Momentum distribution of non-interacting fermions enclosed in a box

We investigate the ground state of the one-dimensional fermionic system enclosed in a hard-wall trap with attractive contact $p$ -wave interactions. Based on the Bethe ansatz method, the explicit wave function is derived by numerically solving the Bethe ansatz equations for the full physical regimes $(\ensuremath{-}\ensuremath{\infty}\ensuremath{\le}{c}_{F}\ensuremath{\le}0)$. With the exact wave function some quantities which are important in many-body physics are obtained, including the one-body density matrix and the momentum distribution of the ground state for finite system. It is shown that the shell structure of the density profiles disappears with the increase of the interaction and in the fermionic Tonks-Girardeau limit the density distribution shows the same behavior as that of an ideal Bose gas. However, the one-body density matrix and the momentum distribution exhibit completely different structures compared with their bosonic counterparts.We investigate the ground state of the one-dimensional fermionic system enclosed in a hard-wall trap with attractive contact $p$-wave interactions. Based on the Bethe ansatz method, the explicit wave function is derived by numerically solving the Bethe ansatz equations for the full physical regimes $(\ensuremath{-}\ensuremath{\infty}\ensuremath{\le}{c}_{F}\ensuremath{\le}0)$. With the exact wave function some quantities which are important in many-body physics are obtained, including the one-body density matrix and the momentum distribution of the ground state for finite system. It is shown that the shell structure of the density profiles disappears with the increase of the interaction and in the fermionic Tonks-Girardeau limit the density distribution shows the same behavior as that of an ideal Bose gas. However, the one-body density matrix and the momentum distribution exhibit completely different structures compared with their bosonic counterparts.

arXiv:0708.3548Physical Review ADec 3, 200727 citations

Quantum information theoretic measures to distinguish fermionized bosons from non-interacting fermions

Barnali Chakrabarti, A. Gammal, N. D. Chavda +1 more

We study the dynamical fermionization of strongly interacting one-dimensional bosons in Tonks-Girardeau limit by solving the time dependent many-boson Schrödinger equation numerically exactly. We establish that the one-body momentum distribution approaches the ideal Fermi gas distribution at the time of dynamical fermionization. The analysis is further complemented by the measures on two-body level. Investigation on two-body momentum distribution, two-body local and non-local correlation clearly distinguish the fermionized bosons from non-interacting fermions. The magnitude of distinguishablity between the two systems is further discussed employing suitable measures of information theory, i.e., the well known Kullback-Leibler relative entropy and the Jensen-Shannon divergence entropy. We also observe very rich structure in the higher-body density for strongly correlated bosons whereas non-interacting fermions do not possess any higher order correlation beyond two-body.We study the dynamical fermionization of strongly interacting one-dimensional bosons in Tonks-Girardeau limit by solving the time dependent many-boson Schrödinger equation numerically exactly. We establish that the one-body momentum distribution approaches the ideal Fermi gas distribution at the time of dynamical fermionization. The analysis is further complemented by the measures on two-body level. Investigation on two-body momentum distribution, two-body local and non-local correlation clearly distinguish the fermionized bosons from non-interacting fermions. The magnitude of distinguishablity between the two systems is further discussed employing suitable measures of information theory, i.e., the well known Kullback-Leibler relative entropy and the Jensen-Shannon divergence entropy. We also observe very rich structure in the higher-body density for strongly correlated bosons whereas non-interacting fermions do not possess any higher order correlation beyond two-body.

arXiv:2402.00372Feb 1, 20240 citations

Momentum distribution of harmonically confined Fermions

Norman Henry March, Luis Miguel Nieto, M. P. Tosi

Physica B Condensed MatterJan 1, 20015 citations

THE MOMENTUM DISTRIBUTION OF INTERACTING FERMI PARTICLES

A.B. Migdal

Sep 1, 19573 citations

We investigate the ground state of the one-dimensional fermionic system enclosed in a hard-wall trap with attractive contact

p

-wave interactions. Based on the Bethe ansatz method, the explicit wave function is derived by numerically solving the Bethe ansatz equations for the full physical regimes $(\ensuremath{-}\ensuremath{\infty}\ensuremath{\le}{c}_{F}\ensuremath{\le}0)$. With the exact wave function some quantities which are important in many-body physics are obtained, including the one-body density matrix and the momentum distribution of the ground state for finite system. It is shown that the shell structure of the density profiles disappears with the increase of the interaction and in the fermionic Tonks-Girardeau limit the density distribution shows the same behavior as that of an ideal Bose gas. However, the one-body density matrix and the momentum distribution exhibit completely different structures compared with their bosonic counterparts.