Abstract

New copper(II) complexes with bis(benzotriazol-1-yl)methane (1,1′-bbtm) were obtained. The complexation of copper ion leads to selective isolation of 1,1′-bbtm from a mixture of bis(benzotriazolyl)methane isomers. Crystal structures of [Cu(1,1′-bbtm)(NO3)2]n (1), [Cu(1,1′-bbtm)(H2O)(NO3)2]n (1a), [Cu3(1,1′-bbtm)4(H2O)8]A6, where A=ClO4− (2), BF4− (3), and of all three bbtm isomers, were characterized by single-crystal X-ray diffraction. Powder diffraction data of bulky compounds are in a good agreement with single-crystal data for 1–3. The structures consist of neutral chain 1∞[Cu(1,1′-bbtm)(H2O)(NO3)2] (1a) and 3∞[Cu (1,1′-bbtm)(NO3)2] framework (1), or positively charged (2, 3) layers 2∞[Cu3(1,1′-bbtm)4(H2O)8]n6n+ formed through 1,1′-bbtm (in 1–3) and NO3− (in 1) bridges. The 1,1′-bbtm molecules are coordinated to copper(II) ions in a bidentate bridging manner by N(3), N(3′) atoms of a triazole rings. Compounds 1–3 were investigated by static magnetic susceptibility method in the range 2–300K. An antiferromagnetic exchange between copper(II) ions was found in 1, J=−0.33cm−1. Compounds 2 and 3 are found to follow the Curie law with magnetic moments almost constant in all the temperature range studied because copper(II) ions are separated by long non-conjugated bridging ligands.

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.