2006
DOI: 10.1016/j.aop.2006.02.009
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Effective Lagrangian Approach to pion photoproduction from the nucleon

Abstract: We present a pion photoproduction model on the free nucleon based on an Effective Lagrangian Approach (ELA) which includes the nucleon resonances ($\Delta(1232)$, N(1440), N(1520), N(1535), $\Delta (1620)$, N(1650), and $\Delta (1700)$), in addition to Born and vector meson exchange terms. The model incorporates a new theoretical treatment of spin-3/2 resonances, first introduced by Pascalutsa, avoiding pathologies present in previous models. Other main features of the model are chiral symmetry, gauge invarian… Show more

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Cited by 58 publications
(109 citation statements)
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References 94 publications
(226 reference statements)
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“…The internal structure of the nucleonic excitations shows up in the values of the electromagnetic coupling constants that appear in the Lagrangian. The model displays chiral symmetry, gauge invariance, and crossing symmetry, and incorporates a consistent treatment of the interaction with spin-3/2 particles that avoids well-known pathologies of previous models [13,14,21]. Furthermore, the dressing of the resonances is considered by means of a phenomenological width which takes into account decays into one and two π 's and one η.…”
Section: The Reaction Modelmentioning
confidence: 99%
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“…The internal structure of the nucleonic excitations shows up in the values of the electromagnetic coupling constants that appear in the Lagrangian. The model displays chiral symmetry, gauge invariance, and crossing symmetry, and incorporates a consistent treatment of the interaction with spin-3/2 particles that avoids well-known pathologies of previous models [13,14,21]. Furthermore, the dressing of the resonances is considered by means of a phenomenological width which takes into account decays into one and two π 's and one η.…”
Section: The Reaction Modelmentioning
confidence: 99%
“…We prefer to use the helicity amplitudes (for their definition and connection with coupling constants see Refs. [13,14,20]) to define the ranges, instead of the electromagnetic coupling constants. We allow them to vary in the range [−1, 1] GeV −1/2 .…”
Section: Minimization Strategymentioning
confidence: 99%
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“…This choice is due to the fact that, since the total cross section of the π 0 production off the proton is very small close to threshold, the ∆(1232) resonance could have a quite important contribution [15], whose effect becomes ever clearer when moving to energies closer to its mass [16]. The effect of the inclusion of this resonance has been thoroughly studied in [17][18][19][20][21][22][23][24]. We show that, although we are not including any additional fitting constants, the dynamics of the ∆(1232) resonance is a sufficient addition to well describe the experimental input even at photon energies higher than 200 MeV.…”
Section: Introductionmentioning
confidence: 99%