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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 (A,V,η,C+) be an oriented time-oriented affine Minkowski space, fix any origin o∈A, and let (f0,f1,f2,f3) be any η-orthonormal ordered basis of V. Its first vector is timelike. Set g0:=f0 if f0∈C+ and g0:=−f0 if f0∈C−, and set gi:=fi for i=1,2,3. This makes g0 future while preserving orthonormality. The time-axis reversal, when needed, has change-of-basis matrix diag⁡(−1,1,1,1) and determinant −1, so it flips the orientation class; retaining f0 leaves that class unchanged.

If (g0,g1,g2,g3) is positively oriented, retain it. Otherwise replace g1 by −g1 (or interchange g1 and g2); this flips the orientation class, preserves orthonormality and leaves the future vector g0 unchanged. Together with o, the resulting basis is an inertial frame. In particular, a past-directed, negatively oriented starting basis needs only the time-axis reversal, giving (o;−f0,f1,f2,f3). This is the explicit construction of Existence of future-oriented inertial frames at every event.

Two-dimensional illustration. In the two-dimensional analogue with A=V=R2 with its translation action, o=(0,0), η(v,w)=−v0w0+v1w1, standard orientation (a basis is positive when its coordinate determinant is positive), and future timelike set C+={v:v0>∣v1∣}, take f0=(−1,0) (past timelike) and f1=(0,1) (spacelike). Then −f0=(1,0) satisfies η(−f0,−f0)=−1, η(f1,f1)=+1 and η(−f0,f1)=0, and −f0 is future; so (−f0,f1) is an η-orthonormal basis with future first vector, and the change of basis has determinant −1. If the original pair was the negatively oriented one, the pair (−f0,f1) is positively oriented and is an inertial frame of the two-dimensional analogue of the model.

Facts & Assumptions

Given: An arbitrary η-orthonormal ordered basis (f0,f1,f2,f3) in the oriented time-oriented affine Minkowski model, an origin o∈A, and the two-dimensional illustration of the Example.

[L1]

An η-orthonormal ordered basis satisfies η(fa,fb)=diag⁡(−1,1,1,1)ab (Every Lorentz form admits an ordered basis with matrix diag(-1,1,1,1)).

[L2]

The timelike set is the disjoint union T=C+⊔C−, and a vector in C+ is future timelike while a vector in C− 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 v0>∣vvec∣ (The timelike set has exactly two convex components, described in orthonormal coordinates).

[L3]

η is bilinear and symmetric, so η(−u,−w)=η(u,w), η(−u,w)=−η(u,w) (Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space).

[L4]

In a finite-dimensional real vector space of positive dimension, the change of basis between two ordered bases has det⁡>0 exactly when they lie in the same orientation class, and det⁡<0 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).

[L5]

An inertial frame is a tuple with an η-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

technique · direct sign computation
1.1L1L2L3L4algebra

By [L1] and [L3], η(f0,f0)=η(−f0,−f0)=−1, so f0,−f0∈T. They lie in opposite components: if both lay in the same component, its convexity [L2] would put 0=12f0+12(−f0) in T, contradicting η(0,0)=0. Thus g0:=f0 when f0∈C+ and g0:=−f0 otherwise is always future. Set gi:=fi for i=1,2,3. Retaining f0 retains the basis, while negating it preserves its norm and all vanishing off-diagonal pairings, since η(−f0,fi)=−η(f0,fi)=0; hence (g0,g1,g2,g3) is η-orthonormal. Its change-of-basis matrix is the identity when f0 is future and diag⁡(−1,1,1,1) when f0 is past. Their determinants are 1 and −1, 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.

1.2givenL3L4algebra

In the two-dimensional illustration, f0=(−1,0) has η(f0,f0)=−1<0 and f00=−1<0, so f0 is past timelike by the explicit two-dimensional convention in the Example; −f0=(1,0) has η(−f0,−f0)=−1 by [L3], (−f0)0=1>0=∣(−f0)vec∣, so −f0 is future timelike by that same convention; and η(−f0,f1)=0, η(f1,f1)=1 are direct evaluations. Hence (−f0,f1) is an η-orthonormal pair with future first vector and with change-of-basis determinant −1, so it is positively oriented exactly when the original pair was negatively oriented.

2.1step 1.1L1L3L4algebra

If (g0,g1,g2,g3) is positively oriented, retain it. Otherwise replacing g1 by −g1 preserves η-orthonormality by the sign computation of step 1.1, leaves the future first vector g0 unchanged, and has change-of-basis matrix diag⁡(1,−1,1,1) of determinant −1. There are exactly two orientation classes by [L4], so reversing the negative class gives the positive class. Interchanging g1 and g2 also has determinant −1 and preserves orthonormality and g0, giving the same alternative correction.

3.1step 1.1step 1.2step 2.1L5algebra∎

In every initial time-orientation and orientation case, steps 1.1 and 2.1 produce an η-orthonormal, future, positively oriented ordered basis, which together with the chosen origin o 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.

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