Abstract

We propose an experiment to measure the electric dipole moment (EDM) of the electron using ultracold YbF molecules. The molecules are produced as a thermal beam by a cryogenic buffer gas source, and brought to rest in an optical molasses that cools them to the Doppler limit or below. The molecular cloud is then thrown upward to form a fountain in which the EDM of the electron is measured. A non-zero result would be unambiguous proof of new elementary particle interactions, beyond the standard model.

Highlights

  • The standard model of elementary particle physics predicts that the electric dipole moment (EDM) of the electron is exceedingly small [1], de 10−38e.cm, as illustrated in figure 1

  • This happens in the standard model through the Yukawa couplings in the quark sector [2], with the first non-vanishing result appearing at the four-loop level [3]

  • To go significantly beyond the current level of EDM sensitivity, one needs a fundamental improvement in the method, which is what we propose here

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Summary

Introduction

The standard model of elementary particle physics predicts that the electric dipole moment (EDM) of the electron is exceedingly small [1], de 10−38e.cm, as illustrated in figure 1. It will be possible to replace the molecular beam by a molecular fountain, where each molecule can precess coherently for almost one second, rather than the current one millisecond This will allow detection of an EDM as small as 1 × 10−30e.cm, corresponding to CP-violating physics at energies up to 100 TeV. Six beams propagating along the Cartesian directions ±x, ±y, ±zare detuned by approximately 5 MHz to the red of resonance in order to form an optical molasses [37] This cools the molecules to a temperature of order Γ/(2kB) = 140μ K, where Γ is the spontaneous decay rate of the A state. We describe each of these steps in more detail

Thermal beam
Magnetic Guide
Laser Cooling
Molecular Fountain
Electron EDM measurement
Findings
Summary

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