High-resolution electron spin resonance spectroscopy of XeF • in solid argon. The hyperfine structure constants as a probe of relativistic effects in the chemical bonding properties of a heavy noble gas atom Electron spin resonance studies of 45 Sc 17 O , 89 Y 17 O , and 139 La 17 O in rare gas matrices: Comparison with ab initio electronic structure and nuclear hyperfine calculations Electronic structure, ground state, and electron paramagnetic resonance spectroscopy of the matrix-isolated (η6-C6H6)V and (η6-C6D6)V half-sandwich transients Magnetic inequivalency of spatially equivalent atoms, in randomly oriented molecules, is demonstrated by isolating ͑ 6 -C 6 H 3 F 3 ͒V in an Ar matrix and recording its electron paramagnetic resonance ͑EPR͒ spectrum. This is the first experimental evidence of magnetic inequivalency in an organometallic complex. Although this phenomenon should exist in all EPR spectra of rigid polyatomic molecules, the extent of its effects crucially depends on the unpaired electron distribution. The analysis of the complete EPR spectrum yields the following spin Hamiltonian parameters: g xx ϭg yy ϭ1.967(3), g zz ϭ2.012͑3͒, ͉A xx ͑V͉͒ϭ͉A yy ͑V͉͒ϭ103.00͑5͒ϫ10 Ϫ4 cm Ϫ1 and ͉A zz ͑V͉͒ϭ10.20͑5͒ϫ10 Ϫ4 cm Ϫ1 . While the principal axes of the g and vanadium hyperfine tensors are parallel to the molecular symmetry axes, those of the three 19 F hyperfine tensors are not aligned with one another. Consequently, their 19 F hyperfine resonance positions are different and a detailed theoretical treatment of this phenomenon is required to fully comprehend and accurately simulate their EPR line shapes. The specific expressions that give rise to these magnetic inequivalencies and the g, 51 V, 19 F, and 1 H hyperfine tensors are derived as a function of the molecular orbital ͑MO͒ coefficients. The magnitudes and signs of the MO coefficients are independently estimated by computing electronic structure of this transient using the local density functional ͑LDF͒ method. The simulation of the experimental EPR spectra followed by the comparison of the experimental and computed spin Hamiltonian tensor components reveal that the complex, when trapped in an Ar matrix at 15 K, has a 2 A 1 ground state. The LDF computations also predict that the molecule is metastable in the gas phase with the 2 E and 2 A 1 states being nearly degenerate. Thus, the influence of the matrix trapping site is a decisive factor in isolating this molecule in a stable form and in determining its ground state. This also explains why the ͑ 6 -C 6 H 3 F 3 ͒V transient is difficult to isolate in high concentrations and to characterize by infrared and electronic absorption spectroscopy.