirm the common intuition by a direct proof, not relying on Wightman axioms. We show that zero-temperature vacuum correlations of fields at real spacetime points are invariant under continuous transformations of a reference frame. We shall use the framework of the closed time path formalism (CTP) [14,15,16] where correlations are defined on the complex path (going downwards with respect to imaginary part). It is defined in a particular reference frame, the invariance is not manifest. Even if the dynamics is symmetric with respect to time reversal, CTP is not (except special cases, e.g. at space-like points or in scattering problems).

Closed time path formalism and definitions
Contour shape independence
Lorentz invariance
Relativistic notation in CTP
Formal proof of invariance
Free theories
Interaction
Incomplete proofs
Absence of time-reversal symmetry
Conclusions
Free Green functions
Wick theorem
Hamiltonian–Lagrangian equivalence for bosonic fields
Hamiltonian–Lagrangian equivalence for fermionic fields
Conservation laws
Wick theorem for path integrals
Full Text
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