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CERN Document Server 2,038 records found  1 - 10nextend  jump to record: Search took 0.86 seconds. 
1.
The Hyper-K Underwater Electronics Assembly project / Hyper-Kamiokande Collaboration
Starting in 2027, the Hyper-Kamiokande experiment in Japan will search for leptonic CP violation in long-baseline accelerator neutrino oscillations with a realistic potential of discovery within 3 to 10 years from the start of the data taking depending on the value of the CP violating phase, to be measured with a resolution better than $23^{\circ}$. [...]
CERN-SPSC-2023-021 ; SPSC-I-260.
- 2023.
Fulltext
2.
Addendum to the Letter of Intent CERN-SPSC-2023-021 ; SPSC-I-260 / Hyper-Kamiokande Collaboration
In August 2023 the Letter of Intent titled ``The Hyper-K Underwater Electronics Assembly project'' (CERN-SPSC-2023-021, SPSC-I-260) was submitted. [...]
CERN-SPSC-2024-004 ; SPSC-M-796.
- 2024.
Fulltext - Original Document (SPSC-I-260)
3.
Scintillator ageing of the T2K near detectors from 2010 to 2021 / T2K Collaboration
The T2K experiment widely uses plastic scintillator as a target for neutrino interactions and an active medium for the measurement of charged particles produced in neutrino interactions at its near detector complex. Over 10 years of operation the measured light yield recorded by the scintillator based subsystems has been observed to degrade by 0.9--2.2% per year. [...]
arXiv:2207.12982.- 2022-10-17 - 35 p. - Published in : JINST 17 (2022) P10028 Fulltext: 2207.12982 - PDF; Publication - PDF;
4.
Hyper-Kamiokande / Mueller, T Ainstitute - Hyper-K.
Approved: 13 March 2023.-
Status: Preparation
External link: Experiment home page
Experiment: RE45
5.
Updated T2K measurements of muon neutrino and antineutrino disappearance using <math display="inline"><mrow><mn>3.6</mn><mo>×</mo><mrow><msup><mrow><mn>10</mn></mrow><mrow><mn>21</mn></mrow></msup></mrow></mrow></math> protons on target / T2K Collaboration
Muon neutrino and antineutrino disappearance probabilities are identical in the standard three-flavor neutrino oscillation framework, but CPT violation and non-standard interactions can violate this symmetry. In this work we report the measurements of $\sin^{2} \theta_{23}$ and $\Delta m_{32}^2$ independently for neutrinos and antineutrinos. [...]
arXiv:2305.09916.- 2023-10-01 - 10 p. - Published in : Phys. Rev. D 108 (2023) 072011 Fulltext: 2305.09916 - PDF; Publication - PDF;
6.
First measurement of muon neutrino charged-current interactions on hydrocarbon without pions in the final state using multiple detectors with correlated energy spectra at T2K / T2K Collaboration
This paper reports the first measurement of muon neutrino charged-current interactions without pions in the final state using multiple detectors with correlated energy spectra at T2K. The data was collected on hydrocarbon targets using the off-axis T2K near detector (ND280) and the on-axis T2K near detector (INGRID) with neutrino energy spectra peaked at 0.6 GeV and 1.1 GeV respectively. [...]
arXiv:2303.14228.- 2023-12-01 - 36 p. - Published in : Phys. Rev. D 108 (2023) 112009 Fulltext: PDF;
7.
Measurements of the $\nu_{\mu}$ and $\bar{\nu}_{\mu}$-induced coherent charged pion production cross cections on $^{12}C$ by the T2K experiment / T2K Collaboration
We report an updated measurement of the $\nu_{\mu}$-induced, and the first measurement of the $\bar{\nu}_{\mu}$-induced coherent charged pion production cross section on $^{12}C$ nuclei in the T2K experiment. This is measured in a restricted region of the final-state phase space for which $p_{\mu,\pi} > 0.2$ GeV, $\cos(\theta_{\mu}) > 0.8$ and $\cos(\theta_{\pi}) > 0.6$, and at a mean (anti)neutrino energy of 0.85 GeV using the T2K near detector. [...]
arXiv:2308.16606.- 2023-11-01 - 15 p. - Published in : Phys. Rev. D 108 (2023) 092009 Fulltext: 2308.16606 - PDF; Publication - PDF;
8.
A Water Cherenkov Test Beam Experiment for Hyper-Kamiokande and Future Large-scale Water-based Detectors / Barbi, M (University of Regina, Department of Physics, Regina, Saskatchewan, Canada) ; Berardi, V (INFN Sezione di Bari and Universita e Politecnico di Bari, Dipartimento Interuniversitario di Fisica, Bari, Italy) ; Bhadra, S (York University, Department of Physics and Astronomy, Toronto, Ontario, Canada) ; Boyd, S (University of Warwick, Department of Physics, Coventry, United Kingdom) ; Bubak, A (University of Silesia, Institute of Physics, Katowice, Poland) ; Buchowicz, A (Warsaw University of Technology, Institute of Radioelectronics and Multimedia Technology, Warsaw, Poland) ; Buizza Avanzini, M (Ecole Polytechnique, IN2P3-CNRS, Laboratoire Leprince-Ringuet, Palaiseau, France) ; Catanesi, MG (INFN Sezione di Bari and Universita e Politecnico di Bari, Dipartimento Interuniversitario di Fisica, Bari, Italy) ; Cederkall, J (Lund University, Department of Physics, Lund, Sweden) ; Coleman, J (University of Liverpool, Department of Physics, Liverpool, United Kingdom) et al.
Water Cherenkov and water-based particle detector technologies are used to realize multi-kiloton scale experiments such as the currently operating Super-Kamiokande experiment, the planned Hyper-Kamiokande experiment and the proposed THEIA detector and ESSnuSB detectors. [...]
CERN-SPSC-2019-042 ; SPSC-I-254.
- 2019.
Fulltext
9.
Measurement of neutrino and antineutrino neutral-current quasielastic-like interactions on oxygen by detecting nuclear de-excitation $\gamma$-rays / T2K Collaboration
Neutrino- and antineutrino-oxygen neutral-current quasielastic-like interactions are measured at Super-Kamiokande using nuclear de-excitation $\gamma$-rays to identify signal-like interactions in data from a $14.94 \ (16.35)\times 10^{20}$ protons-on-target exposure of the T2K neutrino (antineutrino) beam. The measured flux-averaged cross sections on oxygen nuclei are $\langle \sigma_{\nu {\rm -NCQE}} \rangle = 1.70 \pm 0.17 ({\rm stat.}) ^{+ {\rm 0.51}}_{- {\rm 0.38}} ({\rm syst.}) \times 10^{-38} \ {\rm cm^2/oxygen}$ with a flux-averaged energy of 0.82 GeV and $\langle \sigma_{\bar{\nu} {\rm -NCQE}} \rangle = 0.98 \pm 0.16 ({\rm stat.}) ^{+ {\rm 0.26}}_{- {\rm 0.19}} ({\rm syst.}) \times 10^{-38} \ {\rm cm^2/oxygen}$ with a flux-averaged energy of 0.68 GeV, for neutrinos and antineutrinos, respectively. [...]
arXiv:1910.09439.- 2019-12-31 - 19 p. - Published in : Phys. Rev. D 100 (2019) 112009 Article from SCOAP3: PDF; Fulltext: PDF;
10.
Measurement of the charged-current electron (anti-)neutrino inclusive cross-sections at the T2K off-axis near detector ND280 / T2K Collaboration
The electron (anti-)neutrino component of the T2K neutrino beam constitutes the largest background in the measurement of electron (anti-)neutrino appearance at the far detector. The electron neutrino scattering is measured directly with the T2K off-axis near detector, ND280. [...]
arXiv:2002.11986.- 2020-10-19 - 43 p. - Published in : JHEP 2020 (2020) 114 Article from SCOAP3: PDF; Fulltext: PDF;

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