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Jianglai Liu (Shanghai Jiao Tong University)8/31/26, 8:50 AM
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Prof. Kim Siang Khaw (TDLI/SJTU)8/31/26, 8:55 AM
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Yun-Tse Tsai (SLAC)8/31/26, 9:00 AM
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Elena Gramellini (University of Manchester)8/31/26, 9:15 AM
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Maja Olvegård (Uppsala University)8/31/26, 9:30 AM
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Lily Morvaj (PSI)8/31/26, 9:45 AM
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Matheus Hostert (University of Iowa)8/31/26, 10:00 AM
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Akira Takenaka (Sun Yat-sen University)8/31/26, 10:15 AM
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Poonam Mehta (Jawaharlal Nehru University)8/31/26, 10:30 AM
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Felix Cormier (TRIUMF)8/31/26, 11:00 AM
T2K is a long-baseline neutrino experiment operating in Japan which has achieved world-leading measurements of neutrino and anti-neutrino oscillation. The J-PARC accelerator complex produces a stream of muon neutrinos or anti-neutrinos which are measured at a near detector complex as well as at a Water Cherenkov far detector, Super-Kamiokande, 295km away. Near and far detector measurements of...
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Jianming Bian (University of California, Irvine)8/31/26, 11:30 AM
NOvA is a long-baseline, accelerator-based neutrino oscillation experiment, optimized for electron neutrino measurements. It utilizes the upgraded, Megawatt-capable NuMI beam from Fermilab to measure electron-neutrino appearance and muon-neutrino disappearance at its Far Detector in Ash River, Minnesota. NOvA's goals include resolving the neutrino mass hierarchy problem, constraining the...
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黄俊挺 （Junting Huang） (Shanghai Jiao Tong University)8/31/26, 12:00 PM
The Jiangmen Underground Neutrino Observatory (JUNO) is a multi-purpose neutrino experiment located in southern China. It features a \SI{20}{kton} liquid scintillator detector designed primarily to measure antineutrinos emitted from the Taishan and Yangjiang nuclear power plants, both situated at a baseline of 52.5 km. Its core physics goals include determining the neutrino mass ordering and...
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Ben Jargowsky (Boston University)8/31/26, 2:00 PM
Super-Kamiokande is a large water Cherenkov detector located in Mount Ikenoyama, Japan, which recently celebrated its 30th anniversary of operation. We present several new results, including new atmospheric, supernova, and solar analyses. The new atmospheric oscillation analysis includes the period SK VI, the first period where gadolinium was introduced into the water for enhanced neutron...
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Nicholas Latham (King's College London)8/31/26, 2:30 PM
The Hyper-Kamiokande (Hyper-K) is the third generation of underground water Cherenkov detectors in Japan. It will serve as: (1) the far detector for a long-baseline neutrino oscillation experiment for the upgraded, 1.3 MW power, J-PARC muon neutrino/antineutrino beam, and (2) a detector capable of observing proton decays, atmospheric neutrinos, and neutrinos from astronomical sources. The...
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Prof. Davide Sgalaberna (ETH Zurich)8/31/26, 3:00 PM
Scintillator-based detectors are widely used in neutrino experiments owing to their particle-tracking and calorimetry capabilities.
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Traditionally, achieving high spatial resolution alongside a massive active target requires both segmentation and optical separation, that comes at the cost of increased manufacturing complexity and a massive number of readout channels.
To overcome these... -
Prof. Maxim Pospelov (University of Minnesota)8/31/26, 4:00 PM
I review the current status of the Electric Dipole Moment program. Stringent limits on EDMs provide very sensitive constraints on new physics beyond the Standard Model. I also review the predictions of EDMs from the SM source of CP violation.
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Lucy Bailey (UCL)8/31/26, 4:30 PM
After 6 years of taking data, the Muon g-2 Experiment measured the anomalous magnetic moment of the muon to a final precision of 127 ppb. In parallel to this analysis, it is possible to perform a measurement of the muon electric dipole moment (EDM) using the straw tracker detectors. In the Standard Model (SM) EDMs are predicted to be vanishingly small. A non-zero muon EDM would constitute...
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Thomas Benjamin Wester (University of Chicago)8/31/26, 5:00 PM
The Short-Baseline Near Detector (SBND) is one of three liquid argon time projection chamber (LArTPC) neutrino detectors positioned along the axis of the Booster Neutrino Beam (BNB) at Fermilab, and serves as the near detector in the Short-Baseline Neutrino (SBN) Program. The detector just completed its second year of running, collecting over 6.5e20 POT, equivalent to an unprecedented sample...
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Mr 王家斌 （Jiabin Wang） (Shandong University), 谭晓晗 （Xiaohan Tan） (Shandong University)8/31/26, 6:00 PM
The Jiangmen Underground Neutrino Observatory (JUNO) is a multi-purpose neutrino experiment located in southern China, featuring a 20-kton liquid scintillator detector with excellent energy resolution and large target mass. JUNO has been collecting full liquid scintillator data since August 2025. While primarily designed to determine the neutrino mass ordering (NMO) using reactor...
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Mr 曾永浩 (Yonghao Zeng) (Tsung-Dao Lee Institute, Shanghai Jiao Tong University)8/31/26, 6:00 PM
The muon electric dipole moment (EDM) is a sensitive probe of charge-parity (CP) violation and physics beyond the Standard Model. In the Fermilab Muon g−2 experiment, an EDM introduces an additional spin-precession component that produces a vertical oscillation in the decay-positron distribution that can be measured by the calorimeters. For a muon EDM smaller than the current limit set by the...
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朱峻毅 （Junyi Zhu） (Shandong University), 魏俊雅 （Junya Wei） (Shandong University)8/31/26, 6:00 PM
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kton liquid scintillator detector designed for the determination of neutrino mass ordering and precise neutrino oscillation parameter measurements. Accurate reconstruction of cosmic muon tracks is essential for suppressing cosmogenic backgrounds and improving the neutrino signal efficiency.
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In this poster, we present a... -
皮旻 （Min Pi) (武汉大学)8/31/26, 6:00 PM
The Taishan Antineutrino Observatory (TAO) is a compact spherical liquid scintillator detector designed to achieve excellent energy resolution for precision reactor antineutrino measurements. Owing to the compact detector geometry, photon timing information provides limited discrimination for event reconstruction, motivating the development of a reconstruction algorithm based solely on the...
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Roni Dey (TDLI,SJTU)8/31/26, 6:00 PM
The PandaX-20T experiment, a next-generation multi-ton liquid xenon TPC at the China Jinping Underground Laboratory, aims to achieve unprecedented sensitivity for direct dark matter detection. As experiments approach the neutrino-floor regime, efficient suppression of neutron and gamma-induced backgrounds becomes increasingly important. An active Cold Liquid Scintillator (CLS) veto...
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Camilla Forza8/31/26, 6:00 PM
A new Beam Loss Monitor (BLM) is being developed for the J-PARC neutrino beamline. Several detectors will be installed in and immediately downstream of the Main Ring (MR) fast-extraction region, where the 30 GeV proton beam is extracted toward the neutrino production target. Designed for operation in a high-radiation environment and to remain compatible with the planned J-PARC neutrino...
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Luis A. Delgadillo (IHEP)8/31/26, 6:00 PM
The determination of the weak mixing angle, $\sin^2\theta_W$, at low momentum transfers remains a powerful test of the Standard Model and its potential new physics extensions. Here, I will explore some physics opportunities at present and future reactor neutrino experiments through elastic neutrino-electron scattering (E$\nu$ES). I will show the expected sensitivity to the weak mixing angle...
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廖依林 (Yilin Liao)8/31/26, 6:00 PM
Energy Response Model of the JUNO Central Detector
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20 kton liquid scintillator detector that started data-taking since late Aug,2025. The primary physics goal is to determine the neutrino mass ordering through a precision measurement of the reactor anti-neutrino energy spectrum. This requires a precise calibration of energy...
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李赫 (He Li) (Tohoku University)8/31/26, 6:00 PM
The accelerator-based neutrino oscillation experiment T2K aims to investigate neutrino CP violation by measuring differences in oscillation probabilities between neutrinos and antineutrinos. One of the dominant sources of systematic uncertainty in T2K arises from neutrino–nucleus interaction modeling. In particular, tree-level photon-emission contributions to the neutrino–nucleus cross section...
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Pierre Granger (CERN)8/31/26, 6:00 PM
Next-generation neutrino oscillation experiments operate in highly complex parameter spaces where the physics of interest is tightly coupled with multi-dimensional systematic uncertainties. Traditional neutrino oscillation calculators lack gradient information, limiting experimental design, sensitivity forecasting, and profile likelihood fits to computationally expensive, derivative-free grid...
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DEK HAO LIEW, Mohammad Nizam (Xiamen University Malaysia)8/31/26, 6:00 PM
Although large liquid scintillator detectors are primarily designed for reactor antineutrino measurements, their large fiducial volume and excellent energy resolution also enable the observation of atmospheric neutrino interactions. We investigate the potential of machine-learning-assisted event classification to achieve statistical neutrino–antineutrino discrimination in atmospheric neutrino...
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Dr 牛苑好 （Yuanhao Niu) (山西大学理论物理研究所 & 中国科学院高能物理研究所)8/31/26, 6:00 PM
A $10~\mathrm{atm}$ $\mathrm{CF}_4$ based Time Projection Chamber (TPC) is under R&D for detecting reactor antineutrinos via neutrino electron elastic scattering $(\nu - e^- \to \nu - e^-)$. The physics goals are to precisely measure the antineutrino spectrum below the inverse $\beta$ decay threshold and to constrain the neutrino magnetic moment. This requires both high energy resolution and...
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Loris Martinez (IFAE)8/31/26, 6:00 PM
Accurate reconstruction of pion production is essential for neutrino oscillation measurements in water Cherenkov detectors, where undetected or poorly reconstructed pions can bias neutrino energy estimation and event interpretation. This poster presents studies of pion-induced signatures in Cherenkov detectors, with a focus on recovering the decay electron from the π → μ → e decay chain to...
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Zhangming Chen8/31/26, 6:00 PM
Jiangmen Underground Neutrino Observatory (JUNO) is a multi purpose 20 kton liquid scintillator detector located in southern China. A primary physics goal of JUNO is to determine the neutrino mass ordering using reactor antineutrinos. Achieving this goal critically depends on the detector’s excellent energy resolution, which is directly influenced by the accuracy of waveform reconstruction...
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jinhe cui (Institute of Modern Physics)8/31/26, 6:00 PM
This study investigates the production, transport, and optical optimization of secondary μ⁺ beams in HFRS using an integrated G4Beamline–MAD-X model incorporating the graphite target, two-stage separator, key focal planes, and the MF6 exit. Comparisons of forward π⁺ production from ¹⁶O and ¹⁸O beams at different energies show that ¹⁸O at 4.26 GeV/u provides the highest yield and the strongest...
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Dr Bhavna Yadav (Wilczek Quantum Center, SIAS, USTC)8/31/26, 6:00 PM
We investigate Quantum Fisher Information (QFI) as a measurement-independent measure of parameter sensitivity in three-flavor neutrino oscillations. Focusing on the $\nu_\mu \rightarrow \nu_e$ appearance channel, we evaluate the QFI for the leptonic CP-violating phase $\delta_{\rm CP}$, the atmospheric mixing angle $\theta_{23}$, and the atmospheric mass-squared difference $\Delta m_{31}^{2}$...
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徐靖桓 （Jinghuan Xu) (广西大学 & 中国科学院高能物理研究所)8/31/26, 6:00 PM
This poster presents the developmental progress of a time projection chamber (TPC) detector based on gas electron multipliers (GEMs) as the key amplification component. The detector is designed to enable high-precision measurements of the reactor neutrino energy spectrum below the inverse beta decay (IBD) threshold, and to facilitate studies of physics topics such as the neutrino anomalous...
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张荣凭 (Rongping Zhang)8/31/26, 6:00 PM
The Reactor Antineutrino Anomaly (RAA)—a long-standing discrepancy between the measured and predicted antineutrino flux—has been a cornerstone in the search for light sterile neutrinos. In recent years, the anomaly was partially attributed to uncertainties in reactor flux models, particularly the 235U contribution. However, new experimental results, most notably from the BEST gallium...
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Guan Ming Wong (Tsung-Dao Lee Institute, SJTU)8/31/26, 6:00 PM
The muEDM experiment at the Paul Scherrer Institute (PSI) aims to measure the muon electric dipole moment (EDM) - a charge-parity (CP) violating observable - with an unprecedented final sensitivity of 𝜎(𝑑𝜇 ) ≤ 6 × 10−23 𝑒 ⋅ 𝑐𝑚 using the frozen-spin technique. This sensitivity, an improvement of over three orders of magnitude compared to the current limit, would probe beyond-Standard Model new...
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Chisako ISE (Tokyo University of Science)8/31/26, 6:00 PM
The Intermediate Water Cherenkov Detector (IWCD) will be constructed approximately 1 km downstream of the J-PARC neutrino beam target to improve neutrino oscillation measurements in Hyper-Kamiokande by reducing systematic uncertainties, particularly those associated with neutrino interaction cross sections. In this study, simulations were conducted to evaluate the performance of and optimize...
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Ritesh Kumar Pradhan (Indian Institute of Technology, Hyderabad)8/31/26, 6:00 PM
Understanding neutrino-nucleus interactions is important for reducing systematic uncertainties in precise measurements of neutrino oscillation parameters. These interactions can be studied in NOvA, a long-baseline neutrino experiment that measures electron neutrino appearance and muon neutrino disappearance. The NOvA Near Detector, located ~ 1 km from the beam target, records a high statistics...
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34. Top Drift Electronics: Architecture and Production for DUNE’s Far Detector Vertical Drift ModuleKarishma Dhanmeher (Institute of Physics of the 2 Infinities of Lyon, France)8/31/26, 6:00 PM
The Deep Underground Neutrino Experiment (DUNE) represents the next frontier in particle physics, aiming to unlock the mysteries of the neutrino sector through advanced detector technology. The Vertical Drift (FD-VD) is one of the four planned DUNE Far Detector (FD) modules. It features an innovative architecture that replaces traditional wire anodes with perforated printed circuit board (PCB)...
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Dongha Lee (KEK)9/1/26, 9:00 AM
The JSNS2 (J-PARC Sterile Neutrino Search at the J-PARC Spallation
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Neutron Source) experiment searches for neutrino oscillations over a
baseline of 24 m, targeting Δm² values around 1 eV². Its primary goal is
to provide a direct test of the LSND anomaly.
The experiment has carried out physics runs from 2021 to 2026,
accumulating a total exposure of 6 × 10²² protons on target (POT) at... -
Tatsuya Kikawa (Kyoto University)9/1/26, 9:30 AM
A precise understanding of neutrino interactions is essential for fully exploiting the physics potential of current and next-generation neutrino experiments. In particular, uncertainties in neutrino–nucleus interactions and nuclear effects are becoming increasingly important as oscillation measurements enter the precision era. At the same time, measurements of neutrino scattering provide...
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Prof. David Caratelli (UCSB)9/1/26, 10:00 AM
MicroBooNE Status
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Miguel Angel Garcia Peris (University of Manchester)9/1/26, 11:00 AM
Since 2018, the ProtoDUNE programme at CERN has been the cornerstone of the DUNE development effort, providing large-scale prototypes where detector technologies, infrastructure, operational procedures, and analysis and calibration techniques are tested and validated under realistic conditions. With two generations of prototypes already successfully operated and a third generation in...
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Feng Zhang (Laser Fusion Research Center, CAEP)9/1/26, 11:30 AM
Muons, which play a crucial role in both fundamental and applied physics, have traditionally been generated through proton accelerators or from cosmic rays. In this work, we show the first proof of principle experiment for novel muon production with an ultra-short, high-intensity laser device through GeV electron beam bombardment on a lead converter target. The results show that the dominant...
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Poonam Mehta (Jawaharlal Nehru University)9/1/26, 12:00 PMOral contribution
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Kajetan Niewczas (École polytechnique, IN2P3-CNRS, Laboratoire Leprince-Ringuet, France)9/1/26, 2:00 PM
The precise measurement of neutrino properties is among the highest priorities in fundamental particle physics. Accelerator-based neutrino experiments provide a unique framework for such studies, providing oscillation measurements and hints of the CP violation in the leptonic sector. However, since these experiments rely on the interaction of neutrinos with bound nucleons inside atomic nuclei,...
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David Caratelli (UC Santa Barbara)9/1/26, 2:00 PMWG1: Neutrino Oscillation PhysicsOral contribution
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. By leveraging the LArTPC technology's ability to distinguish electron and photon electromagnetic showers, MicroBooNE is able to thoroughly test a number of hypotheses for the origin...
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Camilla Forza9/1/26, 2:00 PM
The T2K experiment has recently completed the upgrade of its off-axis near detector, ND280. Two new gaseous High-Angle Time Projection Chambers (HA-TPCs) have been installed above and below the highly segmented scintillator active target, the Super-Fine Grained Detector (SFGD), to precisely track particles emitted at large angles with respect to the beam direction. The two new gaseous...
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ZHENG YANG HE9/1/26, 2:00 PMOral contribution
The High Intensity heavy-ion Accelerator Facility (HIAF), scheduled to commence operations in 2026, could deliver muons with energies reaching the GeV scale, offering unique advantages for both applied and fundamental research. In the realm of muon imaging, GeV-energy muons provide significantly higher penetration depth. This enables high-resolution muon tomography of large-scale components...
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Ruihu Zhu (Institute of Modern Physics, Chinese Academy of Sciences)9/1/26, 2:25 PM
The large acceptance and high magnetic rigidity of the High Energy Fragment Separator (HFRS) at HIAF provide a promising opportunity to develop a tunable GeV-scale muon beam using a heavy-ion-driven production target. We present a stage-by-stage optimization of the existing HFRS optics using G4beamline simulations and a differential evolution algorithm. The objective function accounts for...
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Giovanni Ferrante (INFN, Section of Milano Bicocca)9/1/26, 2:25 PM
The Taishan Antineutrino Observatory (JUNO-TAO) is a satellite detector of the Jiangmen Underground Neutrino Observatory (JUNO), located 44 m from the 4.6 GW$_{\mathrm{th}}$ core of Unit 1 of the Taishan Nuclear Power Plant. Its primary goal is a precision measurement of the reactor electron-antineutrino ($\bar{\nu}_e$) spectrum with unprecedented energy resolution, providing a...
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Alka Singh (Aligarh Muslim University, Aligarh, Uttar Pradesh - 202002, India)9/1/26, 2:25 PM
In the neutrino/antineutrino energy region of 1-3 GeV, inelastic processes contribute significantly
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to neutrino interaction event rates at the DUNE experiment.
These processes are mainly dominated by single-pion production, with some contribution from
eta production, kaon production, associated particle production, multi-pion production, etc. Generally, single-pion production is understood... -
Nikita Mashin (LPI RAS)9/1/26, 2:25 PMWG1: Neutrino Oscillation PhysicsOral contribution
The DANSS reactor antineutrino spectrometer is located in close proximity to the power reactor at the Kalinin NPP (Russia). A lifting platform allows the detector position to be changed in the range of 11–13 m from the reactor core. More than 10M neutrino events and the long-term experiment operation, covering 5 complete fuel campaigns, provide DANSS with rich experimental data, which is used...
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Kou Oishi (High Energy Accelerator Research Organization (KEK))9/1/26, 2:50 PM
The COMET experiment at J-PARC searches for the charged-lepton-flavour-violating process of coherent muon-to-electron conversion in a muonic atom, $\mu^- N \to e^- N$, with a target single-event sensitivity of $O(10^{-17})$. Its beamline is designed to transport low-energy negative muons produced by a high-intensity proton beam with high efficiency and to maximise the number of stopped muons...
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Seisho Abe (University of Tokyo)9/1/26, 2:50 PM
Neutrino oscillation experiments, such as the Tokai-to-Kamioka (T2K) and Hyper-Kamiokande (HK) experiments, are increasingly limited by uncertainties in neutrino-nucleus interaction modelling. For HK, this issue will become increasingly prominent as the greatly increased statistics will result in systematic uncertainties being a dominant limitation on the experiment’s physics scope, with...
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Shailesh Pincha (Indian Institute of Technology Guwahati)9/1/26, 2:50 PM
DUNE is a future long-baseline neutrino oscillation experiment hosted by Fermilab, USA. It aims to measure neutrino oscillation properties with high precision, supernova and solar neutrinos, and possible signatures of nucleon decay. To measure neutrino oscillation parameters, it uses a beam produced at Fermilab and detects the oscillated neutrinos in a 70 kton Liquid Argon TPC volume (divided...
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Joao Paulo Pinheiro (TDLI)9/1/26, 2:50 PMWG1: Neutrino Oscillation PhysicsOral contribution
Neutrino oscillation experiments probe matter effects induced by non-standard interactions (NSI), but the sensitivity is confined to specific combinations of the underlying operators — leaving orthogonal directions in parameter space completely unconstrained. We show that neutral-current (NC) event rates at long-baseline experiments offer a direct handle on these blind directions, since the...
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63. Analysis of Muon Neutrino Interactions in the Upgraded Near Detector ND280 of the T2K ExperimentDaria Fedorova (INR RAS)9/1/26, 3:15 PM
The Tokai-to-Kamioka (Т2K) experiment is a long-baseline neutrino oscillation experiment designed to precisely measure oscillation parameters and search for CP violation in lepton sector using an intense muon (anti)neutrino beam. The experimental setup consists of the J-PARC proton accelerator complex, the near detector ND280, and the far Super-Kamiokande water Cherenkov detector. Data from...
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孙光豹 (Guangbao Sun) (Wuhan University)9/1/26, 3:15 PMWG5: Neutrinos Beyond PMNSOral contribution
The current experimental framework does not entirely exclude the possibility of weak-strength non-standard interactions (NSIs) between neutrinos and leptons. These interactions are classified into two types: Neutral Current (NC) and Charged Current (CC). NC NSIs affect neutrino propagation through matter, while CC NSIs are crucial for the production and detection of neutrinos. The Borexino...
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Mr Jun Kai Ng (Shanghai Jiao Tong University)9/1/26, 3:15 PM
Precision measurements of muon properties and rare decay processes are ideally performed at repetition rates around 50 kHz, yet existing muon facilities are tied to proton accelerators operating in continuous or low repetition rate pulsed modes, making them mismatched to this requirement. We propose an electron driven muon production scheme at the Shanghai High repetition rate XFEL and Extreme...
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Yi Chen (Tsinghua University)9/1/26, 3:15 PM
We introduce radiative corrections in neutral-current (anti)neutrino-nucleon elastic scattering at $\text{GeV}$ energies within the effective field theory framework. We factorize cross sections into soft and hard functions, clarify the (anti)neutrino flavor dependence at both amplitude and cross-section levels, and improve the quantum chromodynamics (QCD) contributions to low-energy...
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Umut Kose (ETH Zurich)9/1/26, 4:10 PM
Plastic scintillator detectors with 3D granularity and sub-nanosecond time resolution provide simultaneous particle tracking, identification, and calorimetry. The 3DET R&D collaboration has developed a novel additive manufacturing technique that enables the monolithic fabrication of finely segmented 3D scintillators, consisting of a matrix of optically isolated scintillating voxels with...
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Joao Paulo Pinheiro (TDLI)9/1/26, 4:10 PMWG1: Neutrino Oscillation PhysicsOral contribution
Measuring the leptonic CP phase $\delta_{CP}$ and resolving the
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$\theta_{23}$ octant are primary objectives of DUNE and T2HK.
We show that two distinct effects can compromise the reliability of
these measurements. First, the poorly constrained $\nu_e$ and
$\bar{\nu}_e$ cross sections allow energy-dependent distortions that
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周威龙 (Weilong Zhou) (California Institute of Technology)9/1/26, 4:10 PM
Mu2e will search for coherent, neutrinoless muon-to-electron conversion in aluminum, $\mu^- + {}^{27}\mathrm{Al}\to e^- + {}^{27}\mathrm{Al}$, a charged-lepton-flavor-violating process whose observation would be unambiguous evidence for physics beyond the Standard Model. The signal is a monoenergetic electron near $104.97\ \mathrm{MeV}$, close to the endpoint of the muon decay-in-orbit...
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Mr Massimiliano Ferro-Luzzi9/1/26, 4:10 PM
The SHiP/NA67 experiment is a general-purpose intensity-frontier experiment for the search for feebly interacting GeV-scale particles and to perform neutrino physics measurements at the HI-ECN3 (high-intensity) beam facility at the CERN SPS, operated in beam-dump mode, taking full advantage of the available $4\times 10^{19}$ protons per year at 400 GeV. The collaboration is currently...
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Yuki Fujii (Shiga University)9/1/26, 4:35 PM
The COMET experiment searches for neutrinoless conversion of a muon to an electron at J-PARC, JAPAN. The experiment aims to start the first commissioning of the full-set of its muon beamline together with a set of Phase-I detectors to demonstrate the experimental capability. We recently completed the construction of full magnets, and the preparations of detectors are ongoing. In this talk, we...
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Emilio Ciuffoli (IMP, CAS)9/1/26, 4:35 PMWG1: Neutrino Oscillation PhysicsOral contribution
Several experiments in the next few years will determine the value of the CP-violating phase $\delta$. In accelerator neutrino experiments, such a measurement is usually performed by comparing the oscillation probabilities in the neutrino and antineutrino sectors to break degeneracies with other oscillation parameters. Such an approach has some downsides, however: for instance, the cross...
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Xingyu Zhao (ETH Zurich)9/1/26, 4:35 PM
One of the major physics goals of the FASER experiment at CERN LHC is to study the highest-energy human-made neutrinos. These neutrinos enable investigations of neutrino interactions at the TeV energy scale as well as rare processes such as charm production. In the upcoming LHC Run 4, the increased luminosity will lead to significantly higher collision rates, providing substantially larger...
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Prof. 罗潇 (Xiao Luo) (University of California Santa Barbara)9/1/26, 4:35 PM
Searches for beyond the Standard Model (BSM) massive long-lived particles decaying to muon pairs face severe irreducible backgrounds in Liquid Argon Time Projection Chambers (LArTPCs). Standard neutrino interactions regularly produce a muon and a pion in the final state, which are currently indistinguishable in LArTPC data. We address this ambiguity using a novel machine-learning method based...
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Sasha Tomalak (Institute of Theoretical Physics, Chinese Academy of Sciences)9/1/26, 5:00 PMWG2: Neutrino Scattering PhysicsOral contribution
We compute electromagnetic radiative corrections in the inverse beta decay at reactor antineutrino energies within the heavy baryon chiral perturbation theory, provide the most accurate cross-section predictions for this process, present a complete error budget, and investigate impact on the energy reconstruction at JUNO. For the first time, we consistently include quantum electrodynamics,...
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Andre Steklain (Universidade Tecnologica Federal do Parana)9/1/26, 5:00 PM
The Deep Underground Neutrino Experiment (DUNE) is a next-generation neutrino oscillation experiment that will provide new constraints for Beyond Standard Model (BSM) phenomena. Lorentz invariance is one of the fundamental principles of quantum field theory and is closely related to symmetries such as charge, parity, and time (CPT) reversal, which form the foundation of the Standard Model (SM)...
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Afiq Azraei Bin Rishinsa (Heidelberg University (DE))9/1/26, 5:00 PM
The Mu3e Experiment at the Paul Scherrer Institut (PSI) aims to probe for charged lepton flavour violation in the µ⁺ → e⁺e⁻e⁺ decay channel. The Phase-I goal of the experiment will utilise an intense DC muon beam of up to 10⁸ µ⁺/s with a goal of pushing the single-event sensitivity down to 2 × 10⁻¹⁵ on the branching ratio. Achieving this goal necessitates a complex system consisting of an...
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Andrew Cheek (TDLI, SJTU)9/1/26, 5:00 PM
In this talk I will discuss the dark matter science case for the future TRIDENT neutrino telescope. We have recently performed a sensitivity study for galactic dark matter annihilations and found that TRIDENT will be able to reach the thermal relic target for dark matter for masses between 1-100 TeV. We contextualized this result in the wider search for dark matter by studying a specific dark...
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鲁桂昊 (Guihao Lu) (SUN YAT-SEN UNIVERSITY)9/1/26, 5:25 PM
The Muonium-to-Antimuonium Conversion Experiment (MACE) is being developed as a high-intensity muon experiment to search for charged-lepton-flavor violation and physics beyond the Standard Model. MACE Phase-I serves as a forerunner of the full experiment, combining a high-intensity polarized muon beam with a nearly $4\pi$ electromagnetic calorimeter, a SciFi tracking detector, and a tiled...
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Riccardo Triozzi (INFN Padova & Università di Padova)9/1/26, 5:25 PMWG2: Neutrino Scattering PhysicsOral contribution
After successful operation at LNGS and a major upgrade at CERN, the 760-ton ICARUS T600 detector has been running at Fermilab since 2020, collecting neutrino interactions from the BNB and NuMI beams.
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In late 2025, ICARUS reached five years of continuous data taking, demonstrating the maturity of large-scale LAr-TPC technology and its relevance for future experiments such as DUNE.
First... -
Prof. Nakadaira Takeshi (KEK)9/2/26, 9:00 AM
Accelerator-based Neutrino Physics Program
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Prof. Angela Papa (PSI/Pisa)9/2/26, 9:30 AM
NCCR Muoniverse Program
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Prof. Lukáš Gráf (Charles University)9/2/26, 10:00 AM
Neutrino mass and Neutrinoless Double Beta Decay
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Yaoguang Wang (Shandong University)9/2/26, 11:00 AM
Jiangmen Underground Neutrino Observatory (JUNO), the largest liquid scintillator detector ever built, started its physics data-taking in Aug. 2025, aiming to address key questions in neutrino physics such as neutrino mass ordering and precision measurement of neutrino oscillation parameters. JUNO consists of a liquid scintillator central detector, an outer water Cherenkov detector, and an...
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Dr Piotr Podlaski (CERN)9/2/26, 11:30 AM
J-PARC upgrades for Hyper-K
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Prof. Shao-Feng Ge (TDLI-SJTU)9/3/26, 9:00 AM
The neutrino oscillation involves two charged-current interaction vertices for the neutrino production and detection processes, each with a PMNS matrix element. Assuming these two PMNS mixing matrices to be the same, which is the usual case in the SM at the tree level, the oscillation probability is unitary. However, these two PMNS matrices can be different in the presence of RG running due to...
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袁意 (Yi Yuan) (中山大学)9/3/26, 9:30 AM
As second-generation leptons, muons play an important role in both fundamental research and a wide range of technological applications. The Platform for Muon Science and Technology at Sun Yat-sen University focuses on muon-related research and educational programs aimed at training future experts in the field. In this talk, we will introduce the current status of the platform, including its...
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Prof. Huma Haider (Aligarh Muslim University)9/3/26, 10:00 AM
The present status of the field theoretical model studies of the deep inelastic scattering induced by neutrino on the nuclear targets in a wide range of Bjorken variable $x$ and four momentum transfer square $Q^2$ will be presented. The perturbative and non-perturbative effects as QCD corrections, target mass corrections and dynamical higher twist effects have been taken into account at the...
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Yury Gornushkin (JINR)9/3/26, 11:00 AM
The FASER is a compact experiment at the LHC, located 480 m downstream of the ATLAS interaction point along the LHC beamline. It aims to study light, weakly interacting particles produced in the proton collisions at the LHC in the forward region, including exotic particles such as dark photons predicted by some Beyond-the Standard-Model (BSM) models, as well as high energy neutrinos. By...
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Prof. Leon Halić (Ruđer Bošković Institute)9/3/26, 11:30 AM
ESSnuSB Status
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Thomas Leplumey9/3/26, 1:15 PM
The T2K (Tokai to Kamioka) experiment is a long-baseline neutrino oscillation experiment that studies accelerator-produced muon neutrinos and antineutrinos oscillations over a 295 km baseline from J-PARC to the Super-Kamiokande detector in Japan. Its primary goals are the precise measurement of the PMNS mixing angles $\theta_{23}$ and $\theta_{13}$, the mass-squared splitting $\Delta...
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Karishma Dhanmeher (Institute of Physics of the 2 Infinities of Lyon, France)9/3/26, 1:15 PM
The Deep Underground Neutrino Experiment (DUNE) is a global flagship project designed to resolve open questions in neutrino physics, including charge-parity (CP) violation in the leptonic sector, the neutrino mass ordering, and low-energy astrophysical phenomena such as supernova neutrino bursts. To achieve the large fiducial mass and sub-centimeter spatial resolution for these rare events,...
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Yutaro Sato (Niigata Univ.)9/3/26, 1:15 PM
The muon anomalous magnetic moment, $(g-2)_{\mu}$, and the electric dipole moment (EDM) are sensitive probes of physics beyond the Standard Model (SM). Recent measurements of $(g-2)_{\mu}$ show a tension with the SM prediction based on electron-positron collision data, while calculations based on lattice QCD are in better agreement with the experimental value. Clarifying this discrepancy is...
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Pilar Casado9/3/26, 1:15 PM
T2K is a long-baseline experiment for the measurement of neutrino oscillations. The neutrino flux and neutrino-nucleus cross-sections are measured by a suite of near detectors, including ND280, an off-axis multipurpose magnetised detector, WAGASCI, featuring a water-enriched target at a different off-axis angle, and INGRID an on-axis detector composed of sandwiched layers of iron and...
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Valeria Trabattoni (Università degli Studi di Milano e INFN Milano)9/3/26, 1:40 PM
In modern physics, the nature of neutrinos remains one of the major open questions, motivating new experimental efforts to investigate their properties. The Deep Underground Neutrino Experiment (DUNE) is a next-generation international experiment designed to determine the neutrino mass ordering, study CP violation in the neutrino sector, detect neutrinos from astrophysical sources, and search...
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Bruno Zamorano (University of Granada)9/3/26, 1:40 PM
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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Alejandro Nicolas Gacino Olmedo9/3/26, 1:40 PM
T2K is a long-baseline experiment based in Japan and focused on oscillations of neutrinos and antineutrinos. (Anti-)neutrinos from J-PARC are first characterised in the Near Detector (mainly ND280) and, after travelling 295 km, measured in the Far Detector, Super-Kamiokande, in order to extract neutrino oscillation parameters, including the CP-violating phase, within the standard PMNS...
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吕濛 (Meng Lyu) (University of Tokyo)9/3/26, 1:40 PM
The ultra-slow muon (USM), developed for the J-PARC muon g-2/EDM experiment, is produced by laser ionization of thermal muonium using 122 nm and 355 nm laser pulses, a process known as muon cooling. Since late 2025, two beam tests have been conducted using the new high-intensity surface muon beamline dedicated to the J-PARC muon g-2/EDM experiment. During these beam tests, extensive studies of...
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Mr 黄幸运 (Xingyun Huang) (SJTU)9/3/26, 2:05 PM
The muEDM experiment at the Paul Scherrer Institute (PSI) aims to measure the muon electric dipole moment (EDM) with unprecedented sensitivity, targeting a precision of σ($d_\mu$) = 6 × 10⁻²³ e·cm, which represents an improvement by three orders of magnitude over the current limit established by the muon g−2 experiment at Brookhaven National Laboratory (BNL). Central to this effort is the muon...
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Anna Balboni (University & INFN of Ferrara)9/3/26, 2:05 PM
The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline experiment for neutrino physics currently under construction in the US, aiming to measure neutrino oscillation parameters, search for beyond standard model physics, and detect supernova neutrinos. DUNE will include a Near Detector and a Far Detector (FD), located 1300 km away from the ND and 1.5 km underground....
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Hemant Prasad (University of Wroclaw)9/3/26, 2:05 PM
NuWro is a state-of-the-art Monte Carlo generator developed at the University of Wroclaw for simulating neutrino-nucleus interactions. I will present our recent work on fine-tuning of final-state interactions within NuWro. In this, I will present the use of the event reweighting tool to efficiently reweight and adjust the strength of FSI effects in the NuWro Monte Carlo event generator. This...
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Ralte Lalnuntluanga (Tel Aviv University)9/3/26, 2:05 PM
Making high precision measurements of neutrino oscillation parameters requires an unprecedented understanding of neutrino–nucleus scattering. MicroBooNE is able to perform high resolution imaging of numerous final state topologies resulting from neutrino interactions. This talk will give an overview of MicroBooNE's most recent neutrino cross section results. These include our latest...
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张策 (Ce Zhang) (University of Liverpool)9/3/26, 2:30 PM
We propose a next-generation precision measurement of the muon anomalous magnetic moment (muon g−2), at the High Intensity Heavy-Ion Accelerator Facility (HIAF) in China. The project, named CANTON-μ (Coherent Anomalous magNetic momenT ObservatioN with muon), represents the first muon g−2 experiment aimed at surpassing Fermilab precision. It introduces novel approaches based on HIAF's intense...
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Rwik Dharmapal Banerjee (University of Wrocław doctoral student)9/3/26, 2:30 PM
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 describe the argon spectral function framework in NuWro Monte Carlo event generator, with a detailed description of how nuclear information is translated...
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Akari Oka (Keio Univertsity)9/3/26, 3:25 PM
In the Hyper-Kamiokande experiment, controlling systematic uncertainties is essential to achieve the projected precision of long-baseline neutrino oscillation measurements. To constrain uncertainties associated with neutrino interaction cross sections, the Intermediate Water Cherenkov Detector (IWCD) is being developed as a movable water Cherenkov detector located 870 m from J-PARC along the...
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Pierre Granger (CERN)9/3/26, 3:25 PM
The Deep Underground Neutrino Experiment (DUNE) is a pioneering long-baseline neutrino experiment 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 neutrinos, spanning a wide...
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李文哲 (Wenzhe Li)9/3/26, 3:25 PMWG4: Muon PhysicsOral contribution
The Belle and Belle II experiments have collected a $1.6~\mathrm{ab}^{-1}$ sample of $e^+e^-$ collision data at center-of-mass energies near the $\Upsilon(nS)$ resonances. We present searches for the decays $\tau \to \mu\gamma$, $\tau \to \ell\eta$, $\tau\to \ell\pi^0$, and $\tau^-\to \ell^-\alpha$, where $\ell = e$ or $\mu$ and $\alpha$ is an invisible scalar particle. In addition, we...
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Alexey Konovalov (LPI RAS)9/3/26, 3:25 PM
The vGeN ("nu-GeN") setup is collecting data at Kalinin NPP, 11.1 m from the center of a 3.1 GW reactor core, since late 2019. The aim of the experiment is to measure coherent elastic antineutrino-nucleus scattering (CEvNS) as well as to search for antineutrino electromagnetic properties with a 1.4 kg germanium point-contact detector. The talk presents updated results of the experiment on...
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赖浩菁 （Haojing Lai) (Shanghai Jiao Tong University)9/3/26, 3:50 PM
In the Jiangmen Underground Neutrino Observatory (JUNO), cosmogenic muon-induced radioactive isotopes, particularly ⁹Li/⁸He, which undergo β-n decays, produce correlated signals that closely mimic the inverse beta decay (IBD) signature. This constitutes one of the major backgrounds for reactor antineutrino oscillation analyses, with an initial rate of ~60/day before applying any muon veto....
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宋天资 (Tianzi Song) (Sun Yat-sen University)9/3/26, 3:50 PM
Coherent elastic neutrino-nucleus scattering (CEvNS) benefits from the coherent interaction of neutrinos with an entire nucleus at low momentum transfer, resulting in an enhanced cross section that provides a sensitive approach for detecting low-energy neutrinos. The CICENNS (CsI Detector for Coherent Elastic Neutrino-Nucleus Scattering) experiment aims to perform a high-precision measurement...
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Yiwen Yang (University of Oxford)9/3/26, 3:50 PM
Next generation neutrino oscillation experiments, such as JUNO, DUNE, and
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Hyper-Kamiokande, are positioned to collect unprecedented statistics in neutrino
data, enabling high-precision measurements of oscillation parameters. A major
fraction of the data will consist of atmospheric neutrinos, which allows for
independently extracting oscillation parameters and placing constraints... -
Bo Liu (Nankai University)9/3/26, 3:50 PMWG4: Muon PhysicsOral contribution
The Standard Model predicts several rare decay processes of the Higgs boson, including decay to a Z boson and a photon (H->Zgam), decay to a pair of muons (H->mumu), and decay to a pair of electrons (H->ee). The lepton-flavor-violating (LFV) decay of the Higgs boson, on the other hand, is forbidden in the Standard Model but allowed in new physics models. Search for rare and LFV decays of the...
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Aman Gupta (Institute of High Energy Physics (IHEP), Beijing)9/3/26, 4:15 PM
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kiloton liquid scintillator detector with excellent sensitivity to detect neutrinos from the next Core-Collapse Supernova (CCSN). The real-time CCSN monitoring system of JUNO is designed to provide fast and reliable alerts by tracking the increasing event rate of supernova burst neutrinos and pre-supernova neutrinos.
The...
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Luis A. Delgadillo (IHEP)9/3/26, 4:15 PM
Upcoming and present reactor neutrino experiments offer a compelling avenue to probe fundamental neutrino properties beyond flavor oscillations. In this talk, I will discuss the physics potential of a short-baseline reactor experiment, inspired by the JUNO-TAO configuration, to investigate neutrino electromagnetic interactions via electron--neutrino elastic scattering (E$\nu$ES). I will...
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张荣凭 (Rongping Zhang) (IHEP)9/3/26, 4:15 PM
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kton multipurpose liquid scintillator detector located at a depth of 650 meters in South China. Although its primary mission is the determination of the neutrino mass ordering, JUNO’s unprecedented target mass and excellent energy resolution offer a unique opportunity to study geoneutrinos with high statistics.
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Geoneutrinos,... -
Mr 高乐耘 (Leyun Gao) (Peking University)9/3/26, 4:15 PMWG4: Muon PhysicsOral contribution
The MUonE experiment, currently under preparation at CERN, aims to measure the running of the electromagnetic coupling $\alpha$ in the elastic $\mu e$ scattering process, from which the dominant hadronic contribution to the anomalous magnetic moment of the muon can be extracted. We present performance results from the Phase 1 MUonE test-beam campaign carried out in summer 2025 at the CERN SPS...
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IZYAN HAZWANI BINTI HASHIM (Universiti Teknologi Malaysia)9/3/26, 4:40 PMWG4: Muon PhysicsOral contribution
Ordinary Muon Capture (OMC) provides a unique experimental avenue to probe the β+ type nuclear responses essential for understanding double beta decays (DBDs) and astrophysical neutrino interactions. This study leverages high energy-resolution gamma-ray spectroscopy to meticulously identify transition channels in enriched and natural molybdenum. By utilizing high-purity germanium (HPGe)...
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Bingrong Yu (Cornell University)9/3/26, 4:40 PM
Atomic parity violation (APV) provides a unique determination of the weak mixing angle ($\sin^2\theta_W$) at low energies and therefore serves as a powerful precision test of the Standard Model. We show that previous APV calculations omitted a class of one-loop contributions arising from two-neutrino exchange, commonly referred to as "the neutrino force". We compute this contribution to APV...
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Neetu Raj Singh Chundawat (Institute of High Energy Physics, Beijing)9/3/26, 4:40 PM
Quantum estimation theory provides a powerful framework to quantify the ultimate precision with which neutrino oscillation parameters can be inferred. In this work, we use the Quantum Fisher Information (QFI) to study the information content associated with the leptonic CP phase $\delta_{\rm CP}$ in long-baseline experiments and the solar parameters $\Delta m^2_{21}$ and $\theta_{12}$ in...
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Dr Francesco Terranova (CERN)9/4/26, 9:00 AM
The last two decades have witnessed remarkable progress in the measurement of neutrino cross sections relevant to oscillation experiments. At the same time, this growing body of data has exposed significant limitations in our theoretical understanding of neutrino-nucleus interactions and has stimulated the development of new experimental approaches. This effort is particularly timely, as the...
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Pierre Granger (CERN)9/4/26, 9:30 AM
The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino experiment designed to study neutrino oscillations with a high-intensity neutrino beam produced at the Long-Baseline Neutrino Facility (LBNF). The experiment will employ a high-precision near detector complex at Fermilab together with four large liquid argon time projection chambers located 1,300 km...
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Ms Liu Yichun (IHEP)9/4/26, 10:00 AM
Outreach actitivies at IHEP
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Jian Tang (Sun Yat-sen University)9/4/26, 11:00 AM
Advances in accelerator technology have led to significant
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improvements in the quality of muon beams over the past decades.
Investigations of the muon and muonium enable precise measurements of
fundamental constants, as well as searches for new physics beyond the
Standard Model. The spontaneous conversion of muonium to antimuonium is
an interesting charged lepton flavor violation... -
Dr Tianqi Huang (TDLI)9/4/26, 11:30 AM
TRIDENT Status Updates
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Prof. Eric Prebys (University of California, Davis)9/4/26, 12:00 PM
The Fermilab accelerator complex has been operating for over half a century. For many years, the centerpiece of the lab's program was the Tevatron proton-antiproton collider, but beginning in the late 1990, the lab began to develop a high intensity program, aimed at neutrino and rare process physics. With the shutdown of the Tevatron in 2011, this became the primary focus of the lab. This talk...
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9/4/26, 1:00 PM
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Erwan Le Blévec (Laboratoire Leprince-Ringuet)9/4/26, 2:00 PM
NuFact 2026,
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Tsung-Dao Lee Institute,
No.1 Lisuo Road, Pudong New District, Shanghai 201210, China
August 31, 2026 to September 5, 2026
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The Hyper-Kamiokande detector represents the next generation of neutrino observatories, following in the lineage of the Kamiokande and... -
Umut Kose (ETH Zurich)9/4/26, 2:00 PM
The FASER experiment is located 480 m downstream of the ATLAS interaction point at the Large Hadron Collider (LHC), aligned with the beam collision axis. Shielded by approximately 100 meters of rock and concrete, FASER operates in an exceptionally low-background environment that enables unique studies of forward physics. TThe experiment's goals include two complementary physics programs:...
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Feng FANG (Advanced Energy Science and Technology Guangdong Laboratory)9/4/26, 2:00 PM
High-intensity muon beams could enable a muonium-based search for axions through resonant quantum transitions between hyperfine states. Combining theoretical calculations with simulation results, we demonstrate that such a muonium-based experimental approach could complement and tighten constraints on the axion-muon coupling beyond existing limits from the muon g−2 measurement, over the axion...
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Wissal Filali (University of Bonn)9/4/26, 2:25 PMWG2: Neutrino Scattering Physics
The Forward Search Experiment (FASER) at the CERN Large Hadron Collider (LHC) provides access to TeV-scale neutrinos produced in the far-forward region of proton-proton collisions. Using the electronic detector components of FASER and an integrated luminosity of $186 \pm 4~\mathrm{fb}^{-1}$ collected during LHC Run 3 at $\sqrt{s}=13.6~\mathrm{TeV}$, charged-current muon neutrino interactions...
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Arsenii Gavrikov (TDLI, SJTU)9/4/26, 2:25 PMWG1: Neutrino Oscillation PhysicsOral contribution
The Jiangmen Underground Neutrino Observatory (JUNO) is a neutrino experiment located in China with a broad physics program. Following nearly a decade of construction, JUNO began physics data-taking on August 26, 2025. The primary goals of the experiment are the determination of the neutrino mass ordering and the high-precision measurement of neutrino oscillation parameters. JUNO's central...
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Qite Li (Peking University)9/4/26, 2:25 PM
We propose here a set of new proposals and some preliminary experimental results involving probing and knocking with muons (PKMu). There is a wealth of rich physics to explore with GeV muon beams either from dedicated beam or cosmic source. Examples include but not limited to: muon scattering can occur at large angles, providing evidence of potential muon-philic dark matter or dark mediator...
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Nayana Bangaru9/4/26, 2:50 PMWG2: Neutrino Scattering Physics
The SND@LHC detector is a compact, stand-alone experiment designed to measure neutrinos produced at the LHC in a previously unexplored region of pseudorapidity, specifically between 7.2 and 8.6. This region complements those covered by other LHC experiments. The detector is situated 480 meters downstream from IP1 in the unused TI18 tunnel. It is composed of a hybrid system based on an 800 kg...
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Petr Lenskii (Joint Institute for Nuclear Research)9/4/26, 2:50 PMWG1: Neutrino Oscillation PhysicsOral contribution
Jiangmen Underground Neutrino Observatory (JUNO) is a kiloton-scale liquid scintillator detector located in southern China. Its main goals are determination of the neutrino mass ordering (NMO) and high-precision measurement of neutrino oscillation parameters by means of reactor antineutrinos. JUNO started physics data taking in the end of August 2025 and released the world-leading measurement...
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Yu Bao (IHEP)9/4/26, 2:50 PM
Muon station for sciEnce technoLOgy and inDustrY (MELODY) is the first muon source project in China. It aims at both fundamental muon physics and muon applications in various fields. In phase I we will construct a surface muon beam with one muSR spectrometer and one test beam port for technology development and possible muon physics experiment. We also reserve the tunnel for a decay muon...
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陈翔 (Xiang Chen)9/4/26, 3:15 PMOral contribution
We propose DREAMuS (Dark matter REsearch with Advanced Muon Source), a fixed-target experiment at the High-Intensity Heavy-Ion Accelerator Facility (HIAF) in China, designed to search for muon-philic dark-sector particles. DREAMuS uses a GeV-scale muon beam to probe light mediators that preferentially couple to muons and induce lepton-flavor-violating muon-nucleus interactions, followed by...
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Mahesh Jakkapu (Ruđer Bošković Institute, Zagreb, Croatia)9/4/26, 3:15 PM
The NINJA experiment in the T2K beam employs nuclear emulsion detectors to study neutrino interactions. A key advantage of nuclear emulsion technology is its extremely high spatial granularity allowing for sub-micron spatial resolution. This feature enables the reconstruction of short particle tracks originating in the vicinity of the neutrino interaction vertex, allowing for detailed...
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Pablo Barham Alzás (Tel Aviv University)9/4/26, 4:10 PMWG2: Neutrino Scattering PhysicsOral contribution
The extraction of oscillation parameters from next-generation neutrino experiments such as DUNE and Hyper-K will rely on precise estimation of the properties of the incoming neutrino. The relationship between reconstructed and true neutrino energies depends critically on accurate models of neutrino-nucleus interactions, for which uncertainties in nuclear structure and reaction mechanisms are...
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Jean-Baptiste Plancon9/4/26, 4:10 PM
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. The ND280 near detector at J-PARC plays a crucial role to minimize the systematic uncertainties related to the neutrino flux and neutrino-nucleus interactions of the un-oscillated neutrino beam. Part of ND280 has...
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徐宇 (Yu Xu) (先进能源科学与技术广东省实验室)9/4/26, 4:35 PMWG2: Neutrino Scattering PhysicsOral contribution
As next-generation long-baseline experiments DUNE and Hyper-Kamiokande enter a systematics-dominated era, neutrino-nucleus cross-section uncertainties—particularly for antineutrinos in the 0.3–2.5 GeV range—have become the leading limitation on $\delta_{CP}$ extraction. We present a novel narrow-band neutrino beam produced by instrumenting the High Energy Fragment Separator (HFRS) at China's...
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Aman Gupta (Institute of High Energy Physics (IHEP), Beijing)9/4/26, 4:35 PMWG1: Neutrino Oscillation PhysicsOral contribution
We study the impact of combining the present NO$\nu$A and T2K data with simulated data from the JUNO experiment on the determination of the leptonic CP phase and the neutrino mass hierarchy. The current NO$\nu$A data exhibit a hierarchy--$\delta_{\mathrm{CP}}$ degeneracy, admitting both normal hierarchy (NH) with $\delta_{\mathrm{CP}} \in [0,180^\circ]$, and inverted hierarchy (IH) with...
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Dr Ioannis Christodoulou (European Spallation Source)9/4/26, 5:00 PM
The ESSnuSB project aims at searching the matter anti-matter asymmetry at 5 σ significance level, in more than 70% of the lepton Dirac δCP violating phase range, and measuring the phase value with precision. Its first phase, the ESSnuSB, investigated the upgrade of the European Spallation Source to deliver the intense neutrino beam toward a far detector hosted within the Zinkgruvan mine,...
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Leon Halić (Ruđer Bošković Institute)9/4/26, 5:00 PMWG2: Neutrino Scattering PhysicsOral contribution
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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Nikolaos Vassilopoulos (IHEP/CSNS)9/4/26, 5:25 PM
Description of the future plans for accelerator neutrino production at the China Spallation Neutron Source.
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Sota Kobayashi (Tohoku University)9/4/26, 5:25 PM
The key to unraveling the mystery of the matter-dominated universe is believed to lie in CP violation in the lepton sector. The T2K experiment is a long-baseline neutrino oscillation experiment in which neutrinos produced by the J-PARC proton accelerator are detected at Super-Kamiokande, located 295 km away.
MUMON is a detector located about 100 meters downstream of the neutrino production...
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Junting Huang (Shanghai Jiao Tong University)9/5/26, 9:00 AM
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Seisho Abe (University of Tokyo)9/5/26, 9:30 AM
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Eric Prebys (University of California, Davis)9/5/26, 10:00 AM
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Prof. Kim Siang Khaw (TDLI/SJTU)9/5/26, 10:50 AM
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Andrew Cheek (TDLI, SJTU)9/5/26, 11:20 AM
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Tanaz Mohayai (Indiana University)9/5/26, 11:40 AM
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Poonam Mehta (Jawaharlal Nehru University)9/5/26, 12:10 PM
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