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Single-Strand Molecular Wheels and Coordination Polymers in Copper(II) Benzoate Chemistry by the Employment of α-Benzoin Oxime and Azides: Synthesis, Structures, and Magnetic Characterization.

Authors :
Stamatatos, Theocharis C.
Vlahopoulou, Gina
Raptopoulou, Catherine P.
Psycharis, Vassilis
Escuer, Albert
Christou, George
Perlepes, Spyros P.
Source :
European Journal of Inorganic Chemistry; Jul2012, Vol. 2012 Issue 20, p3121-3131, 11p
Publication Year :
2012

Abstract

The use of α-benzoin oxime (bzoxH<subscript>2</subscript>) in copper(II) benzoate chemistry, in the absence or presence of ancillary azido ligands, is reported. The reaction of Cu(O<subscript>2</subscript>CPh)<subscript>2</subscript> ·2H<subscript>2</subscript>O with one equivalent of bzoxH<subscript>2</subscript> in N, N-dimethylformamide (DMF) affords the decanuclear complex [Cu<subscript>10</subscript>(bzox)<subscript>10</subscript>(DMF)<subscript>4</subscript>] ( 1) in good yield. Dissolution of 1 in CH<subscript>2</subscript>Cl<subscript>2</subscript> leads to the subsequent isolation of the solvent-free complex [Cu<subscript>10</subscript>(bzox)<subscript>10</subscript>] ( 2) in moderate yields. Complexes 1 and 2 are isostructural and possess a loop or single-strand molecular wheel topology. The bzox<superscript>2-</superscript> dianions behave as η<superscript>1</superscript>:η<superscript>1</superscript>:η<superscript>2</superscript>:μ<subscript>3</subscript> ligands, which give rise to an overall [Cu<subscript>10</subscript>(μ-ONR)<subscript>10</subscript>(μ-OR′)<subscript>10</subscript>] core. Both 1 and 2 stack to form nanotubular columns with beautiful supramolecular architectures. The reaction of Cu(O<subscript>2</subscript>CPh)<subscript>2</subscript> ·2H<subscript>2</subscript>O with bzoxH<subscript>2</subscript> and NaN<subscript>3</subscript> in a 1:1:1 molar ratio in MeOH gives the bzoxH<subscript>2</subscript>-free complex [Cu(N<subscript>3</subscript>)(O<subscript>2</subscript>CPh)(MeOH)] <subscript>n</subscript> ( 3), which is a 1D chain. The Cu<superscript>II</superscript> atoms in 3 are linked by a single, end-on N<subscript>3</subscript><superscript>-</superscript> group, a syn, syn-η<superscript>1</superscript>:η<superscript>1</superscript>:μ PhCO<subscript>2</subscript><superscript>-</superscript> ion, and an oxygen atom from the bridging MeOH ligand. The 1D chains are hydrogen bonded into 2D sheets through N<subscript>azide</subscript> ···H(O<subscript>MeOH</subscript>) interactions. Variable-temperature, solid-state direct-current magnetic studies were carried out on 1- 3. The data for 1 and 2 indicate very strong antiferromagnetic exchange interactions and a S = 0 ground state, which is expected for even-membered loop arrays of Cu<superscript>II</superscript> atoms. In contrast, 3 exhibits ferromagnetic exchange interactions; the data were fitted to the appropriate equation derived from the Hamiltonian H = - JΣ( S<subscript>i</subscript> · S<subscript>i</subscript><subscript>+1</subscript>), which includes a zJ′ interchain interaction term. The best-fit parameters were J = +49.6(4) cm<superscript>-1</superscript>, g = 2.067(3), and zJ′ = 2.3(1) K. The combined results demonstrate the ligating flexibility of both the bzoxH<subscript>2</subscript> and azido groups and their usefulness in the synthesis of polynuclear Cu<superscript>II</superscript> clusters and coordination polymers. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
14341948
Volume :
2012
Issue :
20
Database :
Complementary Index
Journal :
European Journal of Inorganic Chemistry
Publication Type :
Academic Journal
Accession number :
77059449
Full Text :
https://doi.org/10.1002/ejic.201101292