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Elastic electron–proton scattering (e–p) and the spectroscopy of hydrogen atoms are the two methods traditionally used to determine the proton charge radius,
r
p
. In 2010, a new method using muonic hydrogen atoms
1
found a substantial discrepancy compared with previous results
2
, which became known as the ‘proton radius puzzle’. Despite experimental and theoretical efforts, the puzzle remains unresolved. In fact, there is a discrepancy between the two most recent spectroscopic measurements conducted on ordinary hydrogen
3
,
4
. Here we report on the proton charge radius experiment at Jefferson Laboratory (PRad), a high-precision e–p experiment that was established after the discrepancy was identified. We used a magnetic-spectrometer-free method along with a windowless hydrogen gas target, which overcame several limitations of previous e–p experiments and enabled measurements at very small forward-scattering angles. Our result,
r
p
= 0.831 ± 0.007
stat
± 0.012
syst
femtometres, is smaller than the most recent high-precision e–p measurement
5
and 2.7 standard deviations smaller than the average of all e–p experimental results
6
. The smaller
r
p
we have now measured supports the value found by two previous muonic hydrogen experiments
1
,
7
. In addition, our finding agrees with the revised value (announced in 2019) for the Rydberg constant
8
—one of the most accurately evaluated fundamental constants in physics.
A magnetic-spectrometer-free method for electron–proton scattering data reveals a proton charge radius 2.7 standard deviations smaller than the currently accepted value from electron–proton scattering, yet consistent with other recent experiments.