scholarly journals Resonantly interacting p -wave Fermi superfluid in two dimensions: Tan's contact and the breathing mode

2019 ◽  
Vol 100 (2) ◽  
Author(s):  
Hui Hu ◽  
Xia-Ji Liu
2018 ◽  
Vol 98 (6) ◽  
Author(s):  
Hui Hu ◽  
Brendan C. Mulkerin ◽  
Lianyi He ◽  
Jia Wang ◽  
Xia-Ji Liu

1974 ◽  
Vol 64 (6) ◽  
pp. 1789-1808 ◽  
Author(s):  
Robert Burridge ◽  
Cesar Levy

abstract It has recently been shown (Burridge, 1973) that in two dimensions plane-strain shear cracks lacking cohesion may run at speeds ranging from the Rayleigh-wave to the S-wave speed or possibly at the P-wave speed. On the other hand, it has long been known that in antiplane strain, cracks lacking cohesion must run at least at the S-wave speed. Since locally at the edge of a three-dimensional crack there is a combination of plane and antiplane strain, we have sought and found solutions for circular shear cracks expanding at the S-wave speed and at the P-wave speed. These have finite shear tractions ahead of the crack and so may correspond to frictional sliding in the absence of cohesion. The analysis combines the method of Kostrov (1964b) with the results of Burridge (1973). We carry out a complete evaluation for the displacements and tractions on the fault plane, and far-field radiation for the S-wave-speed crack. The corresponding evaluations for the P-wave speed are not elementary and are not attempted here. As far as the authors are aware, these are the first analytic solutions of three-dimensional crack problems which satisfy a physically plausible fracture criterion for failure under shear.


1987 ◽  
Vol 65 (11) ◽  
pp. 1445-1448
Author(s):  
Alexander L. Fetter

The significance of the order parameter is reviewed for the familiar case of vortices in the rotating Bose superfluid 4He. The triplet p-wave Cooper pairing in the Fermi superfluid 3He introduces new and unusual possibilities. In the rotating B phase, all vortices have singular cores, and several different structures have been investigated. In the rotating A phase, an additional feature is a nonsingular vortex with two quanta of circulation.


2014 ◽  
Vol 16 (1) ◽  
pp. 013001 ◽  
Author(s):  
Jan Willem Abraham ◽  
Michael Bonitz ◽  
Chris McDonald ◽  
Gianfranco Orlando ◽  
Thomas Brabec

Geophysics ◽  
1980 ◽  
Vol 45 (6) ◽  
pp. 1094-1095 ◽  
Author(s):  
A. L. Lucas ◽  
P. N. S. O’Brien ◽  
J. H. Thomas

In transversely isotropic media, the moveout velocity obtained from common‐depth‐point (CDP) analysis may be significantly different from the horizontal velocity of the pseudo‐P wave. In Levin’s (1978) paper, he discusses, among other things, the problem of velocity determination in a medium in which the pseudo‐P wave surface produced by a point source is an ellipsoid of revolution. He points out that one would expect many sedimentary rocks to be transversely isotropic with a vertical axis of symmetry. In his Appendix he proves that an ellipse (using two dimensions for convenience) is one possible shape for the wave surface in such a medium. He also shows, as have others, that in this case CDP velocity analysis measures the velocity of horizontal propagation.


1999 ◽  
Vol 13 (29n31) ◽  
pp. 3799-3807
Author(s):  
Hyun-Tak Kim ◽  
Yong-Jihn Kim ◽  
Kwang-Yong Kang

A ferromagnetic phase with electron carriers and a semiconducting phase with hole carriers were separated in La 1-x Ca x MnO 3 thin films by the van der Pauw method. We conclude that two phases are attributed to the metal-insulator instability. In the ferromagnetic phase for films with anisotropic moments in two dimensions, a remnant resistivity of the order of 10-8Ωm is observed up to 100 K and increases exponentially with temperature up to Tc and above one Tesla as a function of magnetic field strength (a positive magnetoresistivity). The phase below Tc is regarded as a polaronic state with a polaronic tunneling conduction. Possible p-wave condensation (or superconductor) with a parabolic density of states and the phase separation are discussed on the basis of the two-fold degeneracy of eg orbitals.


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