69 research outputs found
Precision Predictions for (Un)Stable WW/4f Production in e +e- Annihilation: YFSWW3/KoralW-1.42/YFSZZ
We present precision calculations of the processes e+ e- -> 4-fermions in
which the double resonant W+ W- and ZZ intermediate states occur. Referring to
these latter intermediate states as the 'signal processes', we show that, by
using the YFS Monte Carlo event generators YFSWW3-1.14 and KoralW-1.42 in an
appropriate combination, we achieve a physical precision on the WW signal
process, as isolated with LEP2 MC Workshop cuts, below 0.5 per cent. We stress
the full gauge invariance of our calculations and we compare our results with
those of other authors where appropriate. In particular, sample Monte Carlo
data are explicitly illustrated and compared with the results of the program
RacoonWW of Denner et al. In this way, we cross check that the total (physical
oplus technical) precision tag for the WW signal process cross section is 0.4
per cent for 200 GeV, for example. Results are also given for 500 GeV with an
eye toward the LC. For the analogous ZZ case, we cross check that our YFSZZ
calculation yields a total precision tag of 2 per cent, when it is compared to
the results of ZZTO and GENTLE of Passarino and Bardin et al., respectively.Comment: 14 pages, 1 figure, 4 tables, presented at RADCOR2000 by B.F.L. War
Coherent Exclusive Exponentiation for Precision Monte Carlo Calculations of Fermion Pair Production / Precision Predictions for (Un)stable W+W- Pairs
We present the new Coherent Exclusive Exponentiation (CEEX), in comparison to
the older Exclusive Exponentiation (EEX) and the semi-analytical Inclusive
Exponentiation (IEX), for the process e+e- -> f-bar f + n(gamma),
f=mu,tau,d,u,s,c,b, with validity for centre of mass energies from tau lepton
threshold to 1 TeV. We analyse 2f numerical results at the Z-peak, 189 GeV and
500 GeV. We also present precision calculations of the signal processes e+e- ->
4f in which the double resonant W+W- intermediate state occurs using our
YFSWW3-1.14 MC. Sample 4f Monte Carlo data are explicitly illustrated in
comparison to the literature at LEP2 energies. These comparisons show that a TU
for the signal process cross section of 0.4 percent is valid for the LEP2 200
GeV energy. LC energy results are also shown.Comment: 5 pages, 4 figures, Presented at ICHEP200
QED Exponentiation for quasi-stable charged particles: the process
All real and virtual infrared singularities in the standard analysis of the
perturbative Quantum Electrodynamics (like that of Yennie-Frautschi-Suura) are
associated with photon emissions from the external legs in the scattering
process. External particles are stable, with the zero decay width. Such
singularities are well understood at any perturbative order and are resummed.
The case of production and decay of the semi-stable {\em neutral} particles
like boson or lepton, with the narrow decay width, ,
is also well understood at any perturbative order and soft photon resummation
can be done. For the absent or loose upper cut-off on the total photon energy
the production and decay process of the semi-stable (neutral)
particles decouples approximately and can be considered quasi-independently. In
particular soft photon resummation can be done separately for the production
and decay process treating semi-stable (neutral) particle as stable. So far,
consistent treatment of the soft photon resummation for semi-stable {\em
charged} particles like boson is not available in the literature and
the aim of this work is to present a solution for this problem. Generally, it
should be feasible because the underlying physics is the same as in the case of
the neutral semi-stable resonances -- in the limit production
and decay processes for charged particles also necessarily decouple due to long
lifetime of the particles. The technical problems to be solved in this work are
related to the fact that semi-stable charged particle are able to emit photons.Comment: Short version has appeared in conference materials, Symmetry 11, 1389
(2019
Performance Evaluation of Road Traffic Control Using a Fuzzy Cellular Model
In this paper a method is proposed for performance evaluation of road traffic
control systems. The method is designed to be implemented in an on-line
simulation environment, which enables optimisation of adaptive traffic control
strategies. Performance measures are computed using a fuzzy cellular traffic
model, formulated as a hybrid system combining cellular automata and fuzzy
calculus. Experimental results show that the introduced method allows the
performance to be evaluated using imprecise traffic measurements. Moreover, the
fuzzy definitions of performance measures are convenient for uncertainty
determination in traffic control decisions.Comment: The final publication is available at http://www.springerlink.co
The Gamma Factory path to high-luminosity LHC with isoscalar beams
There are two main ways to increase LHC luminosity without upgrading CERN injectors: (1) modification of beam-collision optics and (2) reduction of beam transverse emittance. The former is followed in the ongoing high-luminosity upgrade of the LHC (HL-LHC), while the latter, applicable only to ion beams, is described in this contribution. The reduction of the beam emittance can be achieved by employing a laser-cooling technique to bunches of partially stripped ions at the SPS flat-top energy. In the case the isoscalar calcium beams fulfilling the presentbeam-operation constrains, the transverse beam emittance can be reduced in this way by a factor of 5 during the 8 second long cooling phase. This would allow to reach the nucleon–nucleon luminosity L_NN = 4.2 x 10^34 s^(-1)cm^(-2), which is comparable to the levelled luminosity for the HL-LHC proton–proton collisions, but with reduced pile-up background. The calcium–calcium collisions have several advantages over the proton–proton collisions for the electroweak physics, such as precision measurements of the W-boson mass and sin^2_W, clean observation of the Higgs boson decay into bbar in its photoproduction channel or BSM phenomena. If this scheme is confirmed by the future Gamma Factory proof-of-principle experiment, it could be implemented at CERN with minor infrastructure investments. This contribution is based on Ref. [1
Z-boson as "the standard candle" for high precision W-boson physics at LHC
In this paper we propose a strategy for measuring the inclusive W-boson
production processes at LHC. This strategy exploits simultaneously the unique
flexibility of the LHC collider in running variable beam particle species at
variable beam energies, and the configuration flexibility of the LHC detectors.
We propose their concrete settings for a precision measurement of the Standard
Model parameters. These dedicated settings optimise the use of the Z boson and
Drell-Yan pair production processes as ``the standard reference candles''. The
presented strategy allows to factorise and to directly measure those of the QCD
effects which affect differently the W and Z production processes. It reduces
to a level of 10^{-4} the impact of uncertainties in the partonic distribution
functions (PDFs) and in the transverse momentum of the quarks on the
measurement precision. Last but not the least, it reduces by a factor of 10 an
impact of systematic measurement errors, such as the energy scale and the
measurement resolution, on the W-boson production observables.Comment: 20 pages, 4 figure
Inclusion of the QCD next-to-leading order corrections in the quark-gluon Monte Carlo shower
Methodology of including QCD NLO corrections in the quark--gluon Monte Carlo
shower is outlined. The work concentrates on two issues: (i) constructing
leading order (LO) parton shower Monte Carlo from scratch, such that it
rigorously extends collinear factorization into the exclusive (fully
unintegrated) one which we call the Monte Carlo factorization scheme; (ii)
introducing next-to-leading-order (NLO) corrections to the hard process in this
new environment. The presented solution is designed to be extended to the full
NLO level Monte Carlo, including NLO corrections not only in the hard process
but in the whole shower. The issue of the difference between the factorization
scheme implemented in the Monte Carlo (MC) solution and the standard MSbar
scheme is addressed. The principal MC implementation is designed for the
electroweak boson production process at the LHC, but in order to discuss
universality -- process independence, the deep inelastic lepton--hadron
scaterring is also brought into the MC framework.Comment: 28 pages, 6 figures, updated to match journal versio
Precision predictions for W-pair production at LEP2
Theoretical calculations for the W-pair production process at LEP2 in terms
of Monte Carlo event generators RacoonWW and KorlaW&YFSWW3 are reviewed. The
discussion concentrates on precision predictions for the main LEP2 WW
observables. The theoretical precision of the above programs is estimated to be
~0.5% for the total WW cross section sigma_{WW}, ~5MeV for the W-boson mass
M_W, and ~0.005 for the triple-gauge-boson coupling lambda = lambda_{gamma} =
lambda_Z, which is sufficient for the final LEP2 data analyses.Comment: 9 pages, LaTe
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