TY - JOUR
T1 - Mössbauer study of rare-earth ferroborate NdFe3(BO3)4
AU - Nakamura, Shin
AU - Masuda, Takatsugu
AU - Ohgushi, Kenya
AU - Katsufuji, Takuro
N1 - Funding Information:
Acknowledgements The experiments using 57Fe Mössbauer spectroscopy were performed at the Joint Research Center for Environmentally Conscious Technologies in Materials Science at ZAIKEN, Waseda University. This work was financially supported by JSPS KAKENHI, Grant Nos. JP19H05823, JP19H05822, JP19K21837, and JP18H01159.
Funding Information:
The experiments using 57Fe M?ssbauer spectroscopy were performed at the Joint Research Center for Environmentally Conscious Technologies in Materials Science at ZAIKEN, Waseda University. This work was financially supported by JSPS KAKENHI, Grant Nos. JP19H05823, JP19H05822, JP19K21837, and JP18H01159.
Publisher Copyright:
© 2020 The Physical Society of Japan
PY - 2020
Y1 - 2020
N2 - An 57Fe Mössbauer spectroscopic study has been conducted on the single-crystal NdFe3(BO3)4 to investigate its magnetic structure and multiferroicity. In the multiferroic state below the Néel temperature TN = 29 K, the magnitude of the quadrupole coupling constant e2qQ=2 becomes smaller than that in the paramagnetic phase. The decrease is explained by the spin-orbit coupling due to the simultaneous order of Fe3+ and Nd3+ moments, which intensifies the 4 f-3d hybridization. This is consistent with the d-p hybridization mechanism as the origin of the multiferroicity. Although the commensurate antiferromagnetic order along the a-axis is confirmed at 25 K, the pronounced incommensurate order is not recognized at 4.2 K. In the latter, it is probable that the Fe3+ moments are distributed only around the a-axis, such as within the ±10° region, or that they are fluctuating or frustrating, within the c-plane dynamically with the relaxation time of, for example, 10−9 s.
AB - An 57Fe Mössbauer spectroscopic study has been conducted on the single-crystal NdFe3(BO3)4 to investigate its magnetic structure and multiferroicity. In the multiferroic state below the Néel temperature TN = 29 K, the magnitude of the quadrupole coupling constant e2qQ=2 becomes smaller than that in the paramagnetic phase. The decrease is explained by the spin-orbit coupling due to the simultaneous order of Fe3+ and Nd3+ moments, which intensifies the 4 f-3d hybridization. This is consistent with the d-p hybridization mechanism as the origin of the multiferroicity. Although the commensurate antiferromagnetic order along the a-axis is confirmed at 25 K, the pronounced incommensurate order is not recognized at 4.2 K. In the latter, it is probable that the Fe3+ moments are distributed only around the a-axis, such as within the ±10° region, or that they are fluctuating or frustrating, within the c-plane dynamically with the relaxation time of, for example, 10−9 s.
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U2 - 10.7566/JPSJ.89.084703
DO - 10.7566/JPSJ.89.084703
M3 - Article
AN - SCOPUS:85093895139
SN - 0031-9015
VL - 89
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 8
M1 - 084703
ER -