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The differential magnetic relaxation behaviours of slightly distorted triangular dodecahedral dysprosium analogues in a type of cyano-bridged 3d–4f zig-zag chain compounds.

Authors :
Xue, An-Qi
Liu, Yang-Yu
Li, Jia-Xin
Zhang, Yan
Meng, Yin-Shan
Zhu, Wen-Hua
Zhang, Yi-Quan
Sun, Hao-Ling
Wang, Fei
Qiu, Guan-Xia
Liang, Lu-Yu
Wang, Xiang
Gao, Song
Source :
Dalton Transactions: An International Journal of Inorganic Chemistry; 5/28/2020, Vol. 49 Issue 20, p6867-6875, 9p
Publication Year :
2020

Abstract

A class of cyano-bridged 3d–4f zig-zag chain compounds, {RE[TM(CN)<subscript>6</subscript>] (PNO)<subscript>2</subscript>(H<subscript>2</subscript>O)<subscript>4</subscript>}·(H<subscript>2</subscript>O) {RE = Y<superscript>III</superscript>, TM = [Fe<superscript>III</superscript>]<subscript>LS</subscript> (1); RE = Dy<superscript>III</superscript>, TM = [Fe<superscript>III</superscript>]<subscript>LS</subscript> (2), Co<superscript>III</superscript> (3)}, have been synthesized and characterized by single-crystal X-ray diffraction. The rare earth ions in these compounds are situated in a slightly distorted triangular dodecahedral (D<subscript>2d</subscript>) coordination environment. The magnetic properties of compounds 1–3 have been comparatively studied in detail. Under a zero dc field, the temperature dependence of ac susceptibility measurements for YFe (1) indicates the absence of magnetic relaxation stemming from the single anisotropic [Fe<superscript>III</superscript>]<subscript>LS</subscript> ion. The dysprosium analogue DyFe (2) shows only magnetic relaxation behavior with a prominent QTM effect, while DyCo (3) exhibits SIM properties not completely covered by QTM, with an extracted energy barrier of 73 K under a zero dc field. The ab initio calculations indicate that both compounds 2 and 3 are SMMs with well-behaved magnetic relaxation properties primarily from the individual Dy<superscript>III</superscript> ion. Therefore, the different magnetic behaviors exhibited by compound 2 compared to 3 may be ascribed to the stronger QTM effect caused by the extra weak interaction of [Fe<superscript>III</superscript>]<subscript>LS</subscript> ions in 2 as a fluctuating transverse field around the Dy<superscript>III</superscript> ion. The QTM effect for both 2 and 3 is suppressed under an applied dc field with an effective energy barrier of 134 and 150 K, respectively. Compared with compound 2, the higher extracted U<subscript>eff</subscript>/k<subscript>B</subscript> and χ′′(T) peak temperature for 3 should be further attributed to its slightly higher single-ion axiality as calculated and the elimination of the transverse field from the [Fe<superscript>III</superscript>]<subscript>LS</subscript> ion. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
14779226
Volume :
49
Issue :
20
Database :
Complementary Index
Journal :
Dalton Transactions: An International Journal of Inorganic Chemistry
Publication Type :
Academic Journal
Accession number :
143440378
Full Text :
https://doi.org/10.1039/d0dt00990c