TY - JOUR
T1 - Magnetoresistance and anomalous Hall effect of reactive sputtered polycrystalline Ti1 - XCrxN films
AU - Duan, Xiaofei
AU - Mi, Wenbo
AU - Guo, Zaibing
AU - Bai, Haili
N1 - KAUST Repository Item: Exported on 2020-10-01
Acknowledgements: This work was supported by the National Natural Science Foundation of China (51171126) and the Key Project of the Natural Science Foundation of Tianjin City (12JCZDJC27100).
PY - 2013/9
Y1 - 2013/9
N2 - The reactive-sputtered polycrystalline Ti1 - xCrxN films with 0.17 ≤ x ≤ 0.51 are ferromagnetic and at x = 0.47 the Curie temperature TC shows a maximum of ~ 120 K. The films are metallic at 0 ≤ x ≤ 0.47, while the films with x = 0.51 and 0.78 are semiconducting-like. The upturn of resistivity below 70 K observed in the films with 0.10 ≤ x ≤ 0.47 is from the effects of the electron-electron interaction and weak localization. The negative magnetoresistance (MR) of the films with 0.10 ≤ x ≤ 0.51 is dominated by the double-exchange interaction, while at x = 0.78, MR is related to the localized magnetic moment scattering at the grain boundaries. The scaling ρxyA/n ∝ ρxx2.19 suggests that the anomalous Hall effect in the polycrystalline Ti1 - xCrxN films is scattering-independent. © 2013 Elsevier B.V. All rights reserved.
AB - The reactive-sputtered polycrystalline Ti1 - xCrxN films with 0.17 ≤ x ≤ 0.51 are ferromagnetic and at x = 0.47 the Curie temperature TC shows a maximum of ~ 120 K. The films are metallic at 0 ≤ x ≤ 0.47, while the films with x = 0.51 and 0.78 are semiconducting-like. The upturn of resistivity below 70 K observed in the films with 0.10 ≤ x ≤ 0.47 is from the effects of the electron-electron interaction and weak localization. The negative magnetoresistance (MR) of the films with 0.10 ≤ x ≤ 0.51 is dominated by the double-exchange interaction, while at x = 0.78, MR is related to the localized magnetic moment scattering at the grain boundaries. The scaling ρxyA/n ∝ ρxx2.19 suggests that the anomalous Hall effect in the polycrystalline Ti1 - xCrxN films is scattering-independent. © 2013 Elsevier B.V. All rights reserved.
UR - http://hdl.handle.net/10754/562934
UR - https://linkinghub.elsevier.com/retrieve/pii/S0040609013011206
UR - http://www.scopus.com/inward/record.url?scp=84881311534&partnerID=8YFLogxK
U2 - 10.1016/j.tsf.2013.06.068
DO - 10.1016/j.tsf.2013.06.068
M3 - Article
SN - 0040-6090
VL - 542
SP - 348
EP - 354
JO - Thin Solid Films
JF - Thin Solid Films
ER -