Search engine for discovering works of Art, research articles, and books related to Art and Culture
ShareThis
Javascript must be enabled to continue!

Glauber phases in non-global LHC observables: resummation for quark-initiated processes

View through CrossRef
A bstract It has been known for many years that jet cross sections at hadron colliders exhibit double-logarithmic corrections starting at four-loop order, arising from two soft Glauber-gluon interactions between the two colliding partons. The resummation of these “super-leading logarithms” has been achieved only recently by means of a renormalization-group treatment in soft-collinear effective theory. We generalize this result and, within the same framework and for quark-initiated processes, resum the double logarithms arising in the presence of an arbitrary number of Glauber-gluon exchanges. For typical choices of parameters, the higher-order Glauber terms give rise to corrections which are expected to be numerically of the same magnitude as the super-leading logarithms. However, we find that the Glauber series for jet cross sections is dominated by the two-Glauber contribution, if the colliding partons are quarks or anti-quarks.
Title: Glauber phases in non-global LHC observables: resummation for quark-initiated processes
Description:
A bstract It has been known for many years that jet cross sections at hadron colliders exhibit double-logarithmic corrections starting at four-loop order, arising from two soft Glauber-gluon interactions between the two colliding partons.
The resummation of these “super-leading logarithms” has been achieved only recently by means of a renormalization-group treatment in soft-collinear effective theory.
We generalize this result and, within the same framework and for quark-initiated processes, resum the double logarithms arising in the presence of an arbitrary number of Glauber-gluon exchanges.
For typical choices of parameters, the higher-order Glauber terms give rise to corrections which are expected to be numerically of the same magnitude as the super-leading logarithms.
However, we find that the Glauber series for jet cross sections is dominated by the two-Glauber contribution, if the colliding partons are quarks or anti-quarks.

Related Results

Dimension-six electroweak top-loop effects in Higgs production and decay
Dimension-six electroweak top-loop effects in Higgs production and decay
AbstractWe study the next-to-leading order electroweak corrections to Higgs processes from dimension-six top-quark operators in the Standard Model Effective Field Theory approach. ...
US contribution to the High Luminosity LHC Upgrade: focusing quadrupoles and crab cavities
US contribution to the High Luminosity LHC Upgrade: focusing quadrupoles and crab cavities
Abstract In the early 2000’s, the US High Energy Physics community contributing to the Large Hadron Collider (LHC) launched the LHC Accelerator R&D Program (LARP...
Color-Singlet and Color-Octet qq Quark Matters
Color-Singlet and Color-Octet qq Quark Matters
Quarks and antiquarks carry color and electric charges and belong to the color-triplet 3 group and the color-antitriplet 3- group respectively. The product groups of 3 and 3- consi...
Zero-jettiness resummation for top-quark pair production at the LHC
Zero-jettiness resummation for top-quark pair production at the LHC
Abstract We study the resummation of the 0-jettiness resolution variable $$ \mathcal{T} $$ T 0 for the top-quark pair product...
Top-quark physics at the CLIC electron-positron linear collider
Top-quark physics at the CLIC electron-positron linear collider
Abstract The Compact Linear Collider (CLIC) is a proposed future high-luminosity linear electron-positron collider operating at three energy stages, with nomin...
Constraining anomalous gluon self-interactions at the LHC: a reappraisal
Constraining anomalous gluon self-interactions at the LHC: a reappraisal
Abstract Anomalous self-interactions of non-abelian gauge fields can be described by higher dimensional operators featuring gauge-invariant combinations of the...
On the momentum space structure of the quark propagator
On the momentum space structure of the quark propagator
Abstract The structure of the quark propagator in momentum space is explored taking into account non-perturbative QCD dynamics constraints fo...
Top Quark Mass Measurement at TEVATRON and LHC Energies
Top Quark Mass Measurement at TEVATRON and LHC Energies
This research work provides a review of a well heaviest known quark i.e. Top Quark (a fundamental particle ever observed). In hadron collisions, it produces in particle-antiparticl...

Back to Top