2017
DOI: 10.1103/physrevb.96.205129
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Experimental evidence for topological surface states wrapping around a bulk SnTe crystal

Abstract: We demonstrate that the metallic topological surface states wrap on all sides the 3D topological crystalline insulator SnTe. This is achieved by studying oscillatory quantum magneto-transport and magnetization at tilted magnetic fields which enables us to observe simultaneous contributions from neighbouring sample sides. Taking into account pinning of the Fermi energy by the SnTe reservoir we successfully describe theoretically the de Haas-van Alphen oscillations of magnetization. The determined π-Berry phase … Show more

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Cited by 27 publications
(40 citation statements)
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“…3(a). A metallic behavior is observed for all Sn 1−x Mn x Te layers, in agreement with previous reports on Sn 1−x Mn x Te bulk crystals and thick films [43,44,48]. The absence of an increment of ρ xx for T <10 K indicates that the electronic ground state of the Mn doped TCI system SnTe is not insulating, in contrast to e.g.…”
Section: A Longitudinal Resistivity and Magnetoconductancesupporting
confidence: 91%
See 1 more Smart Citation
“…3(a). A metallic behavior is observed for all Sn 1−x Mn x Te layers, in agreement with previous reports on Sn 1−x Mn x Te bulk crystals and thick films [43,44,48]. The absence of an increment of ρ xx for T <10 K indicates that the electronic ground state of the Mn doped TCI system SnTe is not insulating, in contrast to e.g.…”
Section: A Longitudinal Resistivity and Magnetoconductancesupporting
confidence: 91%
“…As evidenced in Fig. 4(a), for the H ⊥ orientation, ∆σ of the reference SnTe layer presents around zero magnetic field an upward cusp: a fingerprint of weak antilocalization (WAL) due to the topological surface states (TSS) stabilized by the M symmetry in rocksalt SnTe(111) [48,50,75]. The WAL in the pristine SnTe layer points at the presence of massless DFs in the TSS at the (111) surface.…”
Section: A Longitudinal Resistivity and Magnetoconductancementioning
confidence: 94%
“…Thus, A, B and C may be found now as the appropriate coefficients of e ±ik0x as in Eq. (31). Explicitly, we have:…”
Section: πmentioning
confidence: 99%
“…Such systems include the 2D surface of a general 3D topological insulator. [25][26][27][28][29][30][31][32][33][34] In such cases, the low-energy electronic states possess linear dispersions and behave as massless Dirac fermions. When time reversal symmetry is broken by, e.g., a local magnetisation 28,35 or a magnetic field [35][36][37][38] then gaps open in the surface band structure.…”
Section: Introductionmentioning
confidence: 99%
“…{110} mirror-plane of rock-salt crystal structure and electronic band inversion of a corresponding bulk crystal. [4][5][6] The topological protection has been experimentally verified for two high symmetry surfaces of SnTe, namely {100} and {111}, first for {100} surfaces of bulk crystals, either after cleaving (in high vacuum) or for naturally grown crystal facets [7][8][9] and then for the respective surfaces of thin films grown by molecular beam epitaxy (MBE) 10,11 or other methods such as hot-wall epitaxy and e-beam evaporation. [12][13][14] With epitaxially grown crystalline layers it is possible to access the topologically protected states on surfaces which are not easy cleavage planes, only reachable when bulk crystals are used.…”
Section: Introductionmentioning
confidence: 99%