{ "id": "1404.0825", "version": "v1", "published": "2014-04-03T10:10:41.000Z", "updated": "2014-04-03T10:10:41.000Z", "title": "Density Functionals in the Presence of Magnetic Field", "authors": [ "Andre Laestadius" ], "comment": "26 pages", "categories": [ "math-ph", "math.MP", "physics.chem-ph", "quant-ph" ], "abstract": "In this paper density functionals for Coulomb systems subjected to electric and magnetic fields are developed. The density functionals depend on the particle density, $\\rho$, and paramagnetic current density, $j^p$. This approach is motivated by an adapted version of the Vignale and Rasolt formulation of Current Density Functional Theory (CDFT), which establishes a one-to-one correspondence between the non-degenerate ground-state and the particle and paramagnetic current density. Definition of $N$-representable density pairs $(\\rho,j^p)$ is given and it is proven that the set of $v$-representable densities constitutes a proper subset of the set of $N$-representable densities. For a Levy-Lieb type functional $Q(\\rho,j^p)$, it is demonstrated that (i) it is a proper extension of the universal Hohenberg-Kohn functional, $F_{HK}(\\rho,j^p)$, to $N$-representable densities, (ii) there exists a wavefunction $\\psi_0$ such that $Q(\\rho,j^p)=(\\psi_0,H_0\\psi_0)_{L^2}$, where $H_0$ is the Hamiltonian without external potential terms, and (iii) it is not convex. Furthermore, a convex and universal functional $F(\\rho,j^p)$ is studied and proven to be equal the convex envelope of $Q(\\rho,j^p)$. For both $Q$ and $F$, we give upper and lower bounds.", "revisions": [ { "version": "v1", "updated": "2014-04-03T10:10:41.000Z" } ], "analyses": { "keywords": [ "magnetic field", "representable density", "paramagnetic current density", "current density functional theory", "density functionals depend" ], "note": { "typesetting": "TeX", "pages": 26, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2014arXiv1404.0825L" } } }