Lett. It is unclear how much of this dependence may be due to the dependence of \(<|u_{k}(0)|^{2}>_{E_{F}}\) on the applied field. Sun, V. Süß, M. Schmidt, U. Schwarz, E. Pippel, P. Werner, R. Hillebrand, T. Förster, E. Kampert, S. Parkin, R. J. Cava, C. Felser, B. Yan, and S. A. Medvedev, “, Superconductivity in Weyl semimetal candidate MoTe, 21. 71, 2839 (2002), Mao, Z.Q., Maeno, Y., NishiZaki, S., Akima, T., Ishiguro, T.: Phys. into a2 by writing them as 2a3(cos(ϕ)|c(+)|2|c(−)|2, where ϕ = 2argc(+)/c(−), minimizing with respect to ϕ and adding the result to the original a2. Lett. Gordon and Breach, London (1999), Woelfle, P.: J. Phys. : Rev. B 90(R), 220511 (2014), Scaffidi, T., Simon, S.H. JETP 3, 920 (1956), Slichter, C.: Principles of Magnetic Resonance, 3rd edn. 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. Research Areas Superconductivity Superconducting order parameter Research Areas Phase transitions Order parameters Superconducting order parameter. I comment on the limitations of the models proposed so far for the superconducting phases of UPt3. (ed.) Learn More ». The detailed H-T phase diagram places constraints on any theory for the multiple superconducting phases. have to investigate how is described in terms of the variables of the 92, 047002 (2004), Yonezawa, S., Kajikawa, T., Maeno, Y.: Phys. 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. Indeed, under a gauge the critical temperature from above. L. Muechler, A. Topp, R. Queiroz, M. Krivenkov, A. Varykhalov, J. Cano, C. R. Ast, and L. M. Schoop, “, Modular arithmetic with nodal lines: Drumhead surface states in ZrSiTe, 37. 3099067 To sign up for alerts, please log in first. C. Fang, H. Weng, X. Dai, and Z. Fang, “, 24. Y.L. electric coupling 2e. physical. Therefore, we have carried out ZF-, The temperature dependence of the muon spin depolarization rate, C. Probing the nonuniform field distribution in the vortex state, In order to investigate the symmetry of the superconducting gap, we note that, To proceed with a quantitative analysis, we consider the local (London) approximation (, The results of this analysis are presented in, Even though a phonon-driven mechanism for superconductivity appears likely, and from there a conventional, In summary, we have reported on a detailed analysis of the electronic structure of the compound NaAlSi. Google Scholar, Lichtenberg, F., Catana, A., Mannhart, J., Schlom, D.G. 51, 341 (2000), Ambegaokar, V., Baratoff, A.: Phys. to render the operator gauge invariant. factor , . (Leipzig) 13 (3), 149 (2004), Maeno, Y., Kittaka, S., Nomura, T., Yonezawa, S., Ishida, K.: J. Phys. This is a preview of subscription content, log in to check access. Q. Wu, S. Zhang, H.-F. Song, M. Troyer, and A. endobj Phys. Chen, M.-W. Chu, R. Sankar, F. Chou, H.-T. Jeng, C.-S. Chang, and T.-M. Chuang, “, Superconducting topological surface states in the noncentrosymmetric bulk superconductor PbTaSe, 25. We use cookies to improve your website experience. Xu, I. Belopolski, N. Alidoust, M. Neupane, G. Bian, C. Zhang, R. Sankar, G. Chang, Z. Yuan, C.-C. Lee, Discovery of a Weyl fermion semimetal and topological Fermi arcs, 3. Soc. Selecting this option will search the current publication in context. It should be noted that, the Knight shift Δω/ωd in a metal is proportional to \({\varDelta } H/H = \frac {8 \pi }{3} <|u_{k}(0)|^{2}>_{E_{F}}{\chi _{e}^{S}} \) where uk(0) is the modulating function of the Bloch function, \(<...>_{E_{F}}\) is the average over the Fermi surface, and \({\chi _{e}^{S}}\) is the total spin susceptibility of the electrons (see ref.

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