Atomic-beam measurement of parity nonconservation in cesium

Abstract

We present a new measurement of parity nonconservation in cesium. In this experiment, a laser excited the 6S\ensuremath{\rightarrow}7S transition in an atomic beam in a region of static electric and magnetic fields. The quantity measured was the component of the transition rate arising from the interference between the parity nonconserving amplitude, ${\mathrm{scrE}}_{\mathrm{PNC}}$, and the Stark amplitude, \ensuremath{\beta}E. Our results are Im${\mathrm{scrE}}_{\mathrm{PNC}/\mathrm{\ensuremath{\beta}}=\mathrm{\ensuremath{-}}1.65\ifmmode\pm\else\textpm\fi{}0.13}$ mV/cm and ${C}_{2p}$=-2\ifmmode\pm\else\textpm\fi{}2, where ${C}_{2p}$ is the proton-axial-vector--electron-vector neutral-current coupling constant. These results are in agreement with previous less precise measurements in cesium and with the predictions of the electroweak standard model. We give a detailed discussion of the experiment with particular emphasis on the treatment and elimination of systematic errors. This experimental technique will allow future measurements of significantly higher precision.