22,730 research outputs found
Axial Contributions at the Top Threshold
We calculate the contributions of the axial current to top quark pair
production in e+ e- annihilation at threshold. The QCD dynamics is taken into
account by solving the Lippmann-Schwinger equation for the P wave production
using the QCD potential up to two loops. We demonstrate that the dependence of
the total and differential cross section on the polarization of the e+ and e-
beams allows for an independent extraction of the axial current induced cross
section.Comment: LaTeX, 12 pages, including 5 Postscript figures using eps
Reply to the Comment on `Deterministic Single-Photon Source for Distributed Quantum Networking'
Reply to the comment of H. J. Kimble [quant-ph/0210032] on the experiment
realizing a "deterministic single-photon source for distributed quantum
networking" by Kuhn, Hennrich, and Rempe [Phys. Rev. Lett. 89, 067901 (2002),
quant-ph/0204147].Comment: 1 page 1 figur
Radiative return at NLO and the measurement of the hadronic cross-section in electron-positron annihilation
Electron-positron annihilation into hadrons plus an energetic photon from
initial state radiation allows the hadronic cross-section to be measured over a
wide range of energies. The full next-to-leading order QED corrections for the
cross-section for e^+ e^- annihilation into a real tagged photon and a virtual
photon converting into hadrons are calculated where the tagged photon is
radiated off the initial electron or positron. This includes virtual and soft
photon corrections to the process e^+ e^- \to \gamma +\gamma^* and the emission
of two real hard photons: e^+ e^- \to \gamma + \gamma + \gamma^*. A Monte Carlo
generator has been constructed, which incorporates these corrections and
simulates the production of two charged pions or muons plus one or two photons.
Predictions are presented for centre-of-mass energies between 1 and 10 GeV,
corresponding to the energies of DAPHNE, CLEO-C and B-meson factories.Comment: 13 pages, 15 figure
Measurement of sigma_Total in e+e- Annihilations Below 10.56 GeV
Using the CLEO III detector, we measure absolute cross sections for e+e- ->
hadrons at seven center-of-mass energies between 6.964 and 10.538 GeV. R, the
ratio of hadronic and muon pair production cross sections, is measured at these
energies with a r.m.s. error <2% allowing determinations of the strong coupling
alpha_s. Using the expected evolution of alpha_s with energy we find
alpha_s(M_Z^2)=0.126 +/- 0.005 ^{+0.015}_{-0.011}, and
Lambda=0.31^{+0.09+0.29}_{-0.08-0.21}.Comment: Comments: Presented at "The 2007 Europhysics Conference on High
Energy Physics," Manchester, England, 19-25 July 2007, to appear in the
proceedings. Three pages, 1 figur
Perspectives for the radiative return at meson factories
The measurement of the pion form factor and, more generally, of the cross
section for electron-positron annihilation into hadrons through the radiative
return has become an important task for high luminosity colliders such as the
Phi- or B-meson factories. This quantity is crucial for predictions of the
hadronic contributions to the anomalous magnetic moment of the muon, and to the
running of the electromagnetic coupling. But the radiative return opens the
possibility of many other physical applications. The physics potential of this
method at high luminosity meson factories is discussed, the last upgraded
version of the event generator PHOKHARA is presented, and future developments
are highlighted.Comment: Presented at SIGHAD03: Worskhop on Hadronic Cross Section at Low
Energy, Pisa,Italy, October 8th-10th, 200
TeV scale Dark Matter and electroweak radiative corrections
Recent anomalies in cosmic rays data, namely from the PAMELA collaboration,
can be interpreted in terms of TeV scale decaying/annihilating Dark Matter. We
analyze the impact of radiative corrections coming from the electroweak sector
of the Standard Model on the spectrum of the final products at the interaction
point. As an example, we consider virtual one loop corrections and real gauge
bosons emission in the case of a very heavy vector boson annihilating into
fermions. We show that the effect of electroweak corrections is relevant, but
not as big as sometimes claimed in the literature. At such high scales, one
loop electroweak effects are so big that eventually higher orders/resummations
have to be considered: we advocate for the inclusion of these effects in parton
shower Montecarlos aiming at the description of TeV scale physics.Comment: Comments added, published versio
Summing up Subleading Sudakov Logarithms
We apply the strategy of regions within dimensional regularization to find
functions involved in evolution equations which govern the asymptotic dynamics
of the Abelian form factor and four-fermion amplitude in the SU(N) gauge theory
in the Sudakov limit up to the next-to-leading logarithmic approximation. The
results are used for the analysis of the dominant electroweak corrections to
the fermion-antifermion pair production in the annihilation at high
energy.Comment: 17 pages LaTeX, missprins corrected, references adde
Next-to-Next-to-Leading Electroweak Logarithms for W-Pair Production at LHC
We derive the high energy asymptotic of one- and two-loop corrections in the
next-to-next-to-leading logarithmic approximation to the differential cross
section of -pair production at the LHC. For large invariant mass of the
W-pair the (negative) one-loop terms can reach more than 40%, which are
partially compensated by the (positive) two-loop terms of up to 10%.Comment: 23 pages, 9 figures, added explanations in section 3, corrected typos
and figures 7, 8,
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