Mansouri & Sexl
[1] consider a "test theory" of relativity in which the transformation between two frames is postulated to be\begin{align}<br />
t &= a(v)\,T + \epsilon(v)\,x\\<br />
x &= b(v)\,(X - vT)<br />
\end{align}where
a,
b and
ε are unknown functions to be determined by experiment. (Note: the first equation intentionally contains
x, not
X.) Special relativity is a special case of this test theory for a particular choice of these three functions. Experiments to test the validity of relativity can be performed from which the values of
a(
v),
b(
v) and
ε(
v) can be estimated. If the experimental values match the values predicted by SR, this is a confirmation of SR.
Mansouri and Sexl point out that the function
ε(
v) depends on the clock sync convention chosen, whereas
a(
v) and
b(
v) are both independent of sync convention. Under these assumptions, they go on to prove a result (pp.506–508) that
slow clock transport and Einstein synchronisation are equivalent if and only if a(v) takes the value predicted by SR, viz<br />
a(v) = \sqrt{1 - v^2/c^2}<br />To avoid any misunderstanding, the term "slow clock transport" is defined to mean in the limit as the speed of clock transport tends to zero (as others have pointed out).
Thus, if you sync clocks by slow clock transport and then measure the one-way speed of light, if you get an answer of
c regardless of direction, you have experimentally confirmed that
a(
v) takes the value predicted by SR.
Reference
[1] Mansouri, R and Sexl, R U (1977), "A Test Theory of Special Relativity: I. Simultaneity and Clock Synchronization",
General Relativity and Gravitation 8 (7), pp.497–513, Bibcode:
1977GReGr...8..497M, DOI:
10.1007/BF00762634
Further reading
Test theories of special relativity,
Wikipedia