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These experiments also confirm agreement between clock synchronization by slow transport and Einstein synchronization. Even though some authors argued that this is sufficient to demonstrate the isotropy of the one-way speed of light, it has been shown that such experiments cannot, in any meaningful way, measure the (an)isotropy of the one way speed of light unless inertial frames and coordinates are defined from the outset so that space and time coordinates as well as slow clock-transport are described isotropically (see sections inertial frames and dynamics and the one-way speed).
1 2 3 4 5 Yuan-Zhong Zhang (1997). Special Relativity and Its Experimental Foundations. World Scientific. ISBN 978-981-02-2749-4. http://www.worldscibooks.com/physics/3180.html
1 2 3 4 5 6 7 8 Anderson, R.; Vetharaniam, I.; Stedman, G. E. (1998), “Conventionality of synchronisation, gauge dependence and test theories of relativity”, Physics Reports 295 (3–4): 93–180, Bibcode: 1998PhR...295...93A, doi:10.1016/S0370-1573(97)00051-3
↑ Michael Tooley (2000). Time, tense, and causation. Oxford University Press. p. 350. ISBN 978-0-19-825074-6. https://books.google.com/books?id=xNHU8Kpy-PsC
1 2 3 4 5 Janis, Allen (2010). "Conventionality of Simultaneity". In Zalta, Edward N. (ed.). Stanford Encyclopedia of Philosophy (英語).
d t ~ ′ = γ ~ [ 1 + κ ⋅ v ~ / c − κ ′ ⋅ v ~ ′ / c ] d t ~ − ( κ ′ + γ ~ v ~ ′ ) ⋅ d x ~ / c − [ γ ~ ( 1 + κ ⋅ v ~ / c ) − 1 ] κ ′ ⋅ v ~ v ~ 2 c v ~ ⋅ d x ~ + γ ~ κ ⋅ v ~ ( κ ⋅ d x ~ ) / c , d x ~ ′ = − γ ~ v ~ d t ~ + d x ~ + [ γ ~ ( 1 + κ ⋅ v ~ / c ) − 1 ] v ~ ⋅ d x v ~ 2 v ~ − γ ~ v ~ ( κ ⋅ d x ~ ) / c , γ ~ = γ ( 1 − κ ⋅ v / c ) , v ~ = v 1 − κ ⋅ v / c , {\displaystyle {\begin{aligned}d{\tilde {t}}'=&{\tilde {\gamma }}\left[1+\kappa \cdot {\tilde {\mathbf {v} }}/c-\kappa '\cdot {\tilde {\mathbf {v} }}'/c\right]d{\tilde {t}}-\left(\kappa '+{\tilde {\gamma }}{\tilde {\mathbf {v} }}'\right)\cdot d{\tilde {\mathbf {x} }}/c\\&-\left[{\tilde {\gamma }}\left(1+\kappa \cdot {\tilde {\mathbf {v} }}/c\right)-1\right]{\frac {\kappa '\cdot {\tilde {\mathbf {v} }}}{{\tilde {\mathbf {v} }}^{2}c}}{\tilde {\mathbf {v} }}\cdot d{\tilde {\mathbf {x} }}+{\tilde {\gamma }}\kappa \cdot {\tilde {\mathbf {v} }}\left(\kappa \cdot d{\tilde {\mathbf {x} }}\right)/c,\\d{\tilde {\mathbf {x} }}'=&-{\tilde {\gamma }}{\tilde {\mathbf {v} }}d{\tilde {t}}+d{\tilde {\mathbf {x} }}+\left[{\tilde {\gamma }}\left(1+\kappa \cdot {\tilde {\mathbf {v} }}/c\right)-1\right]{\frac {{\tilde {\mathbf {v} }}\cdot d\mathbf {x} }{{\tilde {\mathbf {v} }}^{2}}}{\tilde {\mathbf {v} }}-{\tilde {\gamma }}{\tilde {\mathbf {v} }}\left(\kappa \cdot d{\tilde {\mathbf {x} }}\right)/c,\\{\tilde {\gamma }}=&\gamma \left(1-\kappa \cdot \mathbf {v} /c\right),\\{\tilde {\mathbf {v} }}=&{\frac {\mathbf {v} }{1-\kappa \cdot \mathbf {v} /c}},\end{aligned}}}