647 research outputs found
Gauge-Boson Production in Electron-Photon Collisions
We summarize results for the processes within the electroweak Standard Model. We discuss the essential
features of the corresponding lowest-order cross-sections and present numerical
results for the unpolarized cross-sections including the complete
virtual, soft-photonic, and hard-photonic corrections. While at low energies
the weak corrections are dominated by the leading universal corrections, at
high energies we find large, non-universal corrections, which arise from vertex
and box diagrams involving non-Abelian gauge couplings.Comment: 7 pages + 5 figures appended as ps-files (uuencoded), latex, CERN-TH.
6980/9
The Higgs Boson in the Standard Model - From LEP to LHC: Expectations, Searches, and Discovery of a Candidate
The quest for the Higgs boson of the Standard Model, which was a cornerstone
in the physics programme at particle colliders operating at the energy frontier
for several decades, is the subject of this review. After reviewing the
formulation of electroweak symmetry breaking via the Higgs mechanism within the
Standard Model, the phenomenology of the Higgs boson at colliders and the
theoretical and phenomenological constraints on the Standard Model Higgs sector
are discussed. General remarks on experimental searches and the methodology of
statistical interpretation are followed by a description of the phenomenology
of Higgs-boson production and the corresponding precise predictions. The
strategies of the experimental searches and their findings are discussed for
the Large Electron Positron Collider (LEP) at CERN, the proton-antiproton
collider Tevatron at Fermilab, and the proton-proton Large Hadron Collider
(LHC) at CERN. The article concludes with the description of the observation of
a Higgs-like boson at the LHC.Comment: 82 pages, 34 figures, minor modifications, version equivalent to the
one published in Prog. Part. Nucl. Phy
Approximations for W-Pair Production at Linear-Collider Energies
We determine the accuracy of various approximations to the O(alpha)
corrections for on-shell W-pair production. While an approximation based on the
universal corrections arising from initial-state radiation, from the running of
alpha, and from corrections proportional to m_t^2 fails in the Linear-Collider
energy range, a high-energy approximation improved by the exact universal
corrections is sufficiently good above about 500GeV. These results indicate
that in Monte Carlo event generators for off-shell W-pair production the
incorporation of the universal corrections is not sufficient and more
corrections should be included.Comment: 7 pages, late
Techniques for one-loop tensor integrals in many-particle processes
We briefly sketch the methods for a numerically stable evaluation of tensor
one-loop integrals that have been used in the calculation of the complete
electroweak one-loop corrections to \Pep\Pem\to4 fermions. In particular, the
improvement of the new methods over the conventional Passarino--Veltman
reduction is illustrated for some 4-point integrals in the delicate limits of
small Gram (and other kinematical) determinants.Comment: 5 pages, latex, 2 postscript figures, to appear in the proceedings of
the "7th International Symposium on Radiative Corrections (RADCOR2005)",
Shonan Village, 200
Reduction schemes for one-loop tensor integrals
We present new methods for the evaluation of one-loop tensor integrals which
have been used in the calculation of the complete electroweak one-loop
corrections to e+ e- -> 4 fermions. The described methods for 3-point and
4-point integrals are, in particular, applicable in the case where the
conventional Passarino-Veltman reduction breaks down owing to the appearance of
Gram determinants in the denominator. One method consists of different variants
for expanding tensor coefficients about limits of vanishing Gram determinants
or other kinematical determinants, thereby reducing all tensor coefficients to
the usual scalar integrals. In a second method a specific tensor coefficient
with a logarithmic integrand is evaluated numerically, and the remaining
coefficients as well as the standard scalar integral are algebraically derived
from this coefficient. For 5-point tensor integrals, we give explicit formulas
that reduce the corresponding tensor coefficients to coefficients of 4-point
integrals with tensor rank reduced by one. Similar formulas are provided for
6-point functions, and the generalization to functions with more internal
propagators is straightforward. All the presented methods are also applicable
if infrared (soft or collinear) divergences are treated in dimensional
regularization or if mass parameters (for unstable particles) become complex.Comment: 55 pages, latex, some references updated and few comments added,
version to appear in Nucl. Phys.
Electroweak Radiative Corrections to Off-Shell W-Pair Production
We briefly describe the RacoonWW approach to calculate radiative corrections
to e+ e- -> W W -> 4 fermions and present numerical results for the total
W-pair production cross section at LEP2.Comment: 3 pages, 2 figures, talk given at the DPF2000 meeting, Columbus, OH,
August 9-12, 200
Z+jet production at the LHC: Electroweak radiative corrections
The investigation of weak bosons (, )
produced with or without associated hard QCD jets will be of great
phenomenological interest at the LHC. Owing to the large cross sections and the
clean decay signatures of the vector bosons, weak-boson production can be used
to monitor and calibrate the luminosity of the collider, to constrain the PDFs,
or to calibrate the detector. Moreover, the +jet(s) final state constitutes
an important background to a large variety of signatures of physics beyond the
Standard Model. To match the excellent experimental accuracy that is expected
at the LHC, we have worked out a theoretical next-to-leading-order analysis of
+jet production at hadron colliders. The focus of this talk will be on new
results on the full electroweak corrections to +jet production
at the LHC. All off-shell effects are included in our approach, and the finite
lifetime of the boson is consistently accounted for using the complex-mass
scheme. In the following, we briefly introduce the calculation and discuss
selected phenomenological implications of our results.Comment: 5 pages, 2 figures, talk at the "35th International Conference on
High Energy Physics", Paris, France, July 22 -- 28, 201
Probing anomalous quartic gauge-boson couplings via e+e- --> 4fermions+gamma
All lowest-order amplitudes for e+e- --> 4f+gamma are calculated including
five anomalous quartic gauge-boson couplings that are allowed by
electromagnetic gauge invariance and the custodial SU(2)_c symmetry. Three of
these anomalous couplings correspond to the operators L_0, L_c, and L_n that
have been constrained by the LEP collaborations in WWgamma production. The
anomalous couplings are incorporated in the Monte Carlo generator RACOONWW.
Moreover, for the processes e+e- --> 4f+gamma RACOONWW is improved upon
including leading universal electroweak corrections such as initial-state
radiation. The discussion of numerical results illustrates the size of the
leading corrections as well as the impact of the anomalous quartic couplings
for LEP2 energies and at 500GeV.Comment: 27 pages, latex, 42 postscript files, some misprints correcte
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