scholarly journals HTSC cuprate phase diagram using a modified Boson-Fermion-Gossamer model describing competing orders, a quantum critical point and possible resonance complex

2009 ◽  
Vol 109 (15) ◽  
pp. 3516-3532 ◽  
Author(s):  
Richard H. Squire ◽  
Norman H. March ◽  
Michael L. Booth
2015 ◽  
Vol 114 (9) ◽  
Author(s):  
S. K. Goh ◽  
D. A. Tompsett ◽  
P. J. Saines ◽  
H. C. Chang ◽  
T. Matsumoto ◽  
...  

2015 ◽  
Vol 92 (3) ◽  
Author(s):  
N. Kimura ◽  
N. Kabeya ◽  
H. Aoki ◽  
K. Ohyama ◽  
M. Maeda ◽  
...  

2004 ◽  
Vol 272-276 ◽  
pp. 50-51 ◽  
Author(s):  
K.H Kim ◽  
N Harrison ◽  
M Jaime ◽  
G.S Boebinger ◽  
J.A Mydosh

2013 ◽  
Vol 88 (18) ◽  
Author(s):  
M. Monteverde ◽  
J. Lorenzana ◽  
P. Monceau ◽  
M. Núñez-Regueiro

2010 ◽  
Vol 82 (10) ◽  
Author(s):  
S. Sanna ◽  
F. Coneri ◽  
A. Rigoldi ◽  
G. Concas ◽  
S. R. Giblin ◽  
...  

2021 ◽  
Vol 2021 (11) ◽  
Author(s):  
Eunseok Oh ◽  
Taewon Yuk ◽  
Sang-Jin Sin

Abstract We discuss quantum phase transition by a solvable model in the dual gravity setup. By considering the effect of the scalar condensation on the fermion spectrum near the quantum critical point(QCP), we find that there is a topologically protected fermion zero mode associated with the metal to insulator transition. Unlike the topological insulator, our zero mode is for the bulk of the material, not the edge. We also show that the strange metal phase with T-linear resistivity emerges at high enough temperature as far as a horizon exists. The phase boundaries calculated according to the density of states allow us understanding the structures of the phase diagram near the QCP.


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