superconductivity.bib

@article{PhysRevLett.100.096407,
  author = {Fu, Liang and Kane, C. L.},
  title = {{Superconducting Proximity Effect and Majorana Fermions at the Surface of a Topological Insulator}},
  month = mar,
  year = {2008},
  journal = {Phys. Rev. Lett.},
  volume = {100},
  pages = {096407},
  issue = {9},
  numpages = {4},
  publisher = {American Physical Society},
  doi = {10.1103/PhysRevLett.100.096407},
  url = {http://link.aps.org/doi/10.1103/PhysRevLett.100.096407},
  abstract = {We study the proximity effect between an s-wave superconductor and the surface states of a strong topological insulator. The resulting two-dimensional state resembles a spinless px+ipy superconductor, but does not break time reversal symmetry. This state supports Majorana bound states at vortices. We show that linear junctions between superconductors mediated by the topological insulator form a nonchiral one-dimensional wire for Majorana fermions, and that circuits formed from these junctions provide a method for creating, manipulating, and fusing Majorana bound states.}
}

@article{PhysRevLett.87.037004,
  author = {Gor'kov, Lev P. and Rashba, Emmanuel I.},
  title = {{Superconducting 2D System with Lifted Spin Degeneracy: Mixed Singlet-Triplet State}},
  month = jul,
  year = {2001},
  publisher = {American Physical Society},
  journal = {Phys. Rev. Lett.},
  volume = {87},
  pages = {037004},
  issue = {3},
  numpages = {4},
  doi = {10.1103/PhysRevLett.87.037004},
  url = {http://link.aps.org/doi/10.1103/PhysRevLett.87.037004},
  abstract = {Motivated by recent experimental findings, we have developed a theory of the superconducting state for 2D metals without inversion symmetry modeling the geometry of a surface superconducting layer in a field-effect transistor or near the boundary doped by adsorbed ions. In such systems the twofold spin degeneracy is lifted by spin-orbit interaction, and singlet and triplet pairings are mixed in the wave function of the Cooper pairs. As a result, spin magnetic susceptibility becomes anisotropic and Knight shift retains finite and rather high value at T=0.}
}

@incollection{maki1969superconductivity,
  title = {Gapless Superconductivity},
  booktitle = {Superconductivity},
  author = {Maki, K},
  editor = {Parks, R. D.},
  year = {1969},
  publisher = {Dekker, New York}
}

@article{Maki01061964,
  author = {Maki, Kazumi and Tsuneto, Toshihiko},
  title = {{Pauli Paramagnetism and Superconducting State}},
  year = {1964},
  month = jun,
  journal = {Progress of Theoretical Physics},
  volume = {31},
  number = {6},
  pages = {945},
  doi = {10.1143/PTP.31.945},
  url = {https://dx.doi.org/10.1143/PTP.31.945},
  abstract = {The effect of the Pauli paramagnetism on superconductors is discussed in detail. It is shown that the phase transition due to the paramagnetic effect changes its order from the first to the second as temperature increases. The modification of the mixed state in superconductors of the second kind is also discussed.}
}

@article{AbrikosovGorkov1961,
  author = {Abrikosov, A.A. and Gor'kov, L.P.},
  title = {{Contribution to the theory of superconducting alloys with paramagnetic impurities}},
  year = {1961},
  month = dec,
  journal = {Soviet Phys. JETP},
  volume = {12},
  number = {6},
  pages = {1243},
  abstract = {It was demonstrated within the framework of superconductivity theory that the transition temperature, T_c, of a superconductor with paramagnetic impurities is lower than that of a pure metal.  The dependence of T_c on the impurity concentration was determined. At a certain critical concentration the superconductivity disappeared. The thermodynamic and magnetic properties of superconducting alloys in a concentration range close to the critical value were studied in detail. It was found that for T yields O there is no exponential term in the expression for the heat capacity in this region. The concentration dependence of the energy spectrum gap of such a system was determined. It was found that for a concentration n' approx equal 0.9 n_cr the gap disappears and at large concentrations the system has a continuous spectrum.}
}