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Vanishing divergence implies closed Hodge dual

Statement

For the stationary Lorentzian data and a smooth real two-form U, ∇aUab=0 implies d(⋆gU)=0. Thus the word co-closed here means precisely the vanishing-divergence condition, equivalently the displayed Hodge-closure equation.

Facts & Assumptions

[F1]

Use the metric connection and index conventions of Stationary Lorentzian data and tensor conventions.

[F2]

The real Hodge star and its complex extension are those of Complex self-dual forms and metric-dependent contraction.

[F3]

The Hodge formula is (⋆gU)ab=12ϵabcdUcd, and exterior differentiation is alternating differentiation. Lorentzian exterior calculus and Hodge star

[F4]

At each point one may choose coordinates with gab=diag⁡(−1,1,1,1) and first metric derivatives zero. Point-normal and exponential coordinate charts of the metric-selected connection

[F5]

In a positively oriented chart the metric volume form is ϵ=∣det⁡(gab)∣ dx0∧dx1∧dx2∧dx3; its component array is the positive density times the alternating symbol. The metric volume form, current flux through 3-faces and finite-chain charges

Proof

Given: The data and hypotheses in the Statement.

Goal: Prove all asserted identities under these hypotheses.

1.1F1F2F3F4F5algebra

Fix a point p and use [F4], making the chart positively oriented by reversing one spatial coordinate if necessary. The Christoffel symbols and first metric derivatives vanish at p. Write ϵ for the metric volume form of [F5]. Its components are ∣det⁡g∣ times the alternating symbol. Since the determinant is a polynomial in the metric entries and the square-root function is smooth at ∣det⁡g(p)∣=1, the vanishing of their first derivatives gives ∂ϵ(p)=0. For distinct indices a,b,c let j be the missing fourth index. The Hodge formula gives (⋆gU)bc=ϵbcajUaj, with no sum over a,j, since the two complementary terms in the half-sum agree.

2.1step 1.1F1F3F4algebra

At p, cyclically adding derivatives and using ∂ϵ(p)=0 gives (d⋆gU)abc=ϵabcj(∂aUaj+∂bUbj+∂cUcj)=ϵabcj∇kUkj for distinct a,b,c, with only k summed in the last expression; the missing k=j term is zero by antisymmetry. Put Vj=∇kUkj. Metric compatibility gives Vj=gjb∇aUab, with a,b summed. Thus vanishing divergence implies V=0, and the displayed identity makes every distinct-index component of d⋆gU zero. Repeated-index components vanish by alternation. Since p was arbitrary, d⋆gU=0 globally.

3.1step 1.1step 2.1F1F5algebra∎

Conversely, suppose d⋆gU=0. For each j at p, choose the other three indices as a,b,c. The identity in step 2.1 gives 0=ϵabcjVj, with no summation here. By [F5] and the normal metric at p, ϵabcj=±1, so Vj=0 for each j. Lowering the free index in Vj=gjb∇aUab using the nondegenerate metric yields ∇aUab=gbjVj=0, with the contracted indices summed. The point was arbitrary, proving the converse globally and hence the asserted equivalence.

Depends on

Used by · 2

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