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This may just show my ignorance, but I am wondering how to see the following:
For k∈ℕ>0 and a∈ℕ, the expression
Sk(a)≔k−1∑n=0eπik(n+a)2is independent of a if k is even:
kis even⇒∀a(Sk(a)=Sk(0)).In a roundabout way this follows from the modular transformation law of conformal characters of the U(1) WZW model.
But what’s an elementary arithmetic way to see this?
(If the exponent had another factor of “2”, then it would follow easily, also for odd k, by modular arithmetic, now in the other sense of “modular”. But the question is for the exponent as given.)
I guess the squares repeat with period k. If k is even then (k+a)2−a2=2ak+k2 is 0 mod 2k.
I am prepared to find that I am missing the obvious – but could you expand on how this answers the question?
Oh, I think I see what you mean. Right.
Right, so the summands are k-periodic after all, because
eπik(n+k)2=eπik(n2+2nk+k2)=eπikn2eπi(2n+k)⏟1ifkeven=eπikn2and so if we shift n↦n+a in the exponent, then we may just relabel to get rid of the a.
Thanks! :-)
Sorry for being cryptic. A snatched moment when supposed to be supporting my wife in her clothes shopping for our daughter’s wedding!
Best wishes to your daughter!
Meanwhile, I have another puzzlement:
If in my construction of irreps of ^ℤ2⋊SL2(ℤ) (here) I replace the factor
ζ≔eπikthroughout by eπikq, for q∈{1,2,⋯,k−1}, then all conclusions seem to remain valid.
Indeed, it seems to me that if q is chosen to be even, then we no longer need to assume that k is even, because the analogue of the above periodicity of summands (used here) follows already as
eπikq(n+k)2=eπikq(n2+2nk+k2)=eπikqn2eπiq(2n+k)⏟1sinceqeven=eπikqn2This is not a contradiction in itself, but it does seem to be in contradiction to Will Sawin’s reply to me on MO here, where he seems to exclude such irreps of odd k. I must again be missing something.
Thanks, wedding’s this Saturday!
Sorry, I can’t see where the possible mismatch lies from Sawin’s answer.
Yet another small issue I have is the further evaluation of the normalization factor ck (here)
ck=(1√k∑k−1n=0eπikn2)1/3.[edit: the first version of this comment had a misprint in this formula, with √k appearing instead of 1/√k. Now that this is fixed, the following actually comes out as expected]
This wouldn’t be a big deal (except if it came out zero, which it doesn’t) were it not for the fact that the literature seems to think it equals 1 (again Manoliu 98, p. 67).
I don’t know yet how to evaluate this analytically (probably needs some simple trick)
[edit: I see now that this and the following expressions are known as “generalized Gauss sums”]
but computer experiment suggests that for odd k we have
kodd⇒k−1∑n=0eπikn2=1while for the pertinent case of even k we seem to have
keven⇒k−1∑n=0eπikn2=√ki.If we now generalize to ζq as in #7 above and look at q=2, then computer experiment suggests that
k=2r+1⇒k−1∑n=0e2πikn2={√kifreven√kiifroddand
k=2r⇒k−1∑n=0e2πikn2={∝√iifreven0ifroddIf my computations here are correct, then we get an irrep of ^ℤ2⋊SL2(ℤ) whenever this sum is not zero (as it is in the very last case above).
It’s not clear to me how this squares with the mentioned discussion on MO. Maybe I have a mistake, somewhere.
Found my mistake: The previous post had started with a misprint: Instead of √k the first formular has a 1/√k. With that, the following factors of √k cancel out and the end result for the basic case is ck=(−1)1/12, which is actually the expected central charge! (cf. Gannon02 (3.1b) (p. 9)
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