2014
DOI: 10.1063/1.4900486
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Systematic study of doping dependence on linear magnetoresistance in p-PbTe

Abstract: Articles you may be interested in Effect of pressure on the parameters of the superconducting transition in In-doped Pb z Sn1− z Te semiconducting solid solutions Low Temp.

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Cited by 7 publications
(3 citation statements)
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“…[ 52 ] However, the large MR commonly accompanying with intense SdH oscillations at high fields is not ideal for magento‐electric sensing and not beneficial for the applications of topological semimetals single crystals. The MR of single‐crystalline film of PbTe [ 63 ] and Bi 2 Te 3 [ 64 ] is relatively lower due to their lower μ. In addition, polycrystalline materials generally own a much lower MR of 10 1 %–10 3 % than that of single‐crystalline materials, which is due to their rather lower μ of ≈10 3 cm 2 V –1 s –1 or smaller.…”
Section: Resultsmentioning
confidence: 99%
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“…[ 52 ] However, the large MR commonly accompanying with intense SdH oscillations at high fields is not ideal for magento‐electric sensing and not beneficial for the applications of topological semimetals single crystals. The MR of single‐crystalline film of PbTe [ 63 ] and Bi 2 Te 3 [ 64 ] is relatively lower due to their lower μ. In addition, polycrystalline materials generally own a much lower MR of 10 1 %–10 3 % than that of single‐crystalline materials, which is due to their rather lower μ of ≈10 3 cm 2 V –1 s –1 or smaller.…”
Section: Resultsmentioning
confidence: 99%
“…[61,62] The Quantum LMR is usually observed in singlecrystalline bulks and films, whereby all electrons occupy the lowest Landau level in the quantum limit. The linear MR in single crystals of Dirac semimetals of Cd 3 As 2 , [50] LaSb [49] and Na 3 Bi [53] as well as in single-crystalline films of PbTe [63] and Bi 2 Te 3 [64] is categorized as Quantum LMR, which, however, is not applied to polycrystalline NbP 1+x . The classical LMR is discovered in a disordered system, in which macroscopic inhomogeneities create distorted current paths misaligned with the applied voltage at large B, and thus contribute the Hall resistance (ρ yx ∝ B) to the effective MR. [61,62] Many polycrystalline samples are suitable for the classical LMR model, including Ag 2 Se, [65] mosaic-like bilayer graphene, [66] Bi 2 O 2 Se, [67] InSb, [68] and so on.…”
Section: Carrier Transport By Two-bands Model and Unsaturated Quasi-l...mentioning
confidence: 99%
“…However, this simple picture is known to fail in numerous cases. Non-saturating linear TMR has been observed in electronic systems ranging from potassium [1], to doped silicon [2], 2D electron gas system [3], 3D doped semi-conductors and Dirac materials [4][5][6][7][8][9][10][11], density wave materials [12], or correlated materials [13]. LMR, one order of magnitude smaller (than and with an opposite sign to) its transverse counterpart has been observed in silver chalcogenides [5] and topological materials [14,15].…”
mentioning
confidence: 99%