Abstract:We emphasize that recently observed regularities in hadron interactions and deep-inelastic scattering are of preasymptotic nature and it is impossible to make conclusions on the true asymptotic behavior of observables without unitarization procedure. Unitarization is important and changes scattering picture drastically.
“…We can approximate p R (s) by the value of |S(s, b = 0)| 2 which tends to unity at s → ∞. It should be noted that the value √ s R ≃ 2 T eV [11]. Below this energy there is no reflective scattering, α(s) = 0 at s ≤ s R , and therefore corrections to the hadron density are absent.…”
Section: Effects Of the Reflective Scattering Mode For Nuclear Collismentioning
We discuss effects of reflective scattering for heavy nuclei collisions and the deconfined matter formation at the LHC and asymptotical energies. Reflective scattering in hadron collisions leads to decreasing matter density with energy beyond the LHC energies. Limiting form of energy dependence of hadron density is obtained.
“…We can approximate p R (s) by the value of |S(s, b = 0)| 2 which tends to unity at s → ∞. It should be noted that the value √ s R ≃ 2 T eV [11]. Below this energy there is no reflective scattering, α(s) = 0 at s ≤ s R , and therefore corrections to the hadron density are absent.…”
Section: Effects Of the Reflective Scattering Mode For Nuclear Collismentioning
We discuss effects of reflective scattering for heavy nuclei collisions and the deconfined matter formation at the LHC and asymptotical energies. Reflective scattering in hadron collisions leads to decreasing matter density with energy beyond the LHC energies. Limiting form of energy dependence of hadron density is obtained.
“…Numerical estimates [19] show that the ratio σ el (s)/σ tot (s) bocomes close to the asymptotic value 1 at extremely high energies √ s = 500…”
Section: Antishadow Scattering Modementioning
confidence: 99%
“…We consider for illustration the unitarized chiral quark model (section 4). Fit to the total hp cross-sections gives small values for the parameters g and α ( g, α ≪ 1) [19]. It means that at s ≪ s 0 the second term in the square brackets in Eqs.…”
Section: Universal Preasymptoticsmentioning
confidence: 99%
“…(21) and (22) is small and we can expand over it. The numerical value of s 0 is determined by the equation |U(s, 0)| = 1 and is [19] √ s 0 ≃ 2 TeV. At this energy the amplitude has the value |f (s 0 , 0)| = 1/2.…”
Section: Universal Preasymptoticsmentioning
confidence: 99%
“…The region of energies and impact parameters corresponding to the antishadow scattering mode is determined by the conditions Imf (s, b) > 1/2 and η(s, b) < 1/4. The quantitative analysis of the experimental data [19] gives the threshold value of energy:…”
New mode in the hadron scattering is predicted to appear at the energies beyond √ s ≃ 2 TeV: the antishadow scattering mode and the experiments at LHC and VLHC in hadronic reactions will be able to reveal it. The appearance of the antishadow scattering mode at these energies is considered on the basis of unitarity and geometrical notions of hadron interactions. Connections with the nonperturbative-QCD models are discussed.
Numerical predictions for the global characteristics of proton-proton interactions are given for the LHC energy. Possibilities for the discovery of the antishadow scattering mode and its physical implications are discussed.
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