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Existence of an inertial frame whose time axis is a prescribed future timelike direction

Statement

Let (A,V,η,C+) be the oriented time-oriented affine Minkowski space, let d∈V be a future timelike displacement and put T:=−η(d,d)>0 and n:=d/T. Then:

(i) η(n,n)=−1 and n is future timelike, so n is a future unit timelike vector.

(ii) For every event o there is an inertial frame (o;e0,e1,e2,e3) of the model with e0=n.

(iii) For the inertial chart x of any such frame one has x(o+λd)=(λT,0,0,0) for every real λ; in particular x(o)=0 and x(o+d)=(T,0,0,0). Consequently, for any two events p,q with q−p=d, the chart of such a frame represents the displacement q−p by the coordinate vector (T,0,0,0): the spatial coordinates of p and q agree and their time coordinates differ by T.

Facts & Assumptions

Given: The oriented time-oriented affine Minkowski space (A,V,η,C+) and a future timelike displacement d∈V, with T:=−η(d,d)>0 and n:=d/T.

[F1]

Inertial frames and charts: for every event o and every η-orthonormal ordered basis (f0,f1,f2,f3) of V with future first vector and positive orientation, (o;f0,…,f3) is an inertial frame; its chart is x(r)=E−1(r−o) with E(u)=∑auaea the frame's linear isomorphism, and every vector u has unique coordinates u=u0e0+us, us∈S=span⁡(e1,e2,e3) (Inertial frames and inertial charts of the affine Minkowski model, Existence of future-oriented inertial frames at every event).

[F2]

Cone coordinates: in an inertial frame with first vector in C+ one has C+={u:u0>∣us∣} and C−={u:u0<−∣us∣}, and η(u,u)=−(u0)2+∣us∣2; the restriction of η to S is positive definite, (e1,e2,e3) is orthonormal for it, and ∣z∣2=δ(z,z) for z∈S (The timelike set has exactly two convex components, described in orthonormal coordinates, Time orientation, future and past timelike/null/causal vectors, and the closed cones, The Euclidean spatial structure and cross product of an inertial frame).

[F3]

The passive boost B(β) is defined for every parameter β∈R3 with ∣β∣<1 (The passive Lorentz boost with parameter beta); it is a proper orthochronous Lorentz map with inverse B(−β) (The passive boost is a proper orthochronous Lorentz map with inverse B(-beta), Linear and affine Lorentz maps, and the Lorentz group); and if u is future timelike with η(u,u)=−1 and coordinates (u0,us), then the parameter β:=us/u0 satisfies ∣β∣<1 and B(β)u=f0, where f0 is the first vector of the frame used for the coordinates (The passive boost is a proper orthochronous Lorentz map with inverse B(-beta) (iv)).

[F4]

Lorentz maps preserve the metric and the orientation class: for a linear Lorentz map L one has η(Lv,Lw)=η(v,w) for all v,w; the composition and the inverse of Lorentz maps are Lorentz maps, and the proper orthochronous ones form a group; if L is proper, then the oriented volume form ϵ of The oriented volume form epsilon and the permutation symbols of an inertial frame is preserved, ϵ(Lv0,…,Lv3)=ϵ(v0,…,v3); and ϵ takes the value 1 on every positively oriented η-orthonormal basis, so a tuple of four vectors with ϵ-value 1 is positively oriented (Lorentz maps are isomorphisms of determinant ±1 that preserve causal character and permute the cones; the Lorentz sets are groups, The oriented volume form is independent of the positively oriented inertial frame).

[L5]

Square roots and monotonicity: every real c≥0 has a unique c≥0 with (c)2=c (Square roots exist: a unique a≥0 with (a)2=a; the positives are {x2:x≠0}); for x,y≥0 one has x<y  ⟺  x2<y2 (Squaring is monotone on the nonnegatives).

[L6]

Order arithmetic of R: multiplication of an inequality by a positive real preserves it, and a product of positives is positive (Sign rules for products and monotonicity of multiplication); a constant may be added to both sides and inequalities may be added (Order is preserved by adding a constant and by adding inequalities); and the order is trichotomous and transitive, with 1>0 (Ordered field).

Proof

technique · direct
1.1givenF1L5L6algebra

By bilinearity of η and T2=−η(d,d) one has η(n,n)=η(d,d)/T2=(−T2)/T2=−1, so n is timelike and η(n,n)=−1; moreover d is nonzero because it is timelike, so n=d/T is nonzero.

2.1step 1.1givenF1F2L5L6

Fix an event o and an inertial frame (o;f0,f1,f2,f3) with chart y, and write n=n0f0+ns in its coordinates; since n is timelike, [F2] puts it in C+ or C−, and since n=d/T with d0>∣ds∣≥0 and T>0 its first coordinate satisfies n0=d0/T>0, so n lies in C+={u:u0>∣us∣} and is future timelike; in particular n0>∣ns∣≥0.

3.1step 2.1F2F3L5L6algebra

From 1=−η(n,n)=(n0)2−∣ns∣2 we get (n0)2=1+∣ns∣2>∣ns∣2; setting β:=ns/n0 (the coordinate column, identified with the vector β1f1+β2f2+β3f3 of S) one has ∣β∣2=δ(β,β)=∣ns∣2/(n0)2<1, hence ∣β∣<1 by strict monotonicity of squaring on the nonnegatives and ∣β∣≥0; thus the passive boost B(β) is defined.

4.1step 3.1F3

By [F3] (iv), applied to the future timelike unit vector n with coordinates (n0,ns), the boost satisfies B(β)n=f0; and B(β) is proper orthochronous with inverse B(β)−1=B(−β).

5.1step 4.1F1F4

Define e0:=n=B(β)−1f0 and ei:=B(β)−1fi for i=1,2,3; then ea=B(β)−1fa for all a, so η(ea,eb)=η(fa,fb)=diag⁡(−1,1,1,1)ab because a Lorentz map preserves η, and the ordered basis (e0,e1,e2,e3) is η-orthonormal with future first vector e0=n; it is positively oriented because B(β)−1 is proper and preserves the oriented volume form, so ϵ(e0,…,e3)=ϵ(f0,…,f3)=1 for the positively oriented basis (fa), whence the basis (ea) is positively oriented. Therefore (o;e0,e1,e2,e3) is an inertial frame with e0=n, which is (ii).

6.1step 5.1F1algebra

For the chart x=E−1(⋅−o) of any inertial frame (o;e0,…,e3) with e0=n one has E(1,0,0,0)=e0=n and d=Tn, so x(o+λd)=E−1(λd)=λT E−1(n)=λT (1,0,0,0)=(λT,0,0,0) for every real λ, since E−1 is linear; in particular x(o)=0 and x(o+d)=(T,0,0,0), which is (iii).

7.1step 6.1F1algebra∎

Consequently, for events p,q with q−p=d, linearity of E−1 gives x(q)−x(p)=E−1(q−p)=(T,0,0,0), so the spatial coordinates of p and q agree and their time coordinates differ by T; together with steps 1.1, 2.1, 5.1 and 6.1 this proves (i), (ii) and (iii).

Depends on

Dependency tree · 2 levels

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