Danger
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Start by turfing anything that I can't express on a manual typewriter.
But sometimes it's really nice. Consider e.g. the proof that if ##\rho## is a projection operator for the 1-dimensional subspace spanned by a unit vector f (written as |f> when we use bra-ket notation), and A is self-adjoint, then ##\operatorname{Tr}(\rho A)=\langle f,Af\rangle##.micromass said:Dirac notation is only useful if they also teach rigged Hilbert spaces. Without that, it's a pretty awful notation. When I read something in Dirac notation, then I always get confused. If I then read the same thing in ordinary math notation, then I understand it immediately.
Furthermore, I think that Dirac notation tends to obfuscate domain issues. So you're more prone to errors.
My feelings exactly.micromass said:What I want to say is that physicists and mathematicians shouldn't be throwing mud at each other. In fact, we should benifit from each other and work together.
Fredrik said:"Ordinary math notation" (with the convention to have the inner product linear in the second variable):
\begin{align}
\operatorname{Tr}(\rho A) &=\sum_n\langle e_n,\rho A e_n\rangle =\sum_n\left\langle e_n,\langle f,Ae_n\rangle f\right\rangle =\sum_n\langle \langle f,Ae_n\rangle^* e_n,f\rangle =\sum_n\langle \langle Ae_n,f\rangle e_n,f\rangle\\
&=\sum_n\langle \langle e_n,Af\rangle e_n,f\rangle =\langle Af,f\rangle =\langle f,Af\rangle
\end{align}
Office_Shredder said:The only thing that needs to change is
[tex]\sin^2(x)[/tex]
This needs to die in a fire