Abstract

We show how off-resonant light scattering can provide quantitative information on antiferromagnetic ordering of a two-species fermionic atomic gas in a tightly-confined two-dimensional optical lattice. We analyze the emerging magnetic ordering of atoms in the mean-field and in random phase approximations and show how the many-body static and dynamic correlations, evaluated in the standard Feynman-Dyson perturbation series, can be detected in the scattered light signal. The staggered magnetization reveals itself in the magnetic Bragg peaks of the individual spin components. These magnetic peaks, however, can be considerably suppressed in the absence of a true long-range antiferromagnetic order. The light scattered outside the diffraction orders can be collected by a lens a with highly improved signal-to-shot-noise ratio when the diffraction maxima are blocked. The collective and single-particle excitations are identified in the spectrum of the scattered light. We find that the spin-conserving and spin-exchanging atomic transitions convey information on density, longitudinal spin, and transverse spin correlations. The different correlations and scattering processes exhibit characteristic angular distribution profiles for the scattered light and, e.g., the diagnostic signal of transverse spin correlations could be separated from the signal by the scattering direction, frequency, or polarization. We also analyze the detection accuracy by estimating the number of required measurements, constrained by the heating rate that is determined by inelastic light scattering events. The imaging technique could be extended to the two-species fermionic states in other regions of the phase diagram where the ground state properties are still not fully understood.

Highlights

  • The two-species fermionic Hubbard model is one of the most studied models with strong correlation effects in condensed-matter physics, since Anderson proposed in 1987 [1] that the Hubbard model is the minimum model to describe the physics of the high-temperature superconductors [2]

  • With the rapid advance in cooling and trapping technologies of neutral atoms in optical lattices, there is the exciting prospect that the phase diagram of the fermionic Hubbard model can be explored via quantum simulation in an optical lattice setup with ultracold two-species fermionic atomic gas [3,4,5]

  • We study the AFM ground state of the Mott insulator in a two-species fermionic atomic gas trapped in a tightly-confined 2D optical lattice

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Summary

INTRODUCTION

The two-species fermionic Hubbard model is one of the most studied models with strong correlation effects in condensed-matter physics, since Anderson proposed in 1987 [1] that the Hubbard model (or its strong-coupling limit, the t-J model) is the minimum model to describe the physics of the high-temperature superconductors [2]. For atomic species for which it is possible to achieve far-detuned imaging with the laser tuned in between the resonances of the two spin components, one can enhance the optical signatures of the magnetic Bragg peaks This is because the light scattered from the two components can be π phase shifted with respect to each other, making the peaks directly proportional to the staggered magnetization order parameter. We find that in an AFM-ordered two-species state, the scattered light in the near-forward direction is sensitive to the temperature of the atoms and provides a suitable probe of density and longitudinal spin correlations (from spinconserving atomic transitions). A diagrammatic description of the RPA susceptibilities is presented in Appendix A, and the finite-temperature MFT susceptibilities are given in Appendix B

SUMMARY OF KEY RESULTS
OPTICAL LATTICES AND THE HUBBARD MODEL
Low-energy physics of the Hubbard model
Mean-field Hamiltonian
N2s k0
Mean-field susceptibilities at zero temperature
Time-ordered and retarded correlation functions
Mean-field susceptibilities
RPA susceptibilities
RPA correction to the AFM-order parameter
Scattered intensity
Scattered spectrum
Atom losses to higher bands
Two-species atomic gas of 40K
Elastic scattering
Elastic scattering in the presence of short-range correlations
Inelastic intraband scattering
Inelastic losses to higher bands
Optical components for light detection
Measurement accuracy
Distinguishability of transitions by light polarization
VIII. DIAGNOSTICS OF EXCITATIONS FROM SCATTERED SPECTRUM
Single-particle excitations
Collective modes
CONCLUDING REMARKS
RBZD T
Findings
RPA renormalization of the AFM-order parameter

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