Results 21 to 30 of about 1,450 (210)

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrt{s} $$ , s NN $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV

open access: yesJournal of High Energy Physics, 2021
Jet fragmentation transverse momentum (j T) distributions are measured in proton-proton (pp) and proton-lead (p-Pb) collisions at s NN $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV with the ALICE experiment at the LHC.
The ALICE collaboration   +1004 more
doaj   +1 more source

Low-Distortion Long Variable Delay of Linear Frequency Modulated Waveforms

open access: yesIEEE Photonics Journal, 2012
The impulse response of 500-MHz-wide, linear frequency modulated (LFM) waveforms is delayed and advanced by 50 ns using microwave-photonic processing.
Yonatan Stern   +5 more
doaj   +1 more source

J/ψ production as a function of charged-particle multiplicity in p-Pb collisions at s NN $$ \sqrt{s_{\mathrm{NN}}} $$ = 8.16 TeV

open access: yesJournal of High Energy Physics, 2020
Inclusive J/ψ yields and average transverse momenta in p-Pb collisions at a center-of-mass energy per nucleon pair s NN $$ \sqrt{s_{\mathrm{NN}}} $$ = 8.16 TeV are measured as a function of the charged-particle pseudorapidity density with ALICE.
The ALICE collaboration   +1010 more
doaj   +1 more source

Measurement of inclusive charged-particle b-jet production in pp and p-Pb collisions at s NN $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV

open access: yesJournal of High Energy Physics, 2022
A measurement of the inclusive b-jet production cross section is presented in pp and p-Pb collisions at s NN $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV, using data collected with the ALICE detector at the LHC.
The ALICE collaboration   +1013 more
doaj   +1 more source

Water Transport - The Challenge for the Automotive Industry in Slovakia

open access: yesCommunications, 2016
An important factor in choosing the transport mode in the automotive industry is not only the current price but also the shipping time. In some cases the latter one is even crucial and significantly affects the choice of the transport mode.
Tomas Kalina   +3 more
doaj   +1 more source

Die Zukunft der Telekommunikation [PDF]

open access: yesWIRTSCHAFTSINFORMATIK, 2011
Die Telekommunikationsindustrie unterliegt seit zwei Dekaden in besonderem Mase einer Veranderung, hervorgerufen durch den Durchbruch der Architektur des Internets als Kommunikationsinfrastruktur und als Massenmedium sowie durch neue Generationen des Mobilfunks. Diese Dynamik wird sich fortsetzen: Neue Netztechnologien (z. B.
Udo Bub, Arnold Picot, Helmut Krcmar
openaire   +1 more source

Production of $${\pi ^0}$$ π 0 and $$\eta $$ η mesons up to high transverse momentum in pp collisions at 2.76 TeV

open access: yesEuropean Physical Journal C: Particles and Fields, 2017
The invariant differential cross sections for inclusive $$\pi ^{0}$$ π 0 and $$\eta $$ η mesons at midrapidity were measured in pp collisions at $$\sqrt{s}=2.76$$ s = 2.76  TeV for transverse momenta $$0 ...
S. Acharya   +1029 more
doaj   +1 more source

Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N = 2.76 $$ \sqrt{{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV

open access: yesJournal of High Energy Physics, 2017
This is an addendum to the article JHEP 11 (2015) 205 [1]. The figures 3 (right), 4 (right) and 5 are updated with published results on non-prompt J/ψ-meson production from the CMS collaboration [2].
The ALICE collaboration   +985 more
doaj   +1 more source

Constraining the Chiral Magnetic Effect with charge-dependent azimuthal correlations in Pb-Pb collisions at s NN $$ \sqrt{s_{\mathrm{NN}}} $$ = 2.76 and 5.02 TeV

open access: yesJournal of High Energy Physics, 2020
Systematic studies of charge-dependent two- and three-particle correlations in Pb-Pb collisions at s NN $$ \sqrt{s_{\mathrm{NN}}} $$ = 2.76 and 5.02 TeV used to probe the Chiral Magnetic Effect (CME) are presented.
The ALICE collaboration   +1013 more
doaj   +1 more source

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