18–22 May 2025
Europe/Rome timezone

Contribution List

51 out of 51 displayed
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  1. 18/05/2025, 14:00
  2. Angelo SCRIBANO, Christophe Royon (The University of Kansas (US))
    19/05/2025, 09:00
  3. Irene Dutta (Fermi National Accelerator Lab. (US))
    19/05/2025, 09:05
  4. Clarissa Buti (Universita e INFN, Firenze (IT))
    19/05/2025, 09:35
  5. Thomas Conneely (Photek LTD)
    19/05/2025, 10:05
  6. Valentina Sola (Universita e INFN Torino (IT))
    19/05/2025, 11:00
  7. Simon Zhamkochyan (A.I. Alikhanyan National Science Laboratory (Yerevan Physics Institute))
    19/05/2025, 11:30

    A new high-precision timing sensor — the Radio-Frequency Photo Multiplier Tube (RF PMT) — has been recently developed and tested. The detector performs circular scanning of photoelectrons or secondary electrons using a dedicated radio-frequency (RF) deflector operating at 500–1000 MHz. The scanned electrons are detected by a position-sensitive system comprising dual chevron microchannel plates...

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  8. Alexander Kiselev
    19/05/2025, 12:00
  9. 19/05/2025, 12:30
  10. Alexander Davidson (University of Warwick (GB))
    19/05/2025, 15:00

    Owing to their single photon sensitivity and fast rise time, micro-channel-plate photomultipliers (MCP-PMTs) make a good candidate for photon detectors for the Time Of Internally Reflected Cherenkov light detector (TORCH) that is proposed as part of the phase two upgrade of the LHCb experiment. TORCH has a target time resolution per photon of approximately 70 ps, required to achieve an...

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  11. Paul Rene Michel Lecoq (CERN)
    19/05/2025, 15:30
  12. Umberto Savino (Universita e INFN Torino (IT))
    19/05/2025, 16:00

    In the LHC Long Shutdown 3, the ALICE experiment at the LHC will upgrade the three innermost layers of its Inner Tracking System (ITS). This next-generation tracking detector will feature wafer-scale, truly cylindrical Monolithic Active Pixel Sensors (MAPS) fabricated using a 65 nm CMOS imaging process. The sensors, thinned to 50 $\mu m$, will be flexible enough to form ultra-lightweight...

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  13. Prof. Jon Lapington (University of Leicester (GB))
    19/05/2025, 17:00

    MCP-PMT devices represent the state-of-the-art in terms of picosecond timing resolution combined with low noise, high gain, and radiation hardness. However, with experiment upgrades producing higher luminosities, there are concerns over the ability of the existing technologies to achieve sufficiently high rates and longer tube lifetime in terms of extracted charge. To overcome these...

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  14. Dmitry Orlov (Photonis Netherlands), Dmitry Orlov
    19/05/2025, 17:30
  15. 19/05/2025, 18:00
  16. David Gascon (University of Barcelona (ES))
    20/05/2025, 09:00
  17. Andrew Arzac
    20/05/2025, 09:30

    We have recently submitted for fabrication PSEC5, an 8-channel mixed-signal waveform-sampling ASIC targeting 1 ps timing resolution, 200 ns buffer length, and multi-hit capability. Here, we describe the architecture and development process of a modular test system for PSEC5. The system consists of two PCBs: a Design Under Test (DUT) Board, and a Control Board. The Control Board is based on the...

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  18. Dr Camilla Maggio (CAEN SpA)
    20/05/2025, 10:00

    The System for on-Axis Neutrino Detection (SAND), part of the Deep Underground Neutrino Experiment (DUNE), is designed to monitor the long-term stability of the neutrino beam at Fermilab. SAND reuses the lead scintillating-fiber electromagnetic calorimeter (ECAL) of the KLOE experiment with excellent time and energy resolutions. The calorimeter is read-out by approximately 5000 PMTs requiring...

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  19. Dominique Robert Breton (Université Paris-Saclay (FR))
    20/05/2025, 11:00
  20. Mr Richmond Yeung (University of Chicago)
    20/05/2025, 11:30

    1-ps timing resolution is the entry point to signature-based searches relying on secondary/tertiary vertices and particle identification. We describe PSEC5, an 8-channel 40 GS/s waveform-sampling ASIC in the TSMC 65 nm process targetting 1 ps resolution at 20 mW power per channel.
    Each channel consists of four fast and one slow switched capacitor arrays (SCA), allowing ps time resolution...

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  21. Giulia Gioachin (Politecnico di Torino (IT))
    20/05/2025, 12:00
  22. 20/05/2025, 12:30
  23. Paul Rene Michel Lecoq (CERN)
    20/05/2025, 15:00

    Recent advancements in scintillation detection and imaging have focused on two emerging concepts: metascintillators and nanophotonic scintillators. Metascintillators leverage an energy-sharing approach with at least two scintillator components: one with high stopping power and another with fast response characteristics. Conversely, nanophotonic scintillators integrate scintillating materials...

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  24. florian Gautier
    20/05/2025, 15:30
  25. Christophe Royon (The University of Kansas (US))
    20/05/2025, 16:00
  26. Pablo Yepes Stork (Rice University (US))
    20/05/2025, 17:00
  27. Dominik Dannheim (CERN)
    20/05/2025, 17:30

    The increase of the particle flux (pile-up) at the HL-LHC with instantaneous luminosities up to L ≃ 7.5 × $10^{34}$ cm$^{−2}$s$^{−1}$ will have a severe impact on the ATLAS detector reconstruction and trigger performance. The end-cap and forward region where the liquid Argon calorimeter has coarser granularity and the inner tracker has poorer momentum resolution will be particularly affected....

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  28. 20/05/2025, 18:00
  29. Alessio Ghezzi (Universita & INFN, Milano-Bicocca (IT))
    21/05/2025, 09:10

    The Electromagnetic Calorimeter ECAL of the CMS experiment at the Large Hadron Collider at CERN is a homogeneous calorimeter made of lead tungstate scintillating crystals. An upgrade of ECAL is in preparation to cope with the challenging conditions anticipated for the High Luminosity phase of LHC. The endcap part of the ECAL will be replaced by a new detector. In the ECAL barrel the crystals...

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  30. Marko Mihovilovic (Université Paris-Saclay (FR))
    21/05/2025, 09:30
  31. Valentina Sola (Universita e INFN Torino (IT))
    21/05/2025, 10:00

    The High-Luminosity Large Hadron Collider (HL-LHC) will enable a more detailed exploration of new physics phenomena by significantly increasing collision rates, leading to pileup levels of approximately 200 simultaneous interactions. Several CMS systems will undergo substantial upgrades, including the MIP Timing Detector (MTD) project to prepare for this new era. The MTD is designed to...

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  32. Isis Hobus (Nikhef National institute for subatomic physics (NL))
    21/05/2025, 11:00

    During the LHC Long Shutdown 3, the ALICE Collaboration will replace the innermost three layers of the existing ALICE silicon tracker, ITS2. The upgraded inner tracker will consist of cylindrical, wafer-scale monolithic silicon sensors using a 65 nm CMOS imaging process. To evaluate the performance of the technology, test structures were fabricated on a multilayer reticle (MLR1). One such...

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  33. Nicola Neri (Università degli Studi e INFN Milano (IT))
    21/05/2025, 11:30
  34. Dmitry Druzhkin (KIT - Karlsruhe Institute of Technology (DE))
    21/05/2025, 12:00
  35. 21/05/2025, 12:30
  36. Alessio Ghezzi (Universita & INFN, Milano-Bicocca (IT))
    21/05/2025, 15:30

    The High Luminosity phase of the Large Hadron Collider (HL-LHC), with an integrated luminosity of approximately 3000 fb⁻¹ over ten years, will enable experiments to search for rare processes and perform precision measurements. However, it will also present significant challenges for the detectors, due to high pile-up, up to 200 interactions per bunch crossing, and extremely high radiation...

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  37. Joachim Baechler (CERN)
    21/05/2025, 16:00
  38. 21/05/2025, 17:00
  39. Angelo SCRIBANO, Christophe Royon (The University of Kansas (US))
    21/05/2025, 17:30
  40. 22/05/2025, 10:00
  41. Andrew Arzac
  42. Camilla Maggio (UAB), Camilla Maggio (Universitat Autònoma de Barcelona)
  43. Giulia Gioachin (Politecnico di Torino (IT))

    Since the spatial density of particle collisions is expected to rise significantly in the upcoming high-energy physics experiments, silicon detectors are required to provide precise timing information to perform an accurate track reconstruction and particle identification. Several experiments will face this challenge, including the next-generation heavy-ion experiment named ALICE 3, which will...

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  44. Marco Lisboa Leite (Universidade de Sao Paulo (USP) (BR))

    The High Granularity timing detector (HGTD) is one of the ATLAS upgrades and is designed to provide a per-track timing information of tens of ps over the full detector lifetime. This information will contribute to pileup mitigation in the operations of the ATLAS detector at the High-Luminosity LHC. HGTD deploys low gain avalanche silicon detectors (LGADs) with a segmentation into a 15x15...

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  45. Clarissa Buti (Universita e INFN, Firenze (IT))

    Future experiments at hadron colliders require an evolution of the tracking sensor technologies to ensure sufficient radiation hardness and timing resolution to cope with unprecedented fluxes of charged particles.
    3D diamond sensors with laser-graphitized electrodes, featuring strong binding energy, small atomic number and high carrier mobility, could provide an appealing option. However,...

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  46. CMS Collaboration

    The High Luminosity phase of the Large Hadron Collider (HL-LHC), with an integrated luminosity of approximately 3000 fb$^{-1}$ over ten years, will enable experiments to search for rare processes and perform precision measurements. However, it will also present significant challenges for the detectors, due to high pile-up, up to 200 interactions per bunch crossing, and extremely high radiation...

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  47. Dr Dmitry Orlov (Photonis Netherlands)

    We present the PhotonPix™ single-photon counting detector, a plug-and-play solution optimized for high-rate applications requiring exceptional timing precision. The detector integrates a Photonis Fast Timing MCP-PMT with an 8 mm diameter active area, supporting a range of Hi-QE photocathodes optimized for high quantum efficiency, in selected spectral range of 150 nm-900 nm, and low dark count...

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  48. CMS Collaboration

    The High-Luminosity Large Hadron Collider (HL-LHC) will enable a more detailed exploration of new physics phenomena by significantly increasing collision rates, leading to pileup levels of approximately 200 simultaneous interactions. Several CMS systems will undergo substantial upgrades, including the MIP Timing Detector (MTD) project to prepare for this new era. The MTD is designed to...

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  49. Valentina Sola (Universita e INFN Torino (IT))

    Timing resolution of LGAD sensors with different thicknesses, ranging from 45 down to 20 $\mu$m will be presented. The results are obtained through a $\beta$-source stimulus and electron beam test at the DESY facility. A timing resolution down to 16.6 ps has been reached by 20 $\ mum$-thick sensors, reduced to 12.2 ps by using the information from 2 different planes of 20 $\mu$m sensors....

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  50. Jon Lapington, Prof. Jon Lapington (University of Leicester (GB))