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@INPROCEEDINGS{Nandi:1048975,
author = {Nandi, Shibabrata},
title = {{M}agnetic and {T}ransport {P}roperties of {M}n3{X} ({X} =
{G}e, {S}n) {W}eyl {S}emimetal},
reportid = {FZJ-2025-05070},
year = {2025},
abstract = {Topological quantum materials have garnered considerable
attention since their discovery, owing to the observed
anomalous transport properties that originate from their
non-zero Berry curvature. Mn3X compounds show interesting
physical properties like Anomalous Hall Effect (AHE), Planar
Hall effect (PHE), chiral magnetic effect, and non-local
transport properties due to non-vanishing Berry flux
emerging from the Weyl points1. It is widely believed that
the magnetic structure and Weyl properties are intimately
connected.However, the observation of negative longitudinal
magnetoresistance (LMR), AHE, and PHE in Mn3X compounds and
its connection with the chiral magnetic effect is much
debated in the literature. In this talk, I will give a brief
overview of the current understanding of the negative LMR,
AHE, and PHE as observed in Mn3Sn and Mn3Ge
compounds.References:[1] S. Nakatsuji, N. Kiyohara and T.
Higo, Nature (London) 527, 212 (2015)[2] Y. Song, Y. Hao,
and S. Wang, Phys. Rev. B 101, 144422 (2020) [3] A. K.
Nayak, J. E. Fischer, Y. Sun, B. Yan, J. Karel, A. C.
Komarek, C. Shekhar, N. Kumar, W. Schnelle, J. Kübler, C.
Felser, and S. S. P. Parkin, Sci. Adv. 2, e1501870 (2016)
[4] N. Kumar, S. N. Guin, C. Felser, and C. Shekhar, Phys.
Rev. B 98, 041103(R) (2018)},
organization = {(Digital) Institute Seminar JCNS-2,
Forschungszentrum Jülich, JCNS
(Germany)},
subtyp = {Invited},
cin = {JCNS-2 / JARA-FIT},
cid = {I:(DE-Juel1)JCNS-2-20110106 / $I:(DE-82)080009_20140620$},
pnm = {632 - Materials – Quantum, Complex and Functional
Materials (POF4-632) / 6G4 - Jülich Centre for Neutron
Research (JCNS) (FZJ) (POF4-6G4)},
pid = {G:(DE-HGF)POF4-632 / G:(DE-HGF)POF4-6G4},
typ = {PUB:(DE-HGF)31},
url = {https://juser.fz-juelich.de/record/1048975},
}