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Oriented time-oriented orthonormal frame bundle

Statement

Assume ACω. Let (M,g,N,o) be an oriented, time-oriented smooth Lorentzian four-manifold of signature (−,+,+,+). Define Pg+(M) to have fiber over p∈M the linear isometries u:(R4,η)→(TpM,gp) that preserve the chosen orientation and send the standard future cone to the future cone selected by N. With the right action u⋅A:=u∘A, A∈SO+(1,3), this is a smooth right principal SO+(1,3)-bundle. Its fibers consist exactly of positively oriented future-directed orthonormal tetrads. The conclusion is local triviality; it asserts no global section.

Facts & Assumptions

Given: The oriented and time-oriented Lorentzian four-manifold and ACω convention in the Statement.

[F1]

Existence of a smooth future-directed tetrad field near every event: around every point there is an open neighborhood with a smooth future-directed orthonormal tetrad.

[F2]

Oriented smooth manifolds and oriented charts: an orientation is a smooth choice of orientation ray in each determinant line.

[F3]

The change between two future-directed tetrads is a Lorentz matrix: two future-directed tetrads at one point differ by a unique Lorentz matrix with ΛTηΛ=η, det⁡Λ=±1, and Λ00>0.

[F4]

Poincare semidirect group, dual pairing and moment components: under ACω, SO+(1,3) is a six-dimensional matrix Lie group, open in the Lorentz matrix submanifold of GL(4,R); its topology inherits a countable base from that Euclidean matrix space.

[F5]

Smooth principal G-bundle: a smooth right principal bundle has equivariant local product diffeomorphisms to U×G.

[F6]

Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model: M is a Hausdorff second-countable smooth four-manifold; the matrix Lie group SO+(1,3) inherits a countable basis from its finite-dimensional matrix topology.

Proof

1.1givenA1F1F2algebra

For each point p, use [F1] to choose a neighborhood U and a smooth future-directed tetrad E there. Take any coordinate chart around p. Relative to its coordinate determinant frame, the smooth orientation ray [F2] has locally constant sign; shrink around p to keep that sign fixed, and reverse one coordinate if the sign is negative. This gives a local oriented coordinate frame. In it, the determinant of the component matrix of E is a smooth nonzero real function; shrink U to a connected neighborhood of p, so its sign is constant. If that sign is negative, replace E1 by −E1. This preserves orthonormality and the future direction of E0 and makes E positively oriented by [F2]. Thus positively oriented future tetrads exist locally.

1.2givenF3algebra

Let u,v lie in a common fiber of Pg+(M). Since u is an isomorphism, A:=u−1v is the unique real matrix with v=u∘A. The isometry condition gives ATηA=η. Positivity of the two frame orientations gives det⁡A>0, while the Lorentz identity gives det⁡A=±1, hence det⁡A=1. Because u(e0) and v(e0) are future timelike, Ae0 is future timelike; and the invertible Lorentz map A is a homeomorphism of the timelike set. It therefore maps each connected component onto a component, and the image of e0 shows that it preserves the future component. Thus A∈SO+(1,3). This proves that the right action is transitive on each fiber; uniqueness of A proves freeness.

2.1step 1.1step 1.2F4algebra

For a local positively oriented future tetrad section E on U, define ΨE:U×SO+(1,3)→(Pg+(M))∣U by ΨE(p,A)=E(p)∘A. Step 1.2 makes this map bijective. Its set-theoretic inverse sends a frame u over p to (p,E(p)−1∘u). We construct the topology and smooth structure using these bijections, rather than assuming smoothness of functions on the total space.

3.1step 1.2step 2.1F4algebra

If E′ is another such section on an overlap, write E′(p)=E(p)∘A(p). Its coefficients are AIJ(p)=epI(EJ′(p)), hence are smooth functions of the base point: both e and E′ are smooth fields on M. Thus A is a smooth map into the embedded matrix Lie group [F4], and step 1.2 places every value in SO+(1,3). The transition between the charts is (p,B)↦(p,A(p)B), which is smooth; its inverse (p,B)↦(p,A(p)−1B) is smooth because inversion is smooth in the Lie group of [F4]. Declare a subset of the total space open exactly when its preimage under every ΨE is open. The overlap maps just computed are diffeomorphisms on open product domains, so each ΨE is a homeomorphism onto an open subset; combined with base and group coordinate charts, they give a compatible smooth atlas. In this atlas the right action is (p,B,C)↦(p,BC), hence smooth, and the projection is the product projection.

4.1A1step 1.2step 2.1step 3.1F4F5F6∎

The charts of step 2.1 and smooth transitions from step 3.1 give Pg+(M) local products U×SO+(1,3). Different base points separate by the Hausdorff base [F6], and distinct frames over one point separate in the Hausdorff matrix group [F4], so the total space is Hausdorff. For second countability, let B be a countable base of M; for each B∈B contained in at least one local-section neighborhood, use [A1] to select one pair consisting of such a neighborhood and a positively oriented future tetrad on it. The selected countable family of neighborhoods covers M, and countable bases of each selected U×SO+(1,3) give a countable base of the total space by [F4,F6]. Thus the local charts define a smooth manifold structure. Freeness and fiberwise transitivity were proved in step 1.2; by [F5], this is a smooth right principal SO+(1,3)-bundle. The construction supplies local sections only, so no global tetrad is asserted.

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