Chiral perturbation theory of the hyperfine splitting in (muonic) hydrogen.

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Title: Chiral perturbation theory of the hyperfine splitting in (muonic) hydrogen.
Authors: Hagelstein, Franziska1,2,3 (AUTHOR) hagelste@uni-mainz.de, Lensky, Vadim1 (AUTHOR), Pascalutsa, Vladimir1 (AUTHOR)
Source: European Physical Journal C -- Particles & Fields. Aug2023, Vol. 83 Issue 8, p1-18. 18p.
Subjects: Chiral perturbation theory, Hyperfine coupling, Hydrogen, Factor structure, Polynomial chaos, Minkowski space
Abstract: The ongoing experimental efforts to measure the hyperfine transition in muonic hydrogen prompt an accurate evaluation of the proton-structure effects. At the leading order in α , which is O (α 5) in the hyperfine splitting (hfs), these effects are usually evaluated in a data-driven fashion, using the empirical information on the proton electromagnetic form factors and spin structure functions. Here we perform a first calculation based on the baryon chiral perturbation theory (B χ PT). At leading orders it provides a prediction for the proton polarizability effects in hydrogen (H) and muonic hydrogen (μ H). We find large cancellations among the various contributions leading to, within the uncertainties, a zero polarizability effect at leading order in the B χ PT expansion. This result is in significant disagreement with the current data-driven evaluations. The small polarizability effect implies a smaller Zemach radius R Z , if one uses the well-known experimental 1S hfs in H or the 2S hfs in μ H. We, respectively, obtain R Z (H) = 1.010 (9) fm, R Z (μ H) = 1.040 (33) fm. The total proton-structure effect to the hfs at O (α 5) is then consistent with previous evaluations; the discrepancy in the polarizability is compensated by the smaller Zemach radius. Our recommended value for the 1S hfs in μ H is 182.640 (18) meV. [ABSTRACT FROM AUTHOR]
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Database: Engineering Source
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