scholarly journals Four-band extended Hubbard Hamiltonian for the one-dimensional cuprateSr2CuO3:Distribution of oxygen holes and its relation to strong intersite Coulomb interaction

2000 ◽  
Vol 62 (16) ◽  
pp. 10752-10765 ◽  
Author(s):  
R. Neudert ◽  
S.-L. Drechsler ◽  
J. Málek ◽  
H. Rosner ◽  
M. Kielwein ◽  
...  
1991 ◽  
Vol 43 (1-2) ◽  
pp. 3531-3534 ◽  
Author(s):  
W.R Somsky ◽  
D.K Campbell ◽  
H.-Q Lin ◽  
X Wang ◽  
J.E Gubernatis

2009 ◽  
Vol 80 (4) ◽  
Author(s):  
M. I. Makin ◽  
Jared H. Cole ◽  
Charles D. Hill ◽  
Andrew D. Greentree ◽  
Lloyd C. L. Hollenberg

2004 ◽  
Vol 18 (03) ◽  
pp. 357-368 ◽  
Author(s):  
HANA ČENČARIKOVÁ ◽  
PAVOL FARKAŠOVSKÝ

The extrapolation of finite-cluster calculations is used to examine ground-state properties of the one-dimensional Falicov–Kimball model with correlated hopping. It is shown that the correlated hopping strongly influences both the valence transitions and the conducting properties of the model and so it should not be neglected in the correct description of materials with correlated electrons. This is illustrated for two selected values of the Coulomb interaction that represent typical behavior of the model for small and intermediate (strong) interactions. In both cases the insulator–metal transitions (accompanied by continuous or discontinuous valence transitions) induced by correlated hopping are observed.


Open Physics ◽  
2012 ◽  
Vol 10 (4) ◽  
Author(s):  
Dorota Jakubczyk ◽  
Paweł Jakubczyk

AbstractWe discuss the one-dimensional Hubbard model, on finite sites spin chain, in context of the action of the direct product of two unitary groups SU(2)×SU(2). The symmetry revealed by this group is applicable in the procedure of exact diagonalization of the Hubbard Hamiltonian. This result combined with the translational symmetry, given as the basis of wavelets of the appropriate Fourier transforms, provides, besides the energy, additional conserved quantities, which are presented in the case of a half-filled, four sites spin chain. Since we are dealing with four elementary excitations, two quasiparticles called “spinons”, which carry spin, and two other called “holon” and “antyholon”, which carry charge, the usual spin-SU(2) algebra for spinons and the so called pseudospin-SU(2) algebra for holons and antiholons, provide four additional quantum numbers.


1996 ◽  
Vol 53 (14) ◽  
pp. R8828-R8831 ◽  
Author(s):  
Naokazu Shibata ◽  
Tomotoshi Nishino ◽  
Kazuo Ueda ◽  
Chikara Ishii

2021 ◽  
Vol 3 (4) ◽  
Author(s):  
N. Aucar Boidi ◽  
H. Fernández García ◽  
Y. Núñez-Fernández ◽  
K. Hallberg

Author(s):  
Jacob Szeftel

A procedure, dedicated to superconductivity, is extended to study the properties of interacting electrons in normal metals in the thermodynamic limit. Each independent-electron band is shown to split into two correlated-electron bands. Excellent agreement is achieved with Bethe's wave-function for the one-dimensional Hubbard model. The groundstate energy, reckoned for the two-dimensional Hubbard Hamiltonian, is found to be lower than values, obtained thanks to the numerical methods. This analysis applies for any spatial dimension and temperature.


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