Conveners
YSF Plenary
- Andreas Salzburger (CERN)
YSF Plenary
- Paolo Calafiura (Lawrence Berkeley National Lab. (US))
YSF Plenary
- Paolo Calafiura (Lawrence Berkeley National Lab. (US))
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Nilotpal Kakati (Weizmann Institute of Science (IL))01/06/2022, 11:10Plenary
Flavor tagging, the identification of jets originating from b and c quarks, is a critical component of the physics program of the ATLAS experiment at the Large Hadron Collider (LHC). Current flavor tagging algorithms rely on the outputs of "low level" taggers, which focus on particular approaches for identifying the experimental signature of heavy flavor jets. These low level taggers are a...
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Izaac Sanderswood (Univ. of Valencia and CSIC (ES))01/06/2022, 11:30Plenary
The physics reach of the LHCb detector can be extended by reconstructing particles with a long lifetime that decay downstream of the dipole magnet, using only hits in the furthest tracker from the interaction point. This allows for electromagnetic dipole moment measurements, and increases the reach of beyond the Standard Model long-lived particle searches. However, using tracks to reconstruct...
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André Günther (Ruprecht Karls Universitaet Heidelberg (DE))01/06/2022, 11:50Plenary
In Run 3 of the LHC the LHCb experiment faces very high data rates containing beauty and charm hadron decays. Thus the task of the trigger is not to select any beauty and charm events, but to select those containing decays interesting for the LHCb physics programme. LHCb has therefore implemented a real-time data processing strategy to trigger directly on fully reconstructed events. The first...
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Jackson Carl Burzynski (Simon Fraser University (CA))01/06/2022, 12:10Plenary
Searches for long-lived particles (LLPs) are among the most promising avenues for discovering physics beyond the Standard Model at the LHC. However, displaced signatures are notoriously difficult to identify due to their ability to evade standard object reconstruction strategies. In particular, the default ATLAS track reconstruction applies strict pointing requirements which limit sensitivity...
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Carlos Francisco Erice Cid (Boston University (US))02/06/2022, 10:00Plenary
The high luminosity expected from the LHC during the Run 3 and, especially, the Phase II of data taking introduces significant challenges in the CMS event reconstruction chain. The additional computational resources needed to treat this increased quantity of data surpass the expected increase in processing power for the next years.
As a possible solution to this problem, CMS is...
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Anna Alicke02/06/2022, 10:20Plenary
The PANDA experiment at FAIR (Facility for Antiproton and Ion Research) in Darmstadt is a fixed target experiment currently under construction. The accelerator will be operated at energies from 1.5 GeV/c to 15 GeV/c to perform hadron specroscopy and nuclear structure studies. In this context, the production and decay of heavy baryons containing strange quarks, so called hyperons, is of...
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Rocky Bala Garg (Stanford University (US))02/06/2022, 10:40Plenary
The particle track reconstruction is one of the most important part of the full event reconstruction chain and has a profound impact on the detector and physics performance. The underlying tracking software is also very complex and consists of a number of mathematically intense algorithms, each dealing with a particular tracking sub-process. These algorithms have many input parameters, to be...
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Mr Adeel Akram (PANDA Collaboration)02/06/2022, 11:30Plenary
The main purpose of the PANDA (anti-Proton ANnihilation at DArmstadt) experiment at FAIR (Facility for Anti-proton and Ion Research) is to study strong interactions at the scale where quarks form hadrons. In PANDA, a continuous beam of anti-protons ($\bar{p}$), 1.5 GeV/c to 15 GeV/c, will impinge on a fixed hydrogen ($p$) target inside the High Energy Storage Ring (HESR). This creates optimal...
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Alexander Thaler (University of Innsbruck (AT)), David Munoz Perez (Univ. of Valencia and CSIC (ES)), Javier Jimenez Pena (Max Planck Society (DE)), Mariam Chitishvili (Instituto de Física Corpuscular (IFIC)), Paolo Sabatini (Instituto de Fisica Corpuscular (IFIC), Centro Mixto Universidad de Valencia - CSIC)02/06/2022, 11:50Plenary
The algorithm used in the alignment of the Inner Detector of the ATLAS experiment is based on the track-to-hit residual minimization in a sequence of hierarchical levels (ranging from mechanical assembly structures to individual sensors). It aims to describe the detector geometry and its changes in time as accurately as possible, such that the resolution is not degraded by an imperfect...
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Mr Brij Kishor Jashal (Instituto de Física Corpuscular, Valencia)02/06/2022, 12:10Plenary
The LHCb Upgrade in Run 3 has changed its trigger scheme for a full software selection in two steps. The first step, HLT1, will be entirely implemented on GPUs and run a fast selection aiming at reducing the visible collision rate from 30 MHz to 1 MHz.
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This selection relies on a partial reconstruction of the event. A version of this reconstruction starts with two monolithic tracking... -
David Lange (Princeton University (US))Plenary
my abs
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Dominika Karwiec (Warwick)Plenary
There have been several successful examples of Graph Neural Networks (GNNs) applied to the problem of charged particle tracking, including in high-density environments like that of the HL-LHC. Many of these applications have focused on edge-classifying GNNs that are a component of a multi-step pipeline including graph construction, GNN inference, and clustering on the classified edges....
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