Magnon Heat Conductivity and Mean Free Paths in Two-Leg Spin Ladders: A Model-Independent Determination
| dc.creator | Hess, C. | |
| dc.creator | Ribeiro, P. | |
| dc.creator | Büchner, B. | |
| dc.creator | ElHaes, H. | |
| dc.creator | Roth, G. | |
| dc.creator | Ammerahl, U. | |
| dc.creator | Revcolevschi, A. | |
| dc.date | 2005-06-23 | |
| dc.date | 2006-03-17 | |
| dc.date.accessioned | 2026-07-07T06:38:01Z | |
| dc.date.available | 2026-07-07T06:38:01Z | |
| dc.description | The magnon thermal conductivity $κ_{\mathrm{mag}}$ of the spin ladders in $\rm Sr_{14}Cu_{24-x}Zn_xO_{41}$ has been investigated at low doping levels $x=0$, 0.125, 0.25, 0.5 and 0.75. The Zn-impurities generate nonmagnetic defects which define an upper limit for $l_{\mathrm{mag}}$ and therefore allow a clear-cut relation between $l_{\mathrm{mag}}$ and $κ_{\mathrm{mag}}$ to be established independently of any model. Over a large temperature range we observe a progressive suppression of $κ_{\mathrm{mag}}$ with increasing Zn-content and find in particular that with respect to pure $\rm Sr_{14}Cu_{24}O_{41}$ $κ_{\mathrm{mag}}$ is strongly suppressed even in the case of tiny impurity densities where $l_{\mathrm{mag}}\lesssim 374$~Å. This shows unambiguously that large $l_{\mathrm{mag}}\approx 3000$~Å which have been reported for $\rm Sr_{14}Cu_{24}O_{41}$ and $\rm La_{5}Ca_9Cu_{24}O_{41}$ on basis of a kinetic model are in the correct order of magnitude. | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0506595 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0506595 | |
| dc.identifier | Phys. Rev. B 73, 104407 (2006) | |
| dc.identifier | doi:10.1103/PhysRevB.73.104407 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/100594 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.subject | Other Condensed Matter | |
| dc.title | Magnon Heat Conductivity and Mean Free Paths in Two-Leg Spin Ladders: A Model-Independent Determination | |
| dc.type | text |