Assume that the molecule consists of harmonic oscillators, which are connected and can exchange energy with each other.
Assume the possible excitation energy of the molecule to be E, which enables the reaction to occur.
The rate of intra-molecular energy distribution is much faster than that of reaction itself.
As a corollary to the above, the potential energy surface does not have any "bottlenecks" for which certain vibrational modes may be trapped for longer than the average time of the reaction
Derivation
Assume that A* is an excited molecule:
where P stands for product, and A‡ for the critical atomic configuration with the maximum energy E0 along the reaction coordinate.
The unimolecular rate constant is obtained as follows:[8]
where is the microcanonical transition state theory rate constant, is the sum of states for the active degrees of freedom in the transition state, is the quantum number of angular momentum, is the collision frequency between molecule and bath molecules, and are the molecular vibrational and external rotational partition functions.
^Di Giacomo, F. (2015). "A Short Account of RRKM Theory of Unimolecular Reactions and of Marcus Theory of Electron Transfer in a Historical Perspective". Journal of Chemical Education. 92 (3): 476–481. Bibcode:2015JChEd..92..476D. doi:10.1021/ed5001312.
^Lindemann, F. A.; Arrhenius, S.; Langmuir, I.; Dhar, N. R.; Perrin, J.; Mcc. Lewis, W. C. (1922). "Discussion on ?the radiation theory of chemical action?". Transactions of the Faraday Society. 17: 598–606. doi:10.1039/TF9221700598.
^Rice, Oscar Knefler; Ramsperger, Herman Carl (1927), "Theories of unimolecular gas reactions at low pressures", Journal of the American Chemical Society, 49 (7): 1617–1629, doi:10.1021/ja01406a001
^Kassel, Louis Stevenson (1928), "Studies in Homogeneous Gas Reactions I", The Journal of Physical Chemistry, 32 (2): 225–242, doi:10.1021/j150284a007