2014
DOI: 10.1103/physrevb.89.081106
|View full text |Cite
|
Sign up to set email alerts
|

Prediction of a Weyl semimetal inHg1xyCdxMny

Abstract: We study strained Hg1−x−yCdxMnyTe in a magnetic field using a k · p model and predict that the system is a Weyl semimetal with two nodes in an experimentally reasonable region of the phase diagram. We also predict two signatures of the Weyl semimetal phase which arise from tunability of the Weyl node splitting. First, we find that the Hall conductivity is proportional to the average Mn ion spin and thus is strongly temperature dependent. Second, we find an unusual magnetic field angle dependence of the Hall co… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

3
110
0

Year Published

2015
2015
2023
2023

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 142 publications
(113 citation statements)
references
References 24 publications
3
110
0
Order By: Relevance
“…Weyl and 3D Dirac semimetal phases have been predicted in a variety of existing or tailored systems as follows: (i) Pyrochlore iridates could host 24 Weyl nodes through the interplay of SOC and strong electron correlations (Wan et al 2011); (ii) Ferromagnetic HgCr2Se4 spinel with nodes protected by C4 point group symmetry (Xu, Weng, et al 2011;); (iii) Crystalline Cd3As2 (Wang, Weng, et al 2013) and A3Bi (A = Na, K, Rb) (Wang, Sun, et al 2012); (iv) β-cristobalite BiO2; (Young et al 2012) (v) strained Hg1-x-yCdxMnyTe under magnetic field (Bulmash, Liu, and Qi 2014); (vi) TlBiSe2 (Singh et al 2012); (vii) Heterostructure of magnetically doped 3D TI and normal insulator (Burkov and Balents 2011b); and, (viii) A superlattice of alternating layers with odd and even parity orbitals. Experimentally realized 3D Dirac semimetals so far are Cd3As2 Borisenko et al 2014;Ali et al 2014) and Na3Bi .…”
Section: Ivh Weyl and 3d Dirac Semimetalsmentioning
confidence: 99%
“…Weyl and 3D Dirac semimetal phases have been predicted in a variety of existing or tailored systems as follows: (i) Pyrochlore iridates could host 24 Weyl nodes through the interplay of SOC and strong electron correlations (Wan et al 2011); (ii) Ferromagnetic HgCr2Se4 spinel with nodes protected by C4 point group symmetry (Xu, Weng, et al 2011;); (iii) Crystalline Cd3As2 (Wang, Weng, et al 2013) and A3Bi (A = Na, K, Rb) (Wang, Sun, et al 2012); (iv) β-cristobalite BiO2; (Young et al 2012) (v) strained Hg1-x-yCdxMnyTe under magnetic field (Bulmash, Liu, and Qi 2014); (vi) TlBiSe2 (Singh et al 2012); (vii) Heterostructure of magnetically doped 3D TI and normal insulator (Burkov and Balents 2011b); and, (viii) A superlattice of alternating layers with odd and even parity orbitals. Experimentally realized 3D Dirac semimetals so far are Cd3As2 Borisenko et al 2014;Ali et al 2014) and Na3Bi .…”
Section: Ivh Weyl and 3d Dirac Semimetalsmentioning
confidence: 99%
“…Early theoretical proposals require either magnetic ordering in sufficiently large domains (3, 23-26) or fine-tuning of the chemical composition to within 5% in an alloy (23,(25)(26)(27), which proved demanding in real experiments. Recently, our group and a concurrent group successfully proposed the first, to our knowledge, experimentally feasible Weyl semimetal candidate in TaAs material class (28,29).…”
mentioning
confidence: 99%
“…Many theoretical proposals exist for realizing Weyl semimetals that possess interesting physical properties, such as discontinuous Fermi arcs and negative magnetoresistance due to the chiral anomaly. 4,[6][7][8][9][10][19][20][21][22][23][24][25][26][27][28][29]31,32,34 A Weyl node with definite chirality is associated with the Berry curvature and may be thought of as realizations of magnetic monopoles in momentum space.…”
Section: Introductionmentioning
confidence: 99%