TY - JOUR
T1 - Syntheses, crystal structures, ferroelectrics and magnetic properties of [R-BzPy]2[Cu(mnt)2] complexes ([R-BzPy]+ = 1-(4′-R-benzyl)-pyridinium, R = NO2 or Br; mnt2- = maleonitriledithiolate)
AU - Ren, Xiaoming
AU - Ma, Jing
AU - Lu, Changsheng
AU - Yang, Senzu
AU - Meng, Qingjin
AU - Wu, Peiheng
PY - 2003/4/7
Y1 - 2003/4/7
N2 - The structures of two ion-pair complexes, which consist of 1-(4′-R-benzyl)pyridinium (R = NO2 (1), Br (2)) and bis(maleonitriledithiolato)cuprate(II), have been determined by X-ray single crystal analyses, and the results show the stacking patterns in 1 and 2 are different from each other although the difference between the molecular structures of these complexes is only the substituent of the benzene ring, which may arise from the difference of interactions between cations and anions in these two complexes. Complex 1 crystallizes in the non-centrosymmetric space group P1, and dielectric measurements shows ferroelectric behavior with a small hysteresis loop. Quantum chemistry calculation further indicate the electric dipole in a unit cell is 56.5509 Debye, and DSC analysis reveal a Tc of 377 K, from the paraelectric to the ferroelectric phase. The magnetic susceptibilities of these two complexes measured in the temperature range 1.8-260 K show an antiferromagnetic coupling feature between neighboring Cu(II) ions with 0= -0.580 K for 1 and -2.167 K for 2. The polycrystalline EPR spectra of the two complexes at room temperature are different from each other, characterized axial g tensors are g|| of 2.09, g⊥ of 2.02 for 1, and g|| = 2.05, g⊥ = 2.03, A|| = 40.6 × 10-4 cm-1 for 2.
AB - The structures of two ion-pair complexes, which consist of 1-(4′-R-benzyl)pyridinium (R = NO2 (1), Br (2)) and bis(maleonitriledithiolato)cuprate(II), have been determined by X-ray single crystal analyses, and the results show the stacking patterns in 1 and 2 are different from each other although the difference between the molecular structures of these complexes is only the substituent of the benzene ring, which may arise from the difference of interactions between cations and anions in these two complexes. Complex 1 crystallizes in the non-centrosymmetric space group P1, and dielectric measurements shows ferroelectric behavior with a small hysteresis loop. Quantum chemistry calculation further indicate the electric dipole in a unit cell is 56.5509 Debye, and DSC analysis reveal a Tc of 377 K, from the paraelectric to the ferroelectric phase. The magnetic susceptibilities of these two complexes measured in the temperature range 1.8-260 K show an antiferromagnetic coupling feature between neighboring Cu(II) ions with 0= -0.580 K for 1 and -2.167 K for 2. The polycrystalline EPR spectra of the two complexes at room temperature are different from each other, characterized axial g tensors are g|| of 2.09, g⊥ of 2.02 for 1, and g|| = 2.05, g⊥ = 2.03, A|| = 40.6 × 10-4 cm-1 for 2.
UR - http://www.scopus.com/inward/record.url?scp=18944363399&partnerID=8YFLogxK
U2 - 10.1039/b210314a
DO - 10.1039/b210314a
M3 - 文章
AN - SCOPUS:18944363399
SN - 1477-9226
SP - 1345
EP - 1351
JO - Dalton Transactions
JF - Dalton Transactions
IS - 7
ER -