Incommensurate Magnetic Ordering and Spin-Liquid-Like State in a Triangular Lattice BaVS 3: Neutron Diffraction and Scattering Study

2000 ◽  
Vol 69 (9) ◽  
pp. 2763-2766 ◽  
Author(s):  
Hiroyuki Nakamura ◽  
Tomoaki Yamasaki ◽  
Saurav Giri ◽  
Hideto Imai ◽  
Masayuki Shiga ◽  
...  
2014 ◽  
Vol 90 (14) ◽  
Author(s):  
A. Leithe-Jasper ◽  
W. Schnelle ◽  
H. Rosner ◽  
W. Schweika ◽  
O. Isnard

Physica B+C ◽  
1983 ◽  
Vol 120 (1-3) ◽  
pp. 275-279
Author(s):  
M. Sato ◽  
H. Fujishita ◽  
A.R. Moodenbaugh ◽  
S. Hoshino ◽  
B.H. Grier

2019 ◽  
Vol 116 (29) ◽  
pp. 14505-14510 ◽  
Author(s):  
Ruidan Zhong ◽  
Shu Guo ◽  
Guangyong Xu ◽  
Zhijun Xu ◽  
Robert J. Cava

Currently under active study in condensed matter physics, both theoretically and experimentally, are quantum spin liquid (QSL) states, in which no long-range magnetic ordering appears at low temperatures due to strong quantum fluctuations of the magnetic moments. The existing QSL candidates all have their intrinsic disadvantages, however, and solid evidence for quantum fluctuations is scarce. Here, we report a previously unreported compound, Na2BaCo(PO4)2, a geometrically frustrated system with effective spin-1/2 local moments for Co2+ ions on an isotropic 2-dimensional (2D) triangular lattice. Magnetic susceptibility and neutron scattering experiments show no magnetic ordering down to 0.05 K. Thermodynamic measurements show that there is a tremendous amount of magnetic entropy present below 1 K in 0-applied magnetic field. The presence of localized low-energy spin fluctuations is revealed by inelastic neutron measurements. At low applied fields, these spin excitations are confined to low energy and contribute to the anomalously large specific heat. In larger applied fields, the system reverts to normal behavior as evident by both neutron and thermodynamic results. Our experimental characterization thus reveals that this material is an excellent candidate for the experimental realization of a QSL state.


1964 ◽  
Vol 25 (5) ◽  
pp. 462-468 ◽  
Author(s):  
N. Kunitomi ◽  
Y. Hamaguchi ◽  
M. Sakamoto ◽  
K. Doi ◽  
S. Komura

1988 ◽  
Vol 49 (C8) ◽  
pp. C8-2171-C8-2172
Author(s):  
T. Chattopadhyay ◽  
H. Maletta ◽  
W. Wirges ◽  
K. Fischer ◽  
P. J. Brown

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
X. Rao ◽  
G. Hussain ◽  
Q. Huang ◽  
W. J. Chu ◽  
N. Li ◽  
...  

AbstractA recent focus of quantum spin liquid (QSL) studies is how disorder/randomness in a QSL candidate affects its true magnetic ground state. The ultimate question is whether the QSL survives disorder or the disorder leads to a “spin-liquid-like” state, such as the proposed random-singlet (RS) state. Since disorder is a standard feature of most QSL candidates, this question represents a major challenge for QSL candidates. YbMgGaO4, a triangular lattice antiferromagnet with effective spin-1/2 Yb3+ions, is an ideal system to address this question, since it shows no long-range magnetic ordering with Mg/Ga site disorder. Despite the intensive study, it remains unresolved as to whether YbMgGaO4 is a QSL or in the RS state. Here, through ultralow-temperature thermal conductivity and magnetic torque measurements, plus specific heat and DC magnetization data, we observed a residual κ0/T term and series of quantum spin state transitions in the zero temperature limit for YbMgGaO4. These observations strongly suggest that a QSL state with itinerant excitations and quantum spin fluctuations survives disorder in YbMgGaO4.


1988 ◽  
Vol 37 (1) ◽  
pp. 269-282 ◽  
Author(s):  
T. Chattopadhyay ◽  
P. J. Brown ◽  
P. Thalmeier ◽  
W. Bauhofer ◽  
H. G. von Schnering

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