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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
Main Authors: Liu, J. Y., Hu, J., Zhang, Q., Graf, D., Cao, H. B., Radmanesh, S. M. A., Adams, D. J., Zhu, Y. L., Cheng, G. F., Liu, X., Phelan, W. A., Wei, J., Jaime, M., Balakirev, F., Tennant, D. A., DiTusa, J. F., Chiorescu, I., Spinu, L., Mao, Z. Q.
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creator Liu, J. Y.
Hu, J.
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Radmanesh, S. M. A.
Adams, D. J.
Zhu, Y. L.
Cheng, G. F.
Liu, X.
Phelan, W. A.
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Spinu, L.
Mao, Z. Q.
description 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.
doi_str_mv 10.1038/nmat4953
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Y. ; Hu, J. ; Zhang, Q. ; Graf, D. ; Cao, H. B. ; Radmanesh, S. M. A. ; Adams, D. J. ; Zhu, Y. L. ; Cheng, G. F. ; Liu, X. ; Phelan, W. A. ; Wei, J. ; Jaime, M. ; Balakirev, F. ; Tennant, D. A. ; DiTusa, J. F. ; Chiorescu, I. ; Spinu, L. ; Mao, Z. Q.</creator><creatorcontrib>Liu, J. Y. ; Hu, J. ; Zhang, Q. ; Graf, D. ; Cao, H. B. ; Radmanesh, S. M. A. ; Adams, D. J. ; Zhu, Y. L. ; Cheng, G. F. ; Liu, X. ; Phelan, W. A. ; Wei, J. ; Jaime, M. ; Balakirev, F. ; Tennant, D. A. ; DiTusa, J. F. ; Chiorescu, I. ; Spinu, L. ; Mao, Z. Q. ; Los Alamos National Laboratory (LANL), Los Alamos, NM (United States) ; Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)</creatorcontrib><description>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. 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In this Article, we report a new type of magnetic semimetal Sr 1− y Mn 1− z Sb 2 ( y , z &lt; 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 &lt; T &lt; 565 K, but a canted antiferromagnetic order with a ferromagnetic component for T &lt; 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. 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subjects 639/301/119/995
639/766/119/997
Antiferromagnetism
Biomaterials
Breaking
Condensed Matter Physics
Crystals
Electron mass
Fermions
Ferromagnetic materials
High Magnetic Field Science
Magnetic fields
MATERIALS SCIENCE
Metalloids
Metals
Nanotechnology
Optical and Electronic Materials
Photonic crystals
Relativism
Symmetry
Topology
title A magnetic topological semimetal Sr1−yMn1−zSb2 (y, z < 0.1)
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