scholarly journals Possibility of Cooper-pair formation controlled by multi-terminal spin injection

2018 ◽  
Vol 969 ◽  
pp. 012028
Author(s):  
K Ohnishi ◽  
M Sakamoto ◽  
M Ishitaki ◽  
T Kimura
2010 ◽  
Vol 7 (1) ◽  
pp. 21-25 ◽  
Author(s):  
Takeshi Kondo ◽  
Yoichiro Hamaya ◽  
Ari D. Palczewski ◽  
Tsunehiro Takeuchi ◽  
J. S. Wen ◽  
...  

2014 ◽  
Vol 112 (14) ◽  
Author(s):  
K. Jänkälä ◽  
P. Lablanquie ◽  
F. Penent ◽  
J. Palaudoux ◽  
L. Andric ◽  
...  

Author(s):  
Ekkehard Krüger

As shown in former papers, the nonadiabatic Heisenberg model presents a novel mechanism of Cooper pair formation generated by the strongly correlated atomic-like motion of the electrons in narrow, roughly half-filled "superconducting bands". These are energy bands represented by optimally localized spin-dependent Wannier functions adapted to the symmetry of the material under consideration. The formation of Cooper pairs is not the result of an attractive electron-electron interaction but can be described in terms of quantum mechanical constraining forces constraining the electrons to form Cooper pairs. There is theoretical and experimental evidence that only this nonadiabatic mechanism operating in superconducting bands may produce eigenstates in which the electrons form Cooper pairs. These constraining forces stabilize the Cooper pairs in any superconductor, whether conventional or unconventional. Here we report evidence that also the experimentally found superconducting state in bismuth at ambient as well as at high pressure is connected with a narrow, roughly half-filled superconducting band in the respective band structure. This observation corroborates once more the significance of constraining forces in the theory of superconductivity.


1999 ◽  
Vol 59 (2) ◽  
pp. 1556-1561 ◽  
Author(s):  
M. Houbiers ◽  
H. T. C. Stoof

AIP Advances ◽  
2014 ◽  
Vol 4 (8) ◽  
pp. 087126 ◽  
Author(s):  
Rakesh Kar ◽  
Tamal Goswami ◽  
Bikash Chandra Paul ◽  
Anirban Misra

2000 ◽  
Vol 14 (29n31) ◽  
pp. 3312-3321 ◽  
Author(s):  
MASATOSHI ARAI ◽  
YASUO ENDOH ◽  
SETSUKO TAJIMA ◽  
STEPHAN. M. BENNINGTON

According to the recent neutron scattering data on YBCO, it has been concluded that the incommensurability of the spin dynamics is a common feature among oxide high-Tc superconductors, which cannot be explainable by Fermi surface anomaly. In this paper, we speculate a possible scenario of the mechanism of the superconductivity based upon an assumption of the stripe domain structures; RVB-like spin singlet formation plays a primary role for the attractive force for the Cooper pair formation of dopant holes existing in the adjacent charge chain site, which is separated by the spin stripes.


2010 ◽  
Vol 2010 ◽  
pp. 1-36 ◽  
Author(s):  
Pavol Baňacký

Complex electronic ground state of molecular and solid state system is analyzed on the ab initio level beyond the adiabatic Born-Oppenheimer approximation (BOA). The attention is focused on the band structure fluctuation (BSF) at Fermi level, which is induced by electron-phonon coupling in superconductors, and which is absent in the non-superconducting analogues. The BSF in superconductors results in breakdown of the adiabatic BOA. At these circumstances, chemical potential is substantially reduced and system is stabilized (effect of nuclear dynamics) in the antiadiabatic state at broken symmetry with a gap(s) in one-particle spectrum. Distorted nuclear structure has fluxional character and geometric degeneracy of the antiadiabatic ground state enables formation of mobile bipolarons in real space. It has been shown that an effective attractive e-e interaction (Cooper-pair formation) is in fact correction to electron correlation energy at transition from adiabatic into antiadiabatic ground electronic state. In this respect, Cooper-pair formation is not the primary reason for transition into superconducting state, but it is a consequence of antiadiabatic state formation. It has been shown that thermodynamic properties of system in antiadiabatic state correspond to thermodynamics of superconducting state. Illustrative application of the theory for different types of superconductors is presented.


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