Đorđević, Miloš

Link to this page

Authority KeyName Variants
orcid::0000-0002-8407-3236
  • Đorđević, Miloš (868)
Projects
BMWF (Austria), FWF (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MEYS (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), MoER (Estonia) [SF0690030s09], ERDF (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Republic of Korea), WCU (Republic of Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), MSI (New Zealand), PAEC (Pakistan), MSHE (Poland), NSC (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MON (Russia), RosAtom (Russia), RAS (Russia), RFBR (Russia), MSTD (Serbia), SEIDI (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), ThEPCenter (Thailand), IPST (Thailand), NSTDA (Thailand), TUBITAK (Turkey), TAEK (Turkey), NASU (Ukraine), STFC (United Kingdom), DOE (USA), NSF (USA) FMSR (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), Academy of Sciences (Estonia), NICPB (Estonia), Academy of Finland, ME (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Korea), WCU (Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), PAEC (Pakistan), SCSR (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MST (Russia), MAE (Russia), MSTD (Serbia), MICINN (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK (Turkey), TAEK (Turkey), STFC (United Kingdom), DOE (USA), NSF (USA)
FMSR (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN (China), CAS (China), MoST (China), NSFC (China), COLCIEN-CIAS (Colombia), MSES (Croatia), RPF (Cyprus), Academy of Sciences (Estonia), NICPB (Estonia), Academy of Finland, ME (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), PAEC (Pakistan), SCSR (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MST (Russia), MAE (Russia), MSTDS (Serbia), MICINN (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK (Turkey), TAEK (Turkey), STFC (United Kingdom), DOE (USA), NSF (USA), European Union, Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation Ministry of Education, Science and Technological Development, Republic of Serbia, Grant no. 451-03-68/2020-14/200017 (University of Belgrade, Institute of Nuclear Sciences 'Vinča', Belgrade-Vinča)
BMWFW (Austria), FWF (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), CSF (Croatia), RPF (Cyprus), MoER (Estonia), ERC IUT (Estonia), ERDF (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NIH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), MSIP (Republic of Korea), NRF (Republic of Korea), LAS (Lithuania), MOE (Malaysia), UM (Malaysia), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), MBIE (New Zealand), PAEC (Pakistan), MSHE (Poland), NSC (Poland), FCT (Portugal), JINR (Dubna), MON (Russia), RosAtom (Russia), RAS (Russia), RFBR (Russia), MESTD (Serbia), SEIDI (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), MST (Taipei), ThEPCenter (Thailand), IPST (Thailand), STAR (Thailand), NSTDA (Thailand), TUBITAK (Turkey), TAEK (Turkey), NASU (Ukraine), SFFR (Ukraine), STFC (United Kingdom), DOE (USA), NSF (USA) BMWFW (Austria), FWF (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), CSF (Croatia), RPF (Cyprus), MoER (Estonia), ERC IUT (Estonia), ERDF (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NIH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Republic of Korea), WCU (Republic of Korea), LAS (Lithuania), MOE (Malaysia), UM (Malaysia), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), MBIE (New Zealand), PAEC (Pakistan), MSHE (Poland), NSC (Poland), FCT (Portugal), JINR (Dubna), MON (Russia), RosAtom (Russia), RAS (Russia), RFBR (Russia), MESTD (Serbia), SEIDI (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), MST (Taipei), ThEPCenter (Thailand), IPST (Thailand), STAR (Thailand), NSTDA (Thailand), TUBITAK (Turkey), TAEK (Turkey), NASU (Ukraine), SFFR (Ukraine), STFC (United Kingdom), DOE (USA), NSF (USA)
FMSR (Austria), FNRS, FWO (Belgium), CNPq, CAPES, FAPERJ, FAPESP (Brazil), MES (Bulgaria), CERN, CAS, MoST, NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), Academy of Sciences, NICPB (Estonia), Academy of Finland, ME, HIP (Finland), CEA, CNRS/IN2P3 (France), BMBF, Germany, DFG, HGF (Germany), GSRT (Greece), OTKA, NKTH (Hungary), DAE, DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF, WCU (Korea), LAS (Lithuania), CINVESTAV, CONACYT, SEP, UASLP-FAI (Mexico), PAEC (Pakistan), SCSR (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MST, MAE (Russia), MSTD (Serbia), MICINN, CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK, TAEK (Turkey), STFC (United Kingdom), DOE, NSF (USA) BMWF (Austria), FWF (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), MoER (Estonia) [SF0690030s09], ERDF (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Korea), WCU (Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), MSI (New Zealand), PAEC (Pakistan), MSHE (Poland), NSC (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MON (Russia), RosAtom (Russia), RAS (Russia), RFBR (Russia), MSTD (Serbia), SEIDI (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), ThEP (Thailand), IPST (Thailand), NECTEC (Thailand), TUBITAK (Turkey), TAEK (Turkey), NASU (Ukraine), STFC (United Kingdom), DOE (USA), NSF (USA), Marie-Curie programme (European Union), European Research Council (European Union), Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation, Austrian Science Fund (FWF), Belgian Federal Science Policy Office, Fonds pour la Formation a la Recherche dans lIndustrie et dans lAgriculture (FRIA-Belgium), Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium), Ministry of Education, Youth and Sports (MEYS) of Czech Republic, Council of Science and Industrial Research, India, Compagnia di San Paolo (Torino), HOMING PLUS programme of Foundation for Polish Science, European Union, Regional Development Fund
BMWF (Austria), FWF (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), MoER (Estonia) [SF0690030s09], ERDF (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Korea), WCU (Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), MSI (New Zealand), PAEC (Pakistan), MSHE (Poland), NSC (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MON (Russia), RosAtom (Russia), RAS (Russia), RFBR (Russia), MSTD (Serbia), SEIDI (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK (Turkey), TAEK (Turkey), STFC (United Kingdom), DOE (USA), NSF (USA) BMWFW (Austria), FWF (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), CSF (Croatia), RPF (Cyprus), MoER (Estonia), ERC IUT (Estonia), ERDF (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NIH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), MSIP (Republic of Korea), NRF (Republic of Korea), LAS (Lithuania), MOE (Malaysia), UM (Malaysia), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), MBIE (New Zealand), PAEC (Pakistan), MSHE (Poland), NSC (Poland), FCT (Portugal), JINR (Dubna), MON (Russia), RosAtom (Russia), RAS (Russia), RFBR (Russia), MESTD (Serbia), SEIDI (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), MST (Taipei), ThEPCenter (Thailand), IPST (Thailand), STAR (Thailand), NSTDA (Thailand), TUBITAK (Turkey), TAEK (Turkey), NASU (Ukraine), SFFR (Ukraine), STFC (United Kingdom), DOE (U.S.), NSF (U.S.)
BMWFW (Austria), FWF (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), CSF (Croatia), RPF (Cyprus), SENESCYT (Ecuador), MoER (Estonia), ERC IUT (Estonia), ERDF (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NIH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), MSIP (Republic of Korea), NRF (Republic of Korea), LAS (Lithuania), MOE (Malaysia), UM (Malaysia), BUAP (Mexico), CINVESTAV (Mexico), CONACYT (Mexico), LNS (Mexico), SEP (Mexico), UASLP-FAI (Mexico), MBIE (New Zealand), PAEC (Pakistan), MSHE (Poland), NSC (Poland), FCT (Portugal), JINR (Dubna), MON (Russia), RosAtom (Russia), RAS (Russia), RFBR (Russia), RAEP (Russia), MESTD (Serbia), SEIDI (Spain), CPAN (Spain), PCTI (Spain), FEDER (Spain), Swiss Funding Agencies (Switzerland), MST (Taipei), ThEPCenter (Thailand), IPST (Thailand), STAR (Thailand), NSTDA (Thailand), TUBITAK (Turkey), TAEK (Turkey), NASU (Ukraine), SFFR (Ukraine), STFC (United Kingdom), DOE (USA), NSF (USA) FMSR (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), Academy of Sciences (Estonia), NICPB (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Korea), WCU (Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), MSI (New Zealand), PAEC (Pakistan), SCSR (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MON (Russia), RosAtom (Russia), RAS (Russia), RFBR (Russia), MSTD (Serbia), MICINN (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK (Turkey), TAEK (Turkey), STFC (United Kingdom), DOE (USA), NSF (USA)
FMSR (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), Academy of Sciences (Estonia), NICPB (Estonia), Academy of Finland, ME (Finland), HIP (Finland), CEA (France), CNRS (France) [IN2P3], BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Korea), WCU (Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), PAEC (Pakistan), SCSR (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MST (Russia), MAE (Russia), MSTD (Serbia), MICINN (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK (Turkey), TAEK (Turkey), STFC (United Kingdom), DOE (USA), NSF (USA) FMSR (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN, CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), MoER (Estonia) [SF0690030s09], ERDF (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Korea), WCU (Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), MSI (New Zealand), PAEC (Pakistan), MSHE (Poland), NSC (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MON (Russia), RosAtom (Russia), RAS (Russia), RFBR (Russia), MSTD (Serbia), MICINN (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK (Turkey), TAEK (Turkey), STFC (United Kingdom), DOE (USA), NSF (USA)
FMSR (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN (China), CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), Academy of Sciences and NICPB (Estonia), Academy of Finland, ME (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Korea), WCU (Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), PAEC (Pakistan), SCSR (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MST (Russia), MAE (Russia), MSTD (Serbia), MICINN (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK (Turkey), TAEK (Turkey), STFC (United Kingdom), DOE (USA), NSF (USA) FMSR (Austria), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), CERN (China), CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), Academy of Sciences (Estonia), NICPB (Estonia), Academy of Finland, ME (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), BMBF, Germany, DFG (Germany), HGF (Germany), GSRT (Greece), OTKA (Hungary), NKTH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF (Korea), WCU (Korea), LAS (Lithuania), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), PAEC (Pakistan), SCSR (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MST (Russia), MAE (Russia), MSTD (Serbia), MICINN (Spain), CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK (Turkey), TAEK (Turkey), STFC (United Kingdom), DOE (USA), NSF (USA)
FMSR (Austria), FNRS, FWO (Belgium), CNPq, CAPES, FAPERJ, FAPESP (Brazil), MES (Bulgaria), CERN, CAS, MoST, NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), RPF (Cyprus), MoER [SF0690030s09], ERDF (Estonia), Academy of Finland, MEC, HIP (Finland), CEA, CNRS/IN2P3 (France), BMBF, Germany, DFG, HGF (Germany), GSRT (Greece), OTKA, NKTH (Hungary), DAE, DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), NRF, WCU (Korea), LAS (Lithuania), CINVESTAV, CONACYT, SEP, UASLP-FAI (Mexico), MSI (New Zealand), PAEC (Pakistan), MSHE, NSC (Poland), FCT (Portugal), JINR (Armenia), JINR (Belarus), JINR (Georgia), JINR (Ukraine), JINR (Uzbekistan), MON, RosAtom, RAS, RFBR (Russia), MSTD (Serbia), MICINN, CPAN (Spain), Swiss Funding Agencies (Switzerland), NSC (Taipei), TUBITAK, TAEK (Turkey), STFC (United Kingdom), DOE, NSF (USA) High Energy Physics with the CMS Detector
Science and Technology Facilities Council [CMS, ST/K001604/1] SCOAP3
ANPCyT, Argentina, YerPhI (Armenia), ARC, Australia, BMWFW (Austria), FWF (Austria), ANAS, Azerbaijan, SSTC (Belarus), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), NSERC (Canada), NRC (Canada), CFI (Canada), CERN, CONICYT (Chile), CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), CSF (Croatia), RPF (Cyprus), MSMT CR (Czech Republic), MPO CR (Czech Republic), VSC CR (Czech Republic), DNRF (Denmark), DNSRC (Denmark), Lundbeck Foundation (Denmark), MoER (Estonia), ERC IUT (Estonia), ERDF (Estonia), EPLANET (European Union), ERC (European Union), NSRF (European Union), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), GNSF (Georgia), BMBF, Germany, DFG (Germany), HGF (Germany), MPG (Germany), AvH Foundation (Germany), GSRT (Greece), NSRF (Greece), RGC (Hong Kong SAR, China), OTKA (Hungary), NIH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), ISF (Israel), MINERVA (Israel), GIF (Israel), I-CORE (Israel), Benoziyo Center, Israel, INFN (Italy), MEXT (Japan), JSPS (Japan), JINR, MSIP (Republic of Korea), NRF (Republic of Korea), LAS (Lithuania), MOE (Malaysia), UM (Malaysia), CINVESTAV (Mexico), CONACYT (Mexico), SEP (Mexico), UASLP-FAI (Mexico), CNRST (Morocco), FOM (Netherlands), NWO (Netherlands), MBIE (New Zealand), BRF (Norway), RCN (Norway), PAEC (Pakistan), MNiSW (Poland), MSHE (Poland), NCN (Poland), NSC (Poland), GRICES (Portugal), FCT (Portugal), MNE/IFA (Romania), MES of Russia (Russian Federation), MON (Russian Federation), RosAtom (Russian Federation), RAS (Russian Federation), RFBR (Russian Federation), MSTD (Serbia), MESTD (Serbia), MSSR (Slovakia), ARRS (Slovenia), MIZS (Slovenia), DST/NRF (South Africa), MINECO (Spain), SEIDI (Spain), CPAN (Spain), SRC (Switzerland), NSC (Taipei), MST (Taiwan), ThEPCenter (Thailand), IPST (Thailand), STAR (Thailand), NSTDA (Thailand), TUBITAK (Turkey), TAEK (Turkey), NASU (Ukraine), SFFR (Ukraine), STFC (U.K.), Royal Society and Leverhulme Trust (U.K.), DOE (U.S.), NSF (U.S.), Wallenberg Foundation (Sweden), ETH Board (Switzerland), ETH Zurich (Switzerland), PSI (Switzerland), SER (Switzerland), SNSF (Switzerland), UniZH (Switzerland), Cantons of Bern (Switzerland), Cantons of Geneve (Switzerland), Cantons of Zurich (Switzerland), ICREA ANPCyT, Argentina, YerPhI (Armenia), ARC, Australia, BMWFW (Austria), FWF (Austria), ANAS, Azerbaijan, SSTC (Belarus), FNRS (Belgium), FWO (Belgium), CNPq (Brazil), CAPES (Brazil), FAPERJ (Brazil), FAPESP (Brazil), MES (Bulgaria), NSERC (Canada), NRC (Canada), CFI (Canada), CERN, CONICYT (Chile), CAS (China), MoST (China), NSFC (China), COLCIENCIAS (Colombia), MSES (Croatia), CSF (Croatia), RPF (Cyprus), MSMT CR (Czech Republic), MPO CR (Czech Republic), VSC CR (Czech Republic), DNRF (Denmark), DNSRC (Denmark), MoER (Estonia), ERC IUT (Estonia), ERDF (Estonia), Academy of Finland, MEC (Finland), HIP (Finland), CEA (France), CNRS/IN2P3 (France), GNSF (Georgia), BMBF, Germany, DFG (Germany), HGF (Germany), MPG (Germany), GSRT (Greece), RGC (Hong Kong SAR, China), OTKA (Hungary), NIH (Hungary), DAE (India), DST (India), IPM (Iran), SFI (Ireland), ISF (Israel), I-CORE (Israel), Benoziyo Center, Israel, INFN (Italy), MEXT (Japan), JSPS (Japan), JINR, MSIP (Republic of Korea), NRF (Republic of Korea), LAS (Lithuania), MOE (Malaysia), UM (Malaysia), BUAP (Mexico), CINVESTAV (Mexico), CONACYT (Mexico), LNS (Mexico), SEP (Mexico), UASLP-FAI (Mexico), CNRST (Morocco), FOM (Netherlands), NWO (Netherlands), MBIE (New Zealand), RCN (Norway), PAEC (Pakistan), MNiSW (Poland), MSHE (Poland), NCN (Poland), NSC (Poland), FCT (Portugal), MNE/IFA (Romania), MES of Russia (Russian Federation), MON (Russian Federation), NRC KI (Russian Federation), RosAtom (Russian Federation), RAS (Russian Federation), RFBR (Russian Federation), MESTD (Serbia), MSSR (Slovakia), ARRS (Slovenia), MIZS (Slovenia), DST/NRF (South Africa), MINECO (Spain), SEIDI (Spain), CPAN (Spain), SRC (Sweden), Wallenberg Foundation (Sweden), ETH Board (Switzerland), ETH Zurich (Switzerland), PSI (Switzerland), SERI (Switzerland), SNSF (Switzerland), UniZH (Switzerland), Canton of Bern (Switzerland), Canton of Geneva (Switzerland), Canton of Zurich (Switzerland), MOST (Taipei), ThEPCenter (Thailand), IPST (Thailand), STAR (Thailand), NSTDA (Thailand), TUBITAK (Turkey), TAEK (Turkey), NASU (Ukraine), SFFR (Ukraine), STFC (United Kingdom), DOE (United States of America), NSF (United States of America), BELSPO (Belgium), FRIA (Belgium), IWT (Belgium), BCKDF (Canada), Canada Council (Canada), CANARIE (Canada), CRC (Canada), Compute Canada (Canada), FQRNT (Canada), Ontario Innovation Trust (Canada), Leventis Foundation (Cyprus), MEYS (Czech Republic), EPLANET (European Union), ERC (European Union), FP7 (European Union), Horizon 2020 (European Union), Marie Sklodowska-Curie Actions (European Union), Investissements dAvenir Labex and Idex (France), ANR (France), Region Auvergne (France), Fondation Partager le Savoir (France), AvH Foundation (Germany), Herakleitos program - EU-ESF (Greece), Thales program - EU-ESF (Greece), Aristeia program - EU-ESF (Greece), Greek NSRF (Greece), CSIR (India), BSF (Israel), GIF (Israel), Minerva (Israel), BRF (Norway), HOMING PLUS programme of the FPS - EU Regional Development Fund (Poland), Mobility Plus programme of the MSHE (Poland), OPUS programme of the NSC (Poland), NPRP by Qatar NRF (Qatar), Generalitat de Catalunya (Spain), Generalitat Valenciana (Spain), Programa Clarin-COFUND del Principado de Asturias (Spain), Rachadapisek Sompot Fund for Postdoctoral Fellowship, Chulalongkorn University (Thailand), Chulalongkorn Academic into Its 2nd Century Project Advancement Project (Thailand), Royal Society (United Kingdom), Leverhulme Trust (United Kingdom), A.P. Sloan Foundation, Welch Foundation (United States of America)
Austrian Federal Ministry of Science and Research and the Austrian Science Fund, Belgian Fonds de la Recherche Scientifique, and Fonds voor Wetenschappelijk Onderzoek, Brazilian Funding Agencies (CNPq, CAPES, FAPERJ, and FAPESP), Bulgarian Ministry of Education and Science, CERN, Chinese Academy of Sciences, Ministry of Science and Technology, and National Natural Science Foundation of China, Colombian Funding Agency (COLCIENCIAS), Croatian Ministry of Science, Education and Sport, Research Promotion Foundation, Cyprus, Ministry of Education and Research [SF0690030s09], European Regional Development Fund, Estonia, Academy of Finland, Finnish Ministry of Education and Culture, and Helsinki Institute of Physics, Institut National de Physique Nucleaire et de Physique des Particules/CNRS, and Commissariat a lEnergie Atomique et aux Energies Alternatives/CEA, France, Bundesministerium fur Bildung und Forschung, Deutsche Forschungsgemeinschaft, and Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany, General Secretariat for Research and Technology, Greece, National Scientific Research Foundation, and National Office for Research and Technology, Hungary, Department of Atomic Energy and the Department of Science and Technology, India, Institute for Studies in Theoretical Physics and Mathematics, Iran, Science Foundation, Ireland, Istituto Nazionale di Fisica Nucleare, Italy, Korean Ministry of Education, Science and Technology and the World Class University program of NRF, Republic of Korea, Lithuanian Academy of Sciences, Mexican Funding Agencies (CINVESTAV, CONACYT, SEP, and UASLP-FAI), Ministry of Business, Innovation and Employment, New Zealand, Pakistan Atomic Energy Commission, Ministry of Science and Higher Education and the National Science Centre, Poland, Fundacao para a Ciencia e a Tecnologia, Portugal, JINR, Dubna, Ministry of Education and Science of the Russian Federation, the Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, and the Russian Foundation for Basic Research, Ministry of Education, Science and Technological Development of Serbia, Secretaria de Estado de Investigacion, Desarrollo e Innovacion and Programa Consolider-Ingenio, Spain, Swiss Funding Agencies (ETH Board, ETH Zurich, PSI, SNF, UniZH, Canton Zurich, and SER), National Science Council, Taipei, Thailand Center of Excellence in Physics, the Institute for the Promotion of Teaching Science and Technology of Thailand, Special Task Force for Activating Research and the National Science and Technology Development Agency of Thailand, Scientific and Technical Research Council of Turkey, and Turkish Atomic Energy Authority, Science and Technology Facilities Council, UK, U.S. Department of Energy, and the U.S. National Science Foundation, Marie-Curie program and the European Research Council and EPLANET (European Union), Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation, Belgian Federal Science Policy Office, Fonds pour la Formation a la Recherche dans lIndustrie et dans lAgriculture (FRIA-Belgium), Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium), Ministry of Education, Youth and Sports (MEYS) of Czech Republic, Council of Science and Industrial Research, India, Compagnia di San Paolo (Torino), HOMING PLUS program of Foundation for Polish Science, EU, Regional Development Fund, Thalis and Aristeia programs, EU-ESF and the Greek NSRF Austrian Federal Ministry of Science and Research and the Austrian Science Fund, Belgian Fonds de la Recherche Scientifique, Fonds voor Wetenschappelijk Onderzoek, Brazilian Funding Agency (CNPq), Brazilian Funding Agency (CAPES), Brazilian Funding Agency(FAPERJ), Brazilian Funding Agency (FAPESP), Bulgarian Ministry of Education and Science, CERN, Chinese Academy of Sciences, Ministry of Science and Technology, and National Natural Science Foundation of China, Colombian Funding Agency (COLCIENCIAS), Croatian Ministry of Science, Education and Sport, Research Promotion Foundation, Cyprus, Ministry of Education and Research [SF0690030s09], European Regional Development Fund, Estonia, Academy of Finland, Finnish Ministry of Education and Culture, Helsinki Institute of Physics, Institut National de Physique Nucleaire et de Physique des Particules / CNRS, Commissariat a lEnergie Atomique et aux Energies Alternatives / CEA, France, Bundesministerium fur Bildung und Forschung, Deutsche Forschungsgemeinschaft, Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany, General Secretariat for Research and Technology, Greece, National Scientific Research Foundation, National Office for Research and Technology, Hungary, Department of Atomic Energy and the Department of Science and Technology, India, Institute for Studies in Theoretical Physics and Mathematics, Iran, Science Foundation, Ireland, Istituto Nazionale di Fisica Nucleare, Italy, Korean Ministry of Education, Science and Technology, World Class University program of NRF, Republic of Korea, Lithuanian Academy of Sciences, Mexican Funding Agency (CINVESTAV), Mexican Funding Agency (CONACYT), Mexican Funding Agency (SEP), Mexican Funding Agency (UASLP-FAI), Ministry of Business, Innovation and Employment, New Zealand, Pakistan Atomic Energy Commission, Ministry of Science and Higher Education, National Science Centre, Poland, Fundacao para a Ciencia e a Tecnologia, Portugal, JINR, Dubna, Ministry of Education and Science of the Russian Federation, Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, Russian Foundation for Basic Research, Ministry of Education, Science and Technological Development of Serbia, Secretaria de Estado de Investigacion, Desarrollo e Innovacion and Programa Consolider-Ingenio, spain, Swiss Funding Agency (ETH Board), Swiss Funding Agency (ETH Zurich), Swiss Funding Agency (PSI), Swiss Funding Agency (SNF), Swiss Funding Agency (UniZH), Swiss Funding Agency (Canton Zurich), Swiss Funding Agency (SER), National Science Council, Taipei, Thailand Center of Excellence in Physics, Institute for the Promotion of Teaching Science and Technology of Thailand, Special Task Force for Activating Research, National Science and Technology Development Agency of Thailand, Scientific and Technical Research Council of Turkey, Turkish Atomic Energy Authority, Science and Technology Facilities Council, U.K, US Department of Energy, US National Science Foundation, Marie-Curie programme, European Research Council and EPLANET (European Union), Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation, Belgian Federal Science Policy Office, Fonds pour la Formation a la Recherche dans lIndustrie et dans lAgriculture (FRIA-Belgium), Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium), Ministry of Education, Youth and Sports (MEYS) of Czech Republic, Council of Science and Industrial Research, India, Compagnia di San Paolo (Torino), HOMING PLUS programme of Foundation for Polish Science, EU, Regional Development Fund, Thalis and Aristeia programmes, EU-ESF, Greek NSRF
Austrian Federal Ministry of Science and Research, Austrian Science Fund, Belgian Fonds de la Recherche Scientifique, Fonds voor Wetenschappelijk Onderzoek, Brazilian Funding Agency (CNPq), Brazilian Funding Agency (CAPES), Brazilian Funding Agency (FAPERJ), Brazilian Funding Agency (FAPESP), Bulgarian Ministry of Education and Science, CERN, Chinese Academy of Sciences, Ministry of Science and Technology, National Natural Science Foundation of China, Colombian Funding Agency (COLCIENCIAS), Croatian Ministry of Science, Education and Sport, Research Promotion Foundation, Cyprus, Ministry of Education and Research [SF0690030s09], European Regional Development Fund, Estonia, Academy of Finland, Finnish Ministry of Education and Culture, Helsinki Institute of Physics, Institut National de Physique Nucleaire et de Physique des Particules / CNRS, Commissariat a lEnergie Atomique et aux Energies Alternatives / CEA, France, Bundesministerium fur Bildung und Forschung, Deutsche Forschungsgemeinschaft, Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany, General Secretariat for Research and Technology, Greece, National Scientific Research Foundation, National Office for Research and Technology, Hungary, Department of Atomic Energy, Department of Science and Technology, India, Institute for Studies in Theoretical Physics and Mathematics, Iran, Science Foundation, Ireland, Istituto Nazionale di Fisica Nucleare, Italy, Korean Ministry of Education, Science and Technology, World Class University program of NRF, Republic of Korea, Lithuanian Academy of Sciences, CINVESTAV, CONACYT, SEP, UASLP-FAI, Ministry of Science and Innovation, New Zealand, Pakistan Atomic Energy Commission, Ministry of Science and Higher Education, National Science Centre, Poland, Fundacao para a Ciencia e a Tecnologia, Portugal, JINR, Dubna, Ministry of Education and Science of the Russian Federation, Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, Russian Foundation for Basic Research, Ministry of Education, Science and Technological Development of Serbia, Secretaria de Estado de Investigacion, Desarrollo e Innovacion and Programa Consolider-Ingenio, Spain, ETH Board, ETH Zurich, PSI, SNF, UniZH, Canton Zurich, SER, National Science Council, Taipei, Thailand Center of Excellence in Physics, Institute for the Promotion of Teaching Science and Technology of Thailand, Special Task Force for Activating Research, National Science and Technology Development Agency of Thailand, Scientific and Technical Research Council of Turkey, Turkish Atomic Energy Authority, Science and Technology Facilities Council, U.K., US Department of Energy, US National Science Foundation, Marie-Curie programme, European Research Council, EPLANET (European Union), Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation, Belgian Federal Science Policy Office, Fonds pour la Formation a la Recherche dans lIndustrie et dans lAgriculture (FRIA-Belgium), Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium), Ministry of Education, Youth and Sports (MEYS) of Czech Republic, Council of Science and Industrial Research, India, Compagnia di San Paolo (Torino), HOMING PLUS programme of Foundation for Polish Science, EU, Regional Development Fund, Thalis and Aristeia programmes, EU-ESF, Greek NSRF Austrian Federal Ministry of Science and Research, Austrian Science Fund, Belgian Fonds de la Recherche Scientifique, Fonds voor Wetenschappelijk Onderzoek, CNPq, CAPES, FAPERJ, FAPESP, Bulgarian Ministry of Education and Science, CERN, Chinese Academy of Sciences, Ministry of Science and Technology, and National Natural Science Foundation of China, Colombian Funding Agency (COLCIENCIAS), Croatian Ministry of Science, Education and Sport, Croatian Science Foundation, Research Promotion Foundation, Cyprus, Ministry of Education and Research [SF0690030s09], European Regional Development Fund, Estonia, Academy of Finland, Finnish Ministry of Education and Culture, and Helsinki Institute of Physics, Institut National de Physique Nucleaire et de Physique des Particules / CNRS, Commissariat a lEnergie Atomique et aux Energies Alternatives / CEA, France, Bundesministerium fur Bildung und Forschung, Deutsche Forschungsgemeinschaft, Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany, General Secretariat for Research and Technology, Greece, National Scientific Research Foundation, National Innovation Office, Hungary, Department of Atomic Energy, Department of Science and Technology, India, Institute for Studies in Theoretical Physics and Mathematics, Iran, Science Foundation, Ireland, Istituto Nazionale di Fisica Nucleare, Italy, Korean Ministry of Education, Science and Technology, World Class University program of NRF, Republic of Korea, Lithuanian Academy of Sciences, Ministry of Education, and University of Malaya (Malaysia), CINVESTAV, CONACYT, SEP, UASLP-FAI, Ministry of Business, Innovation and Employment, New Zealand, Pakistan Atomic Energy Commission, Ministry of Science and Higher Education, National Science Centre, Poland, Funda, cao para a Ciencia e a Tecnologia, Portugal, JINR, Dubna, Ministry of Education and Science of the Russian Federation, Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, Russian Foundation for Basic Research, Ministry of Education, Science and Technological Development of Serbia, Secretaria de Estado de Investigacion, Desarrollo e Innovacion and Programa Consolider-Ingenio, Spain, ETH Board, ETH Zurich, PSI, SNF, UniZH, Canton Zurich, SER, National Science Council, Taipei, Thailand Center of Excellence in Physics, Institute for the Promotion of Teaching Science and Technology of Thailand, Special Task Force for Activating Research, National Science and Technology Development Agency of Thailand, Scientific and Technical Research Council of Turkey, Turkish Atomic Energy Authority, Science and Technology Facilities Council, U.K., US Department of Energy, and the US National Science Foundation, Marie-Curie programme, European Research Council and EPLANET (European Union), Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation, Belgian Federal Science Policy Office, Fonds pour la Formation a la Recherche dans lIndustrie et dans lAgriculture (FRIA-Belgium), Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium), Ministry of Education, Youth and Sports (MEYS) of Czech Republic, Council of Science and Industrial Research, India, Compagnia di San Paolo (Torino), HOMING PLUS programme of Foundation for Polish Science, EU, Regional Development Fund, Thalis and Aristeia programmes, EU-ESF, Greek NSRF
Austrian Federal Ministry of Science and Research, Austrian Science Fund, Belgian Fonds de la Recherche Scientifique, Fonds voor Wetenschappelijk Onderzoek, CNPq, CAPES, FAPERJ, FAPESP, Bulgarian Ministry of Education and Science, CERN, Chinese Academy of Sciences, Ministry of Science and Technology, National Natural Science Foundation of China, Colombian Funding Agency (COLCIENCIAS), Croatian Ministry of Science, Education and Sport, Croatian Science Foundation, Research Promotion Foundation, Cyprus, Ministry of Education and Research, European Regional Development Fund, Estonia, Academy of Finland, Finnish Ministry of Education and Culture, Helsinki Institute of Physics, Institut National de Physique Nucleaire et de Physique des Particules / CNRS, Commissariat a lEnergie Atomique et aux Energies Alternatives / CEA, France, Bundesministerium fur Bildung und Forschung, Deutsche Forschungsgemeinschaft, Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany, General Secretariat for Research and Technology, Greece, National Scientific Research Foundation, National Innovation Office, Hungary, Department of Atomic Energy, Department of Science and Technology, India, Institute for Studies in Theoretical Physics and Mathematics, Iran, Science Foundation, Ireland, Istituto Nazionale di Fisica Nucleare, Italy, Korean Ministry of Education, Science and Technology, World Class University program of NRF, Republic of Korea, Lithuanian Academy of Sciences, CINVESTAV, CONACYT, SEP, UASLP-FAI, Ministry of Business, Innovation and Employment, New Zealand, Pakistan Atomic Energy Commission, Ministry of Science and Higher Education, National Science Centre, Poland, Fundacao para a Ciencia e a Tecnologia, Portugal, JINR, Dubna, Ministry of Education and Science of the Russian Federation, Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, Russian Foundation for Basic Research, Ministry of Education, Science and Technological Development of Serbia, Secretaria de Estado de Investigacion, Desarrollo e Innovacion and Programa Consolider-Ingenio, Spain, ETH Board, ETH Zurich, PSI, SNF, UniZH, Canton Zurich, SER, National Science Council, Taipei, Thailand Center of Excellence in Physics, Institute for the Promotion of Teaching Science and Technology of Thailand, Special Task Force for Activating Research, National Science and Technology Development Agency of Thailand, Scientific and Technical Research Council of Turkey, Turkish Atomic Energy Authority, Science and Technology Facilities Council, U.K., US Department of Energy, US National Science Foundation, Marie-Curie programme, European Research Council, EPLANET (European Union), Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation, Belgian Federal Science Policy Office, Fonds pour la Formation a la Recherche dans lIndustrie et dans lAgriculture (FRIA-Belgium), Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium), Ministry of Education, Youth and Sports (MEYS) of Czech Republic, Council of Science and Industrial Research, India, Compagnia di San Paolo (Torino), HOMING PLUS programme of Foundation for Polish Science, EU, Regional Development Fund, EU-ESF, Greek NSRF, [SF0690030s09] Austrian Federal Ministry of Science and Research, Austrian Science Fund, Belgian Fonds de la Recherche Scientifique, Fonds voor Wetenschappelijk Onderzoek, CNPq, CAPES, FAPERJ, FAPESP, Bulgarian Ministry of Education and Science, CERN, Chinese Academy of Sciences, Ministry of Science and Technology, National Natural Science Foundation of China, Colombian Funding Agency (COLCIENCIAS), Croatian Ministry of Science, Education and Sport, Croatian Science Foundation, Research Promotion Foundation, Cyprus, Ministry of Education and Research, European Regional Development Fund, Estonia, Academy of Finland, Finnish Ministry of Education and Culture, Helsinki Institute of Physics, Institut National de Physique Nucleaire et de Physique des Particules / CNRS, Commissariat a lEnergie Atomique et aux Energies Alternatives / CEA, France, Bundesministerium fur Bildung und Forschung, Deutsche Forschungsgemeinschaft, Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany, General Secretariat for Research and Technology, Greece, National Scientific Research Foundation, National Innovation Office, Hungary, Department of Atomic Energy, India, Department of Science and Technology, India, Institute for Studies in Theoretical Physics and Mathematics, Iran, Science Foundation, Ireland, Istituto Nazionale di Fisica Nucleare, Italy, Korean Ministry of Education, Science and Technology, Republic of Korea, World Class University program of NRF, Republic of Korea, Lithuanian Academy of Sciences, Ministry of Education (Malaysia), University of Malaya (Malaysia), CINVESTAV, Mexican Funding Agency, CONACYT, Mexican Funding Agency, SEP, Mexican Funding Agency, UASLP-FAI, Mexican Funding Agency, Ministry of Business, Innovation and Employment, New Zealand, Pakistan Atomic Energy Commission, Ministry of Science and Higher Education, Poland, National Science Centre, Poland, Fundacao para a Ciencia e a Tecnologia, Portugal, JINR, Dubna, Ministry of Education and Science of the Russian Federation, Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, Russian Foundation for Basic Research, Ministry of Education, Science and Technological Development of Serbia, Secretaria de Estado de Investigacion, Spain, Desarrollo e Innovacion, Spain, Programa Consolider-Ingenio, Spain, ETH Board, Swiss Funding Agency, ETH Zurich, Swiss Funding Agency, PSI, Swiss Funding Agency, SNF, Swiss Funding Agency, UniZH, Swiss Funding Agency, Canton Zurich, Swiss Funding Agency, SER, Swiss Funding Agency, National Science Council, Taipei, Thailand Center of Excellence in Physics, Institute for the Promotion of Teaching Science and Technology of Thailand, Special Task Force for Activating Research, National Science and Technology Development Agency of Thailand, Scientific and Technical Research Council of Turkey, Turkish Atomic Energy Authority, Science and Technology Facilities Council, UK, US Department of Energy, US National Science Foundation, Marie-Curie programme (European Union), European Research Council (European Union), EPLANET (European Union), Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation, Belgian Federal Science Policy Office (FRIA-Belgium), Fonds pour la Formation a la Recherche dans lIndustrie et dans lAgriculture (FRIA-Belgium), Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium), Ministry of Education, Youth and Sports (MEYS) of Czech Republic, Council of Science and Industrial Research, India, Compagnia di San Paolo (Torino), HOMING PLUS programme of Foundation for Polish Science, EU, Regional Development Fund, Thalis and Aristeia programmes - EU-ESF, Greek NSRF, [SF0690030s09]
Austrian Federal Ministry of Science and Research, Austrian Science Fund, Belgian Fonds de la Recherche Scientifique, Fonds voor Wetenschappelijk Onderzoek, CNPq, CAPES, FAPERJ, FAPESP, Bulgarian Ministry of Education and Science, CERN, Chinese Academy of Sciences, Ministry of Science and Technology, National Natural Science Foundation of China, Colombian Funding Agency (COLCIENCIAS), Croatian Ministry of Science, Education and Sport, Croatian Science Foundation, Research Promotion Foundation, Cyprus, Ministry of Education and Research, Recurrent financing contract [SF0690030s09], European Regional Development Fund, Estonia, Academy of Finland, Finnish Ministry of Education and Culture, Helsinki Institute of Physics, Institut National de Physique Nucleaire et de Physique des Particules / CNRS, Commissariat a lEnergie Atomique et aux Energies Alternatives / CEA, France, Bundesministerium fur Bildung und Forschung, Deutsche Forschungsgemeinschaft, Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany, General Secretariat for Research and Technology, Greece, National Scientific Research Foundation, National Innovation Office, Hungary, Department of Atomic Energy, Department of Science and Technology, India, Institute for Studies in Theoretical Physics and Mathematics, Iran, Science Foundation, Ireland, Istituto Nazionale di Fisica Nucleare, Italy, Korean Ministry of Education, Science and Technology, World Class University program of NRF, Republic of Korea, Lithuanian Academy of Sciences, Ministry of Education, and University of Malaya (Malaysia), CINVESTAV, CONACYT, SEP, UASLP-FAI, Ministry of Business, Innovation and Employment, New Zealand, Pakistan Atomic Energy Commission, Ministry of Science and Higher Education, National Science Centre, Poland, Fundacao para a Ciencia e a Tecnologia, Portugal, JINR, Dubna, Ministry of Education and Science of the Russian Federation, Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, Russian Foundation for Basic Research, Ministry of Education, Science and Technological Development of Serbia, Secretaria de Estado de Investigacion, Desarrollo e Innovacion and Programa Consolider-Ingenio, Spain, ETH Board, ETH Zurich, PSI, SNF, UniZH, Canton Zurich, SER, National Science Council, Taipei, Thailand Center of Excellence in Physics, Institute for the Promotion of Teaching Science and Technology of Thailand, Special Task Force for Activating Research, National Science and Technology Development Agency of Thailand, Scientific and Technical Research Council of Turkey, Turkish Atomic Energy Authority, National Academy of Sciences of Ukraine, State Fund for Fundamental Researches, Ukraine, Science and Technology Facilities Council, U.K., US Department of Energy, US National Science Foundation, Marie-Curie programme, European Research Council, EPLANET (European Union), Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation, Belgian Federal Science Policy Office, Fonds pour la Formation a la Recherche dans lIndustrie et dans lAgriculture (FRIA-Belgium), Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium), Ministry of Education, Youth and Sports (MEYS) of Czech Republic, Council of Science and Industrial Research, India, Compagnia di San Paolo (Torino), HOMING PLUS programme of Foundation for Polish Science, EU, Regional Development Fund, Thalis and Aristeia programmes, EU-ESF, Greek NSRF Austrian Federal Ministry of Science and Research, Austrian Science Fund, Belgian Fonds de la Recherche Scientifique, Fonds voor Wetenschappelijk Onderzoek, CNPq, CAPES, FAPERJ, FAPESP, Bulgarian Ministry of Education and Science, CERN, Chinese Academy of Sciences, Ministry of Science and Technology, National Natural Science Foundation of China, Colombian Funding Agency (COLCIENCIAS), Croatian Ministry of Science, Education and Sport, Croatian Science Foundation, Research Promotion Foundation, Cyprus, Ministry of Education and Research [SF0690030s09], European Regional Development Fund, Estonia, Academy of Finland, Finnish Ministry of Education and Culture, Helsinki Institute of Physics, Institut National de Physique Nucleaire et de Physique des Particules/CNRS, Commissariat a lEnergie Atomique et aux Energies Alternatives/CEA, France, Bundesministerium fur Bildung und Forschung, Deutsche Forschungsgemeinschaft, Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany, General Secretariat for Research and Technology, Greece, National Scientific Research Foundation, National Innovation Office, Hungary, Department of Atomic Energy and the Department of Science and Technology, India, Institute for Studies in Theoretical Physics and Mathematics, Iran, Science Foundation, Ireland, Istituto Nazionale di Fisica Nucleare, Italy, Korean Ministry of Education, Science and Technology and the World Class University program of NRF, Republic of Korea, Lithuanian Academy of Sciences, Mexican Funding Agencies (CINVESTAV, CONACYT, SEP, and UASLP-FAI), Ministry of Business, Innovation and Employment, New Zealand, Pakistan Atomic Energy Commission, Ministry of Science and Higher Education, National Science Centre, Poland, Fundacao para a Ciencia e a Tecnologia, Portugal, JINR, Dubna, Ministry of Education and Science of the Russian Federation, Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, Russian Foundation for Basic Research, Ministry of Education, Science and Technological Development of Serbia, Secretaria a de Estado de Investigacion, Desarrollo e Innovacion and Programa Consolider-Ingenio, Spain, Swiss Funding Agencies (ETH Board, ETH Zurich, PSI, SNF, UniZH, Canton Zurich, and SER), National Science Council, Taipei, Thailand Center of Excellence in Physics, Institute for the Promotion of Teaching Science and Technology of Thailand, Special Task Force for Activating Research, National Science and Technology Development Agency of Thailand, Scientific and Technical Research Council of Turkey, Turkish Atomic Energy Authority, Science and Technology Facilities Council, UK, U.S. Department of Energy, U.S. National Science Foundation, Marie-Curie programme, European Research Council, EPLANET (European Union), Leventis Foundation, A.P. Sloan Foundation, Alexander von Humboldt Foundation, Belgian Federal Science Policy Office, Fonds pour la Formation a la Recherche dans lIndustrie et dans lAgriculture (FRIA-Belgium), Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium), Ministry of Education, Youth and Sports (MEYS) of Czech Republic, Council of Science and Industrial Research, India, Compagnia di San Paolo (Torino), HOMING PLUS programme of Foundation for Polish Science, EU, Regional Development Fund, EU-ESF, Greek NSRF

Author's Bibliography

Study of azimuthal anisotropy of Υ(1S) mesons in pPb collisions at √𝑠NN = 8.16 TeV

Tumasyan, A.; Adam, W.; Andrejkovic, J.; Bergauer, T.; Chatterjee, S.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan

(2024)

TY  - JOUR
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J.
AU  - Bergauer, T.
AU  - Chatterjee, S.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
PY  - 2024
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/13121
AB  - The azimuthal anisotropy of Υ(1S) mesons in high-multiplicity proton-lead collisions is studied using data collected by the CMS experiment at a nucleon-nucleon center-of-mass energy of 8.16 TeV. The Υ(1S) mesons are reconstructed using their dimuon decay channel. The anisotropy is characterized by the second Fourier harmonic coefficients, found using a two-particle correlation technique, in which the Υ(1S) mesons are correlated with charged hadrons. A large pseudorapidity gap is used to suppress short-range correlations. Nonflow contamination from the dijet background is removed using a low-multiplicity subtraction method, and the results are presented as a function of Υ(1S) transverse momentum. The azimuthal anisotropies are smaller than those found for charmonia in proton-lead collisions at the same collision energy, but are consistent with values found for Υ(1S) mesons in lead-lead interactions at a nucleon-nucleon center-of-mass energy of 5.02 TeV.
T2  - Physics Letters B
T1  - Study of azimuthal anisotropy of Υ(1S) mesons in pPb collisions at √𝑠NN = 8.16 TeV
VL  - 850
SP  - 138518
DO  - 10.1016/j.physletb.2024.138518
ER  - 
@article{
author = "Tumasyan, A. and Adam, W. and Andrejkovic, J. and Bergauer, T. and Chatterjee, S. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan",
year = "2024",
abstract = "The azimuthal anisotropy of Υ(1S) mesons in high-multiplicity proton-lead collisions is studied using data collected by the CMS experiment at a nucleon-nucleon center-of-mass energy of 8.16 TeV. The Υ(1S) mesons are reconstructed using their dimuon decay channel. The anisotropy is characterized by the second Fourier harmonic coefficients, found using a two-particle correlation technique, in which the Υ(1S) mesons are correlated with charged hadrons. A large pseudorapidity gap is used to suppress short-range correlations. Nonflow contamination from the dijet background is removed using a low-multiplicity subtraction method, and the results are presented as a function of Υ(1S) transverse momentum. The azimuthal anisotropies are smaller than those found for charmonia in proton-lead collisions at the same collision energy, but are consistent with values found for Υ(1S) mesons in lead-lead interactions at a nucleon-nucleon center-of-mass energy of 5.02 TeV.",
journal = "Physics Letters B",
title = "Study of azimuthal anisotropy of Υ(1S) mesons in pPb collisions at √𝑠NN = 8.16 TeV",
volume = "850",
pages = "138518",
doi = "10.1016/j.physletb.2024.138518"
}
Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Chatterjee, S., Adžić, P., Đorđević, M., Milenović, P.,& Milošević, J.. (2024). Study of azimuthal anisotropy of Υ(1S) mesons in pPb collisions at √𝑠NN = 8.16 TeV. in Physics Letters B, 850, 138518.
https://doi.org/10.1016/j.physletb.2024.138518
Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Chatterjee S, Adžić P, Đorđević M, Milenović P, Milošević J. Study of azimuthal anisotropy of Υ(1S) mesons in pPb collisions at √𝑠NN = 8.16 TeV. in Physics Letters B. 2024;850:138518.
doi:10.1016/j.physletb.2024.138518 .
Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Chatterjee, S., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, "Study of azimuthal anisotropy of Υ(1S) mesons in pPb collisions at √𝑠NN = 8.16 TeV" in Physics Letters B, 850 (2024):138518,
https://doi.org/10.1016/j.physletb.2024.138518 . .

Higher-order moments of the elliptic flow distribution in PbPb collisions at √sNN = 5.02 TeV

Tumasyan, A.; Adam, W.; Andrejkovic, J.; Bergauer, T.; Chatterjee, S.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan; Nađđerđ, Laslo

(2024)

TY  - JOUR
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J.
AU  - Bergauer, T.
AU  - Chatterjee, S.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
AU  - Nađđerđ, Laslo
PY  - 2024
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/13093
AB  - The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, v 2{2k}, are measured up to the tenth order (k = 5) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of      s NN     $$ \sqrt{s_{\textrm{NN}}} $$  = 5.02 TeV. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of 0.607 nb −1. A hierarchy is observed between the coefficients, with v 2{2} > v 2{4} ≳ v 2{6} ≳ v 2{8} ≳ v 2{10}. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event v 2 distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.
T2  - Journal of High Energy Physics
T1  - Higher-order moments of the elliptic flow distribution in PbPb collisions at √sNN = 5.02 TeV
VL  - 2024
IS  - 2
SP  - 1
EP  - 45
DO  - 10.1007/JHEP02(2024)106
ER  - 
@article{
author = "Tumasyan, A. and Adam, W. and Andrejkovic, J. and Bergauer, T. and Chatterjee, S. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan and Nađđerđ, Laslo",
year = "2024",
abstract = "The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, v 2{2k}, are measured up to the tenth order (k = 5) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of      s NN     $$ \sqrt{s_{\textrm{NN}}} $$  = 5.02 TeV. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of 0.607 nb −1. A hierarchy is observed between the coefficients, with v 2{2} > v 2{4} ≳ v 2{6} ≳ v 2{8} ≳ v 2{10}. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event v 2 distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.",
journal = "Journal of High Energy Physics",
title = "Higher-order moments of the elliptic flow distribution in PbPb collisions at √sNN = 5.02 TeV",
volume = "2024",
number = "2",
pages = "1-45",
doi = "10.1007/JHEP02(2024)106"
}
Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Chatterjee, S., Adžić, P., Đorđević, M., Milenović, P., Milošević, J.,& Nađđerđ, L.. (2024). Higher-order moments of the elliptic flow distribution in PbPb collisions at √sNN = 5.02 TeV. in Journal of High Energy Physics, 2024(2), 1-45.
https://doi.org/10.1007/JHEP02(2024)106
Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Chatterjee S, Adžić P, Đorđević M, Milenović P, Milošević J, Nađđerđ L. Higher-order moments of the elliptic flow distribution in PbPb collisions at √sNN = 5.02 TeV. in Journal of High Energy Physics. 2024;2024(2):1-45.
doi:10.1007/JHEP02(2024)106 .
Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Chatterjee, S., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Nađđerđ, Laslo, "Higher-order moments of the elliptic flow distribution in PbPb collisions at √sNN = 5.02 TeV" in Journal of High Energy Physics, 2024, no. 2 (2024):1-45,
https://doi.org/10.1007/JHEP02(2024)106 . .

Computational approaches in the estimation of radiobiological damage for human-malignant cells irradiated with clinical proton and carbon beams

Đorđević, Miloš; Fattori, Serena; Petringa, Giada; Ristić Fira, Aleksandra; Petrović, Ivan; Cuttone, Giacomo; Cirrone, G.A. Pablo

(2024)

TY  - JOUR
AU  - Đorđević, Miloš
AU  - Fattori, Serena
AU  - Petringa, Giada
AU  - Ristić Fira, Aleksandra
AU  - Petrović, Ivan
AU  - Cuttone, Giacomo
AU  - Cirrone, G.A. Pablo
PY  - 2024
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/12241
AB  - Purpose: The use of Monte Carlo (MC) simulations capable of reproducing radiobiological effects of ionising radiation on human cell lines is of great importance, especially for cases involving protons and heavier ion beams. In the latter, huge uncertainties can arise mainly related to the effects of the secondary particles produced in the beam-tissue interaction. This paper reports on a detailed MC study performed using Geant4-based approach on three cancer cell lines, the HTB-177, CRL-5876 and MCF-7, that were previously irradiated with therapeutic proton and carbon ion beams. Methods: A Geant4-based approach used jointly with analytical calculations has been developed to provide a more realistic estimation of the radiobiological damage produced by proton and carbon beams in tissues, reproducing available data obtained from in vitro cell irradiations. The MC “Hadrontherapy” Geant4 application and the Local Effect Model: LEM I, LEM II and LEM III coupled with the different numerical approaches: RapidRusso (RR) and RapidScholz (RS) were used in the study. Results: Experimental survival curves are compared with those evaluated using the highlighted Geant4 MC-based approach via chi-square statistical analysis, for the combinations of radiobiological models and numerical approaches, as outlined above. Conclusion: This study has presented a comparison of the survival data from MC simulations to experimental survival data for three cancer cell lines. An overall best level of agreement was obtained for the HTB-177 cells.
T2  - Physica Medica
T1  - Computational approaches in the estimation of radiobiological damage for human-malignant cells irradiated with clinical proton and carbon beams
VL  - 117
SP  - 103189
DO  - 10.1016/j.ejmp.2023.103189
ER  - 
@article{
author = "Đorđević, Miloš and Fattori, Serena and Petringa, Giada and Ristić Fira, Aleksandra and Petrović, Ivan and Cuttone, Giacomo and Cirrone, G.A. Pablo",
year = "2024",
abstract = "Purpose: The use of Monte Carlo (MC) simulations capable of reproducing radiobiological effects of ionising radiation on human cell lines is of great importance, especially for cases involving protons and heavier ion beams. In the latter, huge uncertainties can arise mainly related to the effects of the secondary particles produced in the beam-tissue interaction. This paper reports on a detailed MC study performed using Geant4-based approach on three cancer cell lines, the HTB-177, CRL-5876 and MCF-7, that were previously irradiated with therapeutic proton and carbon ion beams. Methods: A Geant4-based approach used jointly with analytical calculations has been developed to provide a more realistic estimation of the radiobiological damage produced by proton and carbon beams in tissues, reproducing available data obtained from in vitro cell irradiations. The MC “Hadrontherapy” Geant4 application and the Local Effect Model: LEM I, LEM II and LEM III coupled with the different numerical approaches: RapidRusso (RR) and RapidScholz (RS) were used in the study. Results: Experimental survival curves are compared with those evaluated using the highlighted Geant4 MC-based approach via chi-square statistical analysis, for the combinations of radiobiological models and numerical approaches, as outlined above. Conclusion: This study has presented a comparison of the survival data from MC simulations to experimental survival data for three cancer cell lines. An overall best level of agreement was obtained for the HTB-177 cells.",
journal = "Physica Medica",
title = "Computational approaches in the estimation of radiobiological damage for human-malignant cells irradiated with clinical proton and carbon beams",
volume = "117",
pages = "103189",
doi = "10.1016/j.ejmp.2023.103189"
}
Đorđević, M., Fattori, S., Petringa, G., Ristić Fira, A., Petrović, I., Cuttone, G.,& Cirrone, G.A. P.. (2024). Computational approaches in the estimation of radiobiological damage for human-malignant cells irradiated with clinical proton and carbon beams. in Physica Medica, 117, 103189.
https://doi.org/10.1016/j.ejmp.2023.103189
Đorđević M, Fattori S, Petringa G, Ristić Fira A, Petrović I, Cuttone G, Cirrone GP. Computational approaches in the estimation of radiobiological damage for human-malignant cells irradiated with clinical proton and carbon beams. in Physica Medica. 2024;117:103189.
doi:10.1016/j.ejmp.2023.103189 .
Đorđević, Miloš, Fattori, Serena, Petringa, Giada, Ristić Fira, Aleksandra, Petrović, Ivan, Cuttone, Giacomo, Cirrone, G.A. Pablo, "Computational approaches in the estimation of radiobiological damage for human-malignant cells irradiated with clinical proton and carbon beams" in Physica Medica, 117 (2024):103189,
https://doi.org/10.1016/j.ejmp.2023.103189 . .
1

Simulation of DNA damage using Geant4-DNA: an overview of the “molecularDNA” example application

Chatzipapas, Konstantinos P.; Tran, Ngoc Hoang; Đorđević, Miloš; Živković, Sara; Zein, Sara; Shin, Wook-Geun; Sakata, Dousatsu; Lampe, Nathanael; Brown, Jeremy M. C.; Ristić-Fira, Aleksandra; Petrović, Ivan M.; Kyriakou, Ioanna; Emfietzoglou, Dimitris; Guatelli, Susanna; Incerti, Sebastien

(2023)

TY  - JOUR
AU  - Chatzipapas, Konstantinos P.
AU  - Tran, Ngoc Hoang
AU  - Đorđević, Miloš
AU  - Živković, Sara
AU  - Zein, Sara
AU  - Shin, Wook-Geun
AU  - Sakata, Dousatsu
AU  - Lampe, Nathanael
AU  - Brown, Jeremy M. C.
AU  - Ristić-Fira, Aleksandra
AU  - Petrović, Ivan M.
AU  - Kyriakou, Ioanna
AU  - Emfietzoglou, Dimitris
AU  - Guatelli, Susanna
AU  - Incerti, Sebastien
PY  - 2023
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10661
AB  - Purpose The scientific community shows great interest in the study of DNA damage induction, DNA damage repair, and the biological effects on cells and cellular systems after exposure to ionizing radiation. Several in silico methods have been proposed so far to study these mechanisms using Monte Carlo simulations. This study outlines a Geant4-DNA example application, named “molecularDNA”, publicly released in the 11.1 version of Geant4 (December 2022). Methods It was developed for novice Geant4 users and requires only a basic understanding of scripting languages to get started. The example includes two different DNA-scale geometries of biological targets, namely “cylinders” and “human cell”. This public version is based on a previous prototype and includes new features, such as: the adoption of a new approach for the modeling of the chemical stage, the use of the standard DNA damage format to describe radiation-induced DNA damage, and upgraded computational tools to estimate DNA damage response. Results Simulation data in terms of single-strand break and double-strand break yields were produced using each of the available geometries. The results were compared with the literature, to validate the example, producing less than 5% difference in all cases. Conclusion: “molecularDNA” is a prototype tool that can be applied in a wide variety of radiobiology studies, providing the scientific community with an open-access base for DNA damage quantification calculations. New DNA and cell geometries for the “molecularDNA” example will be included in future versions of Geant4-DNA.
T2  - Precision Radiation Oncology
T1  - Simulation of DNA damage using Geant4-DNA: an overview of the “molecularDNA” example application
VL  - 7
IS  - 1
SP  - 4
EP  - 14
DO  - 10.1002/pro6.1186
ER  - 
@article{
author = "Chatzipapas, Konstantinos P. and Tran, Ngoc Hoang and Đorđević, Miloš and Živković, Sara and Zein, Sara and Shin, Wook-Geun and Sakata, Dousatsu and Lampe, Nathanael and Brown, Jeremy M. C. and Ristić-Fira, Aleksandra and Petrović, Ivan M. and Kyriakou, Ioanna and Emfietzoglou, Dimitris and Guatelli, Susanna and Incerti, Sebastien",
year = "2023",
abstract = "Purpose The scientific community shows great interest in the study of DNA damage induction, DNA damage repair, and the biological effects on cells and cellular systems after exposure to ionizing radiation. Several in silico methods have been proposed so far to study these mechanisms using Monte Carlo simulations. This study outlines a Geant4-DNA example application, named “molecularDNA”, publicly released in the 11.1 version of Geant4 (December 2022). Methods It was developed for novice Geant4 users and requires only a basic understanding of scripting languages to get started. The example includes two different DNA-scale geometries of biological targets, namely “cylinders” and “human cell”. This public version is based on a previous prototype and includes new features, such as: the adoption of a new approach for the modeling of the chemical stage, the use of the standard DNA damage format to describe radiation-induced DNA damage, and upgraded computational tools to estimate DNA damage response. Results Simulation data in terms of single-strand break and double-strand break yields were produced using each of the available geometries. The results were compared with the literature, to validate the example, producing less than 5% difference in all cases. Conclusion: “molecularDNA” is a prototype tool that can be applied in a wide variety of radiobiology studies, providing the scientific community with an open-access base for DNA damage quantification calculations. New DNA and cell geometries for the “molecularDNA” example will be included in future versions of Geant4-DNA.",
journal = "Precision Radiation Oncology",
title = "Simulation of DNA damage using Geant4-DNA: an overview of the “molecularDNA” example application",
volume = "7",
number = "1",
pages = "4-14",
doi = "10.1002/pro6.1186"
}
Chatzipapas, K. P., Tran, N. H., Đorđević, M., Živković, S., Zein, S., Shin, W., Sakata, D., Lampe, N., Brown, J. M. C., Ristić-Fira, A., Petrović, I. M., Kyriakou, I., Emfietzoglou, D., Guatelli, S.,& Incerti, S.. (2023). Simulation of DNA damage using Geant4-DNA: an overview of the “molecularDNA” example application. in Precision Radiation Oncology, 7(1), 4-14.
https://doi.org/10.1002/pro6.1186
Chatzipapas KP, Tran NH, Đorđević M, Živković S, Zein S, Shin W, Sakata D, Lampe N, Brown JMC, Ristić-Fira A, Petrović IM, Kyriakou I, Emfietzoglou D, Guatelli S, Incerti S. Simulation of DNA damage using Geant4-DNA: an overview of the “molecularDNA” example application. in Precision Radiation Oncology. 2023;7(1):4-14.
doi:10.1002/pro6.1186 .
Chatzipapas, Konstantinos P., Tran, Ngoc Hoang, Đorđević, Miloš, Živković, Sara, Zein, Sara, Shin, Wook-Geun, Sakata, Dousatsu, Lampe, Nathanael, Brown, Jeremy M. C., Ristić-Fira, Aleksandra, Petrović, Ivan M., Kyriakou, Ioanna, Emfietzoglou, Dimitris, Guatelli, Susanna, Incerti, Sebastien, "Simulation of DNA damage using Geant4-DNA: an overview of the “molecularDNA” example application" in Precision Radiation Oncology, 7, no. 1 (2023):4-14,
https://doi.org/10.1002/pro6.1186 . .
2
7
5

The effects of a selected methoxy substituted chalcone in human melanoma cells irradiated with γ-rays

Keta, Otilija D.; Petković, Vladana; Đorđević, Neda O.; Đorđević, Miloš; Ivković, Branka; Dobričić, Vladimir

(Kragujevac : Institute for Information Technologies, University of Kragujevac, 2023)

TY  - CONF
AU  - Keta, Otilija D.
AU  - Petković, Vladana
AU  - Đorđević, Neda O.
AU  - Đorđević, Miloš
AU  - Ivković, Branka
AU  - Dobričić, Vladimir
PY  - 2023
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/12088
AB  - Given the well-established potential of chalcones in modulating the response of cancer cells to therapeutic interventions, coupled with the growing imperative to enhance their biological attributes, the objective of this study was to synthesize a methoxy-substituted chalcone (OCH3) and assess its capacity to amplify the inhibitory effects of radiation in melanoma cells known for their resistance to radiotherapy. The A375 melanoma cells were subjected to a clinically relevant dose of 2 Gy gamma irradiation. OCH3 was employed either as a standalone treatment or in conjunction with irradiation. The obtained results unveiled the substantial radiosensitizing potential of OCH3 within this specific cell line. Our subsequent investigations will be designed to investigate the underlying mechanisms that contribute to the radiosensitizing properties of OCH3. Moreover, we intend to evaluate the efficacy of OCH3 against other types of radioresistant cancer cells. The presented data not only illuminates the enhanced therapeutic possibilities offered by OCH3 but also highlights its potential as a valuable agent in addressing a wider array of challenging malignancies.
PB  - Kragujevac : Institute for Information Technologies, University of Kragujevac
C3  - ICCBIKG 2023 : 2nd International Conference on Chemo and Bioinformatics : Book of Proceedings
T1  - The effects of a selected methoxy substituted chalcone in human melanoma cells irradiated with γ-rays
SP  - 471
EP  - 474
DO  - 10.46793/ICCBI23.471K
ER  - 
@conference{
author = "Keta, Otilija D. and Petković, Vladana and Đorđević, Neda O. and Đorđević, Miloš and Ivković, Branka and Dobričić, Vladimir",
year = "2023",
abstract = "Given the well-established potential of chalcones in modulating the response of cancer cells to therapeutic interventions, coupled with the growing imperative to enhance their biological attributes, the objective of this study was to synthesize a methoxy-substituted chalcone (OCH3) and assess its capacity to amplify the inhibitory effects of radiation in melanoma cells known for their resistance to radiotherapy. The A375 melanoma cells were subjected to a clinically relevant dose of 2 Gy gamma irradiation. OCH3 was employed either as a standalone treatment or in conjunction with irradiation. The obtained results unveiled the substantial radiosensitizing potential of OCH3 within this specific cell line. Our subsequent investigations will be designed to investigate the underlying mechanisms that contribute to the radiosensitizing properties of OCH3. Moreover, we intend to evaluate the efficacy of OCH3 against other types of radioresistant cancer cells. The presented data not only illuminates the enhanced therapeutic possibilities offered by OCH3 but also highlights its potential as a valuable agent in addressing a wider array of challenging malignancies.",
publisher = "Kragujevac : Institute for Information Technologies, University of Kragujevac",
journal = "ICCBIKG 2023 : 2nd International Conference on Chemo and Bioinformatics : Book of Proceedings",
title = "The effects of a selected methoxy substituted chalcone in human melanoma cells irradiated with γ-rays",
pages = "471-474",
doi = "10.46793/ICCBI23.471K"
}
Keta, O. D., Petković, V., Đorđević, N. O., Đorđević, M., Ivković, B.,& Dobričić, V.. (2023). The effects of a selected methoxy substituted chalcone in human melanoma cells irradiated with γ-rays. in ICCBIKG 2023 : 2nd International Conference on Chemo and Bioinformatics : Book of Proceedings
Kragujevac : Institute for Information Technologies, University of Kragujevac., 471-474.
https://doi.org/10.46793/ICCBI23.471K
Keta OD, Petković V, Đorđević NO, Đorđević M, Ivković B, Dobričić V. The effects of a selected methoxy substituted chalcone in human melanoma cells irradiated with γ-rays. in ICCBIKG 2023 : 2nd International Conference on Chemo and Bioinformatics : Book of Proceedings. 2023;:471-474.
doi:10.46793/ICCBI23.471K .
Keta, Otilija D., Petković, Vladana, Đorđević, Neda O., Đorđević, Miloš, Ivković, Branka, Dobričić, Vladimir, "The effects of a selected methoxy substituted chalcone in human melanoma cells irradiated with γ-rays" in ICCBIKG 2023 : 2nd International Conference on Chemo and Bioinformatics : Book of Proceedings (2023):471-474,
https://doi.org/10.46793/ICCBI23.471K . .

The CMS High Level Trigger System

Đorđević, Miloš

(2023)

TY  - CONF
AU  - Đorđević, Miloš
PY  - 2023
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/11934
AB  - The CMS experiment at CERN uses a two-level triggering system that is composed of the Level-1 (L1), instrumented by custom-designed electronics with an output rate of 100 kHz, and the High Level Trigger (HLT), a streamlined version of the offline software reconstruction running on a computer farm, with around 1.5 kHz of physics rate stored for further analysis. New trigger algorithms and also new features, as well as an optimized trigger menu at the HLT, are essential in order to be able to successfully record events at higher data loads due to increasing luminosity and pileup at the LHC in Run 3 which has just started. Many measurements and searches will profit from the updates implemented in the CMS trigger. The highlights of Run 2 CMS trigger results will be presented in this proceedings, together with improvements for Run 3.
C3  - Proceedings of Science
T1  - The CMS High Level Trigger System
VL  - 427
SP  - 193246
DO  - 10.22323/1.427.0088
ER  - 
@conference{
author = "Đorđević, Miloš",
year = "2023",
abstract = "The CMS experiment at CERN uses a two-level triggering system that is composed of the Level-1 (L1), instrumented by custom-designed electronics with an output rate of 100 kHz, and the High Level Trigger (HLT), a streamlined version of the offline software reconstruction running on a computer farm, with around 1.5 kHz of physics rate stored for further analysis. New trigger algorithms and also new features, as well as an optimized trigger menu at the HLT, are essential in order to be able to successfully record events at higher data loads due to increasing luminosity and pileup at the LHC in Run 3 which has just started. Many measurements and searches will profit from the updates implemented in the CMS trigger. The highlights of Run 2 CMS trigger results will be presented in this proceedings, together with improvements for Run 3.",
journal = "Proceedings of Science",
title = "The CMS High Level Trigger System",
volume = "427",
pages = "193246",
doi = "10.22323/1.427.0088"
}
Đorđević, M.. (2023). The CMS High Level Trigger System. in Proceedings of Science, 427, 193246.
https://doi.org/10.22323/1.427.0088
Đorđević M. The CMS High Level Trigger System. in Proceedings of Science. 2023;427:193246.
doi:10.22323/1.427.0088 .
Đorđević, Miloš, "The CMS High Level Trigger System" in Proceedings of Science, 427 (2023):193246,
https://doi.org/10.22323/1.427.0088 . .

Geant4-DNA simulation of human cancer cells irradiation with helium ion beams

Chatzipapas, Konstantinos; Đorđević, Miloš; Živković, Sara; Tran, Ngoc Hoang; Lampe, Nathanael; Sakata, Dousatsu; Petrović, Ivan; Ristić-Fira, Aleksandra; Shin, Wook-Geun; Zein, Sara; Brown, Jeremy M.C.; Kyriakou, Ioanna; Emfietzoglou, Dimitris; Guatelli, Susanna; Incerti, Sebastien

(2023)

TY  - JOUR
AU  - Chatzipapas, Konstantinos
AU  - Đorđević, Miloš
AU  - Živković, Sara
AU  - Tran, Ngoc Hoang
AU  - Lampe, Nathanael
AU  - Sakata, Dousatsu
AU  - Petrović, Ivan
AU  - Ristić-Fira, Aleksandra
AU  - Shin, Wook-Geun
AU  - Zein, Sara
AU  - Brown, Jeremy M.C.
AU  - Kyriakou, Ioanna
AU  - Emfietzoglou, Dimitris
AU  - Guatelli, Susanna
AU  - Incerti, Sebastien
PY  - 2023
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/11202
AB  - Purpose: This study aimed to develop a computational environment for the accurate simulation of human cancer cell irradiation using Geant4-DNA. New cell geometrical models were developed and irradiated by alpha particle beams to induce DNA damage. The proposed approach may help further investigation of the benefits of external alpha irradiation therapy. Methods: The Geant4-DNA Monte Carlo (MC) toolkit allows the simulation of cancer cell geometries that can be combined with accurate modelling of physical, physicochemical and chemical stages of liquid water irradiation, including radiolytic processes. Geant4-DNA is used to calculate direct and non-direct DNA damage yields, such as single and double strand breaks, produced by the deposition of energy or by the interaction of DNA with free radicals. Results: In this study, the “molecularDNA” example application of Geant4-DNA was used to quantify early DNA damage in human cancer cells upon irradiation with alpha particle beams, as a function of linear energy transfer (LET). The MC simulation results are compared to experimental data, as well as previously published simulation data. The simulation results agree well with the experimental data on DSB yields in the lower LET range, while the experimental data on DSB yields are lower than the results obtained with the “molecularDNA” example in the higher LET range. Conclusion: This study explored and demonstrated the possibilities of the Geant4-DNA toolkit together with the “molecularDNA” example to simulate the helium beam irradiation of cancer cell lines, to quantify the early DNA damage, or even the following DNA damage response. © 2023 Associazione Italiana di Fisica Medica e Sanitaria
T2  - Physica Medica
T1  - Geant4-DNA simulation of human cancer cells irradiation with helium ion beams
VL  - 112
DO  - 10.1016/j.ejmp.2023.102613
ER  - 
@article{
author = "Chatzipapas, Konstantinos and Đorđević, Miloš and Živković, Sara and Tran, Ngoc Hoang and Lampe, Nathanael and Sakata, Dousatsu and Petrović, Ivan and Ristić-Fira, Aleksandra and Shin, Wook-Geun and Zein, Sara and Brown, Jeremy M.C. and Kyriakou, Ioanna and Emfietzoglou, Dimitris and Guatelli, Susanna and Incerti, Sebastien",
year = "2023",
abstract = "Purpose: This study aimed to develop a computational environment for the accurate simulation of human cancer cell irradiation using Geant4-DNA. New cell geometrical models were developed and irradiated by alpha particle beams to induce DNA damage. The proposed approach may help further investigation of the benefits of external alpha irradiation therapy. Methods: The Geant4-DNA Monte Carlo (MC) toolkit allows the simulation of cancer cell geometries that can be combined with accurate modelling of physical, physicochemical and chemical stages of liquid water irradiation, including radiolytic processes. Geant4-DNA is used to calculate direct and non-direct DNA damage yields, such as single and double strand breaks, produced by the deposition of energy or by the interaction of DNA with free radicals. Results: In this study, the “molecularDNA” example application of Geant4-DNA was used to quantify early DNA damage in human cancer cells upon irradiation with alpha particle beams, as a function of linear energy transfer (LET). The MC simulation results are compared to experimental data, as well as previously published simulation data. The simulation results agree well with the experimental data on DSB yields in the lower LET range, while the experimental data on DSB yields are lower than the results obtained with the “molecularDNA” example in the higher LET range. Conclusion: This study explored and demonstrated the possibilities of the Geant4-DNA toolkit together with the “molecularDNA” example to simulate the helium beam irradiation of cancer cell lines, to quantify the early DNA damage, or even the following DNA damage response. © 2023 Associazione Italiana di Fisica Medica e Sanitaria",
journal = "Physica Medica",
title = "Geant4-DNA simulation of human cancer cells irradiation with helium ion beams",
volume = "112",
doi = "10.1016/j.ejmp.2023.102613"
}
Chatzipapas, K., Đorđević, M., Živković, S., Tran, N. H., Lampe, N., Sakata, D., Petrović, I., Ristić-Fira, A., Shin, W., Zein, S., Brown, J. M.C., Kyriakou, I., Emfietzoglou, D., Guatelli, S.,& Incerti, S.. (2023). Geant4-DNA simulation of human cancer cells irradiation with helium ion beams. in Physica Medica, 112.
https://doi.org/10.1016/j.ejmp.2023.102613
Chatzipapas K, Đorđević M, Živković S, Tran NH, Lampe N, Sakata D, Petrović I, Ristić-Fira A, Shin W, Zein S, Brown JM, Kyriakou I, Emfietzoglou D, Guatelli S, Incerti S. Geant4-DNA simulation of human cancer cells irradiation with helium ion beams. in Physica Medica. 2023;112.
doi:10.1016/j.ejmp.2023.102613 .
Chatzipapas, Konstantinos, Đorđević, Miloš, Živković, Sara, Tran, Ngoc Hoang, Lampe, Nathanael, Sakata, Dousatsu, Petrović, Ivan, Ristić-Fira, Aleksandra, Shin, Wook-Geun, Zein, Sara, Brown, Jeremy M.C., Kyriakou, Ioanna, Emfietzoglou, Dimitris, Guatelli, Susanna, Incerti, Sebastien, "Geant4-DNA simulation of human cancer cells irradiation with helium ion beams" in Physica Medica, 112 (2023),
https://doi.org/10.1016/j.ejmp.2023.102613 . .
2
1
1

The CMS Trigger System

Đorđević, Miloš; Collaboration, on behalf of the CMS

(2022)

TY  - JOUR
AU  - Đorđević, Miloš
AU  - Collaboration, on behalf of the CMS
PY  - 2022
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10555
AB  - The CMS experiment at CERN uses a two-stage triggering system composed of the Level-1 (L1), instrumented with custom-designed hardware boards with an output rate of 100 kHz, and the High Level Trigger (HLT), streamlined version of the offline software reconstruction that runs on the computing farm, allowing to store around 1.5 kHz of rate. New trigger algorithms and new features, as well as optimized trigger menus at both L1 and HLT are mandatory in order to be able to successfully record the events at higher data loads due to increasing luminosity and pileup at the LHC in Run 3. Many measurements and searches will profit from the updates implemented in the CMS trigger. The highlights of Run 2 CMS trigger results will be presented, together with the improvements for Run 3.
T2  - Journal of Physics: Conference Series
T1  - The CMS Trigger System
VL  - 2375
IS  - 1
SP  - 012003
DO  - 10.1088/1742-6596/2375/1/012003
ER  - 
@article{
author = "Đorđević, Miloš and Collaboration, on behalf of the CMS",
year = "2022",
abstract = "The CMS experiment at CERN uses a two-stage triggering system composed of the Level-1 (L1), instrumented with custom-designed hardware boards with an output rate of 100 kHz, and the High Level Trigger (HLT), streamlined version of the offline software reconstruction that runs on the computing farm, allowing to store around 1.5 kHz of rate. New trigger algorithms and new features, as well as optimized trigger menus at both L1 and HLT are mandatory in order to be able to successfully record the events at higher data loads due to increasing luminosity and pileup at the LHC in Run 3. Many measurements and searches will profit from the updates implemented in the CMS trigger. The highlights of Run 2 CMS trigger results will be presented, together with the improvements for Run 3.",
journal = "Journal of Physics: Conference Series",
title = "The CMS Trigger System",
volume = "2375",
number = "1",
pages = "012003",
doi = "10.1088/1742-6596/2375/1/012003"
}
Đorđević, M.,& Collaboration, o. b. o. t. C.. (2022). The CMS Trigger System. in Journal of Physics: Conference Series, 2375(1), 012003.
https://doi.org/10.1088/1742-6596/2375/1/012003
Đorđević M, Collaboration OBOTC. The CMS Trigger System. in Journal of Physics: Conference Series. 2022;2375(1):012003.
doi:10.1088/1742-6596/2375/1/012003 .
Đorđević, Miloš, Collaboration, on behalf of the CMS, "The CMS Trigger System" in Journal of Physics: Conference Series, 2375, no. 1 (2022):012003,
https://doi.org/10.1088/1742-6596/2375/1/012003 . .
1

A Geant4-DNA Evaluation of Radiation-Induced DNA Damage on a Human Fibroblast

Shin, Wook-Geun; Sakata, Dousatsu; Lampe, Nathanael; Belov, Oleg; Tran, Ngoc Hoang; Petrović, Ivan M.; Ristić-Fira, Aleksandra; Đorđević, Miloš; Bernal, Mario A.; Bordage, Marie-Claude; Francis, Ziad; Kyriakou, Ioanna; Perrot, Yann; Sasaki, Takashi; Villagrasa, Carmen; Guatelli, Susanna; Breton, Vincent; Emfietzoglou, Dimitris; Incerti, Sebastien

(2021)

TY  - JOUR
AU  - Shin, Wook-Geun
AU  - Sakata, Dousatsu
AU  - Lampe, Nathanael
AU  - Belov, Oleg
AU  - Tran, Ngoc Hoang
AU  - Petrović, Ivan M.
AU  - Ristić-Fira, Aleksandra
AU  - Đorđević, Miloš
AU  - Bernal, Mario A.
AU  - Bordage, Marie-Claude
AU  - Francis, Ziad
AU  - Kyriakou, Ioanna
AU  - Perrot, Yann
AU  - Sasaki, Takashi
AU  - Villagrasa, Carmen
AU  - Guatelli, Susanna
AU  - Breton, Vincent
AU  - Emfietzoglou, Dimitris
AU  - Incerti, Sebastien
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9961
AB  - Accurately modeling the radiobiological mechanisms responsible for the induction of DNA damage remains a major scientific challenge, particularly for understanding the effects of low doses of ionizing radiation on living beings, such as the induction of carcinogenesis. A computational approach based on the Monte Carlo technique to simulate track structures in a biological medium is currently the most reliable method for calculating the early effects induced by ionizing radiation on DNA, the primary cellular target of such effects. The Geant4-DNA Monte Carlo toolkit can simulate not only the physical, but also the physico-chemical and chemical stages of water radiolysis. These stages can be combined with simplified geometric models of biological targets, such as DNA, to assess direct and indirect early DNA damage. In this study, DNA damage induced in a human fibroblast cell was evaluated using Geant4-DNA as a function of incident particle type (gammas, protons, and alphas) and energy. The resulting double-strand break yields as a function of linear energy transfer closely reproduced recent experimental data. Other quantities, such as fragment length distribution, scavengeable damage fraction, and time evolution of damage within an analytical repair model also supported the plausibility of predicting DNA damage using Geant4-DNA.The complete simulation chain application “molecularDNA”, an example for users of Geant4-DNA, will soon be distributed through Geant4.
T2  - Cancers
T2  - Cancers
T1  - A Geant4-DNA Evaluation of Radiation-Induced DNA Damage on a Human Fibroblast
VL  - 13
IS  - 19
SP  - 4940
DO  - 10.3390/cancers13194940
ER  - 
@article{
author = "Shin, Wook-Geun and Sakata, Dousatsu and Lampe, Nathanael and Belov, Oleg and Tran, Ngoc Hoang and Petrović, Ivan M. and Ristić-Fira, Aleksandra and Đorđević, Miloš and Bernal, Mario A. and Bordage, Marie-Claude and Francis, Ziad and Kyriakou, Ioanna and Perrot, Yann and Sasaki, Takashi and Villagrasa, Carmen and Guatelli, Susanna and Breton, Vincent and Emfietzoglou, Dimitris and Incerti, Sebastien",
year = "2021",
abstract = "Accurately modeling the radiobiological mechanisms responsible for the induction of DNA damage remains a major scientific challenge, particularly for understanding the effects of low doses of ionizing radiation on living beings, such as the induction of carcinogenesis. A computational approach based on the Monte Carlo technique to simulate track structures in a biological medium is currently the most reliable method for calculating the early effects induced by ionizing radiation on DNA, the primary cellular target of such effects. The Geant4-DNA Monte Carlo toolkit can simulate not only the physical, but also the physico-chemical and chemical stages of water radiolysis. These stages can be combined with simplified geometric models of biological targets, such as DNA, to assess direct and indirect early DNA damage. In this study, DNA damage induced in a human fibroblast cell was evaluated using Geant4-DNA as a function of incident particle type (gammas, protons, and alphas) and energy. The resulting double-strand break yields as a function of linear energy transfer closely reproduced recent experimental data. Other quantities, such as fragment length distribution, scavengeable damage fraction, and time evolution of damage within an analytical repair model also supported the plausibility of predicting DNA damage using Geant4-DNA.The complete simulation chain application “molecularDNA”, an example for users of Geant4-DNA, will soon be distributed through Geant4.",
journal = "Cancers, Cancers",
title = "A Geant4-DNA Evaluation of Radiation-Induced DNA Damage on a Human Fibroblast",
volume = "13",
number = "19",
pages = "4940",
doi = "10.3390/cancers13194940"
}
Shin, W., Sakata, D., Lampe, N., Belov, O., Tran, N. H., Petrović, I. M., Ristić-Fira, A., Đorđević, M., Bernal, M. A., Bordage, M., Francis, Z., Kyriakou, I., Perrot, Y., Sasaki, T., Villagrasa, C., Guatelli, S., Breton, V., Emfietzoglou, D.,& Incerti, S.. (2021). A Geant4-DNA Evaluation of Radiation-Induced DNA Damage on a Human Fibroblast. in Cancers, 13(19), 4940.
https://doi.org/10.3390/cancers13194940
Shin W, Sakata D, Lampe N, Belov O, Tran NH, Petrović IM, Ristić-Fira A, Đorđević M, Bernal MA, Bordage M, Francis Z, Kyriakou I, Perrot Y, Sasaki T, Villagrasa C, Guatelli S, Breton V, Emfietzoglou D, Incerti S. A Geant4-DNA Evaluation of Radiation-Induced DNA Damage on a Human Fibroblast. in Cancers. 2021;13(19):4940.
doi:10.3390/cancers13194940 .
Shin, Wook-Geun, Sakata, Dousatsu, Lampe, Nathanael, Belov, Oleg, Tran, Ngoc Hoang, Petrović, Ivan M., Ristić-Fira, Aleksandra, Đorđević, Miloš, Bernal, Mario A., Bordage, Marie-Claude, Francis, Ziad, Kyriakou, Ioanna, Perrot, Yann, Sasaki, Takashi, Villagrasa, Carmen, Guatelli, Susanna, Breton, Vincent, Emfietzoglou, Dimitris, Incerti, Sebastien, "A Geant4-DNA Evaluation of Radiation-Induced DNA Damage on a Human Fibroblast" in Cancers, 13, no. 19 (2021):4940,
https://doi.org/10.3390/cancers13194940 . .
12
11

Measurement of the Wγ Production Cross Section in Proton-Proton Collisions at s=13 TeV and Constraints on Effective Field Theory Coefficients

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan; Milošević, Vukašin

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J. W.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
AU  - Milošević, Vukašin
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9868
AB  - A fiducial cross section for Wγ production in proton-proton collisions is measured at a center-of-mass energy of 13 TeV in 137  fb−1 of data collected using the CMS detector at the LHC. The W→eν and μν decay modes are used in a maximum-likelihood fit to the lepton-photon invariant mass distribution to extract the combined cross section. The measured cross section is compared with theoretical expectations at next-to-leading order in quantum chromodynamics. In addition, 95% confidence level intervals are reported for anomalous triple-gauge couplings within the framework of effective field theory.
T2  - Physical Review Letters
T1  - Measurement of the Wγ Production Cross Section in Proton-Proton Collisions at s=13 TeV and Constraints on Effective Field Theory Coefficients
VL  - 126
SP  - 252002
DO  - 10.1103/PhysRevLett.126.252002
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Andrejkovic, J. W. and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan and Milošević, Vukašin",
year = "2021",
abstract = "A fiducial cross section for Wγ production in proton-proton collisions is measured at a center-of-mass energy of 13 TeV in 137  fb−1 of data collected using the CMS detector at the LHC. The W→eν and μν decay modes are used in a maximum-likelihood fit to the lepton-photon invariant mass distribution to extract the combined cross section. The measured cross section is compared with theoretical expectations at next-to-leading order in quantum chromodynamics. In addition, 95% confidence level intervals are reported for anomalous triple-gauge couplings within the framework of effective field theory.",
journal = "Physical Review Letters",
title = "Measurement of the Wγ Production Cross Section in Proton-Proton Collisions at s=13 TeV and Constraints on Effective Field Theory Coefficients",
volume = "126",
pages = "252002",
doi = "10.1103/PhysRevLett.126.252002"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P., Milošević, J.,& Milošević, V.. (2021). Measurement of the Wγ Production Cross Section in Proton-Proton Collisions at s=13 TeV and Constraints on Effective Field Theory Coefficients. in Physical Review Letters, 126, 252002.
https://doi.org/10.1103/PhysRevLett.126.252002
Sirunyan AM, Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J, Milošević V. Measurement of the Wγ Production Cross Section in Proton-Proton Collisions at s=13 TeV and Constraints on Effective Field Theory Coefficients. in Physical Review Letters. 2021;126:252002.
doi:10.1103/PhysRevLett.126.252002 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Milošević, Vukašin, "Measurement of the Wγ Production Cross Section in Proton-Proton Collisions at s=13 TeV and Constraints on Effective Field Theory Coefficients" in Physical Review Letters, 126 (2021):252002,
https://doi.org/10.1103/PhysRevLett.126.252002 . .
11
8
14

Observation of a New Excited Beauty Strange Baryon Decaying to Ξb−π+π−

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan; Milošević, Vukašin

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J. W.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
AU  - Milošević, Vukašin
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9867
AB  - The Ξb−π+π− invariant mass spectrum is investigated with an event sample of proton-proton collisions at s=13  TeV, collected by the CMS experiment at the LHC in 2016–2018 and corresponding to an integrated luminosity of 140  fb−1. The ground state Ξb− is reconstructed via its decays to J/ψΞ− and J/ψΛK−. A narrow resonance, labeled Ξb(6100)−, is observed at a Ξb−π+π− invariant mass of 6100.3±0.2(stat)±0.1(syst)±0.6(Ξb−)  MeV, where the last uncertainty reflects the precision of the Ξb− baryon mass. The upper limit on the Ξb(6100)− natural width is determined to be 1.9  MeV at 95% confidence level. The low Ξb(6100)− signal yield observed in data does not allow a measurement of the quantum numbers of the new state. However, following analogies with the established excited Ξc baryon states, the new Ξb(6100)− resonance and its decay sequence are consistent with the orbitally excited Ξb− baryon, with spin and parity quantum numbers JP=3/2−.
T2  - Physical Review Letters
T1  - Observation of a New Excited Beauty Strange Baryon Decaying to Ξb−π+π−
VL  - 126
DO  - 10.1103/PhysRevLett.126.252003
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Andrejkovic, J. W. and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan and Milošević, Vukašin",
year = "2021",
abstract = "The Ξb−π+π− invariant mass spectrum is investigated with an event sample of proton-proton collisions at s=13  TeV, collected by the CMS experiment at the LHC in 2016–2018 and corresponding to an integrated luminosity of 140  fb−1. The ground state Ξb− is reconstructed via its decays to J/ψΞ− and J/ψΛK−. A narrow resonance, labeled Ξb(6100)−, is observed at a Ξb−π+π− invariant mass of 6100.3±0.2(stat)±0.1(syst)±0.6(Ξb−)  MeV, where the last uncertainty reflects the precision of the Ξb− baryon mass. The upper limit on the Ξb(6100)− natural width is determined to be 1.9  MeV at 95% confidence level. The low Ξb(6100)− signal yield observed in data does not allow a measurement of the quantum numbers of the new state. However, following analogies with the established excited Ξc baryon states, the new Ξb(6100)− resonance and its decay sequence are consistent with the orbitally excited Ξb− baryon, with spin and parity quantum numbers JP=3/2−.",
journal = "Physical Review Letters",
title = "Observation of a New Excited Beauty Strange Baryon Decaying to Ξb−π+π−",
volume = "126",
doi = "10.1103/PhysRevLett.126.252003"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P., Milošević, J.,& Milošević, V.. (2021). Observation of a New Excited Beauty Strange Baryon Decaying to Ξb−π+π−. in Physical Review Letters, 126.
https://doi.org/10.1103/PhysRevLett.126.252003
Sirunyan AM, Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J, Milošević V. Observation of a New Excited Beauty Strange Baryon Decaying to Ξb−π+π−. in Physical Review Letters. 2021;126.
doi:10.1103/PhysRevLett.126.252003 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Milošević, Vukašin, "Observation of a New Excited Beauty Strange Baryon Decaying to Ξb−π+π−" in Physical Review Letters, 126 (2021),
https://doi.org/10.1103/PhysRevLett.126.252003 . .
18
22
2
28

First measurement of large area jet transverse momentum spectra in heavy-ion collisions

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Ambrogi, F.; Bergauer, T.; Adžić, Petar; Ćirković, Predrag; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan; Stojanović, Milan

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Ambrogi, F.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Ćirković, Predrag
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
AU  - Stojanović, Milan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9864
AB  - Jet production in lead-lead (PbPb) and proton-proton (pp) collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV is studied with the CMS detector at the LHC, using PbPb and pp data samples corresponding to integrated luminosities of 404 μb −1 and 27.4 pb −1, respectively. Jets with different areas are reconstructed using the anti-k T algorithm by varying the distance parameter R. The measurements are performed using jets with transverse momenta (p T) greater than 200 GeV and in a pseudorapidity range of |η| < 2. To reveal the medium modification of the jet spectra in PbPb collisions, the properly normalized ratio of spectra from PbPb and pp data is used to extract jet nuclear modification factors as functions of the PbPb collision centrality, p T and, for the first time, as a function of R up to 1.0. For the most central collisions, a strong suppression is observed for high-p T jets reconstructed with all distance parameters, implying that a significant amount of jet energy is scattered to large angles. The dependence of jet suppression on R is expected to be sensitive to both the jet energy loss mechanism and the medium response, and so the data are compared to several modern event generators and analytic calculations. The models considered do not fully reproduce the data.
T2  - Journal of High Energy Physics
T1  - First measurement of large area jet transverse momentum spectra in heavy-ion collisions
VL  - 2021
IS  - 5
SP  - 284
DO  - 10.1007/JHEP05(2021)284
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Ambrogi, F. and Bergauer, T. and Adžić, Petar and Ćirković, Predrag and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan and Stojanović, Milan",
year = "2021",
abstract = "Jet production in lead-lead (PbPb) and proton-proton (pp) collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV is studied with the CMS detector at the LHC, using PbPb and pp data samples corresponding to integrated luminosities of 404 μb −1 and 27.4 pb −1, respectively. Jets with different areas are reconstructed using the anti-k T algorithm by varying the distance parameter R. The measurements are performed using jets with transverse momenta (p T) greater than 200 GeV and in a pseudorapidity range of |η| < 2. To reveal the medium modification of the jet spectra in PbPb collisions, the properly normalized ratio of spectra from PbPb and pp data is used to extract jet nuclear modification factors as functions of the PbPb collision centrality, p T and, for the first time, as a function of R up to 1.0. For the most central collisions, a strong suppression is observed for high-p T jets reconstructed with all distance parameters, implying that a significant amount of jet energy is scattered to large angles. The dependence of jet suppression on R is expected to be sensitive to both the jet energy loss mechanism and the medium response, and so the data are compared to several modern event generators and analytic calculations. The models considered do not fully reproduce the data.",
journal = "Journal of High Energy Physics",
title = "First measurement of large area jet transverse momentum spectra in heavy-ion collisions",
volume = "2021",
number = "5",
pages = "284",
doi = "10.1007/JHEP05(2021)284"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Adžić, P., Ćirković, P., Đorđević, M., Milenović, P., Milošević, J.,& Stojanović, M.. (2021). First measurement of large area jet transverse momentum spectra in heavy-ion collisions. in Journal of High Energy Physics, 2021(5), 284.
https://doi.org/10.1007/JHEP05(2021)284
Sirunyan AM, Tumasyan A, Adam W, Ambrogi F, Bergauer T, Adžić P, Ćirković P, Đorđević M, Milenović P, Milošević J, Stojanović M. First measurement of large area jet transverse momentum spectra in heavy-ion collisions. in Journal of High Energy Physics. 2021;2021(5):284.
doi:10.1007/JHEP05(2021)284 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Adžić, Petar, Ćirković, Predrag, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Stojanović, Milan, "First measurement of large area jet transverse momentum spectra in heavy-ion collisions" in Journal of High Energy Physics, 2021, no. 5 (2021):284,
https://doi.org/10.1007/JHEP05(2021)284 . .
6
18
2
22

Study of Drell-Yan dimuon production in proton-lead collisions at √sNN = 8.16 TeV

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Ambrogi, F.; Bergauer, T.; Adžić, Petar; Ćirković, Predrag; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Ambrogi, F.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Ćirković, Predrag
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9862
AB  - Differential cross sections for the Drell-Yan process, including Z boson production, using the dimuon decay channel are measured in proton-lead (pPb) collisions at a nucleon-nucleon centre-of-mass energy of 8.16 TeV. A data sample recorded with the CMS detector at the LHC is used, corresponding to an integrated luminosity of 173 nb −1. The differential cross section as a function of the dimuon mass is measured in the range 15–600 GeV, for the first time in proton-nucleus collisions. It is also reported as a function of dimuon rapidity over the mass ranges 15–60 GeV and 60–120 GeV, and ratios for the p-going over the Pb-going beam directions are built. In both mass ranges, the differential cross sections as functions of the dimuon transverse momentum p T and of a geometric variable ϕ * are measured, where ϕ * highly correlates with p T but is determined with higher precision. In the Z mass region, the rapidity dependence of the data indicate a modification of the distribution of partons within a lead nucleus as compared to the proton case. The data are more precise than predictions based upon current models of parton distributions.
T2  - Journal of High Energy Physics
T1  - Study of Drell-Yan dimuon production in proton-lead collisions at √sNN = 8.16 TeV
VL  - 2021
IS  - 5
SP  - 182
DO  - 10.1007/JHEP05(2021)182
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Ambrogi, F. and Bergauer, T. and Adžić, Petar and Ćirković, Predrag and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan",
year = "2021",
abstract = "Differential cross sections for the Drell-Yan process, including Z boson production, using the dimuon decay channel are measured in proton-lead (pPb) collisions at a nucleon-nucleon centre-of-mass energy of 8.16 TeV. A data sample recorded with the CMS detector at the LHC is used, corresponding to an integrated luminosity of 173 nb −1. The differential cross section as a function of the dimuon mass is measured in the range 15–600 GeV, for the first time in proton-nucleus collisions. It is also reported as a function of dimuon rapidity over the mass ranges 15–60 GeV and 60–120 GeV, and ratios for the p-going over the Pb-going beam directions are built. In both mass ranges, the differential cross sections as functions of the dimuon transverse momentum p T and of a geometric variable ϕ * are measured, where ϕ * highly correlates with p T but is determined with higher precision. In the Z mass region, the rapidity dependence of the data indicate a modification of the distribution of partons within a lead nucleus as compared to the proton case. The data are more precise than predictions based upon current models of parton distributions.",
journal = "Journal of High Energy Physics",
title = "Study of Drell-Yan dimuon production in proton-lead collisions at √sNN = 8.16 TeV",
volume = "2021",
number = "5",
pages = "182",
doi = "10.1007/JHEP05(2021)182"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Adžić, P., Ćirković, P., Đorđević, M., Milenović, P.,& Milošević, J.. (2021). Study of Drell-Yan dimuon production in proton-lead collisions at √sNN = 8.16 TeV. in Journal of High Energy Physics, 2021(5), 182.
https://doi.org/10.1007/JHEP05(2021)182
Sirunyan AM, Tumasyan A, Adam W, Ambrogi F, Bergauer T, Adžić P, Ćirković P, Đorđević M, Milenović P, Milošević J. Study of Drell-Yan dimuon production in proton-lead collisions at √sNN = 8.16 TeV. in Journal of High Energy Physics. 2021;2021(5):182.
doi:10.1007/JHEP05(2021)182 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Adžić, Petar, Ćirković, Predrag, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, "Study of Drell-Yan dimuon production in proton-lead collisions at √sNN = 8.16 TeV" in Journal of High Energy Physics, 2021, no. 5 (2021):182,
https://doi.org/10.1007/JHEP05(2021)182 . .
3
3
5

Measurements of the differential cross sections of the production of Z + jets and γ + jets and of Z boson emission collinear with a jet in pp collisions at √s = 13 TeV

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Ambrogi, F.; Bergauer, T.; Adžić, Petar; Ćirković, Predrag; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Ambrogi, F.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Ćirković, Predrag
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9856
AB  - Measurements of the differential cross sections of Z + jets and γ + jets production, and their ratio, are presented as a function of the boson transverse momentum. Measurements are also presented of the angular distribution between the Z boson and the closest jet. The analysis is based on pp collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb −1 recorded by the CMS experiment at the LHC. The results, corrected for detector effects, are compared with various theoretical predictions. In general, the predictions at higher orders in perturbation theory show better agreement with the measurements. This work provides the first measurement of the ratio of the differential cross sections of Z + jets and γ + jets production at 13 TeV, as well as the first direct measurement of Z bosons emitted collinearly with a jet.
T2  - Journal of High Energy Physics
T1  - Measurements of the differential cross sections of the production of Z + jets and γ + jets and of Z boson emission collinear with a jet in pp collisions at √s = 13 TeV
VL  - 2021
IS  - 5
SP  - 285
DO  - 10.1007/JHEP05(2021)285
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Ambrogi, F. and Bergauer, T. and Adžić, Petar and Ćirković, Predrag and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan",
year = "2021",
abstract = "Measurements of the differential cross sections of Z + jets and γ + jets production, and their ratio, are presented as a function of the boson transverse momentum. Measurements are also presented of the angular distribution between the Z boson and the closest jet. The analysis is based on pp collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb −1 recorded by the CMS experiment at the LHC. The results, corrected for detector effects, are compared with various theoretical predictions. In general, the predictions at higher orders in perturbation theory show better agreement with the measurements. This work provides the first measurement of the ratio of the differential cross sections of Z + jets and γ + jets production at 13 TeV, as well as the first direct measurement of Z bosons emitted collinearly with a jet.",
journal = "Journal of High Energy Physics",
title = "Measurements of the differential cross sections of the production of Z + jets and γ + jets and of Z boson emission collinear with a jet in pp collisions at √s = 13 TeV",
volume = "2021",
number = "5",
pages = "285",
doi = "10.1007/JHEP05(2021)285"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Adžić, P., Ćirković, P., Đorđević, M., Milenović, P.,& Milošević, J.. (2021). Measurements of the differential cross sections of the production of Z + jets and γ + jets and of Z boson emission collinear with a jet in pp collisions at √s = 13 TeV. in Journal of High Energy Physics, 2021(5), 285.
https://doi.org/10.1007/JHEP05(2021)285
Sirunyan AM, Tumasyan A, Adam W, Ambrogi F, Bergauer T, Adžić P, Ćirković P, Đorđević M, Milenović P, Milošević J. Measurements of the differential cross sections of the production of Z + jets and γ + jets and of Z boson emission collinear with a jet in pp collisions at √s = 13 TeV. in Journal of High Energy Physics. 2021;2021(5):285.
doi:10.1007/JHEP05(2021)285 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Adžić, Petar, Ćirković, Predrag, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, "Measurements of the differential cross sections of the production of Z + jets and γ + jets and of Z boson emission collinear with a jet in pp collisions at √s = 13 TeV" in Journal of High Energy Physics, 2021, no. 5 (2021):285,
https://doi.org/10.1007/JHEP05(2021)285 . .
1
2
6

Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton–proton collisions at √s=13Te

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Andrejkovic, J.; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan; Milošević, Vukašin

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
AU  - Milošević, Vukašin
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9855
AB  - Production cross sections of the Higgs boson are measured in the  $${\mathrm{H}} \rightarrow {\mathrm{Z}} {\mathrm{Z}} \rightarrow 4\ell $$    H → Z Z → 4 ℓ     ( $$\ell ={\mathrm{e}},{{{\upmu }}_{\mathrm{}}^{\mathrm{}}} $$    ℓ = e ,  μ         ) decay channel. A data sample of proton–proton collisions at a center-of-mass energy of 13 $$\,\text {TeV}$$     TeV    , collected by the CMS detector at the LHC and corresponding to an integrated luminosity of 137 $$\,\text {fb}^{-1}$$      fb  - 1       is used. The signal strength modifier  $$\mu $$   μ   , defined as the ratio of the Higgs boson production rate in the  $$4\ell $$    4 ℓ     channel to the standard model (SM) expectation, is measured to be  $$\mu =0.94 \pm 0.07 \,\text {(stat)} ^{+0.09}_{-0.08} \,\text {(syst)} $$    μ = 0.94 ± 0.07   (stat)  - 0.08   + 0.09    (syst)     at a fixed value of  $$m_{{\mathrm{H}}} = 125.38\,\text {GeV} $$     m H  = 125.38  GeV    . The signal strength modifiers for the individual Higgs boson production modes are also reported. The inclusive fiducial cross section for the  $${\mathrm{H}} \rightarrow 4\ell $$    H → 4 ℓ     process is measured to be  $$2.84^{+0.23}_{-0.22} \,\text {(stat)} ^{+0.26}_{-0.21} \,\text {(syst)} \,\text {fb} $$    2 .  84  - 0.22   + 0.23     (stat)  - 0.21   + 0.26    (syst)  fb    , which is compatible with the SM prediction of  $$2.84 \pm 0.15 \,\text {fb} $$    2.84 ± 0.15  fb     for the same fiducial region. Differential cross sections as a function of the transverse momentum and rapidity of the Higgs boson, the number of associated jets, and the transverse momentum of the leading associated jet are measured. A new set of cross section measurements in mutually exclusive categories targeted to identify production mechanisms and kinematical features of the events is presented. The results are in agreement with the SM predictions.
T2  - European Physical Journal C. Particles and Fields
T1  - Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton–proton collisions at √s=13Te
VL  - 81
IS  - 6
SP  - 488
DO  - 10.1140/epjc/s10052-021-09200-x
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Andrejkovic, J. and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan and Milošević, Vukašin",
year = "2021",
abstract = "Production cross sections of the Higgs boson are measured in the  $${\mathrm{H}} \rightarrow {\mathrm{Z}} {\mathrm{Z}} \rightarrow 4\ell $$    H → Z Z → 4 ℓ     ( $$\ell ={\mathrm{e}},{{{\upmu }}_{\mathrm{}}^{\mathrm{}}} $$    ℓ = e ,  μ         ) decay channel. A data sample of proton–proton collisions at a center-of-mass energy of 13 $$\,\text {TeV}$$     TeV    , collected by the CMS detector at the LHC and corresponding to an integrated luminosity of 137 $$\,\text {fb}^{-1}$$      fb  - 1       is used. The signal strength modifier  $$\mu $$   μ   , defined as the ratio of the Higgs boson production rate in the  $$4\ell $$    4 ℓ     channel to the standard model (SM) expectation, is measured to be  $$\mu =0.94 \pm 0.07 \,\text {(stat)} ^{+0.09}_{-0.08} \,\text {(syst)} $$    μ = 0.94 ± 0.07   (stat)  - 0.08   + 0.09    (syst)     at a fixed value of  $$m_{{\mathrm{H}}} = 125.38\,\text {GeV} $$     m H  = 125.38  GeV    . The signal strength modifiers for the individual Higgs boson production modes are also reported. The inclusive fiducial cross section for the  $${\mathrm{H}} \rightarrow 4\ell $$    H → 4 ℓ     process is measured to be  $$2.84^{+0.23}_{-0.22} \,\text {(stat)} ^{+0.26}_{-0.21} \,\text {(syst)} \,\text {fb} $$    2 .  84  - 0.22   + 0.23     (stat)  - 0.21   + 0.26    (syst)  fb    , which is compatible with the SM prediction of  $$2.84 \pm 0.15 \,\text {fb} $$    2.84 ± 0.15  fb     for the same fiducial region. Differential cross sections as a function of the transverse momentum and rapidity of the Higgs boson, the number of associated jets, and the transverse momentum of the leading associated jet are measured. A new set of cross section measurements in mutually exclusive categories targeted to identify production mechanisms and kinematical features of the events is presented. The results are in agreement with the SM predictions.",
journal = "European Physical Journal C. Particles and Fields",
title = "Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton–proton collisions at √s=13Te",
volume = "81",
number = "6",
pages = "488",
doi = "10.1140/epjc/s10052-021-09200-x"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P., Milošević, J.,& Milošević, V.. (2021). Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton–proton collisions at √s=13Te. in European Physical Journal C. Particles and Fields, 81(6), 488.
https://doi.org/10.1140/epjc/s10052-021-09200-x
Sirunyan AM, Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J, Milošević V. Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton–proton collisions at √s=13Te. in European Physical Journal C. Particles and Fields. 2021;81(6):488.
doi:10.1140/epjc/s10052-021-09200-x .
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Milošević, Vukašin, "Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton–proton collisions at √s=13Te" in European Physical Journal C. Particles and Fields, 81, no. 6 (2021):488,
https://doi.org/10.1140/epjc/s10052-021-09200-x . .
2
27
6
50

Measurement of the Z boson differential production cross section using its invisible decay mode (Z → νν¯) in proton-proton collisions at √s = 13 TeV

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Bergauer, T.; Dragicevic, M.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Bergauer, T.
AU  - Dragicevic, M.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9854
AB  - Measurements of the total and differential fiducial cross sections for the Z boson decaying into two neutrinos are presented at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV. The data were collected by the CMS detector in 2016 and correspond to an integrated luminosity of 35.9 fb −1. In these measurements, events are selected containing an imbalance in transverse momentum and one or more energetic jets. The fiducial differential cross section is measured as a function of the Z boson transverse momentum. The results are combined with a previous measurement of charged-lepton decays of the Z boson. The measured total fiducial cross section for events with Z boson transverse momentum greater than 200 GeV is     3000  − 170   + 180     $$ {3000}_{-170}^{+180} $$  fb.
T2  - Journal of High Energy Physics
T1  - Measurement of the Z boson differential production cross section using its invisible decay mode (Z → νν¯) in proton-proton collisions at √s = 13 TeV
VL  - 2021
IS  - 5
SP  - 205
DO  - 10.1007/JHEP05(2021)205
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Bergauer, T. and Dragicevic, M. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan",
year = "2021",
abstract = "Measurements of the total and differential fiducial cross sections for the Z boson decaying into two neutrinos are presented at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV. The data were collected by the CMS detector in 2016 and correspond to an integrated luminosity of 35.9 fb −1. In these measurements, events are selected containing an imbalance in transverse momentum and one or more energetic jets. The fiducial differential cross section is measured as a function of the Z boson transverse momentum. The results are combined with a previous measurement of charged-lepton decays of the Z boson. The measured total fiducial cross section for events with Z boson transverse momentum greater than 200 GeV is     3000  − 170   + 180     $$ {3000}_{-170}^{+180} $$  fb.",
journal = "Journal of High Energy Physics",
title = "Measurement of the Z boson differential production cross section using its invisible decay mode (Z → νν¯) in proton-proton collisions at √s = 13 TeV",
volume = "2021",
number = "5",
pages = "205",
doi = "10.1007/JHEP05(2021)205"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Adžić, P., Đorđević, M., Milenović, P.,& Milošević, J.. (2021). Measurement of the Z boson differential production cross section using its invisible decay mode (Z → νν¯) in proton-proton collisions at √s = 13 TeV. in Journal of High Energy Physics, 2021(5), 205.
https://doi.org/10.1007/JHEP05(2021)205
Sirunyan AM, Tumasyan A, Adam W, Bergauer T, Dragicevic M, Adžić P, Đorđević M, Milenović P, Milošević J. Measurement of the Z boson differential production cross section using its invisible decay mode (Z → νν¯) in proton-proton collisions at √s = 13 TeV. in Journal of High Energy Physics. 2021;2021(5):205.
doi:10.1007/JHEP05(2021)205 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, "Measurement of the Z boson differential production cross section using its invisible decay mode (Z → νν¯) in proton-proton collisions at √s = 13 TeV" in Journal of High Energy Physics, 2021, no. 5 (2021):205,
https://doi.org/10.1007/JHEP05(2021)205 . .
4
3
6

Precision luminosity measurement in proton–proton collisions at √s=13TeV in 2015 and 2016 at CMS

Sirunyan, A M; Tumasyan, A.; Adam, W; Andrejkovic, J W; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan; Milošević, Vukašin

(2021)

TY  - JOUR
AU  - Sirunyan, A M
AU  - Tumasyan, A.
AU  - Adam, W
AU  - Andrejkovic, J W
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
AU  - Milošević, Vukašin
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10163
AB  - The measurement of the luminosity recorded by the CMS detector installed at LHC interaction point 5, using proton–proton collisions at s=13TeV in 2015 and 2016, is reported. The absolute luminosity scale is measured for individual bunch crossings using beam-separation scans (the van der Meer method), with a relative precision of 1.3 and 1.0% in 2015 and 2016, respectively. The dominant sources of uncertainty are related to residual differences between the measured beam positions and the ones provided by the operational settings of the LHC magnets, the factorizability of the proton bunch spatial density functions in the coordinates transverse to the beam direction, and the modeling of the effect of electromagnetic interactions among protons in the colliding bunches. When applying the van der Meer calibration to the entire run periods, the integrated luminosities when CMS was fully operational are 2.27 and 36.3 fb-1 in 2015 and 2016, with a relative precision of 1.6 and 1.2%, respectively. These are among the most precise luminosity measurements at bunched-beam hadron colliders.
T2  - European Physical Journal C. Particles and Fields
T1  - Precision luminosity measurement in proton–proton collisions at √s=13TeV in 2015 and 2016 at CMS
VL  - 81
IS  - 9
SP  - 800
DO  - 10.1140/epjc/s10052-021-09538-2
ER  - 
@article{
author = "Sirunyan, A M and Tumasyan, A. and Adam, W and Andrejkovic, J W and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan and Milošević, Vukašin",
year = "2021",
abstract = "The measurement of the luminosity recorded by the CMS detector installed at LHC interaction point 5, using proton–proton collisions at s=13TeV in 2015 and 2016, is reported. The absolute luminosity scale is measured for individual bunch crossings using beam-separation scans (the van der Meer method), with a relative precision of 1.3 and 1.0% in 2015 and 2016, respectively. The dominant sources of uncertainty are related to residual differences between the measured beam positions and the ones provided by the operational settings of the LHC magnets, the factorizability of the proton bunch spatial density functions in the coordinates transverse to the beam direction, and the modeling of the effect of electromagnetic interactions among protons in the colliding bunches. When applying the van der Meer calibration to the entire run periods, the integrated luminosities when CMS was fully operational are 2.27 and 36.3 fb-1 in 2015 and 2016, with a relative precision of 1.6 and 1.2%, respectively. These are among the most precise luminosity measurements at bunched-beam hadron colliders.",
journal = "European Physical Journal C. Particles and Fields",
title = "Precision luminosity measurement in proton–proton collisions at √s=13TeV in 2015 and 2016 at CMS",
volume = "81",
number = "9",
pages = "800",
doi = "10.1140/epjc/s10052-021-09538-2"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P., Milošević, J.,& Milošević, V.. (2021). Precision luminosity measurement in proton–proton collisions at √s=13TeV in 2015 and 2016 at CMS. in European Physical Journal C. Particles and Fields, 81(9), 800.
https://doi.org/10.1140/epjc/s10052-021-09538-2
Sirunyan AM, Tumasyan A, Adam W, Andrejkovic JW, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J, Milošević V. Precision luminosity measurement in proton–proton collisions at √s=13TeV in 2015 and 2016 at CMS. in European Physical Journal C. Particles and Fields. 2021;81(9):800.
doi:10.1140/epjc/s10052-021-09538-2 .
Sirunyan, A M, Tumasyan, A., Adam, W, Andrejkovic, J W, Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Milošević, Vukašin, "Precision luminosity measurement in proton–proton collisions at √s=13TeV in 2015 and 2016 at CMS" in European Physical Journal C. Particles and Fields, 81, no. 9 (2021):800,
https://doi.org/10.1140/epjc/s10052-021-09538-2 . .
2
88
7
120

Search for lepton-flavor violating decays of the Higgs boson in the μτ and eτ final states in proton-proton collisions at s =13 TeV

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J. W.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10045
AB  - A search is presented for lepton-flavor violating decays of the Higgs boson to μτ and eτ. The dataset corresponds to an integrated luminosity of 137 fb-1 collected at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV. No significant excess has been found, and the results are interpreted in terms of upper limits on lepton-flavor violating branching fractions of the Higgs boson. The observed (expected) upper limits on the branching fractions are, respectively, B(H→μτ)<0.15(0.15)% and B(H→eτ)<0.22(0.16)% at 95% confidence level.
T2  - Physical Review D
T1  - Search for lepton-flavor violating decays of the Higgs boson in the μτ and eτ final states in proton-proton collisions at s =13 TeV
VL  - 104
SP  - 032013
DO  - 10.1103/PhysRevD.104.032013
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Andrejkovic, J. W. and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan",
year = "2021",
abstract = "A search is presented for lepton-flavor violating decays of the Higgs boson to μτ and eτ. The dataset corresponds to an integrated luminosity of 137 fb-1 collected at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV. No significant excess has been found, and the results are interpreted in terms of upper limits on lepton-flavor violating branching fractions of the Higgs boson. The observed (expected) upper limits on the branching fractions are, respectively, B(H→μτ)<0.15(0.15)% and B(H→eτ)<0.22(0.16)% at 95% confidence level.",
journal = "Physical Review D",
title = "Search for lepton-flavor violating decays of the Higgs boson in the μτ and eτ final states in proton-proton collisions at s =13 TeV",
volume = "104",
pages = "032013",
doi = "10.1103/PhysRevD.104.032013"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P.,& Milošević, J.. (2021). Search for lepton-flavor violating decays of the Higgs boson in the μτ and eτ final states in proton-proton collisions at s =13 TeV. in Physical Review D, 104, 032013.
https://doi.org/10.1103/PhysRevD.104.032013
Sirunyan A, Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J. Search for lepton-flavor violating decays of the Higgs boson in the μτ and eτ final states in proton-proton collisions at s =13 TeV. in Physical Review D. 2021;104:032013.
doi:10.1103/PhysRevD.104.032013 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, "Search for lepton-flavor violating decays of the Higgs boson in the μτ and eτ final states in proton-proton collisions at s =13 TeV" in Physical Review D, 104 (2021):032013,
https://doi.org/10.1103/PhysRevD.104.032013 . .
2
27
2
41

Search for top squark production in fully hadronic final states in proton-proton collisions at s=13 TeV

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan; Milošević, Vukašin

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J. W.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
AU  - Milošević, Vukašin
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10044
AB  - A search for production of the supersymmetric partners of the top quark, top squarks, is presented. The search is based on proton-proton collision events containing multiple jets, no leptons, and large transverse momentum imbalance. The data were collected with the CMS detector at the CERN LHC at a center-of-mass energy of 13 TeV, and correspond to an integrated luminosity of 137  fb−1. The targeted signal production scenarios are direct and gluino-mediated top squark production, including scenarios in which the top squark and neutralino masses are nearly degenerate. The search utilizes novel algorithms based on deep neural networks that identify hadronically decaying top quarks and W bosons, which are expected in many of the targeted signal models. No statistically significant excess of events is observed relative to the expectation from the standard model, and limits on the top squark production cross section are obtained in the context of simplified supersymmetric models for various production and decay modes. Exclusion limits as high as 1310 GeV are established at the 95% confidence level on the mass of the top squark for direct top squark production models, and as high as 2260 GeV on the mass of the gluino for gluino-mediated top squark production models. These results represent a significant improvement over the results of previous searches for supersymmetry by CMS in the same final state.
T2  - Physical Review D
T1  - Search for top squark production in fully hadronic final states in proton-proton collisions at s=13  TeV
VL  - 104
SP  - 052001
DO  - 10.1103/PhysRevD.104.052001
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Andrejkovic, J. W. and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan and Milošević, Vukašin",
year = "2021",
abstract = "A search for production of the supersymmetric partners of the top quark, top squarks, is presented. The search is based on proton-proton collision events containing multiple jets, no leptons, and large transverse momentum imbalance. The data were collected with the CMS detector at the CERN LHC at a center-of-mass energy of 13 TeV, and correspond to an integrated luminosity of 137  fb−1. The targeted signal production scenarios are direct and gluino-mediated top squark production, including scenarios in which the top squark and neutralino masses are nearly degenerate. The search utilizes novel algorithms based on deep neural networks that identify hadronically decaying top quarks and W bosons, which are expected in many of the targeted signal models. No statistically significant excess of events is observed relative to the expectation from the standard model, and limits on the top squark production cross section are obtained in the context of simplified supersymmetric models for various production and decay modes. Exclusion limits as high as 1310 GeV are established at the 95% confidence level on the mass of the top squark for direct top squark production models, and as high as 2260 GeV on the mass of the gluino for gluino-mediated top squark production models. These results represent a significant improvement over the results of previous searches for supersymmetry by CMS in the same final state.",
journal = "Physical Review D",
title = "Search for top squark production in fully hadronic final states in proton-proton collisions at s=13  TeV",
volume = "104",
pages = "052001",
doi = "10.1103/PhysRevD.104.052001"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P., Milošević, J.,& Milošević, V.. (2021). Search for top squark production in fully hadronic final states in proton-proton collisions at s=13  TeV. in Physical Review D, 104, 052001.
https://doi.org/10.1103/PhysRevD.104.052001
Sirunyan A, Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J, Milošević V. Search for top squark production in fully hadronic final states in proton-proton collisions at s=13  TeV. in Physical Review D. 2021;104:052001.
doi:10.1103/PhysRevD.104.052001 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Milošević, Vukašin, "Search for top squark production in fully hadronic final states in proton-proton collisions at s=13  TeV" in Physical Review D, 104 (2021):052001,
https://doi.org/10.1103/PhysRevD.104.052001 . .
4
28
3
34

Constraints on the Initial State of Pb-Pb Collisions via Measurements of Z -Boson Yields and Azimuthal Anisotropy at sNN =5.02 TeV

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Ambrogi, F.; Bergauer, T.; Adžić, Petar; Ćirković, Predrag; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Ambrogi, F.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Ćirković, Predrag
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10043
AB  - The CMS experiment at the LHC has measured the differential cross sections of Z bosons decaying to pairs of leptons, as functions of transverse momentum and rapidity, in lead-lead collisions at a nucleon-nucleon center-of-mass energy of 5.02  TeV. The measured Z boson elliptic azimuthal anisotropy coefficient is compatible with zero, showing that Z bosons do not experience significant final-state interactions in the medium produced in the collision. Yields of Z bosons are compared to Glauber model predictions and are found to deviate from these expectations in peripheral collisions, indicating the presence of initial collision geometry and centrality selection effects. The precision of the measurement allows, for the first time, for a data-driven determination of the nucleon-nucleon integrated luminosity as a function of lead-lead centrality, thereby eliminating the need for its estimation based on a Glauber model.
T2  - Physical Review Letters
T1  - Constraints on the Initial State of Pb-Pb Collisions via Measurements of Z -Boson Yields and Azimuthal Anisotropy at sNN =5.02 TeV
VL  - 127
SP  - 102002
DO  - 10.1103/PhysRevLett.127.102002
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Ambrogi, F. and Bergauer, T. and Adžić, Petar and Ćirković, Predrag and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan",
year = "2021",
abstract = "The CMS experiment at the LHC has measured the differential cross sections of Z bosons decaying to pairs of leptons, as functions of transverse momentum and rapidity, in lead-lead collisions at a nucleon-nucleon center-of-mass energy of 5.02  TeV. The measured Z boson elliptic azimuthal anisotropy coefficient is compatible with zero, showing that Z bosons do not experience significant final-state interactions in the medium produced in the collision. Yields of Z bosons are compared to Glauber model predictions and are found to deviate from these expectations in peripheral collisions, indicating the presence of initial collision geometry and centrality selection effects. The precision of the measurement allows, for the first time, for a data-driven determination of the nucleon-nucleon integrated luminosity as a function of lead-lead centrality, thereby eliminating the need for its estimation based on a Glauber model.",
journal = "Physical Review Letters",
title = "Constraints on the Initial State of Pb-Pb Collisions via Measurements of Z -Boson Yields and Azimuthal Anisotropy at sNN =5.02 TeV",
volume = "127",
pages = "102002",
doi = "10.1103/PhysRevLett.127.102002"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Adžić, P., Ćirković, P., Đorđević, M., Milenović, P.,& Milošević, J.. (2021). Constraints on the Initial State of Pb-Pb Collisions via Measurements of Z -Boson Yields and Azimuthal Anisotropy at sNN =5.02 TeV. in Physical Review Letters, 127, 102002.
https://doi.org/10.1103/PhysRevLett.127.102002
Sirunyan A, Tumasyan A, Adam W, Ambrogi F, Bergauer T, Adžić P, Ćirković P, Đorđević M, Milenović P, Milošević J. Constraints on the Initial State of Pb-Pb Collisions via Measurements of Z -Boson Yields and Azimuthal Anisotropy at sNN =5.02 TeV. in Physical Review Letters. 2021;127:102002.
doi:10.1103/PhysRevLett.127.102002 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Adžić, Petar, Ćirković, Predrag, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, "Constraints on the Initial State of Pb-Pb Collisions via Measurements of Z -Boson Yields and Azimuthal Anisotropy at sNN =5.02 TeV" in Physical Review Letters, 127 (2021):102002,
https://doi.org/10.1103/PhysRevLett.127.102002 . .
2
5
1
7

Search for top squarks in final states with two top quarks and several light-flavor jets in proton-proton collisions at s =13 TeV

Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan; Milošević, Vukašin

(2021)

TY  - JOUR
AU  - Sirunyan, A. M.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J. W.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
AU  - Milošević, Vukašin
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10042
AB  - Many new physics models, including versions of supersymmetry characterized by R-parity violation (RPV), compressed mass spectra, long decay chains, or additional hidden sectors, predict the production of events with top quarks, low missing transverse momentum, and many additional quarks or gluons. The results of a search for new physics in events with two top quarks and additional jets are reported. The search is performed using events with at least seven jets and exactly one electron or muon. No requirement on missing transverse momentum is imposed. The study is based on a sample of proton-proton collisions at s=13TeV corresponding to 137  fb−1 of integrated luminosity collected with the CMS detector at the LHC in 2016–2018. The data are used to determine best fit values and upper limits on the cross section for pair production of top squarks in scenarios of RPV and stealth supersymmetry. Top squark masses up to 670 (870)  GeV are excluded at 95% confidence level for the RPV (stealth) scenario, and the maximum observed local signal significance is 2.8 standard deviations for the RPV scenario with top squark mass of 400  GeV.
T2  - Physical Review D
T1  - Search for top squarks in final states with two top quarks and several light-flavor jets in proton-proton collisions at s =13 TeV
VL  - 104
SP  - 032006
DO  - 10.1103/PhysRevD.104.032006
ER  - 
@article{
author = "Sirunyan, A. M. and Tumasyan, A. and Adam, W. and Andrejkovic, J. W. and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan and Milošević, Vukašin",
year = "2021",
abstract = "Many new physics models, including versions of supersymmetry characterized by R-parity violation (RPV), compressed mass spectra, long decay chains, or additional hidden sectors, predict the production of events with top quarks, low missing transverse momentum, and many additional quarks or gluons. The results of a search for new physics in events with two top quarks and additional jets are reported. The search is performed using events with at least seven jets and exactly one electron or muon. No requirement on missing transverse momentum is imposed. The study is based on a sample of proton-proton collisions at s=13TeV corresponding to 137  fb−1 of integrated luminosity collected with the CMS detector at the LHC in 2016–2018. The data are used to determine best fit values and upper limits on the cross section for pair production of top squarks in scenarios of RPV and stealth supersymmetry. Top squark masses up to 670 (870)  GeV are excluded at 95% confidence level for the RPV (stealth) scenario, and the maximum observed local signal significance is 2.8 standard deviations for the RPV scenario with top squark mass of 400  GeV.",
journal = "Physical Review D",
title = "Search for top squarks in final states with two top quarks and several light-flavor jets in proton-proton collisions at s =13 TeV",
volume = "104",
pages = "032006",
doi = "10.1103/PhysRevD.104.032006"
}
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P., Milošević, J.,& Milošević, V.. (2021). Search for top squarks in final states with two top quarks and several light-flavor jets in proton-proton collisions at s =13 TeV. in Physical Review D, 104, 032006.
https://doi.org/10.1103/PhysRevD.104.032006
Sirunyan A, Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J, Milošević V. Search for top squarks in final states with two top quarks and several light-flavor jets in proton-proton collisions at s =13 TeV. in Physical Review D. 2021;104:032006.
doi:10.1103/PhysRevD.104.032006 .
Sirunyan, A. M., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Milošević, Vukašin, "Search for top squarks in final states with two top quarks and several light-flavor jets in proton-proton collisions at s =13 TeV" in Physical Review D, 104 (2021):032006,
https://doi.org/10.1103/PhysRevD.104.032006 . .
2
7
1
14

Search for resonant and nonresonant new phenomena in high-mass dilepton final states at √s = 13 TeV

Sirunyan, A.; Tumasyan, A.; Adam, W.; Andrejkovic, J.; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan; Milošević, Vukašin

(2021)

TY  - JOUR
AU  - Sirunyan, A.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
AU  - Milošević, Vukašin
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10028
AB  - A search is presented for physics beyond the standard model (SM) using electron or muon pairs with high invariant mass. A data set of proton-proton collisions collected by the CMS experiment at the LHC at     s    $$ \sqrt{s} $$  = 13 TeV from 2016 to 2018 corresponding to a total integrated luminosity of up to 140 fb −1 is analyzed. No significant deviation is observed with respect to the SM background expectations. Upper limits are presented on the ratio of the product of the production cross section and the branching fraction to dileptons of a new narrow resonance to that of the Z boson. These provide the most stringent lower limits to date on the masses for various spin-1 particles, spin-2 gravitons in the Randall-Sundrum model, as well as spin-1 mediators between the SM and dark matter particles. Lower limits on the ultraviolet cutoff parameter are set both for four-fermion contact interactions and for the Arkani-Hamed, Dimopoulos, and Dvali model with large extra dimensions. Lepton flavor universality is tested at the TeV scale for the first time by comparing the dimuon and dielectron mass spectra. No significant deviation from the SM expectation of unity is observed.
T2  - Journal of High Energy Physics
T1  - Search for resonant and nonresonant new phenomena in high-mass dilepton final states at √s = 13 TeV
VL  - 2021
IS  - 7
SP  - 208
DO  - 10.1007/JHEP07(2021)208
ER  - 
@article{
author = "Sirunyan, A. and Tumasyan, A. and Adam, W. and Andrejkovic, J. and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan and Milošević, Vukašin",
year = "2021",
abstract = "A search is presented for physics beyond the standard model (SM) using electron or muon pairs with high invariant mass. A data set of proton-proton collisions collected by the CMS experiment at the LHC at     s    $$ \sqrt{s} $$  = 13 TeV from 2016 to 2018 corresponding to a total integrated luminosity of up to 140 fb −1 is analyzed. No significant deviation is observed with respect to the SM background expectations. Upper limits are presented on the ratio of the product of the production cross section and the branching fraction to dileptons of a new narrow resonance to that of the Z boson. These provide the most stringent lower limits to date on the masses for various spin-1 particles, spin-2 gravitons in the Randall-Sundrum model, as well as spin-1 mediators between the SM and dark matter particles. Lower limits on the ultraviolet cutoff parameter are set both for four-fermion contact interactions and for the Arkani-Hamed, Dimopoulos, and Dvali model with large extra dimensions. Lepton flavor universality is tested at the TeV scale for the first time by comparing the dimuon and dielectron mass spectra. No significant deviation from the SM expectation of unity is observed.",
journal = "Journal of High Energy Physics",
title = "Search for resonant and nonresonant new phenomena in high-mass dilepton final states at √s = 13 TeV",
volume = "2021",
number = "7",
pages = "208",
doi = "10.1007/JHEP07(2021)208"
}
Sirunyan, A., Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P., Milošević, J.,& Milošević, V.. (2021). Search for resonant and nonresonant new phenomena in high-mass dilepton final states at √s = 13 TeV. in Journal of High Energy Physics, 2021(7), 208.
https://doi.org/10.1007/JHEP07(2021)208
Sirunyan A, Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J, Milošević V. Search for resonant and nonresonant new phenomena in high-mass dilepton final states at √s = 13 TeV. in Journal of High Energy Physics. 2021;2021(7):208.
doi:10.1007/JHEP07(2021)208 .
Sirunyan, A., Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Milošević, Vukašin, "Search for resonant and nonresonant new phenomena in high-mass dilepton final states at √s = 13 TeV" in Journal of High Energy Physics, 2021, no. 7 (2021):208,
https://doi.org/10.1007/JHEP07(2021)208 . .
1
78
8
111

Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV

Sirunyan, A.; Tumasyan, A.; Adam, W.; Andrejkovic, J.; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan

(2021)

TY  - JOUR
AU  - Sirunyan, A.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10027
AB  - Measurements of Higgs boson production cross sections and couplings in events where the Higgs boson decays into a pair of photons are reported. Events are selected from a sample of proton-proton collisions at     s    $$ \sqrt{s} $$  = 13 TeV collected by the CMS detector at the LHC from 2016 to 2018, corresponding to an integrated luminosity of 137 fb −1. Analysis categories enriched in Higgs boson events produced via gluon fusion, vector boson fusion, vector boson associated production, and production associated with top quarks are constructed. The total Higgs boson signal strength, relative to the standard model (SM) prediction, is measured to be 1.12±0.09. Other properties of the Higgs boson are measured, including SM signal strength modifiers, production cross sections, and its couplings to other particles. These include the most precise measurements of gluon fusion and vector boson fusion Higgs boson production in several different kinematic regions, the first measurement of Higgs boson production in association with a top quark pair in five regions of the Higgs boson transverse momentum, and an upper limit on the rate of Higgs boson production in association with a single top quark. All results are found to be in agreement with the SM expectations.
T2  - Journal of High Energy Physics
T1  - Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV
VL  - 2021
IS  - 7
SP  - 27
DO  - 10.1007/JHEP07(2021)027
ER  - 
@article{
author = "Sirunyan, A. and Tumasyan, A. and Adam, W. and Andrejkovic, J. and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan",
year = "2021",
abstract = "Measurements of Higgs boson production cross sections and couplings in events where the Higgs boson decays into a pair of photons are reported. Events are selected from a sample of proton-proton collisions at     s    $$ \sqrt{s} $$  = 13 TeV collected by the CMS detector at the LHC from 2016 to 2018, corresponding to an integrated luminosity of 137 fb −1. Analysis categories enriched in Higgs boson events produced via gluon fusion, vector boson fusion, vector boson associated production, and production associated with top quarks are constructed. The total Higgs boson signal strength, relative to the standard model (SM) prediction, is measured to be 1.12±0.09. Other properties of the Higgs boson are measured, including SM signal strength modifiers, production cross sections, and its couplings to other particles. These include the most precise measurements of gluon fusion and vector boson fusion Higgs boson production in several different kinematic regions, the first measurement of Higgs boson production in association with a top quark pair in five regions of the Higgs boson transverse momentum, and an upper limit on the rate of Higgs boson production in association with a single top quark. All results are found to be in agreement with the SM expectations.",
journal = "Journal of High Energy Physics",
title = "Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV",
volume = "2021",
number = "7",
pages = "27",
doi = "10.1007/JHEP07(2021)027"
}
Sirunyan, A., Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P.,& Milošević, J.. (2021). Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV. in Journal of High Energy Physics, 2021(7), 27.
https://doi.org/10.1007/JHEP07(2021)027
Sirunyan A, Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J. Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV. in Journal of High Energy Physics. 2021;2021(7):27.
doi:10.1007/JHEP07(2021)027 .
Sirunyan, A., Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, "Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV" in Journal of High Energy Physics, 2021, no. 7 (2021):27,
https://doi.org/10.1007/JHEP07(2021)027 . .
1
32
1
56

Search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector boson pairs in proton–proton collisions at √s=13TeV

Sirunyan, A.; Tumasyan, A.; Adam, W.; Andrejkovic, J.; Bergauer, T.; Adžić, Petar; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan

(2021)

TY  - JOUR
AU  - Sirunyan, A.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Andrejkovic, J.
AU  - Bergauer, T.
AU  - Adžić, Petar
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10026
AB  - A search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector bosons, using proton–proton collisions at  $$\sqrt{s}=13\,{\text {TeV}} $$     s  = 13  TeV     at the LHC, is reported. The data sample corresponds to an integrated luminosity of 137 $$\,{\text {fb}}^{-1}$$       fb   - 1       collected with the CMS detector. Events are selected by requiring two or three electrons or muons, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. No excess of events with respect to the standard model background predictions is observed. Model independent upper limits at 95% confidence level are reported on the product of the cross section and branching fraction for vector boson fusion production of charged Higgs bosons as a function of mass, from 200 to 3000 $$\,{\text {GeV}}$$     GeV    . The results are interpreted in the context of the Georgi–Machacek model.
T2  - European Physical Journal C. Particles and Fields
T1  - Search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector boson pairs in proton–proton collisions at √s=13TeV
VL  - 81
IS  - 8
SP  - 723
DO  - 10.1140/epjc/s10052-021-09472-3
ER  - 
@article{
author = "Sirunyan, A. and Tumasyan, A. and Adam, W. and Andrejkovic, J. and Bergauer, T. and Adžić, Petar and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan",
year = "2021",
abstract = "A search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector bosons, using proton–proton collisions at  $$\sqrt{s}=13\,{\text {TeV}} $$     s  = 13  TeV     at the LHC, is reported. The data sample corresponds to an integrated luminosity of 137 $$\,{\text {fb}}^{-1}$$       fb   - 1       collected with the CMS detector. Events are selected by requiring two or three electrons or muons, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. No excess of events with respect to the standard model background predictions is observed. Model independent upper limits at 95% confidence level are reported on the product of the cross section and branching fraction for vector boson fusion production of charged Higgs bosons as a function of mass, from 200 to 3000 $$\,{\text {GeV}}$$     GeV    . The results are interpreted in the context of the Georgi–Machacek model.",
journal = "European Physical Journal C. Particles and Fields",
title = "Search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector boson pairs in proton–proton collisions at √s=13TeV",
volume = "81",
number = "8",
pages = "723",
doi = "10.1140/epjc/s10052-021-09472-3"
}
Sirunyan, A., Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Adžić, P., Đorđević, M., Milenović, P.,& Milošević, J.. (2021). Search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector boson pairs in proton–proton collisions at √s=13TeV. in European Physical Journal C. Particles and Fields, 81(8), 723.
https://doi.org/10.1140/epjc/s10052-021-09472-3
Sirunyan A, Tumasyan A, Adam W, Andrejkovic J, Bergauer T, Adžić P, Đorđević M, Milenović P, Milošević J. Search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector boson pairs in proton–proton collisions at √s=13TeV. in European Physical Journal C. Particles and Fields. 2021;81(8):723.
doi:10.1140/epjc/s10052-021-09472-3 .
Sirunyan, A., Tumasyan, A., Adam, W., Andrejkovic, J., Bergauer, T., Adžić, Petar, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, "Search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector boson pairs in proton–proton collisions at √s=13TeV" in European Physical Journal C. Particles and Fields, 81, no. 8 (2021):723,
https://doi.org/10.1140/epjc/s10052-021-09472-3 . .
4
14
1
22

Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te

Sirunyan, A.; Tumasyan, A.; Adam, W.; Bergauer, T.; Dragicevic, M.; Adžić, Petar; Ćirković, Predrag; Đorđević, Miloš; Milenović, Predrag; Milošević, Jovan

(2021)

TY  - JOUR
AU  - Sirunyan, A.
AU  - Tumasyan, A.
AU  - Adam, W.
AU  - Bergauer, T.
AU  - Dragicevic, M.
AU  - Adžić, Petar
AU  - Ćirković, Predrag
AU  - Đorđević, Miloš
AU  - Milenović, Predrag
AU  - Milošević, Jovan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10025
AB  - A search is presented for a heavy vector reso- nance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is per- formed in a Lorentz-boosted regime and is based on data col- lected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137 fb−1. Upper limits are derived on the production of a narrow heavy resonance Z′, and a mass below 3.5 and 3.7 TeV is excluded at 95% confidence level in models where the heavy vector boson couples predomi- nantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3 fb for a Z′ mass between 0.8 and 4.6 TeV, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
T2  - European Physical Journal C. Particles and Fields
T1  - Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te
VL  - 81
IS  - 8
SP  - 688
DO  - 10.1140/epjc/s10052-021-09348-6
ER  - 
@article{
author = "Sirunyan, A. and Tumasyan, A. and Adam, W. and Bergauer, T. and Dragicevic, M. and Adžić, Petar and Ćirković, Predrag and Đorđević, Miloš and Milenović, Predrag and Milošević, Jovan",
year = "2021",
abstract = "A search is presented for a heavy vector reso- nance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is per- formed in a Lorentz-boosted regime and is based on data col- lected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137 fb−1. Upper limits are derived on the production of a narrow heavy resonance Z′, and a mass below 3.5 and 3.7 TeV is excluded at 95% confidence level in models where the heavy vector boson couples predomi- nantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3 fb for a Z′ mass between 0.8 and 4.6 TeV, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.",
journal = "European Physical Journal C. Particles and Fields",
title = "Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te",
volume = "81",
number = "8",
pages = "688",
doi = "10.1140/epjc/s10052-021-09348-6"
}
Sirunyan, A., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Adžić, P., Ćirković, P., Đorđević, M., Milenović, P.,& Milošević, J.. (2021). Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te. in European Physical Journal C. Particles and Fields, 81(8), 688.
https://doi.org/10.1140/epjc/s10052-021-09348-6
Sirunyan A, Tumasyan A, Adam W, Bergauer T, Dragicevic M, Adžić P, Ćirković P, Đorđević M, Milenović P, Milošević J. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te. in European Physical Journal C. Particles and Fields. 2021;81(8):688.
doi:10.1140/epjc/s10052-021-09348-6 .
Sirunyan, A., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Adžić, Petar, Ćirković, Predrag, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, "Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te" in European Physical Journal C. Particles and Fields, 81, no. 8 (2021):688,
https://doi.org/10.1140/epjc/s10052-021-09348-6 . .
5
4
11