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Simultaneity slices and rest distance relative to a future unit timelike vector
Definition
Let be the affine Minkowski space (Oriented time-oriented affine Minkowski space (the spacetime primitives)) and let be future unit timelike, (Timelike, null, spacelike and causal vectors of a Lorentz vector space, Time orientation, future and past timelike/null/causal vectors, and the closed cones).
(a) Rest space. The rest space of is the hyperplane ; by Norms of four-velocity and four-acceleration, and the observer rest-space decomposition clause (c) it is a three-dimensional linear subspace on which restricts to a positive-definite symmetric form, and the orthogonal projection onto it is (eta-orthogonality and orthogonal complements in a Lorentz vector space).
(b) Simultaneity slice. For the simultaneity slice of relative to is the affine hyperplane ; it contains and is three-dimensional, not a single point.
(c) Simultaneity relation. Define if and only if , that is, if and only if . Then is an equivalence relation on whose equivalence classes are exactly the slices ; reflexivity, symmetry and transitivity are consequences of being a linear subspace and are not physical assumptions.
(d) Rest distance. For with define . This is a real number , symmetric in , vanishes exactly when , and satisfies the triangle inequality on each slice, because the restriction of to is a positive-definite inner product.
(e) Dependence on and scope. The relation and the slices depend on the chosen future unit timelike vector : an event with generally has for another future unit (an explicit witness is given on this page). Simultaneity here is defined relative to a prescribed observer vector and is not an absolute relation. For a congruence one may form the pointwise slices ; the separate integrability question concerns the tangent distribution , not the assertion that these affine hyperplanes themselves are its integral hypersurfaces. Integral hypersurfaces can be curved; no global foliation is asserted.
Remarks
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Well-definedness. is three-dimensional because is nondegenerate and (eta-orthogonality and orthogonal complements in a Lorentz vector space); positive definiteness of the restriction of to , together with , and , is clause (c) of Norms of four-velocity and four-acceleration, and the observer rest-space decomposition. Consequently each slice is the translate , an affine hyperplane of dimension three, and is equivalent to , so the equivalence classes of are exactly the slices: this uses linearity of in each variable and linearity of as a subspace, nothing else.
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The rest distance is an inner-product norm. On the slice through the map is the positive-definite symmetric form obtained by restricting to , transported to the affine hyperplane by subtracting ; the axioms of a positive-definite inner product therefore give nonnegativity, symmetry, the vanishing condition and the triangle inequality. No choice principle is used: all objects are finite-dimensional or explicitly parametrized.
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Dependence on the observer vector is not a defect. Two distinct future unit timelike vectors have distinct rest spaces in general, and the relation is the relation of lying in a common slice of the foliation of by hyperplanes orthogonal to the fixed vector . For a congruence the vector varies from point to point, and the affine pointwise slices need not fit together. The Frobenius statement below tests whether there are hypersurfaces with tangent spaces ; it does not identify those hypersurfaces with the entire affine slices . No global simultaneity is asserted by this definition.
Depends on
Oriented time-oriented affine Minkowski space (the spacetime primitives)
Norms of four-velocity and four-acceleration, and the observer rest-space decomposition
eta-orthogonality and orthogonal complements in a Lorentz vector space
Timelike, null, spacelike and causal vectors of a Lorentz vector space
Time orientation, future and past timelike/null/causal vectors, and the closed cones
Dependency tree · 2 levels
Sources
- B. Crowell, Special Relativity, revision 2020-12-10 (author-published undergraduate textbook, 246 PDF pages): Sections 1.1-1.3 pp. 12-28 (vector representation of observer motion, operational radar calibration, time dilation, length-contraction road-trip example), Sections 3.5 and 3.7 pp. 60-68 (four-velocity, acceleration, projection operator), Section 3.9.3 pp. 73-74 (local failure of accelerated simultaneity), Sections 7.1-7.3 pp. 147-151 (Rindler coordinates and nonuniform proper acceleration), Section 8.1 pp. 165-169 (rotating synchronization), Section 9.5 pp. 205-211 (congruences, expansion, Born rigidity); signature (+---) converted to (-+++) and c = 1 formulas converted to x^0 = c t
- S. M. Carroll, Lecture Notes on General Relativity, arXiv:gr-qc/9712019v1 (1997): Chapter 1 pp. 8-16 (inertial frames built from rigid rods and synchronized clocks, simultaneity, time dilation, length contraction) and pp. 26-27 (worldline, proper time (1.97)-(1.99), four-velocity); Chapter 3 pp. 68-71 (proper-time functional)