scholarly journals Emergence of a real-space symmetry axis in the magnetoresistance of the one-dimensional conductor Li0.9Mo6O17

2019 ◽  
Vol 5 (7) ◽  
pp. eaar8027 ◽  
Author(s):  
Jianming Lu ◽  
Xiaofeng Xu ◽  
M. Greenblatt ◽  
R. Jin ◽  
P. Tinnemans ◽  
...  

We report on an emerging symmetry axis in the magnetoresistance of bulk single crystals of quasi–one-dimensional Li0.9Mo6O17 below Tmin = 25 K, the temperature at which the electrical resistivity experiences a minimum. Detailed angle-dependent magnetoresistance sweeps reveal that this symmetry axis is induced by the development of a negative magnetoresistance, which is suppressed only for magnetic fields oriented along the poles of the MoO6 octahedra that form the conducting chains. We show that this unusual negative magnetoresistance is consistent with the melting of dark excitons, composed of previously omitted orbitals within the t2g manifold that order below Tmin. The unveiled symmetry axis in directional magnetic fields not only provides evidence for the crystallization of these dark excitons but also sheds new light on the long-standing mystery of the metal-insulator transition in Li0.9Mo6O17.

1999 ◽  
Vol 60 (11) ◽  
pp. 7950-7955 ◽  
Author(s):  
Eric Jeckelmann ◽  
Chunli Zhang ◽  
Steven R. White

1998 ◽  
Vol 299 (1-2) ◽  
pp. 36-40 ◽  
Author(s):  
T Kawamoto ◽  
T Mori ◽  
Y Misaki ◽  
K Tanaka ◽  
H Mori ◽  
...  

1996 ◽  
Vol 10 (18) ◽  
pp. 863-871
Author(s):  
ARIANNA MONTORSI ◽  
MARIO RASETTI

We study the metal-insulator transition of the d-dimensional Hubbard model by treating the hopping term between adjacent 1-d chains in the frame of a Clifford linearization scheme, and keeping the full model along the chains. A general equation for the critical point is worked out in terms of the correlation functions of the one-dimensional model, assuming that the transition is of the second order. The equation, which holds at any temperature, is here investigated especially at T=0, where the latter condition holds true. The solution shows the existence of an insulating ground state in any d only at half-filling for U strictly positive, as in the exact 1-d case. The transition is found to be related to a parameter reminiscent of entropy.


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