Consider the mode expansion of a (chiral) scalar field confined to a disc with circumference L: ϕ(x)=ϕ0+pϕ2πLx+∞∑n=11√ne−(kna)/2(e−iknx b†n+eiknx bn)
(Fermionic) Vertex operators are defined by Vα(x)=:eiαϕ(x):
:eiαϕ(x):=(L2πa)Δ(α)eiαϕ(x)
Now here are my questions (They may really be "Newbie"-CFT-questions;) ) :
Since the right hand side is only an approximation of of :eiαϕ(x): to lowest order I am wondering whether the left hand-side reproduces the correct (say) fermonic commutators in all cases and whether hand side only partially reproduces the correct fermonic commutators?
If the right-handside only indeed only partially reproduces the correct commutation relations how can we say that a certain product of fermionic operators (say a product of 3 fermionic operators) indeed obeys the correct sermonic commutators when written in the "bosonized language"?
What is the importance of the higher-order terms in aL in the "expansion" of the vertex operator?
Is all this a more general construction in CFT?
I am looking forward to your responses!
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