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A magnetic topological semimetal Sr1−yMn1−zSb2 (y, z < 0.1)
Weyl (WSMs) evolve from Dirac semimetals in the presence of broken time-reversal symmetry (TRS) or space-inversion symmetry. The WSM phases in TaAs-class materials and photonic crystals are due to the loss of space-inversion symmetry. For TRS-breaking WSMs, despite numerous theoretical and experimen...
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Published in: | Nature materials 2017-09, Vol.16 (9), p.905-910 |
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Main Authors: | , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | Weyl (WSMs) evolve from Dirac semimetals in the presence of broken time-reversal symmetry (TRS) or space-inversion symmetry. The WSM phases in TaAs-class materials and photonic crystals are due to the loss of space-inversion symmetry. For TRS-breaking WSMs, despite numerous theoretical and experimental efforts, few examples have been reported. In this Article, we report a new type of magnetic semimetal Sr
1−
y
Mn
1−
z
Sb
2
(
y
,
z
< 0.1) with nearly massless relativistic fermion behaviour (
m
∗
= 0.04 − 0.05
m
0
, where
m
0
is the free-electron mass). This material exhibits a ferromagnetic order for 304 K <
T
< 565 K, but a canted antiferromagnetic order with a ferromagnetic component for
T
< 304 K. The combination of relativistic fermion behaviour and ferromagnetism in Sr
1−
y
Mn
1−
z
Sb
2
offers a rare opportunity to investigate the interplay between relativistic fermions and spontaneous TRS breaking.
Sr
1−
y
Mn
1−
z
Sb
2
(
y
,
z
< 0.1) is reported to be a magnetic topological semimetal exhibiting nearly massless relativistic fermions. |
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ISSN: | 1476-1122 1476-4660 |
DOI: | 10.1038/nmat4953 |