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| 001 | 50386 | ||
| 005 | 20240610120956.0 | ||
| 017 | _ | _ | |a This version is available at the following Publisher URL: http://prc.aps.org |
| 024 | 7 | _ | |a 10.1103/PhysRevC.72.065211 |2 DOI |
| 024 | 7 | _ | |a WOS:000234337400088 |2 WOS |
| 024 | 7 | _ | |a arXiv:nucl-th/0505083 |c nucl-th |2 arXiv |
| 024 | 7 | _ | |a arXiv:oai:arXiv.org:nucl-th/0505083 |2 arXiv |
| 024 | 7 | _ | |a 2128/1713 |2 Handle |
| 035 | _ | _ | |a nucl-th/0505083 |9 arXiv |c nucl-th |
| 035 | _ | _ | |a oai:arXiv.org:nucl-th/0505083 |9 arXiv |z oai:arXiv.org:nucl-th/0505083 |
| 035 | _ | _ | |9 DESY |z D05-10433 |
| 035 | _ | _ | |9 SPIRESTeX |z Polinder:2005sn |
| 037 | _ | _ | |a PreJuSER-50386 |
| 041 | _ | _ | |a eng |
| 082 | _ | _ | |a 530 |
| 084 | _ | _ | |a Physics, Nuclear |2 WoS |
| 100 | 1 | _ | |a Polinder, H. |b 0 |u FZJ |0 P:(DE-Juel1)VDB59427 |
| 245 | _ | _ | |a Soft-core meson-baryon interactions. II. pi N and K+ N scattering |
| 260 | _ | _ | |a Woodbury, NY |b Inst. |c 2005 |
| 264 | _ | 1 | |3 online |2 Crossref |b American Physical Society (APS) |c 2005-12-30 |
| 264 | _ | 1 | |3 print |2 Crossref |b American Physical Society (APS) |c 2005-12-01 |
| 300 | _ | _ | |a 065211 |
| 336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a Output Types/Journal article |2 DataCite |
| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 336 | 7 | _ | |a JOURNAL_ARTICLE |2 ORCID |
| 336 | 7 | _ | |a article |2 DRIVER |
| 440 | _ | 0 | |a Physical Review C |x 0556-2813 |0 4921 |v 72 |
| 500 | _ | _ | |a Record converted from VDB: 12.11.2012 |
| 520 | _ | _ | |a The pi N potential includes the t-channel exchanges of the scalar mesons sigma and f(0), vector meson rho, tensor mesons f(2) and f(2)('), and the Pomeron as well as the s- and u-channel exchanges of the nucleon N and the resonances Delta, Roper, and S-11. These baryonic resonances are not generated dynamically. We consider them, at least partially, as genuine three-quark states, and we treat them in the same way as the nucleon. The Roper and S-11 resonances were needed to find the proper behavior of the phase shifts at higher energies in the corresponding partial waves. The soft-core pi N model gives an excellent fit to the empirical pi N S- and P-wave phase shifts up to T-lab=600 MeV. Also, the scattering lengths have been reproduced well, and the soft-pion theorems for low-energy pi N scattering are satisfied. The soft-core model for the K+N interaction is an SUf(3) extension of the soft-core pi N model. The K+N potential includes the t-channel exchanges of the scalar mesons a(0),sigma, and f(0), vector mesons rho,omega, and phi, tensor mesons a(2),f(2), and f(2)('), and the Pomeron as well as u-channel exchanges of the hyperons Lambda,Sigma,Sigma(1385), and Lambda(1405). The fit to the empirical K+N S-, P-, and D-wave phase shifts up to T-lab=600 MeV is reasonable and certainly reflects the present state of the art. Since the various K+N phase shift analyses are also not very consistent, scattering observables are also compared with the soft-core K+N model. A good agreement for the total and differential cross sections as well as the polarizations is found. |
| 536 | _ | _ | |a Physik der Hadronen |c M01 |2 G:(DE-HGF) |0 G:(DE-Juel1)FUEK241 |x 0 |
| 542 | _ | _ | |i 2005-12-30 |2 Crossref |u http://link.aps.org/licenses/aps-default-license |
| 588 | _ | _ | |a Dataset connected to Web of Science |
| 650 | _ | 7 | |a pi nucleon: elastic scattering |2 INSPIRE |
| 650 | _ | 7 | |a K+ nucleon: elastic scattering |2 INSPIRE |
| 650 | _ | 7 | |a meson: exchange |2 INSPIRE |
| 650 | _ | 7 | |a baryon: exchange |2 INSPIRE |
| 650 | _ | 7 | |a pomeron: exchange |2 INSPIRE |
| 650 | _ | 7 | |a model: potential |2 INSPIRE |
| 650 | _ | 7 | |a symmetry: SU(3) |2 INSPIRE |
| 650 | _ | 7 | |a effective Hamiltonian |2 INSPIRE |
| 650 | _ | 7 | |a effective Lagrangian |2 INSPIRE |
| 650 | _ | 7 | |a renormalization |2 INSPIRE |
| 650 | _ | 7 | |a partial wave analysis |2 INSPIRE |
| 650 | _ | 7 | |a baryon: mixing angle |2 INSPIRE |
| 650 | _ | 7 | |a channel cross section: energy dependence |2 INSPIRE |
| 650 | _ | 7 | |a angular distribution |2 INSPIRE |
| 650 | _ | 7 | |a Theta(1540) |2 INSPIRE |
| 650 | _ | 7 | |a differential cross section |2 INSPIRE |
| 650 | _ | 7 | |a total cross section |2 INSPIRE |
| 650 | _ | 7 | |a numerical calculations |2 INSPIRE |
| 650 | _ | 7 | |a bibliography |2 INSPIRE |
| 700 | 1 | _ | |a Rijken, Th. |b 1 |0 P:(DE-HGF)0 |
| 773 | 1 | 8 | |a 10.1103/physrevc.72.065211 |b American Physical Society (APS) |d 2005-12-30 |n 6 |p 065211 |3 journal-article |2 Crossref |t Physical Review C |v 72 |y 2005 |x 0556-2813 |
| 773 | _ | _ | |a 10.1103/PhysRevC.72.065211 |g Vol. 72, p. 065211 |p 065211 |n 6 |q 72<065211 |0 PERI:(DE-600)2844098-5 |t Physical review / C |v 72 |y 2005 |x 0556-2813 |
| 856 | 7 | _ | |u http://dx.doi.org/10.1103/PhysRevC.72.065211 |u http://hdl.handle.net/2128/1713 |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/50386/files/78660.pdf |y OpenAccess |
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| 913 | 1 | _ | |k M01 |v Physik der Hadronen |l Physik der Hadronen |b Materie |0 G:(DE-Juel1)FUEK241 |x 0 |
| 914 | 1 | _ | |y 2005 |
| 915 | _ | _ | |0 StatID:(DE-HGF)0010 |a JCR/ISI refereed |
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| 920 | 1 | _ | |k IKP-TH |l Institut 3 (Theoretische Kernphysik) |d 31.12.2006 |g IKP |0 I:(DE-Juel1)VDB223 |x 0 |
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