Conveners
Plenary: Introduction
- Shih-Chieh Hsu (University of Washington Seattle (US))
Plenary: Instrumentation in AI Era and BRN
- Jonathan Asaadi (University of Texas at Arlington)
Plenary: Agencies and International
- Mitchell Soderberg
Plenary: Training and Early Career Presentations
- Quentin Buat (University of Washington (US))
Plenary: Training and Early Career Presentations (Cont)
- Quentin Buat (University of Washington (US))
Plenary: A Long-Lived Legacy: Remembering Henry
- There are no conveners in this block
Plenary: HENP Projects and Community
- Jinlong Zhang (Argonne National Laboratory (US))
Plenary: Award Ceremony and Close out
- Jonathan Asaadi (University of Texas at Arlington)
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20/10/2026, 09:00
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Daniel Stephens (ALD, Pacific Northwest National Laboratory)20/10/2026, 09:10
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Shih-Chieh Hsu (University of Washington Seattle (US))20/10/2026, 09:20
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Quentin Buat (University of Washington (US))20/10/2026, 09:30
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Richard Saldanha20/10/2026, 09:50Presentation
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Jonathan Asaadi (University of Texas at Arlington)20/10/2026, 10:10
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Maurice Garcia-Sciveres (Lawrence Berkeley National Lab. (US))20/10/2026, 11:00
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Nhan Tran (Fermi National Accelerator Lab. (US))20/10/2026, 11:25
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Jennifer Ott (University of Hawaii Manoa), Marina Artuso (Syracuse University (US)), Maurice Garcia-Sciveres (Lawrence Berkeley National Lab. (US)), Nhan Tran (Fermi National Accelerator Lab. (US))20/10/2026, 11:45
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Thomas Bergauer (Austrian Academy of Sciences (AT))21/10/2026, 08:30
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Dr HELMUT MARSISKE (U.S. Department of Energy Office of High Energy Physics), Helmut Marsiske (DOE HENP)21/10/2026, 08:55
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Jim Shank (NSF)21/10/2026, 09:15
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Angela Fava (Fermilab), Bob Hirosky (University of Virginia (US)), Dr Peter Sorensen (LBL / Berkeley Lab), Rakshya Khatiwada (Fermilab/Illinois Institute of Technology)21/10/2026, 09:35
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Maxwell Chertok (University of California Davis (US))22/10/2026, 09:00PlenaryPresentation
Breakthroughs in science are invariably the result of novel measurement capabilities. Indeed, the invention of radically new technologies often arises out of attempts to probe beyond the known, and leads to advances in the hands of visionary scientists. In particular, major discoveries in High Energy Physics (HEP) are made using custom state-of-the-art instrumentation. Today, however, the...
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Amanda Lynn Steinhebel (Oak Ridge National Laboratory - (US))22/10/2026, 09:20RDC 2 PhotodectorsPresentation
Photon to Digital Converters (3D-PDCs) are next-generation digital silicon photomultipliers (SiPMs) that vertically integrate a sensing layer of Single Photon Avalanche Diodes (SPADs) with a custom CMOS active quenching circuit and processing electronics. This design enables individual-SPAD control, reducing system noise and offering ~100 ps single-photon timing resolution. The 'fully digital'...
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Samara Steinfeld22/10/2026, 09:35RDC 7 Low-Background DetectorsPresentation
The TESSERACT experiment is a collection of detectors searching for sub-GeV particle dark matter using sensitive transition-edge sensors. The complementary target materials include superfluid helium-4, polar crystals, and semiconductor crystals, each focusing on various low mass dark matter models. Superfluid helium-4 is an interesting target because of its light atomic mass, three signal...
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Chris Albert (California Institute of Technology)22/10/2026, 09:50RDC 8 Quantum & Superconducting SensorsPresentation
Kinetic inductance detectors (KIDs) have demonstrated single photon counting in 14-6 THz. Current efforts focus on extending the range and performance of such photon counting KIDs over 1-100 THz (4-400 meV) range. Exploiting the nonlinearity of thin-film kinetic inductance drastically improves the signal to noise ratio. Kinetic inductance traveling-wave parametric amplifiers (KI-TWPAs) offer...
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Bridget Mack (Syracuse University (US))22/10/2026, 10:05RDC 9 CalorimetryPresentation
Future high luminosity particle physics experiments come with many challenges. In hadron machines high pile-up rates will drive down the efficiencies of current calorimeters if timing information is not added to energy measurements. In general, detectors aspiring to be sensitive to flavor physics observables or ย flavor-tagged jets require hadron identification systems capable of distinguishing...
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Gregor Hieronymus Eberwein (Massachusetts Inst. of Technology (US))22/10/2026, 10:50RDC 3 Solid State TrackingPresentation
The ALICE Inner Tracking System (ITS3) upgrade introduces the first vertex detector based on wafer-scale, reticle-stitched, bent Monolithic Active Pixel Sensors (MAPS). The concept is being adopted for the Silicon Vertex Tracker (SVT) of the future ePIC detector at the Brookhaven National Laboratory (BNL) based Electron Ion Collider (EIC). The MOnolithic Stitched Active pIXel sensor (MOSAIX),...
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Kalindi Gosine (University of Texas at Arlington)22/10/2026, 11:05RDC 4 Readout & ASICsPresentation
Designing networks of communicating digital nodes requires connecting system-level behavior to the RTL from which hardware will be produced. RTLswarm is a parallel, distributed, cycle-accurate simulator that incorporates Verilator-generated C++ RTL models into independently executing node processes coordinated through a messaging network. Software-defined scenarios, tracing, and analysis allow...
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Shih-Chieh Hsu (University of Washington Seattle (US))22/10/2026, 11:35
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Charlie Young (SLAC National Accelerator Laboratory (US))23/10/2026, 08:30
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Sven Vahsen (University of Hawaii (US))23/10/2026, 08:551
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Charlie Young (SLAC National Accelerator Laboratory (US)), Dr Michael Begel (Brookhaven National Laboratory (US)), Prakhar Garg (Yale University), Sven Vahsen (University of Hawaii (US))23/10/2026, 09:201
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Prakhar Garg (Yale University)23/10/2026, 10:30
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Mark Vagins23/10/2026, 10:40
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Matthew Szydagis23/10/2026, 11:00
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Jonathan Asaadi (University of Texas at Arlington)23/10/2026, 11:20
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Jinlong Zhang (Argonne National Laboratory (US))23/10/2026, 11:35