Tuning of magnetic frustration in S=1/2 Kagome lattices {[Cu3(CO3)2(bPe)3](CLO4)2}n and {[Cu3(CO3)2(bPY)3](CLO4)2}n through rigid and flexible ligands
Tuning of magnetic frustration in S=1/2 Kagome lattices {[Cu3(CO3)2(bPe)3](CLO4)2}n and {[Cu3(CO3)2(bPY)3](CLO4)2}n through rigid and flexible ligands
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DOI:
10.1016/j.ssc.2015.01.018
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发表时间:
2015-04-01
影响因子:
2.1
通讯作者:
Nath, R.
中科院分区:
文献类型:
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作者:
Ajeesh, M. O.;Yogi, A.;Nath, R.
Single crystalline and polycrystalline samples of S = 1/2 Kagome lattices {[Cu-3(CO3)(2)(bpe)(3)](CLO4)(2)}(n) and {[Cu-3(CO3)(2)(bpe)(3)](CLO4)(2)}(n), respectively were synthesized. Their structural and magnetic properties were characterized by means of x-ray diffraction and magnetization measurements. Both compounds crystalize in a hexagonal structure (space group P-6) consisting of CuO4 Kagome layers in the ab-plane but linked along c direction through either rigid bpy or flexible bpe ligands to form 3D frame works. Magnetic measurements reveal that both the compounds undergo ferromagnetic ordering (T-c) at low temperatures and the Tc and the extent of frustration could be tuned by changing the nature of the pillar ligands. {[Cu-3(CO3)(2)(bpe)(3)](CLO4)(2)}(n) which is made up of flexible bpe ligands has a Tc of 5.7 K and a Curie-Weiss temperature (theta(cw)) of -39.7 K giving rise to a frustration parameter of | theta(cw) | / Tc similar or equal to 6.96. But the replacement of bpe by a more rigid and electronically delocalized bpy ligand leads to an enhanced Tc similar or equal to 9.3 K and a reduced frustration parameter of | theta(cw) | / Tc similar or equal to 3.54. (C) 2015 Elsevier Ltd. All rights reserved.