Measurement of the proton-antiproton total cross section at the SpS collider by a luminosity dependent method

Augier, C.; Bourotte, J.; Bozzo, M.; Bueno, A.; Cases, R.; Djama, F.; Faugeras, Paul E; Faugier, A; Haguenauer, M.; Herr, W.; Jeanneret, J.B.; Kundrát, V.; Linnecar, T.; Lokajíček, M.; Matthiae, G.; Morelli, Alessandro; Natali, F.; Němeček, S.; Novák, M.; Sanchís, E.; Sette, G.; Smižanská, M.; Velasco, J.

doi:10.1016/0370-2693(94)01485-u

Cited by 29 publications

(13 citation statements)

References 8 publications

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“…These data are reported in Fig. 2 together with the results of the CDF experiment at two different Tevatron energies √ s=1.8TeV and √ s=546GeV [16] and the results of UA(4) at the CERNpp collider at √ s=541GeV [17]. At √ s=1.8TeV CDF found σ tot = 80.03 ± 2.24 mb and σ el /σ tot = 0.246 ± 0.004, at variance with the E710 results.…”

Section: Early Successessupporting

confidence: 60%

Do we understand near-forward elastic scattering up to TeV energies?

Bourrely

Soffer

2015

Int. J. Mod. Phys. A

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In 1970, on purely theoretical grounds, all total hadronic total cross sections were predicted to increase without limit for higher and higher energies. This was contrary to the conventional belief at that time. In 1978, an accurate phenomenological model was formulated for the case of proton-proton and antiproton-proton interactions. The parameters for this model were slightly improved in 1984 using the additional available experimental data. Since then, for thirty years these parameters have not changed. This development, including especially the difficult task of formulating this phenomenological model and the comparison of the predictions of this model with later experimental results, is summarized.

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Section: Early Successessupporting

confidence: 60%

Do we understand near-forward elastic scattering up to TeV energies?

Bourrely

Soffer

2015

Int. J. Mod. Phys. A

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“…These data are reported in Fig. 1 together with the results of the CDF experiment at two different Tevatron energies √ s=1.8TeV and √ s=546GeV [8] and the results of UA(4) at the CERNpp collider at √ s=541GeV [9]. At √ s=1.8TeV CDF found σ tot = 80.03 ± 2.24 mb and σ el /σ tot = 0.246 ± 0.004, at variance with the E710 results.…”

Section: Pre Lhc Era Successessupporting

confidence: 60%

Impact picture for near-forward elastic scattering up to LHC energies

Soffer

Bourrely

2015

AIP Conference Proceedings

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“…(Left) The total and elastic cross section as function of √ s for pp. Experimental data from[44][45][46][47][48][49][50][51][52]. (Right) The total γ ⋆ p cross section as function of Q 2 for W = 220 GeV.…”

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confidence: 99%

Inclusive and exclusive observables from dipoles in high energy collisions

Flensburg

Gustafson

Lönnblad

2011

J. High Energ. Phys.

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We present a new model for simulating exclusive final states in minimum-bias collisions between hadrons. In a series of papers we have developed a Monte Carlo model based on Mueller's dipole picture of BFKL-evolution, supplemented with non-leading corrections, which has shown to be very successful in describing inclusive and semi-inclusive observables in hadron collisions. In this paper we present a further extension of this model to also describe exclusive final states. This is a highly non-trivial extension, and we have encountered many details that influence the description, and for which no guidance from perturbative QCD could be found. Hence we have had to make many choices based on semi-classical and phenomenological arguments. The end result is a new event generator called DIPSY which can be used to simulate complete minimum-bias non-diffractive hadronic collision events. Although the description of data from the Tevatron and LHC is not quite as good as for PYTHIA 8, the most advanced of the general purpose event generator programs for these processes, our results are clearly competitive, and can be expected to improve with careful tuning. In addition, as our model is very different from conventional multiple scattering scenaria, the DIPSY program can be used to gain deeper insight in the soft and semi-hard processes involved both in hadronic and heavy ion collisions.

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Measurement of the proton-antiproton total cross section at the SpS collider by a luminosity dependent method

Cited by 29 publications

References 8 publications

Do we understand near-forward elastic scattering up to TeV energies?

Do we understand near-forward elastic scattering up to TeV energies?

Impact picture for near-forward elastic scattering up to LHC energies

Inclusive and exclusive observables from dipoles in high energy collisions

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