Question on the form of a vertex operator in a proof

Schure
Messages
1
Reaction score
0
[Closed] Question on the form of a vertex operator in a proof

Ok, never mind - I decided to find the solution in a different way.. This is a little too specialized anyway. (Is there a way to delete the thread?)

[STRIKE]Hi,

I am reading paper [1] and I found that formula (33),
\psi(xy)\psi^*(y)=\frac 1{x^{1/2}-x^{-1/2}}\exp\left(\sum_n\frac{(xy)^n-y^n}{n}\alpha_{-n}\right)\exp\left(\sum_n\frac{y^{-n}-(xy)^{-n}}n\alpha_n\right)
is almost in accordance to its alleged source [2, Theorem 14.10], except for the factor at the front, namely,
\frac1{x^{1/2}-x^{-1/2}}.
Does anyone know where that comes from? Probably this comes from the shift of coordinates that happens when Eskin and Okounkov use half-integers for the indices in the infinite wedge representation, instead of the usual whole integers. But I have not found the way to fully justify the term using this.

I'd really appreciate a hint! Thanks!

Schure

[1] A. Eskin and A. Okounkov, Pillowcases and quasimodular forms, http://arxiv.org/pdf/math/0505545.pdf
[2] Kac, Infinite dimensional Lie algebras, 3rd edition[/STRIKE]
 
Last edited:
Physics news on Phys.org
Do stick around Schure, it's good to have some specialized discussion now and again. I find it a nice change of pace from the nth iteration of interpreting quantum mechanics, the twin paradox, or "is string theory science?"

There are some very knowledgeable people who hang out here.
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
Back
Top