Hyperfine-interaction- and magnetic-field-induced Bose-Einstein-statistics suppressed two-photon transitions
M. G. Kozlov, D. English, D. Budker

TL;DR
This paper investigates how hyperfine interactions and magnetic fields can induce two-photon transitions in atoms that are normally forbidden by Bose-Einstein statistics, with implications for experimental tests of fundamental physics.
Contribution
It identifies and evaluates two mechanisms by which hyperfine interactions and magnetic fields relax the selection rule for two-photon transitions, expanding understanding of atomic transition behaviors.
Findings
Hyperfine interactions enable forbidden two-photon transitions in atoms with nuclear spin.
Magnetic fields relax the selection rule via Zeeman splitting and state mixing.
Theoretical results support experimental searches for Bose-Einstein-statistics violations.
Abstract
Two-photon transitions between atomic states of total electronic angular momentum and are forbidden when the photons are of the same energy. This selection rule is analogous to the Landau-Yang theorem in particle physics that forbids decays of vector particle into two photons. It arises because it is impossible to construct a total angular momentum quantum-mechanical state of two photons that is permutation symmetric, as required by Bose-Einstein statistics. In atoms with non-zero nuclear spin, the selection rule can be violated due to hyperfine interactions. Two distinct mechanisms responsible for the hyperfine-induced two-photon transitions are identified, and the hyperfine structure of the induced transitions is evaluated. The selection rule is also relaxed, even for zero-nuclear-spin atoms, by application of an external magnetic field. Once again,…
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