Spin-Peierls transition temperature in the strongly correlated Hubbard model for uniform Heisenberg chains

1988 ◽  
Vol 38 (16) ◽  
pp. 11602-11606 ◽  
Author(s):  
Minette M. Mohan ◽  
Y. Lépine
1987 ◽  
Vol 19 (1-3) ◽  
pp. 855-858
Author(s):  
Chen Xin-Fen ◽  
Duan Hong-Min ◽  
Lin Shu-Yuan ◽  
Wu Pei-Jun ◽  
Zhang Dian-Lin

1988 ◽  
Vol 38 (4) ◽  
pp. 2608-2621 ◽  
Author(s):  
G. Geipel ◽  
W. Nolting

1978 ◽  
Vol 25 (9) ◽  
pp. 699-704 ◽  
Author(s):  
J.R. Cooper ◽  
J. Lukatela ◽  
M. Miljak ◽  
J.M. Fabre ◽  
L. Giral ◽  
...  

Science ◽  
2019 ◽  
Vol 366 (6468) ◽  
pp. 987-990 ◽  
Author(s):  
Edwin W. Huang ◽  
Ryan Sheppard ◽  
Brian Moritz ◽  
Thomas P. Devereaux

Strange or bad metallic transport, defined by incompatibility with the conventional quasiparticle picture, is a theme common to many strongly correlated materials, including high-temperature superconductors. The Hubbard model represents a minimal starting point for modeling strongly correlated systems. Here we demonstrate strange metallic transport in the doped two-dimensional Hubbard model using determinantal quantum Monte Carlo calculations. Over a wide range of doping, we observe resistivities exceeding the Mott-Ioffe-Regel limit with linear temperature dependence. The temperatures of our calculations extend to as low as 1/40 of the noninteracting bandwidth, placing our findings in the degenerate regime relevant to experimental observations of strange metallicity. Our results provide a foundation for connecting theories of strange metals to models of strongly correlated materials.


2020 ◽  
Vol 5 (1) ◽  
Author(s):  
Wen O. Wang ◽  
Jixun K. Ding ◽  
Brian Moritz ◽  
Edwin W. Huang ◽  
Thomas P. Devereaux

2012 ◽  
Vol 26 (20) ◽  
pp. 1250130 ◽  
Author(s):  
L. MAROTTA ◽  
F. SIRINGO

The Gaussian Effective Potential (GEP) is shown to be a useful variational tool for the study of the magnetic properties of strongly correlated electronic systems. The GEP is derived for a single band Hubbard model on a two-dimensional bi-partite square lattice in the strong coupling regime. At half-filling the antiferromagnetic order parameter emerges as the minimum of the effective potential with an accuracy which improves over RPA calculations and is very close to that achieved by Monte Carlo simulations. Extensions to other magnetic systems are discussed.


1997 ◽  
Vol 55 (20) ◽  
pp. R13377-R13380 ◽  
Author(s):  
V. Ya. Pokrovskii ◽  
S. V. Zaitsev-Zotov ◽  
P. Monceau

1991 ◽  
Vol 24 (6) ◽  
pp. L279-L286 ◽  
Author(s):  
Y S Yang ◽  
C J Thompson

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