On the universality of cross sections of hadron -hadron(nuclei) collisions at superhigh energies

نویسندگان

  • M. Strikman
  • M. Zhalov
چکیده

We analyze the pattern of the onset of complete absorption (the black limit) in the high energy hadron-hadron collisions. The black limit arises due to the hard and soft interaction dynamics as a function of the impact parameters b. Both hard and soft mechanisms provide universal dependence of the partial amplitude of the high energy elastic hadronhadron scattering on the impact parameter b and result in the radius of interaction proportional to ln(s/s0). We find that with increase of the collision energies hard interactions lead to a faster increase of the impact parameter range where the partial wave amplitudes are approaching the unitarity limit. Consequently, we argue that at super high energies when the radius of hadronic interactions significantly exceeds static radii of the interacting hadrons(nuclei) the ratio of total cross sections of nucleon-nucleon, meson-nucleon, hadron-nucleus, nucleus-nucleus collisions becomes equal to one. The same universality is also expected for the structure functions of nuclei: F2A(x,Q )/F2N (x,Q 2) → 1, at very small x, and for the ratio σγA/σγp at superhigh energies. We analyze how accounting for the energy dependence of the interaction radii changes the geometry of hadron-nucleus and nucleus-nucleus collisions, the energy dependence of total, absorption and inelastic cross sections, the distribution over the number of wounded nucleons in proton-nucleus collisions and find that these effects are noticeable already for the LHC energies and even more so close to the Greisen-Zatsepin-Kuzmin limit.

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Hadron-hadron and hadron-nuclei collisions at high energies

In the 1960’s-1980’s high quality secondary beams became available at proton synchrotrons of increasing energies (PS, AGS, IHEP, FNAL, SPS). The secondary charged hadron beams contained the six stable or quasi stable charged particles π, K, p, p. The main experimental lines of research were: i) total hadron–hadron (hh) cross section measurements at high energies (plab > 20 GeV/c); ii) elastic h...

متن کامل

Hadron-nuclei collisions at high energies

A brief historical review is made of the hadron-hadron (hh) total cross section and hadronnucleus absorption cross section measurements, made mainly at high energy proton synchrotrons. Then I shall discuss low pt processes, including diffraction processes and fragmentation of nuclei in nucleusnucleus collisions. Nucleus-nucleus collisions at higher energy colliders are then considered, mainly i...

متن کامل

ar X iv : h ep - p h / 06 06 03 7 v 2 3 O ct 2 00 6 Two - Jet Inclusive Cross Sections in Heavy - Ion Collisions in the Perturbative QCD

In the framework of perturbative QCD, double inclusive cross sections for high pt parton production in nucleus-nucleus collisions are computed with multiple rescattering taken into account. The induced long-range correlations between numbers of jets at forward and backward rapidities are found to reach 10÷ 20% for light nuclei at √ s = 200 GeV/c and to be suppressed for heavy nuclei and LHC ene...

متن کامل

Fian/td-98/24 Minijet Transverse Energy Production in the Next-to-leading Order in Hadron and Nuclear Collisions

The transverse energy flow generated by minijets in hadron and nuclear collisions into a given rapidity window in the central region is calculated in the next-to-leading (NLO) order in QCD at RHIC and LHC energies. The NLO transverse energy production in pp collisions cross sections are larger than the LO ones by the factors of KRHIC ∼ 1.9 and KLHC ∼ 2.1 at RHIC and LHC energies correspondingly...

متن کامل

Minijet Transverse Energy Production in the Next-to-leading Order in Hadron and Nuclear Collisions

The transverse energy flow generated by minijets in hadron and nuclear collisions into a given rapidity window in the central region is calculated in the next-toleading (NLO) order in QCD at RHIC and LHC energies. The NLO transverse energy production in pp collisions cross sections are larger than the LO ones by the factors of KRHIC ∼ 1.9 and KLHC ∼ 2.1 at RHIC and LHC energies correspondingly....

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 2004