Resummation of non-global QCD observables
By M. Dasgupta, G. Salam. 2001
270 citations recorded by the source corpus.
Abstract We discuss issues related to the resummation of non-global observables in QCD, those that are sensitive to radiation in only a part of phase space. Examples of such observables are certain single-hemisphere event shapes in e + e − and DIS. Compared to global observables (those sensitive to all emissions, e.g., the e + e − thrust) a new class of single-logarithmic terms arises. These have been neglected in recent calculations in the literature. For a whole set of single hemisphere e + e − and DIS event shapes, we analytically evaluate the first such term, at order α s 2 , and give numerical results for the resummation of these terms in the large- N C limit.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/d613d2d633ba9ac0b1e6138ff03e8f00a25323e4
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Nuclear and High Energy Physics
- Cms Collaboration
- A. Larkoski
- G. Salam
- Jesse Thaler
- G. Soyez
- W. Waalewijn
- Atlas Collaboration
- I. Moult
Citations in the corpus
- The anti-$k_t$ jet clustering algorithm (2008, background): “Examples are the jet-mass distribution [9] and energy flow distributions in restricted regions [10 – 12].”
- Resummed event shapes at hadron - hadron colliders (2004, background): “J H E P 0 8 ( 2 0 0 4 ) 0 6 2 event shapes [37], i.”
- Factorization at the LHC: From PDFs to Initial State Jets (Ph.D. thesis) (2009, background): “ for hadron colliders have been classied and studied in Refs. [27, 28], and are referred to as global event shapes. (Issues related to non-global observables have been discussed for example in Refs. [20, 46, 82, 97].) 1Note that the proof of factorization for the partonic cross section in the parton”
- Jet shapes and jet algorithms in SCET (2010, methodology): “) These issues are related to some types of “non-global” logarithms described by [46, 56, 57, 58] that spoil the simple characterization of NLL accuracy.”
- The Catchment Area of Jets (2008, background): “One should of course bear in mind that the multi-particle structure of the hadron level is such that a single-gluon result cannot contain all the relevant physics — this implies that one should, in future work, examine multi-soft gluon radiation as well, perhaps along the lines of the calculation of”
- Accounting for coherence in interjet Et flow (2002, methodology): “The second source of complexity is the geometry of multi-gluon events, which we treat using a Monte Carlo algorithm like that discussed in [6], which essentially models a tree-like sequence where a colour dipole emits a gluon, thus branching into two dipoles,”
- Towards jetography (2009, background): “(see [133] for more detailed analytic expressions, or [134, 136] for corresponding resummed results in e+e−collisions) and the logarithm can in part compensate the smallness of αs, especially at larger pt.”
- Factorization at the LHC: From parton distribution functions to initial state jets (2010, unknown): “[20, 46, 82, 97].”