Measuring the size of the proton

9th July 2012 Andrea Vacchi, Andrzej Adamczak, Benjamin Andreson, Dimitar Bakalov, Michail Stoilov, Giuseppe Battistoni, Nandini Bhattacharya, Paul Urbach, Mirko Boezio, Walter Bonvicini, Nicola Zampa, Maurizio Bonesini, Miltcho Danailov, Alexander Demidovich, Milohum Dzagli, Komlan Gadedjisso-Tossou, Joe Niemela, Lyubomir Stoychev, Kumar…

9th July 2012

Andrea Vacchi, Andrzej Adamczak, Benjamin Andreson, Dimitar Bakalov, Michail Stoilov, Giuseppe Battistoni, Nandini Bhattacharya, Paul Urbach, Mirko Boezio, Walter Bonvicini, Nicola Zampa, Maurizio Bonesini, Miltcho Danailov, Alexander Demidovich, Milohum Dzagli, Komlan Gadedjisso-Tossou, Joe Niemela, Lyubomir Stoychev, Kumar Sumeet and Roberta Ramponi

An experiment to study an exotic atom with infrared spectroscopy will measure a fundamental parameter related to the spatial dimensions of a proton.
The size of an atom’s nucleus is roughly five orders of magnitude smaller than the size of the atom. Consequently, the nuclear corrections to atomic energy levels are very tiny. However, these corrections have become important in recent high-precision measurements of transitions in the hydrogen atom, which are being performed to test quantum electrodynamics (QED) and to determine related fundamental constants. Today, the interpretation of this data is only limited by the uncertainties in the size of the nucleus, which in the case of hydrogen is a single proton.

The charge radius rp of the proton is a physical parameter that characterizes important aspects of the effective size of the proton. Its value is used together with the Rydberg constant in the calculations of bound-state QED involving hydrogen atoms as well as muonic hydrogen atoms that have a muon orbiting the nucleus rather than the electron. (Muons are like electrons but 200 times heavier.) A recent spectroscopic study of muonic hydrogen resulted in a new measurement of the proton root mean square (rms) charge radius. The reported value, rp=0.84184(67)fm, differs by 5 standard deviations from (and is a factor of 10 more precise than) previous determinations. These earlier values come from three very different methods that are based mostly on electronic hydrogen data. Specifically, a compilation of physical constants (CODATA) gives rp=0.8768(69)fm, the Lamb shift of electronic hydrogen results in rp=0.883(14)fm, and electron scattering from hydrogen yields rp=0.895(18)fm. It is noteworthy that QED considerations show that the electron scattering experiments and the atomic hydrogen spectroscopy determine the same radius. Discussions about the correctness of the theory, experiments, or the adequacy of the models are not leading to satisfactory explanations of this relevant discrepancy.

One way to address the disagreements over the proton charge radius is to measure a different but complementary aspect of the proton electromagnetic structure. The proton Zemach radius, Rp, is a fundamental parameter related to the spatial distribution of both the electric charge and the magnetic moment of the proton. The value of the Zemach radius (and its uncertainty) set limits on the value and uncertainty of the proton charge radius, and vice versa. A measurement of the Zemach radius will, therefore, impose restrictions on the proton charge distribution that will exclude one of the currently competing values of the proton charge radius or part of the models used in the calculations. Alternatively, it will lead to some new conclusions.

There exist three possibilities to determine the numerical value of Rp. One approach based on the analysis of the world data on electron-proton scattering gives Rp=1.086±0.012fm. Another method uses the comparison of theoretical and experimental results for the hydrogen atom to obtain Rp=1.037(16)fm, or a similar value. We suggest a third method, based on the comparison of experimental data and theoretical results for muonic hydrogen. Similar to the recent proton charge radius experiment performed at the Paul Scherrer Institute, our proposed experiment is a spectroscopic investigation of muonic hydrogen that targets a different transition. In particular, we aim to measure the hyperfine splitting of the ground state energy level of muonic-hydrogen by inducing a laser-stimulated singlet-to-triplet transition (3S11S0), as suggested in previous works.

The basic outline of the experimental design is as follows. To produce the muonic hydrogen, pulses from an intense, low energy muon beam strike a hydrogen target. The target shall have cylindrical symmetry, with a cross section on the order of a few square centimeters and a length of a few centimeters. The muon beam pulses should have a repetition rate of 50Hz and a pulse duration of 70ns. Measuring the energy difference (3S11S0) in the muonic hydrogen requires a tunable laser source at a mid-IR wavelength of 6785nm and a line-width <0.07nm, tunable in the range 6785+xxx−3nm with a high power output. All of these parameters will be subject to further simulation and optimization to reach the final experimental set up.

At present, the main experimental challenge is the realization of the laser source, together with a suitably designed external multi-pass cavity to achieve sufficient transition probability and signal-to-noise ratio. We are pursuing two different approaches. In the first, we consider a set-up based on one or more properly engineered distributed-feedback quantum cascade lasers (QCLs). We acquired suitable QCLs and fully characterized them. Our results show that these sources are stable and simple to operate. They are also tunable over the specified wavelength range, with a satisfactory line-width. One limitation is the delivered energy density, so we are investigating how matrixes of QCLs might operate.

In the second approach, we are studying the realization of a tunable, narrow-bandwidth mid-IR source based on a nonlinear optical system. Different nonlinear crystals and frequency down-conversion schemes are under evaluation and testing.

In summary, our present task is to demonstrate the feasibility of a laser source able to induce a sufficient transition probability for the (3S11S0) hyperfine splitting of muonic hydrogen atoms produced in a suitable system of hydrogen target, optical-cavity, and muon beam. The successive step will be to plan and execute this high-precision spectroscopic experiment. It is worth noting that while the development of a source for a highly sensitive system in the mid-IR is important for our experiment, it also has potential impact on medical applications and gas detection in security and environmental monitoring. Such wide applicability should stimulate industrial implementation.