The structure of the density-potential mapping. Part II: Including
magnetic fields
- URL: http://arxiv.org/abs/2303.01357v2
- Date: Sun, 30 Jul 2023 15:17:57 GMT
- Title: The structure of the density-potential mapping. Part II: Including
magnetic fields
- Authors: Markus Penz, Erik I. Tellgren, Mih\'aly A. Csirik, Michael
Ruggenthaler, Andre Laestadius
- Abstract summary: The Hohenberg-Kohn theorem of density-functional theory (DFT) is broadly considered the conceptual basis for a full characterization of an electronic system in its ground state by just the one-body particle density.
We aim at clarifying the status of this theorem within different extensions of DFT including magnetic fields.
- Score: 0.0
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: The Hohenberg-Kohn theorem of density-functional theory (DFT) is broadly
considered the conceptual basis for a full characterization of an electronic
system in its ground state by just the one-body particle density. In this
Part~II of a series of two articles, we aim at clarifying the status of this
theorem within different extensions of DFT including magnetic fields. We will
in particular discuss current-density-functional theory (CDFT) and review the
different formulations known in the literature, including the conventional
paramagnetic CDFT and some non-standard alternatives. For the former, it is
known that the Hohenberg-Kohn theorem is no longer valid due to
counterexamples. Nonetheless, paramagnetic CDFT has the mathematical framework
closest to standard DFT and, just like in standard DFT, non-differentiability
of the density functional can be mitigated through Moreau-Yosida
regularization. Interesting insights can be drawn from both
Maxwell-Schr\"odinger DFT and quantum-electrodynamical DFT, which are also
discussed here.
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