2020/07/27 by Young-Joon Song, K. -W. Lee, Kwan-Woo Lee · 9 citations
Physics and Astronomy · #Advanced Condensed Matter Physics #Band gap #Condensed matter physics #Dirac (video compression format) #Ferromagnetism #Neutrino #Physics #Physics of Superconductivity and Magnetism #Quantum mechanics #Semimetal #Topological Materials and Phenomena #Weyl semimetal #cond-mat.mtrl-sci #cond-mat.str-el
paper · pdf · doi:10.1103/physrevb.102.035155
published in Physical review. B./Physical review. B 102(3) (American Physical Society) · 10 pages with 9 embedded figures (mirror corrections)
openalex publication_date 2020/07/27 · arxiv created 2020/07/28 · arxiv updated 2020/07/29 · openalex created_date 2020/08/03 · openalex updated_date 2026/08/05
Using both an effective three-band model and ab initio calculations, we have investigated various topological features in the cubic ferromagnetic 5d1,2 systems showing large spin-orbit coupling (SOC): Ba2NaOsO6, Sr2SrOsO6, and Ba2BReO6 (B=Mg, Zn). In the presence of time-reversal symmetry (T), spinless Dirac nodal loops linked to each other at the W points appear in the mirror planes. Remarkably, breaking T leads to spinful magnetic Weyl nodal loops (MWNLs) that are robust even at large SOC and correlation strength U variation due to the combination of mirror symmetry and broken T. Additionally, there are two types of magnetic Weyl points with chiral charges |\ensuremathχ|=1,2 along the C4v symmetry line, and another type-II MWNL encircling the zone center, that are dependent on U. Furthermore, the ferromagnetic Ba2ZnReO6 is an ideal half semimetal with MWNLs and magnetic Weyl nodes at the Fermi level without the interference of topologically trivial bulk states. These systems give rise to a remarkably large anomalous Hall conductivity \ensuremathσxy of up to 1160 (\mathrm\ensuremathΩ\phantom\rule0.16em0excm)^\ensuremath-1. Our findings may apply widely for t2g systems with cubic (or slightly distorted) fcc-like structures.