Anisotropy of the Fermi surface, Fermi velocity, many-body enhancement, and superconducting energy gap in Nb

1987 ◽  
Vol 35 (4) ◽  
pp. 1728-1741 ◽  
Author(s):  
G. W. Crabtree ◽  
D. H. Dye ◽  
D. P. Karim ◽  
S. A. Campbell ◽  
J. B. Ketterson
2007 ◽  
Vol 21 (18n19) ◽  
pp. 3290-3293 ◽  
Author(s):  
G. L. ZHAO ◽  
D. BAGAYOKO

The superconducting energy gap of YBa 2 Cu 3 O 7 (YBCO) varies strongly with [Formula: see text] and from a sheet of the Fermi surface to another. The strong anisotropic superconducting gap in high Tc materials such as YBCO has led to conflicting d-wave and s-wave interpretations. We have utilized electronic wave functions from the ab-initio density functional calculation and the related electron-phonon interaction matrix elements for the calculation of the superconducting gap values of YBCO. We have found that the superconducting gap on one sheet of the Fermi surface around S-point only shows a minor variation from about 18 meV to 25 meV. Especially, there is no node on this sheet of the Fermi surface around the S-point. We propose a new test measurement of the superconducting gap of YBCO on this sheet of the Fermi surface around the S-point in the Brillouin zone. This measurement is expected to shed light on the gap symmetry properties of high Tc superconductors.


1988 ◽  
Vol 76-77 ◽  
pp. 35-36 ◽  
Author(s):  
T. Müller ◽  
W. Joss ◽  
J.M. van Ruitenbeek ◽  
U. Welp ◽  
P. Wyder ◽  
...  

2017 ◽  
Vol 114 (8) ◽  
pp. 1844-1849 ◽  
Author(s):  
Aavishkar A. Patel ◽  
Subir Sachdev

We compute parameters characterizing many-body quantum chaos for a critical Fermi surface without quasiparticle excitations. We examine a theory ofNspecies of fermions at nonzero density coupled to aU(1)gauge field in two spatial dimensions and determine the Lyapunov rate and the butterfly velocity in an extended random-phase approximation. The thermal diffusivity is found to be universally related to these chaos parameters; i.e., the relationship is independent ofN, the gauge-coupling constant, the Fermi velocity, the Fermi surface curvature, and high-energy details.


Measurements have been made of the variation with crystal orientation of the anomalous skin resistance of plane surfaces of pure copper at low temperatures and at a frequency of 22700 Mc/s. The resistance is related to the geometrical form of the Fermi surface, and a surface is determined which has the correct shape to account for the experimental results. It is believed that there is no other solution which would give equally good agreement. As determined, the surface, which holds one electron per atom, will not quite fit into the Brillouin zone, overlapping in the (111) directions where the zone boundary is closest to the origin. From an examination of simple models it is concluded that probably there is contact with the zone boundary over small areas around these points, and the energy gap across these boundaries is estimated to be about 71/2 eV. Apart from extension to the boundaries in the (111) directions the Fermi surface is more or less spherical. An estimate is made of the Fermi velocity and its variations over the surface, from which it is concluded that the electronic specific heat should lie between 1.7 and 1.9 times that of a free-electron model of copper. The experimental value is 1.38, and it is tentatively suggested that the discrepancy may find an explanation in the theory of Bohm & Pines. Various transport phenomena are briefly discussed, but no reliable evidence is discovered bearing directly on the shape of the Fermi surface. It is concluded that the method, though laborious in interpretation, may be applied with advantage to other simple metals such as silver and gold.


1981 ◽  
Vol 23 (2) ◽  
pp. 462-473 ◽  
Author(s):  
D. H. Dye ◽  
S. A. Campbell ◽  
G. W. Crabtree ◽  
J. B. Ketterson ◽  
N. B. Sandesara ◽  
...  

1972 ◽  
Vol 50 (21) ◽  
pp. 2568-2573
Author(s):  
C. R. Leavens ◽  
J. P. Carbotte

We have calculated the superconducting energy gap for a large number of points on the irreducible (1/48)th of the Fermi surface of pure single-crystal aluminum both at zero and finite pressure. It is found that the energy gap anisotropy in aluminum increases with increasing pressure.


2021 ◽  
Vol 7 (17) ◽  
pp. eabd9275
Author(s):  
Samuel Beaulieu ◽  
Shuo Dong ◽  
Nicolas Tancogne-Dejean ◽  
Maciej Dendzik ◽  
Tommaso Pincelli ◽  
...  

Fermi surface is at the heart of our understanding of metals and strongly correlated many-body systems. An abrupt change in the Fermi surface topology, also called Lifshitz transition, can lead to the emergence of fascinating phenomena like colossal magnetoresistance and superconductivity. While Lifshitz transitions have been demonstrated for a broad range of materials by equilibrium tuning of macroscopic parameters such as strain, doping, pressure, and temperature, a nonequilibrium dynamical route toward ultrafast modification of the Fermi surface topology has not been experimentally demonstrated. Combining time-resolved multidimensional photoemission spectroscopy with state-of-the-art TDDFT+U simulations, we introduce a scheme for driving an ultrafast Lifshitz transition in the correlated type-II Weyl semimetal Td-MoTe2. We demonstrate that this nonequilibrium topological electronic transition finds its microscopic origin in the dynamical modification of the effective electronic correlations. These results shed light on a previously unexplored ultrafast scheme for controlling the Fermi surface topology in correlated quantum materials.


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