Compton scattering on the proton, neutron, and deuteron in chiral perturbation theory to O(Q^4)

dc.creatorBeane, S. R.
dc.creatorMalheiro, M.
dc.creatorMcGovern, J. A.
dc.creatorPhillips, D. R.
dc.creatorvan Kolck, U.
dc.date2004-03-31
dc.date2004-07-30
dc.date.accessioned2026-07-07T13:05:13Z
dc.date.available2026-07-07T13:05:13Z
dc.descriptionWe study Compton scattering in systems with A=1 and 2 using chiral perturbation theory up to fourth order. For the proton we fit the two undetermined parameters in the O(Q^4) $γ$p amplitude of McGovern to experimental data in the region $ω,\sqrt{|t|} \leq 180$ MeV, obtaining a chi^2/d.o.f. of 133/113. This yields a model-independent extraction of proton polarizabilities based solely on low-energy data: alpha_p=12.1 +/- 1.1 (stat.) +/- 0.5 (theory) and beta_p=3.4 +/- 1.1 (stat.) +/- 0.1 (theory), both in units of 10^{-4} fm^3. We also compute Compton scattering on deuterium to O(Q^4). The $γ$d amplitude is a sum of one- and two-nucleon mechanisms, and contains two undetermined parameters, which are related to the isoscalar nucleon polarizabilities. We fit data points from three recent $γ$d scattering experiments with a chi^2/d.o.f.=26.6/20, and find alpha_N=13.0 +/- 1.9 (stat.) +3.9/-1.5 (theory) and a beta_N that is consistent with zero within sizeable error bars.
dc.description57 pages, 16 figures. Substantial changes. Correction of errors in deuteron calculation results in different values for isoscalar polarizabilities. Results for the proton are unaffected. Text modified to reflect this change, and also to clarify various points
dc.identifierhttps://arxiv.org/abs/nucl-th/0403088
dc.identifierhttp://arxiv.org/abs/nucl-th/0403088
dc.identifierNucl.Phys.A747:311-361,2005
dc.identifierdoi:10.1016/j.nuclphysa.2004.09.068
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/227422
dc.subjectNuclear Theory
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectNuclear Experiment
dc.titleCompton scattering on the proton, neutron, and deuteron in chiral perturbation theory to O(Q^4)
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