TY - JOUR
T1 - Superconductivity and antiferromagnetism in the phase diagram of the frustrated Hubbard model within a variational study
AU - Kobayashi, Kenji
AU - Yokoyama, Hisatoshi
PY - 2010/11/1
Y1 - 2010/11/1
N2 - The interplay between antiferromagnetism (AF) and superconductivity (SC) in cuprates is studied for the two-dimensional Hubbard model with a diagonal transfer t', using a variational Monte Carlo method. Optimizing an improved function for strongly correlated values of U/t, we construct phase diagrams in the d (doping rate)-t'/t space. It is found that the stable state is sensitive to the value of model parameters: For the extremely large values of U/t, a coexisting state is realized for t'/t ≳ -0.15, whose range of doping rate extends as t'/t increases. In contrast, for t'/t= -0.3, AF and SC states are mutually exclusive, and a coexisting state does not appear. As U/t decreases, the area of pure AF extends, and that of coexisting state shrinks. As a result, the coexisting state disappears for t'/t= -0.15 and U/t= 12, probable values for holedoped cuprates. Compared with the t-J model, the Hubbard model has richer phases.
AB - The interplay between antiferromagnetism (AF) and superconductivity (SC) in cuprates is studied for the two-dimensional Hubbard model with a diagonal transfer t', using a variational Monte Carlo method. Optimizing an improved function for strongly correlated values of U/t, we construct phase diagrams in the d (doping rate)-t'/t space. It is found that the stable state is sensitive to the value of model parameters: For the extremely large values of U/t, a coexisting state is realized for t'/t ≳ -0.15, whose range of doping rate extends as t'/t increases. In contrast, for t'/t= -0.3, AF and SC states are mutually exclusive, and a coexisting state does not appear. As U/t decreases, the area of pure AF extends, and that of coexisting state shrinks. As a result, the coexisting state disappears for t'/t= -0.15 and U/t= 12, probable values for holedoped cuprates. Compared with the t-J model, the Hubbard model has richer phases.
KW - Cuprate
KW - Hubbard model
KW - Superconductivity
KW - Variational Monte Carlo method
UR - http://www.scopus.com/inward/record.url?scp=77957897786&partnerID=8YFLogxK
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U2 - 10.1016/j.physc.2010.05.041
DO - 10.1016/j.physc.2010.05.041
M3 - Article
AN - SCOPUS:77957897786
SN - 0921-4534
VL - 470
SP - 1081
EP - 1084
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - 20
ER -