Production of the Nucleon Isobars 1236, 1410, 1518, and 1688 MeV in Proton-Proton Collisions at 2.85, 4.55, 6.06, and 7.88 GeV/<i>c</i>

Blair, I.M.; Taylor, A.E.; Chapman, W. S.; Kalmus, P. I. P.; Litt, J.; Miller, Mike; Scott, David; Sherman, H.; Astbury, A.; Walker, T.G.

doi:10.1103/physrevlett.17.789

Cited by 61 publications

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“…T h e interpretation of the small structure, observed by Barepre et al (1964) in aT(.r-p) at a laboratory momentum of 0.5 Gevlc, as due to the presence of a pionnucleon isobar, has been discussed for some time. A bump at the corresponding centre-of-momentum energy (about 1400 hIev) has been observed in the energy spectrum of protons scattered inelastically off protons (Belletini et al 1965a, ,Inderson et al 1966, Blair et al 1966, and evidence for an isobar in this mass range also comes from phase-shift analysis in pion-nucleon scattering. We may conclude, then, that the structure observed by Bareyre et al can be accounted for by the presence of this isobar with I = J = 4, of mass 1410 k 15 Vel7 (Blair et al 1969).…”

Section: Resonances and Regge Polesmentioning

confidence: 94%

Hadron-nucleon total cross sections at high energies

Galbraith

1969

Rep. Prog. Phys.

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Contents 1. Introduction . 2. The measurement of total cross sections . 2.1. Experimental methods . 2.2. Corrections to measurements . 2.3. Cross sections for pure isospin states . 3.1. Pions . 3.2. Kaons . 4.1. Protons . 4.2. Neutrons . 4.3. Anti-nucleons , 5. Theoretical implications . 5.1. Resonances and Regge poles 5.2. Relative total cross sections, and asymptotic limits 5.3. Forward scattering amplitudes and total cross sections 3. Meson-nucleon total cross sections. 4. Nucleon and anti-nucleon total cross sections on nucleons ..

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Section: Resonances and Regge Polesmentioning

confidence: 94%