scholarly journals COALESCENCE OF ANDREEV BOUND STATES ON THE SURFACE OF A CHIRAL TOPOLOGICAL SEMIMETAL

Author(s):  
V. D. ESIN ◽  
YU. S. BARASH ◽  
A. V. TIMONINA ◽  
N. N. KOLESNIKOV ◽  
E. V. DEVIATOV

JETP Letters ◽  
2021 ◽  
Author(s):  
V. D. Esin ◽  
Yu. S. Barash ◽  
A. V. Timonina ◽  
N. N. Kolesnikov ◽  
E. V. Deviatov


2003 ◽  
Vol 387 (1-2) ◽  
pp. 7-12 ◽  
Author(s):  
M. Krawiec ◽  
B.L. Györffy ◽  
J.F. Annett


2014 ◽  
Vol 119 (6) ◽  
pp. 1034-1041
Author(s):  
Y. Lin ◽  
A. J. Leggett


2017 ◽  
Vol 96 (14) ◽  
Author(s):  
Raffael L. Klees ◽  
Gianluca Rastelli ◽  
Wolfgang Belzig


2018 ◽  
Vol 382 (14) ◽  
pp. 991-994 ◽  
Author(s):  
Han-Zhao Tang ◽  
Ying-Tao Zhang ◽  
Jian-Jun Liu


2020 ◽  
Vol 11 (1) ◽  
Author(s):  
S. Autti ◽  
S. L. Ahlstrom ◽  
R. P. Haley ◽  
A. Jennings ◽  
G. R. Pickett ◽  
...  

Abstract The ground state of a fermionic condensate is well protected against perturbations in the presence of an isotropic gap. Regions of gap suppression, surfaces and vortex cores which host Andreev-bound states, seemingly lift that strict protection. Here we show that in superfluid 3He the role of bound states is more subtle: when a macroscopic object moves in the superfluid at velocities exceeding the Landau critical velocity, little to no bulk pair breaking takes place, while the damping observed originates from the bound states covering the moving object. We identify two separate timescales that govern the bound state dynamics, one of them much longer than theoretically anticipated, and show that the bound states do not interact with bulk excitations.



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