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Related papers: The perturbative odderon intercept

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We present our recent results on the odderon intercept in perturbative QCD, obtained through the solution of the Baxter equation and investigation of the spectrum of the relevant constant of motion.

High Energy Physics - Theory · Physics 2007-05-23 Romuald A. Janik , Jacek Wosiek

The intercept of the odderon trajectory is derived, by finding the spectrum of the second integral of motion of the three reggeon system in high energy QCD. When combined with earlier solution of the appropriate Baxter equation, this leads…

High Energy Physics - Theory · Physics 2009-10-31 R. A. Janik , J. Wosiek

Starting from the leading Odderon solution of the three gluon system in perturbative QCD we introduce, as a first step towards the transition to the nonperturbative region, an infrared cutoff and use the running QCD coupling constant. In…

High Energy Physics - Theory · Physics 2020-05-20 Jochen Bartels , Carlos Contreras , Gian Paolo Vacca

Arguments are presented for the odderon intercept being exactly equal to unity. A variational method is presented based on a complete system of one-gluon functions. For the odderon, the highest intercept calculated by this method is…

High Energy Physics - Phenomenology · Physics 2008-02-03 N. Armesto , M. A. Braun

The odderon singularity is studied in perturbative QCD in the framework of the Bartels-Kwieci\'nski-Praszalowicz (BKP) equation. Arguments for the odderon intercept being exactly equal to unity are given. Besides, a variational method based…

High Energy Physics - Phenomenology · Physics 2016-11-03 N. Armesto , M. A. Braun

The odderon intercept is calculated directly, from its expression via an average energy of the odderon Hamiltonian, using both trial wave functions in the variational approach and the wave function recently constructed by R.A.Janik and…

High Energy Physics - Phenomenology · Physics 2016-09-06 M. A. Braun , P. Gauron , B. Nicolescu

We present and discuss a new bound state solution of the three gluon system in perturbative QCD. It carries the quantum numbers of the odderon, has intercept at one and couples to the impact factor $\gamma^* \to \eta_c$.

High Energy Physics - Phenomenology · Physics 2010-04-06 J. Bartels , L. N. Lipatov , G. P. Vacca

The odderon intercept is calculated directly using the wave function recently constructed by R.A.Janik and J.Wosiek. The results confirm their reported value. It is also found that their solution for $q_3=0$ does not satisfy the…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. A. Braun

The running coupling is introduced into the equation for the odderon via the bootstrap relation. It is shown that the previously found odderon state with a maximal intercept, which is constructed from antisymmetric pomeron wave function,…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. A. Braun

A review on how the Odderon idea does appear in QCD is given. In the last years it has been developed a non-perturbative QCD approach based on the stochastic vacuum model and a perturbative one based on resummation techniques in the small x…

High Energy Physics - Phenomenology · Physics 2015-06-25 G. P. Vacca

A new method is applied to solve the Baxter equation for the one dimensional system of noncompact spins. Dynamics of such an ensemble is equivalent to that of a set of reggeized gluons exchanged in the high energy limit of QCD amplitudes.…

High Energy Physics - Theory · Physics 2008-02-03 J. Wosiek , R. A. Janik

We analyse the momentum space triple Pomeron vertex in perturbative QCD. In addition to the standard form of this vertex which is used in the context of total cross-sections at high energies and in the QCD reggeon field theory, there exists…

High Energy Physics - Phenomenology · Physics 2011-09-13 J. Bartels , M. Braun , G. P. Vacca

A new method is applied to solve the Baxter equation for three coupled, noncompact spins. Due to the equivalence with the system of three reggeized gluons, the intercept of the odderon trajectory is predicted for the first time, as the…

High Energy Physics - Theory · Physics 2016-08-25 J. Wosiek , R. E. Janik

The Hamiltonian derived by Bartels, Kwiecinski and Praszalowicz for the study of high-energy QCD in the generalized logarithmic approximation was found to correspond to the Hamiltonian of an integrable $XXX$ spin chain. We study the odderon…

High Energy Physics - Theory · Physics 2009-10-28 Z. Maassarani , S. Wallon

The ratio of intercept to slope of the Pomeron trajectory is derived in a phenomenological model based on a QCD approach to diffraction.

High Energy Physics - Phenomenology · Physics 2011-01-04 Konstantin Goulianos

I review recent progress in perturbative QCD on two fronts: extending next-to-next-to-leading order QCD corrections to a broader range of collider processes, and applying twistor-space methods (and related spinoffs) to computations of…

High Energy Physics - Phenomenology · Physics 2010-11-15 Lance J. Dixon

The four-pomeron vertex is studied in the perturbative QCD. Its dominating terms of the leading (zeroth and first) orders in the coupling constant and subdominant in the number of colors are constructed. The vertex consists of two terms,…

High Energy Physics - Phenomenology · Physics 2021-12-22 M. A. Braun

The odderon intercept $ \alpha $ is recalculated by the variational method based on conformal invariance. The final result is $\alpha=1-0.339 \alpha_s N/\pi$ in contrast to the published value above unity.

High Energy Physics - Phenomenology · Physics 2007-05-23 M. A. Braun

We present recent developments on the role of the running coupling constant at the intersection of perturbative and nonperturbative QCD. A number of experiments show a smooth transition from small to large scales given by the four-momentum…

High Energy Physics - Phenomenology · Physics 2015-06-11 A. Courtoy , Simonetta Liuti

We calculate the order alpha_s^2 and order alpha_s^3 QCD contributions to colour-singlet exchange in the leading log s approximation. We implement the resulting amplitude at the hadronic level and thus construct the QCD pomeron and odderon…

High Energy Physics - Phenomenology · Physics 2009-10-22 J. R. Cudell , B. U. Nguyen
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