Chiral corrections to processes at low energies
arXiv:1007.5277 · doi:10.1016/j.nuclphysa.2010.08.014
Abstract
We calculate in chiral perturbation theory the double-pion photoproduction processes and at low energies. At leading order these reactions are governed by the chiral pion-pion interaction. The next-to-leading order corrections arise from pion-loop diagrams and chiral-invariant counterterms involving the low-energy constants and . The pertinent production amplitudes and depending on five kinematical variables are given in closed analytical form. We find that the total cross section for neutral pion-pair production gets enhanced in the region by a factor by the next-to-leading order corrections. In contrast to this behavior the total cross section for charged pion-pair production remains almost unchanged in the region in comparison to its tree-level result. Although the dynamics of the pion-pair production reactions is much richer, this observed pattern can be understood from the different influence of the chiral corrections on the pion-pion final state interaction ( versus ). We present also results for the complete set of two-pion invariant mass spectra. The predictions of chiral perturbation theory for the processes can be tested by the COMPASS experiment which uses Primakoff scattering of high-energy pions in the Coulomb field of a heavy nucleus to extract cross sections for reactions with various final states.
arXiv comment19 pages, 14 figures, submitted to Nuclear Physics A
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Cited by in corpus (8)
- Anomalous decay and scattering processes of the eta meson
- Light-Meson Spectroscopy with COMPASS
- First Measurement of Chiral Dynamics in π^- γ-> π^- π^- π^+
- Hadron Spectroscopy with COMPASS -- Newest Results
- Measurement of radiative widths of and
- Radiative corrections to neutral pion-pair production
- Consistency tests of AMPCALCULATOR and chiral amplitudes in SU(3) Chiral Perturbation Theory: A tutorial based approach
- Radiative corrections to the charged pion-pair production process {\boldmath} at low energies