APS March Meeting 2017
Volume 62, Number 4
Monday–Friday, March 13–17, 2017;
New Orleans, Louisiana
Session L23: Interplay of Magnetism, Superconductivity and Unconventional Order in Heavy Fermion Materials
11:15 AM–2:15 PM,
Wednesday, March 15, 2017
Room: New Orleans Theater B
Sponsoring
Unit:
GMAG
Chair: Pengcheng Dai, pdai.utk@gmail.com
Abstract ID: BAPS.2017.MAR.L23.4
Abstract: L23.00004 : Topological nodal superconductivity in the heavy fermion metal UPt3*
1:03 PM–1:39 PM
Preview Abstract
Abstract
Author:
Andriy Nevidomskyy
(Rice University)
The concept of topological states of matter has captured the imagination of physicists in the last decade. Traditionally, such topological phases are predicted to occur in fully gapped insulating or superconducting materials and are characterized by topologically protected gapless excitations on the surface [1]. Recently, it has been realized that such protected surface states may also exist in certain classes of metallic materials with gapless bulk excitations. Here, I will demonstrate the application of this concept, focusing in particular on the low-temperature B-phase of the heavy fermion superconductor UPt$_3$. Josephson interferometry measurements provide strong evidence for the triplet, chiral pairing symmetry in UPt$_3$, which endow the Cooper pairs with orbital angular momentum $L_z =\pm 2$ along the $c$-axis [2]. Such pairing supports both line and point nodes in the superconducting gap, and we show that both types of nodal quasiparticles possess nontrivial topology in the momentum space. In particular, the point nodes located at the intersections of the closed Fermi surfaces with the $c$-axis act as the double monopoles and anti-monopoles of the Berry curvature [3]. Consequently, we predict that the B phase of UPt$_3$ should support an anomalous thermal Hall effect, various magneto-electric effects such as the polar Kerr effect, in addition to the topologically protected Majorana Fermi arcs on the (1,0,0) and (0,1,0) surfaces [3]. At the transition from the B-phase to the A-phase upon increasing temperature, the time reversal symmetry is restored, and the surface Fermi arcs disappear. The effect of quenched disorder on the topologically non-trivial B-phase will also be discussed.\vspace{3mm}
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References:\\
{[1]} M. Z. Hasan and C. L. Kane, "Colloquium: Topological insulators," Rev. Mod. Phys. 82, 3045 (2010).\\
{[2]} J. D. Strand, D. J. Van Harlingen, J. B. Kycia, and W. P. Halperin, "Evidence for complex superconducting order parameter symmetry in the low-temperature phase of UPt$_3$ from Josephson interferometry", Phys. Rev. Lett. 103, 197002 (2009).\\
{[3]} P. Goswami and A. H. Nevidomskyy "Topological Weyl superconductor to diffusive thermal Hall metal crossover in the B-phase of UPt$_3$", Phys. Rev. B 92, 214504 (2015).
*This research is supported by NSF grant no. DMR-1350237
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2017.MAR.L23.4