2,841 research outputs found
The Four-Jet Rate in e+e- Annihilation
We present an analytic expression for the four-jet rate in e+e- annihilation,
calculated using the coherent branching formalism in the Durham scheme. Our
result resums all the leading and next-to-leading kinematic logarithms to all
orders in the QCD strong coupling constant.Comment: 7 pages; Final result for R4 and D7 corrected and a couple of typos
fixe
BFKL predictions at small x from k_T and collinear factorization viewpoints
Hard scattering processes involving hadrons at small are described by a
-factorization formula driven by a BFKL gluon. We explore the equivalence
of this description to a collinear-factorization approach in which the
anomalous dimensions and are expressed as
power series in , or to be precise where
is the moment index. In particular we confront the
collinear-factorization expansion with that extracted from the BFKL approach
with running coupling included.Comment: 11 LaTeX pages, 1 figure (uuencoded
Approximate NNLO Threshold Resummation in Heavy Flavour Decays
We present an approximate NNLO evaluation of the QCD form factor resumming
large logarithmic perturbative contributions in semi-inclusive heavy flavour
decays.Comment: 16 pages, 3 figures, Latex; minor changes; 2 figures adde
THE GLUON DISTRIBUTION AT SMALL x OBTAINED FROM A UNIFIED EVOLUTION EQUATION.
We solve a unified integral equation to obtain the and
dependence of the gluon distribution of a proton in the small regime; where
and are the longitudinal momentum fraction and the transverse
momentum of the gluon probed at a scale . The equation generates a gluon
with a steep behaviour, with , and a
distribution which broadens as decreases. We compare our solutions with, on
the one hand, those that we obtain using the double-leading-logarithm
approximation to Altarelli-Parisi evolution and, on the other hand, to those
that we determine from the BFKL equation.Comment: LaTeX file with 10 postscript figures (uuencoded
Threshold Effects in Slepton-Pair Production at the LHC
We present a study of threshold resummation effects for slepton pair
production at the Large Hadron Collider (LHC). After confirming the known NLO
QCD corrections and generalizing the NLO SUSY-QCD corrections to the case of
mixing squarks in the virtual loop contributions, we employ the Mellin N-space
resummation formalism to compute logarithmically enhanced soft-gluon terms to
all perturbative orders.Comment: 3 pages, 1 figure, presented at HEP 2007 (Manchester, July 2007
The description of F2 at small x incorporating angular ordering
We study the perturbative QCD description of the HERA measurements of using a gluon distribution that is obtained from an evolution
incorporating angular ordering of the gluon emissions, and which embodies both
GLAP and BFKL dynamics. We compare the predictions with recent HERA data for
. We present estimates of the charm component and of .Comment: 8 LaTeX pages + 4 uuencoded figure
Infrared singularities of scattering amplitudes in perturbative QCD
An exact formula is derived for the infrared singularities of dimensionally
regularized scattering amplitudes in massless QCD with an arbitrary number of
legs, valid at any number of loops. It is based on the conjecture that the
anomalous-dimension matrix of n-jet operators in soft-collinear effective
theory contains only a single non-trivial color structure, whose coefficient is
the cusp anomalous dimension of Wilson loops with light-like segments. Its
color-diagonal part is characterized by two anomalous dimensions, which are
extracted to three-loop order from known perturbative results for the quark and
gluon form factors. This allows us to predict the three-loop coefficients of
all 1/epsilon^k poles for an arbitrary n-parton scattering amplitudes,
generalizing existing two-loop results.Comment: 4 pages; v2: typo in eq. (12) fixed, references updated; v3:
additional term in (12
Quark-Gluon Jet Differences at LEP
A new method to identify the gluon jet in 3-jet ``{\bf Y}'' decays of
is presented. The method is based on differences in particle multiplicity
between quark jets and gluon jets, and is more effective than tagging by
leptonic decay. An experimental test of the method and its application to a
study of the ``string effect'' are proposed. Various jet-finding schemes for
3-jet events are compared.Comment: 11 pages, LaTeX, 4 PostScript figures availble from the author
([email protected]), MSUTH-92-0
Sudakov Resummations at Higher Orders
We summarize our recent results on the resummation of hard-scattering
coefficient functions and on-shell form factors in massless perturbative QCD.
The threshold resummation has been extended to the fourth logarithmic order for
deep-inelastic scattering, Drell-Yan lepton pair production and Higgs
production via gluon-gluon fusion. The leading six infrared pole terms have
been derived to all orders in the strong coupling constant for the
photon-quark-quark and the (heavy-top) Higgs-gluon-gluon form factors. These
results have many implications, most notably they lead to a new best estimate
for the Higgs production cross section at the LHC.Comment: 12 pages, LaTeX, 2 eps-figures. Uses modification appbav.cls
(included) of the appolb.cls style. Presented by S.M. and A.V. at the
conferences `Matter to the Deepest', Ustron (Poland), September '05, and
RADCOR 2005, Shonan Village (Japan), October '05. To appear, in the latter
case in shortened form, in the proceeding
A next-to-next-to-leading order calculation of soft-virtual cross sections
We compute the next-to-next-to-leading order (NNLO) soft and virtual QCD
corrections for the partonic cross section of colourless-final state processes
in hadronic collisions. The results are valid to all orders in the dimensional
regularization parameter \ep. The dependence of the results on a particular
process is given through finite contributions to the one and two-loop
amplitudes. To evaluate the accuracy of the soft-virtual approximation we
compare it with the full NNLO result for Drell-Yan and Higgs boson production
via gluon fusion. We also provide a universal expression for the hard
coefficient needed to perform threshold resummation up to
next-to-next-to-leading logarithmic (NNLL) accuracy.Comment: 25 pages, 4 figure
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