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20/05/2019, 09:00Talk
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Manfred Krammer (CERN)20/05/2019, 09:25Talk
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Giovanni Iadarola (CERN)20/05/2019, 09:55Talk
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Luca Malgeri (CERN)20/05/2019, 10:20Talk
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Kevin Frank Einsweiler (Lawrence Berkeley National Lab. (US))20/05/2019, 11:15Talk
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Jochen Klein (Universita e INFN Torino (IT))20/05/2019, 11:40Talk
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Giovanni Passaleva (INFN Florence (IT))20/05/2019, 12:05Talk
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Clara Nellist (Georg August Universitaet Goettingen (DE))20/05/2019, 12:30Talk
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Ejiro Naomi Umaka (University of Houston (US))20/05/2019, 12:45Talk
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Patrick Foldenauer20/05/2019, 14:30
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John Stakely Keller (Carleton University (CA))20/05/2019, 14:30Talk
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Massimiliano Marchisone (Centre National de la Recherche Scientifique (FR))20/05/2019, 14:30
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Radja Boughezal (Argonne National Laboratory)20/05/2019, 14:30
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Dr Luca Mastrolorenzo (Rheinisch Westfaelische Tech. Hoch. (DE))20/05/2019, 14:45
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Adrian Casais Vidal (Instituto Galego de Física de Altas Enerxías (ES))20/05/2019, 14:50
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Cristian Baldenegro Barrera (The University of Kansas (US))20/05/2019, 14:53
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Riccardo Manzoni (ETH Zurich (CH))20/05/2019, 14:54
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Markus Spanring (Austrian Academy of Sciences (AT))20/05/2019, 15:00Talk
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Javier Mauricio Duarte (Fermi National Accelerator Lab. (US))20/05/2019, 15:10
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Hongtao Yang (Lawrence Berkeley National Lab. (US))20/05/2019, 15:15Talk
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Pedro Cal20/05/2019, 15:16
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Francesco Polci (Centre National de la Recherche Scientifique (FR))20/05/2019, 15:18
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Jurgen Engelfried (Instituto de Fisica, Universidad Autonoma de San Luis Potosi, Mexico), Jurgen Engelfried (Univ. Autonoma de San Luis Potosi (MX))20/05/2019, 15:30
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Bernhard Mistlberger (Massachusetts Inst. of Technology (US))20/05/2019, 15:30Talk
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20/05/2019, 15:40
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Murilo Santana Rangel (Federal University of of Rio de Janeiro (BR))20/05/2019, 15:42
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Jorge de Blas (INFN-Padova), Marine Kuna (Université Grenoble Alpes, LPSC), Nicholas Wardle (Imperial College (GB))20/05/2019, 15:45
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Elena Accomando (Southampton University), Elena Accomando (Universita e INFN (IT)), Martino Borsato (Ruprecht Karls Universitaet Heidelberg (DE))20/05/2019, 15:50
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Paolo Gandini (INFN Milano (IT))20/05/2019, 16:30Talk
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Nuno Leonardo (LIP)20/05/2019, 16:54Talk
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Antonio Pich (IFIC, U. Valencia -.)20/05/2019, 17:18Talk
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Yvonne Chiara Pachmayer (Ruprecht Karls Universitaet Heidelberg (DE))20/05/2019, 17:42Talk
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Paula Alvarez Cartelle (Imperial College (GB))21/05/2019, 09:00
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Jennifer Ngadiuba (CERN)21/05/2019, 09:24Talk
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Robin Erbacher (University of California Davis (US))21/05/2019, 09:48Talk
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Martino Borsato (Ruprecht Karls Universitaet Heidelberg (DE))21/05/2019, 10:12Talk
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Shih-Chieh Hsu (University of Washington Seattle (US))21/05/2019, 10:36Talk
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Suchita Kulkarni (Austrian Academy of Sciences (AT))21/05/2019, 11:30
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Gerardo Hernández-Tomé (CINVESTAV)21/05/2019, 11:30
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Emanuele Re (CERN)21/05/2019, 11:30Talk
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Dr Yacine Mehtar-Tani (Brookhaven National Laboratory)21/05/2019, 11:30
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Dorival Gonçalves (University of Pittsburgh)21/05/2019, 11:48Talk
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Jussi Viinikainen (University of Illinois at Chicago (US))21/05/2019, 11:50
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Tamas Almos Vami (Wigner RCP, Budapest (HU))21/05/2019, 11:50
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Grazia Luparello (Universita e INFN Trieste (IT))21/05/2019, 11:52
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Toni Sculac (University of Split. Fac.of Elect. Eng., Mech. Eng. and Nav.Arc)21/05/2019, 12:06Talk
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Martin Rybar (Columbia University (US))21/05/2019, 12:10
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Rosa Simoniello (Johannes Gutenberg Universitaet Mainz (DE))21/05/2019, 12:10
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Jhovanny Andres Mejia Guisao (Centro Invest. Estudios Avanz. IPN (MX))21/05/2019, 12:14
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Chikuma Kato (Tsung-Dao Lee Institute (CN))21/05/2019, 12:24Talk
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Ritsuya Hosokawa (University of Tsukuba (JP))21/05/2019, 12:30
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Nathaniel Joseph Pastika (Baylor University (US))21/05/2019, 12:30
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Jorge de Blas (INFN-Padova), Marine Kuna (Université Grenoble Alpes, LPSC), Nicholas Wardle (Imperial College (GB))21/05/2019, 12:42
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21/05/2019, 12:42
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21/05/2019, 12:50
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21/05/2019, 12:50
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Elena Yatsenko (Shanghai Jiao Tong University (CN) & Tsung-Dao Lee Institute (CN))21/05/2019, 14:30Talk
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Davide Napoletano (Ipht, Saclay)21/05/2019, 14:30Talk
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Nikolina Ilic (Nikhef National institute for subatomic physics (NL))21/05/2019, 14:30
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Karolos Potamianos (Deutsches Elektronen-Synchrotron (DE))21/05/2019, 14:30Talk
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Sascha Mehlhase (Ludwig Maximilians Universitat (DE))21/05/2019, 14:48Talk
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Bugra Bilin (Universite Libre de Bruxelles (BE))21/05/2019, 14:50Talk
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David Yu (Brown University (US))21/05/2019, 14:50
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Dylan George Hsu (Massachusetts Inst. of Technology (US))21/05/2019, 14:52
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Dr Thomas McCauley (University of Notre Dame (US))21/05/2019, 15:06Talk
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Marianna Mazzilli (Universita e INFN, Bari (IT))21/05/2019, 15:08Talk
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Olaf Nackenhorst (Technische Universitaet Dortmund (DE))21/05/2019, 15:10
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Fulvio Piccinini (Universita and INFN (IT))21/05/2019, 15:14
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Javier Mauricio Duarte (Fermi National Accelerator Lab. (US))21/05/2019, 15:24Talk
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Paolo Gandini (INFN Milano (IT))21/05/2019, 15:26
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Michael Aaron Kagan (SLAC National Accelerator Laboratory (US))21/05/2019, 15:30
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Stefano Forte (Università degli Studi e INFN Milano (IT))21/05/2019, 15:36
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Clara Nellist (Georg August Universitaet Goettingen (DE)), Edgar Fernando Carrera Jarrin (Universidad San Francisco de Quito (EC)), Javier Mauricio Duarte (Fermi National Accelerator Lab. (US)), Karolos Potamianos (Deutsches Elektronen-Synchrotron (DE)), Sascha Mehlhase (Ludwig Maximilians Universitat (DE)), Thomas McCauley (University of Notre Dame (US))21/05/2019, 15:42
The proposed topics for discussion are:
Go to contribution page
- Reaching out to society: how to maintain/increase the impact of the LHC?
- LHC Open Data for research: potential, perspectives and challenges. -
21/05/2019, 15:44Talk
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21/05/2019, 15:50
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Stefano Forte (Università degli Studi e INFN Milano (IT))21/05/2019, 16:30Talk
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Roberto Bonciani (Dipartimento di Fisica)21/05/2019, 16:54Talk
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Javier Llorente Merino (Chinese Academy of Sciences (CN))21/05/2019, 17:18Talk
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Chris Pollard (Deutsches Elektronen-Synchrotron (DE))21/05/2019, 17:42Talk
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Christophe Royon (The University of Kansas (US))21/05/2019, 18:06Talk
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Derek Teaney (Stony Brook University)22/05/2019, 09:00Talk
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Antonio Ortiz Velasquez (Universidad Nacional Autonoma (MX))22/05/2019, 09:24Talk
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Olga Evdokimov (University of Illinois at Chicago (US))22/05/2019, 09:48Talk
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Dr Cesar Luiz Da Silva (Los Alamos National Laboratory (US))22/05/2019, 10:12Talk
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Ramona Lea (Universita e INFN Trieste (IT))22/05/2019, 10:36Talk
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Dr Nausheen Shah (Wayne State University)22/05/2019, 11:30
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Prof. Zhongbo Kang (UCLA)22/05/2019, 11:30
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Dominik Karol Derendarz (Polish Academy of Sciences (PL))22/05/2019, 11:30
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Rene Poncelet (Cambridge University)22/05/2019, 11:30Talk
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Henning Kirschenmann (Helsinki Institute of Physics (FI))22/05/2019, 11:50
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Alexander Mann (Ludwig-Maximilians-Universität München (DE))22/05/2019, 11:50
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Nicolo Jacazio (Universita e INFN, Bologna (IT))22/05/2019, 11:55
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Liza Mijovic (University of Edinburgh)22/05/2019, 12:00Talk
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Luigi Longo (CERN)22/05/2019, 12:10
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Vinicius Massami Mikuni (Universitaet Zuerich (CH))22/05/2019, 12:15Talk
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Javier Alberto Murillo Quijada (Universidad de Sonora (MX))22/05/2019, 12:20
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Markus Fasel (Oak Ridge National Laboratory - (US))22/05/2019, 12:24
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Markus Cristinziani (University of Bonn (DE))22/05/2019, 12:30Talk
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Samuel Louis Bein (Hamburg University (DE))22/05/2019, 12:30
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Murilo Santana Rangel (Federal University of of Rio de Janeiro (BR))22/05/2019, 12:42
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22/05/2019, 12:45
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Giulia Negro (Purdue University (US))22/05/2019, 12:45Talk
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22/05/2019, 12:50
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Thomas McCarthy (Max-Planck-Institut für Physik (DE))23/05/2019, 09:00Talk
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Francisco Yumiceva (Florida Institute of Technology (US))23/05/2019, 09:24Talk
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Daniele Zanzi (CERN)23/05/2019, 09:48Talk
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Kirill Melnikov (Karlsruhe Institute of Technology, Germany)23/05/2019, 10:12Talk
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Alessandro Vicini23/05/2019, 10:36Talk
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Mrinal Dasgupta (Unknown)23/05/2019, 11:30
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Tomas Jezo (University of Zurich)23/05/2019, 11:30Talk
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Valentina Cairo (SLAC National Accelerator Laboratory (US))23/05/2019, 11:30
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Andreas Goudelis (LPTHE - Paris)23/05/2019, 11:30
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Alfredo Castaneda (Universidad de Sonora (MX))23/05/2019, 11:48
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William Kalderon (Lund University (SE))23/05/2019, 11:50
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Patrick Kirchgaesser23/05/2019, 11:50
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Clara Nellist (Georg August Universitaet Goettingen (DE))23/05/2019, 12:00Talk
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Cristiane Jahnke (Technische Universitaet Muenchen (DE))23/05/2019, 12:10
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Allison Reinsvold Hall (Fermilab)23/05/2019, 12:10
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Samuel Louis Bein (Hamburg University (DE))23/05/2019, 12:12
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Tae Jeong Kim (Hanyang University (KR))23/05/2019, 12:20Talk
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Goran Simatovic (Nikhef National institute for subatomic physics (NL))23/05/2019, 12:27
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Noam Tal Hod (Weizmann Institute of Science (IL))23/05/2019, 12:30
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Kamil Rafal Deja (Warsaw University of Technology (PL))23/05/2019, 12:36
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Trisha Farooque (Michigan State University (US))23/05/2019, 12:40Talk
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Valentina Cairo (SLAC National Accelerator Laboratory (US))23/05/2019, 12:44
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Elena Accomando (Southampton University), Elena Accomando (Universita e INFN (IT)), Francesco Pandolfi (INFN Rome)23/05/2019, 12:50
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Alexander Savin (University of Wisconsin Madison (US))23/05/2019, 14:30Talk
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Prof. Alejandro Ayala (Instituto de Ciencias Nucleares, Universidad Nacional Autonoma de Mexico), Alejandro Ayala Santander (Federico Santa Maria Technical University (CL))23/05/2019, 14:30
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Violaine Bellee (EPFL - Ecole Polytechnique Federale Lausanne (CH))23/05/2019, 14:30
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James Pinfold (University of Alberta (CA))23/05/2019, 14:30
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Jose Feliciano Benitez (Universidad de Sonora (MX))23/05/2019, 14:48Talk
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Ivan Heredia De La Cruz (Centro de Investigación y de Estudios Avanzados del IPN (MX))23/05/2019, 14:48
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Sebastian Lehner (Austrian Academy of Sciences (AT))23/05/2019, 14:52
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Giuliano Gustavino (University of Oklahoma (US))23/05/2019, 15:06
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Daniel Aloni23/05/2019, 15:06
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Sascha Mehlhase (Ludwig Maximilians Universitat (DE))23/05/2019, 15:10
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Ran Bi (Massachusetts Inst. of Technology (US))23/05/2019, 15:14
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Jaime Norman (Centre National de la Recherche Scientifique (FR))23/05/2019, 15:24Talk
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Dr Antonio Romero Vidal (Universidade de Santiago de Compostela (ES), Instituto Galego de Física de Altas Enerxías (IGFAE))23/05/2019, 15:24
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Malgorzata Kazana (NCBJ Warsaw (PL))23/05/2019, 15:30
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Jakub Kremer (AGH University of Science and Technology (PL))23/05/2019, 15:36
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23/05/2019, 15:42
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Violaine Bellee (EPFL - Ecole Polytechnique Federale Lausanne (CH))23/05/2019, 15:42Talk
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23/05/2019, 15:50
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Laura Reina (Florida State University (US))23/05/2019, 16:30Talk
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Luca Cadamuro (University of Florida (US))23/05/2019, 16:54Talk
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Jahred Adelman (Northern Illinois University)23/05/2019, 17:18Talk
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Linda Finco (University of Nebraska Lincoln (US))23/05/2019, 17:42Talk
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Xiaohu Sun (University of Alberta (CA))23/05/2019, 18:06Talk
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Jens Erler (IF-UNAM)24/05/2019, 09:00Talk
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Maria Moreno Llacer (CERN)24/05/2019, 09:23Talk
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Philip Chang (Univ. of California San Diego (US))24/05/2019, 09:46Talk
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Davide Pagani (TUM - Garching bei München)24/05/2019, 10:09Talk
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Jorge de Blas (INFN-Padova), Markus Schulz (CERN)24/05/2019, 10:36Talk
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Nathan Peter Readioff (LPSC-Grenoble, CNRS/UGA (FR))24/05/2019, 11:30Talk
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German Sborlini (Università di Milano, INFN Milano and IFIC-Valencia)24/05/2019, 11:30
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Dominic Hirschbuehl (Bergische Universitaet Wuppertal (DE))24/05/2019, 11:30Talk
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Luigi Marchese (University of Oxford (GB))24/05/2019, 11:30
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Markus Keil (CERN)24/05/2019, 11:48
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Dylan Sheldon Rankin (Massachusetts Inst. of Technology (US))24/05/2019, 11:48
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Fabio Iemmi (Universita e INFN, Bologna (IT))24/05/2019, 11:50Talk
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Markus Cristinziani (University of Bonn (DE))24/05/2019, 11:52
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Francesco Pandolfi (INFN Rome)24/05/2019, 12:06Talk
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David Miller (University of Chicago (US))24/05/2019, 12:06
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Emma Slade (University of Oxford)24/05/2019, 12:10Talk
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Usama Hussain (University of Wisconsin Madison (US))24/05/2019, 12:14
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Cesar Luiz Da Silva (Los Alamos National Laboratory (US)), Preema Rennee Pais (EPFL - Ecole Polytechnique Federale Lausanne (CH))24/05/2019, 12:24Talk
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Ernst Hellbar (Johann-Wolfgang-Goethe Univ. (DE))24/05/2019, 12:24
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Marc Riembau (Universite de Geneve (CH))24/05/2019, 12:36
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Prolay Mal (National Institute of Science Education and Research (IN))24/05/2019, 12:40Talk
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Chad Wells Freer (Northeastern University (US))24/05/2019, 12:42Talk
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Pierfrancesco Butti (CERN)24/05/2019, 12:42
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Carlos Alberto Vaquera-Araujo (University of Guanajuato)24/05/2019, 14:30
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Karolos Potamianos (Deutsches Elektronen-Synchrotron (DE))24/05/2019, 14:30
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David Miller (University of Chicago (US))24/05/2019, 14:30Talk
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Dr Mariola Klusek-Gawenda (Institute of Nuclear Physics Polish Academy of Sciences)24/05/2019, 14:30
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Norbert Novitzky (University of Tsukuba (JP))24/05/2019, 14:48Talk
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Martha Hilton (University of Manchester (GB))24/05/2019, 14:48
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David Horak (Czech Technical University (CZ))24/05/2019, 14:50
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Riccardo Bellan (Universita e INFN Torino (IT))24/05/2019, 14:55
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Melissa Maria Cruz Torres (CBPF - Brazilian Center for Physics Research (BR))24/05/2019, 15:06
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Michele Selvaggi (CERN), Paolo Giacomelli (Universita e INFN, Bologna (IT))24/05/2019, 15:06Talk
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Prof. Daniel Tapia Takaki (University of Kansas)24/05/2019, 15:10
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Dr Alexander Karlberg (Universitaet Zuerich (CH))24/05/2019, 15:20
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Marcella Bona (Queen Mary University of London (UK))24/05/2019, 15:24
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Paolo Giacomelli (Universita e INFN, Bologna (IT))24/05/2019, 15:24Talk
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Martin Hentschinski (Universidad de las Americas, Puebla)24/05/2019, 15:30
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24/05/2019, 15:42
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Jorge de Blas (INFN-Padova)24/05/2019, 15:42Talk
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Jürgen Reuter (DESY Hamburg, Germany)24/05/2019, 15:45
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24/05/2019, 15:50
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Bertrand Martin Dit Latour (University of Bergen (NO))24/05/2019, 16:45Talk
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Stefano Zambito (Harvard University (US))24/05/2019, 17:09Talk
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Indara Suarez (Boston University (US))24/05/2019, 17:33Talk
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Kelvin Mei (Princeton University)24/05/2019, 17:57Talk
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Carlos E.M. Wagner (University of Chicago)24/05/2019, 18:21Talk
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Dmitri Sergeevich Denisov (Fermi National Accelerator Lab. (US)), Paolo Giacomelli (Universita e INFN, Bologna (IT))25/05/2019, 09:00
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Michael Andreas Winn (Université Paris-Saclay (FR))25/05/2019, 09:01Talk
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Francesco Polci (Centre National de la Recherche Scientifique (FR))25/05/2019, 09:22Talk
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Vladimir Rekovic (Vinca, University of Belgrade (RS)/ CERN / Florida (US))25/05/2019, 09:43Talk
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Ben Nachman (Lawrence Berkeley National Lab. (US))25/05/2019, 10:04Talk
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Andrea Wulzer (CERN and EPFL)25/05/2019, 10:25Talk
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Andrea Wulzer (CERN and EPFL)25/05/2019, 10:45
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Aleandro Nisati (Sapienza Universita e INFN, Roma I (IT))25/05/2019, 11:30Talk
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Andres Sandoval (Johann-Wolfgang-Goethe Univ. (DE))25/05/2019, 11:40Talk
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Jacobo Konigsberg (University of Florida (US))25/05/2019, 12:20Talk
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Nathaniel Craig (UC Santa Barbara)25/05/2019, 13:00Talk
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Jim Olsen (Princeton University (US)), Bruno Mansoulie (Université Paris-Saclay (FR))25/05/2019, 13:40
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Talk
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Dr Adolfo Guevara (Madrid University)
The present approach relies on the SM chiral symmetry breaking pattern $SU(2)_L \otimes SU(2)_R \to SU(2)_{L+R}$, with the EW Goldstone bosons given in a non-linear realization and the Higgs boson described by an EW singlet field. In addition, we assume the presence of new physics heavy states around the TeV scale that do not couple to the SM fermions, only to the SM bosonic sector. However,...
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ATLAS Collaboration, Inga Katarzyna Lakomiec (AGH University of Science and Technology (PL))
The purpose of the ATLAS Roman Pot (ARP) detector is to measure protons scattered at very small angles. ARP aims to study elastic and diffractive events, exclusive production and photon induced interactions. In LHC Run 2, ARP participated in the ATLAS high-luminosity data taking. In addition, several special runs with reduced luminosity were taken. Any cross section measurement requires good...
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Luis Alberto Perez Moreno (Autonomous University of Puebla (MX))UpgradePoster
ALICE (A Large Ion Collider Experiment) is one of the four main experiments at the CERN Large Hadron Collider. The ALICE collaboration plans a major detector upgrade during long shutdown 2, which started at the end of 2018, followed by Run 3 starting in 2021. In Run 3 ALICE will be able to collect 10 nb$^{-1}$ of Pb-Pb collisions at luminosities up to $\mathcal{L}=\, 6 \times 10^{27}$...
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E. Cuautle, A. Mishra, G. Paic ,C. Pajares, R. P. Scharenberg and B Srivastava, Aditya Nath Mishra (ICN-UNAM)
We present the results obtained in the extraction of the main parameters of the QCD inspired approach towards the high density phase transition. Using the percolation model to define the main parameters we have extracted them for all the LHC experimental results from pp to PbPb collisions.
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Omar Vazquez Rueda (Lund University (SE))
In ultra-relativistic heavy-ion collisions at LHC energies, a strongly interacting Quark-Gluon-Plasma (sQGP) is produced. This sQGP behaves like a perfect liquid and its hydrodynamic expansion gives rise to radial flow in heavy-ion collisions. However, similar phenomena have recently also been observed in small collision systems (pp and p$-$A). Current research therefore tries to identify the...
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Juan Carlos Cabanillas Noris
Precise knowledge of what a system requires is a principle that unquestionably marks the success or failure of a software development. Establishing and managing the requirements for the design of a system are fundamental aspects of software engineering. One of the main software systems in a High Energy Physics (HEP) experiment is the Detector Control System (DCS). The DCS allows the control,...
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ATLAS Collaboration, Robin Hayes (University of British Columbia (CA))
Events containing muons in the final state are an important signature for many analyses being carried out at the Large Hadron Collider (LHC), including both standard model measurements and searches for new physics. To be able to study such events, it is required to have an efficient and well-understood muon trigger. The ATLAS muon trigger consists of a hardware based system (Level 1), as well...
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Sascha Mehlhase (Ludwig Maximilians Universitat (DE))
The members of large High Energy Physics (HEP) collaborations come from all over the world. They understand that one significant challenge in teaching experimental HEP is the current location of many potential and valuable students and young researchers. In the case of ATLAS, many of its members come from Latin-American, Middle Eastern and Sub-Saharan countries. Also, they recognise the...
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ATLAS Collaboration, Elham E Khoda (University of British Columbia (CA))
The high energy and luminosity of the LHC allows to study jets and hadronically decaying tau leptons at extreme energies with the ATLAS tracking detector. These topologies lead to charged particles with an angular separation smaller than the size of the ATLAS Inner Detector sensitive elements and consequently to a reduced track reconstruction efficiency. In order to regain part of the track...
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Talk
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ATLAS Collaboration
The Tile Calorimeter (TileCal) is the central section of the hadronic calorimeter of the ATLAS experiment and provides important information for reconstruction of hadrons, jets, hadronic decays of tau leptons and missing transverse energy. It also assists in muon identification. This sampling calorimeter uses steel plates as absorber and scintillating tiles as active medium. The light produced...
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Tamas Almos Vami (Wigner RCP, Budapest (HU))
The Compact Muon Solenoid (CMS) is one of two general-purpose detectors that reconstruct the products of high energy particle interactions at the Large Hadron Collider at CERN. The silicon pixel detector is the innermost component of the CMS tracking system. It determines the trajectories of charged particles originating from the interaction region with high resolution enabling precise...
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Jose Feliciano Benitez (Universidad de Sonora (MX))
Maximally precise calibration of the CMS luminosity measurement is critical for many physics measurements. To guarantee high quality absolute calibration, a complete van der Meer scan program was carried out at the CMS experiment in 2018. The systematic uncertainty on the absolute calibration from the van der Meer scans is derived with a precision of 2.1%. The performance and stability of the...
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Sascha Mehlhase (Ludwig Maximilians Universitat (DE))Poster
Communicating the status and achievements of the ATLAS Experiment has been a core objective of the ATLAS Collaboration since its founding. To match an ever-changing media landscape, ATLAS has tailored its communication strategy to produce content that effectively targets key audiences. The comprehensive approach of ATLAS communications is explored, with a focus on strategic themes, effective...
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Tania Natalie Robens (Rudjer Boskovic Institute (HR))Talk
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Talk
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Diana Rojas-Ciofalo (University of Southampton)
We analyse new signals of Dark Matter (DM) at the Large Hadron Collider (LHC) in a 3-Higgs Doublet Model (3HDM) where only one doublet acquires a Vacuum Expectation Value (VEV), preserving a parity Z2. The other two doublets are inert and do not develop a VEV, leading to a dark scalar sector controlled by Z2, with the lightest CP-even dark scalar H1 being the DM candidate. This leads to the...
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Dr Alfonso Rosado, Dr Sebastián Rosado-Navarro (Fac. de Cs. FIsico-Matemáticas)
We discuss $Z$-production in Deep Inelastic Scattering $e + p \to e + Z + X$ using the Parton Model, in the context of the Standard Model. In contrast to the deep inelastic $ep$-scattering ($e + p \to e + X$), where $\tilde{Q}^{2}$ the transferred momentum square is unique in the case of boson production it depends upon the mechanism involved, that it is related to the EW interaction. We...
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Talk
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Gabriel Palacino (Indiana University (US))Talk
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Jorge de Blas (INFN-Padova), Marine Kuna (Université Grenoble Alpes, LPSC), Nicholas Wardle (Imperial College (GB))
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Dalia Lucero Ramírez Guadarrama (Universidad Iberoamericana (MX))UpgradePoster
We will present a summary of the performance of the improved RPC (iRPC) using several RPC gas mixtures with a low Global Warming Potential (GWP). We have replaced the Freon (R134a) from the official CMS gas mixture with HFO and CO2. The results show promising mixtures for the iRPC for the High Luminosity LHC
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Talk
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Collaboration ATLAS (CERN), Markus Cristinziani (University of Bonn (DE))
A search for the production of three massive vector bosons in $pp$ collisions
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is performed using data at $\sqrt{s} = 13$ TeV recorded with the ATLAS detector
at the Large Hadron Collider in the years 2015--2017, corresponding to an
integrated luminosity of $79.8$ fb$^{-1}$. Events with two same-sign leptons
$\ell$ (electrons or muons) and at least two reconstructed jets are selected to
search... -
Ms Cristal Robles Jacobo
By using the interplay between the growth of the transverse size of the proton in the high energy limit, and the gluonic matter density, with unitarity saturation based on a grey disk model. We explore the evolution of the unitarity saturation in the pp and np total cross section to the asymptotic limit to the geometric scaling.
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Ida Peruzzi (Laboratori Nazionali di Frascati dell'INFN)QCDPoster
The Belle II experiment at the SuperKEKB energy-asymmetric $e^+ e^-$ collider is a substantial upgrade of the B factory facility at KEK in Tsukuba, Japan. It aims to record a factor of 50 times more data than its predecessor. The experiment completed a commissioning run in 2018, and began full operation in early 2019. Belle II is uniquely capable of studying the so-called "XYZ" particles:...
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Hamed Bakhshiansohi (DESY)
The Standard Model is one of the most successful theories at describing the strong, weak, and electromagnetic forces and the interactions between the elementary particles.
The scalar boson discovered in 2012 at the Large Hadron Collider (LHC) might be consistent with the Higgs boson predicted by the Standard Model, thus validating the Higgs mechanism and therefore representing a further...
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Mario Rodriguez Cahuantzi (Autonomous University of Puebla (MX))
The observation of neutral long-lived particles at the LHC would reveal physics beyond the Standard Model and could account for the many open issues in our understanding of our universe. Long-lived particle signatures are well motivated and can appear in many theoretical constructs that address the Hierarchy Problem, Dark Matter, Neutrino Masses and the Baryon Asymmetry of the Universe.
With...
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Silem Téllez
We use three different formalisms to explore the evolution of the scaling variable ($t_D$) given by the transverse momentum squared times the total cross section, from LHC energies to the limit of high energy. Using the eikonal approximation, the grey disk model and the dipole and saturation model, we will show the comparison among these three formalisms in the $t_D$ and in the evolution of...
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Marco MerchandElectroweakPoster
We extend the work of Carone, Chaurasia and Vasquez on non-supersymmetric models of flavor
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based on the double tetrahedral group. Three issues are addressed: (1) the sector of flavorsymmetry-breaking fields is simplified and their potential studied explicitly, (2) a flavorful axion is
introduced to solve the strong CP problem and (3) the model is extended to include the neutrino
sector. We... -
Mr Eligio Cruz-Albaro (Universidad Michoacana de San Nicolas de Hidalgo), Mr David Espinosa-Gomez (Universidad Michoacana de San Nicolas de Hidalgo), Fernando Ramirez-Zavaleta (Universidad Michoacana de San Nicolas de Hidalgo)
Some extended models predict the existence of a new neutral massive gauge boson, identified as the $Z^\prime$ boson, together with flavor-changing neutral currents. In this theoretical framework, we estimate the intensity of couplings regarding the interaction between the $Z^\prime$ boson with the bottom and the strange quarks through the $B^0_s \rightarrow \mu^{+}\mu^{-}$ transition, which...
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Andrea Wulzer (CERN and EPFL)Talk
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Michael Andreas Winn (Université Paris-Saclay (FR))Talk
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Talk
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Riccardo Del Burgo (Universitaet Zuerich (CH))UpgradePoster
The CMS MIP Timing Detector, proposed for the HL-LHC upgrade, will be instrumented with O(10) square meters of ultra-fast Silicon detectors (UFSD) in the forward region. These UFSDs are aimed at measuring the time of passage of each track with a precision of about 30 ps. The sensor that will be used for this task is the low gain avalanche detectors (LGAD). In this contribution, we will present...
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Jens Erler (IF-UNAM)Talk
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James Pinfold (University of Alberta (CA))
The search for physics beyond the Standard Model using dedicated accelerator experiments is presented. The aim of these experiments is to extend the physics reach of the ATLAS and CMS detectors at the LHC in a largely complementary way. As such they represent an important extension of the discovery frontier of particle physics. I shall present the results of the MoEDAL-LHC experiment, that is...
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Janusz Rosiek (University of Warsaw (PL))
I will present the calculation of the h->2 gamma and h->Z gamma decays in the SM EFT at the 1-loop level. I will discuss the calculational setup including derivation of interaction vertices in physical field basis, choice of gauge fixing conditions and choice of the renormalization scheme. The final results for the Br(h->2 gamma) and Br(h->Z gamma) are given as compact semi-analytical...
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Talk
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Yvonne Chiara Pachmayer (Ruprecht Karls Universitaet Heidelberg (DE))Talk
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Talk
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Guy Paic (Universidad Nacional Autonoma (MX))
We study the particle production at high transverse momentum (pT>8 GeV/c) in pp and Pb-Pb collisions at LHC energies. The characterization of the spectra is done using a power-law function and the resulting power-law exponent (n) is studied as a function ofxTfor minimum-biasppcollisions at different√s. The functional form of n as a function of xT exhibits an approximate universal behavior. ...
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Talk
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Mr ALAN IBRAHIM RUIZ OLIVARES (BUAP)Heavy FlavourPoster
High multiplicity pp collisions had shown signals of the possible formation of a collective state on which the clustering color sources give a natural description of the production of strong color fields due to the partonic interactions. We explore the production of Lambda_{c}/D^{0} ratio on high multiplicity pp collisions as a consequence of the production of heavy flavors and the early time...
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Dr Varlen Grabski (Instituto de Fisica UNAM)
During the ongoing Long Shutdown 2 the accelerator complex at CERN will significantly improve
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the performance of the collider by boosting the heavy-ion collision parameters of Run 3 and 4 to well beyond the specifications of the current ALICE setup. For instance, the Pb-Pb instantaneous luminosity during Run 3 will increase by a factor of 5 to 6 and the minimum-bias (MB) Pb-Pb interaction... -
Talk
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Paula Alvarez Cartelle (Imperial College (GB))Talk
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Mr Alejandro Miranda (Cinvestav)
We perform an effective field theory analysis of the τ−→π−π0ντ decays, that includes the most general interactions between Standard Model fields up to dimension six, assuming left-handed neutrinos. We constrain as much as possible the necessary Standard Model hadronic input using chiral symmetry, dispersion relations, data and asymptotic QCD properties. As a result, we set precise (competitive...
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Mr Javier Rendón (Cinvestav)
We analyze the τ−→(Kπ)−ντ decays within an effective field theory description of heavy new physics (NP) modifying the SM left-handed weak charged current and include refined SM input (with controlled uncertainties) for the participant meson form factors exploiting chiral symmetry, dispersion relations and data. We include the leading dimension six operators and work at linear order in the...
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Mr Michael Staelens (University of Alberta)Poster
MoEDAL (Monopole and Exotics Detector at the LHC) is the 7th experi-
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ment, specifically dedicated to investigating beyond the Standard Model sce-
narios by searching for highly ionizing particles, such as magnetic monopoles
or massive pseudo-stable charged particles and multiply electrically charged
particles as messengers of new physics. Sharing the same interaction point as
the LHCb... -
Jürgen Reuter (DESY Hamburg, Germany)
After the discovery of a light Higgs boson, the scattering of electroweak vector bosons (VBS) is even more an eminent search channel for new physics due to the intricate cancellations between gauge and Higgs amplitudes. We will discuss the most general model-independent parameterization for new physics in terms of Standard Model Effective Field Theory (SMEFT), and detail the limitations of...
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Talk
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Talk
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Talk
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Salvador Carrillo Moreno (Universidad Iberoamericana (MX))
Since 2014 several outreach activities have been performed together with IPPOG, Quarknet and DESY programs. We started in Mexico city in 2014 with a workshop with high school teachers and later working with their students. This year the activities have reached five cities in five different Mexican states and are continuing to grow. In 2018 a collaboration with the University of Notre Dame...
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Antonio Ortiz Velasquez (Universidad Nacional Autonoma (MX))Talk
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ATLAS Collaboration, Yoshihiro Shimogama (Waseda University (JP))
The ATLAS experiment has a rich physics program of Standard Model measurements and searches for physics Beyond the Standard Model involving tau leptons. Most of these analyses depend on an efficient tau-lepton trigger that can cope with the overwhelming background from multi-jet events produced in proton-proton collisions at the Large Hadron Collider. The ATLAS trigger system is composed of...
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Laura Reina (Florida State University (US))Talk
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Talk
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Cristian Baldenegro Barrera (The University of Kansas (US))
We will present the first results and the physics prospects from the CMS Precision Proton Spectrometers namely the observation of exclusive dileptons at high mass, and the search for quartic anomalous couplings and axion like particles at high masses at the LHC in the CMS collaboration.
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Talk
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Kirill Melnikov (Karlsruhe Institute of Technology, Germany)Talk
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Prof. Tiago Silva (University of São Paulo)
Several High Energy Physics experiments are adopting Gaseous Electron Multipliers (GEMs) in substitution for the Multi-Wire Proportional Counters (MWPC) either in upgrade plans or in the design stage. The ALICE experiment, for instance, is passing through upgrades that, among other goals, aim the replacement of the MWPC at the readout planes of its Time Projection Chamber (TPC) by a stack of...
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Ramona Lea (Universita e INFN Trieste (IT))Talk
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Collaboration Atlas (CERN)
Poster abstract: Precision measurements of electroweak boson production in $pp$ collisions are considered benchmark tests of the Standard Model. In particular, they provide
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verification for predictions of the electroweak theory and quantum chromodynamics (QCD). The rapidity of electroweak bosons produced in $pp$ collisions is strongly
correlated with the initial quark dynamics. Therefore,... -
Talk
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Talk
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Elisa Fontanesi (Universita e INFN, Bologna (IT))
Prospects for the study of Higgs boson pair (HH) production in the HH→bb4l (l = e, µ) channel are studied in the context of the High-Luminosity LHC. The analysis is performed using a parametric simulation of the Phase-2 CMS detector response provided by the Delphes software and assuming an average of 200 proton-proton collisions per bunch crossing at a center-of-mass energy of 14 TeV. Assuming...
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Martin Hentschinski (Universidad de las Americas, Puebla)
We investigate the energy dependence of the photo-production cross-section of vector mesons $J/\Psi$ and $\Upsilon$, which has been measured by both HERA experiments H1 and ZEUS in electron-proton collisions and by LHC experiments ALICE, CMS and LHCb in ultra-peripheral proton-proton and ultra-peripheral proton-lead collisions. Our study uses 2 particular fits of inclusive unintegrated gluon...
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Talk
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Talk
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ATLAS Collaboration
The Phase-II upgrade plan for the ATLAS Tile Calorimeter facing the High Luminosity LHC (HL-LHC) era includes approximately 1024 radiation-tolerant readout link and control boards (Daughterboards) that will provide full granularity digital data to a fully-digital trigger system off-detector through multi-Gbps optic fibers. The Daughterboard design minimises radiation-induced errors and...
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Michael Aaron Kagan (SLAC National Accelerator Laboratory (US))
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Nora Patricia Estrada Tristan
In this poster we will present the recent results from the NA62 experiment at CERN.
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NA62 is an experiment dedicated to the study of rare kaon decays. Important results such as the Brnching Ratio of $K^+ \to \pi^+ \nu \bar{\nu}$, the search for heavy neutral leptons and the serach for lepton number violating kaon decays will be shown. -
Stefano Forte (Università degli Studi e INFN Milano (IT))Talk
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ATLAS Collaboration, Damiano Vannicola (Sapienza Universita e INFN, Roma I (IT))
The ability to reconstruct almost-straight tracks with good momentum resolution is closely tided to maintaining a good understanding of the ATLAS tracking detectors' alignment and the related uncertainties. Moreover, an optimal selection of muon candidates with TeV-scale transverse momentum (pT) is a critical factor in determining the sensitivity of analyses looking for new high-mass...
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Dr Anton Babaev (Tomsk Polytechnic University)
For precise calibration of luminosity measurements, it is necessary to understand nonlinear effects which affect the single bunch instantaneous luminosity (SBIL) measured by a luminometer. The CMS BRIL group uses data from the hadronic forward (HF) calorimeter, the Pixel Luminosity Telescope (PLT), and the Fast Beam Conditions Monitor (BCM1F) to measure the luminosity. A "mu scan" is a beam...
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Eugenio Berti (Universita e INFN, Firenze (IT))
After data taking in p-p collisions at $\sqrt{s}$ = 13 TeV, the LHCf collaboration sustained a strong analysis effort in order to precisely measure neutral particle production in the very forward region at high energy. These results are expected to have a strong impact on the tuning of phenomenological models used to describe soft hadronic processes. In this contribution, we report about the...
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Mr Pablo Fierro Rojas (IF-BUAP)
One of the key signatures of collectivity in heavy-ion collisions is the appearance of a ridge structure over wide pseudorapidity interval. In this work we explore the contributions from the geometry fluctuations in the initial-state in pp collisions to the ridge structure, estimated from low to high density. Effects show to be relevant for small collision systems unlike in heavy-ion...
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Talk
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Dr Alfredo Castaneda
The Standard Model (SM) is known to be incomplete, it fails at explaining the nature of the cosmological observed dark matter. The introduction of a Dark Sector via an additional U(1)d gauge symmetry added to the SM Lagrangian provides a mechanism to introduce much needed new physics without perturbing the agreement between SM theoretical description and the Electroweak Precision Observables....
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Collaboration ATLAS (CERN), Cristiano Sebastiani (INFN Roma and Sapienza Universita' di Roma (IT))
Several new physics models predict the existence of neutral particles with macroscopic life-times that decay to pairs of leptons and light hadrons with a jet-like structure (lepton-jets). These particles, decaying outside of the interaction region, will give rise to striking signatures in the detectors at the LHC. These can be detected through numerous unconventional signatures: long...
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Collaboration ATLAS (CERN), Kenta Uno (University of Tokyo (JP))
Supersymmetry is one of the most promising theories which extend the Standard Model in order to solve the dark matter and the hierarchy problem. The squark and gluinos are one of primary targets in supersymmetry searches, as the pair production has large cross section at the LHC via the strong interaction. This poster presents recent ATLAS results from searches for gluinos and squarks in final...
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Jan Eysermans (Autonomous University of Puebla (MX))Talk
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Talk
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David Yu (Brown University (US))
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Nikolina Ilic (Nikhef National institute for subatomic physics (NL))
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Talk
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Andres Guillermo Delannoy Sotomayor (University of Tennessee (US))Talk
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Talk
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Talk
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Olaf Nackenhorst (Technische Universitaet Dortmund (DE))
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Nathan Peter Readioff (LPSC-Grenoble, CNRS/UGA (FR))Talk
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Cristian Baldenegro Barrera (The University of Kansas (US))
The existence of pseudoscalars weakly coupled to particles from the Standard Model of particle physics, known as axion-like particles (ALP), would induce anomalous scattering of light-by-light. Searching for these particles relying only on their coupling to the electromagnetic field is challenging. This process can be probed at the Large Hadron Collider (LHC) in production of photon pairs in...
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Cecilia Uribe Estrada (Autonomous University of Puebla (MX))
The High-Luminosity Large Hadron Collider (HL-LHC) upgrade aims to increase its luminosity by a factor of 5 beyond the
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LHC's design value and the integrated luminosity by a factor of 10, increasing the potential for discoveries after 2025.
The increased collision rate of particles will be a challenge for the CMS systems as higher levels of radiation could
degrade them and affect their... -
Hector Bello Martinez
The QCD factorization theorem describes the charged particles production process in strong interactions in high energy collisions. These formalism allow us to understand the perturbative (p-QCD) and non-perturbative regime of QCD. Using p-QCD it is possible to calculate the partonic cross sections of short distance processes; however, hadronic processes can not be computed fully with...
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Roberto Bonciani (Dipartimento di Fisica)Talk
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Talk
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Talk
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Talk
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Alejandro Contreras
QGP an exotic state of matter is created on heavy Ion collisions (nuclear collisions), recent results show some signals that indicate a phase transition in pp collisions, it’s well known that in the presence of QGP the production of baryons and mesons shows a clear modification, we study this observable as a signal of a deconfinament in the system, in concrete, the production of multi-strange...
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Jesús Ricardo Alvarado García (FCM)
By using the string percolation framework we study the shear and bulk viscosity over entropy ratio in addition to studying the mixed effect of the two viscosities in high multiplicity events in $pPb$ and $pp$ collisions at the current LHC energies, where evidence on collective like effects has been found recently on data. Evidence of the formation of a strongly interacting medium similar to...
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Mr Edgar Loza (Universidad de Guadalajara), Edgar Mauricio Loza Ramírez (Universidad de Guadalajara)
Fluctuations may arise from initial state fluctuations and thermodynamical fluctuations, as temperature fluctuations which is an important quantity that allows to probe the fluctuations at early stages of the reaction and to understand QCD transition order for small collision systems. A large number of particles produced at high multiplicity events on pp collisions where signals of...
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Guy Paic (Universidad Nacional Autonoma (MX))
The behavior of the underlying event density dependence on the leading particle transverse momentum has been widely reported and used to tune MC generators to the data of pp collisions. However to our knowledge all the studies have been done, both in data and generators for minimum bias data. We present a work that investigates the behavior of the underlying event in function of the...
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Carlos E.M. Wagner (University of Chicago)Talk
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ATLAS Collaboration, Mr Debottam Bakshi Gupta (University of Texas at Arlington (US))
ATLAS electron and photon triggers covering transverse energies from 5 GeV to several TeV are essential to record signals for a wide variety of physics: from Standard Model processes to searches for new phenomena in both proton-proton and heavy ion collisions. To cope with ever-increasing luminosity and more challenging pile-up conditions at the LHC, the trigger selections needed to be...
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ATLAS Collaboration
In the High Luminosity LHC, planned to start with Run4 in 2026, the ATLAS experiment will be equipped with the Hardware Track Trigger (HTT) system, a dedicated hardware system able to reconstruct tracks in the silicon detectors with short latency. This HTT will be composed of about 700 ATCA boards, based on new technologies available on the market, like high speed links and powerful FPGAs, as...
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ATLAS Collaboration
The ATLAS experiment aims at recording about 1 kHz of physics collisions, starting with an LHC design bunch crossing rate of 40 MHz. To reduce the significant background rate while maintaining a high selection efficiency for rare physics events (such as beyond the Standard Model physics), a two-level trigger system is used.
Events are selected based on physics signatures such as the presence...
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Mr Guillermo Gonzalez-Estrada (Universidad Michoacana de San Nicolas de Hidalgo), Guillermo González Estrada (UMSNH)
We revisit the rare decay of the Higgs boson into two different quarks at the one-loop level in the Standard Model. We implement the GIM mechanism in a strict manner, by performing meticulous Taylor expansions of the amplitude's form factors, in order to get rid of spurious terms. We predict Br$(H\to uc)$=$1.63\times10^{-18}$, Br$(H\to ds)$=$9.07\times10^{-15}$, Br$(H\to...
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Mr Nestor Raul Mancilla Xinto (BUAP), Maria Magdalena Castro Sam (BUAP), Ms Nadia Mariana Leal Reyes (BUAP)
We study the ratio of the pion, kaon and proton particle production on high multiplicity pp collisions at LHC energies, over the transverse momentum spectra corresponding to the energy density of a dilute system in the framework of clustering of color sources to describe the suppression due to initial state effects. Results show suppression for all the multiplicity classes with the strongest...
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Mr Fidel E. Flores-Ocampo (CICFIM-UANL)
The so called rho-pi puzzle has defied every theoretical approach, and it consists in understanding why higher-mass intermediate states are suppressed in favor of rho-pi dynamics. The study of known decays of the psi meson can shed light in solving this puzzle. In several sources it has been introduced the use of a form factor for the meson meson meson vertices due to the internal...
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ATLAS Collaboration
ALFA detector is part of the ATLAS Roman Pot detector dedicated to measure protons scattered at very small angles. ALFA aims to study elastic and diffractive events in special runs with reduced luminosity and optimized beam optics. Precision of the measurement depends on the correct positioning of the ALFA detector with respect to the actual beam position. For this purpose track-based...
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Riccardo Del Burgo (CMS, Universitaet Zuerich (CH))UpgradePoster
After the high-luminosity upgrade of the LHC (HL-LHC), the instantaneous luminosity will increase to unprecedented values of 5-7x10^34cm-2s-1. In order to cope with these conditions the whole CMS silicon tracker detector will be replaced. This presentation describes the upgrade of the inner pixel system. The new inner pixel detector will be composed of three sub-detectors: the barrel detector...
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Antonio Pich (IFIC, U. Valencia -.)
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Tim M.P. Tait (University of California, Irvine)Talk
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Tim M.P. Tait (University of California, Irvine)Talk
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Alessandro ViciniTalk
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Derek Teaney (Stony Brook University)Talk
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Marco Alberto Ayala-Torres (Center for Research and Advanced Studies (Cinvestav))
The performance of several trigger counters based on plastic scintillators with silicon photomultiplier readout is investigated with cosmic rays. Efficiency and time resolution are measured using digital waveform analysis. The obtained results are relevant for trigger subsystems of Baryonic Matter at the Nuclotron (BM@N) and Multi-Purpose Detector (MPD) at the NICA heavy-ion collider. The...
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Talk
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ATLAS Collaboration, Patrawan Pasuwan (Stockholm University (SE))
At the LHC, the number of inelastic proton-proton collisions per second is related to the luminosity. Track counting is one of the methods for luminosity measurement in the ATLAS experiment. It is done by counting the number of charged-particle tracks reconstructed in the inner detector in unbiased triggers, where the number of tracks scales with the number of interactions. Therefore, as long...
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ATLAS Collaboration, Andrzej Smykiewicz (Polish Academy of Sciences (PL))
The High Luminosity LHC (HL-LHC) aims to increase the LHC data-set by an order of magnitude in order to increase its potential for discoveries. The high pileup at the HL-LHC presents a highly challenging environment to particle detectors. To cope with this, the current Inner Detector of the ATLAS experiment will be replaced with a new all-silicon Inner Tracker (ITk). In this poster the...
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Davide Pagani (TUM - Garching bei München)Talk
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Nishita Desai (LUPM, Montpellier)
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Collaboration ATLAS Muon, Haruka Asada (Nagoya University (JP))
The High-Luminosity LHC (HL-LHC) is planned to start the operation in 2026 with an instantaneous luminosity of 7.5 x 1034 cm-2s-1. In order to cope with the event rate higher than that of LHC, the trigger and readout electronics of ATLAS Thin Gap Chamber (TGC) will need to be replaced. All hit data will be transferred from the frontend to the backend boards and exploited by an advanced...
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ATLAS CollaborationUpgrade
The Tile Calorimeter (TileCal) is the hadronic calorimeter covering the central region of the ATLAS experiment. TileCal is a sampling calorimeter with steel as absorber and scintillators as active medium. The scintillators are read-out by wavelength shifting fibers coupled to photomultiplier tubes (PMTs). The analogue signals from the PMTs are amplified, shaped, digitised by sampling the...
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Talk
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Brenda Quezadas Vivian, Ms Brenda Quezadas-Vivian (Universidad Michoacana de San Nicolas de Hidalgo)
Beyond the electromagnetic properties of the top quark, there is also great interest in its static weak properties, which are associated with their interaction with the $Z$ boson. In the present work, the analytical calculation of weak dipole moments for the top quark is presented in the context of models with generalized current sectors, where the existence of a new neutral massive gauge...
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