Pion elastic scattering from polarizedC13in the energy region of theP33resonance

Autor:	Christopher Morris, M. A. Khandaker, R. Ivie, E. Insko, H. Ward, S. I. Penttilä, G. R. Burleson, S. M. Sterbenz, T. Averett, Gerald W Hoffmann, M. Purcell, D. Dehnhard, Soumya Chakravarti, Barry Ritchie, Y. F. Yen, K. Cranston, Yi Ju Yu, J. R. Comfort, J. A. Faucett, N. Tanaka, A. L. Williams, K. Johnson, Steven J. Greene, J. Görgen, C. F. Moore, J. Tinsley, B. Brinkmöller, J. M. O’Donnell, J. J. Jarmer, M. A. Franey, A. Klein, D. A. Smith, J. A. McGill, B. Berman, G. S. Kyle, H. T. Fortune, Martin L Barlett, Ricardo Alarcon
Rok vydání:	1994
Předmět:	Physics Elastic scattering Nuclear and High Energy Physics Scattering Isoscalar Nuclear Theory Momentum transfer Resonance (particle physics) Nuclear physics Scattering amplitude Pion Condensed Matter::Strongly Correlated Electrons Atomic physics Born approximation
Zdroj:	Physical Review C. 50:897-908
ISSN:	1089-490X 0556-2813
DOI:	10.1103/physrevc.50.897
Popis:	A new development in polarized nuclear-target technology has made it possible to measure analyzing power, Ay, in pion elastic scattering from a polarized target.[1] Such measurements provide us with information on the isoscalar spin-flip strength of the nuclear transition which is very difficult to obtain otherwise. Differential cross sections, σ(Θ), for pion elastic scattering from nuclei with non-zero spin are dominated by the spin-independent (∆S = 0) amplitudes. Contributions from the spin-dependent (∆S = 1) amplitudes are usually negligible because σ(Θ) depends on the sum of the squares of those amplitudes. However, the Ay depend on the interference on the spin-independent and spin-dependent scattering amplitudes and are therefore quite sensitive to the spin-dependent forms.
Databáze:	OpenAIRE
Externí odkaz:	https://explore.openaire.eu/search/publication?articleId=doi_________::5d9e3ecbbf0058ee551dc4233d90bc38 https://doi.org/10.1103/physrevc.50.897 Zobrazit plný text záznamu