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The metric pairing is a linear bijection to the dual, and the raised covector in an orthonormal frame
Statement
Let be a -dimensional Lorentz vector space (Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space): is symmetric and bilinear, nondegenerate in the sense that both radicals are (The matrix, left and right radicals, rank, and nondegeneracy of a bilinear form on a finite-dimensional space), and of inertia . Let be the algebraic dual (Linear functionals and the algebraic dual ). Then:
(a) The map , , is linear, and it is injective: means for all , that is .
(b) (The dual family of a finite basis is a basis of the dual space, with the same dimension), so is a linear bijection; equivalently and (Rank-nullity: , Rank and nullity of a linear map with finite-dimensional domain).
(c) Consequently for every covector there is a unique vector with for all ; the assignment , , is linear and is the inverse of (Invertible linear maps, linear isomorphisms, and inverse linear maps), so for and for every ; in particular if and only if .
(d) If is an -orthonormal ordered basis of (Every Lorentz form admits an ordered basis with matrix diag(-1,1,1,1)) and are the values of on that basis, then
that is and for in this basis, and
Hence, for the vector is nonzero and, in the sense of (Timelike, null, spacelike and causal vectors of a Lorentz vector space), it is null exactly when , timelike exactly when (equivalently ), and spacelike exactly when (equivalently ); for one has , which has no causal character.
No orientation, time orientation or affine structure is used, and no choice principle is used.
Facts & Assumptions
Given: A -dimensional real vector space , a Lorentz form on , and the map .
is -dimensional, and is symmetric and bilinear with and inertia (Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space, The matrix, left and right radicals, rank, and nondegeneracy of a bilinear form on a finite-dimensional space).
is the algebraic dual of , and the assignment with is a linear bijection from the bilinear forms on onto ; in particular is a linear map for every bilinear form (Linear functionals and the algebraic dual , Bilinear forms on correspond linearly and bijectively to linear maps , Linear map between vector spaces over the same field).
If is a basis of a finite-dimensional -vector space, then its dual family is a basis of the dual space; consequently (The dual family of a finite basis is a basis of the dual space, with the same dimension).
There is an -orthonormal ordered basis of , that is, for all (Every Lorentz form admits an ordered basis with matrix diag(-1,1,1,1)).
For a linear map with finite-dimensional domain, , where and (Rank-nullity: , Rank and nullity of a linear map with finite-dimensional domain).
A linear map is invertible, equivalently a linear isomorphism, when there is a linear map with and ; such an is unique and written , and is bijective (Invertible linear maps, linear isomorphisms, and inverse linear maps).
A vector is timelike, null or spacelike according as , with , or ; the zero vector has none of these characters, and every nonzero vector has exactly one (Timelike, null, spacelike and causal vectors of a Lorentz vector space).
Proof
The map is linear, and . Since is a bilinear form on , its associated map lies in and for all , so is linear by [L2]. If , then for every , so lies in the left radical of , which is by [L1]; conversely by linearity (equivalently ), so .
The map is surjective. Fix an -orthonormal ordered basis of [L4], with dual family , a basis of by [L3]. For all one has with , by [L4], and the functional takes the same values on the basis ; two linear functionals that agree on a basis agree on every vector, so , which exhibits as a scalar multiple of (here ). Hence every element of the basis of lies in the linear span of , so that span is all of ; therefore is surjective.
The map is a linear bijection, , and the inverse assignment exists with the stated properties. By step 1.1 is injective and by step 1.2 it is surjective, hence bijective; by [L3] and [L1], ; and [L5] applied to the linear map gives the same picture independently, and , with and by step 1.2. By [L6] the inverse is a well-defined linear map, unique, and satisfies and . Writing for , we get for every ; any with for all satisfies , hence by injectivity of , which is the asserted uniqueness. The two inverse equations are exactly for and , and holds if and only if . This proves (a), (b) and (c).
Component formula. Let and keep the orthonormal basis of step 1.2; put and for , where , and set . For every basis vector , bilinearity and orthonormality [L1, L4] give ; hence and for . The functionals (linear in its second argument by [L1]) and agree on the basis , hence on all of ; therefore , and uniqueness in step 2.1 yields .
Quadratic form and causal trichotomy. With from step 3.1, bilinearity and orthonormality give , because and . If then by step 2.1, so [L7] applies: is null exactly when this value is , that is when ; timelike exactly when it is negative, that is when ; and spacelike exactly when it is positive, that is when . If then by step 2.1 and the zero vector has no causal character by [L7]. No orientation, time orientation or affine structure was used, and no choice principle was used.
Depends on
Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space
Linear functionals and the algebraic dual
The matrix, left and right radicals, rank, and nondegeneracy of a bilinear form on a finite-dimensional space
Bilinear forms on correspond linearly and bijectively to linear maps
Rank-nullity:
Rank and nullity of a linear map with finite-dimensional domain
The dual family of a finite basis is a basis of the dual space, with the same dimension
Linear map between vector spaces over the same field
Invertible linear maps, linear isomorphisms, and inverse linear maps
Every Lorentz form admits an ordered basis with matrix diag(-1,1,1,1)
Timelike, null, spacelike and causal vectors of a Lorentz vector space
Dependency tree · 2 levels
Sources
- B. Crowell, Special Relativity, revision 2020-12-10 (author-published undergraduate textbook, 246 PDF pages): Section 6.4 Duality pp. 134-137 (the frequency covector and its dual); signature (+---) converted to (-+++)
- S. Murugesh, Relativity - Special Theory (IIST course notes PH33003/PH43017, last update 2009-02-18, 31 PDF pages): Chapter 6 Waves pp. 25-28, the wave four-vector (6.1)-(6.5) pp. 25-26