A meson-exchange isobar model for the π+d↔pp reaction

1996 ◽  
Vol 74 (5-6) ◽  
pp. 209-225 ◽  
Author(s):  
L. Canton ◽  
G. Cattapan ◽  
P. J. Dortmans ◽  
G. Pisent ◽  
J. P. Svenne

We calculated a broad set of observables for the π+d ↔ pp reaction with a relatively simple meson-exchange isobar model. The comparison between the calculated results and experimental data (including spin observables) shows that the model gives an overall phenomenologically acceptable description of the reaction around the Δ resonance. We also take into account the effects due to the inclusion of the Galilei invariant (pseudovector) recoil term in the πNN vertex, of relativistic corrections to the ρ-exchange component of the ΔN transition potential, and of NN final state interaction in the π+d → p + p process. Rescatterings via pion-nucleon interaction in the S–wave have also been included. The model is sufficiently simple to be extended to the case of pion absorption on other light nuclei, in particular 3He (or tritium).

2003 ◽  
Vol 18 (02n06) ◽  
pp. 190-199 ◽  
Author(s):  
H. ARENHÖVEL ◽  
E. M. DARWISH ◽  
A. FIX ◽  
M. SCHWAMB

The present status of the theoretical description of electromagnetic reactions on the deuteron above pion threshold is reviewed. Three major topics are considered: (i) retardation effects in π-meson exchange contributions to NN-interaction and meson exchange currents in deuteron photodisintegration above π-threshold in the Δ-resonance region, (ii) off-shell effects in the one-body current treated in a simple pion cloud model in, deuteron photodisintegration in and above the Δ-resonance region, and (iii) final state interaction effects in photoproduction of π and η mesons on the deuteron.


Author(s):  
C. Schütz ◽  
J. W. Durso ◽  
K. Holinde ◽  
M. B. Johnson ◽  
B. C. Pearce ◽  
...  

1980 ◽  
Vol 92 (3-4) ◽  
pp. 261-264 ◽  
Author(s):  
E.Kh. Akhmedov ◽  
Yu.V. Gaponov ◽  
I.N. Mishustin

1977 ◽  
Vol 66 (5) ◽  
pp. 425-428 ◽  
Author(s):  
F. Hachenberg ◽  
J. Hüfner ◽  
H.J. Pirner

2003 ◽  
Vol 18 (02n06) ◽  
pp. 290-293 ◽  
Author(s):  
K. MIYAGAWA ◽  
T. MART ◽  
C. BENNHOLD ◽  
W. GLÖCKLE

Kaon photo- and electroproduction processes on the deuteron are investigated theoretically. Modern hyperon-nucleon forces as well as an updated kaon production operator on the nucleon are used. Sizable effects of the hyperon-nucleon final state interaction are seen in various observables.


1980 ◽  
Vol 63 (6) ◽  
pp. 2123-2126 ◽  
Author(s):  
S. Kurihara ◽  
A. Suzuki ◽  
Y. Takahashi ◽  
Y. Futami

1993 ◽  
Vol 08 (20) ◽  
pp. 3425-3455 ◽  
Author(s):  
A. N. IVANOV ◽  
N. I. TROITSKAYA ◽  
M. NAGY

The problem of bosonization of standard local four-quark operators, by involving the penguin operator, with ΔI = 1/2 and ΔS = 1 selection rules, is studied. We show that the well-known Cronin's operator determined within the effective chiral Lagrangian approach with nonlinear realization of chiral SU (3) × SU (3) symmetry (so-called chiral perturbation theory at the hadronic level) can realize the hadronic level description of local four-quark operators with (V − A) × (V − A) quark structure only. Also, it is shown that any attempts to apply Cronin's operator for bosonization of the penguin operator, possessing (V − A) × (V + A) quark structure, are doomed to failure. The latter is explained by the inability of Cronin's operator to describe correctly the s-wave final-state interaction, which is very important for transitions governed by the penguin operator. The asymmetry of quark condensate is calculated. The sign of this asymmetry is opposite to that one assumed in the framework of QCD sum rules.


2019 ◽  
Vol 34 (39) ◽  
pp. 1950322
Author(s):  
Marcello Baldo ◽  
Zahra Asadi Aghbolaghi ◽  
Isaac Vidaña ◽  
Mohsen Bigdeli

It has been found in previous works [M. Baldo and K. Fukukawa, Phys. Rev. Lett. 113, 241501 (2014); K. Fukukawa, M. Baldo, G. F. Burgio, L. Lo Monaco and H.-J. Schulze, Phys. Rev. 92, 065802 (2015)] that the nucleon–nucleon potential of [Y. Fujiwara, M. Kohno, C. Nakamoto and Y. Suzuki Phys. Rev. C 64, 054001 (2001); Y. Fujiwara et al., Phys. Rev. C 65, 014002 (2001)] gives an accurate saturation point in symmetric nuclear matter once the three hole-line contributions are included in the Brueckner–Bethe–Goldstone expansion without the addition of three-body forces in the nuclear Hamiltonian. The potential is based on a quark model of nucleons and on the quark–quark interaction together with quark exchange processes. These features introduce an intrinsic nonlocality of the nucleon–nucleon interaction. In order to clarify the role of the quark degrees of freedom and of the nonlocality in the saturation, we perform a comparative study of this potential and the traditional meson exchange models, exemplified in the CD-Bonn potential. We find that at the Brueckner–Hartree–Fock approximation, which corresponds to the two hole-line level of approximation, the dominant modification of the nucleon–nucleon interaction with respect to CD-Bonn is incorporated in the s-wave channels, where the quark degrees of freedom should be more relevant, in particular for the short range quark exchange processes. However, when the three hole-line contribution is included, we find that the higher partial waves play a relevant role, mainly in the term that describes the effect of the medium on the off-shell propagation of the nucleon.


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