“…Miller et al23 demonstrated that the rate constants for a gas‐phase reaction can be accurately calculated from where Q r ( T ) is the reactants partition function per unit volume and C ff ( t ) is the flux–flux correlation function, Here F̂ = [ Ĥ , h ] is the flux operator, h is the Heaviside step function, β = ( kT ) −1 , and F̂ (β) is the Boltzmannized flux operator By introducing the spectral decomposition of F̂ (β) into Eq. (2), a numerically convenient expression is obtained to evaluate C ff ( t )20, In this expression, f j and | u j 〉 are the eigenvalues and eigenfunctions of F̂ (β), respectively, N f is the number of such eigenfunctions with non‐negligible eigenvalues, and the | u j ( t )〉 is the time‐evolved eigenfunction of F̂ (β), To perform the mixed‐Q/C computations, the Hamiltonian is written as1, 20 In this equation, Ĥ s is the quantum Hamiltonian of the “system,” which only groups a selected set of coordinates, s , and their conjugated momenta. Ideally, s includes all the modes directly involved in the reactive event.…”