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RNS chiral picture-charge selection rule
Formal chiral free-field charge neutrality for a fixed genus-g RNS sector with the stated bosonized background-charge Ward convention; not a superstring measure.
Statement
Fix a closed genus- RNS worldsheet and one chiral sector with the bosonized background convention of RNS bosonized picture charge convention. Here a scalar-picture eigenoperator of charge means an insertion with the constant-shift law for every scalar constant , with all other fields fixed. Equivalently, in the split , ; times shift-invariant derivative or spectator fields is included. This is the scalar-exponent picture convention, not an unspecified total grading involving . For a formal chiral correlator with such picture eigenoperators of charges , a nonzero correlator requires The assertion is conditional on the stated bosonized zero-mode Ward convention and does not define a path-integral measure over moduli.
Statement references
Facts & Assumptions
Given: A compact connected closed genus- surface, one fixed RNS chirality, the bosonized curvature coupling and formal zero-mode Ward functional of RNS bosonized picture charge convention. Full AC is assumed as required by the genus and Gauss–Bonnet suppliers.
RNS bosonized picture charge convention: for , the curvature term is ; insertions of contribute zero-mode exponent ; the formal correlator is neutral only when the total coefficient vanishes.
Genus and Euler characteristic of a compact Riemann surface: under full AC, .
Global Gauss-Bonnet for closed oriented surfaces: ; with the convention fixed in [F1], this gives . The supplier proof carries full AC.
The Axiom of Choice is assumed because [F2] and [F3] require it.
Proof
In the zero-mode split , [F3] and [F2] give the curvature term Therefore contributes , and each insertion contributes by the eigenoperator shift law in the Statement (take ). Their product therefore contributes , including derivative and spectator factors invariant under that shift. The total coefficient is .
By the neutral zero-mode functional in [F1], a nonzero chiral correlator requires this coefficient to vanish. Solving gives . The calculation applies independently to the right-moving chiral copy.
Remarks
Picture charge is not beta-gamma ghost number. The result follows from the explicit curvature coupling and neutral zero-mode convention; it neither chooses PCO locations nor constructs vertical chains or a global superstring integration cycle.