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Existence of a smooth future-directed tetrad field near every event
Statement
Let be a time-oriented smooth Lorentzian four-manifold and let (Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model). Then there is an open neighborhood of and a smooth future-directed tetrad field on (Local frame fields, coordinate frames and tetrad fields), i.e. for all with future-directed for every .
Facts & Assumptions
Given: A time-oriented smooth Lorentzian four-manifold and a point .
A tetrad field on an open set is a tuple of four smooth vector fields that is pointwise a -orthonormal ordered basis, and it is future-directed when its first member is future-directed at every point (Local frame fields, coordinate frames and tetrad fields).
There is an ordered -orthonormal basis of (Every Lorentz form admits an ordered basis with matrix diag(-1,1,1,1)).
For a nonzero timelike one has , and is the future timelike component (Classification of future and past causal vectors by a timelike field, Timelike, null, spacelike and causal vectors of a Lorentz vector space).
The component functions of in a smooth chart are (Smooth covariant 2-tensor fields on a smooth manifold).
The coordinate derivations of a chart form a basis of , and every vector of has a unique coordinate list (Coordinate derivations form a basis of the tangent space, A finite list is an ordered basis if and only if every equals for exactly one ; those scalars are the coordinates of in that ordered basis).
A vector field on a chart domain is smooth exactly when its coordinate component functions are smooth (Smoothness of a vector field is equivalent to smooth coordinate components).
A smooth map between smooth manifolds is continuous ( and smooth maps between smooth manifolds).
If is continuous at and , then there is an open neighborhood of with on ; the same holds with replaced by . (Continuity of a map of topological spaces at a point and globally)
Finite sums, products and composites of maps on Euclidean domains are ( Euclidean maps are closed under componentwise algebra and composition).
On the squaring map has derivative , and for powers and quotients the product and quotient rules hold (Sums, scalar multiples, products and quotients: , , , and when ).
If is open and is injective, with , and is invertible everywhere, then is open and is a diffeomorphism (An injective regular map is a diffeomorphism onto its image).
The smooth structure of the tangent bundle used for smooth vector fields assumes the axiom (The Axiom of Countable Choice ()).
Proof
Choose a smooth chart around . By [L2] there is an ordered -orthonormal basis of ; by [L3], , so after replacing by if necessary we may assume is future-directed, still an orthonormal basis. Expand each uniquely in the coordinate basis, [L5], and define on , with the constants as coefficients. Each is a smooth vector field by [L6] (so that the tangent-bundle smooth structure of [L12] is in force), and .
Consider the smooth functions and on . They are smooth because in the chart they equal the finite sums and of products of smooth functions, using [L4] and [L9]; and , while by step 1.1 and the definition of future-directedness.
By [L7] and [L8] applied to the continuous functions (positive at ) and (positive at ), there is an open neighborhood of on which and .
Define on . The function is on : the map is the inverse of the injective squaring map on whose derivative is invertible everywhere there, so it is by [L11], and has derivatives for every by iterating the product and quotient rules of [L10]; composites and products of maps are by [L9]. Hence is smooth on , and ; since , the field is a positive multiple of at every point, so and is future-directed.
For define on ; these are smooth fields by [L9], and , so lies in the -orthogonal complement of . The function is smooth by [L4] and [L9], and because and . By [L7] and [L8] there is an open containing with on . Define on ; it is smooth by the argument of step 4.1, , and .
Define on , a smooth field with and , and let , smooth with because and . Shrink to an open containing with and define ; then is smooth, and .
Define on , smooth with , and let , smooth with . Shrink to an open containing with and define ; then is smooth, and for .
On the four smooth fields satisfy by steps 4.1-5.1, and is future-directed by step 4.1. The Gram matrix is invertible, so a linear relation implies for all after pairing with , hence ; thus the tuple is pointwise an ordered basis, a future-directed tetrad field on by [L1].
The open neighborhood of and the field have the asserted properties; this proves the theorem.
Remarks
Choice convention. The construction uses smooth vector fields, hence tangent-bundle sections, whose canonical smooth structure assumes the axiom of The Axiom of Countable Choice () as recorded in [L12]; no further choice principle is used, and the construction selects a definite basis at by an explicit finite procedure.
Depends on
Local frame fields, coordinate frames and tetrad fields
Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
Smooth covariant 2-tensor fields on a smooth manifold
Every Lorentz form admits an ordered basis with matrix diag(-1,1,1,1)
Classification of future and past causal vectors by a timelike field
Timelike, null, spacelike and causal vectors of a Lorentz vector space
Coordinate derivations form a basis of the tangent space
A finite list is an ordered basis if and only if every equals for exactly one ; those scalars are the coordinates of in that ordered basis
Smoothness of a vector field is equivalent to smooth coordinate components
and smooth maps between smooth manifolds
Continuity of a map of topological spaces at a point and globally
Euclidean maps are closed under componentwise algebra and composition
Sums, scalar multiples, products and quotients: , , , and when
An injective regular map is a diffeomorphism onto its image
The Axiom of Countable Choice ()
Dependency tree · 2 levels
Sources
- S. M. Carroll, Lecture Notes on General Relativity, arXiv:gr-qc/9712019v1 (1997), Ch. 3 'tetrads and non-coordinate bases', printed pp. 88-91 (PDF pp. 95-98)
- H. S. Reall, Part III General Relativity (Cambridge, October 12, 2022 revision), section 2.2: an orthonormal basis of the tangent space exists at every point and any two are related by a Lorentz transformation, printed pp. 26-28 (PDF pp. 27-29)
- D. Tong, General Relativity (Cambridge Part III Mathematical Tripos, Michaelmas 2019), section 3.1.2: an orthonormal basis of T_pM can always be found at each point, printed p. 93 (PDF p. 100)