Computational schemes for the ground-state pair density

Superconducting gap and attractive interaction between electrons investigated by the current-density functional theory for superconductors

The quantitative description of the Meissner effect can be done by means of the current-density functional theory for superconductors (sc-CDFT), as pointed out by W Kohn. Here, we propose a calculation scheme of the sc-CDFT. In this scheme, the superconducting gap and attractive interaction between electrons are treated as variables, while experimental data are used for the penetration depth. The variables are determined by solving the gap equation of the sc-CDFT simultaneously with the relation between energy gains of the superconducting state in the zero and nonzero magnetic field cases. This scheme is applied to homogeneous electron gas systems immersed in a magnetic field that correspond to simple models for aluminum, tin and indium immersed in a magnetic field. The magnetic field and temperature dependences of the superconducting gap are well reproduced for each case. It is also found that the attractive interaction changes with the magnetic field and temperature, which is consistent with the change in the superconducting gap.

N-representability of the Jastrow wave function pair density of the lowest-order

Conditions for the N-representability of the pair density (PD) are needed for the development of the PD functional theory. We derive sufficient conditions for the N-representability of the PD that is calculated from the Jastrow wave function within the lowest order. These conditions are used as the constraints on the correlation function of the Jastrow wave function. A concrete procedure to search the suitable correlation function is also presented.