Conveners
WG 2
- Ryan Plestid (University of Kentucky)
WG 2
- Julia Tena Vidal (University of Liverpool)
WG 2
- Kajetan Niewczas (UWR)
WG 2
- Lu Ren
WG 2
- Afroditi Papadopoulou (Massachusetts Institute of technology)
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Kajetan Niewczas (UWR)08/09/2021, 12:40Oral
NuWro is a versatile Monte Carlo neutrino event generator, applicable for simulations in the energy range of the accelerator-based neutrino oscillation experiments. Since 2005, the theoretical group of the University of Wrocław, Poland, has been extensively working on its development, successfully comparing to various neutrino cross section measurements. NuWro is a vital tool for event...
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Dr Yoshinari Hayato (University of Tokyo)08/09/2021, 12:58Oral
NEUT is a neutrino-nucleus interaction simulation program library and used for the analyses of Super-K and T2K. Recently, NEUT is also used to simulate pion interactions with the nucleus in the detector simulation. In order to make the users access various functions in NEUT, we have started a project to design
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a set of new APIs for easy access to the implemented total and interaction... -
Julia Tena Vidal (University of Liverpool)08/09/2021, 13:16Oral
The next generation of neutrino oscillation experiments rely on the precise understanding of neutrino interactions in a wide energy range. The GENIE collaboration is constantly engaged in an effort to improve interaction models and fit them against available datasets. A lot of effort is going into pion producing processes, so far focusing on the resonant component of the pion production. This...
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Dr Sebastian Pina-Otey (University of Geneva)08/09/2021, 13:34Oral
The generation of accurate neutrino-nucleus cross section models needed for neutrino oscillation experiments requires simultaneously the description of many degrees of freedom and precise calculations to model nuclear responses. The detailed calculation of complete models makes the Monte Carlo generators slow and impractical. We present exhaustive neural importance sampling, a method based on...
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Arie Bodek (University of Rochester (US))08/09/2021, 13:52Oral
We report on an update (2021) of a phenomelogical model for inelastic neutrino- and electron- nucleon scattering cross sections using effective leading order parton distribution functions with a new scaling variable ξw. Non-perturbative effects are well described using the ξw scaling variable in combination with multiplicative K factors at low Q2. The model describes all inelastic charged...
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Dr Elena Gramellini (Fermilab )08/09/2021, 14:20Oral
MicroBooNE is a liquid argon time projection chamber that operates in the Booster Neutrino Beam at Fermilab. The detector provides high-resolution imaging of neutrino interactions with a low threshold and full angular coverage. Thanks to a high event rate and several years of continuous operation, the MicroBooNE collaboration has obtained the world's largest dataset of neutrino-argon...
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Samantha Sword-Fehlberg (NMSU)08/09/2021, 14:40Oral
The MicroBooNE detector is the world's longest-running liquid argon time projection chamber (LArTPC), currently installed in the Booster Neutrino Beam at Fermilab. 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 relevant...
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Oleksandr Tomalak (University of Kentucky)08/09/2021, 15:00Oral
Charged-current quasielastic scattering is the signal process in modern neutrino oscillation experiments. It also serves as the main tool for the reconstruction of the incoming neutrino energy. Exploiting effective field theory, we factorize neutrino-nucleon quasielastic cross sections into soft, collinear, and hard contributions. We evaluate soft and collinear functions from QED and provide a...
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Dr Osamu Sato (Nagoya University)08/09/2021, 15:20Oral
The data on tau neutrino is very scarce, only a few experiments have detected its interactions. At FNAL beam dump experiment DONUT, tau neutrino interaction cross-section was directly measured with a large systematical (~50%) and statistical (~30%) errors. The main source of systematical error is due to a poor knowledge of the tau neutrino flux. The effective way for tau neutrino production is...
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Dr Noemi Rocco (Fermilab)09/09/2021, 12:40Oral
The advent of high precision measurements of neutrinos and their oscillations calls for accurate predictions of their interactions with nuclear targets utilized in the detectors.
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Achieving a comprehensive description of the different reaction mechanisms active in the broad range of energy relevant for oscillation experiments is a formidable challenge for both particle and nuclear Physics. I... -
Caspar Maria Schloesser (ETH Zurich (CH))09/09/2021, 12:58Oral
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...
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Sam Jenkins (University of Sheffield)09/09/2021, 13:16Oral
The T2K experiment is a long-baseline neutrino oscillation experiment, based in Japan, which measures the oscillation probability of muon neutrinos produced at the JPARC facility, and detected at Super-Kamiokande. A detailed understanding of neutrino-nucleus cross sections is essential to measuring neutrino oscillation parameters. The off-axis near detector ND280 is used to measure a variety...
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Dr Vishvas Pandey (University of Florida)09/09/2021, 13:34Oral
Current and future accelerator-based neutrino facilities utilizing intense neutrino beams and advanced neutrino detectors are focused on precisely determining neutrino oscillation properties and signals of weakly interacting Beyond the Standard Model (BSM) physics. These are all subtle effects, such as extracting the CP violation phase and disentangling parameter degeneracies between...
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Dr Newton Nath (Instituto de Fisica, National Autonomous University of Mexico)09/09/2021, 14:20Oral
In this talk, we will discuss the potential to prove "generalized neutrino interactions", exotic new physics interactions beyond the Standard Model, in the coherent-elastic neutrino-nucleus scattering (CE$\nu$NS) experiments in light of the latest COHERENT- CsI, and LAr data. We will discuss that how CE$\nu$ES processes could constrain these exotic new physics effective couplings, and the...
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Dimitrios Papoulias (University of Ioannina)09/09/2021, 14:38Oral
The current and next generation experiments looking for coherent elastic neutrino-nucleus scattering (CEvNS) and neutrino-electron scattering are a unique tool for exploring exotic neutrino physics via nuclear and electron recoil measurements. In this talk, I will discuss the potential of such experiments in opening new directions on rare event searches beyond the neutrino sector. In...
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Diego RG09/09/2021, 14:56Oral
In this paper, we investigate the impact of different assumptions for the description of the QCD dynamics at high energies on the
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determination of the normalization Φ and spectral index γ of the astrophysical neutrino flux. The distribution of neutrino events at the IceCube is estimated considering the DGLAP, BFKL and CGC approaches and the best estimates for Φ and γ are determined using a... -
Shunzo Kumano (KEK)09/09/2021, 15:14Oral
The structure functions $F_1$, $F_2$, and $F_3$ of the nucleon were measured by neutrino deep inelastic inelastic scattering. These structure functions are expressed by collinear parton distribution functions, which indicate longitudinal momentum distributions of partons. In recent years, 3 dimensional (3D) structure functions have been investigated extensively for clarifying the transverse...
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Eric Van Herwijnen (CERN)09/09/2021, 15:32Oral
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 < 𝜂 < 8.6, complementary to all the other experiments at the LHC. The experiment is to be 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...
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Libo Jiang (Virginia Poly. Inst. & State Univ. (US))09/09/2021, 16:00Oral
Abstract: The ProtoDUNE-SP detector is a single-phase liquid argon time projection chamber with an active volume of 7.2×6.0×6.97m^3. The ProtoDUNE-SP detector also serves as a prototype for the first far detector module of the Deep Underground Neutrino Experiment (DUNE). A charged particle beam was specifically built to deliver multiple particles including charged pions, kaons, protons, muons...
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Leonidas Aliaga Soplin (Fermilab)09/09/2021, 16:20Oral
The NOvA near detector (ND), located at Fermilab, provides an excellent opportunity to measure neutrino-nucleus interactions, which will benefit current and future neutrino experiments. The ND records a high rate of neutrino interactions with energies ranging from 1-5 GeV. In this talk, we present a measurement of the muon-neutrino charged-current inclusive cross sections as a function of the...
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Bryan Joseph Ramson (Fermi National Accelerator Lab. (US))09/09/2021, 16:40Oral
The NOvA experiment is a long-baseline neutrino experiment aiming to con- strain independent elements of the PMNS matrix. The NOvA Near Detector can also serve as a way to measure many different types of neutrino-nucleus cross sections, significantly adding to the world neutrino data and helping to improve models of neutrino scattering that are critical to oscillation measure- ments....
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Dr Huma Haider (Aligarh Muslim University )09/09/2021, 16:58Oral
The effect of nonperturbative and higher order perturbative corrections to all the free nucleon structure functions in the deep inelastic scattering (DIS) of neutrinos on nucleon/nucleus is studied. The target mass correction and higher twist effects are incorporated following the works of Kretzer et al. and Dasgupta et al., respectively. The evaluation of the nucleon structure functions has...
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