We experimentally study the spin dynamics of mesoscopic ensembles of ultracold magnetic spin-3 atoms located in two separated wells of an optical dipole trap.
arXiv:1407.8130 (2014) / Phys. Rev. A 90, 043607 (2014)
We report on the realization of quantum magnetism using a degenerate dipolar gas in an optical lattice. Our system implements a lattice model resembling the celebrated 𝑡−𝐽 model.
arXiv:1306.2754 (2013) / Phys. Rev. Lett. 111, 185305 (2013)
We study dipolar relaxation of a chromium Bose-Einstein condensate loaded into a three-dimensional (3D) optical lattice.
arXiv:1212.5469 (2012) / Phys. Rev. A 87, 051609(R) (2013)
We measure the excitation spectrum of a dipolar chromium Bose-Einstein condensate with Raman-Bragg spectroscopy.
arXiv:1205.6305 (2012) / Phys. Rev. Lett. 109, 155302 (2012)
We study the spinor properties of 𝑆 =3 52Cr condensates, in which dipole-dipole interactions allow changes in magnetization.
arXiv:1103.4819 (2011) / Phys. Rev. Lett. 106, 255303 (2011)
We observe interband transitions mediated by dipole-dipole interactions for an array of 1D quantum gases of chromium atoms, trapped in a 2D optical lattice.
arXiv:1010.3241 (2010) / Phys. Rev. Lett. 106, 015301 (2011)
We have measured the effect of dipole-dipole interactions on the frequency of a collective mode of a Bose-Einstein condensate.
arXiv:1005.2493 (2010) / Phys. Rev. Lett. 105, 040404 (2010)
We study dipolar relaxation in both ultracold thermal and Bose-condensed Cr 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 three-dimensional (3D) to two-dimensional (2D).
arXiv:1002.0222 (2010) / Phys. Rev. A 81, 042716 (2010)
One-dimensional (1D) dipolar quantum gases are characterized by a very special condition where super-strong correlations occur to significantly affect the static and dynamical low-energy behavior.
Laser Phys. 19, 554 (2009) / HAL Id:ensl-00517334 (2010)
