1980
DOI: 10.1021/ic50203a034
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Iron-nitrogen bond lengths in low-spin and high-spin iron(II) complexes with poly(pyrazolyl)borate ligands

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Cited by 126 publications
(95 citation statements)
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“…12 The related FeTp*2 (Tp* = tris (3,5-dimethylpyrazol-yl)borate) is high spin in solution but undergoes spin crossover and is low spin at 78 K and below. 13 The iron(II) complexes of charge-neutral scorpionates such as Tpm = [HC(pz)3] or Tpm* = [HC(pz*)3] (pz* = 3,5-dimethylpyrazol-1-yl) also show highly variable magnetic behaviour. The compounds [Fe(Tpm)2](X)2 (X = PF6, 14 ClO4, 15 NO3,16 BF4 17 ) are low spin at room temperature but undergo SCO above 300 K. [Fe(Tpm*)2](BF4)2 is high spin at room temperature but undergoes an abrupt SCO at 206 K in the solid to give a sample with 50% low-spin sites that originates from a crystallographic phase transition.…”
mentioning
confidence: 99%
“…12 The related FeTp*2 (Tp* = tris (3,5-dimethylpyrazol-yl)borate) is high spin in solution but undergoes spin crossover and is low spin at 78 K and below. 13 The iron(II) complexes of charge-neutral scorpionates such as Tpm = [HC(pz)3] or Tpm* = [HC(pz*)3] (pz* = 3,5-dimethylpyrazol-1-yl) also show highly variable magnetic behaviour. The compounds [Fe(Tpm)2](X)2 (X = PF6, 14 ClO4, 15 NO3,16 BF4 17 ) are low spin at room temperature but undergo SCO above 300 K. [Fe(Tpm*)2](BF4)2 is high spin at room temperature but undergoes an abrupt SCO at 206 K in the solid to give a sample with 50% low-spin sites that originates from a crystallographic phase transition.…”
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confidence: 99%
“…The title compound, [Fe(C 9 H 10 BN 6 ) 2 ], is a polymorph of a compound reported previously [Oliver et al (1980). Inorg.…”
mentioning
confidence: 88%
“…For the crystal structure of the other polymorph measured at room temperature, see : Oliver et al (1980). For iron(II) complexes with the Tp À derivative ligands, see : Janiak et al (2000); Reger et al (2005).…”
Section: Related Literaturementioning
confidence: 99%
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“…The distances of separation as shown in Table 2 are 3.394 Å for HDM and 3.336 for HDE. This suggests ineffective overlap of orbitals thus weak interaction between the orbitals giving rise to bonds with relatively low energy which is possible when the molecules are physically adsorbed unto the metal surface (Oliver et al 1979, Ebenso et al 2010, Bouayed et al 1998, Gece 2008, Obot and Obi-Egbedi 2010. Geometry optimized structures, equilibrium geometry structures and energies of HDM and HDE Fig 2 shows the optimized geometry and equilibrium structures of HDM and HDE.…”
Section: Interaction/binding Energymentioning
confidence: 99%