TY - JOUR
T1 - Improvement of Large Anomalous Hall Effect in Polycrystalline Antiferromagnetic Mn3+xSn Thin Films
AU - Ikeda, Tomoki
AU - Tsunoda, Masakiyo
AU - Oogane, Mikihiko
AU - Oh, Seungjun
AU - Morita, Tadashi
AU - Ando, Yasuo
PY - 2019/7
Y1 - 2019/7
N2 - In order to improve the large anomalous Hall effect (AHE) in Mn3Sn thin films, we eliminated the co-existing Mn2Sn phase in the films by changing the composition; 50 nm thick polycrystalline Mn3+xSn thin films were fabricated on Si/SiO2 substrates by the sputtering method followed by a thermal annealing process in vacuum. The film compositions were Mn70Sn30(sample-A), Mn75Sn25(sample-B), and Mn80Sn20(sample-C) in as-deposited state and were slightly changed to be Mn75Sn25(sample-A), Mn77Sn23(sample-B), and Mn78Sn22(sample-C), respectively, after the annealing at 500 °C. From a structural analysis by X-ray diffractometry, the sample-C was considered to crystallize to Mn3Sn phase without passing the crystallization of Mn2Sn phase at 300 °C, differently from the sample-A. The saturation magnetization, $M-{\mathrm {S}}$, of the sample-A significantly increased below 250 K, corresponding with the Curie temperature of Mn2Sn. On the other hand, $M-{\mathrm {S}}$ did not show significant changes with cooling temperature in the samples-B and-C. An AHE was observed at the room temperature in all the samples. The anomalous Hall conductivity, $\sigma-{\mathrm {AH}}$, at the room temperature increased in magnitude, as the content of Mn increased. The sign of $\sigma-{\mathrm {AH}}$ changed from negative to positive in the sample-A with cooling temperature. On the other hand, the sign remained negative in the sample-C. These differences might be due to the elimination of co-existing Mn2Sn phase in the Mn3Sn thin films with enlarging the Mn content from the stoichiometry. Consequently, we successfully improved the large AHE in polycrystalline antiferromagnetic Mn3Sn thin films.
AB - In order to improve the large anomalous Hall effect (AHE) in Mn3Sn thin films, we eliminated the co-existing Mn2Sn phase in the films by changing the composition; 50 nm thick polycrystalline Mn3+xSn thin films were fabricated on Si/SiO2 substrates by the sputtering method followed by a thermal annealing process in vacuum. The film compositions were Mn70Sn30(sample-A), Mn75Sn25(sample-B), and Mn80Sn20(sample-C) in as-deposited state and were slightly changed to be Mn75Sn25(sample-A), Mn77Sn23(sample-B), and Mn78Sn22(sample-C), respectively, after the annealing at 500 °C. From a structural analysis by X-ray diffractometry, the sample-C was considered to crystallize to Mn3Sn phase without passing the crystallization of Mn2Sn phase at 300 °C, differently from the sample-A. The saturation magnetization, $M-{\mathrm {S}}$, of the sample-A significantly increased below 250 K, corresponding with the Curie temperature of Mn2Sn. On the other hand, $M-{\mathrm {S}}$ did not show significant changes with cooling temperature in the samples-B and-C. An AHE was observed at the room temperature in all the samples. The anomalous Hall conductivity, $\sigma-{\mathrm {AH}}$, at the room temperature increased in magnitude, as the content of Mn increased. The sign of $\sigma-{\mathrm {AH}}$ changed from negative to positive in the sample-A with cooling temperature. On the other hand, the sign remained negative in the sample-C. These differences might be due to the elimination of co-existing Mn2Sn phase in the Mn3Sn thin films with enlarging the Mn content from the stoichiometry. Consequently, we successfully improved the large AHE in polycrystalline antiferromagnetic Mn3Sn thin films.
KW - Anomalous Hall effect (AHE)
KW - Berry-phase
KW - antiferromagnetic materials
KW - kagome lattice
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U2 - 10.1109/TMAG.2019.2899223
DO - 10.1109/TMAG.2019.2899223
M3 - Article
AN - SCOPUS:85067851167
VL - 55
JO - IEEE Transactions on Magnetics
JF - IEEE Transactions on Magnetics
SN - 0018-9464
IS - 7
M1 - 8672635
ER -