Quantum indirect damping state

Now, let us apply the approached model of quantum indirect damping to a situation where a Fermi resonance is possible to occur when the first excited state of the fast mode and the first overtones of some bending modes are close. The basic physical terms are defined in Table VIII. 

Later, it will appear that in the presence of indirect relaxation, Eqs. (91) and (94) Eqs. (92), (95), and Eqs. (93) and (96) respectively, transform into damped forms. Then, at any temperature the density operators in both quantum representations // and /// appear to be those of coherent states at any temperature (see Appendix N) ... 

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