Charged commutants with arbitrary matter
Abstract
A nonzero ghost charge degree annihilates any endomorphism commuting with all tensor ghost modes.
M is an arbitrary complex module. Tensor products and endomorphisms are algebraic; no topology, finite dimension, positivity or irreducibility is assumed. The maps b, c and ghostNumber are the actual maps of BcGhostFock and BcGhostCharge. Bracketed group and module assumptions are anonymous instance arguments.
Definition 1.1 (liftGhost).
Formalization. D5/S3/Quantum/Fermionic/BcGhostChargeTensor.liftGhost (✓ std3).
Source. Repository-derived.
Commentary.
The matter factor is acted on by its identity map.
Definition 1.2 (number).
Formalization. D5/S3/Quantum/Fermionic/BcGhostChargeTensor.number (✓ std3).
Source. Repository-derived.
Commentary.
The tensor ghost-number operator.
Definition 1.3 (B).
Formalization. D5/S3/Quantum/Fermionic/BcGhostChargeTensor.B (✓ std3).
Source. Repository-derived.
Commentary.
Every integer b mode acts on the ghost factor.
Definition 1.4 (C).
Formalization. D5/S3/Quantum/Fermionic/BcGhostChargeTensor.C (✓ std3).
Source. Repository-derived.
Commentary.
Every integer c mode acts on the ghost factor.
Definition 1.5 (partialNumber).
Formalization. D5/S3/Quantum/Fermionic/BcGhostChargeTensor.partialNumber (✓ std3).
Source. Repository-derived.
Commentary.
A finite sum of the actual lifted normal bilinears.
Theorem 1.6 (tensor finite capture).
Proof. Machine-checked in Lean as D5/S3/Quantum/Fermionic/BcGhostChargeTensor.tensor_finite_capture (✓ std3). ∎
Source. Repository-derived.
Commentary.
Each pure tensor inherits a finite capture from its ghost vector. Tensor-product induction combines captures by finite union, so every larger finite set still computes number on the original tensor.
Theorem 1.7 (number commutes of signed modes).
Proof. Machine-checked in Lean as D5/S3/Quantum/Fermionic/BcGhostChargeTensor.number_commutes_of_signed_modes (✓ std3). ∎
Source. Repository-derived.
Commentary.
For epsilon squared equal to one, the two signs cancel in each normal bilinear. At a fixed x choose one finite union capturing x and E x. Commutation with that finite sum identifies number applied to E x with E applied to number x. Epsilon one gives commutation, and epsilon minus one covers anticommutation with both odd families.
Theorem 1.8 (charged commutant vanishes).
Proof. Machine-checked in Lean as D5/S3/Quantum/Fermionic/BcGhostChargeTensor.charged_commutant_vanishes (✓ std3). ∎
Source. Repository-derived.
Commentary.
Finite normal capture first proves that the charge commutator is zero. The stipulated degree d is nonzero, so d times E equal to zero forces E itself to be zero. This uses no scalar-commutant assertion on the tensor product.
The theorem can eliminate a later BRST residual only after that residual is constructed on this tensor carrier and its mode commutation and nonzero degree are proved. It does not construct a total BRST operator, prove nilpotence, or complete the string objective.
References
- Truth anchor:
D5/S3/Quantum/Fermionic/BcGhostChargeTensor.B - Truth anchor:
D5/S3/Quantum/Fermionic/BcGhostChargeTensor.C - Truth anchor:
D5/S3/Quantum/Fermionic/BcGhostChargeTensor.charged_commutant_vanishes - Truth anchor:
D5/S3/Quantum/Fermionic/BcGhostChargeTensor.liftGhost - Truth anchor:
D5/S3/Quantum/Fermionic/BcGhostChargeTensor.number - Truth anchor:
D5/S3/Quantum/Fermionic/BcGhostChargeTensor.number_commutes_of_signed_modes - Truth anchor:
D5/S3/Quantum/Fermionic/BcGhostChargeTensor.partialNumber - Truth anchor:
D5/S3/Quantum/Fermionic/BcGhostChargeTensor.tensor_finite_capture - Dependency: D5/S3/Quantum/Fermionic/BcGhostCharge