In Ward & New (1969), the expression for second harmonic generation (SHG) and third harmonic generation (THG) intensity is derived for the focal volume of a strongly focused gaussian beam (axially thick medium).
The predicted value of the J-integral term in the expression for intensity of SHG under perfect phase matching conditions ($\Delta k=0$) is found to be π on page 184.
While for THG, the value of the J-integral term in the expression for intensity under perfect phase matching conditions ($\Delta k=0$) is found to be zero.
For THG, things seem to make sense. Third harmonic light generated before focus is born with a phase that is π radians out of phase with third harmonic light that is born after focus.
Since there is no phase slippage ($\Delta k$) of the funamental pump wave before and after focus except for that caused by the Gouy phase shift, the third harmonic light destructively interferes since it's π radians out of phase.
I don't understand why if this logic works with THG, it doesn't work for SHG. What am I missing?