Aspects of Berry phase in QFT
Marco Baggio, Vasilis Niarchos, Kyriakos Papadodimas
TL;DR
This work develops a comprehensive Berry-phase framework for quantum field theories, showing that adiabatic parameter variations induce non-trivial geometric phases even in simple QFTs like electromagnetism with a theta term. By leveraging the operator-state correspondence, conformal perturbation theory, and SUSY nonrenormalization properties, the authors connect Berry connections to the geometry of conformal manifolds and Seiberg–Witten moduli spaces, yielding exact results (tt* equations) in 2d N=(2,2) and 4d N=2 SCFTs. They derive explicit curvature formulas for various settings, including Coulomb-branch photons and massive N=1 theories on R × T^3, and establish a general equivalence between Berry curvature and conformal perturbation theory data. The results illuminate how operator mixing under adiabatic deformations encodes deep geometric information about the moduli spaces of QFTs and offer potential experimental probes in systems with tunable theta or coupling parameters.
Abstract
When continuous parameters in a QFT are varied adiabatically, quantum states typically undergo mixing---a phenomenon characterized by the Berry phase. We initiate a systematic analysis of the Berry phase in QFT using standard quantum mechanics methods. We show that a non-trivial Berry phase appears in many familiar QFTs. We study a variety of examples including free electromagnetism with a theta angle, and certain supersymmetric QFTs in two and four spacetime dimensions. We also argue that a large class of QFTs with rich Berry properties is provided by CFTs with non-trivial conformal manifolds. Using the operator-state correspondence we demonstrate in this case that the Berry connection is equivalent to the connection on the conformal manifold derived previously in conformal perturbation theory. In the special case of chiral primary states in 2d N=(2,2) and 4d N=2 SCFTs the Berry phase is governed by the tt* equations. We present a technically useful rederivation of these equations using quantum mechanics methods.
