An intriguing and elementary possibility is that familiar massless particles like the photon could be “continuous spin” particles (CSPs) with a small but nonzero spin Casimir $\rho$. In this case, the familiar two polarization states of the photon are accompanied by an infinite tower of integer spaced helicity modes, with couplings dictated entirely by Lorentz symmetry and the parameter $\rho$. We present a formalism for computing bound state atomic transitions for scalar QED when $\rho \ne 0$, employing path integral methods not often used for bound state computations, but that readily generalize to the CSP case. We compute several illustrative amplitudes and show that $\rho \ne 0$ opens new decay channels for atomic transitions with rates controlled by $\rho \alpha /\omega$ for transition frequency $\omega$. These new channels can appreciably modify the rates of “forbidden” transitions. For example, the lifetime of the hydrogen $2s$ state would be affected at $O(1)$ for $\rho \sim 0.1\mathrm{eV}$, suggesting new directions for fundamental tests of QED in laboratory experiments.

Close

PrevNext

Reuse & PermissionsView figure in article

• Electronic transitions
• Gauge theories
• Lifetimes & widths
• Path integrals
• Perturbation theory
• Phenomenology
• Spontaneous emission