Going to post a few pictures of a derivation, my apologies. I fear that full context needed. At any rate, I'm unable to follow how equation (3.64) obtains from (3.22) by inserting (3.63). We seem to be switching the vectors which are dotted using the BAC-CAB rule, but then it's not clear to me why the cross product $\mathbf k \times (\mathbf k \times \nabla_r E_{F_n})$ vanishes if that's true
@Arjun Yes. Note that the domain of definition is dense, meaning all vectors not in it are limits of sequences of vectors in it, and that the usual definition of a Hilbert basis is also just that you can obtain every vector as a "limit" of the basis vectors (because the sum is allowed to be infinite), so this is consistent.
but at the point where you're worrying about details like dense domains of definitions at all, I would suggest looking into the rigorous version of the spectral theorem in terms of spectral measures or stop worrying, really :P
@ACuriousMind I guess I'll stop worrying soon lol,I definitely lack the mathematical background :D
@ACuriousMind Okay two last questions: 1)So the above thing holds for any arbitrary conditions given that the domain remains dense in L^2? 2)So the "regular" eigenfucntions would lie in the domain of definition right?Will these themselves span whole of L^2 or we need to also consider the generalized eigenfuctions,I remember reading in ballentine we also need to consider the generalized ones.
I have a question about irreducible tensor operators. In the space of some n-rank tensor operator, do these irreducible tensor operators, play the same role that basis kets in a vector space play?
@Mr.Feynman not if anyone had reacted to it already - then the damage is already done, after all, and I'd just ping the people I'd told that with the correction
@EE18 That is not what is happening. Ignore the $\times$ in Equation (3.64) because it is actually a scalar (dot) multiplication, not a cross product at all.
you are, however, absolutely correct that the full context was needed. Definitely needed all 3 pages just to decipher what is happening
@naturallyInconsistent Agreed that the times there is not cross product related. But what I'm saying is that we essentially go from $(\mathbf k \cdot \nabla E_F) \mathbf k$ to $(\mathbf k \cdot \mathbf k) \nabla E_F)$
That sort of transfer is why I was thinking BAC-CAB rule (and the corresponding cross product). How did they do it? This is from page 71 of Nelson's Physics of Solar Cells in case it helps
@EE18 you are correct. That's pretty bad, and not justified
But in the absence of a magnetic field, the only thing that destroys spherical symmetry in favour of cylindrical symmetry is $\vec\nabla E_F$, and that would thus also be the direction of $\vec k$
@naturallyInconsistent I don't follow this argument. Are you saying $\V k$ and $\nabla E_F$ are in the same direction? (I must be misunderstanding since that surely isn't true)