Spin-forbidden reactions

Once a minimum energy crossing point is reached and parameter 1 above is satisfied, the system needs to hop from one diabatic surface to the other, as stated above by parameter 2. At a given energy (E), the rate coefficient [k(E)] of a spin-forbidden reaction can be calculated using the density of rovibrational states of the reactant [ρ(E)] and the effective integrated density of states in the crossing seam between the two surfaces [N_er(E)].

${\displaystyle k(E)=N_{cr}(E)/hp(E)}$

where

${\displaystyle N_{cr}(E)=\int dE_{h}\rho _{cr}(E-E_{h})p_{sh}(E_{h})}$

The probability of hopping (p_sh) is calculated from Landau-Zener theory giving

${\displaystyle p_{sh}(E)=(1-P_{LZ})(1+P_{LZ})}$

where

${\displaystyle P_{LZ}=\exp \left({\frac {-2\pi H_{12}^{2}}{n\Delta F}}{\sqrt {\frac {\mu }{2E}}}\right)}$

in which the spin-orbit coupling derived off the diagonal Hamiltonian matrix element between two electronic states (H₁₂), the relative slope of the two surfaces at the crossing seam [F(Δ)], the reduced mass of the system through its movement along the hopping coordinate (μ), and the kinetic energy of the system passing through the crossing point (E) are used.

It is useful to note that when E_h < E_c (when below the minimum energy crossing point) the probability of hopping between spin states is null.[5]

One example showing the slowing effect of spin-forbidden reaction takes place when Fe(CO)_x is placed under CO pressure. Transitions from x = 2,3,4 to x = 3,4,5 demonstrate a slowing rate when the reactant is in a triplet ground state but the product is in a singlet ground state. In the case of Fe(CO)_x, when x = 2, 3, 4 the iron exists as a triplet in ground state; when x = 5, the iron exists as a singlet in ground state. The kinetics of said system can be represented by:

${\displaystyle {\ce {Fe(CO)2->[{k_{23}}][CO]Fe(CO)3->[{k_{34}}][CO]Fe(CO)4->[{k_{45}}][CO]Fe(CO)5}}}$

where:

${\displaystyle k_{23}=(1.8\pm 0.3)\times 10^{13}\mathrm {cm} ^{3}\mathrm {mol} ^{-1}\mathrm {s} ^{-1}}$,

${\displaystyle k_{34}=(1.3\pm 0.2)\times 10^{13}\mathrm {cm} ^{3}\mathrm {mol} ^{-1}\mathrm {s} ^{-1}}$, and

${\displaystyle k_{45}=(3.5\pm 0.9)\times 10^{10}\mathrm {cm} ^{3}\mathrm {mol} ^{-1}\mathrm {s} ^{-1}}$.

The rate constants above are notably temperature independent, tested at 55 °C, 21 °C, and 10 °C, indicating, according to the authors, that the observed 500 fold reduction in rate occurs due to the spin-forbidden nature of the latter equation and not due to the kinetics of adding an additional ligand.[7]

Insertion into C-H bonds, known as C-H activation, is an integral first step in C-H functionalization.[11] For some metal complexes with identical ligands, C-H activation is rapid when one metal is used and slow when other metals are used, often first row transition metals, due to the spin allowed nature of the former case and the spin-forbidden nature of the latter case. The difference in rates of C-H activation of methane for CoCp(CO), RhCp(CO), and IrCp(CO) readily demonstrate this property. CoCp(CO), the starting material in a C-H activation, exists in a triplet spin state while RhCp(CO) exists in a singlet state, with the triplet state only 5.9 kcal/mol away. IrCp(CO) is unique among these complexes in that its starting state is essentially degenerate between the triplet and singlet states. The given product of C-H insertion, CpMH(CO)(CH₃), where M = Co, Rh, Ir, is in a singlet state meaning that the C-H activation with CoCp(CO) must reach the minimum energy crossing point for the reactant and product's potential energy surfaces, thus requiring relatively high energies to proceed.[12]

Through the use of photolysis, the rate of oxidative addition into silicon-hydrogen bonds has been shown to increase when the starting material is excited to the correct spin-state. CpRe(CO)₂ and CpMn(CO)₂ were subjected to photolysis to change their spin states from triplet to singlet and vice versa, respectively, such that an oxidative addition to Et₃Si-H could occur at a greatly accelerated rate.[13]

Metal-oxo species, due to their small spatial extent of metal-centered d orbitals leading to weak bonding, often have similar energies for both the low spin (${\displaystyle {\ce {M=O}}}$) and high spin configuration (${\displaystyle {\ce {*M-O*}}}$).[14] This similarity in energy between the low- and high spin configurations of oxo-species lends itself to the study of spin-forbidden reactions, such as Mn(salen)-catalyzed epoxidation. The Mn(salen)-oxo species can exist in either a triplet or quintet state. While the product of the quintet lies at a lower energy, both the triplet and quintet products can be observed.[15]