Abstract:We develop a theoretical method going beyond the contact-interaction approximation frequently used in mean-field theories of many-fermion systems, based on the low-energy T matrix of the pair potential to rigorously define the effective radius of the interaction. One of the main consequences of our approach is the possibility to investigate finite-density effects, which are outside the range of validity of approximations based on δ-like potentials. We apply our method to the calculation of density-dependent pr… Show more
“…To extract the unitary parameters thus requires an extrapolation to zero effective range. Range effects in the ufg are also discussed in [14] (large r e ), [4] (Fixed-Node qmc (fnqmc)), and in [15,16] (Bogoliubov-de Gennes (bdg) approximation).…”
We extract the leading effective range corrections to the equation of state of the unitary Fermi gas from ab initio Fixed-Node Quantum Monte Carlo (qmc) (fnqmc) calculations in a periodic box using a Density Functional Theory (dft), and show them to be universal by considering several two-body interactions. Furthermore, we find that the dft is consistent with the best available unbiased qmc calculations, analytic results, and experimental measurements of the equation of state. We also discuss the asymptotic effective-range corrections for trapped systems and present the first qmc results with the correct asymptotic scaling.
“…To extract the unitary parameters thus requires an extrapolation to zero effective range. Range effects in the ufg are also discussed in [14] (large r e ), [4] (Fixed-Node qmc (fnqmc)), and in [15,16] (Bogoliubov-de Gennes (bdg) approximation).…”
We extract the leading effective range corrections to the equation of state of the unitary Fermi gas from ab initio Fixed-Node Quantum Monte Carlo (qmc) (fnqmc) calculations in a periodic box using a Density Functional Theory (dft), and show them to be universal by considering several two-body interactions. Furthermore, we find that the dft is consistent with the best available unbiased qmc calculations, analytic results, and experimental measurements of the equation of state. We also discuss the asymptotic effective-range corrections for trapped systems and present the first qmc results with the correct asymptotic scaling.
“…Hence we neglect the Hartree energy but observe that this has also the positive side effect that it shows more clearly the effect of interactions eventually introduced by the GRPA for quasiparticle excitations in the normal state. Notice that the problems with the Hartree shift ultimately derive from the attempt to describe interactions through the two-body scattering T matrix instead of the bare atom-atom interaction [29]. These problems do not manifest for example in density-functional theories which, when used in the atomic gas context, do not separate the Hartree and exchange-correlation energies [30,31].…”
We study collective excitations of a trapped Fermi gas at finite temperature using the Bogoliubov-de Gennes mean-field theory in conjunction with the generalized random-phase approximation. The collective excitations are analyzed through the density response of a monopole excitation. We show the appearance of several modes at the normal-fluid-superfluid phase-transition temperature: Higgs mode-like pairing amplitude modulations, analogues of the second sound in the trapped gas, and an edge mode that is also the strongest mode in the response.
“…The potential energy curves have been obtained from ab initio quantum chemical calculations using Configuration Interaction with single and double excitations from the reference Hartree-Fock ground state by expanding molecular orbitals in a cc-pVQZ basis set of atomic-centered Gaussians. The singlet and triplet potentials have been used to calculate the interaction as a function of the external magnetic field, taking into account fine and hyperfine structure terms [23].…”
Section: Potential and T -Matrix For The 6 LI Systemmentioning
confidence: 99%
“…We now show how the BdG equation can be rewritten as a function of the T -matrix, and we apply this scheme to investigate an homogeneous system of strongly interacting 6 Li atoms at unitarity [23]. The solution for ultracold atoms at unitarity using FCI requires a nontrivial renormalisation procedure [4].…”
Section: The Gap Equation As a Function Of The T -Matrixmentioning
confidence: 99%
“…We will show that our approach naturally introduces finite-range effects in the system through the dependence of T on the interaction radius of the pair potential, enabling us to discuss the density dependence of the principal thermodynamical observables (gap, chemical potential, transition temperature) [23].…”
We advocate the use of the T -matrix of the pair potential to study the properties of ultracold Fermi gases in the mean-field approximation. Our approach does not require renormalization procedures even in the limit of contact interaction, and it provides a rigorous definition of the range of the potential. We also rewrite the Bogoliubov-de Gennes equation for the pairing function as a function of the T-matrix, and use it to investigate finite-range effects on the main thermodynamic observables in a gas of 6Li atoms at unitarity, calculating the pair potential with ab initio quantum chemical methods
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