This is the rms electric charge radius, $\sqrt {\langle r{}^{2}_{E}\rangle }$.
There are three kinds of measurements of the proton radius: via transitions in atomic hydrogen; via electron scattering off hydrogen; and via muonic hydrogen Lamb shift. Most measurements of the radius of the proton involve electron-proton interactions, the most recent of which is the electron scattering measurement ${{\mathit r}_{{{p}}}}$ = 0.831(14) fm (
XIONG 2019), and the atomic-hydrogen value, ${{\mathit r}_{{{p}}}}$ = 0.833(10) fm (
BEZGINOV 2019). These agree well with another recent atomic-hydrogen value ${{\mathit r}_{{{p}}}}$ = 0.8335(95) fm (
BEYER 2017), and with the best measurement using muonic hydrogen ${{\mathit r}_{{{p}}}}$ = 0.84087(39) fm (
ANTOGNINI 2013), that is far more precise.
The
MOHR 2016 value (2014 CODATA), obtained from the electronic results available at the time, was 0.8751(61) fm. This differs by 5.6 standard deviations from the muonic hydrogen value, leading to the so-called proton charge radius puzzle. See our 2018 edition (Physical Review D98 030001 (2018)) for a further discussion of interpretations of this puzzle. However, reflecting the new electronic measurements, the 2018 CODATA,
TIESINGA 2021, recommended value is 0.8414(19) fm, and the puzzle appears to be resolved.
See our 2014 edition (Chinese Physics C38 070001 (2014)) for values published before 2003.