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Related papers: Rapidity veto effects in the NLO BFKL equation

200 papers

We recalculate, completely within the original BFKL approach and at the next-to-leading order, the jet vertex relevant for the production of Mueller-Navelet jets in proton collisions and of forward jets in DIS. We consider both processes…

High Energy Physics - Phenomenology · Physics 2015-06-03 F. Caporale , D. Yu. Ivanov , B. Murdaca , A. Papa , A. Perri

With the aim to extend the study of inclusive heavy quarkonium production at forward rapidities with the resummation of high partonic center-of-momentum-energy logarithms beyond Leading Logarithmic Approximation (LLA), the explicit analytic…

High Energy Physics - Phenomenology · Physics 2024-10-25 Maxim Nefedov

The next-to-leading order (NLO) Balitsky-Kovchegov (BK) equation describing the high-energy evolution of the scattering between a dilute projectile and a dense target suffers from instabilities unless it is supplemented by a proper…

High Energy Physics - Phenomenology · Physics 2019-05-01 B. Ducloué , E. Iancu , A. H. Mueller , G. Soyez , D. N. Triantafyllopoulos

We solve the BFKL equation in the leading logarithmic approximation numerically in the Yang-Mills theory with the Higgs mechanism for the vector boson mass generation. It can be considered as a model for the amplitude with the correct…

High Energy Physics - Phenomenology · Physics 2014-04-23 Eugene Levin , Lev Lipatov , Marat Siddikov

We investigate the stability under variation of the renormalization, factorization and energy scales entering the calculation of the cross section, at next-to-leading order in the BFKL formalism, for the production of Mueller-Navelet jets…

High Energy Physics - Phenomenology · Physics 2015-06-16 F. Caporale , B. Murdaca , A. Sabio Vera , C. Salas

The Balitsky-Fadin-Kuraev-Lipatov (BFKL) approach for the cross sections at high energy $\sqrt s$ in perturbative QCD is briefly reviewed. The role of gluon Reggeization in the derivation of the BFKL equation and its compatibility with…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Papa

We study the impact of next-to-next-to-leading order (NNLO) QCD corrections on partial decay rates in B --> X_u l nu decays, at leading-order in the 1/m_b expansion for shape-function kinematics. These corrections are implemented within a…

High Energy Physics - Phenomenology · Physics 2010-02-11 C. Greub , M. Neubert , B. D. Pecjak

We study dijet production in proton-proton collisions with a veto on the emission of a third jet in the rapidity region in between the two leading ones. We resum the leading logarithms in the ratio of the transverse momentum of the leading…

High Energy Physics - Phenomenology · Physics 2015-05-28 Rosa Maria Duran Delgado , Jeffrey R. Forshaw , Simone Marzani , Michael H. Seymour

This is a personal recollection of several results involving the phenomenological study of the multi-Regge limit of scattering amplitudes. None of them would have been possible without the encouragement and constant support from Lev…

High Energy Physics - Phenomenology · Physics 2020-06-05 Agustín Sabio Vera

In this paper we consider the influence of non-perturbative corrections on the large $ b $ (impact parameter) behavior of the BFKL amplitude. This is done in the framework of a model where such ``soft'' corrections are taken into account in…

High Energy Physics - Phenomenology · Physics 2009-11-10 Sergey Bondarenko

We resum the recently calculated second order kernel of the BFKL equation. That kernel can be viewed as the sum of a conformally invariant part and a running coupling part. The conformally invariant part leads to a corrected BFKL intercept…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yuri V. Kovchegov , A. H. Mueller

The ``non-Abelian'' part of the quark contribution to the BFKL kernel in the next-to-leading order (NLO) is found in the coordinate representation by direct transfer of the contribution from the momentum representation where it was…

High Energy Physics - Phenomenology · Physics 2008-11-26 Victor S. Fadin , Roberto Fiore , Alessandro Papa

We examine the Regge (high energy) limit of 4-point scattering in both QCD and gravity, using recently developed techniques to systematically compute all corrections up to next-to-leading power in the exchanged momentum i.e. beyond the…

High Energy Physics - Theory · Physics 2017-02-01 A. Luna , S. Melville , S. G. Naculich , C. D. White

In non-diffusive conduction regimes of strongly correlated quantum electron systems, electromagnetic perturbations simultaneously probe the electronic dynamics in time and space: the exchanged energy $\hbar \omega$ excites retarded, i.e.,…

Strongly Correlated Electrons · Physics 2026-05-05 Davide Valentinis

The solution to the non-forward BFKL equation in the Leading Logarithmic approximation is expressed in terms of a sum of iterations of its kernel directly in transverse momentum and rapidity space. Several studies of the non-forward…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jeppe R. Andersen , Agustin Sabio Vera

High-energy collisions of two nucleons on two nucleons are studied in the BFKL approach in the leading approximation in $\alpha_sN_c$. Diagrams with redistribution of colour are considered. It is found that intermediate BKP states…

High Energy Physics - Phenomenology · Physics 2015-06-12 M. A. Braun

We study rapidity gaps between jets in ppbar collisions at the Tevatron by a novel solution of the nonforward BFKL equation including nonleading effects through the consistency constraint and running coupling. Results differ from earlier…

High Energy Physics - Phenomenology · Physics 2015-06-25 R. Enberg , L. Motyka , G. Ingelman

Far off-shell Higgs production in $H \rightarrow WW,ZZ$, is a particularly powerful probe of Higgs properties, allowing one to disentangle Higgs width and coupling information unavailable in on-shell rate measurements. These measurements…

High Energy Physics - Phenomenology · Physics 2015-06-19 Ian Moult , Iain W. Stewart

Search for the gravity with large extra dimensions at collider energies is considered in the trans-Planckian eikonal regime, i.e., when $\sqrt{\hat{s}} \gg M_D \gg \sqrt{-\hat{t}}$. Here $\hat{s}$ and $\hat{t}$ are the Mandelstam variables…

High Energy Physics - Phenomenology · Physics 2026-03-03 Anatolii Iu. Egorov , Victor T. Kim , Viktor A. Murzin , Vadim A. Oreshkin

We have recently derived a factorization formula for the Higgs-boson production cross section in the presence of a jet veto, which allows for a systematic resummation of large Sudakov logarithms of the form alpha_s^n ln^m(p_T^veto/m_H),…

High Energy Physics - Phenomenology · Physics 2015-06-16 Thomas Becher , Matthias Neubert , Lorena Rothen