Issue 2, 2004

A crystallographic, EPR and theoretical study of the Jahn–Teller distortion in [CuTp2] (Tp = tris{pyrazol-1-yl}hydridoborate)

Abstract

Crystals of the title compound (1) contain two independent, centrosymmetric half-molecules per asymmetric unit. While both of these show Jahn–Teller elongated six-coordinate geometries, the lengths of the elongated Cu–N bonds in the two molecules differ by 0.117(2) Å at 30 K. The structure of one of these molecules (molecule A) does not vary with temperature below 350 K. The other molecule (molecule B) shows Cu–N bond lengths that are temperature-dependent between 225 and 375 K, but do not vary further at lower temperature. This indicates a fluxional axis of Jahn–Teller elongation in this molecule at these higher temperatures. Consideration of the thermal parameters in these structures implies that the fluxionality in molecule B is frozen out near 150 K. This conclusion is supported by a Q-band powder EPR study. The d–d transition energies of molecules A and B have been calculated by several density function (DF) methods, including a time-dependent DF calculation. The crystallographic data have been reproduced using the vibronic coupling model of Bürgi and Hitchman. This has shown that the different fluxionality regimes for molecules A and B are not a consequence of their different static molecular structures, but rather reflect their different local environments in the crystal.

Graphical abstract: A crystallographic, EPR and theoretical study of the Jahn–Teller distortion in [CuTp2] (Tp− = tris{pyrazol-1-yl}hydridoborate)

Article information

Article type
Paper
Submitted
07 Oct 2003
Accepted
17 Nov 2003
First published
04 Dec 2003

Dalton Trans., 2004, 236-243

A crystallographic, EPR and theoretical study of the Jahn–Teller distortion in [CuTp2] (Tp = tris{pyrazol-1-yl}hydridoborate)

C. A. Kilner, E. J. L. McInnes, M. A. Leech, G. S. Beddard, J. A. K. Howard, F. E. Mabbs, D. Collison, A. J. Bridgeman and M. A. Halcrow, Dalton Trans., 2004, 236 DOI: 10.1039/B312426F

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