2005/06/03 by Joseph J. Betouras, Joseph Betouras, D. V. Efremov +3
Physics and Astronomy · #Physics of Superconductivity and Magnetism #Quantum and electron transport phenomena #Rare-earth and actinide compounds #cond-mat.mes-hall #cond-mat.str-el
paper · pdf · doi:10.1103/physrevb.72.115112
published as Phys. Rev. B 72, 115112 (2005) · 4 pages,3 figures
arxiv created 2005/06/03 · openalex publication_date 2005/09/14 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/30
We extend previous calculations of the nonanalytic terms in the spin susceptibility \ensuremathχs(T) and the specific heat C(T) to systems in a magnetic field. Without a field, \ensuremathχs(T) and C(T)∕T are linear in T in two dimensions (2D), while in 3D, \ensuremathχs(T)\ensuremath∝T2 and C(T)∕T\ensuremath∝T2\phantom\rule0.2em0exln\phantom\rule0.2em0exT. We show that in a magnetic field, the linear in T terms in 2D become scaling functions of \ensuremathμBH∕T. We present explicit expressions for these functions and show that at high fields \ensuremathμBH⪢T, \ensuremathχs(T,H) scales as \ensuremath|H\ensuremath|. We also show that in 3D, \ensuremathχs(T,H) becomes nonanalytic in a field and at high fields scales as H2\phantom\rule0.2em0exln\ensuremath|H\ensuremath|.