Abstract

Many-body physics poses one of the greatest challenges to science in the 21st century. Still more daunting is the problem of accurately calculating the properties of quantum many-body systems in the strongly correlated regime. Cold atomic gases provide an excellent test ground, for both experimentalists and theorists, to study the exotic and sometimes counterintuitive behavior of quantum many-body problems. Of particular interest is the appearance of collective excitations in these systems, such as the famous Goldstone mode and the elusive Higgs mode. It is particularly important to assess the robustness of theoretical and computational techniques to study such excitations. We build on the unprecedented opportunity provided by the fact that, in some cases, exact numerical predictions can be obtained through quantum Monte Carlo. We use these predictions to assess the accuracy of the Random Phase Approximation, which is widely considered to be a method of choice for the study of the collective excitations in a cold atomic Fermi gas modeled with a Fermi–Hubbard Hamiltonian. We found good agreement between the two methodologies for the dynamic properties, particularly for the position of the Goldstone mode. We also explored the possibility of using a renormalized, effective potential in place of the physical potential. We determined that using a renormalized potential is likely too simplistic a method for improving the accuracy of generalized Random Phase Approximation and that a more sophisticated approach is needed.

Highlights

  • The equations of quantum mechanics provide the most complete description of the world known

  • We provide the new results obtained after using an effective potential in Generalized Random Phase Approximation (GRPA), optimized using our AFQMC

  • The momentum dependent disagreement between AFQMC and GRPA in the intermediate scattering functions raises the possibility of using the AFQMC results to find a renormalized, effective potential Ue f f for GRPA, that would minimize the disagreement between AFQMC and GRPA for a given momentum

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Summary

Introduction

The equations of quantum mechanics provide the most complete description of the world known. By using the Feshbach resonance, different inter-atomic potentials can be engineered This opens the exciting possibility of using cold atoms as physical models of seemingly unrelated systems, from the superfluid interiors of neutron stars to exotic phases in condensed matter physics. Since QMC has seen such dramatic progress over the past 30 years, it is possible, in certain cases, to obtain exact results for some dynamical properties of cold atomic gases [15,16,19]. Though the families of approximate methods do not provide exact results, they are computationally inexpensive and allow the calculation of the real-time dynamical properties of very large systems.

The Fermi–Hubbard Model and Correlation Functions
Comparison of GRPA and AFQMC
Optimizing GRPA Using a Renormalized Effect Potential
Accuracy of GRPA for Static and Dynamic Properties
Conclusions and Future Directions
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