1–6 Sept 2025
Liverpool, UK
Europe/London timezone

Contribution List

162 out of 162 displayed
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  1. yun tse tsai (SLAC)
    01/09/2025, 09:30
    Presentation
  2. Elena Gramellini (University of Manchester)
    01/09/2025, 09:42
    Presentation
  3. Megan Friend (KEK High Energy Accelerator Research Organization (JP))
    01/09/2025, 09:54
    Presentation
  4. Prof. Kim Siang Khaw (Tsung-Dao Lee Institute, Shanghai Jiao Tong University)
    01/09/2025, 10:06
    Presentation
  5. Julia Harz
    01/09/2025, 10:18
    Presentation
  6. Tanaz Mohayai (Indiana University)
    01/09/2025, 11:00
    Presentation
  7. Dr POONAM MEHTA (Jawaharlal Nehru University)
    01/09/2025, 11:12
    Presentation
  8. Prof. Jianming Bian (University of California Irvine (US))
    01/09/2025, 11:30
    Presentation
  9. Yashwanth Sanjeev Prabhu
    01/09/2025, 12:00
    Presentation
  10. Ce Zhang (University of Liverpool (GB))
    01/09/2025, 13:45
    Presentation
  11. Raul GONZALEZ JIMENEZ (Universidad de Sevilla)
    01/09/2025, 14:15
    Presentation
  12. Afroditi Papadopoulou
    01/09/2025, 14:45
    Presentation
  13. Chris Rogers
    01/09/2025, 15:15
    Presentation
  14. Lauren Anthony (Imperial College (GB))
    01/09/2025, 16:15
    Presentation
  15. Tanaz Mohayai (Indiana University)
    01/09/2025, 16:45
    Presentation
  16. Namitha Chithirasreemadam (University of Pisa)
    01/09/2025, 17:30
    WG4 - Muon Physics
    Poster

    The Mu2e experiment will search for the CLFV process of coherent, neutrinoless $\mu^- \rightarrow e^-$ conversion in the field of an Al nucleus. The expected signal is a 104.97 MeV monochromatic conversion electron (CE). The signature feature of Mu2e is the superconducting solenoidal magnetic system that produces a high intensity pulsed muon beam. One of the backgrounds to the CE search is...

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  17. Sinead Eley (University of Liverpool (GB))
    01/09/2025, 17:30
    WG2 - Neutrino Scattering
    Poster

    The LHC offers a unique environment to study neutrinos in the intermediate energy range between those produced in fixed-target accelerator experiments and high-energy astrophysical sources. The FASER experiment takes advantage of the intense, highly collimated flux of light hadrons produced at Interaction Point 1 (IP1) to probe high-energy collider neutrinos. Using the electronic detector...

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  18. Dr Jessie Micallef (Tufts University)
    01/09/2025, 17:30
    WG7 - EDI, Education and Outreach
    Poster

    The "Buddy System" Program is a networking initiative that encourages new connections between collaborators to be formed during collaboration meetings. A survey is sent before upcoming meetings, asking both in-person and virtual attendees who are interested to fill out the form to be matched with 1-2 other collaborators. Based on the responses, including a ranking system for how they want the...

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  19. Patrick Bates
    01/09/2025, 17:30
    WG1 - Neutrino Oscillations
    Poster

    Development of an agnostic global particle identification tool for the ND280 near
    detector

    Patrick Bates

    T2K is a long-baseline neutrino experiment stationed in Japan, with the primary goal of measuring $δ_{cp}$ via comparison of $ν_μ→ν_e$ and $ν^{-}_μ→ν^{-}_e$ oscillation. The ND280 off-axis near detector samples the neutrino beam before oscillation occurs, and allows for...

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  20. Hokuto Kobayashi (University of Tokyo (JP))
    01/09/2025, 17:30
    WG2 - Neutrino Scattering
    Poster

    The Tokai to Kamioka (T2K) experiment is a long-baseline neutrino oscillation experiment aiming to measure CP-violation in the lepton sector. So far, T2K has shown results that disfavor CP conservation with a confidence level of 90%. One of the major systematic uncertainties in the current oscillation analysis is the electron-neutrino cross-section. To reduce these uncertainties, the near...

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  21. Andrew Cudd (University of Colorado Boulder)
    01/09/2025, 17:30
    WG2 - Neutrino Scattering
    Poster

    Neutrino experiments rely on complex and computationally expensive detector simulations to predict observable quantities from neutrino interaction models. The significant cost of these simulations limits the feasibility to generate new detector-level events for changes in the interaction model. An approach often used is to produce a new simulation of only the interaction model, which is much...

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  22. Matteo Feltre (Universita e INFN, Padova (IT))
    01/09/2025, 17:30
    WG6 - Detectors
    Poster

    T2K (Tokai to Kamioka) is a long-baseline neutrino experiment based in Japan, designed to measure neutrino oscillation parameters, including $ \theta_{13} $, $ \delta_{CP}$, $\theta_{23}$, and $\Delta m^2_{32}$. These parameters are determined by studying electron neutrino appearance probabilities and muon neutrino survival probabilities. In recent years, T2K has undergone significant upgrades...

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  23. Dario Pullia (CERN)
    01/09/2025, 17:30
    WG6 - Detectors
    Poster

    The Neutrino Platform at CERN hosts large-scale prototypes for DUNE’s Far Detector, aligned with the SPS beamline pointed towards the North Area.
    The 400 GeV/c SPS protons impacting on the T2 target area may produce exotic particles that could travel ~700 meters to the detectors, in addition to a substantial flux of neutrinos.
    Simulations of the neutrino flux predict that thousands of...

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  24. Unik Limbu
    01/09/2025, 17:30
    WG6 - Detectors
    Poster

    Hyper-Kamiokande (Hyper-K) is a next-generation Water Cherenkov detector designed to study neutrino properties with exceptional accuracy. Precision measurements of neutrino oscillations, charge-parity (CP) violation, atmospheric and solar neutrino studies, as well as proton decay searches, are among the key physics goals of Hyper-K, making accurate detector calibration essential for achieving...

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  25. Xiaohan Tan (Shandong University)
    01/09/2025, 17:30
    WG1 - Neutrino Oscillations
    Poster

    Jiangmen Underground Neutrino Observatory (JUNO) is a next-generation 20-kton liquid scintillator (LS) detector currently under commissioning. JUNO is capable of exploring various physics topics including atmospheric neutrino oscillations. While the atmospheric neutrino flux is initially composed exclusively of muon and electron neutrinos, a large number of them are expected to oscillate to...

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  26. Dr Sam Jenkins (University of Liverpool)
    01/09/2025, 17:30
    WG2 - Neutrino Scattering
    Poster

    The T2K experiment is a long-baseline neutrino oscillation experiment based in Japan, with the primary goal of measuring CP violation through comparing neutrino and antineutrino oscillations. The primary off-axis near detector, ND280, observes the neutrino beam before oscillation, and has the important role of constraining neutrino-nucleus interactions. This is a leading source of systematic...

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  27. Dr Ralte Lalnuntluanga (Tel Aviv University)
    01/09/2025, 17:30
    WG6 - Detectors
    Poster

    For current and upcoming accelerator-based neutrino oscillation experiments, a precise understanding of neutrino-nucleus interactions is crucial to attaining the desired sensitivity. Insufficient knowledge of the energy carried by undetected particles, particularly neutrons, produced in neutrino-nucleus interactions can distort the reconstructed neutrino energy spectrum and introduces bias in...

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  28. jiabin wang (Shandong University)
    01/09/2025, 17:30
    WG1 - Neutrino Oscillations
    Poster

    Jiangmen Underground Neutrino Observatory (JUNO) is a large-scale neutrino experiment located 700 meters underground in Southern China. JUNO is capable of detecting multiple types of neutrinos including atmospheric neutrinos which can undergo both charged current (CC) and neutral current (NC) interactions in the detector. In addition to the standard 3-flavor oscillation measured by CC...

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  29. Charles Kinsman
    01/09/2025, 17:30
    WG4 - Muon Physics
    Poster

    The Mu3e experiment is dedicated to observing charged lepton flavour violation through the neutrino-less decay of a muon to two positrons and an electron. The experiment is located around the Compact Muon Beam Line (CMBL) at the Paul Scherrer Institut, which produces muons at a rate of $10^{8}$ Hz. The experiment aims to observe the decay or exclude a branching ratio greater than $10^{-16}$....

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  30. Adam Tarrant (University of Liverpool)
    01/09/2025, 17:30
    WG6 - Detectors
    Poster

    Next-generation neutrino detectors will require new simulation and reconstruction software. For water and scintillator-based neutrino detectors, RATPAC is a leading simulation framework. The latest release,
    RATPAC-TWO, brings several enhancements over the original version, improving both the usability and collaboration potential between experiments. With the 30-tonne BUTTON experiment at...

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  31. Prof. Simone Donati (Istituto Nazionale di Fisica Nucleare - Pisa)
    01/09/2025, 17:30
    WG7 - EDI, Education and Outreach
    Poster

    Since 1983 the Italian groups collaborating with Fermilab (US) have been running a 2-month summer training program for Master students. While in the first year the program involved only 4 physics students, in the following years it was extended to engineering students. Many students have extended their collaboration with Fermilab with their Master Thesis and PhD.
    The program has involved...

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  32. Mr Balint Bogdan (University of Liverpool), Dr Sam Jenkins (University of Liverpool)
    01/09/2025, 17:30
    WG6 - Detectors
    Poster

    The upcoming Hyper-Kamiokande experiment is a next generation water Cherenkov detector based in Japan. Using an upgraded JPARC neutrino beam, Hyper-K aims to make precision measurements of the CP violating phase $\delta_{CP}$, along with neutrinos from astrophysical sources, and proton decay. With a fiducial volume approximately eight times larger than its predecessor Super-Kamiokande,...

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  33. Dr Ara Ioannisyan (Institute for Theoretical Physics and Modeling)
    01/09/2025, 17:30
    WG2 - Neutrino Scattering
    Poster

    We study the dependence of neutrino-induced $\gamma/\pi^0$ production ($\stackrel{ {(-)}}{\nu_\mu} + A \to \stackrel{ {(-)}}{\nu_\mu}(\mu) +\gamma/\pi^0 + X$) on the target nucleus A, at the $\Delta$ resonance mass region.
    We predict the ratio of the $\gamma / \pi^0$ production rates in NC and CC interactions and for $\nu_\mu$ and $\bar \nu_\mu$ beams:
    - Argon target: $\sim$3.1\%...

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  34. Anezka Klustova
    01/09/2025, 17:30
    WG6 - Detectors
    Poster

    Precise measurements of neutrino oscillations in long-baseline experiments depend on an accurate understanding of neutrino beam properties and neutrino–nucleus interactions—two dominant sources of systematic uncertainty. To reduce these uncertainties, the ND280 near detector of the T2K neutrino experiment in Japan has undergone a major upgrade designed to provide full polar angle acceptance,...

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  35. David Jason Koskinen
    02/09/2025, 09:00
    Presentation
  36. Paul De Jong (Nikhef National institute for subatomic physics (NL))
    02/09/2025, 09:30
    Presentation
  37. Srubabati Goswami
    02/09/2025, 10:00
    Presentation
  38. James Mead (University of Amsterdam / Nikhef)
    02/09/2025, 11:00
    WG6 - Detectors
    Presentation
    WG6

    PTOLEMY aims to measure the lowest neutrino mass by resolving the β-decay endpoint of tritium. A demonstrator, currently under construction at LNGS, will rely on amassing a solid-state source of atomic tritium; a cyclotron radiation-based background suppression system; a novel, compact EM filter; and an O(50meV)-precision spectrometer. PTOLEMY faces many novel technical challenges, and an...

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  39. Sharmistha Chattopadhyay (Institute of Physics, Bhubaneswar, Odisha, India, and Homi Bhabha National Institute, Anushakti Nagar, Mumbai, India)
    02/09/2025, 11:00
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    The information regarding the mass of Earth and its internal structure has primarily been obtained through gravitational measurements and seismic studies, both of which rely on gravitational and electromagnetic interactions, respectively. However, neutrinos offer an independent method for exploring the Earth's interior by utilizing weak interactions, particularly through the effects of Earth’s...

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  40. Luis Pelegrina Gutiérrez (Universidad de Granada)
    02/09/2025, 11:00
    WG2 - Neutrino Scattering
    Presentation
    WG2

    The Short-Baseline Near Detector (SBND) is a 112-ton scale Liquid Argon Time Projection Chamber (LArTPC) neutrino detector positioned in the Booster Neutrino Beam at Fermilab, as part of the Short-Baseline Neutrino (SBN) program. The detector is currently collecting neutrino beam data. Located only 110 m from the neutrino production target, SBND is exposed to a very high flux of neutrinos and...

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  41. Mikio Sakurai (UCL)
    02/09/2025, 11:00
    WG4 - Muon Physics
    Presentation
    WG4

    The Mu3e experiment at the Paul Scherrer Institute (PSI) will search for the charged lepton flavour violating decay µ⁺ → e⁺e⁻e⁺, improving the current best limit set by the SINDRUM experiment by four orders of magnitude.

    Mu3e will be conducted in two phases. Phase I, currently under construction at the πE5 beamline at PSI, will utilise an intense DC surface muon beam of 10⁸ µ⁺/s to reach a...

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  42. Adi Ashkenazi
    02/09/2025, 11:23
    WG2 - Neutrino Scattering
    Presentation
    WG2

    MicroBooNE is a Liquid Argon Time Projection Chamber, able to image neutrino interactions with excellent spatial and timing resolution, enabling the identification of complex final states resulting from neutrino-nucleus interactions. As a result, MicroBooNE has produced a variety of neutrino cross-section measurements on argon, spanning almost four orders of magnitude and across all major...

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  43. Siyuan Chen
    02/09/2025, 11:25
    WG4 - Muon Physics
    Presentation
    WG4

    The spontaneous conversion of muonium to antimuonium is one of the interesting charged lepton flavor violation phenomena, offering a sensitive probe of potential new physics and serving as a tool to constrain the parameter space beyond the Standard Model. The Muonium-to-Antimuonium Conversion Experiment (MACE) is designed to utilize a high-intensity muon beam, a Michel electron magnetic...

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  44. Dr Chiara F Lastoria (LPC Caen, CNRS/IN2P3, Caen (France))
    02/09/2025, 11:25
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    The next generation of neutrino experiments aims to provide high-precision measurements of the neutrino oscillation parameters in order to reveal the major unknowns in neutrino physics. Among them, validating the three-neutrino flavor paradigm while testing the non-unitarity of the neutrino mixing matrix remains one of the most exciting, as it allows the
    exploration of new physics...

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  45. Dr Umut Kose (ETH-Zurich)
    02/09/2025, 11:25
    WG6 - Detectors
    Presentation
    WG6

    Plastic scintillator detectors with 3D granularity and sub-nanosecond time resolution offer simultaneous particle tracking, identification, and calorimetry. However, achieving fine segmentation at scale remains a major challenge due to high manufacturing costs, extended production timelines, and stringent precision requirements. To overcome these barriers, the 3DET R&D collaboration has...

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  46. Luis Mora-Lepin (Florida State University)
    02/09/2025, 11:48
    WG2 - Neutrino Scattering
    Presentation
    WG2

    The Deep Underground Neutrino Experiment (DUNE) is a cutting-edge long-baseline experiment under construction in the United States. DUNE will use a far detector (FD) and a near detector (ND) to sample a high-intensity neutrino beam produced at Fermilab. This experiment aims to conduct precise studies of neutrino oscillations, establish the ordering of neutrino masses, and investigate potential...

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  47. Qiyu Yan
    02/09/2025, 11:50
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    The Jiangmen Underground Neutrino Observatory (JUNO) experiment is a multi-purpose experiment located in southern China. The detector is designed with 20-kton liquid scintillator and currently in its filling stage. The main physics goal of JUNO is to determine the neutrino mass ordering (NMO) via a precise measurement of the reactor neutrino oscillation spectrum. Atmospheric neutrino...

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  48. Richard Diurba (University of Bern)
    02/09/2025, 11:50
    WG6 - Detectors
    Presentation
    WG6

    The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino oscillation experiment with the primary goal of measuring the mass hierarchy and CP-violating phase. Neutrinos will be measured at two detector facilities, namely a Near Detector (ND) located at Fermilab close to where the neutrino beam is produced by the Long-Baseline Neutrino Facility (LBNF) and a Far...

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  49. Qiang Li (Peking University (CN))
    02/09/2025, 11:50
    WG4 - Muon Physics
    Presentation
    WG4

    We propose here a set of new methods involving probing and knocking with muons (PKMu). There is a wealth of rich physics to explore with GeV muon beams. Examples include but not limited to: muon scattering can occur at large angles, providing evidence of potential muon-philic dark matter or dark mediator candidates; muon-electron scattering can be used to detect new types of bosons associated...

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  50. Dr Stephen Dolan (CERN)
    02/09/2025, 12:11
    WG2 - Neutrino Scattering
    Presentation
    WG2

    The ICARUS experiment, utilising Liquid Argon Time Projection Chamber (LAr TPC) technology, has been installed at Fermilab in Chicago, Illinois, following its initial operation in Italy and subsequent refurbishment at CERN. ICARUS has successfully been taking physics data at Fermilab since June 2022. While the experiment's primary objective is to function as the far detector of the Short...

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  51. Pierre Granger (CERN)
    02/09/2025, 12:15
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    The Deep Underground Neutrino Experiment (DUNE) is a pioneering long baseline neutrino experiment situated in the US that will feature multi-kiloton scale Liquid Argon Time Projection Chambers (LArTPCs). Beyond its primary beam neutrino objectives, DUNE's cutting-edge technology offers a unique opportunity to investigate atmospheric neutrinos with unprecedented precision. Atmospheric...

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  52. Tristan Daret (Université Paris-Saclay (FR))
    02/09/2025, 13:45
    WG6 - Detectors
    Presentation
    WG6

    T2K is a long-baseline experiment measuring neutrino and antineutrino oscillations by observing the disappearance of muon neutrinos, as well as the appearance of electron neutrinos, over a long 295km distance. The ND280 near detector at J-PARC plays a crucial role to minimise the systematic uncertainties related to the neutrino flux and neutrino-nucleus cross-sections as it measures the...

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  53. Masato Kimura (IPNS, KEK)
    02/09/2025, 13:45
    WG4 - Muon Physics
    Presentation
    WG4

    The J-PARC muon g-2/EDM experiment aims to precisely measure the anomalous magnetic moment and electric dipole moment based on a novel low-emittance muon beam. Such a beam is realized by a muon linear accelerator following a cooled muon source, which allows to employ different techniques than the BNL and FNAL experiments such as a compact storage ring without electric focusing and track...

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  54. Shirley Li (UC Irvine)
    02/09/2025, 13:45
    WG2 - Neutrino Scattering
    Presentation
  55. Rohan Rajagopalan
    02/09/2025, 13:45
    WG5 - Neutrinos Beyond PMNS
    Presentation
    WG5

    The Short-Baseline Near Detector (SBND) is a 112-ton liquid argon time projection chamber 110 m away from the Booster Neutrino Beam (BNB) target at Fermilab (Illinois, USA). The close location to the BNB origin makes the experiment sensitive to physics beyond the Standard Model (BSM) produced in the beam. Thanks to its advanced scintillation light detection system, a timing resolution at the...

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  56. Marvin Pfaff (Imperial College (GB)), Paul-Bogdan Jurj, Rohan Kamath (Imperial College London)
    02/09/2025, 13:45
    WG4 - Muon Physics
    Presentation
    WG3

    The neutrinos from STORed Muons (nuSTORM) facility enables precise neutrino physics studies through the use of innovative neutrino beams created by muon decay, which is characterised by well-defined flavour composition and energy spectra of the neutrino beam. Combined with precise muon flux measurements, with a final target of $\%$-level precision in neutrino flux determination, this will...

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  57. Adi Ashkenazi (Tel Aviv University (IL))
    02/09/2025, 14:10
    WG2 - Neutrino Scattering
    Presentation

    The e4nu collaboration investigates lepton-nucleus interactions to deepen our understanding of neutrino behavior in nuclear environments. By leveraging the similarities between electron-nucleus and neutrino-nucleus interactions, e4nu utilizes a broad phase space of exclusive electron scattering data. This data, collected on nuclear targets similar to those used in neutrino oscillation...

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  58. Magnus Handley
    02/09/2025, 14:10
    WG5 - Neutrinos Beyond PMNS
    Presentation
    WG5

    MicroBooNE is an 85-tonne active mass liquid argon time projection chamber (LArTPC) at Fermilab. Between 2015-2021, the detector recorded neutrino interactions from the Booster Neutrino Beam (BNB) and Neutrinos at the Main Injector (NuMI) beams. MicroBooNE's capabilities for fine-grained tracking, particle identification, and calorimetry make it a powerful detector not just to explore neutrino...

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  59. Matteo Feltre (Universita e INFN, Padova (IT))
    02/09/2025, 14:10
    WG6 - Detectors
    Presentation
    WG6

    The off-axis magnetic near detector of the T2K experiment has recently completed a significant upgrade, including the construction and installation of two new Time Projection Chambers (TPC) equipped with innovative resistive Micromegas technology and a field cage composed of thin composite walls. In this presentation, we will give an overview of the design and key features of the new TPCs,...

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  60. Dr Max Topp-Mugglestone (CERN)
    02/09/2025, 14:10
    WG3 - Accelerator Physics
    Presentation
    WG3

    The European Spallation Source Neutrino Super Beam + ( ESSnuSB+) project aims to make precision measurements of neutrino-nucleus interaction cross sections. To do this it will utilize the impact of a 1.25 MW proton pulse from the ESS (European Spallation Source) Linac on a target with the ultimate aim of creating a muon and electron neutrino beam from a muon decay ring (based on a low-energy...

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  61. Zejia Lu
    02/09/2025, 14:10
    WG4 - Muon Physics
    Presentation
    WG4

    The Muon g-2 Experiment at Fermilab has achieved a significant milestone by measuring the muon anomalous magnetic moment with a precision of 127 parts per billion (ppb), surpassing its original design goal of 140 ppb. This presentation provides an overview of the analysis of the anomalous precession frequency using the Run-4/5/6 dataset, which is crucial for the Muon g-2 measurement. We will...

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  62. Maja Olvegaard (Uppsala University (SE))
    02/09/2025, 14:35
    WG3 - Accelerator Physics
    Presentation
    WG3

    The ESS Neutrino SuperBeam project (ESSnuSB) is a proposed neutrino long-baseline experiment at ESS, Lund, Swedem, which aims at measuring the leptonic CP-violating phase, $\delta_{CP}$. By using the high-intensity ESS linear accelerator to produce the world's brightest pulsed neutrino source, the measurement will reach a uniquely high precision. In order to further enhance the precision, the...

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  63. Marilisa De Serio (Universita e INFN, Bari (IT))
    02/09/2025, 14:35
    WG6 - Detectors
    Presentation
    WG6

    Resistive Plate Chambers are gaseous detectors extensively used in several domains of Physics given their excellent time and space resolution.
    When operated in avalanche mode they make use of a high-performance high- Global Warming Potential gas mixture based on C2H2F4 and SF6, both fluorinated greenhouse components.

    The RPC ECOGas@GIF++ Collaboration is carrying on an intense R&D...

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  64. Dr Stephen Dolan (CERN)
    02/09/2025, 14:35
    WG2 - Neutrino Scattering
    Presentation

    To achieve the ambitious goal of characterising neutrino flavour oscillations with percent-level precision, current and future long-baseline neutrino oscillation experiments must significantly reduce existing systematic uncertainties. Among the most challenging are those associated with modelling neutrino–nucleus interactions in the few-GeV energy range.

    To address this, the T2K...

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  65. Dr Saskia Charity (University of Liverpool (GB))
    02/09/2025, 14:35
    WG4 - Muon Physics
    Presentation
    WG4

    The MUonE experiment at CERN aims to determine the leading-order hadronic contribution to the muon by an innovative approach, using elastic scattering of 160 GeV muons on atomic electrons in a low-Z target. The M2 beam line at CERN provides the necessary intensity needed to reach the statistical goal in few years of data taking. The experimental challenge relies in the precise control of the...

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  66. Afroditi Papadopoulou
    02/09/2025, 15:00
    WG2 - Neutrino Scattering
    Presentation

    Making high-precision measurements of neutrino oscillation parameters requires an unprecedented understanding of neutrino-nucleus scattering. This is especially urgent for upcoming experiments like DUNE and Hyper-K. To help fulfill this need, MicroBooNE has produced an extensive set of neutrino cross-section results that probe both the leptonic and hadronic components of the interaction. This...

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  67. Dominika Vasilkova
    02/09/2025, 15:00
    WG4 - Muon Physics
    Presentation
    WG4

    The new Muon g-2 experiment at Fermilab, while primarily designed to measure the muon's anomalous magnetic moment, also offers the unique opportunity to perform a world-leading search for the muon's electric dipole moment (EDM). Within the Standard Model, the muon EDM is predicted to be vanishingly small, orders of magnitude smaller than the reach of current experiments. However, some BSM...

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  68. Andre Fabiano Steklain Lisboa (The Federal University of Technology - Parana (BR))
    02/09/2025, 15:00
    WG6 - Detectors
    Presentation
    WG6

    The Deep Underground Neutrino Experiment (DUNE) will utilize liquid argon time projection chamber (LArTPC) technology to address key questions in neutrino physics, such as CP violation and the neutrino mass ordering. The Phase II Far Detector modules will employ vertical drift single-phase LArTPCs with an active volume of 13 m × 13 m × 60 m and dual anode planes. We propose a novel photon...

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  69. Themis Bowcock
    02/09/2025, 15:25
    WG4 - Muon Physics
    Presentation
    WG4

    We outline the physics case for the study of hadron edms that follow on from the successful FNAL g-2 muon experiment. The long term goal is making measurements of edms at, or below, the standard model expectation to provide quantifiable insight into the outstanding strong CP problem. The frozen spin technique spin technique is introduced and a possible lattice for the construction of such a...

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  70. Jiajun Liao
    02/09/2025, 16:15
    WG5 - Neutrinos Beyond PMNS
    Presentation
    WG5

    High energy collider neutrinos have been observed for the first time by the FASER$\nu$ experiment. The detected spectrum of collider neutrinos scattering off nucleons can be used to probe neutrinophilic mediators with GeV-scale masses. We perform an analysis on the measured muon spectra at FASER$\nu$, and find that the bounds on the vector mediator from the current FASER$\nu$ data are...

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  71. Lavinia Russo (Centre National de la Recherche Scientifique (FR))
    02/09/2025, 16:15
    WG2 - Neutrino Scattering
    Presentation
    WG2

    We present the implementation of the Martini–Ericson–Chanfray–Marteau RPA-based (anti)neutrino cross section model in the GENIE neutrino event generator. The implementation includes both the quasielastic (1p1h) and multinucleon (npnh) interaction channels. The presentation will begin with an overview of the theoretical foundations of the model. Validation steps are then discussed, along with...

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  72. Carmen Palomares (CIEMAT - Centro de Investigaciones Energéticas Medioambientales y Tec. (ES))
    02/09/2025, 16:15
    WG6 - Detectors
    Presentation
    WG6

    The Deep Underground Neutrino Experiment (DUNE) is a dual-site experiment for long-baseline neutrino oscillation studies, capable of resolving the neutrino mass hierarchy and CP-violation. DUNE will also be sensitive to supernova neutrinos and processes beyond the Standard Model. The Far Detector (FD) will consist of four liquid argon TPCs (17 kton each) equipped with systems for detecting...

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  73. Masato Kimura (IPNS, KEK)
    02/09/2025, 16:15
    WG4 - Muon Physics
    Presentation

    Acceleration of cooled muons is a promising technology for realizing a low-emittance muon beam, which is essential for noble muon sciences such as precise measurements of the muon dipole moments and muon microscopy. This technology is being developed at the Material and Life science experimental Facility at J-PARC. There, muons are cooled down to thermal energy though Muonium formation...

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  74. Clara Cuesta Soria (CIEMAT)
    02/09/2025, 16:15
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline experiment that will determine neutrino mass ordering (> 5$\sigma$), discover leptonic CP violation if nearly maximal violation, precisely measure neutrino oscillation parameters, observe astrophysical neutrinos, and search for processes beyond the standard model. The experiment will consist of four modules of...

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  75. Qiyu Yan
    02/09/2025, 16:38
    WG2 - Neutrino Scattering
    Presentation
    WG2

    Pion production is one of the critical interaction systematic uncertainties in neutrino oscillation measurements. Recent GiBUU development has introduced many improvements in the treatment of pion production, including the $2\pi$ background in neutrino interactions. We present a comprehensive study of charge current neutrino-induced pion production with the GiBUU model by examining the...

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  76. Takuya Tashiro
    02/09/2025, 16:40
    WG6 - Detectors
    Presentation
    WG6

    Hyper-Kamiokande, the next-generation Water-Cherenkov detector, is being prepared to start operation in 2028 to reveal the neutrino properties and to search for nucleon decays.
    It utilizes approximately 20,000 newly designed 50-cm PMTs, which are produced by Hamamatsu Photonics as R12860, to detect the Cherenkov light emitted in the inner detector with higher photon detection efficiency,...

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  77. Andres Lopez Moreno (Centre National de la Recherche Scientifique (FR))
    02/09/2025, 16:40
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    The Deep Underground Neutrino Experiment (DUNE) will provide a unique opportunity to simultaneously measure the oscillation parameters in the high- and low-energy regimes. DUNE's liquid argon time projection chamber (LArTPC) technology provides a charged-current (CC) and an elastic-scattering (ES) interaction channel that, when simultaneously exploited, enable precision measurements of the...

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  78. Jiaoyang/ 娇瑒 Li/李 (Fermi National Accelerator Laboratory)
    02/09/2025, 16:40
    WG5 - Neutrinos Beyond PMNS
    Presentation
    WG5

    The Short-Baseline Near Detector (SBND) is one of three Liquid Argon Time Projection Chamber (LArTPC) detectors used in the Short-Baseline Neutrino (SBN) programme at Fermilab. As the near detector in the SBN programme, the SBND is located just 100 metres from the target along the Booster Neutrino Beam (BNB). SBND offers sensitivity to a broad range of new physics scenarios, including the...

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  79. Cynthia (Thia) Keppel
    02/09/2025, 16:40
    WG3 - Accelerator Physics
    Presentation

    High-intensity proton beams are routinely used to generate secondary beams of particles such as neutrinos and muons.. High-current (∼100 µA), medium-energy (1 - 10 GeV), continuous-wave electron beams with a delivered large integrated charge (∼1000 C/y) can be also used to generate secondary beams. After interaction with a thin target in fixed-target experiments at the Thomas Jefferson...

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  80. Mr Rwik Dharmapal Banerjee (University of Wrocław doctoral student)
    02/09/2025, 17:00
    WG2 - Neutrino Scattering
    Presentation
    WG2

    Reliable theoretical modeling of neutrino-nucleus interactions is an essential requirement for current and next-generation neutrino-oscillation experiments, such as MicroBooNE and DUNE, which use argon as the target material. In this talk, I will present recent advancements in the treatment of the quasi-elastic (QE) channel in the NuWro Monte Carlo event generator. We implement the...

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  81. Han-Jie Cai (Institute of Modern Physics, Chinese Academy of Sciences)
    02/09/2025, 17:05
    WG4 - Muon Physics
    Presentation

    A high-intensity muon source named MuST has been proposed for several years at IMPCAS in China. Utilizing the 5-mA proton beam of CiADS linac on targets, multiple muon beamlines can be fed, and the intensity of the DC muon beam is expected to be record-breaking. Here, the conceptual layout of MuST, including the tandem targets, the muon beamlines, and the terminals, is presented. The plan and...

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  82. Krzysztof Dygnarowicz (Warsaw University of Technology (PL))
    02/09/2025, 17:05
    WG6 - Detectors
    Presentation
    WG6

    The Water Cherenkov Test Experiment (WCTE) at CERN is designed to test various technologies and techniques related to water Cherenkov detectors, which may later be implemented in the Hyper-Kamiokande experiment. WCTE consists of 97 multi-PMT photosensors placed in a water tank (~3.8 m in diameter, ~3.6 m in height, total water mass ~41 tonnes). Each multi-PMT contains nineteen 3" PMTs and...

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  83. William Gregory Dallaway (University of Toronto (CA))
    02/09/2025, 17:05
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    Our understanding of three-flavor neutrino oscillations has undergone significant improvement. However, most progress has come from studying $\nu_e$ and $\nu_\mu$ while the $\nu_\tau$ remains the least explored particle in the Standard Model. The Deep Underground Neutrino Experiment (DUNE), a next-generation long-baseline neutrino experiment under construction, is designed to address this...

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  84. Kiran Sharma
    02/09/2025, 17:05
    WG5 - Neutrinos Beyond PMNS
    Presentation
    WG5

    The standard approach to observing Time reversal (T) symmetry violation formally corresponds to exchanging neutrino flavors of the neutrino source and detector, which is experimentally challenging. We propose an alternative framework to test T violation without interchanging the source and detector, but using the L-odd components in the transition probabilities. We compare the data at...

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  85. Hemant Prasad
    02/09/2025, 17:23
    WG2 - Neutrino Scattering
    Presentation
    WG2

    NuWro, a state-of-the-art Monte Carlo generator developed by theorists at the University of Wroclaw, simulates neutrino-nucleus interactions. This talk will demonstrate NuWro's capabilities, methodologies, and applications in simulating neutrino-nucleus interactions across a wide energy range, from a few MeV's to hundreds of GeV. Lastly, I will present the highlights of NuWro v25.03 which was...

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  86. Dr Sam Jenkins (University of Liverpool)
    02/09/2025, 17:30
    WG6 - Detectors
    Presentation
    WG6

    The upcoming Hyper-Kamiokande experiment is a next-generation water Cherenkov experiment which will be based in Japan. Hyper-K aims to make precision measurements of CP-violation and other neutrino oscillation parameters, atmospheric and solar neutrinos, supernova neutrinos, and proton decay. With a fiducial volume approximately eight times larger than its predecessor Super-Kamiokande, Hyper-K...

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  87. Eric Baussan
    03/09/2025, 09:00
    Presentation
  88. Andreas Knecht
    03/09/2025, 09:30
    Presentation
  89. Jessica Esquivel
    03/09/2025, 10:00
    Presentation
  90. Anezka Klustova
    03/09/2025, 10:30
  91. Unik Limbu
    03/09/2025, 10:35
  92. Dario Pullia (CERN)
    03/09/2025, 10:40
  93. Ara Ioannisyan (A.Alikhanyan National Science Laboratory (AM))
    03/09/2025, 10:45
  94. Dr Jessie Micallef (Tufts University (and MIT))
    03/09/2025, 10:50
  95. Patrick Bates
    03/09/2025, 10:55
  96. Dr Veera Mikola (University of Glasgow)
    03/09/2025, 11:40
    Presentation
  97. Pierre Granger (CERN)
    03/09/2025, 12:10
    Presentation
  98. Chandan Hati (Instituto de Física Corpuscular (IFIC), CSIC‐Universitat de València, Spain)
    03/09/2025, 12:40
    Presentation
  99. Dr Mauricio Bustamante (Niels Bohr Institute)
    04/09/2025, 09:30
    Presentation
  100. Sei Ban (ICEPP, U.Tokyo)
    04/09/2025, 10:00
    Presentation
  101. Prof. Jianming Bian (University of California Irvine (US))
    04/09/2025, 11:00
    WG6 - Detectors
    Presentation
    WG6

    DUNE is the flagship next-generation neutrino experiment in the United States, designed to decisively measure neutrino CP violation and determine the mass hierarchy. It utilizes the Liquid Argon Time Projection Chamber (LArTPC) technology, which provides exceptional spatial resolution and the potential to accurately identify final state particles and neutrino interactions. However, the...

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  102. Claudio Coletta (Università di Milano-Bicocca e INFN-MIB)
    04/09/2025, 11:00
    WG5 - Neutrinos Beyond PMNS
    Presentation
    WG5

    The JUNO detector (Jiangmen Underground Neutrino Observatory), located in Jiangmen, southern China, is currently in its commissioning phase. Its main goal is to determine the neutrino mass ordering and to reduce uncertainties on oscillation parameters. Thanks to its huge liquid scintillator mass (20 kton), its high radiopurity and excellent energy resolution, JUNO is an ideal candidate to...

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  103. Guilherme Soares
    04/09/2025, 11:00
    WG2 - Neutrino Scattering
    Presentation
    WG2

    The SND@LHC experiment was designed to perform measurements with neutrinos produced at the LHC within the unexplored pseudo-rapidity range of 7.2 < 𝜂 < 8.6. Located 480 m downstream of IP1 in the unused TI18 tunnel, this compact and stand-alone experiment employs a hybrid detector system consisting of 800 kg of tungsten plates interleaved with emulsion and electronic trackers, complemented by...

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  104. Namitha Chithirasreemadam (University of Pisa)
    04/09/2025, 11:00
    WG4 - Muon Physics
    Presentation
    WG4

    The Mu2e experiment at Fermilab will search for the coherent, neutrinoless conversion of a negative muon into an electron in the field of an aluminum nucleus, an example of Charged Lepton Flavor Violation (CLFV). Observation of CLFV at Mu2e would be an unambiguous signal of physics beyond the Standard Model (BSM). Mu2e aims to improve upon the current best sensitivity on the conversion rate by...

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  105. Marc Andre Jebramcik (CERN)
    04/09/2025, 11:00
    WG3 - Accelerator Physics
    Presentation

    The poor knowledge of neutrino cross sections at the GeV scale is projected to be responsible for some of the leading sources of uncertainty in next-generation oscillation experiments. Building on the ideas and R&D from ENUBET and NuTAG, we present a proposal for the nuSCOPE experiment (see arXiv:2503.21589). nuSCOPE is a high-precision, short-baseline neutrino experiment at CERN that employs...

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  106. Simon Thor (ETH Zurich (CH))
    04/09/2025, 11:23
    WG2 - Neutrino Scattering
    Presentation
    WG2

    The ForwArd Search ExpeRiment (FASER) is designed to search for particles produced in the far-forward region of pp collisions at the LHC at CERN. Its primary goals are to detect high-energy neutrinos and light, feebly interacting new particles predicted by extensions of the Standard Model. Since its inception in 2022, FASER has collected close to 200/fb of data during LHC Run 3, leading to...

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  107. Ryo Nagai
    04/09/2025, 11:25
    WG4 - Muon Physics
    Presentation
    WG4

    The COMET experiment at J-PARC is designed to search for the neutrinoless, coherent conversion of a muon to an electron in the field of a nucleus ($\mu^-N \to e^-N$), a process that violates charged lepton flavor conservation and is forbidden in the Standard Model. The experiment aims to reach a single-event sensitivity of $\mathcal{O}(10^{-17})$, improving the current upper limit by four...

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  108. Gabriela Vitti Stenico (The University of Edinburgh)
    04/09/2025, 11:25
    WG6 - Detectors
    Presentation
    WG6

    ProtoDUNE is a Liquid Argon Time Projection Chamber (LArTPC) and one of the prototypes for the future Deep Underground Neutrino Experiment (DUNE). Besides testing and improving LArTPC detection performance, ProtoDUNE goals also reside in exploring the interaction of charged particles with Liquid Argon to enhance the particle reconstruction capabilities for the future neutrino interactions in...

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  109. Anthony Onillon (Max-Planck-Institut für Kernphysik)
    04/09/2025, 11:25
    WG5 - Neutrinos Beyond PMNS
    Presentation
    WG5

    The KATRIN experiment is designed to measure the mass of the electron antineutrino by studying the high-energy end of the tritium β decay spectrum. In addition, KATRIN is also a well-suited instrument to explore the sterile neutrino hypothesis. The existence of sterile neutrinos would cause a kink-like distortion in the spectrum.

    Using the same datasets as for active neutrino mass, KATRIN...

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  110. Alysia Marino (University of Colorado Boulder (US))
    04/09/2025, 11:25
    WG3 - Accelerator Physics
    Presentation

    Long-baseline accelerator neutrino experiments rely on the neutrinos from the decays of hadrons produced in hadron-nucleus interactions. Uncertainties in the hadron production yields from these interactions dominate the neutrino flux uncertainties in these beams. This talk will highlight recent results from CERN’s SPS Heavy Ion and Neutrino Experiment (NA61/SHINE), which has produced...

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  111. Laura-Iuliana Munteanu (CERN)
    04/09/2025, 11:45
    WG2 - Neutrino Scattering
    Presentation
    WG2

    The poor knowledge of neutrino cross sections at the GeV scale is projected to be responsible for some of the leading sources of uncertainty in next-generation oscillation experiments. Building on the ideas and R&D from ENUBET and NuTAG, we present a proposal for the nuSCOPE experiment (see arXiv:2503.21589). nuSCOPE is a high-precision, short-baseline neutrino experiment at CERN that employs...

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  112. Paolo Walter Cattaneo (Pavia University and INFN (IT))
    04/09/2025, 11:50
    WG4 - Muon Physics
    Presentation
    WG4

    Searches for charged lepton flavor violation in the muon sector stand out among the most sensitive and clean probes for physics beyond the Standard Model. Currently, $\mu^+ \to e^+ \gamma$ experiments provide the best constraints in this field and, in the coming years, new experiments investigating the processes of $\mu^+ \to e^+e^+e^-$ and $\mu \to e$ conversion in the nuclear field are...

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  113. Ian Heitkamp
    04/09/2025, 11:50
    WG3 - Accelerator Physics
    Presentation

    The Tokai-to-Kamioka (T2K) experiment uses high intensity beams of neutrinos and anti-neutrinos produced at the Japan Proton Accelerator Research Complex (J-PARC) to measure neutrino oscillations over a baseline of 295 km, and search for evidence of CP violation. Neutrinos come from in-flight decays of charged hadrons produced from interactions of 30 GeV protons in a long graphite target. The...

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  114. Dr Jessie Micallef (Tufts University (and MIT))
    04/09/2025, 11:50
    WG6 - Detectors
    Presentation
    WG6

    In the global scientific effort to better understand how neutrinos fit (or don’t) within the bounds of the Standard Model, the Deep Underground Neutrino Experiment (DUNE) aims to make precise neutrino oscillation measurements to determine the neutrino mass ordering and determine the value of neutrino Charge-Parity (CP) violation. To accomplish this, DUNE has a host of near detectors that will...

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  115. Tomas Jezo (WWU ITP)
    04/09/2025, 12:08
    WG2 - Neutrino Scattering
    Presentation
    WG2

    We present a new global analysis of nuclear PDFs in the nCTEQ approach. Building on a modern proton baseline without nuclear data, we combine and update previous separate analyses that focused on JLab neutral-current DIS, neutrino DIS and dimuon production, and the currently available LHC data, in particular on W/Z and heavy quark production. For the latter, we not only employ a data-driven...

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  116. Radoslav Marchevski (École Polytechnique Fédérale de Lausanne (EPFL))
    04/09/2025, 12:15
    Presentation

    Neutrino tagging is a new experimental approach for accelerator-based neutrino experiments. The method consists in associating a neutrino interaction with the meson decay (i.e. or ) in which the neutrino was originally produced. The properties of the neutrino can then be estimated kinematically from the decay incoming and outgoing charged particles. The reconstruction of these particles...

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  117. Marvin Pfaff (Imperial College (GB))
    04/09/2025, 13:45
    WG1 - Neutrino Oscillations
    Presentation

    Current neutrino experiments are making world-leading measurements of the PMNS parameters and will continue to collect data and improve their analyses to push towards the precision era, which will be fully realised with the next generation of oscillation experiments. These next-generation experiments will not only be able to make precision measurements of the PMNS parameters but will also be...

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  118. Katharina Lachner (ETH Zurich (CH))
    04/09/2025, 13:45
    WG2 - Neutrino Scattering
    Presentation
    WG2

    The T2K experiment's primary off-axis near detector, ND280, has the essential role of constraining the main systematic uncertainties that affect neutrino oscillation measurements. Among the leading sources of these uncertainties are neutrino-nucleon interaction cross sections, which must be more precisely understood to fully exploit the potential of current and future long-baseline neutrino...

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  119. Piotr Podlaski (KEK High Energy Accelerator Research Organization (JP))
    04/09/2025, 13:45
    WG3 - Accelerator Physics
    Presentation
    WG3

    A high-intensity 30 GeV proton beam produced by the J-PARC Main Ring (MR) accelerator is used to generate one of the world’s most intense conventional neutrino beams, which plays a central role in J-PARC’s long-baseline neutrino program. This beam supports the ongoing T2K experiment and will provide accelerator neutrinos to the forthcoming Hyper-Kamiokande experiment, currently under...

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  120. Felice Nenna (Universita e INFN, Bari (IT))
    04/09/2025, 13:45
    WG4 - Muon Physics
    Presentation
    WG4

    Tests of lepton flavor conservation and universality offer a sensitive probe for physics beyond the Standard Model (SM), with several BSM scenarios predicting deviations accessible at the CMS experiment. This contribution presents an overview of CMS results from searches for Lepton Flavor Violation (LFV) and Lepton Flavor Universality (LFU) violation in proton-proton collisions at a...

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  121. Davide Sgalaberna (ETH Zurich (CH))
    04/09/2025, 13:45
    WG6 - Detectors
    Presentation
    WG6

    The Tokai-to-Kamiokande (T2K) experiment is a long-baseline neutrino experiment based in Japan. T2K obtained results that disfavour CP conservation with a 90% confidence level so far. The (anti)neutrino beam created at J-PARC is characterised at the near detector before measuring the oscillated spectrum using the Super-Kamiokande detector 296 km away. Toward more precise measurements of...

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  122. Dr César Jesús-Valls (CERN)
    04/09/2025, 14:08
    WG2 - Neutrino Scattering
    Presentation
    WG2

    The T2K experiment has operated for over a decade using the on-axis near detector INGRID and ND280 as the primary near detector for oscillation and neutrino interaction physics at 2.5 degrees off-axis, both located at JPARC. Recent upgrades to T2K include an increased power at JPARC's neutrino beamline, detector upgrades to ND280, and the installation of a second near detector,...

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  123. Ian Heitkamp
    04/09/2025, 14:10
    WG3 - Accelerator Physics
    Presentation
    WG3

    T2K is a long baseline off-axis neutrino experiment located in Japan with the goal of precisely measuring neutrino oscillations. To maintain stable beam operation, a muon monitor (MUMON) is used to indirectly measure the neutrino beam direction and intensity via the coincident muons. Ongoing work continues at J-PARC to prepare the beamline for higher intensity beam operation up to a planned...

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  124. Dr Ligang Xia (Nanjing University (CN))
    04/09/2025, 14:10
    WG4 - Muon Physics
    Presentation
    WG4

    The Standard Model predicts several rare Higgs boson processes, including decays into a Z boson and a photon, a low-mass lepton pair and a photon, or a meson and a photon. Observing these rare decays would offer new and complementary insights into the Higgs boson's coupling structure beyond the more commonly studied channels. In addition, searches for lepton-flavor-violating decays of the...

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  125. Soniya Samani (Universite de Geneve (CH))
    04/09/2025, 14:10
    WG6 - Detectors
    Presentation
    WG6

    Precision measurements of neutrino oscillation parameters in the Tokai to Kamioka (T2K) long-baseline neutrino experiment require a robust and accurate understanding of neutrino–nucleus interactions. The T2K near detector complex, ND280, is specifically designed to constrain neutrino flux parameters and cross-section models through detailed analyses of neutrino interactions. As part of the...

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  126. Sho Sugama (Yokohama National University)
    04/09/2025, 14:10
    WG5 - Neutrinos Beyond PMNS
    Presentation

    We study a method to test the unitarity of the PMNS matrix by using only
    the long baseline neutrino oscillation experiment, such as the combination of
    the T2HK experiment and the one with the $\nu_e$ beam from a future neutrino
    factory at J-PARC. Without a specific parametrization, one can directly extract
    the elements of the lepton mixing matrix by observing the energy dependence of
    the...

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  127. Seungho Han
    04/09/2025, 14:30
    WG2 - Neutrino Scattering
    Presentation
    WG2

    We present preliminary measurements on $\nu_\mu$ charged-current interactions on water, obtained from the first physics run of the NINJA experiment. The interactions were recorded using nuclear emulsion detectors with a 75 kg water target exposed to a J-PARC $\nu_\mu$ beam of mean energy 0.86 GeV and a total exposure of $4.8\times10^{20}$ protons on target. The sub-micrometer spatial...

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  128. Dr Jessie Micallef (Tufts University (and MIT))
    04/09/2025, 14:35
    WG1 - Neutrino Oscillations
    Presentation

    MicroBooNE uses a liquid argon time projection chamber (LArTPC) detector to investigate the observed anomalous low energy excess (LEE) of single electromagnetic shower events reported by the MiniBooNE experiment. After five years of data taking from two accelerator beamlines at Fermilab, MicroBooNE has recently published results testing explanations for the MiniBooNE anomaly, including three...

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  129. Davide Sgalaberna (ETH Zurich (CH))
    04/09/2025, 14:35
    WG6 - Detectors
    Presentation
    WG6

    Hyper-Kamiokande will start collecting accelerator neutrino data in 2028 to search for leptonic CP violation. The largest systematic uncertainty, $\Delta (\sigma_{{\nu}_e}/\sigma_{\bar{\nu}_e})$, is related to the ratio between the electron neutrino and antineutrino cross section. A not proper modeling could generate an ambiguous asymmetry in the ratio between the $\nu_{\mu} \to \nu_e$ and...

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  130. Rui Franqueira Ximenes (CERN)
    04/09/2025, 14:35
    WG3 - Accelerator Physics
    Presentation
    WG3

    The International Muon Collider Collaboration (IMCC) is studying a multi-TeV muon collider. One of the most challenging aspects is the MW-class production Target, which must withstand nanosecond-scale and high-intensity proton bunches, while delivering optimal pion-muon yields from the start of the frontend. In addition to the high thermal shock and average power, resistance to fatigue and...

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  131. Anezka Klustova
    04/09/2025, 14:52
    WG2 - Neutrino Scattering
    Presentation
    WG2

    Understanding both neutrino and antineutrino interactions in the few-GeV regime is necessary for precision measurements of neutrino oscillations. In particular, it is crucial to study the nuclear effects that can alter final-state topology and kinematics, potentially biasing neutrino energy reconstruction. MINERvA is a high-statistics cross-section experiment designed to study such nuclear...

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  132. Luis Mora-Lepin (Florida State University)
    04/09/2025, 15:00
    WG6 - Detectors
    Presentation
    WG6

    The Accelerator Neutrino Neutron Interaction Experiment (ANNIE) is a 26-ton gadolinium loaded water Cherenkov detector installed on the Booster Neutrino Beam (BNB) line at Fermilab. ANNIE physics goals include measuring the neutron multiplicity in neutrino-nucleus interactions and the charged current cross-section of muon neutrino interactions with water. In addition, ANNIE serves as a...

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  133. Javier Garcia Marcos
    04/09/2025, 16:05
    WG2 - Neutrino Scattering
    Presentation
    WG2

    Liquid argon serves as detector material in several present and future accelerator-based neutrino experiments, such as MicroBooNE, SBND, ICARUS [1] and DUNE [2].

    Therefor, precise information about the structure of the target nucleus—that is, the binding energies and momentum distributions of the nucleons—is crucial for accurate modeling of neutrino–nucleus cross sections. This is...

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  134. Samuel Grant (ARGONNE NATIONAL LABORATORY)
    04/09/2025, 16:15
    WG4 - Muon Physics
    Presentation

    The Mu2e experiment at Fermilab will conduct a world-leading search for Charged Lepton Flavour Violation (CLFV) in neutrino-less muon-to-electron conversion in the field of a nucleus. In doing so, it will provide a powerful probe into physics beyond the Standard Model, which can greatly enhance the rates of CLFV processes. To accomplish this measurement, which will constitute an...

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  135. Prof. Helen O'Keeffe (Lancaster University)
    04/09/2025, 16:15
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    T2K is a long-baseline neutrino oscillation experiment, measuring the oscillation of neutrinos and antineutrinos produced at J-PARC facility which then travel 295 km across Japan to its far detector, Super Kamiokande. T2K has been taking data since 2009 and sets world-leading constraints on many neutrino oscillation parameters within the standard PMNS three-flavour mixing paradigm, including...

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  136. paloma Rodriguez Casale (Universidad de Granada)
    04/09/2025, 16:27
    WG2 - Neutrino Scattering
    Presentation
    WG2

    We compute the contribution of meson-exchange currents (MEC) to the one-particle
    emission transverse response of nuclear matter, including short-range correlations (SRC)
    within the independent pair approximation. Our results show a significant enhancement
    of the transverse response in electron scattering, in contrast to independent-particle
    models that neglect SRC [1]. SRC are incorporated...

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  137. Pierre Boistier (CEA Paris-Saclay, Université Paris-Saclay (FR))
    04/09/2025, 16:40
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    T2K is a long-baseline neutrino oscillation experiment located in Japan. Its aim is to undertake precise measurements of the atmospheric parameters |dm2_23|, sin2theta23 and to search for CP-violation within the leptonic sector, which would manifest as a discrepancy between neutrino and anti-neutrino oscillations. Thanks to its focussing horns, the T2K experiment has the faculty to produce...

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  138. Timothy Hume (Paul Scherrer Institute)
    04/09/2025, 16:40
    WG4 - Muon Physics
    Presentation

    A dedicated search for the muon electric dipole moment using the frozen-spin technique [1] promises to extend our reach towards physics beyond the Standard Model incorporating additional sources of CP violation. The muEDM Collaboration is developing a compact frozen-spin trap [2] to enable a first demonstration of this technique, with a target sensitivity of $6\times10^{-23}\,e\mathrm{cm}$,...

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  139. Arie Bodek (University of Rochester (US))
    04/09/2025, 16:50
    WG2 - Neutrino Scattering
    Presentation
    WG2

    We report on global extractions of the $\rm^{12}C$, $\rm^{40}Ca$ and $\rm^{56}Fe$ longitudinal (${\cal R}_L$) and transverse (${\cal R}_T$) nuclear electromagnetic response functions from an analysis of all available electron scattering and photoprodution data on these nuclei. The response functions are extracted for energy transfer $\nu$, spanning the nuclear excitation,...

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  140. Vanessa Cerrone (University of Padova / INFN Padova)
    04/09/2025, 17:05
    WG1 - Neutrino Oscillations
    Presentation
    WG1

    The Jiangmen Underground Neutrino Observatory (JUNO) is a next-generation neutrino experiment in South China currently in its commissioning phase. Situated under 650 meters of rock overburden ($\sim$1800 meters water equivalent), JUNO’s central detector consists of a 20-kton liquid scintillator target housed in a 35.4-meter-diameter acrylic sphere. It achieves remarkable 75% photocathode...

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  141. Matthias Hooft (Ghent university)
    04/09/2025, 17:13
    WG2 - Neutrino Scattering
    Presentation
    WG2

    Single-pion production provides an important contribution to the total neutrino-nucleus interaction cross section in neutrino oscillation experiments. This contribution improves the Ghent Hybrid model in the delta-resonance region. The philosophy of this work is to incorporate as much physics constraints as possible while keeping the amount of fitted parameters as low as possible. The model is...

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  142. Aaron Meyer
    04/09/2025, 17:35
    WG2 - Neutrino Scattering
    Presentation
    WG2

    The Axial Form Factor Extracted from Elementary Targets"
    Abstract: Next generation neutrino oscillation experiments are poised to provide answers to key questions about the nature of the neutrino. The nucleon axial form factor is a vital ingredient for constructing nucleon amplitudes and predicting quasielastic scattering cross sections, a primary measurement process for flagship oscillation...

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  143. Zhiyuan Chen (Institute of High Energy Physics, Chinese Academy of Sciences)
    05/09/2025, 09:00
    Presentation
  144. Davide Meloni (Universita' di Roma 3)
    05/09/2025, 09:30
    Presentation
  145. José I. Crespo-Anadón (CIEMAT (Spain))
    05/09/2025, 10:00
    Presentation
  146. Matt Mears (University of Sheffield)
    05/09/2025, 11:00
    Presentation
  147. Felix Kling (DESY)
    05/09/2025, 11:30
    Presentation
  148. k Mavrokoridis (University of Liverpool (GB))
    05/09/2025, 12:00
    Presentation
  149. Alexander Valishev (Fermilab)
    05/09/2025, 14:00
    Presentation
  150. Megan Friend (KEK High Energy Accelerator Research Organization (JP))
    05/09/2025, 14:30
    Presentation
  151. Ana Margarida TEIXEIRA
    05/09/2025, 15:00
    Presentation
  152. Zahra Khajeh Tabrizi
    05/09/2025, 16:00
    Presentation
  153. Jan Sobczyk
    05/09/2025, 16:30
    Presentation
  154. Diego Aristizabal (Universidad Tecnica Federico Santa Maria (USM))
    05/09/2025, 17:00
    Presentation
  155. yun tse tsai (SLAC)
    06/09/2025, 09:00
    Presentation
  156. Elena Gramellini (University of Manchester)
    06/09/2025, 09:30
    Presentation
  157. Maja Olvegaard (Uppsala University (SE))
    06/09/2025, 10:00
    Presentation
  158. Simon Corrodi
    06/09/2025, 11:00
    Presentation
  159. Matheus Hostert
    06/09/2025, 11:30
    Presentation
  160. Dr Akira Takenaka (Shanghai Jiao Tong University, Tsung-Dao Lee Institute)
    06/09/2025, 12:00
    Presentation
  161. Dr POONAM MEHTA (Jawaharlal Nehru University)
    06/09/2025, 12:30
    Presentation
  162. Steven Robertson (IPP / University of Alberta)
    WG4 - Muon Physics
    Presentation
    WG4

    The Belle and Belle II experiments have collected a $1.6~\mathrm{ab}^{-1}$ sample of $e^+e^-$ collision data at centre-of-mass energies near the $\Upsilon(nS)$ resonances. This sample contains approximately 1.5 billion $e^+e^-\to \tau^+\tau^{-}$ events, which we use to search for lepton-flavour violating decays. We present searches for $\tau\to\ell\gamma$, tau decay to three charged leptons,...

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