002316934 001__ 2316934 002316934 005__ 20250106052724.0 002316934 0248_ $$aoai:cds.cern.ch:2316934$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT 002316934 0247_ $$2DOI$$9arXiv$$a10.1016/j.physletb.2018.11.009$$qpublication 002316934 037__ $$9arXiv$$aarXiv:1805.04407$$chep-ex 002316934 037__ $$9arXiv:reportnumber$$aCERN-EP-2018-122 002316934 035__ $$9arXiv$$aoai:arXiv.org:1805.04407 002316934 035__ $$9Inspire$$aoai:inspirehep.net:1672788$$d2025-01-05T13:42:57Z$$h2025-01-06T03:21:31Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d 002316934 035__ $$9Inspire$$a1672788 002316934 041__ $$aeng 002316934 088__ $$9CERN-EP-DRAFT-ALICE-2018-026 002316934 100__ $$aAcharya, Shreyasi$$iINSPIRE-00570928$$uCalcutta, VECC$$vVariable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India 002316934 245__ $$aDielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} = 13$ TeV 002316934 260__ $$c2019-01-10 002316934 269__ $$aGeneva$$bCERN$$c08 May 2018 002316934 300__ $$a14 p 002316934 506__ [email protected] 002316934 506__ $$malice-member [CERN] 002316934 506__ $$mcds-ph-ep-publications-referee [CERN] 002316934 500__ $$9arXiv$$a23 pages, 5 captioned figures, 3 tables, authors from page 18, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/4291 002316934 520__ $$9Elsevier$$aThe measurement of dielectron production is presented as a function of invariant mass and transverse momentum ( pT ) at midrapidity ( |ye|<0.8 ) in proton–proton (pp) collisions at a centre-of-mass energy of s=13 TeV. The contributions from light-hadron decays are calculated from their measured cross sections in pp collisions at s=7 TeV or 13 TeV. The remaining continuum stems from correlated semileptonic decays of heavy-flavour hadrons. Fitting the data with templates from two different MC event generators, PYTHIA and POWHEG, the charm and beauty cross sections at midrapidity are extracted for the first time at this collision energy: dσcc¯/dy|y=0=974±138(stat.)±140(syst.)±214(BR)μb and dσbb¯/dy|y=0=79±14(stat.)±11(syst.)±5(BR)μb using PYTHIA simulations and dσcc¯/dy|y=0=1417±184(stat.)±204(syst.)±312(BR)μb and dσbb¯/dy|y=0=48±14(stat.)±7(syst.)±3(BR)μb for POWHEG. These values, whose uncertainties are fully correlated between the two generators, are consistent with extrapolations from lower energies. The different results obtained with POWHEG and PYTHIA imply different kinematic correlations of the heavy-quark pairs in these two generators. Furthermore, comparisons of dielectron spectra in inelastic events and in events collected with a trigger on high charged-particle multiplicities are presented in various pT intervals. The differences are consistent with the already measured scaling of light-hadron and open-charm production at high charged-particle multiplicity as a function of pT . Upper limits for the contribution of virtual direct photons are extracted at 90% confidence level and found to be in agreement with pQCD calculations. 002316934 520__ $$9arXiv$$aThe measurement of dielectron production is presented as a function of invariant mass and transverse momentum ($p_{\rm T}$) at midrapidity ($|y_{\rm e}|<0.8$) in proton-proton (pp) collisions at a centre-of-mass energy of $\sqrt{s}=13$ TeV. The contributions from light-hadron decays are calculated from their measured cross sections in pp collisions at $\sqrt{s}=7$ TeV or 13 TeV. The remaining continuum stems from correlated semileptonic decays of heavy-flavour hadrons. Fitting the data with templates from two different MC event generators, PYTHIA and POWHEG, the charm and beauty cross sections at midrapidity are extracted for the first time at this collision energy: ${\rm d}\sigma_{\rm c\bar{c}}/{\rm d}y|_{y=0}=974\pm138(\rm{stat.})\pm140(\rm{syst.})~\mu{\rm b}$ and ${\rm d}\sigma_{\rm b\bar{b}}/{\rm d}y|_{y=0}=79\pm14(\rm{stat.})\pm11(\rm{syst.})~\mu{\rm b}$ using PYTHIA simulations and ${\rm d}\sigma_{\rm c\bar{c}}/{\rm d}y|_{y=0}=1417\pm184(\rm{stat.})\pm204(\rm{syst.})~\mu{\rm b}$ and ${\rm d}\sigma_{\rm b\bar{b}}/{\rm d}y|_{y=0}=48\pm14(\rm{stat.})\pm7(\rm{syst.})~\mu{\rm b}$ for POWHEG. These values, whose uncertainties are fully correlated between the two generators, are consistent with extrapolations from lower energies. The different results obtained with POWHEG and PYTHIA imply different kinematic correlations of the heavy-quark pairs in these two generators. Furthermore, comparisons of dielectron spectra in inelastic events and in events collected with a trigger on high charged-particle multiplicities are presented in various $p_{\rm T}$ intervals. The differences are consistent with the already measured scaling of light-hadron and open-charm production at high charged-particle multiplicity as a function of $p_{\rm T}$. Upper limits for the contribution of virtual direct photons are extracted at 90% confidence level and found to be in agreement with pQCD calculations. 002316934 540__ $$3Preprint$$aCC-BY-4.0$$uhttp://creativecommons.org/licenses/by/4.0/ 002316934 540__ $$3publication$$aCC-BY-4.0$$bElsevier$$uhttp://creativecommons.org/licenses/by/4.0/ 002316934 542__ $$3Preprint$$dCERN$$g2018 002316934 542__ $$fThe Author 002316934 562__ $$cPublic comments 002316934 595__ $$aCERN EDS 002316934 65017 $$2SzGeCERN$$aParticle Physics - Experiment 002316934 65017 $$2arXiv$$anucl-ex 002316934 65017 $$2SzGeCERN$$aNuclear Physics - Experiment 002316934 65017 $$2arXiv$$ahep-ex 002316934 6531_ $$9CERN$$aQCD 002316934 6531_ $$9CERN$$aheavy quark production 002316934 6531_ $$9CERN$$alepton production 002316934 6531_ $$9CERN$$aexperimental results 002316934 693__ $$aCERN LHC$$eALICE 002316934 690C_ $$aCERN 002316934 690C_ $$aARTICLE 002316934 700__ $$aTorales - Acosta, Fernando$$iINSPIRE-00721639$$uUC, Berkeley 002316934 700__ $$aAdamova, Dagmar$$iINSPIRE-00261412$$uRez, Nucl. Phys. Inst. 002316934 700__ $$aAdolfsson, Jonatan$$iINSPIRE-00571154$$uLund U. 002316934 700__ $$aAggarwal, Madan Mohan$$iINSPIRE-00180711$$uPanjab U. 002316934 700__ $$aAglieri Rinella, Gianluca$$iINSPIRE-00249866$$jORCID:0000-0002-9611-3696$$uCERN 002316934 700__ $$aAgnello, Michelangelo$$iINSPIRE-00360901$$jORCID:0000-0002-0760-5075$$uTurin Polytechnic 002316934 700__ $$aAgrawal, Neelima$$iINSPIRE-00381545$$uIndian Inst. Tech., Mumbai 002316934 700__ $$aAhammed, Zubayer$$iINSPIRE-00180720$$uCalcutta, VECC 002316934 700__ $$aAhn, Sang Un$$iINSPIRE-00254695$$jORCID:0000-0001-8847-489X$$uKISTI, Daejeon 002316934 700__ $$aAiola, Salvatore$$iINSPIRE-00381830$$jORCID:0000-0001-6209-7627$$uYale U. 002316934 700__ $$aAkindinov, Alexander$$iINSPIRE-00061314$$jORCID:0000-0002-7388-3022$$uMoscow, ITEP 002316934 700__ $$aAl-turany, Mohammad$$iINSPIRE-00571954$$uDarmstadt, EMMI 002316934 700__ $$aAlam, Sk Noor$$iINSPIRE-00415748$$uCalcutta, VECC 002316934 700__ $$aSilva De Albuquerque, Danilo$$iINSPIRE-00560229$$uCampinas State U. 002316934 700__ $$aAleksandrov, Dmitry$$iINSPIRE-00158344$$uKurchatov Inst., Moscow 002316934 700__ $$aAlessandro, Bruno$$iINSPIRE-00250010$$jORCID:0000-0001-9680-4940$$uINFN, Turin 002316934 700__ $$aAlfaro Molina, Jose Ruben$$iINSPIRE-00249844$$uMexico U. 002316934 700__ $$aAli, Yasir$$iINSPIRE-00574063$$uCOMSATS, Islamabad 002316934 700__ $$aAlici, Andrea$$iINSPIRE-00249832$$jORCID:0000-0003-3618-4617$$uEnrico Fermi Ctr., Rome$$uBologna U.$$uINFN, Bologna 002316934 700__ $$aAlkin, Anton$$iINSPIRE-00245838$$jORCID:0000-0002-2205-5761$$uBITP, Kiev 002316934 700__ $$aAlme, Johan$$iINSPIRE-00249819$$jORCID:0000-0003-0177-0536$$uBergen U. 002316934 700__ $$aAlt, Torsten$$iINSPIRE-00249807$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aAltenkamper, Lucas$$iINSPIRE-00639902$$jORCID:0000-0002-7695-8456$$uBergen U. 002316934 700__ $$aAltsybeev, Igor$$iINSPIRE-00307325$$jORCID:0000-0002-8079-7026$$uSt. Petersburg State U. 002316934 700__ $$aAnaam, Mustafa Naji$$iINSPIRE-00655662$$uHua-Zhong Normal U. 002316934 700__ $$aAndrei, Cristian$$iINSPIRE-00249783$$jORCID:0000-0001-8535-0680$$uBucharest, IFIN-HH 002316934 700__ $$aAndreou, Dimitra$$iINSPIRE-00640214$$uCERN 002316934 700__ $$aAndrews, Harry Arthur$$iINSPIRE-00563780$$uBirmingham U. 002316934 700__ $$aAndronic, Anton$$iINSPIRE-00261430$$jORCID:0000-0002-2372-6117$$uMunster U.$$uDarmstadt, EMMI 002316934 700__ $$aAngeletti, Massimo$$iINSPIRE-00656483$$uCERN 002316934 700__ $$aAnguelov, Venelin$$iINSPIRE-00244018$$uHeidelberg U. 002316934 700__ $$aAnson, Christopher Daniel$$iINSPIRE-00240940$$jORCID:0000-0001-6244-4713$$uCreighton U. 002316934 700__ $$aAnticic, Tome$$iINSPIRE-00062373$$uBoskovic Inst., Zagreb 002316934 700__ $$aAntinori, Federico$$iINSPIRE-00175367$$jORCID:0000-0002-7366-8891$$uINFN, Padua 002316934 700__ $$aAntonioli, Pietro$$iINSPIRE-00058331$$jORCID:0000-0001-7516-3726$$uINFN, Bologna 002316934 700__ $$aAnwar, Rafay$$iINSPIRE-00563792$$uHouston U. 002316934 700__ $$aApadula, Nicole$$iINSPIRE-00287608$$uLBL, Berkeley 002316934 700__ $$aAphecetche, Laurent Bernard$$iINSPIRE-00058998$$jORCID:0000-0001-7662-3878$$uSUBATECH, Nantes 002316934 700__ $$aAppelshaeuser, Harald$$iINSPIRE-00250020$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aArcelli, Silvia$$iINSPIRE-00250042$$jORCID:0000-0001-6367-9215$$uBologna U.$$uINFN, Bologna 002316934 700__ $$aArnaldi, Roberta$$iINSPIRE-00261446$$jORCID:0000-0001-6698-9577$$uINFN, Turin 002316934 700__ $$aArnold, Oliver Werner$$iINSPIRE-00537106$$uTech. U., Munich (main)$$uMunich, Tech. U., Universe 002316934 700__ $$aArsene, Ionut Cristian$$iINSPIRE-00261457$$jORCID:0000-0003-2316-9565$$uOslo U. 002316934 700__ $$aArslandok, Mesut$$iINSPIRE-00245664$$uHeidelberg U. 002316934 700__ $$aAugustinus, Andre$$iINSPIRE-00261469$$uCERN 002316934 700__ $$aAverbeck, Ralf Peter$$iINSPIRE-00063377$$uDarmstadt, EMMI 002316934 700__ $$aAzmi, Mohd Danish$$iINSPIRE-00249731$$uAligarh Muslim U. 002316934 700__ $$aBadala, Angela$$iINSPIRE-00249728$$jORCID:0000-0002-0569-4828$$uINFN, Catania 002316934 700__ $$aBaek, Yong Wook$$iINSPIRE-00249716$$uInha U.$$uGangneung-Wonju Natl. U. 002316934 700__ $$aBagnasco, Stefano$$iINSPIRE-00028794$$jORCID:0000-0001-6062-6505$$uINFN, Turin 002316934 700__ $$aBailhache, Raphaelle Marie$$iINSPIRE-00247346$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aBala, Renu$$iINSPIRE-00261473$$jORCID:0000-0002-4116-2861$$uJammu U. 002316934 700__ $$aBaldisseri, Alberto$$iINSPIRE-00064101$$uIRFU, Saclay 002316934 700__ $$aBall, Markus$$iINSPIRE-00386117$$uBonn U., HISKP 002316934 700__ $$aBaral, Rama Chandra$$iINSPIRE-00289153$$uNISER, Jatni 002316934 700__ $$aBarbano, Anastasia Maria$$iINSPIRE-00506685$$uTurin U.$$uINFN, Turin 002316934 700__ $$aBarbera, Roberto$$iINSPIRE-00250052$$jORCID:0000-0001-5971-6415$$uCatania U.$$uINFN, Catania 002316934 700__ $$aBarile, Francesco$$iINSPIRE-00249702$$jORCID:0000-0003-2088-1290$$uINFN, Bari 002316934 700__ $$aBarioglio, Luca$$iINSPIRE-00575020$$jORCID:0000-0002-7328-9154$$uTurin U.$$uINFN, Turin 002316934 700__ $$aBarnafoldi, Gergely Gabor$$iINSPIRE-00261490$$uWigner RCP, Budapest 002316934 700__ $$aBarnby, Lee Stuart$$iINSPIRE-00064600$$jORCID:0000-0001-7357-9904$$uDaresbury 002316934 700__ $$aRamillien Barret, Valerie$$iINSPIRE-00261503$$uClermont-Ferrand U. 002316934 700__ $$aBartalini, Paolo$$iINSPIRE-00064862$$uHua-Zhong Normal U. 002316934 700__ $$aBarth, Klaus$$iINSPIRE-00522252$$uCERN 002316934 700__ $$aBartsch, Esther$$iINSPIRE-00506794$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aBastid, Nicole$$iINSPIRE-00065071$$uClermont-Ferrand U. 002316934 700__ $$aBasu, Sumit$$iINSPIRE-00360931$$uWayne State U. 002316934 700__ $$aBatigne, Guillaume$$iINSPIRE-00057450$$jORCID:0000-0001-8638-6300$$uSUBATECH, Nantes 002316934 700__ $$aBatyunya, Boris$$iINSPIRE-00180230$$uDubna, JINR 002316934 700__ $$aBatzing, Paul Christoph$$iINSPIRE-00382071$$uOslo U. 002316934 700__ $$aBazo Alba, Jose Luis$$iINSPIRE-00047770$$jORCID:0000-0001-9148-9101$$uLima, Pont. U. Catolica 002316934 700__ $$aBearden, Ian Gardner$$iINSPIRE-00261515$$jORCID:0000-0003-2784-3094$$uBohr Inst. 002316934 700__ $$aBeck, Hans$$iINSPIRE-00261523$$uHeidelberg U. 002316934 700__ $$aBedda, Cristina$$iINSPIRE-00382119$$uUtrecht U. 002316934 700__ $$aBehera, Nirbhay Kumar$$iINSPIRE-00299673$$jORCID:0000-0002-1999-9876$$uInha U. 002316934 700__ $$aBelikov, Iouri$$iINSPIRE-00250068$$uStrasbourg, IPHC 002316934 700__ $$aBellini, Francesca$$iINSPIRE-00244351$$jORCID:0000-0003-3498-4661$$uCERN 002316934 700__ $$aBello Martinez, Hector$$iINSPIRE-00506861$$jORCID:0000-0003-1315-5549$$uPuebla U., Mexico 002316934 700__ $$aBellwied, Rene$$iINSPIRE-00180735$$uHouston U. 002316934 700__ $$aEspinoza Beltran, Lucina Gabriela$$iINSPIRE-00563992$$uSinaloa U. 002316934 700__ $$aBelyaev, Vladimir$$iINSPIRE-00386131$$uMoscow Phys. Eng. Inst. 002316934 700__ $$aBencedi, Gyula$$iINSPIRE-00360943$$jORCID:0000-0002-9040-5292$$uWigner RCP, Budapest 002316934 700__ $$aBeole, Stefania$$iINSPIRE-00261543$$jORCID:0000-0003-4673-8038$$uTurin U.$$uINFN, Turin 002316934 700__ $$aBercuci, Alexandru$$iINSPIRE-00261560$$uBucharest, IFIN-HH 002316934 700__ $$aBerdnikov, Yaroslav$$iINSPIRE-00066204$$uSt. Petersburg, INP 002316934 700__ $$aBerenyi, Daniel$$iINSPIRE-00245794$$uWigner RCP, Budapest 002316934 700__ $$aBertens, Redmer Alexander$$iINSPIRE-00382235$$uTennessee U. 002316934 700__ $$aBerzano, Dario$$iINSPIRE-00245123$$jORCID:0000-0003-4390-9321$$uCERN$$uINFN, Turin 002316934 700__ $$aBetev, Latchezar$$iINSPIRE-00250085$$uCERN 002316934 700__ $$aBhaduri, Partha Pratim$$iINSPIRE-00574074$$uCalcutta, VECC 002316934 700__ $$aBhasin, Anju$$iINSPIRE-00180740$$jORCID:0000-0002-3687-8179$$uJammu U. 002316934 700__ $$aBhat, Inayat Rasool$$iINSPIRE-00415990$$uJammu U. 002316934 700__ $$aBhatt, Himani$$iINSPIRE-00585216$$uIndian Inst. Tech., Mumbai 002316934 700__ $$aBhattacharjee, Buddhadeb$$iINSPIRE-00385476$$jORCID:0000-0002-3755-0992$$uGauhati U. 002316934 700__ $$aBhom, Jihyun$$iINSPIRE-00287624$$uCracow, INP 002316934 700__ $$aBianchi, Antonio$$iINSPIRE-00584065$$jORCID:0000-0003-0343-7497$$uTurin U.$$uINFN, Turin 002316934 700__ $$aBianchi, Livio$$iINSPIRE-00254651$$jORCID:0000-0003-1664-8189$$uHouston U. 002316934 700__ $$aBianchi, Nicola$$iINSPIRE-00139110$$jORCID:0000-0001-6861-2810$$uFrascati 002316934 700__ $$aBielcik, Jaroslav$$iINSPIRE-00180768$$uPrague, Tech. U. 002316934 700__ $$aBielcikova, Jana$$iINSPIRE-00180776$$jORCID:0000-0003-1659-0394$$uRez, Nucl. Phys. Inst. 002316934 700__ $$aBilandzic, Ante$$iINSPIRE-00261580$$jORCID:0000-0003-0002-4654$$uMunich, Tech. U., Universe$$uTech. U., Munich (main) 002316934 700__ $$aBiro, Gabor$$iINSPIRE-00548333$$uWigner RCP, Budapest 002316934 700__ $$aBiswas, Rathijit$$iINSPIRE-00522421$$uBose Inst., Kolkata$$uCAPSS, Kolkata 002316934 700__ $$aBiswas, Saikat$$iINSPIRE-00525263$$jORCID:0000-0003-3578-5373$$uBose Inst., Kolkata$$uCAPSS, Kolkata 002316934 700__ $$aBlair, Justin Thomas$$iINSPIRE-00531266$$jORCID:0000-0002-4681-3002$$uTexas U. 002316934 700__ $$aBlau, Dmitry$$iINSPIRE-00247320$$jORCID:0000-0002-4266-8338$$uKurchatov Inst., Moscow 002316934 700__ $$aBlume, Christoph$$iINSPIRE-00067666$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aBoca, Gianluigi$$iINSPIRE-00067697$$jORCID:0000-0002-2829-5950$$uPavia U., Dept. Fis. 'A. Volta' 002316934 700__ $$aBock, Friederike$$iINSPIRE-00246175$$jORCID:0000-0003-4185-2093$$uCERN 002316934 700__ $$aBogdanov, Alexey$$iINSPIRE-00261637$$uMoscow Phys. Eng. Inst. 002316934 700__ $$aBoldizsar, Laszlo$$iINSPIRE-00307799$$uWigner RCP, Budapest 002316934 700__ $$aBombara, Marek$$iINSPIRE-00261642$$jORCID:0000-0001-7333-224X$$uKosice U. 002316934 700__ $$aBonomi, Germano$$iINSPIRE-00068097$$jORCID:0000-0003-1618-9648$$uU. Brescia 002316934 700__ $$aBonora, Matthias$$iINSPIRE-00563828$$uCERN 002316934 700__ $$aBorel, Herve$$iINSPIRE-00068253$$uIRFU, Saclay 002316934 700__ $$aBorissov, Alexander$$iINSPIRE-00254729$$uMunster U. 002316934 700__ $$aBorri, Marcello$$iINSPIRE-00286268$$uLiverpool U. 002316934 700__ $$aBotta, Elena$$iINSPIRE-00250108$$jORCID:0000-0002-5054-1521$$uTurin U.$$uINFN, Turin 002316934 700__ $$aBourjau, Christian$$iINSPIRE-00537054$$jORCID:0000-0001-6745-5139$$uBohr Inst. 002316934 700__ $$aBratrud, Lars$$iINSPIRE-00246212$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aBraun-munzinger, Peter$$iINSPIRE-00069060$$jORCID:0000-0003-2527-0720$$uDarmstadt, EMMI 002316934 700__ $$aBregant, Marco$$iINSPIRE-00261672$$uSao Paulo U. 002316934 700__ $$aBroker, Theo Alexander$$iINSPIRE-00382350$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aBroz, Michal$$iINSPIRE-00246094$$uPrague, Tech. U. 002316934 700__ $$aBrucken, Erik Jens$$iINSPIRE-00019412$$jORCID:0000-0001-5926-3516$$uHelsinki Inst. of Phys. 002316934 700__ $$aBruna, Elena$$iINSPIRE-00181319$$jORCID:0000-0001-5427-1461$$uINFN, Turin 002316934 700__ $$aBruno, Giuseppe Eugenio$$iINSPIRE-00314938$$jORCID:0000-0001-6247-9633$$uCERN$$uBari U.$$uINFN, Bari 002316934 700__ $$aBudnikov, Dmitry$$iINSPIRE-00249577$$uRFNC-VNIIEF, Sarov 002316934 700__ $$aBuesching, Henner$$iINSPIRE-00241182$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aBufalino, Stefania$$iINSPIRE-00289290$$jORCID:0000-0002-0413-9478$$uTurin Polytechnic 002316934 700__ $$aBuhler, Paul$$iINSPIRE-00563836$$uStefan Meyer Inst. Subatomare Phys. 002316934 700__ $$aBuncic, Predrag$$iINSPIRE-00178263$$uCERN 002316934 700__ $$aBusch, Oliver$$iINSPIRE-00261698$$uTsukuba U. 002316934 700__ $$aButhelezi, Edith Zinhle$$iINSPIRE-00261702$$jORCID:0000-0002-8880-1608$$uiThemba LABS 002316934 700__ $$aBashir Butt, Jamila$$iINSPIRE-00040297$$uCOMSATS, Islamabad 002316934 700__ $$aBuxton, Jesse Thomas$$iINSPIRE-00507048$$uOhio State U. 002316934 700__ $$aCabala, Jan$$iINSPIRE-00560262$$uKosice Tech. U. 002316934 700__ $$aCaffarri, Davide$$iINSPIRE-00249565$$uNikhef, Amsterdam 002316934 700__ $$aCaines, Helen Louise$$iINSPIRE-00177317$$uYale U. 002316934 700__ $$aCaliva, Alberto$$iINSPIRE-00382423$$jORCID:0000-0002-2543-0336$$uDarmstadt, EMMI 002316934 700__ $$aCalvo Villar, Ernesto$$iINSPIRE-00248154$$uLima, Pont. U. Catolica 002316934 700__ $$aSoto Camacho, Rabi$$iINSPIRE-00644124$$uPuebla U., Mexico 002316934 700__ $$aCamerini, Paolo$$iINSPIRE-00070739$$jORCID:0000-0002-9261-9497$$uTrieste U.$$uINFN, Trieste 002316934 700__ $$aCapon, Aaron Allan$$iINSPIRE-00563959$$uStefan Meyer Inst. 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U., Munich (main)$$uMunich, Tech. 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Appl. Sci. 002316934 700__ $$aHamar, Gergoe$$iINSPIRE-00262460$$jORCID:0000-0002-2268-7830$$uWigner RCP, Budapest 002316934 700__ $$aHamid, Mohammed$$iINSPIRE-00655672$$uHua-Zhong Normal U. 002316934 700__ $$aHamon, Julien Charles$$iINSPIRE-00548368$$jORCID:0000-0003-1134-8507$$uStrasbourg, IPHC 002316934 700__ $$aHannigan, Ryan$$iINSPIRE-00653583$$jORCID:0000-0003-4518-3528$$uTexas U. 002316934 700__ $$aHaque, Md Rihan$$iINSPIRE-00539842$$uUtrecht U. 002316934 700__ $$aHarlenderova, Alena$$iINSPIRE-00649693$$uDarmstadt, EMMI 002316934 700__ $$aHarris, John William$$iINSPIRE-00301628$$jORCID:0000-0002-8535-3061$$uYale U. 002316934 700__ $$aHarton, Austin Vincent$$iINSPIRE-00245718$$uChicago State U. 002316934 700__ $$aHassan, Hadi$$iINSPIRE-00572743$$uLPSC, Grenoble 002316934 700__ $$aHatzifotiadou, Despina$$iINSPIRE-00244493$$jORCID:0000-0002-7638-2047$$uINFN, Bologna$$uEnrico Fermi Ctr., Rome 002316934 700__ $$aHayashi, Shinichi$$iINSPIRE-00361149$$uTokyo U. 002316934 700__ $$aHeckel, Stefan Thomas$$iINSPIRE-00245584$$jORCID:0000-0002-9083-4484$$uFrankfurt U., Inst. 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Tech., Mumbai 002316934 700__ $$aNania, Rosario$$iINSPIRE-00172055$$jORCID:0000-0002-6039-190X$$uINFN, Bologna$$uEnrico Fermi Ctr., Rome 002316934 700__ $$aNappi, Eugenio$$iINSPIRE-00110416$$jORCID:0000-0003-2080-9010$$uINFN, Bari 002316934 700__ $$aNarayan, Amrendra$$iINSPIRE-00470117$$jORCID:0000-0003-3814-9559$$uIndian Inst. Tech., Mumbai 002316934 700__ $$aNaru, Muhammad Umair$$iINSPIRE-00507883$$jORCID:0000-0001-6489-0784$$uCOMSATS, Islamabad 002316934 700__ $$aNassirpour, Adrian Fereydon$$iINSPIRE-00664110$$uLund U. 002316934 700__ $$aFerreira Natal Da Luz, Pedro Hugo$$iINSPIRE-00511516$$uSao Paulo U. 002316934 700__ $$aNattrass, Christine$$iINSPIRE-00301613$$jORCID:0000-0002-8768-6468$$uTennessee U. 002316934 700__ $$aRosado Navarro, Sebastian$$iINSPIRE-00548422$$uPuebla U., Mexico 002316934 700__ $$aNayak, Kishora$$iINSPIRE-00416777$$uNISER, Jatni 002316934 700__ $$aNayak, Ranjit$$iINSPIRE-00548439$$jORCID:0000-0001-6988-0606$$uIndian Inst. 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Tech., Indore 002316934 700__ $$aThakur, Sanchari$$iINSPIRE-00568433$$uCalcutta, VECC 002316934 700__ $$aThomas, Deepa$$iINSPIRE-00290473$$jORCID:0000-0003-3408-3097$$uTexas U. 002316934 700__ $$aThoresen, Freja$$iINSPIRE-00578196$$uBohr Inst. 002316934 700__ $$aTieulent, Raphael Noel$$iINSPIRE-00244918$$jORCID:0000-0002-2106-5415$$uLyon, IPN 002316934 700__ $$aTikhonov, Anatoly$$iINSPIRE-00560412$$uMoscow, INR 002316934 700__ $$aTimmins, Anthony Robert$$iINSPIRE-00183330$$uHouston U. 002316934 700__ $$aToia, Alberica$$iINSPIRE-00020233$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aTopilskaya, Nataliya$$iINSPIRE-00585230$$uMoscow, INR 002316934 700__ $$aToppi, Marco$$iINSPIRE-00575047$$uFrascati 002316934 700__ $$aRojas Torres, Solangel$$iINSPIRE-00648200$$uSinaloa U. 002316934 700__ $$aTripathy, Sushanta$$iINSPIRE-00564720$$jORCID:0000-0002-0061-5107$$uIndian Inst. 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Subatomare Phys. 002316934 700__ $$aWeber, Steffen Georg$$iINSPIRE-00510469$$uDarmstadt, EMMI 002316934 700__ $$aWegrzynek, Adam$$iINSPIRE-00572414$$jORCID:0000-0002-3155-0887$$uCERN 002316934 700__ $$aWeiser, Dennis Franz$$iINSPIRE-00537176$$uHeidelberg U. 002316934 700__ $$aWenzel, Sandro Christian$$iINSPIRE-00287872$$uCERN 002316934 700__ $$aWessels, Johannes Peter$$iINSPIRE-00178848$$jORCID:0000-0003-1339-286X$$uMunster U. 002316934 700__ $$aWesterhoff, Uwe$$iINSPIRE-00246123$$uMunster U. 002316934 700__ $$aWhitehead, Andile Mothegi$$iINSPIRE-00537181$$uCape Town U. 002316934 700__ $$aWiechula, Jens$$iINSPIRE-00290727$$uFrankfurt U., Inst. Kernphys. 002316934 700__ $$aWikne, Jon$$iINSPIRE-00250749$$uOslo U. 002316934 700__ $$aWilk, Grzegorz Andrzej$$iINSPIRE-00135952$$uWarsaw, Inst. Nucl. 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U. 002316934 700__ $$aYoon, Jin Hee$$iINSPIRE-00537195$$uInha U. 002316934 700__ $$aYurchenko, Volodymyr$$iINSPIRE-00510512$$uBITP, Kiev 002316934 700__ $$aZaccolo, Valentina$$iINSPIRE-00361691$$jORCID:0000-0002-6499-752X$$uINFN, Turin 002316934 700__ $$aZaman, Ali$$iINSPIRE-00385199$$uCOMSATS, Islamabad 002316934 700__ $$aZampolli, Chiara$$iINSPIRE-00247387$$jORCID:0000-0002-2608-4834$$uCERN 002316934 700__ $$aCorrea Zanoli, Henrique Jose$$iINSPIRE-00510636$$uSao Paulo U. 002316934 700__ $$aZardoshti, Nima$$iINSPIRE-00522360$$uBirmingham U. 002316934 700__ $$aZarochentsev, Andrey$$iINSPIRE-00246638$$jORCID:0000-0002-3502-8084$$uSt. Petersburg State U. 002316934 700__ $$aZavada, Petr$$iINSPIRE-00138107$$uPrague, Inst. Phys. 002316934 700__ $$aZavyalov, Nikolay$$iINSPIRE-00290800$$uRFNC-VNIIEF, Sarov 002316934 700__ $$aZbroszczyk, Hanna Paulina$$iINSPIRE-00183708$$uWarsaw U. of Tech. 002316934 700__ $$aZhalov, Mikhail$$iINSPIRE-00254612$$uSt. Petersburg, INP 002316934 700__ $$aZhang, Xiaoming$$iINSPIRE-00290818$$uHua-Zhong Normal U. 002316934 700__ $$aZhang, Yonghong$$iINSPIRE-00385253$$uHua-Zhong Normal U. 002316934 700__ $$aZhang, Zuman$$iINSPIRE-00531444$$uHua-Zhong Normal U.$$uClermont-Ferrand U. 002316934 700__ $$aZhao, Chengxin$$iINSPIRE-00385310$$uOslo U. 002316934 700__ $$aZherebchevskii, Vladimir$$iINSPIRE-00639969$$uSt. Petersburg State U. 002316934 700__ $$aZhigareva, Natalia$$iINSPIRE-00385354$$uMoscow, ITEP 002316934 700__ $$aZhou, Daicui$$iINSPIRE-00290834$$uHua-Zhong Normal U. 002316934 700__ $$aZhou, You$$iINSPIRE-00290856$$jORCID:0000-0002-7868-6706$$uBohr Inst. 002316934 700__ $$aZhou, Zhuo$$iINSPIRE-00417116$$uBergen U. 002316934 700__ $$aZhu, Hongsheng$$iINSPIRE-00361728$$uHua-Zhong Normal U. 002316934 700__ $$aZhu, Jianhui$$iINSPIRE-00361715$$uHua-Zhong Normal U. 002316934 700__ $$aZhu, Ya$$iINSPIRE-00651777$$uHua-Zhong Normal U. 002316934 700__ $$aZichichi, Antonino$$iINSPIRE-00172134$$uBologna U.$$uINFN, Bologna$$uEnrico Fermi Ctr., Rome 002316934 700__ $$aZimmermann, Markus Bernhard$$iINSPIRE-00385420$$uCERN 002316934 700__ $$aZinovjev, Gennady$$iINSPIRE-00290880$$uBITP, Kiev 002316934 700__ $$aZmeskal, Johann$$iINSPIRE-00564793$$uStefan Meyer Inst. Subatomare Phys. 002316934 700__ $$aZou, Shuguang$$iINSPIRE-00571982$$uHua-Zhong Normal U. 002316934 710__ $$5PH 002316934 710__ $$gALICE Collaboration 002316934 773__ $$c505-518$$pPhys. Lett. B$$v788$$y2019 002316934 859__ [email protected] 002316934 8564_ $$81402120$$s695404$$uhttp://cds.cern.ch/record/2316934/files/CERN-EP-DRAFT-ALICE-2018-026 - draft.pdf$$yDraft (restricted)$$zStamped by WebSubmit: 09/05/2018 002316934 8564_ $$82213960$$s48627$$uhttp://cds.cern.ch/record/2316934/files/ULS_B_S_nocut_mb.png$$y00007 Opposite-sign spectrum $N_{+-}$, the combinatorial background $B$ and the signal $S$ in minimum-bias (left) and high-multiplicity (right) events. Only statistical uncertainties are shown. 002316934 8564_ $$82213961$$s50908$$uhttp://cds.cern.ch/record/2316934/files/FigHFmass.png$$y00010 Projection of the heavy-flavour dielectron fit (grey line) in inelastic \pp collisions at $\sqrts = 13\TeV$ onto the dielectron mass (left) and \ptee (right) using the \PYTHIA and \POWHEG event generators. The lines show the charm (red) and beauty (magenta) contributions after the fit. The global scale uncertainty on the \pp luminosity (5\%) is not shown. The statistical and systematic uncertainties of the data are shown as vertical bars and boxes. The fits with \PYTHIA and \POWHEG result in a $\chi^2/{\rm ndf}$ of $57.8/66$ and $52.6/66$, respectively. 002316934 8564_ $$82213962$$s48065$$uhttp://cds.cern.ch/record/2316934/files/ULS_B_S_nocut_hm.png$$y00004 Opposite-sign spectrum $N_{+-}$, the combinatorial background $B$ and the signal $S$ in minimum-bias (left) and high-multiplicity (right) events. Only statistical uncertainties are shown. 002316934 8564_ $$82213963$$s949473$$uhttp://cds.cern.ch/record/2316934/files/1805.04407.pdf$$yFulltext 002316934 8564_ $$82213964$$s75444$$uhttp://cds.cern.ch/record/2316934/files/Signal_cocktail_pt0_pythia.png$$y00008 The dielectron cross section in inelastic \pp collisions at $\sqrts = 13\TeV$ as a function of invariant mass (left) and of pair transverse momentum in different mass intervals (right). The global scale uncertainty on the \pp luminosity (5\%) is not shown. The statistical and systematic uncertainties of the data are shown as vertical bars and boxes. The expectation from the hadronic decay cocktail is shown as a band, and the bottom left plot shows the ratio data to cocktail together with the cocktail uncertainty. 002316934 8564_ $$82213965$$s1233804$$uhttp://cds.cern.ch/record/2316934/files/scoap3-fulltext.pdf$$yArticle from SCOAP3 002316934 8564_ $$82213966$$s31344$$uhttp://cds.cern.ch/record/2316934/files/Ratio_ptbin4.png$$y00005 Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity in different \ptee intervals. The statistical and systematic uncertainties of the data are shown as vertical bars and boxes. The expectation from the hadronic decay cocktail calculation is shown as a grey band. 002316934 8564_ $$82213967$$s55526$$uhttp://cds.cern.ch/record/2316934/files/Signal_cocktail_pteespectra.png$$y00001 The dielectron cross section in inelastic \pp collisions at $\sqrts = 13\TeV$ as a function of invariant mass (left) and of pair transverse momentum in different mass intervals (right). The global scale uncertainty on the \pp luminosity (5\%) is not shown. The statistical and systematic uncertainties of the data are shown as vertical bars and boxes. The expectation from the hadronic decay cocktail is shown as a band, and the bottom left plot shows the ratio data to cocktail together with the cocktail uncertainty. 002316934 8564_ $$82213968$$s47867$$uhttp://cds.cern.ch/record/2316934/files/FigHFpt.png$$y00009 Projection of the heavy-flavour dielectron fit (grey line) in inelastic \pp collisions at $\sqrts = 13\TeV$ onto the dielectron mass (left) and \ptee (right) using the \PYTHIA and \POWHEG event generators. The lines show the charm (red) and beauty (magenta) contributions after the fit. The global scale uncertainty on the \pp luminosity (5\%) is not shown. The statistical and systematic uncertainties of the data are shown as vertical bars and boxes. The fits with \PYTHIA and \POWHEG result in a $\chi^2/{\rm ndf}$ of $57.8/66$ and $52.6/66$, respectively. 002316934 8564_ $$82213969$$s29948$$uhttp://cds.cern.ch/record/2316934/files/Ratio_ptbin1.png$$y00002 Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity in different \ptee intervals. The statistical and systematic uncertainties of the data are shown as vertical bars and boxes. The expectation from the hadronic decay cocktail calculation is shown as a grey band. 002316934 8564_ $$82213970$$s34091$$uhttp://cds.cern.ch/record/2316934/files/Ratio_ptbin0.png$$y00003 Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity. The statistical and systematic uncertainties of the data are shown as vertical bars and boxes. The expectation from the hadronic decay cocktail calculation is shown as a grey band. 002316934 8564_ $$82213971$$s31539$$uhttp://cds.cern.ch/record/2316934/files/Ratio_ptbin3.png$$y00000 Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity in different \ptee intervals. The statistical and systematic uncertainties of the data are shown as vertical bars and boxes. The expectation from the hadronic decay cocktail calculation is shown as a grey band. 002316934 8564_ $$82213972$$s31798$$uhttp://cds.cern.ch/record/2316934/files/Ratio_ptbin2.png$$y00006 Ratio of dielectron spectra in HM and INEL events scaled by the charged-particle multiplicity in different \ptee intervals. The statistical and systematic uncertainties of the data are shown as vertical bars and boxes. The expectation from the hadronic decay cocktail calculation is shown as a grey band. 002316934 9031_ $$aApproval requested for number CERN-EP-2018-122$$bCERN-EP-2018-122$$cEPPHAPP$$d2018-05-08 15:03:36$$e2018-05-15 15:03:[email protected]$$swaiting 002316934 9031_ $$aDocument approved$$bCERN-EP-2018-122$$cEPPHAPP$$d2018-05-09 17:19:[email protected]$$sapproved 002316934 916__ $$sn$$w201819 002316934 960__ $$a13 002316934 980__ $$aALICE_Papers 002316934 980__ $$aARTICLE