Going back to the first measurements of a muonic atom, Oct 2010, we have
> For the transition, they needed look no further than a Lamb shift. A Lamb shift occurs when an electron moves between the 2s and 2p energy levels in an atom. The difference in binding energy between the two is very small, and leaves little room for external effects to muck up the measurements. The researchers found that the muonic hydrogen needed to be shot with a laser with a frequency of 50 terahertz in order to transition up to the 2p state. When they plugged this measurement into a quantum electrodynamics equation that relates proton radius to binding energies, they found the needed energy indicated a proton radius of 0.841 femtometers—four percent smaller and five standard deviations off the currently accepted radius of 0.876 femtometers.
From way back, even with the normal hydrogen atom the Lamb shift has been infamous. Explaining the precise measured value defeated more than one Nobel prizewinning physicist (including Dirac) before Hans Bethe (I think) got it right. Its precise value required the mathematics of the renormalization of mass (an electron changes mass due to the cloud of virtual particles in the vacuum it sits in). The Lamb shift currently provides a measurement of the fine-structure constant α to better than one part in a million.
More on the Lamb shift at https://en.wikipedia.org/wiki/Lamb_shift
Now, where does the radius of the proton appear in all this mathematics?
Possibly in this way.
“This result diverges when no limits about the integral (at both large and small frequencies). As mentioned above, this method is expected to be valid only when ν > πc/a0, or equivalently k > π/a0. Therefore, we can choose the upper and lower limit of the integral and these limits make the result converge.” Here a0 is the Bohr radius https://en.wikipedia.org/wiki/Bohr_radius
“The Bohr radius (a0) is a physical constant, approximately equal to the most probable distance between the proton and electron in a hydrogen atom in its ground state. In the simplest atom, hydrogen, a single electron orbits the nucleus and its smallest possible orbit, with lowest energy, has an orbital radius almost equal to the Bohr radius. (It is not exactly the Bohr radius due to the reduced mass effect. They differ by about 0.1%.) The Bohr radius including the effect of reduced mass in the hydrogen atom depends on the Compton wavelength of the proton, effectively the proton’s size.
Could it be, I wonder, that what we’re seeing here is a change in the mean distance between the proton and orbiting particle (electron or muon) due to the induced movement of the proton (or quarks within the proton)? A muon, because of its larger mass, orbits close and so the induced motion of the proton is larger than that due to the electron. This would change the Bohr radius of the hydrogen atom slightly and hence (this is only a wild guess, remember) the effective radius of the proton. It’s a thought, but if this was the case then that would also change our interpretation of the Lamb shift for the normal hydrogen atom, which would totally put the wind up the whole of QED. ie. They broke physics.
Unless their experiment is wrong.
So, let’s go back to the original muon hydrogen paper from 2010.
http://www.nature.com/nature/journal/v466/n7303/full/nature09250.html
“The size of the proton” by Pohl et al. in Nature.
Summary:
> The root-mean-square charge radius, r_p, has been determined with an accuracy of 2% (at best) by electron–proton scattering experiments. To 1%, this value is based mainly on precision spectroscopy of atomic hydrogen. Here we use pulsed laser spectroscopy to measure a muonic Lamb shift. Our result implies that either the Rydberg constant has to be shifted, or the calculations of the QED effects in atomic hydrogen or muonic hydrogen atoms are insufficient. The muon is about 200 times heavier than the electron. The atomic Bohr radius is correspondingly about 200 times smaller. S states are shifted because the muon’s wavefunction at the location of the proton is non-zero. In contrast, P states are not significantly shifted (Note: remember your S,P,D etc orbitals, the Lamb shift is the energy difference between the S and P orbitals).
> The Lamb shift in muonic hydrogen is the sum of radiative, recoil, and proton structure contributions
OK, so in the paper they’ve already considered and eliminated both of my wild guesses above, the induced motion of the proton and the induced motion of the quarks. In fact, it turns out that ONLY these are related to the radius of the proton. So my wild guess above was the opposite of the solution, it was the problem. The induced motion of the proton is proportional to the radius of the proton squared and the induced motion of the quarks is proportional to the radius of the proton cubed.
I don’t see any fundamental flaw in the experiment or results.
Short of having an expert in fundamental physics look at these results, I have to agree that they broke physics. The most reasonable explanation I can see is that their assumed constant attached to “the radius of the proton cubed” is wrong. That would be an error not in QED but on QCD, which is easier to stomach.