Single-water-dipole-layer-driven Reversible Charge Order Transition in 1T-TaS2

Nano Letters ◽  
2020 ◽  
Vol 20 (12) ◽  
pp. 8854-8860
Author(s):  
Shiwei Shen ◽  
Bin Shao ◽  
Chenhaoping Wen ◽  
Xiaoqiu Yuan ◽  
Jingjing Gao ◽  
...  
2002 ◽  
Vol 65 (17) ◽  
Author(s):  
R. Klingeler ◽  
J. Geck ◽  
R. Gross ◽  
L. Pinsard-Gaudart ◽  
A. Revcolevschi ◽  
...  

1999 ◽  
Vol 60 (12) ◽  
pp. R8417-R8421 ◽  
Author(s):  
Matthias Vojta ◽  
R. E. Hetzel ◽  
R. M. Noack

2003 ◽  
Vol 17 (04n06) ◽  
pp. 799-804 ◽  
Author(s):  
A. PAOLONE ◽  
R. CANTELLI ◽  
G. ROUSSE ◽  
C. MASQUELIER ◽  
M. FERRETTI

We studied the charge order transition of LiMn 2 O 4 by means of anelastic spectroscopy, measuring the Young's modulus, E, and the elastic energy loss function, Q-1. Our measurements confirm the occurrence of a phase transition at 296 K on cooling, showing a large hysteresis on heating. Around the transition temperature the Young's modulus shape reveals that there is at least one elastic constant, possibly c44, decreasing lowering the temperature. Moreover the anelastic spectroscopy results confirm that the transformation is characterised by the coexistence of two phases in a narrow temperature range. The time constant of the transformation of the cubic into the orthorhombic phase sharply decreases lowering T from 296 to 290 K and then increases on further cooling to 289 K. The strong decrease of the time constant around 290 K can be related to the reduction of the c44 elastic constant.


2012 ◽  
Vol 9 (5) ◽  
pp. 1161-1163 ◽  
Author(s):  
Mitsuharu Nagasawa ◽  
Tokiko Nagasawa ◽  
Koichi Ichimura ◽  
Kazushige Nomura

2010 ◽  
Vol 405 (11) ◽  
pp. S113-S115 ◽  
Author(s):  
M. Nagasawa ◽  
T. Nagasawa ◽  
K. Ichimura ◽  
K. Nomura

Author(s):  
Daigo Ohki ◽  
Genki Matsuno ◽  
Yukiko Omori ◽  
Akito Kobayashi

The optical conductivity in the charge order phase is calculated in the extended Hubbard model describing an organic Dirac electron system α-(BEDT-TTF)2I3 using the mean field theory and the Nakano-Kubo formula. A peak structure due to interband excitation being characteristic in two-dimensional Dirac electron system is found above the charge order gap. It is shown that the peak structure originates from the Van Hove singularities of the conduction and valence bands, where those singularities are located at a saddle point between two Dirac cones in momentum space. The frequency of the peak structure exhibits drastic change in the vicinity of the charge order transition.


2008 ◽  
Vol 81 (7-8) ◽  
pp. 717-727 ◽  
Author(s):  
Hans M. Christen ◽  
Maria Varela ◽  
Dae Ho Kim

2001 ◽  
Vol 89 (11) ◽  
pp. 6627-6629 ◽  
Author(s):  
C. Stephen Hellberg

2020 ◽  
Vol 26 (S2) ◽  
pp. 2034-2035
Author(s):  
Noah Schnitzer ◽  
Elisabeth Bianco ◽  
Alemayehu Admasu ◽  
Jaewook Kim ◽  
Sang-Wook Cheong ◽  
...  

1999 ◽  
Vol 82 (20) ◽  
pp. 4046-4049 ◽  
Author(s):  
R. Pietig ◽  
R. Bulla ◽  
S. Blawid

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