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Related papers: Pomerons

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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

The soft pomeron successfully correlates a wide variety of data. Its properties seem rather simple: it couples to single quarks and its coupling factorises.

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

A wide variety of experimental data in hadronic reactions are described in terms of the exchange of an object called the soft pomeron. It is nonperturbative in origin and is perhaps associated with glueballs. The HERA measurements of $\nu…

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

New structure-function data are in excellent agreement with the existence of a hard pomeron, with intercept about 1.4. It gives a very economical description of the data. Having fixed 2 parameters from the data for the real-photon cross…

High Energy Physics - Phenomenology · Physics 2009-11-07 A Donnachie , P V Landshoff

We show that simple Regge pole fits to the imaginary and the real part of the elastic amplitude in pp and pbar p collisions give a value of 1.096+0.012-0.009 for the pomeron intercept. Preliminary results of the new global fits to all…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. R. Cudell , K. Kang , S. K. Kim

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

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

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

It is demonstrated that the hard pomeron intercept value can be estimated directly from the data on the proton unpolarized structure function: $\alpha_{\rm P}^h(0)-1=0.317\pm 0.028$.

High Energy Physics - Phenomenology · Physics 2014-06-10 A. A. Godizov

The equation for the hard pomeron with a running coupling introduced on the basis of the bootstrap requirement is solved numerically. Two supercritical pomerons are found with the intercept minus 1 of the leading one of the order 0.35-0.5…

High Energy Physics - Phenomenology · Physics 2009-10-28 Mikhail Braun , Gian Paolo Vacca , Giovanni Venturi

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

Key issues in pomeron physics include whether the hard and soft pomerons are distinct objects, and whether the hard pomeron is already present in amplitudes at $Q^2=0$. It is urgent to learn how to combine perturbative and nonperturbative…

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

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

A traditional Regge model with a $Q^2$-independent Pomeron intercept closed (or equal) to one is constructed in order to describe the available data on the proton structure function. A Dipole Pomeron model which does not explicitly violate…

High Energy Physics - Phenomenology · Physics 2014-11-17 P. Desgrolard , A. Lengyel , E. Martynov

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

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

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

Exclusive vector meson production from real and virtual photons is a good probe of pomeron physics. In particular, it sheds light on how the soft pomeron is related to nonperturbative QCD, and how it couples to heavy flavours. It also…

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

We investigate some aspects and consequences of the extrema bounds for the soft Pomeron intercept, recently determined by means of global fits to $pp$ and $\bar{p}p$ total cross section data at both accelerator and cosmic-ray energy regions…

High Energy Physics - Phenomenology · Physics 2009-11-10 E. G. S. Luna , M. J. Menon , J. Montanha

We apply the tensor-pomeron model to small-$x$ deep-inelastic lepton-proton scattering and photoproduction. Our model includes a soft and a hard tensor pomeron as well as a reggeon contribution. Data with c.m. energies $6 < \sqrt{s} < 318$…

High Energy Physics - Phenomenology · Physics 2020-01-23 Daniel Britzger , Carlo Ewerz , Sasha Glazov , Otto Nachtmann , Stefan Schmitt
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