QCD and Collider Physics

By R. Ellis, W. J. Stirling, B. R. Webber. 2003

392 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/913bb236fa6ff5bb389176e339a5364fb28c2e54

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Citations in the corpus

The color glass condensate and hadron production in the forward region (2005, methodology): “with the LO splitting functions as given in [25].”
Probing Novel Scalar and Tensor Interactions from (Ultra)Cold Neutrons to the LHC (2011, background): “To determine the transverse mass distribution of the electron–neutrino pair we start with [128]”
A perturbative framework for jet quenching (2012, background): “However, it is worth noting that the choices of t ≈ θ2 and t ≈ k2 ⊥ emerge as better suited when inspecting the radiation pattern of two subsequent emissions since they better capture effects related to the emergence of destructive interference in non-angular-ordered emissions [4, 59, 60].”
Herwig++ physics and manual (2008, background): “17) is then just the usual soft eikonal dipole function describing soft gluon radiation by a colour dipole [63], at least for the majority of cases where the colour partner is massless or nearly massless.”
QCD matrix elements + parton showers. The NLO case (2012, background): “There are two possible formulations of the respective no-branching probability, which can be interchanged and which are fully equivalent [45,46].”
The midpoint between dipole and parton showers (2015, unknown): “The Altarelli-Parisi splitting functions would give Γ(N) = −2HN , with HN the Nth harmonic number, and K(N) = 1/N [24].”
Interference effects in medium-induced gluon radiation (2011, background): “This ‘dipole antenna’ is a familiar set–up for studies of interference and angular ordering for radiation in the vacuum [28, 29] and has been generalized in Refs.”
Determination of fragmentation functions and their uncertainties (2007, background): “The fragmentation function is defined by the hadronproduction cross section and the total hadronic cross section [10]:”
Towards an all-orders calculation of the electroweak bubble wall velocity (2020, background): “It can be derived more generally based on spinor algebra [25] and is the basis for both analytic resummation techniques as well as parton showers [88].”
Collinearly-improved BK evolution meets the HERA data (2015, background): “not enhanced by a large logarithm) ᾱ2 s terms, this looks like what is called the “fastest apparent convergence” (fac) scheme [60–62].”
QCD Matrix Elements + Parton Showers (2001, background): “11) Recall that in coherent parton branching the evolution variable is the emission angle [16] and the corresponding scale is the parton energy times the angle [17].”
Infrared structure at NNLO using antenna subtraction (2013, background): “2 Next-to-leading order splitting kernels The one-loop quark-quark and quark-antiquark splitting kernels, P 1qiqj and P 1 qiq̄j , contain a non-trivial flavour structure and are classified according to flavour singlet, P S,1 ij , and flavour non-singlet, P V,1 ij contributions [71].”
Unraveling hadron structure with generalized parton distributions (2005, background): “The studies of jets explicitly demonstrated that they carry genuine properties, computable from the first principles, of their predecessors—quarks and gluons [29].”
Parton Distributions in Nucleons and Nuclei (2020, methodology): “In this respect, our review updates and extends the reviews provided in References 4 and 5 and presents a critical snapshot of PDFs as a bridge between low-and high-energy physics.”
Matrix elements and parton showers in hadronic interactions. (2002, background): “For further details I would like to refer to [16].”
Jet angular correlation in vector-boson fusion processes at hadron colliders (2009, background): “This is well known as the knowledge of the QCD parton branching; a quark-antiquark pair from the gluon, g∗ → qq̄, has the strong correlation between the gluon polarization and the decay plane, while for g∗ → gg the correlation is weak [51].”
Antenna subtraction at NNLO with hadronic initial states: initial-final configurations (2009, methodology): “Owing to their large production cross sections, various jet observables can be measured to a high statistical accuracy, thus making them ideal for precision studies [1, 2]:”