Elastic photonuclear cross sections for bremsstrahlung from relativistic ions
Autor: | Ulrik I. Uggerhøj, R. E. Mikkelsen, Allan Sørensen |
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Jazyk: | angličtina |
Rok vydání: | 2015 |
Předmět: |
Physics
Elastic scattering Nuclear and High Energy Physics Photon Nuclear Theory 010308 nuclear & particles physics Scattering Bremsstrahlung Absorption cross section FOS: Physical sciences Optical theorem 01 natural sciences Nuclear Theory (nucl-th) Nuclear physics Dipole 0103 physical sciences Nuclear cross section Atomic physics 010306 general physics Instrumentation |
Zdroj: | Mikkelsen, R E, Sørensen, A H & Uggerhøj, U I 2016, ' Elastic photonuclear cross sections for bremsstrahlung from relativistic ions ', Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, vol. 372, pp. 58-66 . https://doi.org/10.1016/j.nimb.2016.02.003 |
DOI: | 10.1016/j.nimb.2016.02.003 |
Popis: | In this paper, we provide a procedure to calculate the bremsstrahlung spectrum for virtually any relativistic bare ion with charge 6e or beyond, Z ⩾ 6 , in ultraperipheral collisions with target nuclei. We apply the Weizsacker–Williams method of virtual quanta to model the effect of the distribution of nuclear constituents on the interaction of the ion with the radiation target. This leads to a bremsstrahlung spectrum peaking at 2 γ times the energy of the giant dipole resonance ( γ is the projectile energy in units of its rest energy). A central ingredient in the calculation is the cross section for elastic scattering of photons on the ion. This is only available in the literature for a few selected nuclei and, usually, only in a rather restricted parameter range. Hence we develop a procedure applicable for all Z ⩾ 6 to estimate the elastic scattering. The elastic cross section is obtained at low to moderate photon energies, somewhat beyond the giant dipole resonance, by means of the optical theorem, a dispersion relation, and data on the total absorption cross section. The cross section is continued at higher energies by invoking depletion due to loss of coherence in the scattering. Our procedure is intended for any ion where absorption data is available and for moderate to high energies, γ ≳ 10 . |
Databáze: | OpenAIRE |
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