scholarly journals Coexistence of a double-Qspin-density wave and a multi-Qpair-density wave in cuprate oxide superconductors

2006 ◽  
Vol 73 (9) ◽  
Author(s):  
Fusayoshi J. Ohkawa
1994 ◽  
Vol 235-240 ◽  
pp. 1049-1050 ◽  
Author(s):  
T. Maruyama ◽  
Y. Aiura ◽  
Y. Nishihara ◽  
T. Ito ◽  
K. Oka ◽  
...  

1991 ◽  
Vol 185-189 ◽  
pp. 303-308 ◽  
Author(s):  
M. Tachiki ◽  
T. Koyama ◽  
S. Takahashi

1996 ◽  
Vol 10 (15) ◽  
pp. 705-716
Author(s):  
MING-LIANG ZHANG ◽  
ZHONG-XIAN ZHAO

Spin and charge fluctuation are obtained from a two-band model making use of saddle point approximation in path-integral form.


1999 ◽  
Vol 13 (01) ◽  
pp. 25-48 ◽  
Author(s):  
DAVID DJAJAPUTRA ◽  
JOHN RUVALDS

We investigate the response of an electron system which exhibits ideal nesting features. Using the standard Matsubara formalism we derive analytic expressions for the imaginary and real parts of the bare particle–hole susceptibility. The imaginary part has sharp peaks whose maxima at the nesting momenta approximately scale with (ω/T). The peak lineshapes resemble neutron scattering data on chromium and some copper oxide superconductors. The real part of the bare susceptibility at the nesting vectors diverges logarithmically at low temperatures. Analytic formulas for the first vertex correction to the susceptibility are derived for a Hubbard interaction and its momentum and temperature variations are calculated numerically. This term detracts substantially from the ordinary RPA terms for intermediate values of the Coulomb repulsion. Exact cancellation of a certain class of diagrams at half filling is shown to result from particle–hole symmetry. We discuss the consequences of these results for spin fluctuation theories of high temperature superconductors and spin density wave instabilities.


1988 ◽  
Vol 52 (22) ◽  
pp. 1915-1917 ◽  
Author(s):  
M. K. Wu ◽  
J. R. Ashburn ◽  
C. A. Higgins ◽  
C. W. Fellows ◽  
B. H. Loo ◽  
...  

2001 ◽  
Vol 689 ◽  
Author(s):  
John B. Goodenough

ABSTRACTThe phase diagram of La2-xSrxCuO4 is interpreted. From the virial theorem, it is argued that the cross-over from localized to itinerant electronic behavior in the range 0 < x < 0.3 is characterized by fluctuations between two equilibrium Cu-O bond lengths. Cooperative local fluctuations give rise to one-hole correlation bags of 5 to 6 copper centers on the underdoped side, to strong-correlation fluctuations in an itinerant-electron matrix on the overdoped side. Spinodal phase segregation between an antiferromagnetic, insulating parent phase and the superconductive phase occurs in the underdoped compositions, between the superconductive phase and the metallic overdoped phase on the other side of the phase diagram. Ordering of the fluctuations into a travelling bipolaronic charge-density/spin-density wave of composition x ≈?1/6 yields heavy fermions of symmetry (x2− y2) coexisting with light electrons; the high-temperature superconductive pairs are condensed out from the heavy fermions.


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