Abstract

Experimental measurements of muonic hydrogen bound states have recently started to take place and provide a powerful setting in which to study the properties of QCD. We profit from the power of effective field theories (EFTs) to provide a theoretical framework in which to study muonic hydrogen in a model independent fashion. In particular, we compute expressions for the Lamb shift and the hyperfine splitting. These expressions include the leading logarithmic O (mμ α 6 ) terms, as well as the leading hadronic effects. Most remarkably, our analyses include the determination of the spin-dependent and spin-independent structure functions of the forward virtualphoton Compton tensor of the proton to O (p 3 ) in HBET and including the Delta particle. Using these results we obtain the leading hadronic contributions to the Wilson coeffcients of the lepton-proton four fermion operators in NRQED. The spin-independent coeffcient yields a pure prediction for the two-photon exchange contribution to the muonic hydrogen Lamb shift, which is the main source of uncertainty in our computation. The spindependent coeffcient yields the prediction of the hyperfine splitting. The use of EFTs crucially helps us organizing the computation, in such a way that we can clearly address the parametric accuracy of our result. Furthermore, we review in the context of NRQED all the contributions to the energy shift of O (mμ α 5 , as well as those that scale like mr α 6 × logarithms.

Highlights

  • In these proceedings we study those systems composed by a lepton and a proton which are weakly bounded by the electromagnetic force, and in particular muonic hydrogen

  • We devote most of our effort to the hadronic effects that arise from the two photon exchange (TPE) in the last term in Eq (8)

  • We develop the N3LO NRQED potential for different masses. We apply this computation to muonic hydrogen, and in particular to its Lamb shift and hyperfine splitting, for which we obtain a theoretical prediction in a model independent way in an effective field theories (EFTs) framework

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Summary

Introduction

In these proceedings we study those systems composed by a lepton and a proton which are weakly bounded by the electromagnetic force, and in particular muonic hydrogen. Hadronic information is encoded in the interaction of the baryon and the lepton it is bounded to, when one takes into account the effects of the hadron’s finite size They are a good place to learn about the physics inside hadrons upon comparison with experimental measurements. This is known as heavy baryon chiral perturbation theory (HBChPT) In this setting, we include the Delta particle ∆(1232), which is only ∼300 MeV away from the nucleon mass and couples strongly to the pion-nucleon sector. For the physics of our interest we can integrate out the soft scales obtaining a theory for ultrasoft photons, namely pNRQED [5] This theory has the proper degrees of freedom to describe systems such as positronium, muonium, hydrogen, muonic hydrogen, etc

Muonic Hydrogen
The Lamb shift and the proton radius
QED corrections
Hadronic effects
The hyperfine splitting
The HF splitting in hydrogen
The HF splitting in muonic hydrogen
Findings
Conclusions

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