Tunnelling effects on surface bound states in unconventional superconductors
By S. Kashiwaya, Yukio Tanaka. 2000
784 citations recorded by the source corpus.
Subfields: Atomic and Molecular Physics, and Optics, Condensed Matter Physics, Electronic, Optical and Magnetic Materials
View Paper: https://www.semanticscholar.org/paper/d20653e21f17ccd6c2135ba7fd30655f4305f80c
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In Atomic and Molecular Physics, and Optics
- Y. Ando
- Masatoshi Sato
- E. Il'ichev
- Alexander V. Balatsky
- M. Kupriyanov
- A. Golubov
- K. Kawabata
- Ken Shiozaki
In Condensed Matter Physics
- Y. Ando
- Masatoshi Sato
- E. Il'ichev
- Alexander V. Balatsky
- M. Kupriyanov
- A. Golubov
- A. Gurevich
- P. Hirschfeld
In Electronic, Optical and Magnetic Materials
Citations in the corpus
- Scanning tunneling spectroscopy of high-temperature superconductors (2006, neutral): “Phys., Vol. 79, No. 1, January–March 2007 enhanced conductance—the so-called zero-bias conductance peak—instead of a gap at EF Kashiwaya and Tanaka, 2000 .”
- Topological superconductors: a review (2016, background): “They are very sensitive to the phase of the superconducting wavefunctions, and thus provide useful information on the pairing symmetry [47, 48].”
- Impurity-induced states in conventional and unconventional superconductors (2004, background): “…rich phenomena related to the surfaces playing the role of extended impurities that can also lead to the formation of the bound states (Aprili et al., 1998; Blonder et al., 1982; Buchholtz and Zwicknagl, 1981; Covington et al., 1997; Fogelström et al., 1997; Hu, 1994; Kashiwaya and Tanaka, 2000).”
- The current-phase relation in Josephson junctions (2004, background): “…the physics of the Joseph- 1See, for example, Kupriyanov and Likharev, 1990; Braginski, 1992; Sigrist and Rice, 1995; van Harlingen, 1995; Delin and Kleinsasser, 1996; Kashiwaya and Tanaka, 2000; Tsuei and Kirtley, 2000; Löfwander et al., 2001; Makhlin et al., 2001; Hilgenkamp and Mannhart, 2002.”
- Grain boundaries in high-Tc superconductors (2002, background): “The high RnA values of typically 10 28 V cm2, which correspond to resistivities of the order of 1021 V cm for an assumed effective thickness of a resistive region of ;1 nm (Chaudhari, Dimos, and Mannhart, 1990), are indicative 11See, for example, Millis, 1994; Barash et al., 1995; Bruder et al., 199”