The effect of randomness on the quantum spin system TlKCuCl with ${\boldmath $x$}$ = 0.44 studied by the Zero-field Muon-Spin-Relaxation (ZF-SR) method
arXiv:0705.1383 · doi:10.1143/JPSJ.76.074704
Abstract
Zero-field muon-spin-relaxation (ZF-{\boldmath }SR) measurements were carried out down to 80 mK on the randomness bond system TlKCuCl with = 0.44. Time spectra are well fitted by the stretched exponential function . The muon spin relaxation rate increases rapidly with decreasing temperature, and tends to 0.5 at 80 mK. The divergent increase of suggests the critical slowing down of the frequency of the Cu-3{\it d} spin fluctuations toward a spin frozen state below 80 mK, and the root-exponential-like behavior of the time spectrum indicates that the origin of the relaxation is possibly the spatially-fixed fluctuating dilute moments.
arXiv commentAccepted on J. Phys. Soc. Jpn
References in corpus (13)
- Realization of Bose-Einstein condensation of dilute magnons in TlCuCl
- Quantum Criticality: competing ground states in low dimensions
- Field- and pressure-induced magnetic quantum phase transitions in TlCuCl_3
- Magnon Dispersion in the Field-Induced Magnetically Ordered Phase of TlCuCl3
- Observation of Field-Induced Transverse Néel Ordering in the Spin Gap System TlCuCl
- Disordered Bose-Einstein Condensates in Quasi One-Dimensional Magnetic Microtraps
- Field-Induced Magnetic Ordering in the Quantum Spin System KCuCl
- Phase Transition, Longitudinal Spin Fluctuations and Scaling in a Two-Layer Antiferromagnet
- Bose-Einstein Condensation of Magnons in TlCuCl3: Phase diagram and specific heat from a self-consistent Hartee-Fock calculation with a realistic dispersion relation
- Random Bond Effect in the Quantum Spin System (TlK)CuCl
- Bose-Glass Phases in Disordered Quantum Magnets
- Pressure-Induced Magnetic Quantum Phase Transition in Gapped Spin System KCuCl3
- Muon spin relaxation and rotation study on the solid solution of the two spin-gap systems (CH3)2CHNH3-CuCl3 and (CH3)2CHNH3-CuBr3