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Relativistic non-interacting electron gas in a magnetic field

Abstract

The ground state properties of a noninteracting relativistic electron gas are investigated as a function of the strength of a uniform applied magnetic field for two and three dimensions. The calculation of the de Haas-van Alphen terms in the density is also presented. 3 refs.
Publication Date:
Dec 31, 1994
Product Type:
Technical Report
Report Number:
UM-P-94/89
Reference Number:
SCA: 665400; PA: AIX-26:019187; EDB-95:033009; SN: 95001330668
Resource Relation:
Other Information: PBD: [1994]
Subject:
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; ELECTRON GAS; GROUND STATES; DE HAAS-VAN ALPHEN EFFECT; INTEGRAL EQUATIONS; LAPLACE TRANSFORMATION; MAGNETIC FIELDS; REST MASS; THREE-DIMENSIONAL CALCULATIONS; TWO-DIMENSIONAL CALCULATIONS; 665400; QUANTUM PHYSICS ASPECTS OF CONDENSED MATTER
OSTI ID:
10113858
Research Organizations:
Melbourne Univ., Parkville, VIC (Australia). School of Physics
Country of Origin:
Australia
Language:
English
Other Identifying Numbers:
Other: ON: DE95616903; TRN: AU9414240019187
Availability:
OSTI; NTIS (US Sales Only); INIS
Submitting Site:
INIS
Size:
9 p.
Announcement Date:
Jun 30, 2005

Citation Formats

Glasser, M L, and Frankel, N E. Relativistic non-interacting electron gas in a magnetic field. Australia: N. p., 1994. Web.
Glasser, M L, & Frankel, N E. Relativistic non-interacting electron gas in a magnetic field. Australia.
Glasser, M L, and Frankel, N E. 1994. "Relativistic non-interacting electron gas in a magnetic field." Australia.
@misc{etde_10113858,
title = {Relativistic non-interacting electron gas in a magnetic field}
author = {Glasser, M L, and Frankel, N E}
abstractNote = {The ground state properties of a noninteracting relativistic electron gas are investigated as a function of the strength of a uniform applied magnetic field for two and three dimensions. The calculation of the de Haas-van Alphen terms in the density is also presented. 3 refs.}
place = {Australia}
year = {1994}
month = {Dec}
}