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Orthogonal projection away from the symmetry plane

Statement

At a point where the matrix H of Gram determinant for the two symmetry directions is invertible, write its inverse as Hij and put P(V)=V−XiHijg(Xj,V). Then P(V) is orthogonal to both generators, P(Xi)=0, and P is the identity on vectors orthogonal to both. The symmetric form q(V,W)=g(V,W)−g(V,Xi)Hijg(Xj,W) equals g(PV,PW) and annihilates the orbit plane. All conventions are those of Stationary Lorentzian data and tensor conventions. No global quotient coordinate or positivity theorem is asserted.

Facts & Assumptions

[F1]

The metric is symmetric and the invertible Gram matrix has HijHjk=δki; repeated indices i,j are summed over 1,2. Gram determinant for the two symmetry directions Stationary Lorentzian data and tensor conventions

Proof

**Given:**The metric, generators and invertible Gram matrix.

Goal: Check projection and the displayed form.

1.1givenF1

Direct substitution gives g(Xk,PV)=g(Xk,V)−HkiHijg(Xj,V)=0. Substitution of V=Xk gives P(Xk)=0. If g(Xj,V)=0 for both j, the defining formula gives PV=V.

2.1F1step 1.1∎

Expand g(PV,PW). The two cross terms are each −g(V,Xi)Hijg(Xj,W), and the quadratic term restores one copy by the inverse identity. The resulting expression is exactly q(V,W); the projection property then shows it annihilates the orbit plane.

Depends on

Used by · 2

Dependency tree · 2 levels

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