The cancellation of 3'rd harmonic distortion by local feedback is, however, on page 94 of 'Analog Integrated Circuits for Communication' by Don Pederson and K. Mayaram. You might find this textbook in your university library.
In 1973, I did ask Dr. Meyer, privately, whether higher orders were easily cancelled as well, but he said that he did not know of any approach at the time. I am not surprised at this time after rereading the class notes on the subject, because:
"The term involving a(3) in (1.42) is due to third order distortion in the forward amplifier. The term involving a(2) is due to second order distortion in the forward amplifier being fed back and combining with the fundamental signals to produce third order distortion. Thus the error signal S(e) contains second order distortion as well as linear terms. These two combine in the second order nonlinearity to produce third order distortion. This process is called second order interaction. It is interesting to note that if a(3) is zero, but a(2) is non-zero, then b(3) will be finite. That is, even if the original amplifier had no third order distortion, the application of feedback can create third order distortion via second order interaction. ..."
The basic equation relating to the above commentary is:
b(3) = {a(3)[ 1+a(1)f ] - 2a(2)squared times f } / [ 1+a(1) times f ] to the fifth power
