TY - JOUR
T1 - Polar Layered Magnet Ba2Cu3(SeO3)4F2 Composed of Bitriangular Chains
T2 - Observation of 1/3-Magnetization Plateau
AU - Yalikun, Alimujiang
AU - Wang, Yanhong
AU - Shi, Nian
AU - Chen, Yiwen
AU - Huang, Hao
AU - Koo, Hyun Joo
AU - Ouyang, Zhongwen
AU - Xia, Zhengcai
AU - Kremer, Reinhard K.
AU - Whangbo, Myung Hwan
AU - Lu, Hongcheng
N1 - Publisher Copyright:
© 2024 American Chemical Society
PY - 2024
Y1 - 2024
N2 - We prepared a new polar layered quantum magnet Ba2Cu3(SeO3)4F2, by a combined use of F- and pyramidal SeO32- anions, determined its crystal structure by X-ray diffraction, and characterized its magnetic properties by magnetization, electron spin resonance (ESR) and specific heat measurements, and by density functional theory calculations. The title compound has first experimentally reported bitriangular chains of Cu2+ ions aligned along the b direction to form layers parallel to the ab plane, and these layers are separated by Ba2+ ions. The magnetic susceptibility data reveal that, despite strong predominant antiferromagnetic intrachain interactions indicated by the large negative Weiss temperature θ of −143.9 K within bitriangular chains, no long-range order occurs down to 2 K. The latter, further confirmed by the specific heat measurements, is attributed to the extremely weak interlayer interaction. The spins in each bitriangular chain become ferrimagnetically ordered to exhibit a 1/3-magnetization plateau, which persists at least up to 30 T. This reveals that each bitriangular chain acts as an S = 1/2 entity at low temperatures, as observed from the decrease of the effective magnetic moment Peff from 3.67 μB in the high temperature range to 1.89 μB in the low temperature range, equivalently, from three free Cu2+ ions to only one effective Cu2+ ion per formula unit. In each layer of Ba2Cu3(SeO3)4F2, the interaction between adjacent ferrimagnetic chains is ferromagnetic rather than antiferromagnetic, contrary to the observations in other reported cases.
AB - We prepared a new polar layered quantum magnet Ba2Cu3(SeO3)4F2, by a combined use of F- and pyramidal SeO32- anions, determined its crystal structure by X-ray diffraction, and characterized its magnetic properties by magnetization, electron spin resonance (ESR) and specific heat measurements, and by density functional theory calculations. The title compound has first experimentally reported bitriangular chains of Cu2+ ions aligned along the b direction to form layers parallel to the ab plane, and these layers are separated by Ba2+ ions. The magnetic susceptibility data reveal that, despite strong predominant antiferromagnetic intrachain interactions indicated by the large negative Weiss temperature θ of −143.9 K within bitriangular chains, no long-range order occurs down to 2 K. The latter, further confirmed by the specific heat measurements, is attributed to the extremely weak interlayer interaction. The spins in each bitriangular chain become ferrimagnetically ordered to exhibit a 1/3-magnetization plateau, which persists at least up to 30 T. This reveals that each bitriangular chain acts as an S = 1/2 entity at low temperatures, as observed from the decrease of the effective magnetic moment Peff from 3.67 μB in the high temperature range to 1.89 μB in the low temperature range, equivalently, from three free Cu2+ ions to only one effective Cu2+ ion per formula unit. In each layer of Ba2Cu3(SeO3)4F2, the interaction between adjacent ferrimagnetic chains is ferromagnetic rather than antiferromagnetic, contrary to the observations in other reported cases.
UR - http://www.scopus.com/inward/record.url?scp=85201154131&partnerID=8YFLogxK
U2 - 10.1021/acs.chemmater.4c01294
DO - 10.1021/acs.chemmater.4c01294
M3 - Article
AN - SCOPUS:85201154131
SN - 0897-4756
JO - Chemistry of Materials
JF - Chemistry of Materials
ER -