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Emanuele Angelo Bagnaschi (CERN/INFN Laboratori Nazionali di Frascati)27/09/2023, 09:00
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Jorgen D'Hondt (Vrije Universiteit Brussel (BE))27/09/2023, 09:05
In person
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Tatsuya Nakada (EPFL - Ecole Polytechnique Federale Lausanne (CH))27/09/2023, 09:25
In-person
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Daniel Schulte (CERN), Dr Tatiana Pieloni (EPFL)27/09/2023, 10:30
In-person
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Mogens Dam (University of Copenhagen (DK)), Nadia Pastrone (Universita e INFN Torino (IT))27/09/2023, 11:00
Remote (Mogens Dam) + in-person (Nadia Pastrone)
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Federico Buccioni27/09/2023, 11:30
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Leonhard Reichenbach (University of Bonn (DE))27/09/2023, 12:00
The Key4hep project aims to provide a turnkey software solution for the full experiment life-cycle, based on established community tools. Several future collider communities (CEPC, CLIC, EIC, FCC, and ILC) have joined to develop and adapt their workflows to use the common data model EDM4hep and common framework. Besides sharing of existing experiment workflows, one focus of the Key4hep project...
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Daniele Calzolari (CERN)27/09/2023, 12:05
Circular muon colliders offer the exciting potential to collide lepton beams at previously unattained center-of-mass energies. However, a notable technological challenge arises due to the continuous decay of stored muons. This decay introduces significant complexities for both collider and detector design. The secondary radiation fields generated by the decay electrons and positrons can...
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Carlo Giraldin27/09/2023, 12:10
In the panorama of future colliders, a muon collider represents a very promising choice that would enable a vast physics program. However, the beam-induced background generated from the decay of the muons along the ring is a challenging aspect both from the hardware and the software side. Indeed, despite the presence of a pair of tungsten absorber cones, that mitigate the flux of particles...
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Leonardo Toffolin (Universita degli Studi di Udine (IT))27/09/2023, 12:15
The Standard Model prediction for the $Z$-boson pole $b$-quark forward-backward asymmetry is calculated to be $(A_{FB}^{0,b})_{th} = 0.1030 \pm 0.0002$. From the experimental point of view, $A_{FB}^b$ as measured by the large electron-positron (LEP) collider at the $Z$-pole is $A_{FB}^{0,b} = 0.0992 \pm 0.0016$, which remains today the electroweak precision observable with the largest...
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Armin Ilg (University of Zurich)27/09/2023, 12:20
The FCC-ee is a proposed future $e^+e^-$ collider capable of producing an unparalleled number of Higgs, Z, and W bosons, as well as of top quarks, in very clean experimental conditions. Up to four experiments can detect the collision products, with IDEA being one of the proposed detector concepts. A plethora of measurements at the FCC-ee rely on precise and accurate measurements of bottom and...
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Luca Castelli27/09/2023, 12:25
Muon collisions are considered a promising mean for exploring the energy frontier, leading to a detailed study of the possible feasibility issues. Beam intensities of the order of $10^{12}$ muons per bunch are needed to achieve the necessary luminosity, generating a high flux of secondary and tertiary particles that reach both the machine elements and the detector region. A strategy to reduce...
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Alessandro Frasca (University of Liverpool (GB))27/09/2023, 12:30
The Future Circular Collider (FCC) study explores the feasibility of post-LHC colliders with a circumference of almost 100 km. As a first stage, a high-luminosity electron-positron collider (FCC-ee) is envisaged, with a beam energy ranging from 45.6 GeV (Z pole) to 182.5 GeV (ttbar threshold). The most intense radiation source at FCC-ee interaction region (IR) is the production of synchrotron...
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Gregor Krzmanc (ETH Zurich)27/09/2023, 12:35
Reconstructing particles from raw detector outputs at the FCC is a challenging task due to complex detector geometries and highly granular, unique shower shapes. Conventional computer vision approaches are typically not suitable for application to the sparse detector outputs, so other methods more suited for unstructured data shall be consulted. We employ E(n) equivariant graph neural networks...
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Shivani Sanjay Lomte (University of Wisconsin Madison (US))27/09/2023, 12:40
A future high energy muon collider can probe the multi-TeV regime and greatly improve our understanding of the Higgs self-coupling. One of the major challenges to detector performance is the beam induced background (BIB) which comes from muon decays along the beam pipe. The upstream and downstream electromagnetic showers blanket the detector with low energy photons, electrons and neutrons....
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Emanuela Musumeci (IFIC - Univ. of Valencia and CSIC (ES))27/09/2023, 12:45
The analysis of the long-range particle correlations can
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yield valuable insights into the initial state of matter and
potentially reveal the existence of Beyond the Standard Model
scenarios, such as the "Hidden Valley"(HV) one. In this work, we are
interested in QCD-like hidden sectors in which the production of HV
matter would enhance and enlarge azimuthal correlations of... -
27/09/2023, 12:55
In front of the building
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Enrico Bothmann (University of Göttingen)27/09/2023, 13:00
Remote
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Anke Biekoetter (JGU Mainz)27/09/2023, 13:30
In person
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Giovanni Dal Maso27/09/2023, 13:55
In person
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Mauro Pieroni (CERN)27/09/2023, 14:20
In person
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Iaroslava Bezshyiko (University of Zurich (CH))27/09/2023, 14:45
Remote
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Ivan Vorobyev (CERN)27/09/2023, 15:10
In person
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Richard Hawkings (CERN)27/09/2023, 16:00
In person
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Eliezer Rabinovici (Weizmann Institute of Science (IL))27/09/2023, 16:35
In person
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Francesco Giffoni, Massimo Florio27/09/2023, 17:05
Remote
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Roberto Losito (CERN)27/09/2023, 17:35
In person
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Emanuele Angelo Bagnaschi (CERN/INFN Laboratori Nazionali di Frascati), Laurent Dufour (CERN), Nima Zardoshti (CERN), Silvia Ferrario Ravasio (CERN)27/09/2023, 18:00
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Armin Ilg (University of Zurich), Emanuele Angelo Bagnaschi (CERN/INFN Laboratori Nazionali di Frascati), Lydia Brenner (Nikhef National institute for subatomic physics (NL))27/09/2023, 18:15
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