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Stress-tensor Ward identity on the sphere

Statement

For a fixed-coordinate sphere Virasoro block family of def-cft-fixed-coordinate-sphere-virasoro-block-family, the stress-tensor insertion is G(w)=∑j=1n(hj(w−zj)2+1w−zj∂zj)F(z). The constant Laurent coefficient of this expression at w=zi, which is the block with L−2 inserted at slot i, equals ∑j≠i(hj(zi−zj)2+1zi−zj∂zj)F(z).

Facts & Assumptions

Given: Distinct zj, primary weights hj, and a block family with stress insertion G as in Fixed-coordinate sphere Virasoro block family.

[F1]

Fixed-coordinate sphere Virasoro block family supplies functionals Φz on the algebraic tensor product, with F(z) their evaluation on the chosen primary tuple; the Laurent coefficient of Gz at ti0 is Φz(v1⊗⋯⊗L−2vi⊗⋯⊗vn). It also supplies the stated primary principal parts, absence of other finite poles, and O(w−4) behavior at infinity.

[F2]

The same definition supplies the three global Ward identities for translations, dilations, and special conformal transformations.

[F3]

Fixed-coordinate sphere Virasoro block family adopts the local Laurent indexing T(t)=∑mLmt−m−2 for its stress-tensor matrix element. Thus its constant coefficient at t=0 is the block with L−2 inserted, as specified in [F1].

Proof

1.1F1F2algebra

Set R(w)=∑j(hjF(w−zj)−2+(∂zjF)(w−zj)−1). By [F1], G−R has no principal part at any finite zj, hence is entire on C. Expanding at infinity gives R(w)=∑j∂zjFw+∑j(zj∂zjF+hjF)w2+∑j(zj2∂zjF+2zjhjF)w3+O(w−4). Each of the first three coefficients vanishes by [F2], so R(w)=O(w−4). Also G(w)=O(w−4) by [F1]. Thus the entire function G−R tends to zero at infinity and is identically zero by Liouville's theorem.

2.1F1F3step 1.1algebra∎

Around w=zi, the j=i terms of R have only powers (w−zi)−2 and (w−zi)−1, so contribute no constant Laurent coefficient. Every j≠i term is analytic at zi, with constant coefficient hjF/(zi−zj)2+(∂zjF)/(zi−zj). By [F3], the constant coefficient of G is the L−2-insertion. Summing these terms proves the second formula.

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