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Runze Zhao (IHEP, CAS)Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is the world’s largest liquid scintillator experiment that detects neutrinos mainly via inverse beta decay (IBD) with protons. It is designed to determine the mass hierarchy of neutrinos using 20 kton of liquid scintillator (LS) located 52.5 km away from two nuclear power plants. It took approximately 6 months to fill LS from February 2025,...
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Julia Ryshkewitch (Boston University)New Technologies for Neutrino PhysicsPoster
The Eos detector is a ton-scale testbed for next-generation neutrino experiments, evaluating novel liquid scintillator technologies including water-based liquid scintillator (WbLS). A key requirement for WbLS development is the ability to separate Cherenkov and scintillation light, motivating controlled calibration studies with well-defined electron sources. To support these studies, we have...
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Justin MuellerNeutrino OscillationsPoster
We present the status of a joint search for muon neutrino disappearance in the Booster Neutrino Beam at Fermilab using the Short-Baseline Neutrino (SBN) Program's two-detector configuration, SBND and ICARUS. Charged-current interactions consistent with muon neutrinos and containing only a muon and at least one proton in the final state are reconstructed and selected using the SPINE deep...
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Sam Hedges (Virginia Tech)New Technologies for Neutrino PhysicsPoster
Coherent elastic neutrino-nucleus scattering (CEvNS) can induce defects in crystal lattices that persist over long time scales. In certain materials, electrons can become trapped in these defects, turning them optically active (i.e. color centers). This enables neutrino-induced nuclear recoils to be imaged using fluorescence microscopy. We present commissioning data from the Virginia Tech...
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Tanaz Mohayai (Indiana University)New Technologies for Neutrino PhysicsPoster
High-pressure gaseous argon time projection chambers (HPgTPCs) represent an emerging detector paradigm for neutrino physics, combining increased target density with the intrinsic tracking and low thresholds of gaseous detectors. This approach enables detailed reconstruction of exclusive final states, improved particle identification, and sensitivity to low-energy and rare processes —...
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Adam Wong (University of Sussex)New Technologies for Neutrino PhysicsPoster
The AntiMatter-OTech (AM-OTech) project, funded by the European Innovation Council (EIC) and UK Research and Innovation (UKRI), is a pioneering initiative in nuclear security and reactor diagnostics. Led by a collaboration of European academic institutions and EDF, AM-OTech explores the use of antineutrinos from nuclear fission as a non-intrusive, real-time probe for monitoring industrial...
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Max Dornfest (University of Hawaiʻi at Mānoa)Reactor NeutrinosPoster
We present a potential improvement over the standard method developed to determine antineutrino directionality in inverse-beta-decay detectors. The previously developed method in monolithic and segmented detectors underestimated angular uncertainty in the low-count regime. We will cover our latest publication on a new directionality algorithm and our current work in progress.
We have...
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Florian Fraenkle (Karlsruhe Institute of Technology)Neutrino MassPoster
The KArlsruhe TRItium Neutrino (KATRIN) experiment is a large-scale effort with the objective to determine the effective electron anti-neutrino mass with an unprecedented sensitivity of better than 0.3 eV (90% CL) using $\beta$-decay spectroscopy of molecular tritium. The measurement setup consists of a high luminosity windowless gaseous molecular tritium source, a differential and cryogenic...
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Hasung SongNew Technologies for Neutrino PhysicsPoster
The Eos experiment is a 4-tonne monolithic optical detector operating at University of California, Berkeley campus. Eos serves as a testbed for next generation detector technologies for neutrino experiments. Eos has taken data with a suite of calibration sources in multiple target media. The collaboration is now exploring the detector's use case beyond a testbed.
We propose deployment of...
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Larry Zhao (University of California Irvine)Neutrino OscillationsPoster
NOvA (NuMI Off-Axis $\nu_e$ Appearance) is a long baseline neutrino experiment designed to measure the oscillation of muon neutrinos to electron neutrinos over a distance of 810 km. NOvA uses a near and far detector to observe $\nu_\mu$ disappearance and $\nu_e$ appearance of neutrinos produced by the NuMI beam at Fermilab. NOvA uses a Bayesian analysis framework in addition to its Frequentist...
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Cullen Sullivan (Tufts University)Accelerator NeutrinosPoster
Using its 10-year dataset, NOvA makes competitive measurements of neutrino oscillation parameters $\Delta m^2_{32}$, $\theta_{23}$, $\theta_{13}$, and $\delta_{CP}$ using an 810 km baseline ranging from the NuMI beam at Fermilab to the far detector in Minnesota. NOvA uses a method called "extrapolation" to control systematic uncertainties. First, simulation-data discrepancies are measured...
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Zhongyi WuReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kton liquid-scintillator neutrino experiment designed to precisely measure reactor neutrino oscillations and determine the neutrino mass ordering. 20-inch photomultiplier tubes (LPMTs) provide the dominant photon statistics for energy reconstruction, but their charge response can exhibit a time-dependent instrumental non-linearity,...
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子谦 向Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kton liquid scintillator detector designed to achieve a target energy resolution of 3% at 1 MeV through precise control of detector response and reconstruction systematics. Accurate three-dimensional positioning of calibration sources is a key requirement for this goal. JUNO employs an ultrasonic positioning system to determine the...
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Jiaqi HuiReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) central detector is an acrylic spherical vessel filled with 20 kton of liquid scintillator, with an inner diameter of 35.4 m. JUNO is designed to achieve an unprecedented energy resolution of about 3% at 1 MeV and an energy nonlinearity better than 1%, enabling a precise determination of the neutrino mass ordering, high-precision...
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Jianrun Hu (Sun Yat-sen University), Jun Cao (Institute of High Energy Physics, Chinese Academy of Sciences), Yichen Li (Institute of High Energy Physics, Beijing)Reactor NeutrinosPoster
The Taishan Antineutrino Observatory (TAO), a satellite detector of the Jiangmen Underground Neutrino Observatory (JUNO), aims to measure reactor antineutrinos with unprecedented energy resolution. Achieving this precision relies heavily on the performance of its high-coverage, cryogenically operated silicon photomultipliers (SiPMs). To fully exploit their performance, precise channel-level...
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Shao-Hsuan Chiu (Chang Gung University, Taoyuan, Taiwan)Neutrino OscillationsPoster
The rephasing-invariant, squared, elements of the mixing matrix can be derived from the characteristic matrix associated with the mass matrix in a transparent way. This formulation leads to certain invariants and an alternative expression for the squared Jarlskog invariant $J^{2}$. Possible applications to the study of neutrino oscillation in matter and that to the normalization group...
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Srikar Gadamsetty (University of California, Berkeley)New Technologies for Neutrino PhysicsPoster
Eos is a multi-ton-scale demonstrator for future hybrid neutrino detectors that leverages both Cherenkov and scintillation light. Several novel technologies are being explored at this testbed, including Water-based Liquid Scintillator (WbLS). In this presentation, I will discuss the status of external neutron and γ background reconstruction in the Eos detector utilizing a Plutonium Beryllium...
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Hokuto Kobayashi (University of Tokyo (JP))Accelerator NeutrinosPoster
The 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 at a confidence level of 90%. One of the major systematic uncertainties in the current oscillation analysis arises from the uncertainty in neutrino cross-sections. To reduce these uncertainties and perform more...
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Ohana Benevides Rodrigues (Illinois Institute of Technology)Applications and Neutrino Impacts on HumanityPoster
The Reactor Operations Antineutrino Detection Surface Testbed Rover (ROADSTR) prototype detector is a 60-kg reactor-antineutrino detector, comprised of a 2-dimensional array of 36 6Li-doped pulse-shape-sensitive plastic scintillator bars. It collected data recently at multiple locations with diverse environmental characteristics, including the underground P-Tunnel facility at the Nevada...
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Maria Gabriela Manuel Alves (Illinois Institute of Technology)Accelerator NeutrinosPoster
A proper understanding of the capabilities and fidelity of low-energy reconstruction is crucial for taking advantage of MeV-scale neutrino physics opportunities in LArTPCs. This poster will present an analysis resulting in the first-ever demonstration of LArTPC energy resolution in the MeV regime. A measurement of the resolution of energy reconstruction in the MicroBooNE LArTPC at ~1.5 MeV was...
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Dr Tyler Stokes (Yale University (US))New Technologies for Neutrino PhysicsPoster
The Deep Underground Neutrino Experiment (DUNE) is designed to make precision measurements of neutrino oscillations with the primary goals of establishing the mass ordering and searching for Charge-Parity (CP) violation in the lepton sector. The DUNE Far Detectors will employ Liquid Argon Time Projection Chambers (LArTPCs) containing approximately 70 ktons of liquid argon, with 40 ktons...
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Tianzi Song (Sun Yat-Sen University (CN))Accelerator NeutrinosPoster
Coherent Elastic Neutrino-Nucleus Scattering (CEvNS) provides significant enhancement of low-energy neutrino cross section through coherent interaction with an entire nucleus. The CICENNS (CsI Detector for Coherent Elastic Neutrino-Nucleus Scattering) experiment aims to perform a high-precision measurement of CEvNS using neutrinos from the China Spallation Neutron Source (CSNS). A neutrno...
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Isabel Colon Rivera (Duke University)Accelerator NeutrinosPoster
The COHERENT collaboration has measured coherent elastic neutrino-nucleus scattering (CEvNS) on CsI, argon, and most recently germanium. While efforts are underway to obtain precision measurements of CEvNS on NaI and argon with new tonne-scale detectors, the opportunity of measuring CEvNS on other liquid noble targets with the CENNS-10 detector now exists.
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A CEvNS measurement on neon will... -
Jiwon Ryu (Kyoungpook National University)Sterile NeutrinosPoster
The JSNS²-II (J-PARC Sterile Neutrino Search at the J-PARC Spallation Neutron Source) experiment searches for sterile neutrino oscillations using neutrinos from muon decay at rest. At the J-PARC Material and Life Science Experimental Facility (MLF), a 3 GeV proton beam is injected onto a mercury target, producing muon antineutrinos. As the second phase of the JSNS², the experiment employs a...
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Zev Imani (Tufts University)New Technologies for Neutrino PhysicsPoster
Given the challenges in LArTPC event reconstruction, we present the first steps toward a fully automated inference pipeline mapping 2D detector images to event properties. Inspired by the success of denoising diffusion probabilistic models (DDPMs) in natural image generation, we developed a modified latent diffusion model capable of conditionally generating single-particle LArTPC images with...
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Licheng FENG (Kyoto University)Accelerator NeutrinosPoster
Atmospheric Neutral Current Quasi-Elastic (NCQE) interactions are a dominant background for the Super-Kamiokande Diffuse Supernova Neutrino Background (DSNB) search. The large uncertainty in Atmospheric NCQE interactions is a key bottleneck limiting DSNB sensitivity. We use NCQE events from the T2K neutrino beam to constrain this uncertainty and to validate selection cuts. We analyzed the...
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Han ZhangReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kiloton liquid scintillator detector located approximately 650 m underground in southern China. JUNO’s primary goals are to determine the neutrino mass ordering and precisely measure the neutrino oscillation parameters $\Delta m^2_{31}$, $\Delta m^2_{21}$, and $\rm{sin}^2\theta_{12}$. The measurement relies on reactor antineutrinos...
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Koichiro Yasuda (UCLA)Reactor NeutrinosPoster
We present a model-independent reconstruction of the reactor antineutrino spectrum below the inverse beta decay (IBD) threshold (1.8 MeV) using coherent elastic neutrino–nucleus scattering (CEvNS). Our approach adapts halo-independent techniques from direct dark matter detection and recasts the inference problem in terms of convex geometry, enabling the reconstruction of the integrated...
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Xiaoying LuReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kton liquid scintillator detector with the primary goal of determining the neutrino mass ordering. The suppression of cosmogenic backgrounds, such as $^{9}\text{Li}/^{8}\text{He}$, is critical for achieving JUNO's sensitivity. Since these backgrounds are highly correlated with muon trajectories in both space and time, precise muon...
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Cailian Jiang (Nanjing University)Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) has reported its first physics results, highlighting its capability for precision measurements of neutrino oscillation parameters. Achieving this precision requires a robust inverse beta decay (IBD) event selection and stringent control of background contributions. Among cosmogenic isotopes, the $\beta$-$n$ decay of long-lived $^{9}$Li and...
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Ping Zhang (Shanghai Jiao Tong University), marta colomer (ULB (IIHE))1Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) aims to determine the neutrino mass ordering and perform precision measurements of neutrino oscillation parameters. Its central detector consists of a 35.4-m-diameter acrylic sphere holding 20 kton of liquid scintillator, immersed in a 44-m-deep water pool for radioactive shielding and a water Cherenkov muon veto. Cosmogenic neutrons,...
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Enze Zhang (Institute of High Energy Physics, China)Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20 kton liquid
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scintillator detector located 52.5 km from multiple reactor cores in south China to determine the neutrino mass ordering. To achieve this science goal, waveform reconstruction plays an essential role as it directly influences the energy resolution of the PMTs. In this poster, two waveform reconstruction algorithms, COTI... -
Miles Garcia (University of Delaware)Sterile NeutrinosPoster
Sterile neutrinos are a popular solution to neutrino anomalies in the short baseline sector. The IceCube Neutrino Observatory is uniquely positioned to search for the sterile neutrino signal separately from the short baseline experiments by looking for the matter-enhanced resonant oscillation of TeV-energy muon neutrinos travelling through the earth into the sterile state. Previous sterile...
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Dr Rick Mueller (Penn State University)Neutrino MassPoster
The Project 8 collaboration aims to determine the absolute neutrino mass with a sensitivity of 40 meV/c² by performing Cyclotron Radiation Emission Spectroscopy (CRES) on tritium beta-decay electrons. To achieve the necessary statistics, the experiment is transitioning from waveguide-based detectors to large-volume resonant microwave cavities operating at sub-GHz frequencies. This shift...
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Rosmarie Irma Wirth (GSI & JGU), 董灏杰 donghj (IHEP)Reactor NeutrinosPoster
The JUNO experiment, aiming to determine the neutrino mass ordering among other neutrino studies, is a next-generation neutrino experiment located in China. JUNO has constructed a giant underground liquid scintillator detector and started data taking in 2025. The Data Quality Monitoring (DQM) system plays a critical role throughout the data taking, quality control, and physics analysis stages....
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Avik Ghosh (Iowa State University)Accelerator NeutrinosPoster
The Deep Underground Neutrino Experiment (DUNE) is a flagship long-baseline neutrino experiment designed to make precision measurements of neutrino oscillations and to search for physics beyond the Standard Model using massive LArTPC (Liquid Argon Time Projection Chamber) detectors. Accurate electronic-noise simulation is essential for low-energy physics in LArTPCs. More realistic noise...
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Thomas Wester (University of Chicago)Accelerator NeutrinosPoster
In the Short-Baseline Neutrino (SBN) Program’s two-detector oscillation searches, detector-related systematic uncertainties are expected to be the dominant source of uncertainty due to cancellations in flux and cross section uncertainties between the near and far detectors. Traditional approaches for evaluating detector systematics rely on varying a fixed set of known sources of uncertainties...
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Yuxuan Wang (California Institute of Technology)Accelerator NeutrinosPoster
We present a data-driven charge–light matching technique for DUNE ND-LAr, in which an attention-based network trained on single-flash data predicts the light response of topologically clustered charge deposits and assigns each cluster a nanosecond-precision t_0 via likelihood alignment. Performance is demonstrated both in high-pile-up ND-LAr simulation and on real 2×2 Demonstrator data in the...
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Seung Mok Lee (Carnegie Mellon university)Accelerator NeutrinosPoster
Coherent elastic neutrino–nucleus scattering (CEνNS) has opened a new avenue for new-physics searches. The COHERENT collaboration leads precision measurements of CEνNS at Oak Ridge National Laboratory (ORNL); however, these measurements are currently limited by the 10% uncertainty in the neutrino flux. To better constrain the neutrino flux, we have deployed a pair of water Cherenkov detectors...
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Carsten Rott (University of Utah)New Technologies for Neutrino PhysicsPoster
The IceCube Neutrino Observatory is the world’s largest neutrino telescope, located at the South Pole. IceCube has delivered numerous scientific results using the Antarctic ice as its detection medium. Building on its success and aiming to enhance the observatory’s sensitivity to neutrinos in the GeV energy range, the IceCube Upgrade, featuring new optical modules and calibration devices, was...
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Cedric Cerna (CENBG/CNRS)Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a large-scale
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neutrino experiment designed to address multiple physics goals such as determining
neutrino mass hierarchy, precisely measuring oscillation parameters, neutrino
detection from supernova, sun, and earth, etc. with its central detector (CD) requiring
a 20 kt liquid scintillator (LS) volume, ultra-low radioactive... -
Prof. Michael Wurm (Johannes Gutenberg Universitaet Mainz (DE))Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20 kt liquid scintillator experiment in Jiangmen (China). Its main scientific goal is to determine the neutrino mass ordering by measuring electron antineutrinos. To achieve this goal the liquid scintillator had to go through several purification plants on site to ensure it meets the optical and radiopurity requirements.
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The 20m³... -
Samuele Sangiorgio (Lawrence Livermore National Laboratory)New Technologies for Neutrino PhysicsPoster
The possible existence of additional heavy or right-handed (sterile) neutrino states remains a key window onto physics beyond the Standard Model. Heavy neutrinos in the keV mass range are particularly compelling as potential dark-matter candidates. Establishing or ruling out the existence of heavy neutrinos in this region of parameter space would represent a major milestone, with the potential...
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Jiangmei YangNew Technologies for Neutrino PhysicsPoster
The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino oscillation experiment. A critical component of the DUNE Near Detector (ND) is a Liquid Argon Time Projection Chamber (LArTPC) called ND-LAr. A novel pixelated charge readout technology, LArPix, has been developed for use in ND-LAr and other LArTPCs. This technology has been implemented in the 2x2...
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44. Detecting geoneutrinos from the ocean floor: Overview of the Ocean Bottom Detector (OBD) projectMisaki Hosoya (Tohoku University)GeoneutrinosPoster
Geoneutrinos are the electron antineutrinos produced by beta decays of radioactive isotopes within the Earth. By detecting them, we can get information about the planet's radiogenic heat production and the distribution of heat-producing elements in the Earth. However, due to their extremely small mass and weak interactions, geoneutrinos are incredibly challenging to detect.
Nonetheless, in...
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Eli Mygatt WardAccelerator NeutrinosPoster
At Oak Ridge National Laboratory (ORNL), the COHERENT collaboration completed construction of a heavy water Cherenkov detector in the summer of 2023 to measure the neutrino flux from the Spallation Neutron Source (SNS) via the scattering of neutrinos on deuterium nuclei, with the primary aim of improving the precision of past and future CEvNS measurements. Thus far, the SNS neutrino flux has...
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Ms Mei YE (Institute of High Energy Physics，Chinese Academy of Sciences)Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a multipurpose neutrino experiment featuring the world’s largest liquid scintillator detector. With a 20-kton target mass instrumented with more than 17,000 20-inch and 25,600 3-inch photomultiplier tubes (PMTs), JUNO enables neutrino measurements with unprecedented precision.To ensure the stable operation of this highly complex detector,...
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Nicholas Craft (Drexel University)Reactor NeutrinosPoster
The Precision Reactor Oscillation and SPECTrum (PROSPECT) experiment is a short-baseline reactor experiment that was located at the High Flux Isotope Reactor (HFIR), an 85MW highly-enriched uranium reactor at Oak Ridge National Laboratory (ORNL). A goal of PROSPECT is to measure the absolute neutrino flux, a measurement that is dependent on several detector characteristics and variables that...
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Aya El Boustani (Institute of Physics, Johannes Gutenberg University of Mainz)Neutrino MassPoster
Direct measurements of the tritium β-decay spectrum near its endpoint provide one of the most sensitive probes of the absolute neutrino mass. Project 8 and KATRIN both pursue this goal using distinct experimental techniques. Reaching next-generation sensitivity will require atomic tritium, since the molecular final-state distribution introduces intrinsic broadening of the observed spectrum....
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Aobo LiNew Technologies for Neutrino PhysicsPoster
In large neutrino experiments such as the Deep Underground Neutrino Experiment (DUNE), estimating detector response uncertainties typically requires simulation samples that consume substantial computing resources and time. To mitigate this challenge, we present DetSuM, an uncertainty-aware surrogate model designed to capture the detector response variations with reduced computing load compared...
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Jessica Burns (University of Cincinnati)Sterile NeutrinosPoster
NOvA is a long-baseline neutrino oscillation experiment utilizing two functionally identical liquid scintillator detectors located 14 mrad off-axis from the NuMI beam at Fermilab. The position of the Near Detector (ND), 1 km from the neutrino production target, means it sees a range of off-axis angles (12.6-17.2 mrad), resulting in a noticeable energy gradient across the detector face. In...
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Panagiotis Englezos (UC Berkeley)New Technologies for Neutrino PhysicsPoster
Hybrid neutrino detectors combine Cherenkov and scintillation light to achieve directional sensitivity and high light yield, enhancing particle identification and event reconstruction. Water-based liquid scintillators (WbLS) enable this hybrid approach through tunable mixtures of Cherenkov and scintillation light. A pioneering testbed for WbLS is Eos, a 20-tonne detector located at the...
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David Drobner (University of Pennsylvania)Reactor NeutrinosPoster
Precision measurements in the SNO+ experiment require an accurate characterization of the detector's background profile. This work investigates anomalous background events identified in the reactor antineutrino analysis, hypothesized to arise from the elastic scattering of alpha particles on protons within the liquid scintillator.
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While alpha particles are typically heavily quenched, recoil... -
洸樹 林New Technologies for Neutrino PhysicsPoster
The Hyper-Kamiokande (HK) experiment aims to discover CP violation in the lepton sector by measuring the neutrino oscillation probabilities through the detection of accelerator neutrinos at the near detectors located immediately downstream of the beam source and at the far detector located 295 km away. While the far detector measures neutrinos using a water target, the existing magnetized near...
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Yasuhiro Nishimura (Keio University (JP))New Technologies for Neutrino PhysicsPoster
An R12860 photomultiplier tubes (PMTs) with a box-and-line dynode structure, manufactured by Hamamatsu Photonics, has been developed for the next-generation water Cherenkov detector, Hyper-Kamiokande. Detector operation is scheduled to begin in 2028, featuring the world’s largest target mass of 260 kton of ultra-pure water, enabling a broad physics program including neutrino studies and...
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Yoomin Oh (Institute for Basic Science)New Technologies for Neutrino PhysicsPoster
We developed a software trigger utilizing the Pearson linear correlation coefficient or so-called $r$ which quantifies the resemblance between a slice of continuous data stream and the signal template. The $r$ trigger method was found to outperform conventional approaches using the pulse amplitude in terms of lowering the threshold in a time-varying noise environment. Combining with a simple...
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Camilla Forza (Universita e INFN, Padova (IT))New Technologies for Neutrino PhysicsPoster
The off-axis near detector ND280 of the T2K experiment has recently undergone a major upgrade. As part of this upgrade, two new gaseous High-Angle Time Projection Chambers (HA-TPCs) were installed above and below the SuperFGD, a highly segmented scintillator target. This configuration allows precise reconstruction of particles produced at large angles with respect to the neutrino beam. The...
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Haohui CheAccelerator NeutrinosPoster
Three-dimensional projection scintillator detectors have demonstrated excellent imaging and tracking performance in recent accelerator-based neutrino experiments. To build on this concept, Brookhaven National Laboratory (BNL) is developing a liquid implementation that removes physical voxel boundaries while preserving fine-grained three-dimensional reconstruction. The approach employs an...
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Ayana Asai (Okayama University (JP))Accelerator NeutrinosPoster
The Tokai-to-Kamioka (T2K) experiment is a long-baseline neutrino oscillation experiment. It observes a neutrino beam produced at J-PARC with the Super-Kamiokande detector, located 295 km away, to search for CP violation(CPV) in the lepton sector. T2K has already obtained results suggesting CPV with more than 90% confidence level, and the goal is to confirm this indication with higher...
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Praveen Kumar (University of Alabama)New Technologies for Neutrino PhysicsPoster
Water-based Liquid Scintillator (WbLS) has emerged as a compelling medium for next-generation, large-scale neutrino experiments. By combining the high light yield of organic scintillators with the directionality and cost-effectiveness of Cherenkov detectors, WbLS offers enhanced sensitivity for measuring the CP-violating phase in long-baseline oscillations and detecting low-energy neutrinos....
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Yuhan (Hank) Hua (Imperial College (GB))Accelerator NeutrinosPoster
The T2K and NOvA experiments study neutrino oscillations using predominantly muon and antimuon flavor accelerator neutrino beams from J-PARC in Japan and Fermilab in the United States, respectively. Observations of muon and electron neutrino interactions in the experiments' Far Detectors, at baselines of hundreds of km from the neutrino source, permit inferences on parameters of the PMNS...
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Omar A. Alterkait (Tufts University / SLAC)New Technologies for Neutrino PhysicsPoster
Next-generation neutrino experiments such as DUNE and Hyper-Kamiokande will operate massive, monolithic detectors at unprecedented beam intensities and event rates. This places enormous demands on simulation, both in the sheer statistical volume required by modern analyses and in the precision of detector modeling needed for systematic control in oscillation measurements. Traditional...
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Weiran Xu (Stanford University)New Technologies for Neutrino PhysicsPoster
Optically levitated micrometer-scale objects provide a unique capability to measure the vector momentum of small impulses through their center-of-mass motion, preserving directional information at momentum transfers where conventional detectors typically lack directional sensitivity. We operate a vector force sensor based on optically levitated dielectric microspheres, trapped in a single-beam...
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Anika Katt (Boston University)New Technologies for Neutrino PhysicsPoster
Eos is a four-ton detector developed to study hybrid neutrino detection with water-based liquid scintillator (WbLS), combining the directional sensitivity of Cherenkov light with the high photon yield of scintillation. A central objective is to demonstrate directional reconstruction of low-energy electrons in a medium where Cherenkov photons are embedded within a dominant scintillation signal....
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Christine KrausApplications and Neutrino Impacts on HumanityPoster
Large-scale physics experiments rely on diverse, interdisciplinary teams and long-term sustainability, making equity, diversity, and inclusion (EDI) essential components of scientific excellence. SNOLAB has undertaken a coordinated effort to strengthen EDI across its user community, with particular attention to student and early-career researcher engagement, collaboration-level initiatives,...
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Aleena Rafique (Argonne National Laboratory (US))New Technologies for Neutrino PhysicsPoster
Large-scale neutrino experiments increasingly depend on advanced computing technologies to support complex simulation, reconstruction, and analysis workflows. We present DUNE-GPT, a web-based computing and workflow platform developed as an enabling technology for the Deep Underground Neutrino Experiment (DUNE).
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DUNE-GPT provides a unified interface for searching internal documentation and... -
AJ Nielsen (University of California Irvine (US))Accelerator NeutrinosPoster
The 2x2 Demonstrator and the Full Scale Demonstrator (FSD) are prototypes of the Liquid Argon Time Projection Chamber (ND-LAr) that will be used in the Near Detector complex of the Deep Underground Neutrino Experiment (DUNE). These detectors incorporate several innovations to cope with the high level of pile-up expected at ND-LAr, such as the adoption of a modular design and the use of a...
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Lin Si (Stanford University)New Technologies for Neutrino PhysicsPoster
Pre-breakdown high-voltage phenomena (HVPs)—notably electroluminescence (EL) and micro-discharges—limit the stability and background performance of liquid xenon time-projection chambers (LXe TPCs) in neutrinoless double-beta decay ($0\nu\beta\beta$) and Dark Matter searches. We present results from a 10 kg LXe high-voltage testbed at Stanford, designed to characterize these HVPs and evaluate...
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Chinmay Murthy (University of Texas at Austin), Hanyi Chen1Accelerator NeutrinosPoster
The NuMI Off-axis $\nu_e$ Experiment (NOvA) is a long-baseline neutrino oscillation experiment that studies a neutrino beam produced by the Neutrinos at the Main Injector (NuMI) facility at Fermilab to constrain the PNFS mixing angles, the neutrino mass hierarchy, and the CP-violating phase $\delta_{CP}$. These parameters are extracted by comparing the spectra of muon neutrinos and electron...
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Nupur Oza (Columbia University)Neutrino OscillationsPoster
The Short Baseline Neutrino (SBN) program at Fermilab employs a near detector, SBND, and a far detector, ICARUS, to measure muon neutrino disappearance and electron neutrino appearance and disappearance from the muon neutrino-dominated Booster Neutrino Beam. The use of the same liquid argon time projection chamber (LArTPC) technology in both detectors and the same neutrino beam enables a...
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Laura Iuliana Munteanu (CERN)New Technologies for Neutrino PhysicsPoster
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. Current neutrino scattering measurements are difficult to perform and interpret due to the broad-band nature of artificial neutrino beams and associated neutrino flux uncertainties. Building on the ideas and R&D...
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Wonsang Hwang (Department of Physics, Kyung Hee Univ)Sterile NeutrinosPoster
The JSNS2 (J-PARC Sterile Neutrino Search at the J-PARC Spallation Neutron Source) experiment searches for neutrino oscillations at a 24m baseline, targeting Δm² of order 1 eV². For short-baseline oscillation analyses, precise control of the reconstructed energy scale and spatial uniformity of the detector response is essential to reduce systematic uncertainties. In this study, we utilize...
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Akira Takenaka (Sun Yat-sen University)1Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kton liquid scintillator detector located ~650 m underground in southern China. Its primary physics goal is to determine the neutrino mass ordering (NMO) by precisely measuring the energy spectrum of reactor antineutrinos at a baseline of ~53 km. Following nearly a decade of construction, the JUNO detector began official operation on...
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Raphaël GAZZINI (lp2ib)Reactor NeutrinosPoster
The JUNO (Jiangmen Underground Neutrino Observatory) detector is outfitted with two light collection systems, a set of Large PMTs (LPMTs, 20-inch) and a set of Small PMTs (SPMTs, 3-inch). LPMTs collect the majority of light, whereas SPMTs work in the single photon counting regime and have a linear energy response based on counting hits. Thus, SPMTs provide semi-independant, complementary...
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Roberto Mandujano (University of California Irvine)Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20 kton liquid scintillator detector and began data-taking in full liquid scintillator state from August 2025. The primary physics goal is to determine the neutrino mass ordering through a precise measurement of the reactor anti-neutrino energy spectrum via the inverse beta decay (IBD). This requires a dedicated calibration of energy...
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Dr Charles Prior (RAND)Applications and Neutrino Impacts on HumanityPoster
Neutrino detection has been proposed as a complementary monitoring tool for current reactor designs, yet adoption has remained limited due to perceptions that such technologies do not provide meaningful improvements over existing safeguards methodologies. However, the emergence and potential widespread deployment of advanced nuclear reactors poses significant challenges to traditional...
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Shogo Horiuchi (Keio University)New Technologies for Neutrino PhysicsPoster
Hyper-Kamiokande, the successor to Super-Kamiokande, is a next-generation water Cherenkov detector scheduled to begin operation in 2028. It aims to measure neutrino oscillation parameters, including the CP-violating phase and the mass ordering, with significantly higher precision than Super-Kamiokande. This improvement is enabled by its fiducial volume, which is 8.4 times larger, leading to...
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Hannah Binney (MIT)Neutrino MassPoster
The Project 8 experiment is pioneering cyclotron radiation emission spectroscopy (CRES) to measure the energy spectrum of beta electrons emitted in the decay of tritium, with the goal of improving sensitivity to the neutrino mass to 0.04 eV. The current prototype, the Cavity CRES Apparatus (CCA), will be the first CRES detector with resonant cavity geometry, enabling scalability, improved...
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Zhenxiong XieNew Technologies for Neutrino PhysicsPoster
Water Cherenkov and liquid scintillator detectors represent two complementary approaches in neutrino physics. Water Cherenkov detectors provide particle track direction and particle identification (PID) through Cherenkov ring topology, while liquid scintillator detectors offer higher light yield and lower energy thresholds. Water-based liquid scintillator (WbLS) is designed to combine the...
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Barbara CaccianigaReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kiloton multipurpose liquid scintillator detector located in Guangdong Province, China. It is designed to address several fundamental open questions in neutrino physics. Following the completion of detector construction in 2024, JUNO entered the data taking phase in September 2025.
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Positioned at an optimized baseline of... -
Yiqi LiuNew Technologies for Neutrino PhysicsPoster
Microchannel plate photomultiplier tubes (MCP-PMTs) working in
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photon-counting mode are critical for extremely low-light detection in
next-generation liquid-based neutrino experiments. Recent advancements
utilizing atomic layer deposition at the MCP end-face have pushed
photoelectron collection efficiencies to nearly 100%. However, this
introduces a complex, non-Gaussian single-electron... -
Gabriel Oliveira (Universidade Estadual de Campinas - UNICAMP)New Technologies for Neutrino PhysicsPoster
Liquid Argon Time Projection Chambers (LArTPCs), such as those for the DUNE experiment, require oxygen contamination levels below 100 ppt to ensure long electron lifetimes and maximize physics reach. While commercial copper-based adsorbents (e.g., BASF Cu-0226 S) are the current standard, there is a continuous search for media with higher capture capacity and better cost-effectiveness....
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Astrid AnkerNew Technologies for Neutrino PhysicsPoster
Precise measurements of electron capture (EC) decays provide a sensitive probe of physics beyond the Standard Model, as the final state contains a neutrino and a recoiling atom, allowing any new massive particle coupled to the neutrino to be detected through momentum conservation via the nuclear recoil. The Beryllium Electron capture in Superconducting Tunnel Junctions (BeEST) collaboration...
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Joseph Lau (UCLA)Applications and Neutrino Impacts on HumanityPoster
We present a modern reassessment of the feasibility of neutrino beam communication using muon sources, motivated by two influential but conflicting studies in 2003 and 2010. The 2003 paper, using pion-decay neutrino beamlines, concluded that neutrino communication is not practical, while the 2010 paper argued that a muon storage ring neutrino factory could reach feasible rates. In this work,...
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Weijun Li (Institute of High Energy Physics, Chinese Academy of Science)1Reactor NeutrinosPoster
Reactor antineutrino experiments enable precision measurements of neutrino oscillation parameters through the observed energy spectrum. The Jiangmen Underground Neutrino Observatory (JUNO) aims to achieve unprecedented precision, requiring tight control of detector-related systematic uncertainties. In the early phase of data taking with limited statistics, accurate normalization—driven...
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Cristobal Ignacio Morales Reveco (GSI Helmholtzzentrum für Schwerionenforschung, RWTH Aachen University, Johannes Gutenberg-Universität Mainz)GeoneutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) in China, successfully started taking physics data in August 2025, following a 15-year journey from design to completion. Designed to determine the neutrino mass ordering, JUNO is located 52.5 km from eight nuclear reactors, making reactor antineutrinos the dominant signal source. Nonetheless, thanks to its large size of 20 kton of liquid...
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Dario Pullia (CERN, APC)Accelerator NeutrinosPoster
The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline oscillation experiment, aiming to address fundamental questions about neutrino oscillations, CP violation, and the origin of matter–antimatter asymmetry. At CERN, the ProtoDUNE detectors play a crucial role in preparing for the DUNE far detector construction and operation through extensive testing of detector...
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Dongha Lee (KEK)Sterile NeutrinosPoster
The JSNS2 (J-PARC Sterile Neutrino Search at the J-PARC Spallation Neutron Source) experiment searches for neutrino oscillations over a baseline of 24 meters, targeting Δm² values near 1 eV². Our goal is to perform a direct test of the LSND anomaly.
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We conducted long physics runs from 2021 to 2025, accumulating a total exposure of 5.1 × 10²² protons on target (POT) at J-PARC.
The data... -
Mr Yongchang Lee (Seoul National University)Sterile NeutrinosPoster
keV-scale sterile neutrinos are well-motivated warm dark matter candidates. While astrophysical constraints rely on cosmological assumptions, laboratory beta-decay measurements provide a complementary and largely model-independent approach by searching for spectral distortions. The LiFE-SNS project measures the full tritium beta-decay spectrum using neutron-irradiated LiF crystals with...
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Adam Jude Aurisano (University of Cincinnati (US))Sterile NeutrinosPoster
NOvA is a long-baseline experiment with two functionally identical detectors with a Near Detector placed 1 km from the neutrino source at Fermilab and a Far Detector 810 km away at Ash River, Minnesota. NOvA uses a very high-intensity (∼900 kW) beam of neutrinos and antineutrinos from Fermilab’s NuMI beamline, together with two functionally identical detectors placed 14 mrad off the beam axis....
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Afroditi PapadopoulouNeutrino InteractionsPoster
The neutrino direction reconstruction is of importance in the context of DUNE sub-GeV atmospheric oscillation studies. In this work, we investigate the expected precision of the reconstructed neutrino direction using a 𝜈𝜇-argon quasielasticlike event topology with one muon and one proton in the final state in the MicroBooNE liquid argon time projection chamber. MicroBooNE allows for a...
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Vanessa Cerrone (University of Padova / INFN Padova)Neutrino OscillationsPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a reactor neutrino experiment located in South China. JUNO’s primary objective is to determine the neutrino mass ordering (NMO) and precisely measure three oscillation parameters, $\Delta m_{31}^{2}$, $\Delta m_{21}^{2}$, and $\sin^2\theta_{12}$, opening a new era of precision neutrino oscillation physics. JUNO detects electron...
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Prof. Gabriel Orebi Gann (University of California, Berkeley / Lawrence Berkeley National Laboratory)Applications and Neutrino Impacts on HumanityPoster
Modern large-scale experiments depend on sustained, international collaboration across decades. While detector innovation and analytical advances drive discovery, long-term scientific success also relies on robust human infrastructure: retention, leadership development, and research environments that enable scientists to thrive across career stages. Persistent disparities in visibility,...
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Darcy Newmark (Massachusetts Institute of Technology)2New Technologies for Neutrino PhysicsPoster
This poster presents the demonstrated and potential physics capabilities for liquid argon light collection detectors able to resolve both scintillation and Cherenkov signals. This work builds on the first event-by-event observation of Cherenkov radiation from sub-MeV electrons in a high-yield scintillator (liquid argon) detector (PRL 135 (2025) 17, 171804, PRD 112 (2025) 7, 072010),...
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Adam Lister (University of Wisconsin - Madison)Sterile NeutrinosPoster
The NOvA experiment’s most recent search for eV-scale sterile neutrinos under a 3+1 model simultaneously analyses muon neutrino and neutral current datasets from the NuMI beam at it's Near (~1km baseline) and Far (810 km baseline) detectors to look for oscillations consistent with a sterile neutrino. The analysis is systematically limited in the region of parameter space where $\Delta m^2_{41}...
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Yousen Zhang (Brookhaven National Laboratory)Accelerator NeutrinosPoster
The Deep Underground Neutrino Experiment (DUNE) is a next-generation neutrino oscillation experiment with near and far detectors. The DUNE Near Detector employs a pixelated liquid argon Time Projection Chamber (ND-LAr). Its pixelated readout system, LArPix, provides direct imaging of charge deposition through zero-suppressed, data-driven sampling. While this design enables high-rate operation...
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Yusuke Koshio (Okayama Univ.)Accelerator NeutrinosPoster
The NA61/SHINE Collaboration has successfully measured hadron production in hadron–nucleus interactions over a momentum range of 30–120 GeV/c for neutrino experiments. These measurements have provided essential inputs for neutrino experiments such as T2K and those at Fermilab. Recently, there has been an increasing demand for NA61/SHINE to perform measurements with hadron beams at momenta...
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Walter Pettus (Indiana University)Neutrino MassPoster
An atomic tritium source is a key component of the Project 8 experiment, which targets a neutrino mass sensitivity of 40 meV. This atomic source is critical to overcome the statistical and systematic limitations inherent to molecular tritium sources, which have been employed by prior experiments. The source begins with a high flux (~10$^{19}$ atoms/sec) dissociator, with both thermal cracker...
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Guangbao Sun (Wuhan University), Dr Xuefeng Ding (IHEP)Reactor NeutrinosPoster
Precision reactor neutrino experiments rely on forward-folded reconstructed energy spectrum fitting to measure oscillation parameters and determine the neutrino mass ordering. These analyses require repeated convolution of reactor fluxes, inverse beta decay (IBD) cross sections, and detector response models. When constructing frequentist confidence intervals using the Feldman–Cousins method,...
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Bruno Gelli (UC Davis)New Technologies for Neutrino PhysicsPoster
The Accelerator Neutrino Neutron Interaction Experiment (ANNIE) is a gadolinium-doped water Cherenkov detector located on the Booster Neutrino Beam (BNB) at Fermilab. Its primary physics goals include measuring neutron multiplicity in neutrino–nucleus interactions and determining the charged-current cross section of muon neutrinos. In addition to its physics program, ANNIE serves as a testbed...
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Chuang Xu1Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) hosts the world's largest liquid scintillator detector, dedicated to measuring the neutrino mass ordering (NMO). The determination of NMO is highly sensitive to energy resolution, which is critically degraded by radioactive backgrounds, particularly from photomultiplier tubes (PMTs). JUNO employs 17,596 20-inch and 25,587 3-inch PMTs, whose...
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Christopher Sauer (UCSB)Accelerator NeutrinosPoster
Numerous new physics models predict massive long-lived particles that can decay to muon pairs. However, searching for such di-muon BSM signals in LArTPC-based neutrino experiments is challenging because of the nearly irreducible neutrino background that includes one muon and one pion in the final states. The primary limiting factor is the insufficient distinction between muons and pions due to...
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Erin Yandel (LANL)Accelerator NeutrinosPoster
The MicroBooNE experiment is an 85-ton active volume liquid argon time projection chamber (LArTPC) neutrino detector situated in the Fermilab Booster Neutrino Beam. One of the main goals for MicroBooNE is to investigate the “low energy excess” (LEE) of electromagnetic events observed by the MiniBooNE experiment by leveraging the unique capabilities of the LArTPC technology to distinguish...
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Yuri Bae (University of Minnesota)Accelerator NeutrinosPoster
Deep Underground Neutrino Experiment (DUNE) is a next-generation, long-baseline neutrino oscillation experiment that will utilize an intense neutrino beam from Fermilab to measure neutrino oscillation parameters with unprecedented precision. The DUNE-PRISM near detector concept employs an off-axis measurement strategy to mitigate neutrino-nucleus interaction uncertainties; however, this...
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Zhonghua Qin (Institute of High Energy Physics, Chinese Academy of Sciences)New Technologies for Neutrino PhysicsPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a new-generation neutrino experiment equipped with a total of 20,348 20-inch photomultiplier tubes (PMTs), which include 17,596 PMTs for the central detector and 2,752 PMTs for the VETO detector. Following over a decade of construction, JUNO commenced its scientific operation in August 2025. This poster presents a comprehensive overview...
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Junjie Jiang (Shanghai Jiao Tong University), Marco Grassi (Universita e INFN, Padova (IT))Reactor NeutrinosPoster
Located in the Jiangmen City, Guangdong Province, China, the Jiangmen Underground Neutrino Observatory (JUNO) is an experiment with a spherical central detector (CD) filled with ultra-pure liquid scintillator surrounded by a pool filled with ultra-pure water (WP). About 17,612 large 20-inch PMTs and 25,600 smaller 3-inch PMTs were instrumented to collect the light from CD and a few thousands...
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Diego Venegas Vargas (Johns Hopkins University)Sterile NeutrinosPoster
The PROSPECT, STEREO, and Daya Bay experiments have each delivered important
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contributions to reactor antineutrino research. PROSPECT and STEREO focus on
short-baseline (~10 m) measurements using highly enriched uranium (HEU) research reactors,
where nearly all antineutrinos originate from U-235 fissions. Meanwhile, Daya Bay investigates
antineutrino emissions from low-enriched uranium... -
Rosmarie Irma Wirth (GSI Helmholtzzentrum für Schwerionenforschung GmbH)Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is designed to determine the neutrino mass ordering and to perform precision measurements of the neutrino oscillation parameters. JUNO consists of a 20-kt liquid scintillator target monitored by a double calorimetry system consisting of 17596 20-inch large photomultiplier tubes (LPMTs) complemented by a 3-inch small photomultiplier tube...
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Dr Fei Li (IHEP, CAS, China)Reactor NeutrinosPoster
The JUNO data acquisition system reads data from about 7,000 electronic channels. It collects data from roughly 20,000 20-inch PMTs and 25,000 3-inch PMTs. Implemented on a computing cluster of about 100 nodes, the system uses cluster-parallel DAQ software. It forms a large-scale distributed DAQ. It can perform real-time acquisition and online processing of the central detector at a 1 kHz...
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Liangjian Wen, Minghua Liao (Sun Yat-Sen University (CN))Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) experiment has completed its construction, and officially started data taking. Its primary physics goals are to determine the neutrino mass ordering and to perform high-precision measurements of neutrino oscillation parameters. The JUNO data production is designed to reconstruct RTRAW data files, and to generate Event Summary Data (ESD)...
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Mingxia Sun (The Institute of High Energy Physics of the Chinese Academy of Sciences)Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kiloton multi-purpose liquid scintillator detector designed to determine the neutrino mass ordering and measure neutrino oscillation parameters with sub-percent precision. Following the completion of construction, JUNO began its first physics data taking phase in August 2025 and released world-leading precision measurements on the...
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Min Pi (武汉大学), Tobias LachenmaierReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kton multi-purpose underground liquid scintillator (LS) detector, with the determination of the neutrino mass hierarchy as one of its primary physics goals. The optical transparency of the LS is of utmost importance for JUNO in order to achieve its unprecedented 3% energy resolution. In this poster, we present a method for measuring...
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Haoqi LuReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) features a 20-kton liquid scintillator detector located 700 meters underground, with the primary goal of determining the neutrino mass ordering. To effectively identify cosmic muons and suppress associated backgrounds, a dedicated Water Cherenkov veto system has been constructed. This system surrounds the central detector and is filled with...
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Pascoal José Giglio PagliusoNew Technologies for Neutrino PhysicsPoster
The target for neutrino and dark matter experiments usually rely on liquified noble gases with extremely high grade of purity , in particular, regarding level oxygen contamination (< 100 ppt). Ultra-pure Liquid Argon (LAr) is the chosen target for the Long Baseline Neutrino Facility (LBNF) – Deep Underground Neutrino Experiment (DUNE). Brazilian in-Kind contribution for LBNF-DUNE cryogenics...
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Alexander Antonakis (University of California, Santa Barbara), Sparshita Dey1New Technologies for Neutrino PhysicsPoster
The Liquid Argon Charge Amplification Devices (LArCADe) project is an R&D effort aimed at developing instrumentation capable of lowering detection thresholds for ionization signatures in liquid and gaseous argon detectors and achieving O(100 𝜇m) position resolution. The core concept is the use of sharp “tip arrays” that generate strong local electric-field enhancement, enabling charge...
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Inwook Kim (Lawrence Livermore National Laboratory)Sterile NeutrinosPoster
The Beryllium Electron Capture in Superconducting Tunnel Junctions (BeEST) experiment searches for sub-MeV heavy neutrino mass eigenstates. High doses of $^7$Be are directly implanted into high-resolution superconducting tunnel junction (STJ) cryogenic sensors, which measure the nuclear recoil energy of the $^7$Li daughters with 1–2 eV energy resolution. If heavy neutrino states exist,...
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Jisu ParkNeutrino OscillationsPoster
The JSNS²-II (the second phase of the J-PARC Sterile Neutrino Search at the J-PARC Spallation Neutron Source) experiment aims to search for sterile neutrinos using two detectors located at baselines of 24 m and 48 m. To directly test the LSND anomaly, JSNS²-II employs the same neutrino source, the same neutrino target, and the same interaction channel as the LSND experiment. At the J-PARC...
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Alejandro Yankelevich (University of California, Irvine)New Technologies for Neutrino PhysicsPoster
Liquid argon time projection chambers (LArTPCs) such as the Deep Underground Neutrino Experiment (DUNE) must maintain high argon purity as electronegative impurities can capture drift electrons, degrading signal quality and raising the detection threshold of particle energy depositions. A purity monitor is a miniature TPC that measures the electron lifetime by comparing the charge collected...
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Mr Max de Carlos Generowicz (University of Sussex)New Technologies for Neutrino PhysicsPoster
LiquidO is an innovative scintillator-based radiation detector concept whose core principle is the self-segmentation of the detector volume via stochastic light confinement in an opaque medium. Light produced in the scintillator is confined near its creation point thanks to the short scattering length of the material, and efficiently collected by a lattice of wavelength-shifting optical fibres...
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Elise Novitski (University of Washington)Neutrino MassPoster
We present the design concept for the Project 8 Low Frequency Apparatus. The Project 8 Collaboration is planning to make a neutrino mass measurement using the tritium endpoint method with a sensitivity of 40 meV. The Project 8 experiment is designed around the use of Cyclotron Radiation Emission Spectroscopy (CRES). The experiment is divided into four phases, with Phases I and II already...
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Nathan Higginbotham (University College London)Neutrino MassPoster
Determining the absolute neutrino mass is one of the primary objectives in particle physics today. While oscillation experiments have constrained the differences between the mass eigenstates, the absolute scale is unknown. The Quantum Technologies for Neutrino Mass (QTNM) collaboration aims to address this by utilising Cyclotron Radiation Emission Spectroscopy (CRES) with an atomic tritium...
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Sumita Ghosh (Lawrence Livermore National Lab)Applications and Neutrino Impacts on HumanityPoster
MAD-PSD is one of two reactor antineutrino detection subsystems constructed by the Mobile Antineutrino Demonstrator (MAD) project. Constructed from large bar castings of 6Li-doped pulse shape discriminating (PSD) plastic scintillator, this device is designed to perform reactor monitoring measurements with little to no overburden. MAD-PSD is formed from 64 plastic scintillator bars with...
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Maria Martinez CasalesNew Technologies for Neutrino PhysicsPoster
High precision measurements of neutrino interactions are essential for the success of future neutrino oscillation experiments. Understanding the interaction rate and precise energy spectrum requires understanding of neutrino interactions and nuclear effects. Measuring interactions in a light nuclear target , such as Hydrogen or deuterium, would provide highly valuable input to reduce reduce...
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Ryan Bouabid (Los Alamos National Laboratory)Accelerator NeutrinosPoster
The COHERENT collaboration reports a new measurement of coherent elastic neutrino–nucleus scattering (CEvNS) using low-threshold high-purity germanium detectors deployed at the Spallation Neutron Source at Oak Ridge National Laboratory. This result extends the first observation by significantly increasing statistics, improving sensitivity to low nuclear recoil energies, and enhancing...
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Dr Matthew Strait (Fermilab)Accelerator NeutrinosPoster
Modern neutrino experiments require precision reconstruction of events. A
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crucial component of this reconstruction is the stopping power for charged
particles, calculated using the Bethe equation. The main free parameter of the
Bethe equation is the mean excitation energy (the "I-value"), which in most
cases cannot be calculated, but must be measured for each substance. In many
cases,... -
Yiwen Xiao (University of California Irvine (US))Neutrino OscillationsPoster
Neutrino–electron elastic scattering is a purely leptonic process with a precisely calculable Standard Model cross section, providing an in situ constraint on accelerator neutrino flux predictions. Using data collected with the NOvA Near Detector in forward horn current mode, we perform a measurement of neutrino–electron elastic scattering and apply a flux-constraint technique based on the...
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Jiahui Wei (Institute of High Energy Physics, CAS)Reactor NeutrinosPoster
The intrinsic $^{14}$C background in liquid scintillator is a major source of low-energy events in JUNO and affects detector performance, including energy resolution, with consequences for low-energy physics analyses. A precise determination of the $^{14}$C decay rate therefore serves multiple purposes such as detector characterisation and background modelling.
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In this poster, we present... -
Vincent Kueviakoe (Nikhef)Neutrino OscillationsPoster
KM3NeT/ORCA will be a Cherenkov neutrino detector of approximately 7 Mton under construction at a depth of 2450 meters in the Mediterranean Sea, off the coast of Toulon, France. The detector is designed as an array of 115 detection lines composed of multi-photomultipliers optical modules. Its primary scientific goals are the determination of the neutrino mass ordering as well as the...
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Jacob McLaughlin (Illinois Institute of Technology)New Technologies for Neutrino PhysicsPoster
The Short-Baseline Near Detector (SBND) of the Short-Baseline Neutrino (SBN) Program is a liquid argon time-projection-chamber equipped with 11,264 charge-readout wires, cryogenic digitization of wire signals, and 120 photomultiplier tubes. These tools provide excellent signal-to-noise ratios and best-in-class light collection efficiency, lowering effective analysis thresholds to the...
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Luis Zazueta Reyes (Syracuse University)Accelerator NeutrinosPoster
The Deep Underground Neutrino Experiment (DUNE) will be a next-generation long baseline neutrino oscillation experiment that will employ LArTPC technology in a near detector placed at Fermilab and a far detector at the Sanford Underground Research Facility, at a baseline of 1300 km. The DUNE Liquid Argon Near Detector (ND-LAr) design takes into account the high neutrino intensity expected from...
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Dirceu Noriler (University of Campinas), Pascoal José Giglio Pagliuso (Universudade Estadual De Campinas (UNICAMP))New Technologies for Neutrino PhysicsPoster
The next generation of liquid argon time projection chambers, such as those in the Deep Underground Neutrino Experiment (DUNE), requires highly pure liquid argon for optimal detector performance. Even trace amounts of electronegative contaminants, especially oxygen, capture drifting electrons and reduce signal amplitude. This contamination compromises spatial resolution. Achieving and...
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Dante Totani (Colorado State University - U.S.)Neutrino OscillationsPoster
ICARUS is a liquid argon time projection chamber (LArTPC) neutrino experiment at Fermilab. Located ~600 m from the Booster Neutrino Beam (BNB) target, it serves as the far detector in the Short-Baseline Neutrino (SBN) Program. The primary objective of the SBN Program is to probe short-baseline neutrino oscillations motivated by anomalous electron-like event excesses observed in previous...
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Shweta Yadav (University of Texas at Arlington)Neutrino OscillationsPoster
The Short-Baseline Neutrino (SBN) program at Fermilab searches for signatures of sterile neutrinos with mass-squared splittings at the O(1) eV2 scale, motivated by anomalies previously reported by the LSND and MiniBooNE experiments. We present a search for such signatures using the muon neutrino disappearance channel. This analysis exploits the large statistics of fully inclusive...
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Guang Luo (Sun Yat-sen university), Jun Cao (Institute of High Energy Physics, Chinese Academy of Sciences), Yichen Li (Institute of High Energy Physics, Beijing)Reactor NeutrinosPoster
As a satellite detector of the Jiangmen Underground Neutrino Observatory (JUNO), Taishan Antineutrino Observatory (TAO/JUNO-TAO) is positioned ~ 44 meters from a reactor core of the Taishan Nuclear Power Plant. Its ton-scale liquid scintillator detector, instrumented with high-coverage Silicon Photomultipliers (SiPMs) operating at cryogenic temperatures, achieves an exceptional light yield and...
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Haojing LaiReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO), the world's largest liquid scintillator (LS) detector, has started physics data taking since Aug. 26th，2025. The primary goal of JUNO is to determine the neutrino mass ordering. A critical challenge in this measurement is the cosmogenic 9Li/8He background induced by the passing muons. Without suppression, their estimated rate (70~80 per...
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Michael Robert Quintieri (University of Notre Dame (US))Accelerator NeutrinosPoster
Long-baseline neutrino experiments stand to benefit from reduced neutrino flux uncertainties. In order to reduce these uncertainties, NA61/SHINE, a fixed target experiment using beams from CERN’s SPS, provides improved measurements of hadron production for constraining neutrino flux uncertainties. The experiment has made a variety of measurements using thin-target data, as well as several...
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Daniel Ferlewicz (Centre National de la Recherche Scientifique (FR))New Technologies for Neutrino PhysicsPoster
Hyper-Kamiokande will start collecting accelerator neutrino data in 2028 to measure the leptonic CP violating phase, $\delta_{CP}$. The largest systematic uncertainty is knowledge of the ratio between the electron neutrino and antineutrino cross sections, $\Delta (\sigma_{{\nu}_e}/\sigma_{\bar{\nu}_e})$. Improper modeling could generate an ambiguous asymmetry in any measured difference...
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Nicole Pallat (University of Minnesota)Sterile NeutrinosPoster
Various short-baseline neutrino experiments observe anomalies that challenge the three-flavor neutrino oscillation model, consistent with a hypothetical “sterile” neutrino that does not interact via the weak force. This poster presents a near detector event selection at the Short-Baseline Near Detector (SBND), developed for the first search for neutral current (NC) disappearance at...
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Nathaniel Bowden (Lawrence Livermore National Laboratory)Applications and Neutrino Impacts on HumanityPoster
There are several application efforts underway in the U.S. that focus on antineutrino detection in the ‘near-field’, within 100m of a monitored location. The efforts to be described in this poster are based on technologies that use Inverse Beta Decay and Li-6 as a neutron capture agent since this supports compact systems with high efficiency and excellent background rejection. These include...
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Benda Xu (Tsinghua University), Zhangming Chen (Shanghai Jiao Tong University)1Reactor NeutrinosPoster
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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Leon PickardApplications and Neutrino Impacts on HumanityPoster
Recent advances in low-energy antineutrino detection have expanded the range of environments and applications in which neutrinos can serve as unique, penetrating probes. We report new results on the potential use of neutrino detectors to constrain fission yield in nearby energetic events, based on a detailed sensitivity study of inverse beta decay detection in realistic background conditions....
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Mohammad Adil Aman (Florida State University)New Technologies for Neutrino PhysicsPoster
The Accelerator Neutrino Neutron Interaction Experiment (ANNIE) is a 26-ton water-based neutrino detector located at Fermilab, approximately 110 m downstream of the Booster Neutrino Beam (BNB). ANNIE utilizes both photomultiplier tubes (PMTs) and advanced photodetectors, specifically Large Area Picosecond Photodetectors (LAPPDs), to detect Cherenkov light emitted by leptons produced in...
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Tatiana Araya-Santander (Universidad Católica del Norte)1Reactor NeutrinosPoster
Using the 59.1-day publicly released JUNO spectrum, we study the impact of isotropic Standard Model Extension coefficients on the antineutrino survival probability. We perform two-dimensional $\Delta \chi^2$ scans exploring the joint parameter space of CPT-even and CPT-odd Lorentz invariance violating coefficients. Our analysis provides JUNO-based constraints on isotropic LIV parameter...
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Nico Stirling (University of Helsinki, Helsinki Institute of Physics)Neutrino OscillationsPoster
Neutrino oscillations are experimentally established, yet their description within quantum field theory remains conceptually subtle—particularly how to define the oscillating one-particle neutrino state. Many formulations recover the phenomenology by introducing the coherent production of flavour states as superpositions of mass eigenstates and by modeling production/detection with external...
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Dr Peter Filip (Institute of Physics, ASCR, Prague)Applications and Neutrino Impacts on HumanityPoster
We discuss the possibility of table-top experiments to demonstrate the neutrino-induced torque on macroscopic matter. The proposed setup employs a small, ferromagnetic, e.g., ring-shaped, samples magnetically levitated above a superconductor and containing nuclei that undergo electron capture (EC) decay. At deep cryogenic temperatures, nuclear spin polarization of the EC-decaying nuclei...
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Dowling Wong (KIT - Karlsruhe Institute of Technology (DE))New Technologies for Neutrino PhysicsPoster
The search for sub-GeV dark matter and precision measurements of low-energy neutrino processes motivate detectors capable of stable operation at eV-scale energy thresholds. The DELight experiment employs superfluid helium-4 instrumented with magnetic microcalorimeters (MMC-based LAMCALs), targeting eV-scale baseline resolution and projected nuclear-recoil thresholds near 10 eV. Such...
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Liangjian Wen, Yuning Su (Sun Yat-Sen University (CN))New Technologies for Neutrino PhysicsPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a large-scale and multi-purpose neutrino experiment located 700 meters underground in southern China. The project began its design phase in 2013, has completed detector construction and started data taking in 2025. To provide a fundamental software framework supporting detector design, algorithm development, and long-term data processing...
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Yongpeng ZhangNew Technologies for Neutrino PhysicsPoster
ypzhang1991@ihep.ac.cn, IHEP, China
On behalf of the JUNO CollaborationThe Jiangmen Underground Neutrino Observatory (JUNO) is a large-scale, multi-physics neutrino experiment that utilizes tens of thousands of photomultiplier tubes (PMTs) to achieve unprecedented energy resolution. Signals from the PMTs are processed by front-end readout electronics and converted into...
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Jaret Heise (Sanford Underground Research Facility)Accelerator NeutrinosPoster
The Sanford Underground Research Facility (SURF) began operation in 2007 as a facility dedicated to advancing compelling multidisciplinary scientific research. SURF is one of the deepest laboratory sites and offers the largest footprint in the world for scientific pursuits, including physics campuses on the 4850-foot level where the LUX-ZEPLIN, MAJORANA DEMONSTRATOR, and CASPAR experiments are...
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Sander Katz (UC, Berkeley)New Technologies for Neutrino PhysicsPoster
On Behalf of the LiquidO Collaboration
Particle tracking and identification are important for rare-event searches and can be achieved using physical detector segmentation in scintillation and Cherenkov detectors. Virtual segmentation within a monolithic active volume can be achieved using an opaque medium that stochastically confines emitted light near its origin. This concept, first...
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Taisiia Smirnova (University of California, Riverside)New Technologies for Neutrino PhysicsPoster
DarkSide-20k is a next-generation liquid argon experiment designed for direct dark matter searches at the Gran Sasso National Laboratory. However, cosmogenic backgrounds impose strict requirements on veto performance, making the 650-ton Outer Veto subsystem essential for protecting the WIMP signal region. Reliable operation of the muon veto requires quantitative understanding of its optical...
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Brunilda MucogllavaNeutrino MassPoster
To overcome statistical and systematic limitations arising from the rovibrational final-state distribution of molecular tritium, future precision mass-measurement experiments are pursuing atomic tritium sources. Within the KArlsruhe Mainz Atomic Tritium Effort (KAMATE), we investigate the dissociation fraction of thermal effusive atomic sources. In these sources, molecular gas is directed...
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Eva Sabater Andres (University of Sussex (GB))1Accelerator NeutrinosPoster
The Deep Underground Neutrino Experiment (DUNE) is a next generation long-baseline experiment designed with a primary goal of providing definitive measurements of the neutrino mass ordering and the Charge Parity (CP)-violating phase $\delta_{CP}$. A key component in reaching these goals is the DUNE Near Detector (ND) complex, placed 574 m from the beam target, and tasked with characterising...
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Mariusz Girgus (University of Warsaw)Neutrino OscillationsPoster
Energy of atmospheric neutrinos observed in the Super-Kamiokande detector ranges from hundreds of MeV to a TeV scale, while the baseline spans from 10km to 13000km. The broad energy and baseline distributions of atmospheric neutrinos result in a range of L/E which spans four orders of magnitude and contains multiple minima and maxima of the muon neutrino survival probability. On the other...
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Lukas BiegerReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a multi-purpose neutrino experiment whose primary objective is the determination of the neutrino mass ordering using a 20-kt liquid scintillator detector. During the filling phase, the Online Scintillator Internal Radioactivity Investigation System (OSIRIS) monitored the radiopurity of the liquid scintillator to ensure that the required...
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Maria Artero Pons (Universita e INFN, Padova (IT))Sterile NeutrinosPoster
The Short-Baseline Neutrino (SBN) program at Fermilab aims to perform a definitive search for light sterile neutrinos using multiple liquid argon time projection chamber detectors. We present the status of an analysis of muon neutrino charged-current interactions in two SBN detectors (SBND and ICARUS), selecting fully contained events with one muon and at least one proton in the final state,...
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V Hewes (University of Cincinnati)Neutrino OscillationsPoster
Liquid Argon Time Projection Chamber (LArTPC) detectors provide excellent spatial resolution, offering the potential to reconstruct a broad range of complicated topologies such as tau neutrino interactions, atmospheric neutrinos, nucleon decay events and others. However, realizing this potential requires sophisticated reconstruction algorithms capable of leveraging the wealth of information...
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Zepeng Li (University of Hawaii)New Technologies for Neutrino PhysicsPoster
We present the development and comprehensive characterization of a large-volume cryogenic pure CsI detector system designed for coherent elastic neutrino-nucleus scattering (CEνNS) measurements and low-energy rare-event searches. The detector system employs two 3.3 kg high-purity CsI crystals operated at approximately 95 K with dual-ended 3-inch photomultiplier tube readout.
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At cryogenic... -
Tanner KaptanogluNew Technologies for Neutrino PhysicsPoster
In this poster we present the first results from Eos, a four-tonne fiducial optical detector located at the University of California, Berkeley. The primary goal of Eos is to demonstrate the performance capabilities of scintillation-based, “hybrid” detector technology for future neutrino detectors, such as Theia. The data presented were collected between July 2024 and May 2025, during which...
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Fengpeng AN (Sun Yat-sen University), Jun Cao (Institute of High Energy Physics, Chinese Academy of Sciences), Yichen Li (Institute of High Energy Physics, Beijing)Reactor NeutrinosPoster
The Taishan Antineutrino Observatory (TAO), a satellite experiment of JUNO, is a ton-scale Gd-doped liquid scintillator detector designed to measure the reactor antineutrino spectrum with exceptional energy resolution. Located 9.6 meters underground at the Taishan nuclear power plant, its shallow depth necessitates an efficient veto system to suppress cosmogenic backgrounds. This poster...
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Denis Torres (South Dakota School of Mines and Technology)New Technologies for Neutrino PhysicsPoster
The Deep Underground Neutrino Experiment (DUNE) is a long baseline neutrino oscillation experiment that relies on a precise Photon Detection System (PDS) to provide accurate timing information, enhance sensitivity to low-energy and non-beam events, and support detector performance studies in liquid argon time projection chambers. Achieving these goals requires a well-understood and stable...
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Miriama RajaoalisoaNeutrino OscillationsPoster
NOvA is a long-baseline neutrino oscillation experiment with two functionally identical detectors: a Near Detector (ND) at Fermilab, placed 1 km from the neutrino source, and a Far Detector (FD) located 810 km away from the ND in Minnesota. NOvA's primary physics goals are precision measurements of neutrino oscillation parameters $\theta_{23}$ and $\Delta m^2_{32}$, sensitivity to the neutrino...
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Jun Cao (Institute of High Energy Physics, Chinese Academy of Sciences), Yichen Li (Institute of High Energy Physics, Beijing)Reactor NeutrinosPoster
The Taishan Antineutrino Observatory (TAO) is a satellite experiment of JUNO, featuring a ton-scale liquid scintillator detector located about 44 m from a reactor core at the Taishan Nuclear Power Plant. TAO detects reactor antineutrinos via inverse beta decay (IBD). An array of silicon photomultipliers (SiPMs) with high photocathode coverage and photon detection efficiency provides a high...
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Garrett WendelNew Technologies for Neutrino PhysicsPoster
Next-generation rare event searches require robust particle identification and background rejection at the MeV scale, driving demand for high-resolution topological imaging. The LiquidO paradigm achieves this by utilizing an opaque monolithic medium to stochastically confine scintillation light, preserving detailed event topology. This localized light is sampled by an embedded lattice of...
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Dr Manoj Kumar Singh (Institute of Physics, Academia Sinica, Taipei 115201, Taiwan)1Reactor NeutrinosPoster
The intense flux of low-energy reactor electron antineutrinos ($\bar{\nu}_{e}$), together with compact low-threshold germanium detectors, provides a powerful experimental platform for precision measurements of coherent elastic neutrino-nucleus scattering ($\nu A_{el}$) [1,2] as well as sensitive probes of neutrino electromagnetic properties [3]. We will present recent experimental results from...
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Phillip BarbeauAccelerator NeutrinosPoster
Ge-mini, a member of the COHERENT suite of detectors, is an array of high-purity germanium semiconductor detectors designed to measure coherent elastic neutrino-nucleus scattering (CEvNS). In this weak neutral-current interaction, the nuclear form factor is primarily sensitive to the neutron spatial distribution and causes a loss of coherence at higher momentum transfers, which appears as a...
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Stephan Meighen-Berger (University of Iowa)Neutrino OscillationsPoster
We propose a new approach to measure the CP-violating phase in neutrino mixing using atmospheric neutrinos, improving upon prior work. Because it is subject to systematic uncertainties that differ from those affecting accelerator-based measurements, the two approaches are complementary, and their combination can yield stronger constraints on $\delta_\mathrm{CP}$. In particular, the differing...
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Aditya MaratheNeutrino OscillationsPoster
NuMI Off-axis Electron Neutrino Appearance (NOvA) experiment is an accelerator long-baseline neutrino oscillation experiment at Fermilab. It aims for a precise measurement of the neutrino oscillation parameters. We present the latest NOvA constraints on the magnitudes of the Pontecorvo-Maki-Nakagawa-Sakata (PMNS) matrix elements, and outline the initial steps toward exploring the unitarity of...
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Brandon Weiss (Columbia)Sterile NeutrinosPoster
We present PROfit, a new open-source C++ framework designed for efficient and robust estimation of neutrino oscillation parameters, systematic uncertainties, and beyond-the-Standard-Model (BSM) physics, with particular emphasis on reliable global optimization in high-dimensional parameter spaces and rigorous treatment of systematics. Initially developed for the Short-Baseline Neutrino (SBN)...
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Alejandro Sonzogni (Brookhaven National Laboratory)1Reactor NeutrinosPoster
Understanding the magnitude and features of the highly precise IBD antineutrino spectra published by the Daya Bay, NEOS, and RENO collaboration have been a challenging and rewarding intellectual quest. With respect to the Huber-Mueller model, these spectra show an overall 5% overprediction in the total yield, known as the Reactor Antineutrino Anomaly (RAA), and an underprediction in the 4-6...
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Jiaxi Liu (UCI)New Technologies for Neutrino PhysicsPoster
NOvA is a long-baseline neutrino experiment studying neutrino oscillations by detecting neutrinos from the NuMI beam at Fermilab. Its physics analysis relies on accurate prong segmentation, which involves matching each hit to its source particle and identifying the particle type. This task has commonly been addressed using a combination of traditional clustering algorithms and convolutional...
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Artur SztucNeutrino OscillationsPoster
NOvA is a long-baseline neutrino oscillation experiment that studies the accelerator-produced neutrino beam from the NuMI facility at Fermilab. With a near detector located close to the beam source and a far detector situated 810 km downstream, NOvA measures muon-neutrino disappearance and electron-neutrino appearance in both neutrino and antineutrino mode operation. A combined analysis of...
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Emerson Bannister (University of Sussex)Accelerator NeutrinosPoster
The NOvA (NuMI Off-Axis electron neutrino Appearance) Experiment is a long-baseline neutrino oscillation experiment composed of two functionally identical detectors, a 300 ton Near Detector, and a 14 kton Far Detector separated by 809 km and placed 14 mrad off the axis of the NuMI neutrino beam created at Fermilab. This configuration enables NOvA's rich neutrino physics program, which includes...
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William Tripp (Tufts University Department of Physics and Astronomy)Accelerator NeutrinosPoster
The widely-used (anti)neutrino event generator GENIE accounts for only tree level Charged-Current
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(CC) (anti)neutrino interactions. In this poster we begin by summarizing previous research into second order QED radiative corrections. After summarizing the theoretical corrections to cross-section distributions in $Q^2$ and $E_\nu$ we analyze the effects of Radiative corrections implemented... -
Andrea Mattera (Brookhaven National Laboratory)Reactor NeutrinosPoster
Next-generation reactor experiments, such as JUNO, will be providing high-fidelity data at high energies, opening a new window into precision neutrino physics. In this energy range, the summation method, rather than conversion calculations, is the only approach capable of providing informative predictions of the antineutrino spectrum.
A critical nuclear data input that has been...
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David Martinez Caicedo (South Dakota School of Mines and Technology)New Technologies for Neutrino PhysicsPoster
The Deep Underground Neutrino Experiment (DUNE) is a next generation long-baseline neutrino experiment that will send an intense beam of neutrinos through two detector complexes: a near detector complex located at Fermilab (Chicago), and a far detector complex located ~1.5 km underground at Sanford Underground Research Facility (SURF) in South Dakota.
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One of the DUNE Far Detector (FD) modules... -
Marco Beretta (INFN-MI)Reactor NeutrinosPoster
JUNO (Jiangmen Underground Neutrino Observatory) is a neutrino experiment located in China, 52.5 km away from two nuclear power plants. It is be the largest liquid scintillator experiment in the world, designed to detect neutrinos and antineutrinos using 20 kton of organic liquid scintillator contained in a large acrylic vessel with a diameter of 35 m.
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The experiment started data taking in... -
Logan Lebanowski (University of California, Berkeley)GeoneutrinosPoster
SNO+ is a liquid scintillator experiment preparing to search for the lepton-flavor-violating process of neutrinoless double beta decay using more than one tonne of Te. With about 780 tonnes of highly-radiopure scintillator located 2 km underground in Ontario, Canada, SNO+ is also able to study antineutrinos from nuclear reactors at least 240 km away and antineutrinos from radioactive decays...
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Nicholas Meredith (North Carolina State University)Accelerator NeutrinosPoster
The COHERENT collaboration performed a reanalysis of the data collected at Oak Ridge National Laboratory's Spallation Neutron Source with its high-purity germanium detector array, Ge-mini. Reanalysis of the "Campaign-2" dataset was motivated by the successful analysis of the "Campaign-3" dataset; which extended coherent elastic neutrino–nucleus scattering (CEvNS) measurements in Ge-mini to a...
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Takumi Omori (University of Tsukuba)Neutrinoless Double Beta DecayPoster
Neutrinoless double beta decay (0$\nu$2$\beta$) would provide experimental evidence for the Majorana nature of neutrinos. Its half-lives can be interpreted in terms of the effective neutrino mass through the phase-space factors and nuclear matrix elements (NMEs). However, theoretical uncertainties in the NMEs lead to an uncertainty of roughly one order of magnitude in the extracted effective...
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Emin Yuksel (Middle East Technical University (TR))Accelerator NeutrinosPoster
The DsTau (NA65) experiment at CERN is designed to measure the inclusive differential cross section for $D_s$-meson production in proton–nucleus (p–A) interactions, where the $D_s$ meson decays into a tau lepton and a tau neutrino. The DsTau detector is based on the nuclear emulsion technique, which provides exceptional spatial resolution and enables precise detection of short-lived particles...
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Matteo CadedduSterile NeutrinosPoster
The Gallium Anomaly, a persistent discrepancy exceeding 5$\sigma$ between measured and predicted neutrino capture rates on $^{71}$Ga from $^{51}$Cr and $^{37}$Ar radioactive sources (GALLEX, SAGE, and BEST), has challenged particle physics for over three decades. This deficit has widely been interpreted as a possible signature of short-baseline oscillations involving eV-scale **sterile...
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Zelimir Djurcic (Argonne National Laboratory (US))New Technologies for Neutrino PhysicsPoster
We study the feasibility of producing monochromatic, low-energy electron antineutrinos via bound-$\beta$ decay of fully stripped radioactive ions and detecting them via resonant antineutrino-induced electron capture on the corresponding isobaric ``mirror'' nucleus. This approach exploits the time-reversed relationship to electron capture and, at resonance, can yield capture cross sections many...
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Luis Mora-Lepin (Florida State University)1Accelerator NeutrinosPoster
The Deep Underground Neutrino Experiment (DUNE) is a cutting-edge, long-baseline experiment under construction in the United States, based on large liquid-argon time projection chambers (LArTPCs). The DUNE Near Detector LArTPC (ND-LAr) will employ a novel modular architecture using a pixelated LArPix charge readout. To validate this design and characterize detector response, the 2×2...
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Carsten Rott (University of Utah), Jorge Torres (University of Utah)New Technologies for Neutrino PhysicsPoster
The IceCube Neutrino Observatory, a neutrino detector located at the South Pole, has recently added six new strings equipped with optical modules and dedicated calibration devices to the central region of the existing array as part of the IceCube Upgrade, completed in early 2026. Among this new instrumentation is a camera-based calibration system, a novel addition deployed on all primary...
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Koh ByoungcheolReactor NeutrinosPoster
The NEON experiment aims to detect coherent elastic neutrino–nucleus scattering (CEvNS) induced by reactor electron antineutrinos using a 16.5 kg NaI(Tl) detector. The detector is installed at a distance of 23.7 m from the Hanbit Unit-6 reactor core in Yeonggwang, South Korea. Data taking began in April 2022, and stable operations have accumulated 860 days of reactor-on data and 223 days of...
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Natalie Tianai Ma (University of California, Irvine)New Technologies for Neutrino PhysicsPoster
The Deep Underground Neutrino Experiment (DUNE) is a flagship long-baseline neutrino oscillation experiment that will use large Liquid-Argon Time Projection Chambers (LArTPCs) to study neutrino properties. DUNE will deploy custom cold electronics for TPC readout, placing stringent requirements on long-term stability and pre-installation Quality Control (QC) of ASIC chips. Robotic Testing...
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Viacheslav Li (Lawrence Livermore National Laboratory)New Technologies for Neutrino PhysicsPoster
Future large neutrino detectors will benefit from scalable scintillation media, fast photosensors, and low power electronics capable of precise timing and high channel density. We present two complementary R&D thrusts under development at Lawrence Livermore National Laboratory.
First, we describe an automated, data driven workflow for the synthesis and characterization of water based...
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Jesse MendezSterile NeutrinosPoster
The Standard Model of particle physics posits the existence of three distinct neutrino flavors. Several anomalous observations inconsistent with the three flavor Standard Model neutrino oscillations have motivated the hypothesis that there exists at least one additional neutrino state, termed the ‘sterile neutrino’ that does not interact directly with matter. Among these anomalies, LSND and...
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Nathaniel Rowe (University of Chicago)Neutrino OscillationsPoster
The Short-Baseline Neutrino (SBN) program at Fermilab is searching for neutrino oscillations over a short baseline as a signature of a sterile neutrino with a mass splitting of about 1eV2. Such oscillations would drive the disappearance of muon neutrinos in the Booster Neutrino Beam between the detectors of the SBN Program. We present progress on an analysis to search for muon neutrino...
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Katherine Dugas (University of California, Irvine)Reactor NeutrinosPoster
High-energy cosmic rays enter Earth's atmosphere where they interact with atmospheric particles to generate charged mesons that subsequently decay into muons. As the atmosphere warms, the density decreases, increasing the mean free path of pions and kaons and therefore the probability that they decay into cosmic ray muons before undergoing a secondary interaction. This leads to a measurable...
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Estela A. Garcés (FES-C UNAM)Reactor NeutrinosPoster
Coherent elastic neutrino–nucleus scattering (CEνNS) provides a sensitive probe of neutrino electromagnetic properties thanks to its enhancement at low momentum transfer. Reactor antineutrinos, with typical energies of a few MeV, are particularly well suited to explore electromagnetic contributions that grow at low nuclear recoil energies.
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In this work, we present a phenomenological study of... -
Dr Prabhjot Singh (Louisiana State University)1Accelerator NeutrinosPoster
SBND is a liquid argon time projection chamber in Fermilab’s Short-Baseline Neutrino Program, located 110 m from the neutrino source and operating in a high-rate environment with unprecedented statistics. Charged particles from neutrino interactions ionize the argon, and the resulting electrons drift to the anode wires, inducing current signals recorded as raw waveforms. These waveforms are a...
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Cecile Nathalie Jollet (Centre National de la Recherche Scientifique (FR))Reactor NeutrinosPoster
JUNO is a multi-purpose experiment with a broad physics program that requires a precise understanding of the detector’s response. Simulation software plays a crucial role in the JUNO experiment, offering a flexible and consistent framework for conducting simulation studies across its diverse physics goals.
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The simulation includes detailed descriptions of all detector components, electronics,... -
Xiaojie LUO (The Institute of High Energy Physics of the Chinese Academy of Sciences)Neutrino OscillationsPoster
We present a standalone measurement of afterpulses in the 20-inch photomultiplier tubes (PMTs) used in the Jiangmen Underground Neutrino Observatory (JUNO) experiment. A dedicated afterpulse test setup was constructed, in which intense external light pulses were injected into the PMTs. The afterpulse time distributions were obtained by recording subsequent hits following the primary signals...
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Mr Huayu Dai (The Chinese University of Hong Kong, Shenzhen)1Reactor NeutrinosPoster
Coherent Elastic Neutrino-Nucleus Scattering (CEvNS) is a well-understood Standard Model (SM) process with an enhanced cross section for MeV neutrinos, making it a sensitive probe to beyond-SM physics. A deviation from the prediction indicates beyond-SM physics, such as non-standard interactions, while agreement would further increase our confidence in the SM. The large cross-section also...
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Doug Pinckney (Massachusetts Institute of Technology)Reactor NeutrinosPoster
The RICOCHET experiment aims to perform a precision measurement of coherent elastic neutrino-nucleus scattering (CE$\nu$NS) at the Institut Laue-Langevin (ILL) research nuclear reactor. While the ILL reactor provides a 4 order of magnitude larger antineutrino flux relative to spallation sources such as the SNS, these antineutrinos are more challenging to detect due to their 10x lower energy. ...
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Miroslav Macko (Polish Academy of Sciences (PL))Neutrinoless Double Beta DecayPoster
SuperNEMO is searching for the hypothesised lepton-number-violating process, neutrinoless double-beta decay (0νββ). Extending NEMO-3’s world-leading design, our isotope-agnostic tracker-calorimeter architecture has the unique ability to track trajectories and energies of individual particles. This is a vital background-rejection tool, and enables detailed studies of the Standard Model...
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Yushi Yoshioka (Nagoya University)Sterile NeutrinosPoster
This poster reports the current status of the sterile neutrino search in the Super-Kamiokande experiment using atmospheric neutrinos.
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A comprehensive sterile neutrino search framework has been developed based on nuSQuIDS, extending the existing Super-Kamiokande oscillation analysis to incorporate sterile neutrino scenarios. This framework enables a simultaneous scan over the full set of... -
Rogan Clark (UCLouvain)1Sterile NeutrinosPoster
Various results across several neutrino experiments, originating with the LSND and MiniBooNE anomalies, and explored recently with MicroBooNE and KATRIN publications, indicate a tension between the standard 3 neutrino oscillation model, and a 3+1 model including an additional ~1eV2 mass scale sterile neutrino. Atmospheric neutrino experiments, which measure in the GeV energy regime, are...
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Sakiko Nishimori (KEK High Energy Accelerator Research Organization (JP))Accelerator NeutrinosPoster
Reliable estimation of accelerator neutrino beam fluxes is essential for precise neutrino oscillation measurements, particularly in searches for CP violation in the leptonic sector. In long-baseline neutrino experiments, uncertainties in the neutrino flux represent one of the dominant contributions to the total uncertainty on oscillation parameters. The largest component of the flux...
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Andrea Barros (Universidad del Atlantico), Dr Mario A Acero (Universidad del Atlantico)Neutrino OscillationsPoster
NOvA is a long-baseline accelerator neutrino experiment with sensitivity to effects beyond the standard three-flavor oscillation framework. In this work, we study invisible neutrino decay within neutrino oscillations in the context of the NOvA experiment and its impact on measurement of the standard three-flavour parameters. Neutrino decay has been implemented in the oscillation probability...
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Zachary Larsen (University of California, Berkeley)New Technologies for Neutrino PhysicsPoster
Optical liquid detectors have been the workhorse of neutrino physics for decades and continue to play a leading role. Despite the relative simplicity of their detector technologies, they have significant room to improve or expand their capabilities, from making simultaneous use of Cherenkov and scintillation light to the loading of various isotopes that enable studies of rare decays or...
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Lawson Michael Mccoy (University of California Irvine (US))Accelerator NeutrinosPoster
The ForwArd Search ExpeRiment is an experiment located at CERN on the LHC downstream of the ATLAS detector. FASER is positioned behind 480 meters of rock and cement and collision line of sight axis, making it well suited for detecting feebly interacting neutral particles in the forward region such as the neutrino. FASER has published several results measuring the neutrino Charged-Current (CC)...
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Mingyu LiNew Technologies for Neutrino PhysicsPoster
The RICOCHET experiment at the Institut Laue–Langevin (ILL) in Grenoble, France,
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is a neutrino observatory targeting low-energy reactor antineutrinos (<10 MeV) via
nuclear recoils. Exploiting the coherent enhancement of the cross section, RICOCHET
opens a low-energy sensitivity frontier that enables searches for physics beyond the
Standard Model with modest exposure. RICOCHET has been... -
Prof. Wouter Van De Pontseele (Colorado School of Mines)Neutrino MassPoster
The Project 8 collaboration aims to measure the absolute neutrino mass using Cyclotron Radiation Emission Spectroscopy (CRES). While early phases successfully demonstrated CRES at ~27 GHz using small-scale waveguide-based detectors, the experiment is transitioning to large-volume resonant cavities to achieve the necessary sensitivity and statistics. This design shift necessitates a strong...
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Tristan Schefke (Louisiana State University (US))Neutrino OscillationsPoster
T2K is a long-baseline experiment for the measurement of neutrino and antineutrino oscillations. (Anti)neutrinos are produced by the J-PARC accelerator and measured at the ND280 near detector, and then at the Super-Kamiokande far-detector, in Kamioka. The most recent results of neutrino oscillations will be presented, featuring world-leading sensitivities on the search of Charge-Parity...
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Jingyu ZhuReactor NeutrinosPoster
The JUNO Collaboration has recently released its first reactor antineutrino oscillation result, achieving unprecedented precision in the measurement of \Delta m^2_{21} and \sin^2\theta_{12}. We emphasize that the accurate determination and modeling of the terrestrial matter density profile are fundamental for extracting the oscillation parameters and probing the neutrino mass ordering. This...
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mingi choe (KyungPook National University, Rebublic of Korea)Accelerator NeutrinosPoster
A CsI Detector for Coherent Elastic Neutrino-Nucleus Scattering (CICENNS) experiment is under preparation for a high-precision CEvNS research using neutrinos produced by the China Spallation Neutron Source (CSNS). Utilizing a total of 300kg CsI(Na) crystal scintillator, it aims to deliver precisely measured CEvNS cross-section and explore new physics beyond the Standard Model.
To manage...
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Yuyi Wang (Tsinghua University)New Technologies for Neutrino PhysicsPoster
Photomultiplier tubes (PMTs) are widely deployed at neutrino experiments for photon counting. When multiple photons hit a PMT consecutively, their photoelectron (PE) pulses pile up, hindering precise counting and timing measurements. We introduce Fast Stochastic Matching Pursuit (FSMP) to analyze PMT signal waveforms into individual PEs using a reversible-jump Markov-chain Monte Carlo...
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Diana Parno (Carnegie Mellon University)Neutrino MassPoster
After six years of successful operations, the Karlsruhe Tritium Neutrino (KATRIN) experiment has concluded its first phase of endpoint measurements of the tritium beta spectrum. Combining an intense windowless, gaseous tritium source with a precise integrating energy filter, KATRIN has set the world’s best direct limit on the absolute mass scale of the neutrino: $m_\beta < 0.45~eV$ (90% C.L.),...
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Ibukun Olusola (Virginia Tech)1Reactor NeutrinosPoster
MAD-CHANDLER 650 is a highly segmented anti-neutrino detector composed
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of plastic scintillating cubes. Building on the demonstrated performance of
the MiniCHANDLER prototype, MAD-C-650 implements an expanded target
volume, improved optical isolation to enable efficient detection of reactor antineutrinos
at short baselines.
This poster will present the detectors design, subsystem... -
Natalie Jones (Duke University)Accelerator NeutrinosPoster
COHERENT studies low-energy neutrino-nucleus interactions on various target nuclei. Charged-current interactions occur on high-Z shielding materials and produce a sizable background. Detector subsystems use lead shielding, and so measuring this background rate is of great importance. A 2021 measurement gave an interaction rate less than one third times the simulated prediction. One possible...
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Loic-René LABITReactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is broad-scope neutrino experiment located China. The main goal of the experiment is to determine the neutrino mass ordering through the oscillation pattern of reactor antineutrinos. The muon tracker referred to as Top Tracker (TT) is part of JUNO's veto system. The Top Tracker is key to track the muons crossing the Central Detector (CD),...
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Mariya Mollova (APC-Paris)New Technologies for Neutrino PhysicsPoster
The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino experiment designed to address the fundamental open questions in neutrino physics. Its Far Detector, located 1300 km from the neutrino source and 1.5 km underground, will comprise four massive liquid argon time projection chamber (LArTPC) modules, one of which will be equipped with the Vertical Drift...
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Jacob Zettlemoyer (Indiana University)New Technologies for Neutrino PhysicsPoster
The discovery of coherent elastic neutrino nucleus scattering (CEvNS) has brought about a rich physics program after it was first detected almost a decade ago by the COHERENT collaboration. The sole observable for a CEvNS interaction is a very rare low-energy nuclear recoil, requiring both an intense neutrino source and a low detection threshold. An additional pathway towards CEvNS detection...
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Jingbo Wang (South Dakota School of Mines and Technology)Accelerator NeutrinosPoster
The Accelerator Neutrino Neutron Interaction Experiment (ANNIE) is a 26-ton gadolinium-doped water Cherenkov detector operating on the Booster Neutrino Beam at Fermilab. The experiment's primary physics program is to measure the neutrino–nucleus interactions in water at the ~1 GeV energy scale, with a focus on neutrino-induced neutron production and interaction cross sections. Current analyses...
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Tao Hu (IHEP,China)1Reactor NeutrinosPoster
The Jiangmen Underground Neutrino Observatory (JUNO) is a multi-purpose experiment located in southern China, whose primary goal is to determine the neutrino mass ordering and perform precision measurements of the neutrino oscillation parameters. The experiment's central detector is a 35.4 m diameter acrylic sphere filled with 20-kt liquid scintillator (LS). The LS is composed of LAB solvent...
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Daniel Kodroff (Lawrence Berkeley National Lab)New Technologies for Neutrino PhysicsPoster
The Quantum Invisible Particle Search (QuIPS) experiment aims to detect sterile neutrinos in the keV-to-few-MeV mass range through weak nuclear decays. Our innovative detector system combines a nanometer-scale silica sphere in an optomechanical laser trap with active-pixel and scintillating detectors to achieve full kinematic reconstruction of beta decays. Nanospheres loaded with radioisotopes...
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Clarke Hardy (Yale University)New Technologies for Neutrino PhysicsPoster
The Quantum Invisible Particle Search (QuIPS) collaboration is developing a search for keV-MeV scale sterile neutrinos utilizing nanometer-scale silica spheres trapped at the focus of a laser in high vacuum. Such levitated optomechanical systems have opened up new pathways for testing fundamental physics with quantum-limited sensitivity, due to their extreme isolation from the surrounding...
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Jane O'Reilly (Duke University)Accelerator NeutrinosPoster
The COHERENT collaboration is deploying a tonne-scale sodium-iodide (NaI) detector, dubbed the NaI neutrino experiment at the Tonne scale (NaIvETe), at the Spallation Neutron Source at Oak Ridge National Laboratory. COHERENT has deployed a suite of neutrino detectors to measure low-energy neutrino-nucleus interactions on various target nuclei. With the deployment of NaIvETe, we plan to measure...
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Daeun Jung (Sungkyunkwan University), Dr Ji-Young CHOI (Seoyeong University), Jubin Park (Soongsil University and OMEG institute), Dr Sang Yong KIM (Chonnam National University), SunWoo GwonSterile NeutrinosPoster
The Reactor Experiment for Neutrinos and Exotics (RENE) aims to search for sterile neutrinos in the Δm²≈2 eV² region, motivated by the Reactor Antineutrino Anomaly. The detector consists of a cylindrical target volume filled with 270 liters of Gd-loaded liquid scintillator (Gd-LS), and a surrounding box-shaped gamma catcher with approximately 3,000 liters of liquid scintillator (LS). The...
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Benjamin Randolph Smithers (TRIUMF (CA))Accelerator NeutrinosPoster
The Water Cherenkov Test Experiment (WCTE) was a 30-ton water Cherenkov detector built in the CERN East Area T9 beam line to receive a flux of electrons, muons, charged pions, and protons ranging in momentum from 100-1200 MeV/c. It was designed and implemented with two primary goals in mind. First, it served as a test-bed for technologies developed for the Hyper-Kamiokande and Intermediate...
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Annalea Corallo (Universita e INFN, Ferrara (IT))Accelerator NeutrinosPoster
The Short-Baseline Near Detector (SBND) is the near detector of the Short-Baseline Neutrino Program, located only 110 m away from the Booster Neutrino Beam (BNB) target at Fermilab (Illinois, USA). SBND employs key detection technologies: a 112-ton Liquid Argon Time Projection Chamber for ionization electrons, an advanced Photon Detection System (PDS) made up of photomultiplier tubes and...
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Meishu Lu (Technical University of Munich)1New Technologies for Neutrino PhysicsPoster
The first physics results from the Jiangmen Underground Neutrino Observatory (JUNO) have demonstrated the strong scientific potential of next-generation, large-scale liquid scintillator neutrino detectors. Beyond precision oscillation measurements, further advances in detector concepts are essential to enhance the sensitivity to rare-event searches in possible future upgrades of the JUNO...
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Benedetta Corcione (Sapienza Università di Roma)New Technologies for Neutrino PhysicsPoster
Transition-edge sensors (TESs) are thin superconducting films operated close to their critical temperature, which have been employed as micro-calorimeters with excellent intrinsic energy resolution in the detection of single photons. Recent works have explored their potential for the detection of single electrons. This research could be highly valuable for the PTOLEMY collaboration, which...
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Zhihao Xu (Tohoku University)1GeoneutrinosPoster
Geophysical studies indicate that the Earth’s interior is highly heterogeneous, containing large-scale structures. One of the most prominent features is the Large Low Shear Velocity Provinces (LLSVPs), imaged by seismic tomography as regions with anomalously slow earthquake wave velocities relative to the surrounding mantle beneath the Pacific Ocean and Africa. The origin of these structures...
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Dr Jessie Micallef (Tufts University (and MIT))1Accelerator NeutrinosPoster
To accomplish precision measurements of neutrino oscillation, DUNE will use the world's most intense neutrino beam, expecting over 100 neutrino interactions in the near-site detector per spill. Resolving the overlapping particle signatures in the near detector will be vital for providing precision neutrino oscillation measurements in tandem with the far site’s multiple, 17-kt detectors. The...
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Leon Tong (University of Minnesota, Twin Cities)Accelerator NeutrinosPoster
The NOvA Transformer Energy Estimator (Transformer_EE) is a universal machine learning tool currently used to infer the incoming beam neutrino energy and the outgoing lepton energy in both near and far detectors. It uses a unique, highly flexible framework for simultaneous multivariate prediction that supports many possible loss functions. A spectral reweighting and flattening scheme lessens...
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Gabor Galgoczi (BNL)New Technologies for Neutrino PhysicsPoster
Optical photon tracking in Geant4 is a major computational bottleneck for simulating Liquid Argon (LAr) detectors, where scintillation light is central to event reconstruction and triggering. The cost of traditional CPU-based optical simulation severely limits the production of high-statistics samples needed for training deep learning models and developing AI/ML-based reconstruction...
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Michael Leyton (CERN)GeoneutrinosPoster
Radioactive decays are responsible for approximately 40% of the Earth’s total heat flow. The geo-neutrinos produced by these decays provide important clues about the origin, formation and thermal evolution of our planet, as well as the composition of its interior. Since existing measurements of geo-neutrinos are all non-directional, they do not provide model-independent information about the...
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Alexandra Moor (University of Sheffield (GB))Neutrino OscillationsPoster
The Deep Underground Neutrino Experiment (DUNE) is an upcoming next generation long baseline neutrino oscillation experiment that is expected to start taking data in the late 2020s. Consequently, a significant portion of the current work revolves around modelling, prototyping, and other forms of preparation, much of it using Monte-Carlo simulation before a full-scale dataset has been produced....
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Yashwanth Bezawada (UC Berkeley)New Technologies for Neutrino PhysicsPoster
Future kilotonne-scale, scintillation-based neutrino detectors, such as Theia, plan to exploit new and yet to be developed technologies to simultaneously measure Cherenkov and scintillation signals in order to provide a rich and broad physics program. These hybrid detectors will be based on fast timing photodetectors, novel liquid scintillators, and spectral sorting. This poster focuses on a...
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Olivia Dalager (Fermilab)New Technologies for Neutrino PhysicsPoster
The Short-Baseline Near Detector (SBND) is a liquid argon time projection chamber for detecting neutrinos from Fermilab's Booster Neutrino Beam. Located 110 m downstream of the beam target, SBND collects both ionization electrons and scintillation photons from particle interactions within the detector volume. The photon detection system (PDS) consists of both PMTs and X-ARAPUCAs, a novel...
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