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Related papers: The Soft Pomeron

200 papers

Soft pomeron fits reproduce all zero-Q2 data for light quarks, but run into problems at HERA for heavy mesons and for high Q2, and at the Tevatron for W diffractive production. I review the basic properties of the soft pomeron, and outline…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. R. Cudell

New small-$x$ data indicate the existence of two pomerons: the usual soft pomeron with intercept close to 1.08, and a hard pomeron with intercept about 1.4

High Energy Physics - Phenomenology · Physics 2007-05-23 P V Landshoff

We show that the introduction of an additional, hard, singularity in soft forward amplitudes enables one to improve considerably the fits using a simple-pole structure for the soft pomeron.

High Energy Physics - Phenomenology · Physics 2007-05-23 J. R. Cudell , A. Lengyel , E. Martynov , O. V. Selyugin

The LHC has released precise measurements of elastic proton-proton scattering that provide a unique constraint on the asymptotic behavior of the scattering amplitude at high energies. Recent reanalyses of part of these data indicate that…

High Energy Physics - Phenomenology · Physics 2021-01-27 M. Broilo , D. A. Fagundes , E. G. S. Luna , M. Peláez

Soft materials, such as colloidal suspensions, polymer solutions, and biological systems, are typically multicomponent mixtures of macromolecules and simpler components (e.g., microions, monomers, solvent) that can assemble into complex…

Soft Condensed Matter · Physics 2015-05-13 Alan R. Denton

We present a preliminary report on the determination of the intercepts and couplings of the soft pomeron and of the rho/omega and f/a trajectories from the largest data set available for all total cross sections and real parts of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. R. Cudell , V. V. Ezhela , K. Kang , S. B. Lugovsky , N. P. Tkachenko

A brief review on the Dipole Pomeron model is given. The model not only describes data on hadron-hadron interactions, but also allows to describe data on the proton structure function with a $Q^2$ independent intercept. Moreover the chosen…

High Energy Physics - Phenomenology · Physics 2016-11-23 E. Martynov

Regge theory provides a very simple and economical description of data for (i) the proton structure function with x<0.07 and all available Q^2 values, (ii) the charm structure function, and (iii) gamma p --> J/psi p. The data are all in…

High Energy Physics - Phenomenology · Physics 2009-10-31 A Donnachie , P V Landshoff

We summarize the main features of available experimental results on soft and hard diffraction and draw conclusions about the nature of the pomeron.

High Energy Physics - Phenomenology · Physics 2007-05-23 Konstantin Goulianos

New properties of the quark correlator are found via equations of motion. As a first result, approximate relations can be established among the "soft" functions; one such relation may help in determining the quark transversity in a nucleon.…

High Energy Physics - Phenomenology · Physics 2017-08-23 E. Di Salvo

We recall the main properties of inclusive particle distributions expected for Pomeron-proton and Pomeron-Pomeron interactions. Due to the small size of the Pomeron we expect larger transverse momenta of secondaries and a smaller…

High Energy Physics - Phenomenology · Physics 2019-08-14 V. A. Khoze , A. D. Martin , M. G. Ryskin

A comparative phenomenological analysis of Regge models with and without a hard Pomeron component is performed using a common set of recently updated data. It is shown that the data at small $x$ do not indicate explicitly the presence of…

High Energy Physics - Phenomenology · Physics 2011-09-13 P. Desgrolard , E. Martynov

Regge models for proton structure function with and without a hard Pomeron contribution are compared with all available data in the region $W>3$ GeV, $Q^{2}\leq 3000$ GeV$^{2}$ and $x<0.75$. It is shown that the data do not support a hard…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Desgrolard , E. Martynov

We review the evidence for the presence of a hard singularity in soft forward amplitudes, and give an estimate of its trajectory and couplings.

High Energy Physics - Phenomenology · Physics 2009-11-11 J. R. Cudell , A. Lengyel , E. Martynov , O. V. Selyugin

Using the largest data set available, we determine the best values that the data at t=0 (total cross sections and real parts of the hadronic amplitudes) give for the intercepts and couplings of the soft pomeron and of the rho/omega and a/f…

High Energy Physics - Phenomenology · Physics 2014-11-17 J. R. Cudell , V. Ezhela , K. Kang , S. Lugovsky , N. Tkachenko

It is demonstrated that the "soft pomeron" (together with a secondary reggeon) describing cross-sections of hadron-hadron collisions is fairly able to describe the energy dependence of cross-sections of exclusive (virtual) photoproduction…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. A. Petrov , A. V. Prokudin

We consider simple-pole descriptions of soft elastic scattering for pp, pbar p, pi+ p, pi- p, K+ p and K- p. We work at t and s small enough for rescatterings to be neglected, and allow for the presence of a hard pomeron. After building and…

High Energy Physics - Phenomenology · Physics 2011-03-23 J. R. Cudell , A. Lengyel , E. Martynov

The BFKL pomeron is swamped by the soft pomeron, at least at t=0.

High Energy Physics - Phenomenology · Physics 2007-05-23 P V Landshoff

The introduction of a hard singularity in fits to total cross sections and to the ratio of real to imaginary parts enables to reproduce perfectly the data for sqrt(s)< 100 GeV using only simple-pole parametrisations, both for the soft and…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. R. Cudell , A. Lengyel , E. Martynov , O. V. Selyugin

The hard pomeron component needed to reproduce small-x data seems to be present in elastic scattering at moderate energy. If this is the case, it is likely that the total cross section at the LHC will be appreciably larger than previously…

High Energy Physics - Phenomenology · Physics 2007-10-30 J. R. Cudell , A. Lengyel , E. Martynov , O. V. Selyugin
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