2006
DOI: 10.1088/1742-6596/51/1/046
|View full text |Cite
|
Sign up to set email alerts
|

Cu-NMR study on the disordered quantum spin magnet with the Bose-glass ground state

Abstract: Cu-NMR study has been performed on the disordered spin-gap system Tl1−xKxCuCl3 In the high-field H > HC=∆/µB, where ∆ is the spin-gap, the hyperfine field becomes extremely inhomogeneous at low temperatures due to the field-induced magnetic order, indicating that the ordered spin state must be different from the pure TlCuCl3. In the low field H < HC, a saturating behavior in the longitudinal nuclear spin relaxation rate T −1 1 was observed at low temperatures, indicating existence of the magnetic ground state … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

3
7
0

Year Published

2006
2006
2009
2009

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 9 publications
(10 citation statements)
references
References 19 publications
3
7
0
Order By: Relevance
“…As for x = 0.20, the increase and the saturation of the muon-spin-relaxation rate were observed at low temperatures, which is possibly a precursor to the Bose-glass phase at T =0. 23,24 These results are consistent with the theoretical and experimental predictions that the Bose-glass phase is expected to appear for x Ͼ 0. [25][26][27][28][29][30] In the case of x = 0.44 and 0.58, the increase of is observed, which suggests the slowing down of the frequency of the Cu 3d spin fluctuations toward a spin frozen state below 20 mK in contrast to the predicted Bose-glass phase, and the rootexponential-like behavior of the time spectrum indicates that the origin of the relaxation is possibly the spatially fixed fluctuating dilute moments.…”
Section: Introductionsupporting
confidence: 88%
“…As for x = 0.20, the increase and the saturation of the muon-spin-relaxation rate were observed at low temperatures, which is possibly a precursor to the Bose-glass phase at T =0. 23,24 These results are consistent with the theoretical and experimental predictions that the Bose-glass phase is expected to appear for x Ͼ 0. [25][26][27][28][29][30] In the case of x = 0.44 and 0.58, the increase of is observed, which suggests the slowing down of the frequency of the Cu 3d spin fluctuations toward a spin frozen state below 20 mK in contrast to the predicted Bose-glass phase, and the rootexponential-like behavior of the time spectrum indicates that the origin of the relaxation is possibly the spatially fixed fluctuating dilute moments.…”
Section: Introductionsupporting
confidence: 88%
“…36,37) These results are consistent with the theoretical prediction that the Bose-glass phase is expected to appear for x > 0. However, it is not yet known whether or not another ground state apart from the Bose-glass phase and the gapped state appears when the randomness is enhanced with increasing the concentration of x in the system.…”
Section: )supporting
confidence: 89%
“…The evidence of the localization has actually been reported in the other disordered quantum spin system ͑Tl, K͒ CuCl 3 , which is believed to have the ground state of the Bose glass, [8][9][10] as a discrepancy between the temperature dependence of the uniform and the local magnetization-the latter of which is probed by NMR shift. 11 In the present case, our tentative NMR study shows a different temperature dependence between NMR shift and the uniform susceptibility. This also supports the Bose-glass picture.…”
Section: Discussionmentioning
confidence: 41%
“…6,7 A disordered spin system is one of the candidates that bear the ground state of the Bose glass. Although possibility of the experimental detection of the Bose-glass phase by either macroscopic [8][9][10] or microscopic 11,12 probes was repeatedly suggested in the solid solution of two different spin-gap systems, details still remain obscure.…”
Section: Introductionmentioning
confidence: 99%