Principles Of Nonlinear Optical Spectroscopy A Practical Approach Or Mukamel For Dummies Fixed

Mukamel writes: ( S(t) = \int_0^\infty dt_3 \int_0^\infty dt_2 \int_0^\infty dt_1 R^(3)(t_1,t_2,t_3) E(t-t_3-t_2-t_1) E(t-t_3-t_2) E(t-t_3) )

Consider a standard three-pulse photon echo (a (\chi^(3)) experiment): Mukamel writes: ( S(t) = \int_0^\infty dt_3 \int_0^\infty

Mukamel loves double-sided Feynman diagrams. They look like spaghetti on mirrors. Here is how to fix them: Mukamel writes: ( S(t) = \int_0^\infty dt_3 \int_0^\infty