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Marek Bombara (Pavol Jozef Safarik University (SK))09/12/2024, 14:00
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Adam Takacs (Heidelberg University)09/12/2024, 14:20
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Antonia Strubig (Stockholm University (SE))09/12/2024, 15:30
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Silvio Donato (Universita & INFN Pisa (IT))09/12/2024, 16:20
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09/12/2024, 17:30
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Pavol Bartos (Comenius University (SK))10/12/2024, 09:00
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Silvio Donato (Universita & INFN Pisa (IT))10/12/2024, 09:45
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Michal Kreps (University of Warwick (GB))10/12/2024, 11:00
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Lucia Anna Tarasovicova (Pavol Jozef Safarik University (SK))10/12/2024, 11:45
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Daniel Tapia Takaki (University of Kansas)10/12/2024, 13:50
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Jaroslav Bielcik (Czech Technical University in Prague (CZ))10/12/2024, 14:25
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Diana Krupova (Czech Technical University in Prague (CZ))10/12/2024, 15:00
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Jaroslav Adam (Czech Technical University in Prague (CZ))10/12/2024, 15:55
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Prof. Jesus Guillermo Contreras Nuno (Czech Technical University in Prague (CZ))10/12/2024, 16:40
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Dr Gergely Gabor Barnafoldi (HUN-REN Wigner Research Centre for Physics (HU))10/12/2024, 17:05
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Juraj Bracinik (University of Birmingham (GB))11/12/2024, 09:00
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Dr Marco Musich (Universita & INFN Pisa (IT))11/12/2024, 09:45
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Michael Prouza (FZU - Institute of Physics of the Czech Academy of Sciences)11/12/2024, 10:50
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Petr Tobiska (Institute of Physics, Czech Academy of Sciences)11/12/2024, 11:35
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Patrik Čechvala (Institute of Physics, Czech Academy of Sciences)11/12/2024, 12:20
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11/12/2024, 14:00
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Pawel Kopciewicz (CERN)12/12/2024, 09:00
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Roman Lietava (University of Birmingham (GB))12/12/2024, 09:45
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Ishaan Ahuja (Pavol Jozef Safarik University (SK))12/12/2024, 10:10
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Anton Andronic (Universität Münster (DE))12/12/2024, 10:55
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Zuzana Paulinyova (Pavol Jozef Safarik University (SK))12/12/2024, 11:40
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Dr Jacopo Pinzino (Universita & INFN Pisa (IT))12/12/2024, 12:05
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Stephen Hillier (University of Birmingham (GB))12/12/2024, 14:00
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Lennart Uecker (Heidelberg University (DE))12/12/2024, 14:45
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Anton Albert Riedel (Technische Universitaet Muenchen (DE))12/12/2024, 16:00
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Manos Vourliotis (Univ. of California San Diego (US)), Silvia Goy Lopez (CIEMAT - Centro de Investigaciones Energéticas Medioambientales y Tec. (ES)), Silvia Goy Lopez (Centro de Investigaciones Energéti cas Medioambientales y Tecno), Sioni Paris Summers (CERN)12/12/2024, 16:45
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Marian Krivda (University of Birmingham (GB))12/12/2024, 17:30
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12/12/2024, 19:00
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Nicolò Jacazio (Universita e INFN, Bologna (IT))13/12/2024, 09:00
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Gergely Suranyi (Wigner Research Centre for Physics, Budapest, Hungary)13/12/2024, 09:45
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Monika Robotková (Nuclear Physics Institute, Czech Academy of Sciences)13/12/2024, 10:35
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Melinda Orosz (University of Debrecen (HU))13/12/2024, 11:00
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Sun Zhandong (HUN-REN Institute for Nuclear Research)13/12/2024, 11:25
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Peter Kalinak (Slovak Academy of Sciences (SK))13/12/2024, 11:50
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Ishaan Ahuja (Pavol Jozef Safarik University (SK))
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Dr Gergely Gabor Barnafoldi (HUN-REN Wigner Research Centre for Physics (HU))
Nuclei having 4n number of nucleons are theorized to possess clusters of α particles (4He nucleus). The Oxygen nucleus ($^{16}$O) is a doubly magic nucleus, where the presence of an α-clustered nuclear structure grants additional nuclear stability. In this study, we exploit the anisotropic flow coefficients to discern the effects of an α-clustered nuclear geometry w.r.t. a Woods-Saxon nuclear...
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Theodoros Chatzistavrou (National Technical Univ. of Athens (GR))
The CMS trigger system is undergoing significant upgrades to prepare for the challenging conditions of the High Luminosity LHC (HL-LHC), where extreme pileup and higher event rates will push the system to its limits. At Level-1 (L1), new hardware and advanced algorithms, including machine learning, are being deployed to process data at rates up to 750 kHz, approximately 7.5 times the current...
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Dr Marco Musich (Universita & INFN Pisa (IT))
CMS selects interesting events using a two-tiered trigger system. The first level (L1), composed of custom hardware processors, uses information from the calorimeters and muon detectors to select events at a rate of around 110 kHz within a fixed latency of about 4\mus. The second level, the high-level trigger (HLT), consists of a farm of processors running a version of the full event...
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Zhandong Sun
In recent studies of small system collisions at RHIC, significant suppression of high transverse momentum (high $p_T$) neutral hadrons has been observed in high-activity events, contrasted by an unexpected enhancement in low-activity events. This phenomenon, seen in $d$+Au and $p$+Au collisions at $\sqrt{s_{NN}} = 200$ GeV, challenges conventional interpretations of nuclear modification based...
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Gergely Suranyi (Wigner Research Centre for Physics, Budapest, Hungary)
HUN-REN Wigner RCP’s Regard gaseous tracking detector development team has been constructing particle detectors for almost two decades. Part of the development is a contribution to fundamental research, but there is also a growing emphasis on applied research, particularly in the field of muography. Since the pioneering measurements of the first field-use muon detector almost 15 years ago,...
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Patrik Čechvala (Institute of Physics, Czech Academy of Sciences)
Imaging Atmospheric Cherenkov Telescopes (IACTs) are specific ground-based optical telescopes with large reflective surfaces that enable the observation of high-energy cosmic gamma rays through the observation of Cherenkov light emitted by particles of Extensive Air Showers (EAS) generated by primary gamma photons in the atmosphere.
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The Single-Mirror Small Size Telescope (SST-1M) is a... -
Petr Tobiska (Institute of Physics, Czech Academy of Sciences)
The Pierre Auger Observatory is conceived to study ultra-high-energy
cosmic rays from about 10^17 eV to beyond 10^20 eV. It is a
multi-hybrid Observatory comprising 1660 surface detector stations
spread over an area of 3000 km^2 overlooked by 27 fluorescence
telescopes located at four sites at its periphery.Phase I of data-taking spanned from its beginning in 2004 to the end
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of 2022,... -
Peter Kalinak (Slovak Academy of Sciences (SK))
A transition of nuclear matter to a state of deconfined quarks and gluons
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(the Quark Gluon Plasma) occurs at sufficiently high-energy densities and temperatures. This is achieved in the laboratory by reaching these conditions with collisions of heavy nuclei in which an enhancement in the production of strange hadrons with respect to the small collision systems is observed.
Since the... -
Monika Robotková (Nuclear Physics Institute, Czech Academy of Sciences)
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Marian Krivda (University of Birmingham (GB))
A firmware for the Central Trigger Processor (CTP) at ALICE experiment for LHC Run 3 is written in VHDL language. The most of the VHDL code was verified in a simulations using a simple procedures written also in VHDL or by writing data into file and then by checking of a data consistency in a software. In addition to the simulations also a real hardware tests were performed by a test scripts....
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Melinda Orosz (University of Debrecen (HU))
The PHENIX experiment at RHIC already published results on $\pi^0$ and $\eta$ production in $\sqrt{s_{NN}}=200$\,GeV Au+Au collisions based on data taken 2004, 2007 and 2010. In the 2014 and 2016 data taking periods large amount of new data were collected, about ten times the previous statistics. This allows both to extend the $p_T$-range of the measurements and improve on systematic...
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