Avoided Quantum Criticality in YBa_2Cu_3O_y and La_{2-x}Sr_xCuO_4
| dc.creator | Sonier, J. E. | |
| dc.creator | Callaghan, F. D. | |
| dc.creator | Ando, Y. | |
| dc.creator | Kiefl, R. F. | |
| dc.creator | Brewer, J. H. | |
| dc.creator | Kaiser, C. V. | |
| dc.creator | Pacradouni, V. | |
| dc.creator | Sabok-Sayr, S. -A. | |
| dc.creator | Sun, X. F. | |
| dc.creator | Komiya, S. | |
| dc.creator | Hardy, W. N. | |
| dc.creator | Bonn, D. A. | |
| dc.creator | Liang, R. | |
| dc.date | 2006-10-02 | |
| dc.date.accessioned | 2026-07-07T07:27:18Z | |
| dc.date.available | 2026-07-07T07:27:18Z | |
| dc.description | Spin-glass magnetism confined to individual weakly interacting vortices is detected in two different families of high-transition-temperature (T_c) superconductors, but only in samples on the low-doping side of the low-temperature normal state metal-to-insulator crossover (MIC). Our findings unravel the mystery of the MIC, but more importantly identify the true location of the field-induced quantum phase transition (QPT) in the superconducting state. The non-uniform appearance of magnetism in the vortex state favours a surprisingly exotic phase diagram, in which spatially inhomogeneous competing order is stabilized at the QPT, and an `avoided' quantum critical point (QCP) is realized at zero magnetic field. | |
| dc.description | 4 pages, 3 figures, submitted to PRL | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0610051 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0610051 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/117333 | |
| dc.subject | Superconductivity | |
| dc.title | Avoided Quantum Criticality in YBa_2Cu_3O_y and La_{2-x}Sr_xCuO_4 | |
| dc.type | text |