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Institute
- Informatik (1577) (remove)
The inclusive charged particle transverse momentum distribution is measured in proton–proton collisions at s=900 GeV at the LHC using the ALICE detector. The measurement is performed in the central pseudorapidity region (|η|<0.8) over the transverse momentum range 0.15<pT<10 GeV/c. The correlation between transverse momentum and particle multiplicity is also studied. Results are presented for inelastic (INEL) and non-single-diffractive (NSD) events. The average transverse momentum for |η|<0.8 is 〈pT〉INEL=0.483±0.001 (stat.)±0.007 (syst.) GeV/c and 〈pT〉NSD=0.489±0.001 (stat.)±0.007 (syst.) GeV/c, respectively. The data exhibit a slightly larger 〈pT〉 than measurements in wider pseudorapidity intervals. The results are compared to simulations with the Monte Carlo event generators PYTHIA and PHOJET.
Harmonic decomposition of two particle angular correlations in Pb–Pb collisions at √sNN=2.76 TeV
(2012)
Angular correlations between unidentified charged trigger (t) and associated (a) particles are measured by the ALICE experiment in Pb–Pb collisions at √sNN=2.76 TeV for transverse momenta 0.25<pTt,a<15 GeV/c, where pTt>pTa. The shapes of the pair correlation distributions are studied in a variety of collision centrality classes between 0 and 50% of the total hadronic cross section for particles in the pseudorapidity interval |η|<1.0. Distributions in relative azimuth Δϕ≡ϕt−ϕa are analyzed for |Δη|≡|ηt−ηa|>0.8, and are referred to as “long-range correlations”. Fourier components VnΔ≡〈cos(nΔϕ)〉 are extracted from the long-range azimuthal correlation functions. If particle pairs are correlated to one another through their individual correlation to a common symmetry plane, then the pair anisotropy VnΔ(pTt,pTa) is fully described in terms of single-particle anisotropies vn(pT) as VnΔ(pTt,pTa)=vn(pTt)vn(pTa). This expectation is tested for 1⩽n⩽5 by applying a global fit of all VnΔ(pTt,pTa) to obtain the best values vn{GF}(pT). It is found that for 2⩽n⩽5, the fit agrees well with data up to pTa∼3–4 GeV/c, with a trend of increasing deviation as pTt and pTa are increased or as collisions become more peripheral. This suggests that no pair correlation harmonic can be described over the full 0.25<pT<15 GeV/c range using a single vn(pT) curve; such a description is however approximately possible for 2⩽n⩽5 when pTa<4 GeV/c. For the n=1 harmonic, however, a single v1(pT) curve is not obtained even within the reduced range pTa<4 GeV/c.
Rapidity and transverse momentum dependence of inclusive J/ψ production in pp collisions at √s=7 TeV
(2011)
The ALICE experiment at the LHC has studied inclusive J/ψ production at central and forward rapidities in pp collisions at √s=7 TeV. In this Letter, we report on the first results obtained detecting the J/ψ through the dilepton decay into e+e− and μ+μ− pairs in the rapidity ranges |y|<0.9 and 2.5<y<4, respectively, and with acceptance down to zero pT. In the dielectron channel the analysis was carried out on a data sample corresponding to an integrated luminosity Lint=5.6 nb−1 and the number of signal events is NJ/ψ=352±32(stat.)±28(syst.); the corresponding figures in the dimuon channel are Lint=15.6 nb−1 and NJ/ψ=1924±77(stat.)±144(syst.). The measured production cross sections are σJ/ψ(|y|<0.9)=10.7±1.0(stat.)±1.6(syst.)−2.3+1.6(syst.pol.)μb and σJ/ψ(2.5<y<4)=6.31±0.25(stat.)±0.76(syst.)−1.96+0.95(syst.pol.)μb. The differential cross sections, in transverse momentum and rapidity, of the J/ψ were also measured.
The first measurement of two-pion Bose–Einstein correlations in central Pb–Pb collisions at √sNN=2.76 TeV at the Large Hadron Collider is presented. We observe a growing trend with energy now not only for the longitudinal and the outward but also for the sideward pion source radius. The pion homogeneity volume and the decoupling time are significantly larger than those measured at RHIC.
Inclusive transverse momentum spectra of primary charged particles in Pb–Pb collisions at √sNN=2.76 TeV have been measured by the ALICE Collaboration at the LHC. The data are presented for central and peripheral collisions, corresponding to 0–5% and 70–80% of the hadronic Pb–Pb cross section. The measured charged particle spectra in |η|<0.8 and 0.3<pT<20 GeV/c are compared to the expectation in pp collisions at the same sNN, scaled by the number of underlying nucleon–nucleon collisions. The comparison is expressed in terms of the nuclear modification factor RAA. The result indicates only weak medium effects (RAA≈0.7) in peripheral collisions. In central collisions, RAA reaches a minimum of about 0.14 at pT=6–7 GeV/c and increases significantly at larger pT. The measured suppression of high-pT particles is stronger than that observed at lower collision energies, indicating that a very dense medium is formed in central Pb–Pb collisions at the LHC.
Augmented Reality ist eine Technologie, mit der die Wahrnehmung der realen Umgebung durch computergenerierte Sinnesreize verändert bzw. erweitert wird. Zur Erweiterung dieser „angereicherten Realität“ werden virtuelle Informationen wie z.B. 3D-Objekte, Grafiken und Videos in Echtzeit in Abbildern der realen Umgebung dargestellt. Die Erweiterungen helfen dem Anwender Aufgaben in der Realität auszuführen, da sie ihm Informationen bereitstellen, die er – ohne AR – nicht unmittelbar wahrnehmen könnte. Die Zielsetzung ist, dem Benutzer den Eindruck zu vermitteln, dass die reale Umgebung und die virtuellen Objekte koexistent miteinander verschmelzen. Für AR-Anwendungen existieren zahlreiche potenzielle Einsatzgebiete, doch verhindern bisher einige Probleme die Verbreitung dieser Technologie. Einer breiten Nutzung von AR-Anwendungen steht beispielsweise die Problematik gegenüber, dass deren Erstellung hohe programmiertechnische Anforderungen an die Entwickler stellt. Zur Verminderung dieser Probleme ist es wünschenswert Benutzern ohne Programmierkenntnisse (Autoren) die Entwicklung von AR-Anwendungen zu ermöglichen. Zum anderen bestehen technologische Probleme bei den für die Registrierung der virtuellen Objekte essenziellen Trackingverfahren. Weiterhin weisen die bisherigen AR-Anwendungen im Allgemeinen und die mittels autorenorientierter Systeme erstellten AR-Applikationen im Besonderen Defizite bezüglich der Authentizität der Darstellungen auf. Dabei sind hauptsächlich inkorrekte Verdeckungen und unrealistische Schatten bei den virtuellen Objekten verantwortlich für den Verlust des Koexistenzeindrucks. In dieser Arbeit wird unter Berücksichtigung der Trackingprobleme und auf Basis von Analysen, die die wichtigsten Authentizitätskriterien bestimmen, ein Konzept zur authentischen Integration von virtuellen Objekten in AR-Anwendungen erarbeitet und dargelegt. Auf diesem Integrationsprozess basierend werden Konzepte für Werkzeuge mit grafischen Benutzungsschnittstellen abgeleitet, mit denen Autoren die Erstellung von AR-Anwendungen mit hoher Darstellungsauthentizität ermöglicht wird. Einerseits verfügen die mit diesen Werkzeugen erstellten AR-Anwendungen über eine verbesserte Registrierung der virtuellen Objekte. Andererseits stellen die Werkzeuge Lösungen bereit, damit die virtuellen Objekte der AR-Anwendungen korrekte Verdeckungen aufweisen und über Schatten und Schattierungseffekte verfügen, die mit der tatsächlichen Beleuchtungssituation der realen Umgebung übereinstimmen. Sämtliche dieser Autorenwerkzeuge basieren auf einem in dieser Arbeit dargelegten Prinzip, bei dem die authentische Integration mittels leicht verständlicher bzw. wenig komplexer Arbeitsschritte und auf Basis der Verwendung einer Bildsequenz der realen Zielumgebung stattfindet. Die Konzepte dieser Arbeit werden durch die Implementierung der Autorenwerkzeuge validiert. Dabei zeigt sich, dass die Konzepte technisch umsetzbar sind. Die Evaluierung basiert auf der Gegenüberstellung eines in dieser Arbeit entwickelten Anforderungskatalogs und verdeutlicht die Eignung des Integrationsprozesses und der davon abgeleiteten Konzepte der Autorenwerkzeuge. Die Autorenwerkzeuge werden in eine bestehende, frei verfügbare AR-Autorenumgebung integriert.
The ALICE experiment has measured low-mass dimuon production in pp collisions at √s=7 TeV in the dimuon rapidity region 2.5<y<4. The observed dimuon mass spectrum is described as a superposition of resonance decays (η,ρ,ω,η′,ϕ) into muons and semi-leptonic decays of charmed mesons. The measured production cross sections for ω and ϕ are σω(1<pt<5 GeV/c,2.5<y<4)=5.28±0.54(stat)±0.49(syst) mb and σϕ(1<pt<5 GeV/c,2.5<y<4)=0.940±0.084(stat)±0.076(syst) mb. The differential cross sections d2σ/dydpt are extracted as a function of pt for ω and ϕ. The ratio between the ρ and ω cross section is obtained. Results for the ϕ are compared with other measurements at the same energy and with predictions by models.
he first measurements of the invariant differential cross sections of inclusive π0 and η meson production at mid-rapidity in proton–proton collisions at s=0.9 TeV and s=7 TeV are reported. The π0 measurement covers the ranges 0.4<pT<7 GeV/c and 0.3<pT<25 GeV/c for these two energies, respectively. The production of η mesons was measured at s=√7 TeV in the range 0.4<pT<15 GeV/c. Next-to-Leading Order perturbative QCD calculations, which are consistent with the π0 spectrum at s=0.9 TeV, overestimate those of π0 and η mesons at s=√7 TeV, but agree with the measured η/π0 ratio at s=√7 TeV.
The ALICE Collaboration has made the first measurement at the LHC of J/ψ photoproduction in ultra-peripheral Pb–Pb collisions at sNN=2.76 TeV. The J/ψ is identified via its dimuon decay in the forward rapidity region with the muon spectrometer for events where the hadronic activity is required to be minimal. The analysis is based on an event sample corresponding to an integrated luminosity of about 55 μb−1. The cross section for coherent J/ψ production in the rapidity interval −3.6<y<−2.6 is measured to be dσJ/ψcoh/dy=1.00±0.18(stat)−0.26+0.24(syst) mb. The result is compared to theoretical models for coherent J/ψ production and found to be in good agreement with those models which include nuclear gluon shadowing.