4.2 Article

Spin and density self-ordering in dynamic polarization gradients fields

期刊

PHYSICAL REVIEW RESEARCH
卷 3, 期 1, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevResearch.3.013173

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资金

  1. European Union (EU) [721465]
  2. ESQ fellowship of the Austrian Academy of Sciences (OAW)
  3. Lise-Meitner Fellowship of the Austrian Science Fund (FWF) [M2438-NBL]
  4. FWF [I3964-N27]
  5. National Agency for Research (ANR) of France
  6. Marie Curie Actions (MSCA) [721465] Funding Source: Marie Curie Actions (MSCA)

向作者/读者索取更多资源

In this study, we investigate the zero-temperature quantum phase diagram of a two-component Bose-Einstein condensate in an optical cavity. The coupled atom-cavity system demonstrates key aspects of the t-J-V-W model, showcasing a rich phase diagram with multiple density and spin-ordered phases that can be controlled through pump strength and detuning. Real-time observation of emitted fields can provide strong signatures of the realized phase and facilitate the determination of phase transition lines.
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 a 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 ferromagnetic and antiferromagnetic order along the cavity axis, which can be controlled via the pump strength and detuning. 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.

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