First we take into account the coupling of the pomeron and odderon on the minimal level, introducing all nonlinear terms different from zero but restricting the partial waves for both ϕ and ψ to l = 0 (that is taking the pomeron at L = 0 and odderon at L = 1) The resulting Pomeron ϕ 0 coupled to odderon ψ 0 and the corresponding gluon density turn out to be practically the same as without

Soft Pomeron in holographic QCD. A Ballon-Bayona, RC Quevedo, MS Unity of pomerons from gauge/string duality. A Ballon-Bayona, RC Quevedo, MS

Recent data from LHC13 In a consistent QCD approach to diffractive DIS gluons in the pomeron have soft $z_{g}$ distribution and very broad intrinsic $k_{\perp}$ distribution. The latter Pris: 1999 kr. inbunden, 2002. Skickas inom 5-7 vardagar. Köp boken Pomeron Physics and QCD av Sandy Donnachie (ISBN 9780521780391) hos Adlibris. Pris: 619 kr. Häftad, 2005.

Pomeron

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Lipatov (BFKL) Pomeron [1]. Attempts to test experimentally this sector of QCD have started in last years, mainly considering processes where specific conditions

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The Odderon helped explain the mysterious differences in the The Pomeron is a Regge trajectory introduced by Chew and Frautschi in 1961 to account for the then approximate constant behavior of total cross sections with increasing s.

A realistic model for the Pomeron is proposed on the basis of two mechanisms of multiperipheral and diffractive productions. It is a basic assumption. Lipatov (BFKL) Pomeron [1]. Attempts to test experimentally this sector of QCD have started in last years, mainly considering processes where specific conditions The BFKL equation is derived from the Feynman rules of perturbative QCD and its solution obtained. The physical properties of the "pomeron" that emerges are 29 Sep 2008 During the 1960s it was found that, with the inclusion of the pomeron, Regge theory provides a very successful description of a huge quantity of The elements of the Regge theory, Pomeron in QCD and high energy scattering in AdS/CFT correspondence are presented.
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It is the meeting place of the ‘old’ particle physics with the ‘new’. Since by ‘old’ we mean over 30 years ago it is necessary to commence our study of high energy scattering in QCD with an introduction to (or recap of) Regge theory.
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19 Sep 2013 Reggeons in QFT The reggeized Gluon The BFKL Equation Applications Colour Dipoles Running Coupling. Hard. The Pomeron in QCD.

Funktionell. POMERON DIM 070 3 W 40 K. White. 8718696173787 Artikelnr: 915005808301 Kategorier: Hem, Order Tagg: Philips. Beskrivning. Beskrivning.

The POMERON is a hypothetical particle named in 1961 after the Russian physicist Isaak Pomeranchuk. Carrying no charge and thought to have spin 2, the dynamic pomeron is related to our understanding of quantum chromodynamics (QCD) and is currently thought of more as “pomeron behavior” than an actual particle candidate.

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PY - 1999/8/19. Y1 - 1999/8/19. N2 - We show that the asymmetry in the fractional energy of charm versus anticharm jets produced in high energy diffractive photoproduction is sensitive to the interference of the Odderon (C=-) and Pomeron (C=+) exchange amplitudes in QCD. At multi-TeV energies, on the other hand, proton interactions are expected to be mediated purely by gluons. In particular, elastic scattering at low-momentum transfer and high energies has long been explained by the exchange of a pomeron – a “colour-neutral” virtual glueball made up of an even number of gluons. Pomeron, tensor, vector, and scalar were discussed in Ref. [3] in view of the experimental results from Ref. [2]. Only the tensor ansatz for the Pomeron was found to be compatible with the experiment. Also, some historical remarks on different views of the Pomeron were made in Ref. [3].