The spectroscopic properties of the high-spin Fe(III)-alkylperoxo model complex [Fe(6-Me(3)TPA)(OHx)(00(t)Bu)](x+) (1; TPA = tris(2-pyridylmethyl)amine, Bu-t = tert-butyl, x = 1 or 2) are defined and related to density functional calculations of corresponding models in order to determine the electronic structure and reactivity of this system. The Raman spectra of 1 show four peaks at 876, 842, 637, and 469 cm(-1) that are assigned with the help of normal coordinate analysis, and corresponding force constants have been determined to be 3.55 mdyn/Angstrom for the O-O and 2.87 mdyn/Angstrom for the Fe-O bond. Complex I has a broad absorption feature around 560 nm that is assigned to a charge-transfer (CT) transition from the alkylperoxo pi (v)* to a t(2g) d orbital of Fe(lll) with the help of resonance Raman profiles and MCD spectroscopy. An additional contribution to the Fe-O bond arises from a a interaction between pi (h)* and an e(g) d orbital of iron. The electronic structure of 1 is compared to the related low-spin model complex [Fe(TPA)(OHx)(OO`Bu)](x+) and the reaction coordinate for O-O homolysis is explored for both the low-spin and the high-spin Fe(III)-alkylperoxo systems. Importantly, there is a barrier for homolytic cleavage of the O-O bond on the high-spin potential energy surface that is not present for the low-spin complex, which is therefore nicely set up for O-O homolysis. This is reflected by the electronic structure of the low-spin complex having a strong Fe-O and a weak O-O bond due to a strong Fe-O sigma interaction. In addition, the reaction coordinate of the Fe-O homolysis has been investigated, which is a possible decay pathway for the high-spin system, but which is thermodynamically unfavorable for the low-spin complex.