-
24/10/2022, 10:00
-
Prof. JONGHEE YOO (Seoul National University), Prof. Un Ki Yang (Seoul National University (KR))24/10/2022, 10:10
-
Prof. Teppei Katori (King's College London)24/10/2022, 10:20
-
Kevin McFarland (University of Rochester), Tejin Cai (York University), Tejin Cai24/10/2022, 11:20
-
Xin Qian (Brookhaven National Laboratory), Xin Qian (Brookhaven National Laboratory (US))24/10/2022, 11:45
The MicroBooNE liquid argon time projection chamber (LArTPC) experiment operated in the Fermilab Booster Neutrino and Neutrinos at the Main Injector beams from 2015-2021. Among the major physics goals of the experiment is a detailed investigation of neutrino-nucleus interactions. MicroBooNE currently possesses the world's largest neutrino-argon scattering data set, and more than 30 ongoing...
Go to contribution page -
Cesar Jesus Valls (IFAE-BIST), César Jesús-Valls (IFAE)24/10/2022, 12:10
A detailed understanding of neutrino-nucleus interactions is essential for the precise measurement of neutrino oscillations at long baseline experiments, such as T2K. The T2K near detector complex, designed to constrain the T2K flux and cross section models, also provides a complementary program of neutrino interaction cross-section measurements. Through the use of multiple target materials...
Go to contribution page -
Amy Filkins24/10/2022, 14:00
In an era of precision neutrino oscillation experiments using improved technology that generate large statistical samples, it is important to understand the properties of neutrino interactions on nuclei over a large volume of kinematic phase space. The MINERvA experiment, which utilizes the NuMI neutrino beam at Fermilab, measures cross sections across multiple materials ranging from helium to...
Go to contribution page -
Derek Doyle (Colorado State University)24/10/2022, 14:25
NOvA is a long-baseline neutrino oscillation experiment designed to measure the $\nu_\mu\rightarrow\nu_e$ and $\bar\nu_\mu\rightarrow\bar\nu_e$ oscillation rates for subsequent extraction of the oscillation parameters of the 3-flavor PMNS model. The NOvA detectors are exposed to Fermilab's NuMI beam, the most powerful accelerator-based neutrino beam in the world. In addition to producing...
Go to contribution page -
Prof. Un-Ki Yang (Seoul National University (KR))24/10/2022, 14:45
-
Dr Jorge Morfin (Fermilab)24/10/2022, 15:05
-
Dr Yu Seon Jeong (Chung-Ang University)24/10/2022, 16:10
Neutrino experiments at the LHC such as FASER$\nu$, SND@LHC and potentially the FPF will detect neutrinos at the energy range of a few GeV to a few TeV. In neutrino scattering, there is a transition region from the so-called shallow inelastic scattering (SIS) to deep inelastic scattering (DIS). Although the boundary of the SIS and DIS is not clearly defined, the SIS region is generally...
Go to contribution page -
Oleksandr Tomalak24/10/2022, 16:30
We consider charged-current neutrino scattering on individual nucleons. Exploiting effective field theory, we factorize neutrino-nucleon cross sections into soft, collinear, and hard contributions. We evaluate soft and collinear functions from QED, provide a model for the hard contribution with expected infrared and collinear behavior and specify corresponding uncertainties. We present results...
Go to contribution page -
Prof. Raul Gonzalez Jimenez (Complutense University of Madrid)24/10/2022, 16:50
Within the framework of a relativisitic mean-field approach, I will discuss some relevant nuclear effects that affect neutrino-nucleus cross sections at the energies of interest for neutrino-oscillation experiments, such as Pauli blocking, binding energies and hadron final state interactions. I will stress the differences between this relativistic and quantum mechanical approach and the models...
Go to contribution page -
Akihiro Minamino (Yokohama National University)24/10/2022, 17:15
The NINJA experiment aims to study neutrino-nucleus interactions in the 1 GeV energy region with a nuclear emulsion-based detector. The nuclear emulsion is suitable for measuring the positions and angles of charged particles from neutrino interactions since it has a sub-µm spatial resolution. The sub-micron spatial resolution of the emulsion detector allows us to detect short tracks of...
Go to contribution page -
Noah Steinberg (Fermi National Accelerator Laboratory)25/10/2022, 09:00
The ability of current and next generation accelerator based neutrino oscillation measurements to reach their desired sensitivity and provide new insight into the nature of our Universe, requires a high-level of understanding of the neutrino-nucleus interactions. These include precise estimation of the relevant cross sections and the reconstruction of the incident neutrino energy from the...
Go to contribution page -
Camillo Mariani (Virginia Poly. Inst. & State Univ. (US))25/10/2022, 09:30
In this talk I will present the recent results on inclusive and exclusive electron scattering cross section measurements on Ar at Jefferson Lab Hall A. I will describe how this experiment will inform the future neutrino oscillation experiment like DUNE and I will describe how the electron scattering data can be used to determine accurate nuclear model that describes neutrino-nucleus...
Go to contribution page -
Arie Bodek (University of Rochester (US))25/10/2022, 10:00
Reliable modeling of quasielastic (QE) lepton scattering on nuclei is of great interest to neutrino oscillations experiments, especially at low values of the 3-momentum transfer $\bf \vec q$. We report on a phenomenological fit to all available electron scattering data on $\rm ^{12}_6C$ (about 8000 differential cross section measurements) and $\rm ^{12}_OC$ (about 250 measurements) within...
Go to contribution page -
Laura Munteanu (CERN)25/10/2022, 10:50
The Deep Underground Neutrino Experiment (DUNE) is a next generation experiment aiming to answer a wide range of open questions in neutrino physics. Its broad program includes a long-baseline (LBL) neutrino oscillation analysis, whose goal is to measure neutrino oscillation parameters with unprecedented precision. The intense beam exposure, coupled with the size of the near and far detectors...
Go to contribution page -
77. Modelling neutrino-nucleus interactions for the T2K experiment (rescheduled on Thursday morning)Dr Stephen Dolan (CERN)25/10/2022, 11:15
In order to achieve the ambitious goal of characterising neutrino flavour oscillations with percent-level precision, it is critical for current and future long-baseline neutrino oscillation experiments to substantially reduce existing systematic uncertainties. The most challenging of such systematic uncertainties is related with the modelling few-GeV neutrino-nucleus interactions.
To...
Go to contribution page -
Clarence Wret (University of Rochester (US))25/10/2022, 11:40
T2K is a world-leading long baseline neutrino oscillation experiment in Japan, studying the appearance of electron neutrinos and the disappearance of muon neutrinos in a muon neutrino beam, using both neutrinos and anti-neutrinos. With these four channels, T2K provides measurements of one neutrino mass splitting, two neutrino mixing angles, and the CP violating phase in the PMNS paradigm. T2K...
Go to contribution page -
Christophe Bronner25/10/2022, 12:05
The NEUT interaction generator is used by the T2K, Super-Kamiokande and Hyper-Kamiokande to simulate the interaction of neutrinos in the their Monte-Carlo simulations produced to study neutrino oscillations or measure cross-sections. The generator uses a number of different models for the different types of interactions, and in this presentation we will focus on the 2 models related to...
Go to contribution page -
Yoshikazu Nagai (Eötvös Loránd University (HU))25/10/2022, 14:00Talk
In current measurements of accelerator-based neutrino experiments, neutrino flux uncertainties represent a leading systematic uncertainty. Neutrino beams are created from the decays of secondary hadrons produced in hadron-nucleus interactions. Primary and secondary hadron production processes for neutrino beams are the leading source of flux uncertainty. Therefore, precise hadron production...
Go to contribution page -
Teresa Lackey (Fermilab)25/10/2022, 14:30Talk
One of the leading sources of systematic uncertainty in neutrino experiments is the modeling of the neutrino flux. Neutrino flux uncertainties are dominated by hadron scattering and hadron production cross section uncertainties, and new, dedicated measurements are needed. The EMPHATIC collaboration aims to measure the forward-scattering and production of hadrons for a variety of beam momenta...
Go to contribution page -
Prof. Andrea Longhin (Universita e INFN, Padova (IT))25/10/2022, 14:50Talk
The main source of systematic uncertainty on neutrino cross section measurements at the GeV scale is represented by the poor knowledge of the initial flux. The goal of cutting down this uncertainty to 1% can be achieved through the monitoring of charged leptons produced in association with neutrinos, by properly instrumenting the decay region of a conventional narrow-band neutrino beam. Large...
Go to contribution page -
Callum David Wilkinson (Lawrence Berkeley National Lab. (US))25/10/2022, 15:10Talk
The low-nu method has been discussed as a "standard candle" in the context of accelerator neutrino beam experiments which require a precise understanding of the neutrino flux. The method utilizes a sub-sample of events where there is low energy-transfer to the nucleus, and requires that the interaction cross section is approximately constant for this sub-sample as a function of neutrino...
Go to contribution page -
Anezka Klustova25/10/2022, 15:30Talk
High-intensity neutrino beams are an essential tool to study neutrino physics. Both neutrino oscillation experiments and cross-section measurements require a precise prediction of the neutrino flux. MINERvA is a dedicated on-axis high-statistics neutrino-nucleus scattering experiment in the NuMI beamline at Fermilab with an intensive campaign to study the neutrino flux. We performed several...
Go to contribution page -
Marco Roda (University of Liverpool (GB))25/10/2022, 16:20
-
Dr Luke Pickering (Royal Holloway, University of London)25/10/2022, 16:50
-
Dr Clarence Wret (University of Rochester (US))25/10/2022, 17:20
-
Prof. Inkyu Park (University of Seoul, Department of Physics (KR))25/10/2022, 20:00
-
Deborah Appel Harris (York University (CA))26/10/2022, 09:00
This talk will cover two different analyses of muon neutrino charged current interactions on a CH target, as recorded by MINERvA in the NuMI Medium Energy beam. The first analysis focuses on the 0-pion data set which has the advantage that the recoil energy in this set is dominated by the sum of the kinetic energies of the protons that are ejected from the target nucleus. Because of the...
Go to contribution page -
Andrew Olivier26/10/2022, 09:25
Quasi-elastic (QE) interactions are important to model well because they are a large component of the total antineutrino cross section at low momentum transfer and a great way to reconstruct antineutrino energy in principle. In practice, final state interactions (FSI) on heavy nuclei complicate selecting QE interactions, and neutron production by antineutrino QE interactions complicates...
Go to contribution page -
Dr Jeffrey Kleykamp (University of Mississippi), Prof. Steven Manly (University of Rochester)26/10/2022, 09:45
The MINERvA experiment at Fermilab presents results from several analyses of quasielastic-like (QE-like) $\nu_{\mu}$ interactions on a variety of nuclear targets in the NuMI neutrino beams. In the low energy ($<$E$_{\nu}>\sim$3 GeV) beam, components of the muon-proton momentum imbalance, \tkidptx ~and \tkidpty, are used to probe Fermi motion, binding energy, and non-QE contributions in...
Go to contribution page -
Dr Caspar Maria Schloesser (Universite de Geneve (CH))26/10/2022, 10:10
T2K is a long baseline neutrino oscillation experiment, located in Japan. A muon (anti)neutrino beam peaked at 600 MeV is produced in the J-PARC facility and measured by near detectors and the Super-Kamiokande far detector. The main goal is to measure the neutrino oscillation parameters. T2K can run in both neutrino and antineutrino mode, enhancing the sensitivity to charge-parity violation...
Go to contribution page -
London Cooper-Troendle26/10/2022, 10:30
One of the main physics goals of the MicroBooNE experiment at Fermilab is to perform high-statistics measurements of neutrino-argon interaction cross sections. These measurements will be essential for future neutrino oscillation experiments, including the Short-Baseline Neutrino program and the Deep Underground Neutrino Experiment, to achieve an unprecedented level of precision. Inclusive...
Go to contribution page -
Afroditi Papadopoulou26/10/2022, 10:50
Making high-precision measurements of neutrino oscillation parameters requires an unprecedented understanding of neutrino-nucleus scattering. In this work, we present the progress towards the first charged current double-differential cross sections in kinematic imbalance variables. These variables characterize the imbalance in the plane transverse to an incoming neutrino. We use events with a...
Go to contribution page -
Julia Tena vidal26/10/2022, 11:30
This talk presents the latest GENIE tuning of CC0$\pi$ datasets from MiniBooNE, T2K and MINERvA. A partial tune for each experiment is performed, providing a common base for the discussion of tensions between datasets. The results offer an improved description of nuclear CC0$\pi$ datasets as well as data-driven uncertainties for each experiment. This work is a step towards a GENIE global tune...
Go to contribution page -
Aaron Meyer (University of California Berkeley)26/10/2022, 11:50
Next generation neutrino oscillation experiments are poised to provide answers to key questions about the nature of the neutrino. The axial form factor is a vital ingredient in the nucleon amplitudes used to predict quasielastic scattering, a primary signal measurement process for flagship neutrino oscillation experiments, yet the uncertainty on this form factor is vastly underestimated by the...
Go to contribution page -
Noah Steinberg (Fermi National Accelerator Laboratory)26/10/2022, 12:10
The next generation of neutrino oscillation experiments require precise predictions of neutrino-nucleus cross sections as well as control over their uncertainties, including the contribution of model dependence to the overall error budget. To this end we compare two methods of computing $CC0\pi$ flux folded cross sections; an ab-initio method based on Greens Function Monte Carlo, and a Quantum...
Go to contribution page -
Callum David Wilkinson (Lawrence Berkeley National Lab. (US)), Deborah Appel Harris (York University (CA)), Kevin Scott Mc Farland-Porter (University of Rochester (US)), Prof. Xin Qian (Brookhaven National Laboratory (US))26/10/2022, 14:00
-
Andrzej Michal Szelc (University of Edinburgh)26/10/2022, 14:30
Measurements of neutrino-nucleus interactions provide an important benchmark for the theoretical models needed to perform precision neutrino oscillation analyses. An understanding of electron neutrino scattering is crucial for determination of charge parity (CP) violation in the leptonic sector. Potential mismodeling of these interactions can limit the sensitivity of forthcoming experiments...
Go to contribution page -
Dr Michael Hudson Kirby (Fermi National Accelerator Lab. (US)), Michael Kirby (Fermi National Accelerator Laboratory)26/10/2022, 14:50
The MicroBooNE detector is the world's longest-running liquid argon time projection chamber (LArTPC) and recently completed operating in the Fermilab Booster Neutrino Beam. One of the primary physics goals of MicroBooNE is to perform detailed studies of neutrino-argon scattering cross sections, which are critical for the success of future neutrino oscillation experiments. At neutrino energies...
Go to contribution page -
Prof. Omar Benhar (INFN, Roma)26/10/2022, 15:10
Recent results showing that lattice calculations provide a remarkably good description of the measured vector form factors of the nucleon indicate that this approach has reached a high level of reliability. I will report the results of calculations of the cross section of the process 12C(νμ,μ- p) averaged over the neutrino fluxes of the MiniBooNE and T2K experiments. The analysis has been...
Go to contribution page -
Andrew Olivier26/10/2022, 15:30Poster
Neutron production by antineutrino interactions is an important source of uncertainty for long baseline oscillation experiments. Neutrons are a source of missing energy for calorimetry-based oscillation experiments, and an extra neutron from an antineutrino CCQE-like interaction can be evidence of a 2p2h interaction. Both problems bias oscillation measurements' energy estimators, yet few...
Go to contribution page -
Anezka Klustova26/10/2022, 15:35Poster
The MINER$\nu$A experiment was designed to perform precision studies of neutrino-nucleus scattering in the GeV regime on various nuclear targets using the high-intensity NuMI beam at Fermilab. This poster outlines the current progress on MINER$\nu$A’s first inclusive charged-current analysis of antineutrino interactions on iron, lead, and water using antineutrino energy and Bjorken $x$. The...
Go to contribution page -
Sang Yong KIM (Seoul National University)26/10/2022, 15:40Poster
The RENO Collaboration reports a measured value of the smallest neutrino mixing angle (θ13) based on ~2900 days of reactor electron antineutrino events with a delayed signal of neutron capture on hydrogen (H). The neutron captures on H emitting a 2.2 MeV γ-ray are not easily detected because of high environmental radioactivity below 3.5 MeV, Due to satisfactory purification of liquid...
Go to contribution page -
Wonjun Lee26/10/2022, 15:45Poster
We report a conceptual design of the nearest neutrino detector, which primarily aims to search for the sterile neutrino oscillation at $\Delta m_{41}^2 \sim 2 eV^2$. The joint study of RENO and NEOS experiments showed a hint for the sterile neutrinos at $\Delta m_{41}^2 \sim 2.4 eV^2$ and $\sim 1.7 eV^2$, which overlap with the allowed region by the Reactor Anti-neutrino Anomaly. This Nearest...
Go to contribution page -
SunWoo Gwon26/10/2022, 15:50Poster
Neutrino oscillation experiments require a precise measurement of the neutrino energy. However, the kinematic detection of the final state neutrons in the neutrino interaction is missing in current neutrino oscillation experiments. A novel 3D projection scintillator tracker can detect the neutron kinetic energy and direction on an event-by-event basis. Through neutron detection, the neutrino...
Go to contribution page -
HW Park (Chonnam National University, Department of physics)26/10/2022, 15:55Poster
Bi-alkali photomultiplier tube (PMT) has a maximum quantum efficiency (QE) around 430nm. Fluor components dissolved in liquid scintillator (LS) are needed to have an emission wavelength in the PMT’s QE region. We analyzed digital images for estimating the spectrum of LS, instead of using a spectrophotometer. Digital image was taken by camera based on complementary metal oxide semiconductor...
Go to contribution page -
Dojin Kim26/10/2022, 16:00Poster
We report the measured reactor antineutrino spectra from the fission of $^{235}$U and $^{239}$Pu using 2,500 days of RENO near detector data. The change of fission fraction and thus reactor neutrino yield during a fuel cycle can be used to separate $^{235}$U and $^{239}$Pu contributions to the observed yields. The antineutrino spectra from the $^{235}$U and $^{239}$Pu fission are obtained from...
Go to contribution page -
Eric Vazquez-Jauregui26/10/2022, 16:30
Supernovae emit large fluxes of neutrinos which can be detected by detectors on Earth. Future tonne-scale detectors will be sensitive to several neutrino interaction channels, with thousands of events expected if a supernova emerges in the galaxy neighborhood. There are limited tools to study the interaction rates of supernova neutrinos, although a plethora of available supernova models exist....
Go to contribution page -
Makoto Sakuda (Okayama University)26/10/2022, 16:50
We first discuss and determine the isospin mixing of the two $2^-$ states (12.53 MeV and 12.97 MeV) of $^{16}$O nucleus using the inelastic electron scattering data. We then evaluate the cross section of 4.4-MeV $\gamma$ rays produced in the neutrino neutral-current (NC) reaction $^{16}$O($\nu, \nu$')$^{16}$O$(12.97 {\rm MeV}, 2^-$) with a water Cherenkov detector at the low energy below 100...
Go to contribution page -
Tsutomu Fukuda (Nagoya Univ.)26/10/2022, 17:10
NINJA experiment aims to study Sub-Multi GeV neutrino-nucleus interactions and the exploration of a sterile neutrino using an Emulsion Cloud Chamber (ECC) as the main detector at J-PARC neutrino beamline.
Go to contribution page
Thanks to sub-micron spatial resolution and high granularity of ECC, charged particles such as slow protons with a momentum of 200 MeV/c can be measured with high detection... -
Hyoungku Jeon (SungKyunKwan University)26/10/2022, 17:30
Kaon Decay-At-Rest (KDAR) provides a neutrino signal with well-known neutrino energy, which is an important probe for measuring the neutrino cross-section in an energy range that is otherwise difficult to access experimentally. The J-PARC Sterile Neutrino Search at the J-PARC Spallation Neutron Source (JSNS2) experiment is in a unique place for measuring monoenergetic neutrinos at 236 MeV from...
Go to contribution page -
Doo Jin Kim27/10/2022, 09:00
Since the first discovery of coherent elastic neutrino-nucleus scattering (CEvNS) events, a lot of experiments are operational or projected for precision measurements of CEvNS. Such experiments typically feature low energy and high intensity of particles including neutrinos, while their detectors feature low threshold and proximity to their source points. Therefore, they are expected to...
Go to contribution page -
Daniel Pershey27/10/2022, 09:20
The COHERENT collaboration made the first measurement of coherent elastic neutrino nucleus scattering (CEvNS) in 2017 using a low-background, 14.6-kg CsI[Na] detector at the Spallation Neutron Source (SNS). We have also measured CEvNS using a 24-kg argon scintillation calorimeter. These measurements are part of a multi-target campaign to measure CEvNS on four nuclei, Na, Ar, Ge, and Cs/I, to...
Go to contribution page -
Eric Vazquez-Jauregui27/10/2022, 09:45
The scintillating bubble chamber is a new technology under development ideal for coherent elastic neutrino-nucleus scattering (CE$\nu$NS) detection at reactor sites. The SBC collaboration is building a 10-kg bubble chamber using liquid argon with the potential to reach and maintain sub-keV energy thresholds. This detector will combine the event-by-event energy resolution of a liquid noble...
Go to contribution page -
Rex Tayloe (Indiana University), Rex Tayloe (Indiana U.)27/10/2022, 10:05
Neutrino interactions with a ton-scale liquid argon detector for the COHERENT experiment
The COHERENT collaboration operates an array of detectors at the ORNL Spallation Neutron Source (SNS) to measure coherent elastic neutrino nucleus scattering (CEvNS), low-energy inelastic neutrino interactions, and to search for dark matter. We observed the first CEvNS events in 2017 with a...
Go to contribution page -
Dr InSoo Lee (IBS)27/10/2022, 10:25
Coherent elastic neutrino-nucleus scattering (CEvNS) can provide interesting physics such as measuring neutrino properties and proving non-standard interactions.
Go to contribution page
Neutrino Elastic-scattering Observation with NaI(Tl) experiment (NEON) aims to detect this CEvNS in a NaI(Tl) crystal using reactor anti-electron neutrino at Hanbit nuclear power plant.
NEON detector consists of a total of 16 kg... -
Dr Stephen Dolan (CERN)27/10/2022, 10:40
In order to achieve the ambitious goal of characterising neutrino flavour oscillations with percent-level precision, it is critical for current and future long-baseline neutrino oscillation experiments to substantially reduce existing systematic uncertainties. The most challenging of such systematic uncertainties is related with the modelling few-GeV neutrino-nucleus interactions.
To...
Go to contribution page -
Minoo Kabirnezhad (Imperial College London)28/10/2022, 09:00
I have developed a single pion production model in neutrino-nucleon interaction:
Go to contribution page
https://inspirehep.net/literature/1634864 .
Then I used electron scattering data to extract the nucleon form factors:
https://inspirehep.net/literature/1802724 ,
and recently I extended the model to the transition region between resonance and Deep Inelastic regions (high momentum transfer, Q^2, and hadron... -
Rob Fine (Los Alamos National Laboratory), Rob Fine (Los Alamos National Laboratory)28/10/2022, 09:25
MicroBooNE is a 100-ton-scale liquid argon TPC that ran in the Fermilab Booster Neutrino Beam from 2015-2021. MicroBooNE has recorded hundreds of thousands of neutrino interactions, many of which include pions in the final state. In particular, neutral pions are a key background to any search for low-energy electron neutrinos and sub-GeV signatures of physics beyond the Standard Model. Thus,...
Go to contribution page -
Matthew Judah (University of Pittsburgh (US))28/10/2022, 09:45
NOvA is a long-baseline neutrino oscillation experiment designed to measure muon (anti)neutrino disappearance and electron (anti)neutrino appearance in Fermilab's NuMI beam. It uses two functionally identical liquid scintillator detectors separated by 810km and a narrow band beam centered around $E_{\nu} = 2$ GeV. Energetic neutral pions produced in resonant, deep-inelastic, or final state...
Go to contribution page -
Danaisis Vargas Oliva (University of Toronto (CA))28/10/2022, 10:05
The long baseline neutrino experiment Tokai-to-Kamiokande (T2K), located in Japan, measures neutrino oscillation parameters. The J-PARC accelerator complex in Tokai produces a beam of neutrinos; these are detected in the near detector (ND280) and at the far detector (Super-Kamiokande). Muon neutrino charged current interactions in ND280 are used to predict the event rate at the far detector....
Go to contribution page -
Prof. Kevin McFarland (University of Rochester)28/10/2022, 10:55
The enormous flux of neutrinos the NuMI's medium energy beam enables a number of new measurements of coherent and incoherent pion production on MINERvA's scintillator and passive carbon, water, iron, and lead targets. These measurements show a number of discrepancies with current generator models, and provide information about the correct scaling of single pion production with different...
Go to contribution page -
Mr SunWoo Gwon (Chung-Ang University)28/10/2022, 11:20
Long-baseline neutrino oscillation experiments rely on detailed models of neutrino interactions on nuclei. These models constitute an important source of systematic uncertainty, in part because current detectors have been blind to final state neutrons. A novel three-dimensional projection scintillator, called SuperFGD, will be the tracker of the upgraded off-axis near detector of the T2K...
Go to contribution page -
Christopher Thorpe28/10/2022, 11:40
The MicroBooNE detector is a liquid argon time projection chamber (LArTPC) that operated in both the Booster Neutrino and the Neutrinos at the Main Injector beams at Fermilab. The LArTPC detector technology provides excellent spatial resolution and particle discrimination capabilities. From 2015 through 2021, MicroBooNE accumulated the world's largest neutrino-argon scattering data set, which...
Go to contribution page -
Supraja Balasubramanian28/10/2022, 14:00Talk
The Short-Baseline Near Detector (SBND) will be one of three Liquid Argon Time Projection Chamber (LArTPC) neutrino detectors positioned along the axis of the Booster Neutrino Beam (BNB) at Fermilab, as part of the Short-Baseline Neutrino (SBN) Program. The detector is currently in the construction phase and is anticipated to begin operation in 2023. SBND is characterized by superb imaging...
Go to contribution page -
Lauren Yates (Fermilab)28/10/2022, 14:20Talk
The Short-Baseline Near Detector (SBND) is a 100-ton scale Liquid Argon Time Projection Chamber neutrino detector positioned in the Booster Neutrino Beam at Fermilab, as part of the Short-Baseline Neutrino (SBN) program. The detector is currently under construction and is anticipated to begin operation in 2023. Located only 110 m from the neutrino production target, it will be exposed to a...
Go to contribution page -
Dr Stephen Dolan (CERN)28/10/2022, 14:40Talk
The ICARUS experiment, employing a LAr TPC, has been installed at Fermilab in Chicago, Illinois after its original run in Italy and subsequent refurbishment and is now in a stage of advanced commissioning and preparation for analyses. While a main goal of the detector is to serve as the far detector of the Short Baseline Neutrino program searching for sterile neutrino signatures, ICARUS has a...
Go to contribution page -
Laura Munteanu (CERN)28/10/2022, 15:00Talk
Neutrino oscillation physics has now entered the precision era. In parallel with needing larger detectors with which to collect more data, future experiments further require a significant reduction of systematic uncertainties with respect to what is currently available. In the neutrino oscillation measurements from the T2K experiment the systematic uncertainties related to neutrino interaction...
Go to contribution page -
Yifan Chen (SLAC National Accelerator Laboratory (US))28/10/2022, 16:00Talk
The Deep Underground Neutrino Experiment (DUNE) adopts a design of modularised LArTPC for the near detector. It is equipped with revolutionary pixelated readout which enables true 3D projection of particle passages. The pixelated readout eliminates projection ambiguity presented in wire-readout LArTPCs and is particularly suitable for busy detector environment close to the intense neutrino...
Go to contribution page -
Dr Daiki Hayakawa (Chiba University (JP))28/10/2022, 16:20Talk
FASER$\nu$ at the LHC is designed to directly detect collider neutrinos of all three flavors and provide new measurements of their cross-sections at energies higher than those detected from any previous artificial sources. In the pilot run data taken in 2018, we observed the first neutrino interaction candidates at the LHC, paving the way for studying neutrinos from high-energy colliders. In...
Go to contribution page -
Ouseph C.J. (National Tsing Hua University Taiwan)28/10/2022, 16:40Talk
FASER$\nu$ is a newly approved (working) high-energy neutrino scattering experiment using the neutrino beam from the decays of hadrons downstream from the interaction point of ATLAS and positioned at about 480 m away from the ATLAS detector. We are exploring the features of FASER$\nu$ for the Deep-Inelastic Neutrino Nucleon Neutral current scattering. We study the various BSM physics scenarios...
Go to contribution page -
Chun Sil Yoon (Department of Physics Education and RINS)28/10/2022, 17:00Talk
SND@LHC is a compact and stand-alone experiment to perform measurements with neutrinos produced at the LHC in a hitherto unexplored pseudo-rapidity region of $7.2 < \eta < 8.6$, complementary to all the other experiments at the LHC. The experiment is located 480 m downstream of IP1 in the unused TI18 tunnel. The detector is composed of a hybrid system based on an 800 kg target mass of tungsten...
Go to contribution page -
Prof. Natalie Yvonne Jachowicz (Ghent University (BE))29/10/2022, 10:00Talk
-
Dr Callum David Wilkinson (Lawrence Berkeley National Lab. (US))29/10/2022, 10:40Talk
-
Dr Jorge G. Morfin29/10/2022, 11:20Talk
-
29/10/2022, 11:30Talk
-
Travis Olson (University of Houston)
This talk presents a measurement of the double-differential cross section for inclusive, charged-current νμ-nucleus scattering in the predominantly hydrocarbon medium of the NOvA near detector. The cross section is expressed in terms of 3-momentum transfer and available hadronic energy, variables well-suited to elicit the 2-particle-2-hole (2p2h) contribution in the 1-3 GeV region of incident...
Go to contribution page -
Danaisis Vargas Oliva (University of Toronto (CA))Poster
The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino experiment under construction in the US. The experiment is formed by a broadband neutrino beam from Fermilab to the Sanford Underground Research Facility (SURF) in Lead, South Dakota, a high-precision near detector, and a large liquid argon time-project chamber (LArTPC) far detector. It has a broad...
Go to contribution page -
Mr Connor Johnson (Colorado State University), Prabhjot Singh
NOvA is a long-baseline neutrino experiment aiming to measure the neutrino oscillation parameters, especially the lepton violating phase deltaCP. The high flux received at the NOvA near detector makes the perfect environment for precision measurements of neutrino interactions. In this talk, we present our measurement and predictions of muon anti-neutrino inclusive cross section as a triple...
Go to contribution page
Choose timezone
Your profile timezone: