Glauber quark and gluon contributions to quark energy loss at next-to-leading order and next-to-leading twist

Abstract

The higher-twist formalism is used at $O({\alpha }_s^2)$ to compute all possible medium-induced single-scattering emission kernels for an incoming highly energetic and virtual quark traversing the nuclear environment. The effects of the heavy-quark mass scale are taken into account [Phys. Rev. C 94, 054902 (2016)] both in the initial state as well as in the final state, along with interactions involving both in-medium Glauber gluons and quarks [Nucl. Phys. A 793, 128 (2007)], as well as coherence effects [Phys. Rev. C 105, 024908 (2022)]. As this study is a continuation of our work on medium-induced photon production [Phys. Rev. C 112, 025204 (2025)], the general factorization procedure for $e$-$A$ deep-inelastic scattering is still used. An incoming quark energy loss in the nuclear medium yields four possible scattering kernels $K_i$ with the following final states: (i) $q+g$, (ii) $g+g$, (iii) $q+{\bar{q}}^{\prime }$, where the quark $q$ may have a flavor different from the antiquark ${\bar{q}}^{\prime }$, and (iv) $q+q^{\prime }$, where, again, $q$ may have a flavor different from $q^{\prime }$. The collisional kernels include full phase factors from all non-vanishing diagrams and complete first-order derivative in the longitudinal direction ($k^{-}$) as well as second-order derivative in the transverse momentum ($k_{\perp }$) gradient expansion. Furthermore, in-medium parton distribution functions and the related jet transport coefficients have a hard transverse-momentum dependence (of the emitted quark or gluon) present within the phase factor.

arXiv comment66 pages, 23 figures, single column; Updated introduction and discussion; Matched to published version [Phys. Rev. C 113, 055207 (2026)]

References in corpus (57)

• Computing Quark and Gluon Distribution Functions for Very Large Nuclei
• Operator expansion for high-energy scattering
• Nonlinear Gluon Evolution in the Color Glass Condensate: I
• The Color Glass Condensate
• The Wilson renormalization group for low x physics: towards the high density regime
• The BFKL Equation from the Wilson Renormalization Group
• Nonlinear Gluon Evolution in the Color Glass Condensate: II
• Unitarization of the BFKL Pomeron on a Nucleus
• The Renormalization Group Equation for the Color Glass Condensate
• Transport coefficients in high temperature gauge theories: (II) Beyond leading log
• The Wilson renormalization group for low x physics: Gluon evolution at finite parton density
• Transport coefficients in high temperature gauge theories: (I) Leading-log results
• Fluctuating Glasma initial conditions and flow in heavy ion collisions
• Multiple Parton Scattering in Nuclei: Parton Energy Loss
• Photon and Gluon Emission in Relativistic Plasmas
• Relating different approaches to nonlinear QCD evolution at finite gluon density
• Multiple Scattering, Parton Energy Loss and Modified Fragmentation Functions in Deeply Inelastic eA Scattering
• Extracting jet transport coefficient from jet quenching at RHIC and LHC
• Effective Kinetic Theory for High Temperature Gauge Theories
• Linearized Boltzmann transport model for jet propagation in the quark-gluon plasma: Heavy quark evolution
• MARTINI: An event generator for relativistic heavy-ion collisions
• Energy Loss of Leading Partons in a Thermal QCD Medium
• Phenomenological constraints on the transport properties of QCD matter with data-driven model averaging
• Effective kinetic description of event-by-event pre-equilibrium dynamics in high-energy heavy-ion collisions
• Matching the Nonequilibrium Initial Stage of Heavy Ion Collisions to Hydrodynamics with QCD Kinetic Theory
• Hard collinear gluon radiation and multiple scattering in a medium
• A lattice study of the jet quenching parameter
• Extending Soft-Collinear-Effective-Theory to describe hard jets in dense QCD media
• Incorporating Space-Time Within Medium-Modified Jet Event Generators
• Coherent QCD multiple scattering in proton-nucleus collisions
• Multiple Parton Scattering in Nuclei: Modified DGLAP Evolution for Fragmentation Functions
• The Gluon Propagator in non-Abelian Weizsäcker-Williams fields
• Multistage Monte-Carlo simulation of jet modification in a static medium
• Multi-messenger heavy-ion collision physics
• Higher twist jet broadening and classical propagation
• Jet broadening in deeply inelastic scattering
• Nuclear modification of leading hadrons and jets within a virtuality ordered parton shower
• Multiple scattering effects on heavy meson production in p+A collisions at backward rapidity
• Calculating the Jet Quenching Parameter $\hat{q}$ in Lattice Gauge Theory
• The JETSCAPE framework: p+p results
• Multiple Parton Scattering in Nuclei: Quark-quark Scattering
• Initial-state cold nuclear matter energy loss effects on inclusive jet production in p+A collisions at RHIC and LHC
• Bayesian quantification of strongly-interacting matter with color glass condensate initial conditions
• Early-times Yang-Mills dynamics and the characterization of strongly interacting matter with statistical learning
• A global extraction of the jet transport coefficient in cold nuclear matter
• Drag induced radiative loss from semi-hard heavy quarks
• Bayesian Inference analysis of jet quenching using inclusive jet and hadron suppression measurements
• The medium-modified $g\to c\bar{c}$ splitting function in the BDMPS-Z formalism
• Next-to-leading order transverse momentum broadening for Drell-Yan production in p+A collisions
• Nuclear enhanced power corrections to DIS structure functions
• Failure of the collinear expansion in calculation of the induced gluon emission
• Final State Gluon Emission in Deep-Inelastic Scattering at Next-to-Leading Twist
• Leading order, next-to-leading order, and non-perturbative parton collision kernels: effects in static and evolving media
• Quenching jets increases their flavor
• Medium-enhanced $c\bar{c}$ radiation
• Color Glass Condensate meets High Twist Expansion
• Diffractive Physics Program at the Electron-Ion Collider's (EIC) 2nd Detector