4.6 Article

Structural, spectroscopic and magnetic properties of a novel copper(II) L-tyrosinato complex

Journal

RSC ADVANCES
Volume 4, Issue 108, Pages 63150-63161

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/c4ra10717a

Keywords

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Funding

  1. Polish Ministry of Science and Higher Education of the Republic of Poland for the Faculty of Chemistry, Wroclaw University of Technology and for Faculty of Chemistry, University of Wroclaw

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The complex [Cu(L-Tyr)(2)(H2O)]center dot H2O (1) (L-Tyr = L-tyrosine) was obtained as crystals and characterized by Xray, spectroscopic (FT-IR, FT-Raman, NIR-vis-UV, and EPR) and magnetic methods. The monomeric complex crystallized in the monoclinic P2(1) symmetry with a = 11.967 (1) angstrom, b = 5.9986 (4) angstrom, c = 14.936 (1) angstrom. The amino N and carboxylate O atoms of chelating L-tyrosinate anions together with the O atom of water molecules create a slightly distorted square pyramidal environment around the Cu(II) ions (s = 0.11). The distance of about 5.998(1) angstrom [Cu(L-Tyr)(2)(H2O)] units is involved in a polymeric chain based on N(1)-H center dot center dot center dot O(4) vi and N(2)-H center dot center dot center dot O(5)(vi) hydrogen bonds. The d-d band found in the polycrystallinereflectance spectrum at 15 700 cm(-1) is composed of three B-2(1)(d(x2-y2)) -> (2)A(1) (d(z2)), B-2(1) -> B-2(2)(d(xy)) and B-2(1) -> E-2 (d(xz) approximate to d(yz)) transitions with energies 14 880, 15 800 and 19 950 cm(-1), respectively. In DMSO solution the complex preserves its square pyramidal geometry as evidenced by an intensive band at ca. 16 400 cm(-1). The EPR spectral parameters for powder (g(parallel to) = 2.236 and g(perpendicular to) = 2.063) and DMSO frozen solution (g(parallel to) = 2.250, g(perpendicular to) = 2.055, and A(parallel to) = 180 G) correspond to an axial symmetry of the Cu(II) coordination geometry with the d(x2-y2) orbital as a ground state of the unpaired electron. Furthermore, the frozen solution spectrum revealed signals corresponding to S = 1 spin states of Cu(II) ions coupled by dipole-dipole interactions with distinctly resolved hyperfine splitting due to two copper nuclei (vertical bar D vertical bar = 0.0468 cm(-1), g(parallel to) = 2.238, g(perpendicular to) = 2.06 and A(parallel to) = 85 G). The variable-temperature magnetic susceptibility measurements revealed the existence of a weak ferromagnetic interaction between neighboring copper(II) ions through the N-H center dot center dot center dot O hydrogen bonds.

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