$^1$H-NMR Spin-Lattice Relaxation Rate of IPACu(Cl$_{x}$Br$_{1-x}$)$_3$ with $x=0$ and 0.35
| dc.creator | Oosawa, A. | |
| dc.creator | Suzuki, T. | |
| dc.creator | Kanada, K. | |
| dc.creator | Goto, T. | |
| dc.creator | Manaka, H. | |
| dc.date | 2009-03-13 | |
| dc.date | 2009-03-20 | |
| dc.date.accessioned | 2026-07-07T12:54:13Z | |
| dc.date.available | 2026-07-07T12:54:13Z | |
| dc.description | The spin-lattice relaxation rate $T_1^{-1}$ of $^1$H-NMR has been measured in (CH$_3$)$_2$CHNH$_3$Cu(Cl$_x$Br$_{1-x}$)$_3$ with $x=0$ and 0.35, in order to investigate the microscopic magnetism of systems. Previous macroscopic magnetization and specific heat measurements suggested that these two exist in a singlet-dimer phase. The temperature dependence of $T_1^{-1}$ in an $x=0$ system decreased exponentially toward zero, indicating microscopic evidence of the gapped singlet ground state, which is consistent with the macroscopic experiments. At the same time, in the $x=0.35$ system, $T_1^{-1}$ showed a sharp peak structure at around 7.5 K though no splitting of $^1$H-NMR spectra indicative of the magnetic ordering was observed. We discuss the observed sharp peak structure in the $x=0.35$ system with the soft mode toward the exotic magnetic ground state suggested by the recent $μ$SR experiments. | |
| dc.description | submitted to JPSJ (accepted and will appear in the issue of No. 5) | |
| dc.identifier | https://arxiv.org/abs/0903.2318 | |
| dc.identifier | http://arxiv.org/abs/0903.2318 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/223852 | |
| dc.subject | Statistical Mechanics | |
| dc.title | $^1$H-NMR Spin-Lattice Relaxation Rate of IPACu(Cl$_{x}$Br$_{1-x}$)$_3$ with $x=0$ and 0.35 | |
| dc.type | text |