2016
DOI: 10.1038/srep27294
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Anomalous electronic structure and magnetoresistance in TaAs2

Abstract: The change in resistance of a material in a magnetic field reflects its electronic state. In metals with weakly- or non-interacting electrons, the resistance typically increases upon the application of a magnetic field. In contrast, negative magnetoresistance may appear under some circumstances, e.g., in metals with anisotropic Fermi surfaces or with spin-disorder scattering and semimetals with Dirac or Weyl electronic structures. Here we show that the non-magnetic semimetal TaAs2 possesses a very large negati… Show more

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Cited by 90 publications
(95 citation statements)
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“…Negative magnetoresistance has been observed experimentally for NbAs 2 [17,18], TaAs 2 [17] and TaSb 2 [17,20]. Anomalous, albeit not negative, magnetoresistance has been observed for NbSb 2 [12] and TaAs 2 [15]. However, there are also experiments which point to the opposite, which is that there is no negative magnetoresistance in these materials.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Negative magnetoresistance has been observed experimentally for NbAs 2 [17,18], TaAs 2 [17] and TaSb 2 [17,20]. Anomalous, albeit not negative, magnetoresistance has been observed for NbSb 2 [12] and TaAs 2 [15]. However, there are also experiments which point to the opposite, which is that there is no negative magnetoresistance in these materials.…”
Section: Introductionmentioning
confidence: 99%
“…This effect could be of help in the search for an explanation of the anomalous magnetoresistance in these materials. Recently, transition metal dipnictides of the type AB 2 (A ä{Ta, Nb}, B ä{As, Sb}) have gained a lot of attention [12][13][14][15][16][17][18][19] for their giant magnetoresistance. These materials are semimetals, but without a direct closure of the band gap.…”
mentioning
confidence: 99%
“…However, a negative longitudinal MR was also observed in other materials: semimetals without Weyl nodes near the Fermi energy, e.g. in MPn 2 (M=Nb, Ta; Pn=As, Sb) [34][35][36][37], the zero band-gap semiconductor GdPtBi [38], and in layered metals with a large quasi twodimensional Fermi surface, such as the highly conductive delafossites PdCoO 2 and PtCoO 2 and the ruthenate Sr 2 RuO 4 [39]. In all these materials a magnetic field induces a strong enhancement of the resistance anisotropy r r = A xx zz .…”
Section: Introductionmentioning
confidence: 99%
“…The calculation also shows that Nb(Ta)As 2 and NbSb 2 are close to the compensated semimetals with equal electron and hole densities. Both the electron and hole bands are weakly topological, leading to a fragile surface state [57].…”
Section: Bulk and Surface Electron Statesmentioning
confidence: 99%
“…Luo et al reported that the LMR of TaAs 2 reaches an extremely large number (−98%) in 3 T at 2 K, which persists up to 150 K [57] [ Fig. 8(d)].…”
Section: Negative Longitudinal Magnetoresistancementioning
confidence: 99%