002899115 001__ 2899115
002899115 005__ 20241202040648.0
002899115 0248_ $$aoai:cds.cern.ch:2899115$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002899115 037__ $$9arXiv$$aarXiv:2405.19069$$chep-ex
002899115 035__ $$9arXiv$$aoai:arXiv.org:2405.19069
002899115 035__ $$9Inspire$$aoai:inspirehep.net:2791203$$d2024-12-01T19:03:07Z$$h2024-12-02T03:00:10Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002899115 035__ $$9Inspire$$a2791203
002899115 041__ $$aeng
002899115 100__ $$aKhatun, Anisa$$uU. Kansas, Lawrence$$vDepartment of Physics and Astronomy, The University of Kansas. Lawrence, Kansas, 66045 USA
002899115 245__ $$9arXiv$$aUPC physics with ALICE in Run 3
002899115 269__ $$c2024-05-29
002899115 300__ $$a8 p
002899115 500__ $$9arXiv$$a8 pages, 10 figures, UPC 2023: Proceedings of the International
Workshop on the Physics of Ultra Peripheral Collisions, 10-15 December, 2023
002899115 520__ $$9arXiv$$aThe ALICE experiment has undergone a major detector upgrade for Run 3, expanding its detection capabilities for a wide variety of studies. The new continuous readout has significantly enhanced the physics potential for ultra-peripheral collision analyses. In this talk, we discussed some of the physics analyses that can be carried out in ultra-peripheral collisions using the Run 3 data and presented some of the first physics performance plots in both proton-proton and heavy-ion collisions.
002899115 540__ $$3preprint$$aCC BY 4.0$$uhttp://creativecommons.org/licenses/by/4.0/
002899115 65017 $$2arXiv$$anucl-ex
002899115 65017 $$2SzGeCERN$$aNuclear Physics - Experiment
002899115 65017 $$2arXiv$$ahep-ex
002899115 65017 $$2SzGeCERN$$aParticle Physics - Experiment
002899115 690C_ $$aCERN
002899115 690C_ $$aPREPRINT
002899115 693__ $$aCERN LHC$$eALICE
002899115 710__ $$gALICE Collaboration
002899115 773__ $$wC23-12-11.2
002899115 8564_ $$82533022$$s37044$$uhttp://cds.cern.ch/record/2899115/files/Schematic-diagram-for-the-production-of-vector-mesons-in-UPCs.png$$y00000 Typical exclusive vector meson production in UPC (left). The photon can also break up the target (right).
002899115 8564_ $$82533023$$s574065$$uhttp://cds.cern.ch/record/2899115/files/Run2.png$$y00005 UPC event in Run 2 at forward rapidity (left) and UPC event in Run 3 at midrapidity (right).
002899115 8564_ $$82533024$$s80822$$uhttp://cds.cern.ch/record/2899115/files/Inclusive_upc.png$$y00001 Typical exclusive vector meson production in UPC (left). The photon can also break up the target (right).
002899115 8564_ $$82533025$$s290283$$uhttp://cds.cern.ch/record/2899115/files/jpgacc419f6_hr.png$$y00010 Projection of ALICE Run 3 with Focal acceptance in Run 4 ratio of energy dependence: Exclusive $\psi(2S)$ to J/$\psi$ photoproduction cross section (left) and dissociative J/$\psi$ to exclusive J/$\psi$ photoproduction cross sections (right).
002899115 8564_ $$82533026$$s378391$$uhttp://cds.cern.ch/record/2899115/files/invkaonpion.png$$y00016 Raw invariant mass distributions of two pions and two kaons candidates of CEP events in pp collisions.
002899115 8564_ $$82533027$$s176485$$uhttp://cds.cern.ch/record/2899115/files/2020-02-26-SodingALICE.png$$y00004 a) Run 1 : $\sim$ 7k events \cite{rhorun1}. b) Run 2 : $\sim$ 60k events \cite{rhorun2}.
002899115 8564_ $$82533028$$s8552$$uhttp://cds.cern.ch/record/2899115/files/dataflow.png$$y00002 Schematic view of data-taking procedure.
002899115 8564_ $$82533029$$s67698$$uhttp://cds.cern.ch/record/2899115/files/Lightbylight_alicecut.png$$y00012 The light-by-light scattering process (left) and contributions from resonances decays into two photons as a function of the invariant mass (right)~\cite{lyltheory}.
002899115 8564_ $$82533030$$s12522$$uhttp://cds.cern.ch/record/2899115/files/pt_fwd_0.png$$y00008 Coherent $\rho^{0}$ invariant mass distribution (left) and \pt \ distribution of exclusive J/$\psi$ (right).
002899115 8564_ $$82533031$$s37457$$uhttp://cds.cern.ch/record/2899115/files/ATLASlimit.png$$y00013 The value of $a_{\tau}$ measured by ATLAS (left) and ALICE simulation with Run 3 acceptance for $a_{\tau}$ (right)~\cite{taoAtlas}.
002899115 8564_ $$82533032$$s269252$$uhttp://cds.cern.ch/record/2899115/files/CEPevents.png$$y00015 Schematic diagram of various CEP events.
002899115 8564_ $$82533033$$s169734$$uhttp://cds.cern.ch/record/2899115/files/2015-Apr-09-minv.png$$y00003 a) Run 1 : $\sim$ 7k events \cite{rhorun1}. b) Run 2 : $\sim$ 60k events \cite{rhorun2}.
002899115 8564_ $$82533034$$s64765$$uhttp://cds.cern.ch/record/2899115/files/LbL_chargedparticles.png$$y00011 The light-by-light scattering process (left) and contributions from resonances decays into two photons as a function of the invariant mass (right)~\cite{lyltheory}.
002899115 8564_ $$82533035$$s4140716$$uhttp://cds.cern.ch/record/2899115/files/2405.19069.pdf$$yFulltext
002899115 8564_ $$82533036$$s196503$$uhttp://cds.cern.ch/record/2899115/files/jpgacc419f5_hr.png$$y00009 Projection of ALICE Run 3 with Focal acceptance in Run 4 ratio of energy dependence: Exclusive $\psi(2S)$ to J/$\psi$ photoproduction cross section (left) and dissociative J/$\psi$ to exclusive J/$\psi$ photoproduction cross sections (right).
002899115 8564_ $$82533037$$s91539$$uhttp://cds.cern.ch/record/2899115/files/limits_comb_0.png$$y00014 The value of $a_{\tau}$ measured by ATLAS (left) and ALICE simulation with Run 3 acceptance for $a_{\tau}$ (right)~\cite{taoAtlas}.
002899115 8564_ $$82533038$$s34363$$uhttp://cds.cern.ch/record/2899115/files/rho0_invariantmass_0.png$$y00007 Coherent $\rho^{0}$ invariant mass distribution (left) and \pt \ distribution of exclusive J/$\psi$ (right).
002899115 8564_ $$82533039$$s1134724$$uhttp://cds.cern.ch/record/2899115/files/ALICERun3dimuon.png$$y00006 UPC event in Run 2 at forward rapidity (left) and UPC event in Run 3 at midrapidity (right).
002899115 960__ $$a11
002899115 962__ $$b2897266$$k$$nplaya del carmen20231211
002899115 980__ $$aConferencePaper
002899115 980__ $$aPREPRINT