Good evening,
I am just reading the wonderful book by H. Georgi "Lie Algebras in Particle Physics", and I'm having a problem with one of the proves. While talking about complex representations especially in SU(3) the author states that the conjugate representation of a representation with Dynkin coefficients (n,m) has Dynkin coefficients (m,n). He argues that the highest weight of (n,m) is $n\mu^1+m\mu^2$ while the lowest one is $-n\mu^2-m\mu^1$, where $\mu^i$ are the fundamental weights, while the heighest weight of (m,n) is just $n\mu^2+m\mu^1$, so it is the negative of the lowest weight of (n,m) and from that he follows over a few steps that (m,n) must be the conjugate representation. What I don't get, and what Georgi doesn't really explain, is why $-n\mu^2-m\mu^1$ shall be the lowest weight of (n,m). I worked it out for some examples, but I can't figure out a simple argument for all n,m (as it should be, if Georgi doesn't bother to explain further). Do you have some ideas? Greetings from Heidelberg,
Markus Zetto