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Infrared singularities of QCD amplitudes with massive partons (0904.1021v3)

Published 7 Apr 2009 in hep-ph and hep-th

Abstract: A formula for the two-loop infrared singularities of dimensionally regularized QCD scattering amplitudes with an arbitrary number of massive and massless legs is derived. The singularities are obtained from the solution of a renormalization-group equation, and factorization constraints on the relevant anomalous-dimension matrix are analyzed. The simplicity of the structure of the matrix relevant for massless partons does not carry over to the case with massive legs, where starting at two-loop order new color and momentum structures arise, which are not of the color-dipole form. The resulting two-loop three-parton correlations can be expressed in terms of two functions, for which some general properties are derived. This explains observations recently made by Mitov et al. in terms of symmetry arguments.

Citations (179)

Summary

Infrared Singularities of QCD Amplitudes with Massive Partons

The paper "Infrared singularities of QCD amplitudes with massive partons" by Thomas Becher and Matthias Neubert provides a detailed investigation into the infrared (IR) singularities of Quantum Chromodynamics (QCD) scattering amplitudes involving both massive and massless partons. The authors present a formula that accounts for the two-loop IR singularities using dimensionally regularized QCD with arbitrary numbers of parton legs. They address the renormalization group equations and factorization constraints affecting the relevant anomalous-dimension matrices.

Key Findings and Contributions

  • Anomalous-Dimension Matrix and Renormalization: The paper derives expressions for the two-loop terms of the anomalous-dimension matrix crucial for QCD amplitudes. Notably, while massless parton amplitudes have a simplified structure modeled by color-dipole forms, massive partons introduce novel color and momentum correlations starting at two-loop order.
  • Two-Parton Correlations: The formula reveals color-dipole structures similar to massless cases but accommodates massive partons by introducing velocity-dependent cusp angles. For massless partons, the simplicity observed at two-loop order implies that IR poles are predominantly governed by two-parton interactions.
  • Three-Parton Correlations: The paper emphasizes that, with massive legs, complex three-parton correlations arise, constrained by symmetry arguments but absent in massless QCD. These new terms remarkably express correlations among three-parton legs, indicating intricate three-gluon interactions specific to massive partons.

Implications and Theoretical Significance

The research elucidates the perturbative QCD structure when dealing with massive scattering processes, particularly illuminating the discrepancies compared to massless theories often considered simpler due to the prevalence of decoupled dipole forms. The divergence of structures for massive partons at higher loops signifies new forms of partonic interactions, specifically impacting models of heavy-quark production and potentially influencing computation strategies for related collider processes.

Practical Implications

For practitioners in QCD and particle physics, the derived expressions for IR singularities of massive partons are critically useful for correct interpretations of amplitude computations. The paper's findings are significant for improving precision analyses in hadron collider environments such as the LHC, where heavy flavor QCD processes are frequent.

Future Research Avenues

Given the complexity introduced by massive parton legs beyond leading order, further studies may focus on fully characterizing the three-parton contributions in asymptotic energy limits where perturbative approximations are viable. Investigations into the practical applicability of these theoretical predictions in computational simulations could contribute to reducing uncertainties in phenomenological studies.

In summary, the paper by Becher and Neubert marks a vital step in understanding the full landscape of QCD amplitude singularities involving massive partons. Their work provides a foundational framework for exploring more sophisticated QCD interactions in theoretical and practical contexts, paving the way for future advancements in high-energy particle physics.