Isobar Production and Elastic Scattering in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi><mml:mo>−</mml:mo><mml:mi>p</mml:mi></mml:math>Interactions from 6 to 30<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mfrac><mml:mrow><mml:mi mathvariant="normal">GeV</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:mfrac></mml:math>

Edelstein, R. M.; Carrigan, R. A.; Hien, N. C.; McMahon, T.; Nadelhaft, I.; Anderson, E. W.; Bleser, E.; Collins, G. B.; Fujii, Terushige; Menes, J.; Turkot, F.

doi:10.1103/physrevd.5.1073

Cited by 56 publications

(26 citation statements)

References 69 publications

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“…Diffractive processes can be rather well identified with respect to the nondiffractive ones because of their specific kinematical configurations. When a proton in the final states of the reaction of Equation 47 is quasi-elastically scattered while the other one flares into a many-particle hadronic state X. a typical rapiditl configura tion is obtained. This is illustrated in Figure 32A.…”

Section: Diff Ractive Excitation Of Large-mass H Adronic Statesmentioning

confidence: 99%

“…Equation 27 is used to extract proton-nucleon cross sections from proton-deuteron data. Proton-proton missing-mass spectra derived from proton-deuteron data at PL = 50 and 275 GeV Ie are compared in Figure SB with previous proton-proton data at 20 GeV/e obtained at the AGS (47). The broad bump at M2 � 2 GeV2 is attributed to the production of the 1.4 GeV "enhance ment" and the structure at M2 � 2.8 Gey2 is identified with the excitation of the well-known resonant state N(J690).…”

Section: Kaon Diffraction Dissociationmentioning

confidence: 99%

“…They were obtained by the USSR-USA collaboration working at Fermilab from the deuteron data by means ofEquation 27. The open triangles were measured at the AGS(47). The curves are only to guide the eye.…”

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confidence: 99%

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Diffraction of Hadronic Waves

Amaldi¹,

Jacob²,

Matthiae³

1976

Annu. Rev. Nucl. Sci.

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Section: Diff Ractive Excitation Of Large-mass H Adronic Statesmentioning

confidence: 99%

Section: Kaon Diffraction Dissociationmentioning

confidence: 99%

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Diffraction of Hadronic Waves

Amaldi¹,

Jacob²,

Matthiae³

1976

Annu. Rev. Nucl. Sci.

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“…These resonances have also been studied with pp→pN * reactions [3]. The dispersion of the masses found by different experiments, remains generally less than 20 MeV.…”

Section: Introductionmentioning

confidence: 99%

πNandηpdeexcitation channels of theN*and Δ baryon

et al. 2005

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“…However, in this paper these two bumps will be regarded as the sum of the resonances with nearly equal masses, since these bumps were observed by missing mass experiments. 3 …”

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confidence: 99%

Differential Cross Section and Polarization Effects in pp -> pN* and SU(6) O(3) Structure

Hirano

Iwata

Matsuda

et al. 1974

Progress of Theoretical Physics

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1801On the basis of the symmetric quark model, the differential cross section and the polarization effect in pp-7pN* is calculated. These quantities are related to the NN elastic scattering amplitude by assuming that N and N* have SU(6) Q$)0(3) structure. Our results show that it seems possible to explain the reaction NN-7NN* by their SU(6)Q$)0(3) structure. However, our knowledge on the helicity and isospin dependence of the input NN elastic scattering amplitude is not enough to derive more detailed conclusions.(NQ) amplitude in § 2 and the explicit form of the overlapping integral will be obtained in § 3. In § 4 the NQ amplitude will be expressed in terms of the NN elastic scattering amplitude. In § 5 the N* production amplitude, the differential cross section and the polarization of N*, etc., will be expressed in terms of the NN elastic scattering amplitude. In § 6 we will present the phenomenological NN elastic scattering amplitudes which are used as input and the numerical results will be presented in § 7. Section 8 will be devoted to the summary and discussion.

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Isobar Production and Elastic Scattering inp−pInteractions from 6 to 30GeVc

Abstract: Differential cross sections have been measured for nucleon-isobar production and elastic scattering in p -p interactions from 6.2 to 29.7 GeV/c in the laboratory angle range 8 < O , ,

Cited by 56 publications

References 69 publications

Diffraction of Hadronic Waves

Diffraction of Hadronic Waves

πNandηpdeexcitation channels of theN*and Δ baryon

Differential Cross Section and Polarization Effects in pp -> pN* and SU(6) O(3) Structure

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