The role of Coulomb interaction in elastic and almost elastic scattering of hadrons from nuclei

Czyż, W.; Leśniak, L.; Wołek, H.

doi:10.1016/0550-3213(70)90034-9

“…Then (51) suggests that the contribution to the Figure 8: A comparison of elastic (points, the lower set of data points and the lower curve) and combined elastic plus nucleus-dissociative (triangles,the upper set of data points and the upper curve) p 12 C scattering data [117,118]. The theoretical calculations are from Czyz et al [116].…”

Section: The Diffraction Slope: Variations From Elastic Scattering Tomentioning

confidence: 99%

“…16. Figure 16: The kinematical variables entering the k ⊥ factorization representation (116) for vector meson production amplitudes.…”

Section: The Impact Factor Representation For the Helicity Amplitudesmentioning

confidence: 99%

Diffractive vector meson production at HERA: From soft to hard QCD

Иванов

¹

,

Николаев

²

,

Savin

³

2006

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“…Ona can, in principle, use the individual amplitudes which have Coulomb interactions built into them (this very tedious calculation has been done, e.g., in refs. [16,17], but we shall consider the; effects produced by the average Coulomb potential produced by the whole nucleus [15] which produces almost identical results [16,17].…”

Section: (Iii)mentioning

confidence: 99%

Interactions of high energy particles with nuclei

Czyż¹

1975

3

0

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Elastic scattering and diffractive production processes induced in nuclear targets by high energyprojectiles are discussed in this article. Special attention is paid to the interaction of high energi.-hadrons and photons. Interactions of high energy electrons and neutrinos are briefly mentioned. The common features of all these processes are emphasized throughout the article: The multiple scattering and shadowing processes inside of the target nuclei. An effort is made to develop a unified way of treating nuclear interactions of particles which are either hadrons or exhibit some hadronic components in such interactions. This article is divided into seven sections: (1) Introduction, (2) Description of multiple scattering, (3) Elastic scattering of hadrons from nuclei, (4) Diffractive dissociation and diffractive excitation, (5) Diffractive production of hadrons in hadron-nucleon collisions, (6) Shadowing effects in inelastic electron-nucleus scattering, (7) Shadowing effects in neutrino reactions on nuclei.

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“…The crucial point is that at a sufficiently large (p, p ′ ) momentum transfer such that the recoil energy exceeds the typical nuclear binding energy, which can viewed as hard scattering, the t-distribution of scattered protons in quasielastic (nucleus-dissociative) pA → p ′ A * is the same as in elastic pp scattering, [115,116]. The quasielastic pA → p ′ A * becomes sort of a deep inelastic scattering with quasifree bound nucleons behaving as partons of a nucleus and quasifree pN → p ′ N scattering being a counterpart of the Rutherford scattering of leptons off charged partons in DIS off the proton.…”

Section: B∆mentioning

confidence: 99%

“…Then (51) suggests that the contribution to the Figure 8: A comparison of elastic (points, the lower set of data points and the lower curve) and combined elastic plus nucleus-dissociative (triangles,the upper set of data points and the upper curve) p 12 C scattering data [117,118]. The theoretical calculations are from Czyz et al [116]. diffraction slope from the pY transition B pY ≈ B N , so that in SD and DD into low-mass states…”

mentioning

confidence: 99%