Critical properties of the S=1 spin dimer compound Ba3Mn2O8
| dc.creator | Suh, S. | |
| dc.creator | Al-Hassanieh, K. A. | |
| dc.creator | Samulon, E. C. | |
| dc.creator | Brooks, J. S. | |
| dc.creator | Clark, W. G. | |
| dc.creator | Kuhns, P. L. | |
| dc.creator | Lumata, L. L. | |
| dc.creator | Reyes, A. | |
| dc.creator | Fisher, I. R. | |
| dc.creator | Brown, S. E. | |
| dc.creator | Batista, C. D. | |
| dc.date | 2009-05-05 | |
| dc.date.accessioned | 2026-07-07T13:12:08Z | |
| dc.date.available | 2026-07-07T13:12:08Z | |
| dc.description | Ba3Mn2O8 is a hexagonally coordinated Mn5+ S=1 spin dimer system with small uniaxial single-ion anisotropy. 135,137Ba NMR spectroscopy is used to establish the lower critical field Hc1 of distinct field-induced phases for H parallel to c,H perpendicular to c, and measure the longitudinal (Ml) and transverse (Mt) magnetizations in the vicinity of the quantum critical point (QCP). Ml_parallel (T, Hc1), Ml_perpendicular (T, Hc1) are reproduced by solving a low-energy model for a dilute gas of interacting bosons. Ml_parallel(T goes to 0, H = Hc1) (Ml_perpendicular(T goes to 0, H = Hc1)) follows the expectation for a BEC (Ising-like) QCP. | |
| dc.description | 5 pages, 6 figures | |
| dc.identifier | https://arxiv.org/abs/0905.0718 | |
| dc.identifier | http://arxiv.org/abs/0905.0718 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/229497 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | Critical properties of the S=1 spin dimer compound Ba3Mn2O8 | |
| dc.type | text |