[PDF] Top 20 Event Generators for Multi Hadronic Production in e+e− Collisions
Has 10000 "Event Generators for Multi Hadronic Production in e+e− Collisions" found on our website. Below are the top 20 most common "Event Generators for Multi Hadronic Production in e+e− Collisions".
Event Generators for Multi Hadronic Production in e+e− Collisions
... The vacuum polarization (VP) has been calculated by many groups and is available in the literature. Comparisons between them are given in Ref. [12]. There are notable differences below 1.6 GeV, and above 2.0 GeV; visible ... See full document
9
Measurement of the cross section for Z → e+e production in pp collisions at √s=7 TeV
... at 100 GeV /c for hadrons and muons, and an impact parameter resolution of 20 µm for tracks with high transverse momentum. Charged hadrons are identified using two ring- imaging Cherenkov detectors. Photon, electron and ... See full document
21
Universality of particle production and energy balance in hadronic and nuclear collisions
... multiparticle production in nucleus-nucleus (AA) and hadronic interactions in view of a new scaling obtained ...in hadronic and the most central (head-on) AA collisions and on the number of ... See full document
9
Precise measurements of the hadronic cross sections with the CMD-3 and SND detectors at the VEPP-2000 e+ e− collider
... the e + e − → hadrons cross sections in the wide energy range up to 2 GeV, studies of known and searches for new vector mesons, studies of n¯ n and p p ¯ production cross sections near threshold and ... See full document
8
Hadronic resonances from ALICE in pp collisions
... In section 2 a brief introduction of the detector characteristics which a ff ect this analysis is pre- sented. Tracking and particle identification are discussed. In section 3 the analysis is described with emphasis on ... See full document
8
Jet physics in hadronic collisions: theoretical remarks
... One more observation is worthwhile. Even though the shower-only approach gives a good description of inclu- sive multijet rates, there is no guarantee that kinemati- cal correlations among the jets are equally well ... See full document
6
E-by-e fluctuations of initial conditions in interactions of light, intermediate and heavy nuclei at energies 4 - 200 GeV per nucleon
... the E-by-E initial state fluctuations has been revealed by AL- ICE collaboration ...particle production is driven by colli- sion geometry instead of the system ... See full document
8
Hadron production in e+e−collisions at BABAR and implications on the muon anomalous magnetic moment
... clusive hadronic cross sections. This method allows high statistics e + e − experiments running at a fixed center-of- mass ...lower e ff ective ... See full document
7
Studies of soft QCD at LHCb
... Abstract. This paper summarises two analyses of minimum bias data collected with the LHCb detector from pp collisions at the LHC. The geometry, tracking and particle identification system of the LHCb experiment ... See full document
5
Hadron resonance production and final state hadronic interactions with UrQMD at LHC
... Table 1 shows the branching ratios of di ff erent baryonic resonances, decaying to hyperon + Kaon, implemented in UrQMD. While many of them are known [28] some of them have large errors (or- ange) and some branching ... See full document
8
Prediction of the particle production in pp collisions with the MPD detector at NICA collider
... proton-proton collisions have been extensively used as a baseline reference for nucleus-nucleus ...the Multi–Purpose Detector (MPD) to register data from small systems at the energy range of ...as ... See full document
7
New results from the NA49 experiment on hadron production in p+p and p+C interactions and survey of backward hadrons in p+C collisions
... kaon production in proton-proton and proton, anti-proton, neutron, deuteron and triton production in proton-carbon collisions at 158 GeV/c beam momentum are ... See full document
5
An Overview of Recent Results from STAR
... Heavy quarks, charm and bottom, are produced by the hard process in the initial interactions with large momentum transfer before QGP formed. They have different interactions with the QGP compare to light quarks. Hence, ... See full document
11
Recent results of the hadronic cross section measurements with the CMD-3 detector at e+e− collider VEPP-2000
... The e + e − → K + K − η process has been earlier studied by ...main production mechanism is e + e − → φ(1680) → ...the e + e − → φ(1020)η process are shown in ... See full document
6
Transition formfactors γ* → γf2 (1270) and γ* → γa2 (1320) in the e+e− collisions
... [5], solid line above 5 GeV is drawn with zero vector widths, dashed lines are their continuations.. The experimental BaBar point [1] is shown also.[r] ... See full document
6
EFFECTS OF VISCOSITY IN MAGNETOPLASMADYNAMICS GENERATORS EUR 520 e
... Reprinted from the Proceedings of the "Symposium on Magnetoplasmadynamic Electrical Power Generation,, - Newcastle upon Tyne England - September 1902.. Some effects associated with the v[r] ... See full document
10
The investigation of spin effects in (e,2e) collisions
... In experimental physics it is essential to consider the relevant theory, so that the information gathered from the experiment can be optimised. That is, the theory guides the experiment to areas of interest and which may ... See full document
128
Numerical investigation of finite-volume effects for the HVP
... volume e ff ects from lattice scalar QED is straight- forward: expectation values are calculated from the discretised scalar QED path integral, and this is repeated for several lattice ... See full document
8
First results from p–Pb collisions at the LHC
... cle production and the role of initial state e ff ects in QCD at small-x ...ractive collisions and reported in the laboratory sys- tem ...nucleon–nucleon collisions (as for exam- ple modeled ... See full document
6
Search for charged Higgs bosons in e(+)e(-) collisions at root s=181-184 GeV
... Pair production of charged Higgs bosons occurs mainly via s-channel exchange of a photon or a Z boson; in two-doublet models, the couplings are completely specified in terms of the electric charge and u W , making ... See full document
12
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