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A conjugate representation reverses the cubic anomaly polynomial

Statement

Let H=SU(3)×U(1), let E=C3 have representation ρE(g,z)=zg, and let E∗ be its dual representation. For a smooth background connection AE on a smooth manifold X, use the induced dual connection AE∗=−AET and curvatures FE=dAE+AE∧AE and FE∗=dAE∗+AE∗∧AE∗. With the degree-six polynomial I6 defined above, one has

I6(E∗,AE∗)=−I6(E,AE).

For the canonical Chern–Simons transgression

Q5(E,AE):=3i24π2∫01tr⁡E ⁣(AE∧FE,t∧FE,t) dt,FE,t:=t dAE+t2AE∧AE,

the dual transgression satisfies Q5(E∗,AE∗)=−Q5(E,AE). Thus any common linear descent of this conjugate pair has zero total cubic polynomial and zero total first consistent descent representative.

Facts & Assumptions

Given: The group H, its defining representation E, the dual representation E∗, a smooth connection AE, its induced dual connection, and the cubic polynomial normalization.

[F1]

Degree-six cubic trace polynomial for a chiral representation: I6(ρ,Aρ)=i24π2tr⁡Vρ(Fρ∧Fρ∧Fρ), and the dual connection is represented by AE∗=−AET.

Proof

1.1givenF1algebra

Transposing the curvature formula gives FE∗=−FET: for the one-form AE, graded transposition gives (AE∧AE)T=−AET∧AET, so d(−AET)+(−AET)∧(−AET)=−(dAE+AE∧AE)T.

2.1F1step 1.1algebra

Since each entry of FE is a two-form, reversing the order of two curvature factors contributes (−1)2⋅2=1. Hence tr⁡((FET)3)=tr⁡((FE3)T)=tr⁡(FE3). The three minus signs in FE∗3=(−FET)3 therefore give I6(E∗,AE∗)=−I6(E,AE) by [F1].

3.1F1step 1.1algebra∎

For every t∈[0,1], the same transposition calculation applied to AE,t=tAE gives FE∗,t=−FE,tT. Thus the integrand defining Q5(E∗,AE∗) is −tr⁡(AET∧FE,tT∧FE,tT). The trace of a transpose reverses the order of the three factors; cyclically moving the degree-one factor past the two degree-two factors contributes sign (−1)1(2+2)=1. The integrand is therefore −tr⁡(AE∧FE,t∧FE,t). Integration over t proves the transgression identity and the stated cancellation under a common linear descent.

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