Equivalence of quark models and universality predictions for high-energy scattering

Freund, P.

doi:10.1007/bf02756391

Cited by 13 publications

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“…One interesting consequence of the model is the prediction that oT(pp> > oT(pn), Freund (1965) has deduced a relation between nucleon-and pion-nucleon total cross sections of the form: If, in the asymptotic limit, oT(pp)-+oT(pn), equation ( 20) again implies aT(fip) > aT(pn>a I n the simple quark model, where one postulates that a nucleon comprises three quarks, and a meson, a quark and an anti-quark, the basic interaction in, say, the meson-nucleon collision, shown in figure 27, is the single scattering of a quark in one hadron by a quark in the other. On this basis, relations between various total cross sections have been obtained by Levin and Frankfurt (1965), Lipkin and Scheck (1966), Van Hove (1966) andFreund (1966).…”

Section: Ao(xy> Ut('y) -Ot('y)mentioning

confidence: 99%

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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