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000050386 0247_ $$2DOI$$a10.1103/PhysRevC.72.065211
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000050386 0247_ $$2arXiv$$aarXiv:nucl-th/0505083$$cnucl-th
000050386 0247_ $$2arXiv$$aarXiv:oai:arXiv.org:nucl-th/0505083
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000050386 035__ $$9arXiv$$anucl-th/0505083$$cnucl-th
000050386 035__ $$9arXiv$$aoai:arXiv.org:nucl-th/0505083$$zoai:arXiv.org:nucl-th/0505083
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000050386 084__ $$2WoS$$aPhysics, Nuclear
000050386 1001_ $$0P:(DE-Juel1)VDB59427$$aPolinder, H.$$b0$$uFZJ
000050386 245__ $$aSoft-core meson-baryon interactions. II. pi N and K+ N scattering
000050386 260__ $$aWoodbury, NY$$bInst.$$c2005
000050386 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2005-12-30
000050386 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2005-12-01
000050386 300__ $$a065211
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000050386 440_0 $$04921$$aPhysical Review C$$v72$$x0556-2813
000050386 500__ $$aRecord converted from VDB: 12.11.2012
000050386 520__ $$aThe 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.
000050386 536__ $$0G:(DE-Juel1)FUEK241$$2G:(DE-HGF)$$aPhysik der Hadronen$$cM01$$x0
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000050386 650_7 $$2INSPIRE$$api nucleon: elastic scattering
000050386 650_7 $$2INSPIRE$$aK+ nucleon: elastic scattering
000050386 650_7 $$2INSPIRE$$ameson: exchange
000050386 650_7 $$2INSPIRE$$abaryon: exchange
000050386 650_7 $$2INSPIRE$$apomeron: exchange
000050386 650_7 $$2INSPIRE$$amodel: potential
000050386 650_7 $$2INSPIRE$$asymmetry: SU(3)
000050386 650_7 $$2INSPIRE$$aeffective Hamiltonian
000050386 650_7 $$2INSPIRE$$aeffective Lagrangian
000050386 650_7 $$2INSPIRE$$arenormalization
000050386 650_7 $$2INSPIRE$$apartial wave analysis
000050386 650_7 $$2INSPIRE$$abaryon: mixing angle
000050386 650_7 $$2INSPIRE$$achannel cross section: energy dependence
000050386 650_7 $$2INSPIRE$$aangular distribution
000050386 650_7 $$2INSPIRE$$aTheta(1540)
000050386 650_7 $$2INSPIRE$$adifferential cross section
000050386 650_7 $$2INSPIRE$$atotal cross section
000050386 650_7 $$2INSPIRE$$anumerical calculations
000050386 650_7 $$2INSPIRE$$abibliography
000050386 7001_ $$0P:(DE-HGF)0$$aRijken, Th.$$b1
000050386 77318 $$2Crossref$$3journal-article$$a10.1103/physrevc.72.065211$$bAmerican Physical Society (APS)$$d2005-12-30$$n6$$p065211$$tPhysical Review C$$v72$$x0556-2813$$y2005
000050386 773__ $$0PERI:(DE-600)2844098-5$$a10.1103/PhysRevC.72.065211$$gVol. 72, p. 065211$$n6$$p065211$$q72<065211$$tPhysical review / C$$v72$$x0556-2813$$y2005
000050386 8567_ $$uhttp://hdl.handle.net/2128/1713$$uhttp://dx.doi.org/10.1103/PhysRevC.72.065211
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