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20/06/2022, 13:00
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Maria Robles Manzano (Johannes Gutenberg Universitaet Mainz (DE))20/06/2022, 13:05
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Alessandra Palazzo (INFN Lecce e Universita del Salento (IT))20/06/2022, 13:10
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Paul Schütze (Deutsches Elektronen-Synchrotron (DE))20/06/2022, 13:20
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Alexander Gerbershagen (CERN)20/06/2022, 13:30Lecture
The lecture covers the basics of the secondary and tertiary beam generation for the test beams at CERN. It covers the basics of beam-matter interaction and summarises the processes of secondary particles production at the target stations. It introduces the Atherton parametrisation and the particle zoo available at CERN North Area. Subsequently, it covers the design of transfer beam lines, beam...
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Shuvay Singh (CERN)20/06/2022, 14:30Talk
In the context of EP R&D, CERN is developing a multi-purpose superconducting magnet test facility to be used for future detector and electronic device testing at the North Area beam-test area. The facility will serve as a replacement of the existing M1 and Morpurgo magnets that have been in operation since the late 70s. The facility is envisioned to serve all the testing requirements for the...
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Dipanwita Banerjee (CERN)20/06/2022, 14:50Talk
The CERN beam lines of the North and the East Area are designed to deliver beams of secondary and tertiary particles as well as attenuated primary protons and ions from the SPS and PS accelerators. Typically, hadrons, electrons, and muons in the energy range up to 360 GeV/c at a maximum flux of 10^7 - 10^8 particles per SPS extraction are served to the experimental areas. Following the Long...
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Ralf Diener (Deutsches Elektronen-Synchrotron (DE))20/06/2022, 15:10Talk
The DESY II Test Beam Facility was in operation from March to December in 2021, starting with local and national users before continuing from May on in normal mode welcoming international groups. After the winter shutdown, the facility resumed operation in February 2022.
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In this contribution, a review over the test beam period in 2021 and the current status is given. This includes first... -
Dohun Kim20/06/2022, 15:30Talk
The R-Weg is a former transfer beamline from the DESY II synchrotron to DORIS. Recently,
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it has been recommissioned to serve as a high-rate electron beam line. The full DESY II
beam with up to $1.5 \times 10^{10}$ e$^-$ per bunch can be dumped at a rate of 12.5 Hz. The available
high rates allow not only for precise detector tests, but also electron irradiation campaigns.
To ensure safe... -
Nathaniel Joseph Pastika (Fermi National Accelerator Lab. (US))20/06/2022, 15:50Talk
The Fermilab Test Beam Facility is a world class facility for testing and characterizing particle detectors. With two operational low intensity beam lines, the facility can deliver a variety of particle types and momenta ranging from 120 GeV protons in the primary beam line down to 200 MeV particles in the tertiary beam line. In order to meet the needs of future detectors, the facility is...
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Evan Niner (Fermilab)20/06/2022, 16:30Talk
An Irradiation Test Area(ITA) has been operating at Fermilab since 2021 with a beam delivering 400 MeV protons at an intensity up to 2.7e15 protons per hour. This talk will cover lessons learned and present status of the facility, user application process, and future upgrade plans.
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Martin R. Jaekel (CERN)20/06/2022, 16:50Talk
The upcoming High-Luminosity upgrade of the CERN Large Hadron Collider (HL-LHC) and the R&D on future accelerators (FCC) require radiation hardness tests and detector qualifications. The reference facilities at CERN for muon gas detectors is the GIF++, located on the H4 beam-line in the SPS North Area.
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The last years were dominated by the mass production tests for the ATLAS Phase 1 upgrade,... -
Blerina Gkotse (CERN)20/06/2022, 17:10Talk
The CERN Proton Irradiation Facility (IRRAD) is a reference facility for performing irradiation experiments and qualification of tracking and calorimetry detectors, important for the upgrade of CERN Large Hadron Collider (HL-LHC) and for the R&D on future CERN accelerators. After the CERN Long Shutdown 2, the IRRAD facility has undergone through several changes on hardware and software...
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Adrian Herkert (Deutsches Elektronen-Synchrotron (DE))20/06/2022, 17:30Talk
Beam telescopes have become integral to the infrasctructure of many test beam facilities today. At the DESY II Test Beam the EUDET-type beam telescopes have represented the standard for the better part of a decade by now. The monolithic architecture of the MIMOSA26 pixel sensor combined with the small pitch (18.4 µm) makes it particularly suited for tracking low momentum particles.
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In the... -
Milou Van Rijnbach (University of Oslo (NO))20/06/2022, 17:50Talk
MALTA is part of the Depleted Monolithic Active Pixel sensors designed in TowerJazz 180nm imaging technology. The MALTA sensor has been produced on Cz substrates in view of optimising the signal for efficiency and time resolution. A custom telescope with MALTA planes has been developed for a testbeam campaign at SPS (CERN) using up to six MALTA tracking planes and the ability to host several...
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Federico Ronchetti (Universita degli Studi dell'Insubria & INFN, Milano-Bicocca (IT))20/06/2022, 18:10Talk
The INSULAB beam test setup is made up by different detectors for
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precision tracking, trigger setup, multiplicity counting and energy
measurements. The tracking system consists in a set of double-sided
microstrip silicon telescopes with a high spatial resolution (~ 5 um)
and large area single-sided microstrip silicon detector (resolution down
to ~ 30 um) for the precise measurements of... -
Kazuyoshi Carvalho Akiba (Nikhef)20/06/2022, 18:30Talk
A single arm beam telescope based on the recently developed Timepix4 ASIC was built in order to perform first tests of synchronous multiple-detector readout and track reconstruction. The Timepix4 is a hybrid pixel detector readout ASIC designed to record time-of-arrival (TOA) and time-over-threshold (TOT) simultaneously in each pixel. It has a 448x512 pixel matrix with square pixels at a 55 μm...
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Ryan Heller (Fermi National Accelerator Lab. (US))20/06/2022, 18:50Talk
The Fermilab Test Beam Facility (FTBF) featured an all-silicon telescope based on pixel detectors from the phase-0 of the CMS pixel detector. In the past few years, the demand for more precision tracking pushed the facility to upgrade the pixel telescope with newer and more precise silicon strip detectors. In the past few months, the facility decided to simplify the system removing the old...
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Michael Campbell (CERN)21/06/2022, 09:00Lecture
Hybrid pixel detectors were first developed to address the needs of particle tracking at the heart of the large LHC experiments. The key property of these detectors is the ability to detect particles with a high signal to noise ratio even at very high speed permitting clean reconstruction of the LHC events. In the Medipix project we adapted the same hybrid pixel approach firstly to X-ray...
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David Cussans (University of Bristol (GB))21/06/2022, 10:20Talk
Beam-lines supported by the EUDET, AIDA and AIDA-2020 projects provided a standard hardware and software interface for triggering and synchronization between any beam-telescope installed on the beam-line. The hardware used is called a Trigger/Timing Logic Unit (TLU).
The AIDA-Innova project will provide a new TLU with a higher specification than the existing EUDET and AIDA(-2020) TLUs while...
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Alexander Becker ((for the CMS collaboration))21/06/2022, 10:40Talk
The endcap calorimeters of CMS will be upgraded a single High Granularity Calorimeter (HGCAL) for the HL-LHC. The HGCAL is a sampling calorimeter that will use silicon sensors as well as scintillator tiles as active material and be operated at -30 C. The silicon section will have several sensor thicknesses and there will be multiple sensor geometries based on 8" wafers. The readout of the...
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Lucian Scharenberg (CERN, University of Bonn (DE))21/06/2022, 11:00Talk
RD51 is a CERN-based research collaboration, focusing on the development and advancement of Micro-Pattern Gaseous Detectors (MPGDs). One of the major outcomes of these activities was the development of a joint multi-purpose electronic readout system, the Scalable Readout System (SRS). It allows to read out small R&D set-ups up to mid-sized experiments with various front-end ASICs (APV25 and...
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Eric Buschmann (CERN)21/06/2022, 11:20Talk
Developing a new silicon detector requires significant effort for preparing the readout hardware and software for the prototype to be operated in the laboratory and test beams. The Caribou DAQ framework significantly reduces the development effort and cost for such readout systems. By utilizing modern system-on-chip (SoC) platforms, it combines programmable logic and a processing system and...
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Simon Spannagel (Deutsches Elektronen-Synchrotron (DE))21/06/2022, 11:40Talk
Allpix Squared is a versatile, open-source simulation framework for silicon pixel detectors. Its goal is to ease the implementation of detailed simulations for both single sensors and more complex setups with multiple detectors. While originally created for silicon detectors in high-energy physics, it is capable of simulating a wide range of detector types for various application scenarios,...
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Adriana Simancas (Deutsches Elektronen-Synchrotron (DE))21/06/2022, 12:00Talk
Monolithic CMOS sensors have found their way through imaging technologies into High Energy Physics thanks to multiple advantages in particle detection. Their main characteristic is the integration of an active sensor and readout in a single chip, which provides a reduction in production effort, costs and material. The Tangerine project aims to develop the next generation of silicon pixel...
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Manuel Alejandro Del Rio Viera (Deutsches Elektronen-Synchrotron (DE))21/06/2022, 12:20Talk
The rapid evolution of High Energy Physics experiments demands the development of improved detectors. The Tangerine project’s goal is to develop the next generation of small collection electrode monolithic silicon pixel detectors using the 65nm CMOS imaging process which offers a higher logic density and overall lower power consumption compared to previously used processes. One objective of...
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Sara Ruiz Daza21/06/2022, 12:40Talk
Monolithic CMOS sensors enable the development of detectors with a low material budget and a low fabrication cost. Moreover, using a small collection electrode results in a small sensor capacitance, a low analogue power consumption, and a large signal-to-noise ratio. These characteristics have become very attractive in the development of new silicon sensors for charged particle tracking at...
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Jan Visser (Nikhef National institute for subatomic physics (NL))21/06/2022, 14:30Tutorial
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Walter Wuensch (CERN)22/06/2022, 09:00Lecture
A very hot topic in radiation oncology is so-called FLASH therapy which involves delivering an entire radiation treatment in a few hundred ms, or less. This fast delivery can reduce toxicity to healthy tissue while maintaining tumor control expanding the parameter space for treatment. The effect has been observed in experiments and clinical translation is now underway. As part of this effort,...
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Gianpiero Vignola (Deutsches Elektronen-Synchrotron (DE))22/06/2022, 10:20Talk
The characteristics of the Monolithic Active Pixel Sensors such as small thicknesses, pixel pitches and cost have made this detector type increasingly attractive for applications in high energy physics in recent years. The TANGERINE project at DESY aims to push research in this field in order to develop a fully integrated 65 nm CMOS pixel chip for future application in beam-test facilities or...
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Rudy Ceccarelli (Universita e INFN, Firenze (IT))22/06/2022, 10:40Talk
The High Luminosity upgrade of the CERN Large Hadron Collider (HL-LHC) calls for new high-radiation tolerant silicon pixel sensors, capable of withstanding fluences up to 2.3E16 neq/cm2 (1MeV equivalent neutrons). In this presentation results obtained in beam tests experiments with 3D and planar pixel sensors interconnected with the RD53A readout chip are reported. RD53A is the first prototype...
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Mr Roberto Russo (Nikhef National institute for subatomic physics (NL))22/06/2022, 11:00Talk
The ALPIDE telescope is a continuously evolving tracking telescope based on the TowerJazz 180 nm CMOS ALICE PIxel DEtector (ALPIDE). The ALPIDE is a high efficiency, high spatial resolution monolithic active pixel sensor designed for the recently commissioned ALICE Inner Tracker System (ITS2).
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This telescope is one of the main R&D tools for the test and characterization of new sensors and... -
Surabhi Sharma (Deutsches Elektronen-Synchrotron (DE))22/06/2022, 11:20Talk
Future particle physics experiments are motivated by the increase in luminosity and thus the need for intelligent tracking detectors providing fast track and momentum information to select events of interest. The next generation tracking detectors are mostly all silicon detectors and thus finding a cost effective solution to maximize the output is important. Therefore the commercial CMOS...
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John Dervan (Northeastern University (US))22/06/2022, 11:40Talk
The Compact Muon Solenoid (CMS) detector at the CERN Large Hadron Collider (LHC) is undergoing an extensive upgrade program to prepare for the challenging conditions of the High-Luminosity LHC (HL-LHC). A new timing detector in CMS will measure minimum ionizing particles (MIPs) with a time resolution of 30-40 ps for MIP signals at a rate of 2.5 Mhit/s per channel at the beginning of HL-LHC...
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Ryan Heller (Fermi National Accelerator Lab. (US))22/06/2022, 12:00Talk
Low-gain avalanche diodes (LGADs) will be employed in the CMS MIP Timing Detector (MTD) upgrade to mitigate the high levels of pileup expected in the High Luminosity phase of the LHC. Over the last several years, LGAD sensors with radiation tolerant gain implants have been developed, successfully providing gain even after the fluences expected at the HL-LHC, in excess of 1 x 10^15 neq/cm^2....
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Dr Vagelis Gkougkousis (CERN)22/06/2022, 12:20Talk
The proven radiation hardness of 3D technologies up to fluencies exceeding 1$x10^{16}n_{eq}/cm^{2}$ makes them a prime candidate for next generation high energy physics experiments. In addition, the decoupling of the charge generation and drift volumes unique in these structures, provides excellent timing characteristics without radiation hardness comprise or the need for additional...
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Justus Braach (CERN, Hamburg University (DE))22/06/2022, 12:40Talk
Vertex and tracking detectors for future high-energy physics experiments face stringent requirements in view of their spatial and temporal measurement performance as well as the projected experimental conditions.
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Within the ATTRACT FASTPIX project, a monolithic pixel sensor demonstrator chip has been developed in a modified 180 nm CMOS imaging process technology, targeting sub-nanosecond... -
Theo Moretti (Universite de Geneve (CH))22/06/2022, 14:00Talk
"The MONOLITH ERC Advanced project targets the development of very thin monolithic pixel sensors capable of reaching picosecond-level resolution combined with high granularity. To achieve such performance the project profits from the 130nm SiGe BiCMOS technology by IHP to produce very fast, low noise and low power front-end electronics. Small prototypes have been tested at the H8 SPS beam...
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Mr Matteo Milanesio (Universite de Geneve (CH))22/06/2022, 14:20Talk
The MONOLITH H2020 ERC Advanced project aims at the development of fully monolithic highly granular pixel sensors with picosecond time stamping capabilities. To reach a picosecond precise sensor response, a thin gain layer has been implemented deep inside a high-resistivity epitaxial layer. By moving the gain layer away from the pixel implantation, the pixel size can be reduced down to 50 µm,...
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Berkan Kaynak (CERN, Istanbul University (TR))22/06/2022, 14:40Talk
Test beams are frequently used for developing high resolution Time-of-Flight (ToF) equipment. To investigate the timing properties of detectors under test, a reliable and reproducible time reference counter (TRC) would be an important asset for a test beam facility. Frequently ToF detectors are calibrated only occasionally and it may be difficult to guarantee that their calibration is...
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Nicola Minafra (The University of Kansas (US))22/06/2022, 15:00Talk
The Extra Low Energy Antiproton (ELENA) is the new deceleration ring installed in the Antimatter Factory at CERN. Thanks to the introduction of ELENA, the antimatter experiments will receive an antiproton beam with an energy down to 100 keV, allowing improved performance and opening the door to new and exciting discoveries.
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On the other hand, such a low energy beam required the development of... -
Sofia Colombi22/06/2022, 15:20Talk
The FOOT (FragmentatiOn Of Target) collaboration aims at improving cancer treatments in particle therapy and optimizing passive countermeasures in space radioprotection by studying the interaction of typical beams with reference targets. On the one hand, particle therapy employs proton and carbon beams to deliver a uniform dose in the tumor region, minimizing the damage to the surrounding...
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Federica Cuna (INFN Lecce e Universita del Salento (IT))22/06/2022, 15:40Talk
Particle identification is one of the crucial and difficult task for the high energy physics experiments, like the future FCC-ee, CEPC, SCTF. The ionization of matter by charged particles is the primary mechanism used for particle identification (dE/dx), but the large uncertainties in the total energy deposition represent a limit to the particle separation capabilities. The cluster counting...
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Gordana Lastovicka Medin (University of Montenegro (ME))22/06/2022, 16:00Talk
In this presentation we highlight the most significant outcomes from the systematic study of heavily Irradiated LGAD using the femtosecond laser test beam facility at ELI Beamlines. Instability and LGAD’s deaths associated to Single Event Burnout (SEB) from Highly Ionising Particles (HIP) are tested. Questions such as what the safe margin for operation is; is the sensor mortality a threshold...
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Dr Anatoli Romaniouk (National Research Nuclear University MEPhI (RU))23/06/2022, 09:00Lecture
Transition radiation detectors is one of the not destructive particle Identification techniques widely used in high energy and cosmic-ray physics.
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The change of the electromagnetic field of a charged particle at a transition between media with different refractive indices leads to the emission of electromagnetic radiation, so-called transition radiation (TR). In the optical range transition... -
Louie Dartmoor Corpe (CERN)23/06/2022, 10:20Talk
The expected increase of the particle flux at the high luminosity phase of the LHC (HL-LHC) with instantaneous luminosities up to L ≃ 7.5×1034 cm−2 s-1 will have a severe impact on the ATLAS detector performance. The pile-up is expected to increase on average to 200 interactions per bunch crossing. The reconstruction and trigger performance for electrons, photons as well as jets and transverse...
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Adam Rennie (University of Glasgow (GB))23/06/2022, 10:40Talk
The Phase-II upgrade of the LHC during Long Shutdown 3 (LS3) aims to reach a peak instantaneous luminosity of $7.5\times 10^{34}\mathrm{cm^{-2}s^{-1}}$, which corresponds to an average of about 200 inelastic proton-proton collisions per beam-crossing. To cope with these conditions, the ATLAS tracking system will be replaced by an all-silicon Inner Tracker (ITk). The ITk will be operational for...
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Radek Privara (Palacky University (CZ))23/06/2022, 11:00Talk
In order to cope with the occupancy and radiation doses expected at the High-Luminosity LHC, the ATLAS experiment will replace its Inner Detector with an all-silicon Inner Tracker (ITk), containing pixel and strip subsystems. The strip subsystem will be built from modules, consisting of one n+-in-p silicon sensor, one or two PCB hybrids containing the front-end electronics, and one powerboard...
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Sejla Hadzic (Max Planck Society (DE))23/06/2022, 11:20Talk
For the HL-LHC upgrade, the current tracking system of the ATLAS experiment will be replaced by an all-silicon system, called the Inner Tracker (ITk), consisting of an inner Pixel Detector and an outer Strip Detector.
Go to contribution pageThe ITk Pixel Detector has two types of modules foreseen: triplet modules with 3D sensors in the innermost layer, and quad modules with planar sensors in the other... -
6. Study of the ATLAS Tile Calorimeter response to beams of particles using Phase II upgrade readoutTamar Zakareishvili (Ivane Javakhishvili Tbilisi State University (GE))23/06/2022, 11:40Talk
The Large Hadron Collider (LHC) Phase II upgrade aims to increase the instantaneous accelerator luminosity.
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A new readout system of the ATLAS Tile Calorimeter (TileCal) is needed to meet the trigger's requirements, to cope with the higher radiation levels and the ageing of the current electronics. It has to handle longer latencies of up to 35 µs at such high pileup levels.
Prototypes of the... -
Sahibjeet Singh (University of Toronto (CA))23/06/2022, 12:00Talk
The Liquid Argon Calorimeters are employed by ATLAS for all electromagnetic calorimetry in the pseudo-rapidity region |η| < 3.2, and for hadronic and forward calorimetry in the region from |η| = 1.5 to |η| = 4.9. They also provide inputs to the first level of the ATLAS trigger. After successful period of data taking during the LHC Run-2 between 2015 and 2018 the ATLAS detector entered into the...
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54. The monolithic ASIC for the high precision preshower detector of the FASER experiment at the LHCChiara Magliocca (Universite de Geneve (CH))23/06/2022, 12:20Talk
The FASER experiment at the LHC will be instrumented with a high precision W-Si preshower to identify and reconstruct electromagnetic showers produced by two O(TeV) photons at distances down to 200µm.
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The new detector will feature a monolithic silicon ASIC with hexagonal pixels of 65 µm side, with extended dynamic range for the charge measurement and capability to store the charge information... -
Markus Tobias Prim (University of Bonn (DE))23/06/2022, 12:40Talk
FASER, or the Forward Search Experiment, is a new experiment at CERN designed to complement the LHC's ongoing physics programme, extending its discovery potential to light and weakly-interacting particles that may be produced copiously at the LHC in the far-forward region. New particles targeted by FASER, such as long-lived dark photons or dark scalars, are characterised by a signature with...
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Paul Schütze (Deutsches Elektronen-Synchrotron (DE)), Adriana Simancas (Deutsches Elektronen-Synchrotron (DE)), Manuel Alejandro Del Rio Viera (Autonomous University of Puebla (MX)), Simon Spannagel (Deutsches Elektronen-Synchrotron (DE))23/06/2022, 14:00Tutorial
Scope of the tutorial
The goal of this interactive tutorial is to understand the usage of basic functionalities of the Allpix Squared simulation framework, and methods to extract some of the relevant quantities for sensor studies. Participants are encouraged to follow along on their own computers. A task and instructions will be provided and walked through, covering the basic concepts of...
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Lennart Huth (Deutsches Elektronen-Synchrotron (DE))23/06/2022, 14:00Tutorial
The AIDA trigger logic unit and EUDAQ2 provide a common infrastructure platform to integrate a large variety of devices with the EUDET-type reference telescopes at test beams. Since test-beam time is always limited, users rely on a stable and common interface for their devices. The tutorial will provide a solid basis to optimally prepare your next successful test beam campaign.
The tutorial...
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Lennart Huth (Deutsches Elektronen-Synchrotron (DE))23/06/2022, 16:30Tutorial
The AIDA trigger logic unit and EUDAQ2 provide a common infrastructure platform to integrate a large variety of devices with the EUDET-type reference telescopes at test beams. Since test-beam time is always limited, users rely on a stable and common interface for their devices. The tutorial will provide a solid basis to optimally prepare your next successful test beam campaign.
The tutorial...
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Finn Feindt (Deutsches Elektronen-Synchrotron (DE))23/06/2022, 16:30Tutorial
Corryvreckan is a software framework dedicated to the analysis of test-beam data. It employs a modular concept, providing algorithms for typical analysis steps like pixel masking, clustering, tracking, alignment and for the reconstruction of commonly investigated observables like detection efficiency, spatial and temporal resolution or material budget. This approach allows for a flexible...
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Younes Otarid (DESY)24/06/2022, 09:00Talk
The Large Hadron Collider (LHC) will undergo a major “High Luminosity” upgrade with the goal of delivering a peak instantaneous luminosity of about $5-7.5 \times 10^{34}cm^{-2}s^{-1}$ by 2027. In order for the CMS experiment to cope with the higher radiation levels and data rates, the current CMS Silicon Tracker will be replaced. The upgraded Outer Tracker will introduce a new module concept,...
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Ginger Cheng (Deutsches Elektronen-Synchrotron (DE))24/06/2022, 09:20Talk
The foreseen Large Hadron Collider upgrade is expected to deliver an integrated luminosity that is one order of magnitude larger after 2027. Rare processes and new phenomena may be observed in this high luminosity era. The Phase-II Outer Tracker upgrade of the CMS experiment is required to surmount higher radiation and increased event rate. Transverse momentum ($P_T$) discrimination is...
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Anna Stamerra (Universita e INFN, Bari (IT))24/06/2022, 09:40Talk
The High-Luminosity LHC (HL-LHC) will deliver proton-proton collisions at 5-7.5 times the nominal LHC luminosity, with an expected number of 140-200 pp-interactions per bunch crossing. To maintain the performance of muon triggering and reconstruction under high background radiation, the forward part of the Muon spectrometer of the CMS experiment will be upgraded with Gas Electron Multiplier...
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Liliana Congedo (University of Bari and Istituto Nazionale di Fisica Nucleare - Bari)24/06/2022, 10:00Talk
Resistive Plate Chambers are operated in several experiments tipically with large fractions of Tetrafluoroethane (C2H2F4) commonly known as R134a, a gas with a high Global Warming Potential (GWP) that has been recently banned by the European Union.
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Within the HEP Community, many studies are ongoing to find a good replacement for such component for RPCs working in avalanche mode. One... -
24/06/2022, 10:20Talk
EXTRA - Electron X-ray Transition RAdiation - is the experiment of one of the 2021 winning teams of the Beamline for Schools (BL4S) competition.
In this contribution, the students will present their experiment, show results and share their experiences from their participation in BL4S
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Mr Malinda de Silva (Deutsches Elektronen-Synchrotron (DE))24/06/2022, 11:00Talk
For the HL-LHC phase, the calorimeter endcap of the CMS detector will be upgraded with a High Granularity Calorimeter (HGCAL), a sampling calorimeter which will use silicon sensors as well as scintillator tiles read out by silicon photomultipliers (SiPMs) as active material (SiPM-on-tile). The complete HGCAL will be operated at -30 degC. The SiPMs will be used in areas where the expected...
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Mr Fabian Hummer (Max-Planck-Institut fuer Physik)24/06/2022, 11:20Talk
The SiPM-on-Tile technology, where small plastic scintillator tiles are directly read out with SiPMs, has been developed for the CALICE Analog Hadron Calorimeter (AHCAL), and has been adopted for parts of the hadronic section of the CMS HGCAL. For future electron-positron colliders, a single cell time stamping on the sub-nanosecond level for energy deposits corresponding to single...
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Ms Alpana Alpana (Indian Institute of Science Education and Research (IN))24/06/2022, 11:40Talk
Calorimetry at the High Luminosity-Large Hadron Collider faces two enormous challenges particularly in the forward direction: radiation tolerance and unprecedented in-time event pileup. To meet these challenges, the CMS experiment has decided to replace its current endcap calorimeters with a High Granularity Calorimeter (HGCAL), featuring a previously unrealized transverse and longitudinal...
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Antoine Laudrain (Johannes Gutenberg Universitaet Mainz (DE))24/06/2022, 12:00Talk
The Analogue Hadron Calorimeter (AHCAL) developed by the CALICE collaboration is a scalable engineering prototype for a detector at future electron-positron energy frontier colliders. It is a sampling calorimeter of steel absorber plates and 3*3 cm^2
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plastic scintillator tiles individually read out by silicon photomultipliers (SiPMs) as active material. The front-end ASICS (SPIROC2E) are... -
Steffen Stärz (McGill University, (CA))Talk
A new era of hadron collisions will start around 2029 with the High-Luminosity LHC which will allow to collect ten times more data than what has been collected during 10 years of operation at LHC. This will be achieved by higher instantaneous luminosity at the price of higher number of collisions per bunch crossing.
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In order to withstand the high expected radiation doses, the ATLAS Liquid... -
Paul Schütze (Deutsches Elektronen-Synchrotron (DE)), Adriana Simancas (Deutsches Elektronen-Synchrotron (DE)), Manuel Alejandro Del Rio Viera (Autonomous University of Puebla (MX)), Simon Spannagel (Deutsches Elektronen-Synchrotron (DE))Tutorial
Scope of the tutorial
The goal of this interactive tutorial is to understand the usage of basic functionalities of the Allpix Squared simulation framework, and methods to extract some of the relevant quantities for sensor studies. Participants are encouraged to follow along on their own computers. A task and instructions will be provided and walked through, covering the basic concepts of...
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Jan Visser (Nikhef National institute for subatomic physics (NL))Talk
Historically, one can point to innovations that were a result of earlier efforts to build detectors for particle physics experiments or to work together more effectively. Two such developments, indispensable in our everyday life are the invention of the world wide web and the touch screen at CERN; combined in nearly all our phones.
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Nowadays, we could be asked to show what societal benefits... -
Finn Feindt (Deutsches Elektronen-Synchrotron (DE))Tutorial
Corryvreckan is a software framework dedicated to the analysis of test-beam data. It employs a modular concept, providing algorithms for typical analysis steps like pixel masking, clustering, tracking, alignment and for the reconstruction of commonly investigated observables like detection efficiency, spatial and temporal resolution or material budget. This approach allows for a flexible...
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