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Sugawara modes satisfy Virasoro at every noncritical complex level
Statement
Let be a finite-dimensional complex simple Lie algebra with invariant form normalized so long roots have square . On every restricted affine-current module of complex level as in Restricted affine-current module, the operators of Sugawara modes and their normal ordering satisfy Consequently these operators and define a representation of Virasoro algebra in the L_m convention. No energy grading, unitarity, irreducibility or integrability is assumed. The critical level is excluded from this normalized formula.
Facts & Assumptions
Given: The restricted affine-current module , its noncritical level , and integers .
Sugawara modes and their normal ordering: writing , for a -orthonormal complex basis, with the split at ; these sums are locally finite and basis independent.
Sugawara modes act on affine currents with weight one: on this entire module class.
Restricted affine-current module: all sufficiently large positive current modes annihilate any fixed vector.
Virasoro algebra in the L_m convention fixes the bracket and cubic central normalization appearing in the Statement.
Proof
Choose a -orthonormal basis and abbreviate . Existence follows by finite diagonalization of the nondegenerate symmetric complex form, rescaling each nonzero diagonal entry by a complex square root. Put and let mean for and for ; this subscript specifies the split, not an intrinsic index of . Expanding by [F2] gives This equality is algebraic on each . Truncate the original quadratic sum at ; it stabilizes on and by [F1], so its commutator stabilizes to the left side. On the right, in the positive tail the rightmost indices are or , and in the negative tail they are or ; [F4] kills all these tails for large . Thus the displayed sum is locally finite on , and fixed reindexings below do not create limiting errors.
Reindex the first term by . It becomes , whereas the desired normal order is . The second term already has the latter order. Their normally ordered coefficients combine to . The order difference in the first term is For it is the commutator for ; for it is its negative for ; for it is zero. Therefore Every correction sum is finite, including all zero-index endpoints.
By [F3], , since and . The correction in step 2.1 is consequently times . For , the finite sum is . For , put in the negative interval; it becomes . At both sides vanish. These finite arithmetic identities follow by induction from and . Dividing step 2.1 by gives exactly the stated central charge. The resulting brackets and the scalar central action satisfy [F5], hence give the claimed Virasoro representation, including when .
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Sources
- Peter Haine, The Segal–Sugawara construction, §§3.2–3.3 (standard reference, not scraped)