scholarly journals d-wave holographic superconductor vortex lattice and non-Abelian holographic superconductor droplet

2010 ◽  
Vol 82 (12) ◽  
Author(s):  
Hua-Bi Zeng ◽  
Zhe-Yong Fan ◽  
Hong-Shi Zong
1998 ◽  
Vol 44 (3) ◽  
pp. 367-373 ◽  
Author(s):  
J Shiraishi ◽  
M Kohmoto ◽  
K Maki
Keyword(s):  

2002 ◽  
Vol 66 (13) ◽  
Author(s):  
Michael A. Hermele ◽  
Luca Marinelli
Keyword(s):  

2002 ◽  
Vol 367 (1-4) ◽  
pp. 46-49 ◽  
Author(s):  
M. Takigawa ◽  
M. Ichioka ◽  
K. Machida

2010 ◽  
Vol 470 ◽  
pp. S564-S565
Author(s):  
Kenta M. Suzuki ◽  
Masanori Ichioka ◽  
Kazushige Machida

2010 ◽  
Vol 81 (2) ◽  
Author(s):  
Kengo Maeda ◽  
Makoto Natsuume ◽  
Takashi Okamura

1996 ◽  
Vol 10 (22) ◽  
pp. 2699-2721 ◽  
Author(s):  
JI-HAI XU ◽  
YONG REN ◽  
C. S. TING

YBa 2 Cu 3 O 7 (YBCO) exhibits a large anisotropy between the a (or y) and b (or x) axes in the CuO2 planes. This anisotropy can be modeled by introducing an anisotropic mass parameter λ = mx /my. Assuming a d-wave pairing interaction together with a repulsive on-site Coulomb interaction, we developed a Ginzburg–Landau theory for a d-wave superconductor with mass anisotropy in the presence of a magnetic field. We show that the order parameter always has s + d symmetry. The vortex structures for λ = 1 and λ > 1 have been numerically studied. For high T c cuprates with tetragonal structure (λ = 1), the vortex shows a four-fold symmetry and the vortex lattice may have oblique or triangular structure depending on the strength of the applied magnetic field, temperature, and the other parameters. For YBCO we choose λ = 2, the single vortex has an elliptic shape, and the vortex lattice always shows an oblique structure. All these results are in good agreement with experimental measurements.


Author(s):  
Jun’ichi Shiraishi ◽  
Mahito Kohmoto ◽  
Kazumi Maki
Keyword(s):  

Sign in / Sign up

Export Citation Format

Share Document