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Slow magnetic relaxation of mononuclear complexes based on uncommon Kramers lanthanide ions CeIII, SmIII and Yb III
被引:6
|作者:
Leng, Ji-Dong
[1
,2
]
Hua, Qiu-Yan
[1
,2
]
Liu, Wen-Ting
[3
]
Tao, Ze-Xian
[1
,2
]
Tan, Nai-Wen
[1
,2
]
Wang, Yu-Fei
[1
,2
]
Lin, Wei-Quan
[1
,2
]
机构:
[1] Guangzhou Univ, Sch Chem & Chem Engn, Guangzhou Higher Educ Mega Ctr, 230 Wai Huan Xi Rd, Guangzhou 510006, Peoples R China
[2] Guangzhou Univ, Inst Clean Energy & Mat, Guangzhou Higher Educ Mega Ctr, 230 Wai Huan Xi Rd, Guangzhou 510006, Peoples R China
[3] Guangdong Univ Educ, Sch Chem & Mat Sci, Guangzhou 510303, Peoples R China
关键词:
MOLECULAR MATERIALS;
BLOCKING;
ANISOTROPY;
EXCHANGE;
D O I:
10.1039/d2dt00766e
中图分类号:
O61 [无机化学];
学科分类号:
070301 ;
081704 ;
摘要:
Based on the uncommon Kramers ions Ce-III, Sm-III and Yb-III, complexes [Ce(dppbO(2))(2)Cl-3] (1, dppbO(2) = 1,2-bis(diphenylphosphino)benzene dioxide), [Sm(dppbO(2))(2)Cl-3] (2) and [Yb(dppbO(2))(2)Cl-2]Cl (3) toward single-ion magnets were obtained and fully characterized. Complexes 1 and 2 are isostructural seven-coordinate with distorted geometries between a capped trigonal prism and a capped octahedron, while 3 is six-coordinate with an octahedral geometry. Dynamic magnetic property measurements reveal their field induced slow magnetic relaxation behaviours. Fits to the temperature dependent relaxation time (tau) result in effective barriers of 38(2), 11.7(2) and 20.2(6) cm(-1) for 1, 2 and 3, respectively, as well as relatively low Raman exponents (3.4(2) for 1 and 2.1(1) for 3). Ab initio calculations were then performed and they indicated that the first excited Kramers doublets (KDs) for 1, 2 and 3 lie at ca. 291, 63.5 and 137 cm(-1), respectively, which are much higher than the fitting results. Combining the significant transverse magnetic moments between the ground state KDs and the first excited KDs, we thus attribute the dominant relaxation pathway of the three compounds to a Raman process, while quantum tunnelling of magnetization and direct relaxation processes may coexist. In this case, the obtained effective barriers in a high temperature region for 1 and 3 are actually the energies of the vibrational modes, which lead to second-order Raman processes with exponential temperature dependence.
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页码:12661 / 12669
页数:9
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