PELTIER EFFECT IN NS MICROCONTACTS
| dc.creator | BARDAS, A. | |
| dc.creator | AVERIN, D. | |
| dc.date | 1995-05-22 | |
| dc.date.accessioned | 2026-07-07T03:07:43Z | |
| dc.date.available | 2026-07-07T03:07:43Z | |
| dc.description | We have calculated the heat current in the normal metal/insulator/ superconductor contacts with arbitrary transparency of the insulator barrier. In the tunneling limit (small transparencies), the heat flow out of the normal metal reaches its maximum at temperature $T\simeq 0.3Δ$. At higher values of transparency, the interplay between single-particle tunneling and Andreev reflection determines optimum transparency which maximizes the density of heat flow out of the normal metal. In clean contacts, the optimum transparency is about $0.1$ at $T=0.3Δ$ and decreases with temperature roughly as $(T/Δ)^{3/2}$. In disordered contacts, disorder enhances Andreev reflection and shifts the optimum point towards smaller transparencies. The optimal ratio of the barrier resistance to the resistance of the normal electrode is $R_N/R_T \simeq 0.01$ at $T=0.3 Δ$ and decreases with temperature similarly to clean contacts. For disordered contacts we also plot current-voltage characteristics for arbitrary values of the ratio $R_N/R_T$. | |
| dc.description | 14 Pages, REVTEX 3.0, 6 figures available upon request | |
| dc.identifier | https://arxiv.org/abs/cond-mat/9505097 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/9505097 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/27272 | |
| dc.subject | Condensed Matter | |
| dc.title | PELTIER EFFECT IN NS MICROCONTACTS | |
| dc.type | text |