Conveners
Plenary: Introduction
- Evelyn Jean Thomson (University of Pennsylvania (US))
Plenary: Instrumentation Overview
- Jinlong Zhang (Argonne National Laboratory (US))
- Jonathan Asaadi (University of Texas at Arlington)
Plenary: National Initiatives
- Mitchell Franck Newcomer (University of Pennsylvania (US))
Plenary: Early Career Research
- Ira Joseph Kroll (University of Pennsylvania (US))
Plenary: High Priority Big Projects
- Sally Seidel (University of New Mexico (US))
Plenary: Award ceremony, RDC Highlights, Closeout
- Jonathan Asaadi (University of Texas at Arlington)
- Jinlong Zhang (Argonne National Laboratory (US))
-
Mark Trodden07/10/2025, 09:00Plenary talk
-
07/10/2025, 09:15
-
Evelyn Jean Thomson (University of Pennsylvania (US))07/10/2025, 09:30Plenary talk
-
Jinlong Zhang (Argonne National Laboratory (US)), Jonathan Asaadi (University of Texas at Arlington)07/10/2025, 09:45
-
Thomas Bergauer (Austrian Academy of Sciences (AT))07/10/2025, 11:00
-
Maurice Garcia-Sciveres (Lawrence Berkeley National Lab. (US))07/10/2025, 11:25
-
Dr HELMUT MARSISKE (U.S. Department of Energy Office of High Energy Physics)07/10/2025, 11:50
-
07/10/2025, 11:55
-
07/10/2025, 12:00
-
Shih-Chieh Hsu (University of Washington Seattle (US))08/10/2025, 08:45PlenaryPlenary talk
This talk presents an overview of the major national AI initiatives driving today's scientific breakthroughs, focusing on the Department of Energyโs AI for Science efforts, including the FASST and hardware-aware AI programs, and the National Science Foundationโs AI research institutes and AI2 ecosystem. The presentation highlights how these initiatives foster foundational AI model development,...
Go to contribution page -
Silvia Zorzetti08/10/2025, 09:10
-
Gabriella Carini08/10/2025, 09:35
-
Brig Williams, Hugh Williams (University of Pennsylvania (US))08/10/2025, 10:00
-
Mohamed Hijas Mohamed Farook (University of New Mexico (US))09/10/2025, 09:00RDC 3 Solid State TrackingParallel session talk
Low Gain Avalanche Diodes (LGADs) are silicon sensors renowned for their ability to deliver fast timing, especially in high energy and nuclear physics. They achieve a timing resolution of 20-30 picoseconds through an internal multiplication process that creates a controlled avalanche of charge carriers, producing a gain of 10-100. Some variants of LGADs can also track particle trajectories...
Go to contribution page -
Victor Turbiner (SLAC National Accelerator Laboratory (US))09/10/2025, 09:15RDC 3 Solid State TrackingParallel session talk
Current and future particle trackers are beginning to incorporate timing measurements as part of the readout electronics. The ATLAS HGTD and CMS MTD timing detectors for the HL-LHC are already capable of sub-50 picosecond-level resolution, and tracking detectors for future colliders such as the muon or 10 TeV hadron colliders will require similar or better levels of time resolution with pixel...
Go to contribution page -
Guang Yang (Brookhaven National Lab)09/10/2025, 09:30RDC 9 CalorimetryParallel session talk
Since the entry to the precision era for the nuclear and high-energy physics communities, excellent particle detection capability is highly demanded for each part of the detection system. A homogeneous EM-Calorimeter could provide excellent energy resolution for electrons and photons in a wide dynamic range allowing rapidity coverage, particle containment and granularity. However, concerns of...
Go to contribution page -
Harsh Purwar (University of Hawaii at Mฤnoa, Honolulu, HI, USA)09/10/2025, 09:45RDC 5 Trigger & DAQPlenary talk
As SuperKEKB approaches its target instantaneous luminosity of $6\times 10^{35}$ cm$^{-2}$ s$^{-1}$, its only particle detector, Belle II comprised of several subdetectors*, is also undergoing constant upgrades and changes. Closer to its target luminosity, the Belle II detector expects to receive very large data samples that have much higher background and radiation levels. Single event upsets...
Go to contribution page -
William Matava (University of California at Berkeley)09/10/2025, 10:00RDC 7 Low-Background DetectorsParallel session talk
The TESSERACT experiment will deploy 3 unique detector modules based on a common transition edge sensor-based readout to search for sub-GeV dark matter. HeRALD will use sensors with silicon or sapphire substrates to image radiative and quasiparticle emission from a target of superfluid helium-4 . SPICE will use sensors fabricated on sapphire and gallium arsenide substrates sensitive to both...
Go to contribution page -
Ritoban Basu Thakur09/10/2025, 10:15RDC 8 Quantum & Superconducting SensorsParallel session talk
QUAntum LImited PHotons In the Dark Experiment (QUALIPHIDE) searches for Hidden Photons (HP) as dark matter. Quantum sensing techniques, such as photon counting, enable exploring new phase space for both HPs and axion like particles as candidates for dark matter. We have fielded a deeper than standard quantum limit search with single photon resolving MKIDs. This newest version of QUALIPHIDE...
Go to contribution page -
Evelyn Jean Thomson (University of Pennsylvania (US)), Jinlong Zhang (Argonne National Laboratory (US)), Jonathan Asaadi (University of Texas at Arlington)09/10/2025, 10:30Parallel session talk
-
Brooke Russell (Massachusetts Institute of Technology)10/10/2025, 09:00
-
Liza Brost (Brookhaven National Laboratory (US))10/10/2025, 09:22
-
Isobel Ojalvo (Princeton University (US))10/10/2025, 09:47
-
Oskar Hartbrich (ORNL)10/10/2025, 10:10
-
Olivia Seidel10/10/2025, 11:05
-
Earl Russell Tang Almazan (University of California,Santa Cruz (US))10/10/2025, 11:30
-
Jonathan Asaadi (The University of Texas at Arlington)10/10/2025, 11:55
-