Abstract

We study the zero-temperature quantum phase diagram for a two-component Bose-Einstein condensate in an optical cavity. The two atomic spin states are Raman coupled by two transverse orthogonally-polarized, blue detuned plane-wave lasers inducing a repulsive cavity potential. For weak pump the lasers favor a state with homogeneous density and predefined uniform spin direction. When one pump laser is polarized parallel to the cavity mode polarization, the photons coherently scattered into the resonator induce a polarization gradient along the cavity axis, which mediates long-range density-density, spin-density, and spin-spin interactions. We show that the coupled atom-cavity system implements central aspects of the $t$-$J$-$V$-$W$ model with a rich phase diagram. At the mean-field limit we identify at least four qualitatively distinct density- and spin-ordered phases including ferro- and anti-ferromagnetic order along the cavity axis, which can be controlled via the pump strength and detuning. A real time observation of amplitude and phase of the emitted fields bears strong signatures of the realized phase and allows for real-time determination of phase transition lines. Together with measurements of the population imbalance most properties of the phase diagram can be reconstructed.

Highlights

  • Quantum gas cavity QED—ultracold atoms near zero temperature coupled to photons in high-Q cavity modes—has become an outstanding experimental platform to study coherent many-body quantum dynamics in a precisely controllable and readily observable form [1,2]

  • We study the zero-temperature quantum phase diagram for a two-component Bose-Einstein condensate in an optical cavity

  • We theoretically studied combined spin and density selfordering of a spinor Bose-Einstein condensate (BEC) inside an optical cavity, transversally illuminated by two orthogonally polarized pump lasers in a restricted one-dimensional (1D) geometry

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Summary

INTRODUCTION

Quantum gas cavity QED—ultracold atoms near zero temperature coupled to photons in high-Q cavity modes—has become an outstanding experimental platform to study coherent many-body quantum dynamics in a precisely controllable and readily observable form [1,2]. Making use of several atomic Zeeman sublevels allows one to emulate pseudospin dynamics in ultracold atomic gases It was suggested theoretically [7,8,9,10,11,12] that cavity-enhanced Raman transitions can induce long-range periodic spin-spin interactions. Using cavity-enhanced Raman coupling in a scheme via two external pump lasers and a cavity mode blue detuned with respect to the atomic transitions, we encounter dynamical polarization gradients. The polarization modulation of the effective dynamic light field along the cavity axis induces dominantly long-range interactions among the atoms via the p-band self-ordering [20,21,22]. Phase diagrams than for spinless particles [3,6,21,33,34,35,36,37], as we discuss in the following

CAVITY-INDUCED LONG-RANGE INTERACTIONS AND THE EFFECTIVE SPIN HAMILTONIAN
MEAN-FIELD PHASE DIAGRAM
YZ-AFM phase
FM phase
XY-AFM phase
CONCLUSIONS
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