TY - JOUR
T1 - MnII, CuII and CoII coordination polymers showing antiferromagnetism, and the coexistence of spin frustration and long range magnetic ordering
AU - Li, Ya Min
AU - Xiao, Chang Yu
AU - Zhang, Xu Dong
AU - Xu, Yan Qing
AU - Lun, Hui Jie
AU - Niu, Jing Yang
PY - 2013/10/14
Y1 - 2013/10/14
N2 - Based on the ligand 1,2-H2bdc (1,2-H2bdc = 1,2-benzenedicarboxylic acid), three 2D coordination polymers [Mn(1,2-bdc)] n (1), [Cu(1,2-bdc)]n (2) and [Co3(OH) 2(1,2-bdc)2]n (3), have been prepared and characterized. In comparison with the mononuclear Mn unit of compound 1, paddle-wheel binuclear Cu2(CO2)4 and trinuclear Co3(OH) building units are observed in 2 and 3, respectively. Also, the bdc2- ligands adopt different coordination modes in the three compounds. The resulting two frustrated lattices have been observed, such as the triangular lattice for 2 and the Kagomé lattice for 3, and thus, both complexes 2 and 3 show spin frustrated antiferromagnetic properties. In addition, the magnetic hysteresis loops reveal the existence of the long range ordering in 2 and 3. Comparatively, the magnetic measurements indicate that compound 1 exhibits a weak antiferromagnetic interaction, and the fit of the variable-temperature magnetic susceptibility data to the empirical equation leads to the following parameters: J = -0.80(1) cm-1 and g = 2.02.
AB - Based on the ligand 1,2-H2bdc (1,2-H2bdc = 1,2-benzenedicarboxylic acid), three 2D coordination polymers [Mn(1,2-bdc)] n (1), [Cu(1,2-bdc)]n (2) and [Co3(OH) 2(1,2-bdc)2]n (3), have been prepared and characterized. In comparison with the mononuclear Mn unit of compound 1, paddle-wheel binuclear Cu2(CO2)4 and trinuclear Co3(OH) building units are observed in 2 and 3, respectively. Also, the bdc2- ligands adopt different coordination modes in the three compounds. The resulting two frustrated lattices have been observed, such as the triangular lattice for 2 and the Kagomé lattice for 3, and thus, both complexes 2 and 3 show spin frustrated antiferromagnetic properties. In addition, the magnetic hysteresis loops reveal the existence of the long range ordering in 2 and 3. Comparatively, the magnetic measurements indicate that compound 1 exhibits a weak antiferromagnetic interaction, and the fit of the variable-temperature magnetic susceptibility data to the empirical equation leads to the following parameters: J = -0.80(1) cm-1 and g = 2.02.
UR - http://www.scopus.com/inward/record.url?scp=84883898103&partnerID=8YFLogxK
U2 - 10.1039/c3ce41046c
DO - 10.1039/c3ce41046c
M3 - Article
AN - SCOPUS:84883898103
SN - 1466-8033
VL - 15
SP - 7756
EP - 7762
JO - CrystEngComm
JF - CrystEngComm
IS - 38
ER -