The Shapiro delay has already been experimentally verified and used (see two examples at the end of this answer).
Let us assume a radio beam between $ A $ and $ B $ at radial coordinates $ r_A $ and $ r_B $ respectively from a massive object of mass $ M $, with the massive object "between" $ A $ and $ B $, and $ r_0 $ the minimum distance of the radio beam to the center of the massive object.
The two-way duration of the radio beam according to Newton theory is:
$$ T_{Newt}=\frac{2}{c}\left(\sqrt{r_A^2-r_0^2}+\sqrt{r_B^2-r_0^2}\right) $$
with $ c $ speed of the light in vacuum.
The two-way duration actually measured $ T $ is always greater than $ T_{Newt} $ and after a few calculations, whereas $ r_0\ll r_A $ and $ r_0\ll r_B $, the delay $ \Delta T $ - called Shapiro delay or light delay - can be defined as:
$$ T-T_{Newt}=\Delta T\simeq\frac{4GM}{c^3}\left[\ln{\left(\frac{4r_Ar_B}{r_0^2}\right)+1}\right]\ \ \ \ \ [1]$$
with $ G $ gravitational constant and $ M $ mass of the massive object.
Numerical examples:
$ [a] $ for a Mars probe, the maximum delay is around $ 0.24\ ms$. Thanks to the
Cassini probe, it was shown in 2003 that the delay of light is consistent with general relativity (i.e. formula $ [1] $) to within $ 2\ 10^{-5} $.
$ [b] $ in 2010, the Shapiro effect was used to precisely measure the mass of a neutron star in a binary system with a white dwarf. The neutron star is observed
as a pulsar. Once per orbit, the white dwarf passes in front of the neutron star and we then observe a delay of $ 25\ \mu s $ in arrival time of the pulses, which can be interpreted as the Shapiro effect
effect due to the gravitational field of the white dwarf. From this, we deduce the mass of the white dwarf and, via the orbital parameters, that of the neutron star: $ M=1.97\pm 0.04 $ mass of the Sun.
Hoping to have answered the question,
Best regards.