scholarly journals Using Disorder to Identify Bogoliubov Fermi-Surface States

2021 ◽  
Vol 127 (25) ◽  
Author(s):  
Hanbit Oh ◽  
Daniel F. Agterberg ◽  
Eun-Gook Moon
Keyword(s):  
1996 ◽  
Vol 437 ◽  
Author(s):  
Eli Rotenberg ◽  
J. D. Denlinger ◽  
S. D. Kevan ◽  
K. W. Goodman ◽  
J. G. Tobin ◽  
...  

AbstractThe electronic states at the Fermi surface determine diverse properties such as magnetism, chemical bonding, and phonon-electron coupling. Using a conventional hemispherical analyzer at the ultraESCA beamline 7.0 of the Advanced Light Source, we have measured Fermi contours of the bulk and surface states of Cu(001) and Ag(001). For bulk states, we used uniform sampling in k-space by varying both the electron takeoff angle as well as the photon energy. Three-dimensional plots (in k-space) of bulk and surface states at the Fermi level can easily be achieved within one or two synchrotron shifts. Surface states, whose momentum is independent of k-perpendicular, are easily mapped if sufficiently dense angular sampling is performed. The states crossing the Fermi level at X in the surface Brillouin Zone of Cu(100) and Ag(100) are presented as examples.


2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Danica Krstovska ◽  
Aleksandar Skeparovski

Abstract Surface quantum states in quasi-two dimensional organic conductors induced by an external magnetic field tilted in the plane of the layers are obtained and analyzed. In tilted magnetic fields, these states arise from the transitions of the electrons between the closed orbits on the sides of the Fermi surface determined by the electron momentum along the magnetic field direction p B and the coordinate of the center of electron revolution Z. By far, in organic conductors, the surface states have not been studied for tilted magnetic fields. In this work, we have performed detail analyses of the surface states in a tilted in-plane magnetic field by calculating the surface energy spectrum and surface wave functions in order to address their properties and features. We find that, in a tilted magnetic field, the surface levels have higher energies compared to those at zero tilt angle but can be observed only up to a certain tilt angle. The resonant magnetic field and angular values at which the peaks in the surface oscillations should be observed are obtained. Further theoretical and new experimental studies of the surface states in a tilted magnetic field might give new insights into the surface properties of quasi-two dimensional organic conductors. Additionally, they may reveal new information about the parameters of the Fermi surface of organic conductors necessary for its reconstruction.


2018 ◽  
Vol 30 (18) ◽  
pp. 185601
Author(s):  
K Shrestha ◽  
V Marinova ◽  
B Lorenz ◽  
C W Chu
Keyword(s):  

1984 ◽  
Vol 49 (7) ◽  
pp. 623-626 ◽  
Author(s):  
R.G. Jordan ◽  
P.J. Durham

2000 ◽  
Vol 85 (24) ◽  
pp. 5194-5197 ◽  
Author(s):  
A. Damascelli ◽  
D. H. Lu ◽  
K. M. Shen ◽  
N. P. Armitage ◽  
F. Ronning ◽  
...  

2013 ◽  
Vol 82 (12) ◽  
pp. 124706 ◽  
Author(s):  
Shigeki Miyasaka ◽  
Akira Takemori ◽  
Tatsuya Kobayashi ◽  
Shinnosuke Suzuki ◽  
Satoshi Saijo ◽  
...  

2018 ◽  
Vol 98 (10) ◽  
Author(s):  
A. Takemori ◽  
T. Hajiri ◽  
S. Miyasaka ◽  
Z. H. Tin ◽  
T. Adachi ◽  
...  

1999 ◽  
Vol 68 (4) ◽  
pp. 1398-1403 ◽  
Author(s):  
Taichi Okuda ◽  
Masato Kotsugi ◽  
Kan Nakatsuji ◽  
Masao Fujikawa ◽  
Shigemasa Suga ◽  
...  

1997 ◽  
Vol 04 (02) ◽  
pp. 391-408 ◽  
Author(s):  
J. OSTERWALDER

Angle-resolved ultraviolet photoelectron spectroscopy (ARUPS) data are usually measured spectrum by spectrum at various emission angles or photon energies in order to observe the dispersion of energy bands in solids and on their surfaces. In these lecture notes an alternative experimental procedure is described which yields a direct mapping of constant energy surfaces within the band structure, and specifically of the Fermi surface. This approach appears very promising, in particular when applied to magnetic systems and systems with narrow bands. Fermi surfaces of surface states are seen in direct relation to the underlying bulk Fermi surface.


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