Abstract
Motivated by the experimental detection of superconductivity in the low-carrier density half-Heusler compound YPtBi, we study the pairing instabilities of three-dimensional strongly spin-orbit coupled semimetals with a quadratic band touching point. In these semimetals the electronic structure at the Fermi energy is described by spin j=32 quasiparticles, which are fundamentally different from those in ordinary metals with spin j=12. For both local and nonlocal pairing channels in j=32 materials we develop a general approach to analyzing pairing instabilities, thereby providing the computational tools needed to investigate the physics of these systems beyond phenomenological considerations. Furthermore, applying our method to a generic density-density interaction, we establish that: (i) The pairing strengths in the different symmetry channels uniquely encode the j=32 nature of the Fermi surface band structure - a manifestation of the fundamental difference with ordinary metals. (ii) The leading odd-parity pairing instabilities are different for electron doping and hole doping. Finally, we argue that polar phonons, i.e., Coulomb interactions mediated by the long-ranged electric polarization of the optical phonon modes, provide a coupling strength large enough to account for a Kelvin-range transition temperature in the s-wave channel, and are likely to play an important role in the overall attraction in non-s-wave channels. Moreover, the explicit calculation of the coupling strengths allows us to conclude that the two largest non-s-wave contributions occur in nonlocal channels, in contrast with what has been commonly assumed.
| Original language | English |
|---|---|
| Article number | 214514 |
| Journal | Physical Review B |
| Volume | 96 |
| Issue number | 21 |
| DOIs | |
| State | Published - 28 Dec 2017 |
| Externally published | Yes |
Bibliographical note
Publisher Copyright:© 2017 American Physical Society.
Funding
We thank Leon Balents, Max Metlitski, and Doug Scalapino for useful discussions. L.S. also acknowledges Leon Balents and Eun-Gook Moon for a prior collaboration on a related topic. L.S. and J.R. were supported by the Gordon and Betty Moore Foundation through scholarships of the EPiQS initiative under Grant No. GBMF4303. L.S. also acknowledges the hospitality of the KITP, where part of this work was carried out, and NSF Grant PHY-1125915. P.A.L. was supported by the DOE under Grant No. FG02-03ER46076. L.F. and J.W.F.V. acknowledge funding by the DOE Office of Basic Energy Sciences, Division of Materials Sciences and Engineering under Award No. DE-SC0010526.
| Funders | Funder number |
|---|---|
| DOE Office of Basic Energy Sciences | |
| National Science Foundation | PHY-1125915 |
| U.S. Department of Energy | |
| Directorate for Mathematical and Physical Sciences | 1125915 |
| Gordon and Betty Moore Foundation | |
| Division of Materials Sciences and Engineering |