Hauptseite > Publikationsdatenbank > Pion- und Photoabsorption an Kernen im Delta-Resonanzbereich > print |
001 | 848413 | ||
005 | 20210129234124.0 | ||
024 | 7 | _ | |a 2128/19057 |2 Handle |
037 | _ | _ | |a FZJ-2018-03649 |
041 | _ | _ | |a German |
088 | 1 | _ | |a Juel-2540 |
088 | _ | _ | |a Juel-2540 |2 JUEL |
100 | 1 | _ | |a Körfgen, Bernd |0 P:(DE-Juel1)132176 |b 0 |e Corresponding author |u fzj |
245 | _ | _ | |a Pion- und Photoabsorption an Kernen im Delta-Resonanzbereich |
260 | _ | _ | |a Jülich |c 1991 |b Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag |
300 | _ | _ | |a 91 p. |
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336 | 7 | _ | |a Report |b report |m report |0 PUB:(DE-HGF)29 |s 1529580456_9484 |2 PUB:(DE-HGF) |
336 | 7 | _ | |a TECHREPORT |2 BibTeX |
490 | 0 | _ | |a Berichte des Forschungszentrums Jülich |v 2540 |
520 | _ | _ | |a In charge-exchange reactions and in $\pi$-absorption at intermediate energies the $\Delta$ peak position in nuclei is shifted downwards in energy compared to the $\Delta$-excitation of the nucleon. For electromagnetic probes the experimental data do not show such a shift. We describe the excitation of the $\Delta$ in nuclei consistently for all these different probes using the isobar-hole-model ($\Delta$N$^{-1}$-model). The shift of the $\Delta$ peak position in chargeexchange reactions and in $\pi$-absorption is due to an attractive $\Delta$N$^{-1}$-residual interaction in the spin-longitudinal ($\overrightarrow{\sigma} \cdot \overrightarrow{q}$) channel. A $\Delta$N$^{-1}$-residual interaction consisting of the $\pi$-exchange potential alone is too attractive in the spin-longitudinal channel and shifts the $\Delta$ peak position for $\pi$-absorption to too low energies. In order to reproduce the $\Delta$ peak position we have to include short range correlations in the $\Delta$N$^{-1}$-residual interaction. This is done either by adding a $\delta$-force, parametrized through the Landau-Migdal-parameter g$^{'}_{\Delta \Delta}$, to the $\pi$-exchange potential, or by multiplying the $\pi$-exchange potential with a correlation-function. This leads to a repulsive $\Delta$N$^{-1}$-residual interaction in the spin-transverse ($\overrightarrow{\sigma}$ x $\overrightarrow{q}$) channel, which shifts the $\Delta$ peak position in the calculations for photo-absorption to higher energies compared to the photo-absorption on the nucleon. |
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856 | 4 | _ | |u https://juser.fz-juelich.de/record/848413/files/J%C3%BCl_2540_K%C3%B6rfgen.pdf |y OpenAccess |
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