### Abstract

The density functional theory of atomic electrons in strong magnetic fields is generalized to finite-temperature systems. General integral formulations are developed in the format of Mermin-Kohn-Sham finite-temperature density functional theory. The lowest order of the general theory leads to a temperature-dependent extended Thomas-Fermi (TETF)-like functional, which is simple enough to be analyzed. The general theory provides a new way of calculating the equilibrium properties of many-electron systems in strong magnetic fields.

Original language | English (US) |
---|---|

Pages (from-to) | 323-332 |

Number of pages | 10 |

Journal | Journal of Statistical Physics |

Volume | 59 |

Issue number | 1-2 |

DOIs | |

State | Published - Apr 1990 |

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### Keywords

- Density functional
- finite temperature
- magnetic fields

### ASJC Scopus subject areas

- Statistical and Nonlinear Physics
- Physics and Astronomy(all)
- Mathematical Physics

### Cite this

*Journal of Statistical Physics*,

*59*(1-2), 323-332. https://doi.org/10.1007/BF01015572

**Finite-temperature density functional theory of atoms in strong magnetic fields.** / Li, Shiwei; Percus, Jerome.

Research output: Contribution to journal › Article

*Journal of Statistical Physics*, vol. 59, no. 1-2, pp. 323-332. https://doi.org/10.1007/BF01015572

}

TY - JOUR

T1 - Finite-temperature density functional theory of atoms in strong magnetic fields

AU - Li, Shiwei

AU - Percus, Jerome

PY - 1990/4

Y1 - 1990/4

N2 - The density functional theory of atomic electrons in strong magnetic fields is generalized to finite-temperature systems. General integral formulations are developed in the format of Mermin-Kohn-Sham finite-temperature density functional theory. The lowest order of the general theory leads to a temperature-dependent extended Thomas-Fermi (TETF)-like functional, which is simple enough to be analyzed. The general theory provides a new way of calculating the equilibrium properties of many-electron systems in strong magnetic fields.

AB - The density functional theory of atomic electrons in strong magnetic fields is generalized to finite-temperature systems. General integral formulations are developed in the format of Mermin-Kohn-Sham finite-temperature density functional theory. The lowest order of the general theory leads to a temperature-dependent extended Thomas-Fermi (TETF)-like functional, which is simple enough to be analyzed. The general theory provides a new way of calculating the equilibrium properties of many-electron systems in strong magnetic fields.

KW - Density functional

KW - finite temperature

KW - magnetic fields

UR - http://www.scopus.com/inward/record.url?scp=34249956438&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=34249956438&partnerID=8YFLogxK

U2 - 10.1007/BF01015572

DO - 10.1007/BF01015572

M3 - Article

AN - SCOPUS:34249956438

VL - 59

SP - 323

EP - 332

JO - Journal of Statistical Physics

JF - Journal of Statistical Physics

SN - 0022-4715

IS - 1-2

ER -