scholarly journals Charge order and its connection with Fermi-liquid charge transport in a pristine high-Tc cuprate

2014 ◽  
Vol 5 (1) ◽  
Author(s):  
W. Tabis ◽  
Y. Li ◽  
M. Le Tacon ◽  
L. Braicovich ◽  
A. Kreyssig ◽  
...  
2006 ◽  
Vol 435 (1-2) ◽  
pp. 1-7
Author(s):  
Yukio Tanaka ◽  
Satoshi Kashiwaya ◽  
Yasuhiro Asano ◽  
Takehito Yokoyama

2020 ◽  
Author(s):  
Jiawei Wang ◽  
Jiebin Niu ◽  
Bin Shao ◽  
Guanhua YANG ◽  
Congyan Lu ◽  
...  

Abstract Organic conjugated polymers demonstrate great potential in the transistor, solar cell and light-emitting diodes. The performances of those devices are fundamentally governed by charge transport within the active materials. However, the morphology-property relationships and the underpinning charge transport mechanism in polymers remain unclear. Particularly, whether the nonlinear charge transport in doped conducting polymers, i.e., anomalous non-Ohmic behaviors at low temperature, is appropriately formulated within non-Fermi liquid picture is not clear. In this work, via varying crystalline degrees of samples, we carried out systematic investigations on the charge transport nonlinearity in conducting polymers. Possible charge carriers’ dimensionality was discussed with experiments when varying the molecular chain’s crystalline orders. A heterogeneous-resistive-network (HRN) model was proposed based on the tied link between Fermi liquids (FL) and Luttinger liquids (LL), related to the high-ordered crystalline zones and weak-coupled amorphous regions, respectively. This mesoscopic HRN model is experimentally supported by precise electrical and microstructural characterizations, together with theoretic evaluations. Significantly, such model well describes the nonlinear transport behaviors in conducting polymers universally and provides new insights into the microstructure-correlated charge transport in organic conducting/semiconducting systems.


1998 ◽  
Vol 12 (29n31) ◽  
pp. 3023-3026
Author(s):  
De-Hua Lin ◽  
Xingang Wu

Studying the change of the cuprate's crystal structure based on doping and then the effect on its high-T c superconductivity, is an effective way to seek the mechanism of superconductivity. We explore the doping effect in the cuprate's crystal structure, such as the property of Cu-O layers, the interlayer spacing, the density of carriers and so on. Then, by considering the effect of the nuclear spin, we construct a three-dimensional superconductivity model, which is a correction of the nonphonon mechanism in a layered Fermi-Liquid.


2000 ◽  
Vol 276-278 ◽  
pp. 780-781
Author(s):  
A Mirmelstein ◽  
A Podlesnyak ◽  
N Golosova ◽  
V Bobrovskii ◽  
E Mitberg ◽  
...  

1987 ◽  
Vol 01 (03n04) ◽  
pp. 1089-1096
Author(s):  
D. Schmeltzer

The system X–La–Cu–O is described as a Fermi liquid with antiferromagnetic interaction. This interaction gives rise to two types of fluctuations, magnetic and superconducting. As a result, we find a free energy which contains two order parameters which at high temperature give rise to superconductivity and at low temperature to reentry-like paramagnetism. For two-dimensional systems, topological effects give rise to fractional statistics and as a result superconductivity appears when the topological angle θ gives rise to a Bose statistic.


1990 ◽  
Vol 04 (08) ◽  
pp. 561-564 ◽  
Author(s):  
K. H. JOHNSON

Recent angle-resolved photoemission studies of the valence-band states of the high-T c superconductor, Bi 2( Ca,Sr,La )3 Cu 2 O 8, have led workers to conclude that the electronic states at the Fermi energy (E F ) have mainly O 2px and 2py symmetry, while O 2pz-like states are not allowed by the C4υ(∆5) symmetry of these states. Nevertheless, a complete projection of the basis functions for the C4υ symmetry group ∆5 (or "E") representation indicates both O 2px, 2py and O 2pz orbital contributions at E F . The O 2px and 2py components are nonbonding, whereas the O 2pz orbitals overlap under the influence of significant Cu (dxz,yzπ*)− O (pzπ) antibonding hybridization to form spatially delocalized O (pzπ)− O (pzπ) bonding molecular orbitals parallel to the Cu–O x − y (a − b) planes. The doubly-degenerate O (pzπ)− O (pzπ) "bonds" and their associated shallow "double-well" potentials are the basis for Fermi-liquid character and a dynamic Jahn-Teller mechanism for Cooper pairing first proposed in 1983 and first applied to high-T c oxides in 1987.


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