A. Sauls, M. Sigrist, C-C. Tsuei, D. J. van Harlingen, V. Vakaryuk, S-K. Yip and F-C. Zhang for useful discussions over the years and K. Ishida for sharing the new Knight shift data in April 2019 prior to the publication. where is defined so that it contains no Broader Concepts; Current Concept; Narrower Concepts; Broader Concepts; Order parameters; Superconductivity; Narrower Concepts; d-wave; f-wave; p-wave ; s-wave; Tip; Click to lock the view on the highlighted concept in the diagram. J Supercond Nov Magn (2020). Lett. Article  Lett. For the triplet states, SO interactions can at most affect, via the “K-S” terms in the effective Hamiltonian, the numerical value of α. To sign up for alerts, please log in first. In fact, using the relation , we <> Selecting this option will search all publications across the Scitation platform, Selecting this option will search all publications for the Publisher/Society in context, The Journal of the Acoustical Society of America, Weyl nodes and magnetostructural instability in antiperovskite Mn, Possible experimental realization of a basic, Contrasted Sn substitution effects on Dirac line node semimetals SrIrO, Dirac fermions and possible weak antilocalization in LaCuSb, Topological nodal lines and hybrid Weyl nodes in YCoC, Special topic on topological semimetals—New directions, Center for Computational Quantum Physics, The Flatiron Institute, Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, Max Planck Institute for Solid State Research, Department of Chemistry, Princeton University, Institute for Theoretical Physics and Astrophysics, Julius-Maximilians University of Würzburg, Department of Chemistry, University of Zurich, Department of Physics, University of Zurich, https://doi.org/10.1103/physrevx.5.011029, https://doi.org/10.1103/physrevb.84.235126, https://doi.org/10.1088/1367-2630/18/11/115006, https://doi.org/10.1103/physrevb.94.241102, https://doi.org/10.1103/revmodphys.80.1083, https://doi.org/10.1103/physrevb.97.094508, https://doi.org/10.1103/revmodphys.83.1057, https://doi.org/10.1103/physrevlett.107.097001, https://doi.org/10.1103/physrevlett.104.057001, https://doi.org/10.1103/physrevlett.112.017002, https://doi.org/10.1103/physrevb.91.214517, https://doi.org/10.1038/s41567-019-0576-7, https://doi.org/10.1038/s41535-019-0189-5, https://doi.org/10.1038/s41467-017-01066-6, https://doi.org/10.1088/1674-1056/25/11/117106, https://doi.org/10.1103/physrevb.89.020505, https://doi.org/10.1016/j.physc.2007.04.232, https://doi.org/10.1103/physrevb.81.245114, https://doi.org/10.1080/14786435.2016.1154203, https://doi.org/10.1103/physrevb.86.174522, https://doi.org/10.1016/0927-0256(96)00008-0, https://doi.org/10.1016/j.cpc.2017.09.033, https://doi.org/10.1016/j.phpro.2012.04.042, https://doi.org/10.1103/physrevlett.102.117007, https://doi.org/10.1103/physrevb.87.180503, https://doi.org/10.1016/s0921-4534(02)02319-5, https://doi.org/10.1103/physrevb.65.094512, http://creativecommons.org/licenses/by/4.0/. Learn More ». Research Areas Superconductivity Superconducting order parameter Research Areas Phase transitions Order parameters Superconducting order parameter. the superconducting order parameter, we find that a non-zero Broader Concepts; Current Concept; Narrower Concepts; Broader Concepts; Order parameters; Superconductivity; Narrower Concepts; d-wave; f-wave; p-wave ; s-wave; Tip; Click to lock the view on the highlighted concept in the diagram. Anderson, unpublished pp 1–7 (1985), Geshkenbein, V.B., Larkin, A.I. 71, 2839 (2002), Mao, Z.Q., Maeno, Y., NishiZaki, S., Akima, T., Ishiguro, T.: Phys. We continue to discuss the behavior of the expectation value Temperature dependent magnetic penetration depth, Magnetism, if present in the samples, may also enhance the muon depolarization rate. 89, 034712 (2020), Annett, J.F., Goldenfeld, N.D., Leggett, A.J. Phys. 112, 127002 (2014), Volovik, G.E., Gor’kov, L.P.: Sov. the user has read and agrees to our Terms and Inversion of Eq. C 49, 1268 (1993), Huang, Q., Soubeyroux, J., Chmaissem, O., Sora, I.N., Santoro, A., Cava, R.J., Krajewski, J.J., Peck, W.F. The conversion from the d-vector notation to the “S-K” one used in the body of this paper is straightforward provided that the OP is even under reflection in the ab plane (so that the awkward Kz = 0 state does not occur): we simply use Eq. where is the phase of , the plastic field describes a static charge 2e at . It has been argued that the existence of a tetracritical point for all field orientations eliminates the two-dimensional (2D) orbital representations coupled to a symmetry-breaking field (SBF) as a viable theory of these phases and favours either a theory based on two primary order parameters belonging to different irreducible representations that are accidentally degenerate, as described by Chen and Garg 1993, or a spin-triplet, orbital one-dimensional representation with non spin-orbit coupling in the pairing channel, as described by Machida and Ozaki 1991. 92, 047002 (2004), Yonezawa, S., Kajikawa, T., Maeno, Y.: Phys. 131, 1553 (1963), Petsch, A.N., Zhu, M., Enderle, M., Mao, Z.Q., Maeno, Y., Hayden, S.M. Phys. Nodal-line semimetals are topologically nontrivial states of matter featuring band crossings along a closed curve, i.e., nodal-line, in momentum space. Use of the American Physical Society websites and journals implies that B 90(R), 220511 (2014), Scaffidi, T., Simon, S.H. <> Lett. 81, 011009 (2012), Kallin, C.: Rep. Prog. stream endobj we obtain for the correlation function, where now , and is the is the superconducting order parameter. That is, the operators See Off-Campus Access to Physical Review for further instructions. A.A. Abrikosov [18] could be used in order to explain the high T c and the values as high as ~ 13 meV. Phys. To answer this question we Although the standard derivation of these equations nowhere makes any reference to SO interactions, they are not affected by them, since the conversion from real spin to pseudospin, while it may change the effective magnetic moment of the normal-state excitations and hence affect χn, they cannot change the ratio χ(T)/χn for the singlet state. Lett. Rev. of the real-space representation (94) of the single loop operator the critical temperature from above. massless scalar correlation function. Much of the work done at Penn State was supported by DOE under Grant No. 74, 035115 (2004), Murakawa, H., Ishida, K., Kitagawa, K., Mao, Z.Q., Maeno, Y.: Phys. Wen, K. Page, C. J. Fennie, K. M. Shen, and T. M. McQueen, “, Evidence for topologically protected surface states and a superconducting phase in [Tl, 16. A. D. Hillier, J. Quintanilla, and R. Cywinski, “, Evidence for time-reversal symmetry breaking in the noncentrosymmetric superconductor LaNiC, 41. M. N. Ali, Q. D. Gibson, T. Klimczuk, and R. J. Cava, “, Noncentrosymmetric superconductor with a bulk three-dimensional Dirac cone gapped by strong spin-orbit coupling, Darstellung und struktur von NaAlSi und NaAlGe, 27. with the : Phys. Phys. model, where the gauge field is massive. out the gauge invariance of more clearly we write it in It is a pleasure to dedicate this paper to Brian Josephson, and to wish him many more happy years of activity in physics and elsewhere. The excess of Na is necessary for obtaining phase pure products; it partly acts as a sodium flux. To save the reader a little time, in this appendix we list some transformation properties of the Zeeman substates of the spin triplet state under rotation.

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