Control of dipolar relaxation in external fields
B. Pasquiou, G. Bismut, Q. Beaufils, A. Crubellier, E. Mar\'echal, P., Pedri, L. Vernac, O. Gorceix, B. Laburthe-Tolra

TL;DR
This paper investigates methods to control dipolar relaxation in ultra-cold chromium gases using magnetic fields and optical lattices, providing precise measurements of scattering lengths and insights into stability and dynamics of dipolar quantum gases.
Contribution
It introduces three control techniques for dipolar relaxation, offers the most precise measurements of the chromium atom scattering length, and explores the effects of reduced dimensionality and radio-frequency fields on relaxation processes.
Findings
Dipolar relaxation can be strongly suppressed at specific non-zero magnetic fields.
Precise determination of the chromium atom scattering length as approximately 103 a0.
Dipolar relaxation rate decreases significantly in reduced dimensionality and can be tuned with rf fields.
Abstract
We study dipolar relaxation in both ultra-cold thermal and Bose-condensed chromium atom gases. We show three different ways to control dipolar relaxation, making use of either a static magnetic field, an oscillatory magnetic field, or an optical lattice to reduce the dimensionality of the gas from 3D to 2D. Although dipolar relaxation generally increases as a function of a static magnetic field intensity, we find a range of non-zero magnetic field intensities where dipolar relaxation is strongly reduced. We use this resonant reduction to accurately determine the S=6 scattering length of chromium atoms: . We compare this new measurement to another new determination of , which we perform by analysing the precise spectroscopy of a Feshbach resonance in d-wave collisions, yielding . These two measurements provide by far the most precise…
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