AGT conjecture for genus-one Liouville conformal blocks

Let ai=(ai,ai)\boldsymbol a_i=(a_i,-a_i) for 1iN1\leq i\leq N. The Liouville conformal block is

B(c,k~,h~,q~)=TrqdVk1,kNhN(xN)Vk3,k2h2(x2)Vk2,k1h1(x1),\mathcal{B}(c,\tilde{k},\tilde{h},\tilde{q})=\operatorname{Tr} q^d V^{h_N}_{k_1,k_N}(x_N)\cdots V^{h_2}_{k_3,k_2}(x_2)V^{h_1}_{k_2,k_1}(x_1),

with q=x1=q1qNq=x_1=q_1\cdots q_N and xixi+11=qi+1x_i x_{i+1}^{-1}=q_{i+1}. Define

Δm,n=m(t1+t2n)t1t2.\Delta_{m,n}=\frac{m(t_1+t_2-n)}{t_1t_2}.

AGT conjecture. One has

Z(t1,t2,a~,m~,q~)=Z(t1,t2,m~,q~)B(c,k~,h~,q~),Z(t_1,t_2,\tilde{\boldsymbol a},\tilde{m},\tilde{q})=Z'(t_1,t_2,\tilde{m},\tilde{q})\mathcal{B}(c,\tilde{k},\tilde{h},\tilde{q}),

under the substitution

c=1+6(t1+t2)2t1t2,ki=(t1+t2)24ai24t1t2,hi=Δmi,mi,c=1+6\frac{(t_1+t_2)^2}{t_1t_2},\qquad k_i=\frac{(t_1+t_2)^2-4a_i^2}{4t_1t_2},\qquad h_i=\Delta_{m_i,m_i},

where

Z=(q;q)2Δm1,m1++2ΔmN,mN1i<j(xixj1;q)2Δmi,mj(xi1xjq;q)2Δmj,mi,Z'=(q;q)_\infty^{2\Delta_{m_1,m_1}+\cdots+2\Delta_{m_N,m_N}-1}\prod_{i<j}(x_i x_j^{-1};q)_\infty^{2\Delta_{m_i,m_j}}(x_i^{-1}x_jq;q)_\infty^{2\Delta_{m_j,m_i}},

and (x;q)=i0(1xqi)(x;q)_\infty=\prod_{i\geq0}(1-xq^i). This is the proposed relation between Nekrasov partition functions and Liouville conformal blocks for a genus-one Riemann surface with NN punctures; the parser supplies no evidence resolving it.

Sources & referencesView supporting material

Primary source

Erik Carlsson, “AGT and the Segal-Sugawara construction”, arXiv:1509.00075 (2015).

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