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Worked construction of a future-oriented inertial frame from an arbitrary orthonormal basis
Example
Worked example of the sign and orientation adjustments. Let be an oriented time-oriented affine Minkowski space, fix any origin , and let be any -orthonormal ordered basis of . Its first vector is timelike. Set if and if , and set for . This makes future while preserving orthonormality. The time-axis reversal, when needed, has change-of-basis matrix and determinant , so it flips the orientation class; retaining leaves that class unchanged.
If is positively oriented, retain it. Otherwise replace by (or interchange and ); this flips the orientation class, preserves orthonormality and leaves the future vector unchanged. Together with , the resulting basis is an inertial frame. In particular, a past-directed, negatively oriented starting basis needs only the time-axis reversal, giving . This is the explicit construction of Existence of future-oriented inertial frames at every event.
Two-dimensional illustration. In the two-dimensional analogue with with its translation action, , , standard orientation (a basis is positive when its coordinate determinant is positive), and future timelike set , take (past timelike) and (spacelike). Then satisfies , and , and is future; so is an -orthonormal basis with future first vector, and the change of basis has determinant . If the original pair was the negatively oriented one, the pair is positively oriented and is an inertial frame of the two-dimensional analogue of the model.
Facts & Assumptions
Given: An arbitrary -orthonormal ordered basis in the oriented time-oriented affine Minkowski model, an origin , and the two-dimensional illustration of the Example.
An -orthonormal ordered basis satisfies (Every Lorentz form admits an ordered basis with matrix diag(-1,1,1,1)).
The timelike set is the disjoint union , and a vector in is future timelike while a vector in is past timelike (Time orientation, future and past timelike/null/causal vectors, and the closed cones); the components are convex, and in orthonormal coordinates whose time-axis basis vector is future, the future timelike vectors are exactly those with (The timelike set has exactly two convex components, described in orthonormal coordinates).
is bilinear and symmetric, so , (Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space).
In a finite-dimensional real vector space of positive dimension, the change of basis between two ordered bases has exactly when they lie in the same orientation class, and exactly when they lie in different classes. There are exactly two such classes; an orientation chooses one as positive, and bases in the other are negatively oriented (Orientation of a finite-dimensional real vector space).
An inertial frame is a tuple with an -orthonormal, future, positively oriented ordered basis, and such frames with arbitrary origin exist (Inertial frames and inertial charts of the affine Minkowski model, Existence of future-oriented inertial frames at every event).
Verification
By [L1] and [L3], , so . They lie in opposite components: if both lay in the same component, its convexity [L2] would put in , contradicting . Thus when and otherwise is always future. Set for . Retaining retains the basis, while negating it preserves its norm and all vanishing off-diagonal pairings, since ; hence is -orthonormal. Its change-of-basis matrix is the identity when is future and when is past. Their determinants are and , respectively, so [L4] shows that the orientation is retained in the first case and reversed in the second. In particular, past-directed negative input becomes future-directed positive input.
In the two-dimensional illustration, has and , so is past timelike by the explicit two-dimensional convention in the Example; has by [L3], , so is future timelike by that same convention; and , are direct evaluations. Hence is an -orthonormal pair with future first vector and with change-of-basis determinant , so it is positively oriented exactly when the original pair was negatively oriented.
If is positively oriented, retain it. Otherwise replacing by preserves -orthonormality by the sign computation of step 1.1, leaves the future first vector unchanged, and has change-of-basis matrix of determinant . There are exactly two orientation classes by [L4], so reversing the negative class gives the positive class. Interchanging and also has determinant and preserves orthonormality and , giving the same alternative correction.
In every initial time-orientation and orientation case, steps 1.1 and 2.1 produce an -orthonormal, future, positively oriented ordered basis, which together with the chosen origin is an inertial frame by [L5]. Step 1.2 verifies the displayed two-dimensional illustration. Thus the recipe realizes the construction of Existence of future-oriented inertial frames at every event from arbitrary orthonormal input, including the past-directed negative example.
Depends on
Every Lorentz form admits an ordered basis with matrix diag(-1,1,1,1)
Time orientation, future and past timelike/null/causal vectors, and the closed cones
Inertial frames and inertial charts of the affine Minkowski model
Existence of future-oriented inertial frames at every event
Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space
Orientation of a finite-dimensional real vector space
The timelike set has exactly two convex components, described in orthonormal coordinates