Dynamical coupled-channels effects on pion photoproduction

Juliá-Dı́az, B.; Lee, T.-S. H.; Matsuyama, Akihiko; Satô, Tôru; Smith, L. C.

doi:10.1103/physrevc.77.045205

Cited by 122 publications

(265 citation statements)

References 36 publications

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“…The amplitude A 3/2 is significantly underestimated in all quark models for Q 2 < 2 GeV 2 . Dynamical models predict large meson-cloud contributions to this amplitude [83] that could explain the discrepancy.…”

Section: N(1520) D 13 Resonancementioning

confidence: 99%

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Electroexcitation of nucleon resonances from CLAS data on single pion electroproduction

Aznauryan¹,

Burkert²,

Biselli³

et al. 2009

Phys. Rev. C

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252

380

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We present results on the electroexcitation of the low mass resonances (1232)P 33 , N (1440)P 11 , N (1520)D 13 , and N (1535)S 11 in a wide range of Q 2 . The results were obtained in the comprehensive analysis of data from the Continuous Electron Beam Accelerator Facility (CEBAF) large acceptance spectrometer (CLAS) detector at the Thomas Jefferson National Accelerator Facility (JLab) on differential cross sections, longitudinally polarized beam asymmetries, and longitudinal target and beam-target asymmetries for π electroproduction off the proton. The data were analyzed using two conceptually different approaches-fixed-t dispersion relations and a unitary isobar model-allowing us to draw conclusions on the model sensitivity of the obtained electrocoupling amplitudes. The amplitudes for the (1232)P 33 show the importance of a meson-cloud contribution to quantitatively explain the magnetic dipole strength, as well as the electric and scalar quadrupole transitions. They do not show any tendency of approaching the pQCD regime for Q 2 6 GeV 2 . For the Roper resonance, N (1440)P 11 , the data provide strong evidence that this state is a predominantly radial excitation of a three-quark (3q) ground state. Measured in pion electroproduction, the transverse helicity amplitude for the N (1535)S 11 allowed us to obtain the branching ratios of this state to the πN and ηN channels via comparison with the results extracted from η electroproduction. The extensive CLAS data also enabled the extraction of the γ * p → N (1520)D 13 and N (1535)S 11 longitudinal helicity amplitudes with good precision. For the N (1535)S 11 , these results became a challenge for quark models and may be indicative of large meson-cloud contributions or of representations of this state that differ from a 3q excitation. The transverse amplitudes for the N (1520)D 13 clearly show the rapid changeover from helicity-3/2 dominance at the real photon point to helicity-1/2 dominance at Q 2 > 1 GeV 2 , confirming a long-standing prediction of the constituent quark model.

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Section: N(1520) D 13 Resonancementioning

confidence: 99%

“…[15,19] assuming that N(1440)P 11 is the first radial excitation of the 3q ground state. Although the models [15,19] fail to describe numerically the data at small Q 2 , this can have the natural explanation in the meson-cloud contributions, which are expected to be large for low Q 2 [83]. …”

Section: B N(1440) P 11 Resonancementioning

confidence: 99%

Electroexcitation of nucleon resonances from CLAS data on single pion electroproduction

Aznauryan¹,

Burkert²,

Biselli³

et al. 2009

Phys. Rev. C

Self Cite

252

380

View full text Add to dashboard Cite

show abstract

“…More importantly, the model describes successfully the differential cross section and target polarization asymmetries as shown in Ref. [9].…”

Section: Full Coupled-channels Model (I): Meson-baryon Interactionmentioning

confidence: 91%

“…The parameter values used in this model are given in Ref. [9]. Once the meson-baryon sector is fixed we will, in a first stage, leave it unchanged and produce a first description of the single meson photoproduction data.…”

Section: Full Coupled-channels Model (I): Meson-baryon Interactionmentioning

confidence: 99%