Relationship between the thermopower and entropy of strongly correlated electron systems
| dc.creator | Zlatic, V. | |
| dc.creator | Monnier, R. | |
| dc.creator | Freericks, J. | |
| dc.creator | Becker, K. W. | |
| dc.date | 2005-12-13 | |
| dc.date | 2007-01-18 | |
| dc.date.accessioned | 2026-07-07T07:41:22Z | |
| dc.date.available | 2026-07-07T07:41:22Z | |
| dc.description | A number of recent experiments report the low-temperature thermopower $α$ and specific heat coefficients $γ=C_V/T$ of strongly correlated electron systems. Describing the charge and heat transport in a thermoelectric by transport equations, and assuming that the charge current and the heat current densities are proportional to the number density of the charge carriers, we obtain a simple mean-field relationship between $α$ and the entropy density $\cal S$ of the charge carriers. We discuss corrections to this mean-field formula and use results obtained for the periodic Anderson and the Falicov-Kimball models to explain the concentration (chemical pressure) and temperature dependence of $α/γT$ in EuCu$_2$(Ge$_{1-x}$Si$_x$)$_2$, CePt$_{1-x}$Ni$_x$, and YbIn$_{1-x}$Ag${_x}$Cu$_4$ intermetallic compounds. % We also show, using the 'poor man's mapping' which approximates the periodic Anderson lattice by the single impurity Anderson model, that the seemingly complicated behavior of $α(T)$ can be explained in simple terms and that the temperature dependence of $α(T)$ at each doping level is consistent with the magnetic character of 4{\it f} ions. | |
| dc.description | 11 pages | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0512288 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0512288 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/122084 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | Relationship between the thermopower and entropy of strongly correlated electron systems | |
| dc.type | text |