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Showing papers on "Neutrino detector published in 2021"


Journal ArticleDOI
B. Abi1, R. Acciarri2, M. A. Acero3, George Adamov4  +979 moreInstitutions (156)
TL;DR: Of the many potential beyond the Standard Model (BSM) topics DUNE will probe, this paper presents a selection of studies quantifying DUNE’s sensitivities to sterile neutrino mixing, heavy neutral leptons, non-standard interactions, CPT symmetry violation, Lorentz invariance violation, and other new physics topics that complement those at high-energy colliders and significantly extend the present reach.
Abstract: The Deep Underground Neutrino Experiment (DUNE) will be a powerful tool for a variety of physics topics. The high-intensity proton beams provide a large neutrino flux, sampled by a near detector system consisting of a combination of capable precision detectors, and by the massive far detector system located deep underground. This configuration sets up DUNE as a machine for discovery, as it enables opportunities not only to perform precision neutrino measurements that may uncover deviations from the present three-flavor mixing paradigm, but also to discover new particles and unveil new interactions and symmetries beyond those predicted in the Standard Model (SM). Of the many potential beyond the Standard Model (BSM) topics DUNE will probe, this paper presents a selection of studies quantifying DUNE’s sensitivities to sterile neutrino mixing, heavy neutral leptons, non-standard interactions, CPT symmetry violation, Lorentz invariance violation, neutrino trident production, dark matter from both beam induced and cosmogenic sources, baryon number violation, and other new physics topics that complement those at high-energy colliders and significantly extend the present reach.

102 citations


Journal ArticleDOI
TL;DR: The SNO+ experiment as mentioned in this paper is located 2 km underground at SNOLAB in Sudbury, Canada and performs a low background search for neutrinoless double beta (0) decay using 780 tonnes of liquid scintillator loaded with 3.9 tonnes of natural tellurium, corresponding to 1.3 tonnes of [130]Te.
Abstract: The SNO+ experiment is located 2 km underground at SNOLAB in Sudbury, Canada. A low background search for neutrinoless double beta (0) decay will be conducted using 780 tonnes of liquid scintillator loaded with 3.9 tonnes of natural tellurium, corresponding to 1.3 tonnes of [130]Te. This paper provides a general overview of the SNO+ experiment, including detector design, construction of process plants, commissioning efforts, electronics upgrades, data acquisition systems, and calibration techniques. The SNO+ collaboration is reusing the acrylic vessel, PMT array, and electronics of the SNO detector, having made a number of experimental upgrades and essential adaptations for use with the liquid scintillator. With low backgrounds and a low energy threshold, the SNO+ collaboration will also pursue a rich physics program beyond the search for 0 decay, including studies of geo- and reactor antineutrinos, supernova and solar neutrinos, and exotic physics such as the search for invisible nucleon decay. The SNO+ approach to the search for 0 decay is scalable: a future phase with high [130]Te-loading is envisioned to probe an effective Majorana mass in the inverted mass ordering region.

71 citations


Journal ArticleDOI
B. Abi1, R. Acciarri2, M. A. Acero3, George Adamov4  +975 moreInstitutions (155)
TL;DR: The Deep Underground Neutrino Experiment (DUNE) as discussed by the authors is a 40kton underground liquid argon time projection chamber experiment, which is sensitive to the electron-neutrinos flavor component of the burst of neutrinos expected from the next Galactic core-collapse supernova.
Abstract: The Deep Underground Neutrino Experiment (DUNE), a 40-kton underground liquid argon time projection chamber experiment, will be sensitive to the electron-neutrino flavor component of the burst of neutrinos expected from the next Galactic core-collapse supernova. Such an observation will bring unique insight into the astrophysics of core collapse as well as into the properties of neutrinos. The general capabilities of DUNE for neutrino detection in the relevant few- to few-tens-of-MeV neutrino energy range will be described. As an example, DUNE's ability to constrain the $ u_e$ spectral parameters of the neutrino burst will be considered.

58 citations


Journal ArticleDOI
TL;DR: Together, the larger rates and higher axion energies imply a stronger bound on the mass of the QCD axion and better prospects for direct detection in a large underground neutrino detector from a nearby galactic supernova.
Abstract: We calculate the axion emission rate from reactions involving thermal pions in matter encountered in supernovae and neutron star mergers, identify unique spectral features, and explore their implications for astrophysics and particle physics. We find that it is about 2-5 times larger than nucleon-nucleon bremsstrahlung, which in past studies was considered to be the dominant process. The axion spectrum is also found be much harder. Together, the larger rates and higher axion energies imply a stronger bound on the mass of the QCD axion and better prospects for direct detection in a large underground neutrino detector from a nearby galactic supernova.

54 citations


Journal ArticleDOI
TL;DR: The Radio Neutrino Observatory Greenland (RNO-G) as mentioned in this paper is the first radio detector for in-ice neutrino signals, which uses an array of radio sensors to measure neutrinos above 10 PeV.
Abstract: This article presents the design of the Radio Neutrino Observatory Greenland (RNO-G) and discusses its scientific prospects. Using an array of radio sensors, RNO-G seeks to measure neutrinos above 10 PeV by exploiting the Askaryan effect in neutrino-induced cascades in ice. We discuss the experimental considerations that drive the design of RNO-G, present first measurements of the hardware that is to be deployed and discuss the projected sensitivity of the instrument. RNO-G will be the first production-scale radio detector for in-ice neutrino signals.

48 citations


Journal ArticleDOI
TL;DR: The supernova early warning system (SNEWS) has been operating as a simple coincidence between neutrino experiments in automated mode since 2005 as discussed by the authors, and it can provide an early warning for the subsequent electromagnetic fireworks, as well as signal to other detectors with significant backgrounds.
Abstract: The next core-collapse supernova in the Milky Way or its satellites will represent a once-in-a-generation opportunity to obtain detailed information about the explosion of a star and provide significant scientific insight for a variety of fields because of the extreme conditions found within. Supernovae in our galaxy are not only rare on a human timescale but also happen at unscheduled times, so it is crucial to be ready and use all available instruments to capture all possible information from the event. The first indication of a potential stellar explosion will be the arrival of a bright burst of neutrinos. Its observation by multiple detectors worldwide can provide an early warning for the subsequent electromagnetic fireworks, as well as signal to other detectors with significant backgrounds so they can store their recent data. The supernova early warning system (SNEWS) has been operating as a simple coincidence between neutrino experiments in automated mode since 2005. In the current era of multi-messenger astronomy there are new opportunities for SNEWS to optimize sensitivity to science from the next galactic supernova beyond the simple early alert. This document is the product of a workshop in June 2019 towards design of SNEWS 2.0, an upgraded SNEWS with enhanced capabilities exploiting the unique advantages of prompt neutrino detection to maximize the science gained from such a valuable event.

47 citations


Journal ArticleDOI
Rasha Abbasi1, Markus Ackermann, Jenni Adams2, Juanan Aguilar3  +372 moreInstitutions (50)
TL;DR: In this article, a reconstruction method based on convolutional architectures and hexagonally shaped kernels is presented, which is robust towards systematic uncertainties in the simulation and has been tested on experimental data.
Abstract: Continued improvements on existing reconstruction methods are vital to the success of high-energy physics experiments, such as the IceCube Neutrino Observatory. In IceCube, further challenges arise as the detector is situated at the geographic South Pole where computational resources are limited. However, to perform real-time analyses and to issue alerts to telescopes around the world, powerful and fast reconstruction methods are desired. Deep neural networks can be extremely powerful, and their usage is computationally inexpensive once the networks are trained. These characteristics make a deep learning-based approach an excellent candidate for the application in IceCube. A reconstruction method based on convolutional architectures and hexagonally shaped kernels is presented. The presented method is robust towards systematic uncertainties in the simulation and has been tested on experimental data. In comparison to standard reconstruction methods in IceCube, it can improve upon the reconstruction accuracy, while reducing the time necessary to run the reconstruction by two to three orders of magnitude.

31 citations


Journal ArticleDOI
M. L. Chen1
TL;DR: The SNO+ experiment as discussed by the authors retrofitted the SNO detector by replacing its heavy water target with a liquid scintillator one, which has several features that are ideal for new investigations.
Abstract: The SNO+ experiment will retrofit the SNO detector [1] by replacing its heavy water target with a liquid scintillator one. The SNO detector has several features that are ideal for new investigations.

30 citations


Journal ArticleDOI
TL;DR: In this paper, the authors consider the production of a ''fast flux'' of hypothetical millicharged particles (mCPs) in the interstellar medium, and calculate the expected signal for direct dark matter detection aimed at electron recoil.
Abstract: We consider the production of a ``fast flux'' of hypothetical millicharged particles (mCPs) in the interstellar medium. We consider two possible sources induced by cosmic rays: (a) $pp\ensuremath{\rightarrow}(\mathrm{meson})\ensuremath{\rightarrow}\phantom{\rule{0ex}{0ex}}(\mathrm{mCP})$, which adds to atmospheric production of mCPs, and (b) cosmic-ray upscattering on a millicharged component of dark matter. We notice that the galactic magnetic fields retain mCPs for a long time, leading to an enhancement of the fast flux by many orders of magnitude. In both scenarios, we calculate the expected signal for direct dark matter detection aimed at electron recoil. We observe that in scenario (a) neutrino detectors (ArgoNeuT and Super-Kamiokande) still provide superior sensitivity compared to dark matter detectors (XENON1T). However, in scenarios with a boosted dark matter component, the dark matter detectors perform better, given the enhancement of the upscattered flux at low velocities. Given the uncertainties, both in the flux generation model and in the actual atomic physics leading to electron recoil, it is still possible that the XENON1T-reported excess may come from a fast mCP flux, which will be decisively tested with future experiments.

28 citations


Journal ArticleDOI
TL;DR: In this article, the neutrino cross section between 60 TeV and 10 PeV was measured using the high-energy starting event (HESE) sample from IceCube with 7.5 years of data.
Abstract: The flux of high-energy neutrinos passing through the Earth is attenuated due to their interactions with matter. The interaction rate is determined by the neutrino interaction cross section and affects the flux arriving at the IceCube Neutrino Observatory, a cubic-kilometer neutrino detector embedded in the Antarctic ice sheet. We present a measurement of the neutrino cross section between 60 TeV and 10 PeV using the high-energy starting event (HESE) sample from IceCube with 7.5 years of data. The result is binned in neutrino energy and obtained using both Bayesian and frequentist statistics. We find it compatible with predictions from the Standard Model. While the cross section is expected to be flavor independent above 1 TeV, additional constraints on the measurement are included through updated experimental particle identification (PID) classifiers, proxies for the three neutrino flavors. This is the first such measurement to use a ternary PID observable and the first to account for neutrinos from tau decay.

28 citations


Journal ArticleDOI
TL;DR: In this paper, the authors used three years of publicly available IceCube data to search for evidence of neutrino emission from the blazars and non-blazar Active Galactic Nuclei (AGN) contained the Fermi 4LAC catalog.
Abstract: The origin of the astrophysical neutrino flux reported by the IceCube Collaboration remains an open question. In this study, we use three years of publicly available IceCube data to search for evidence of neutrino emission from the blazars and non-blazar Active Galactic Nuclei (AGN) contained the Fermi 4LAC catalog. We find no evidence that these sources produce high-energy neutrinos, and conclude that blazars can produce no more than 15% of IceCube's observed flux. The constraint we derive on the contribution from non-blazar AGN, which are less luminous and more numerous than blazars, is significantly less restrictive, and it remains possible that this class of sources could produce the entirety of the diffuse neutrino flux observed by IceCube. We anticipate that it will become possible to definitively test such scenarios as IceCube accumulates and releases more data, and as gamma-ray catalogs of AGN become increasingly complete. We also comment on starburst and other starforming galaxies, and conclude that these sources could contribute substantially to the signal observed by IceCube, in particular at the lowest detected energies.

Journal ArticleDOI
TL;DR: In this paper, the effects of charged current and neutral current on neutrino nonstandard interactions (NSI) are discussed, and the authors derive limits on charged current NSI and find that more data is required to compete with the existing limits.
Abstract: Neutrino nonstandard interactions (NSI) can be constrained using coherent elastic neutrino-nucleus scattering. We discuss here two aspects in this respect, namely effects of (i) charged current NSI in neutrino production, and (ii) CP-violating phases associated with neutral current NSI in neutrino detection. Effects of $CP$-phases require the simultaneous presence of two different flavor-changing neutral current NSI parameters. Applying these two scenarios to the COHERENT measurement, we derive limits on charged current NSI and find that more data is required to compete with the existing limits. Regarding $CP$-phases, we show how the limits on the NSI parameters depend dramatically on the values of the phases. Incidentally, the same parameters influencing coherent scattering also show up in neutrino oscillation experiments. We find that COHERENT provides complementary constraints on the set of NSI parameters that can explain the discrepancy in the best-fit value of the standard $CP$-phase obtained by T2K and $\mathrm{NO}\ensuremath{ u}\mathrm{A}$, while the significance with which the large mixing angle (LMA)-Dark-solution is ruled out can be weakened by the presence of additional NSI parameters introduced here.

Journal ArticleDOI
TL;DR: In this paper, a two-zone radiation model of blazars where an inner/outer blob close to/far from the supermassive black hole is invoked was proposed to investigate the 2014-2015 neutrino flare associated with the blazar TXS 0506+056.
Abstract: In this work, we investigate the 2014-2015 neutrino flare associated with the blazar TXS 0506+056 and a recently discovered muon neutrino event IceCube-200107A in spatial coincidence with the blazar 4FGL J0955.1+3551, under the framework of a two-zone radiation model of blazars where an inner/outer blob close to/far from the supermassive black hole are invoked. An interesting feature that the two sources share in common is that no evidence of GeV gamma-ray activity is found during the neutrino detection period, probably implying a large opacity for GeV gamma rays in the neutrino production region. In our model, continuous particle acceleration/injection takes place in the inner blob at the jet base, where the hot X-ray corona of the supermassive black hole provides target photon fields for efficient neutrino production and strong GeV gamma-ray absorption. We show that this model can self-consistently interpret the neutrino emission from both two blazars in a large parameter space. In the meantime, the dissipation processes in outer blob are responsible for the simultaneous multi-wavelength emission of both sources. In agreement with previous studies of TXS 0506+056 and, an intense MeV emission from the induced electromagnetic cascade in the inner blob is robustly expected to accompany the neutrino flare in our model could be used to test the model with the next-generation MeV gamma-ray detector in the future.

Journal ArticleDOI
TL;DR: In this paper, the authors investigated the sensitivity of future liquid-argon DarkSide-20k and ARGO detectors to supernova neutrinos via coherent elastic neutrino-nucleus scattering.
Abstract: Future liquid-argon DarkSide-20k and ARGO detectors, designed for direct dark matter search, will be sensitive also to core-collapse supernova neutrinos, via coherent elastic neutrino-nucleus scattering. This interaction channel is flavor-insensitive with a high-cross section, enabling for a high-statistics neutrino detection with target masses of $\sim$50~t and $\sim$360~t for DarkSide-20k and ARGO, respectively. Thanks to the low-energy threshold of $\sim$0.5~keV$_{nr}$ achievable by exploiting the ionization channel, DarkSide-20k and ARGO have the potential to discover supernova bursts throughout our galaxy and up to the Small Magellanic Cloud, respectively, assuming a 11-M$_{\odot}$ progenitor star. We report also on the sensitivity to the neutronization burst, whose electron neutrino flux is suppressed by oscillations when detected via charged current and elastic scattering. Finally, the accuracies in the reconstruction of the average and total neutrino energy in the different phases of the supernova burst, as well as its time profile, are also discussed, taking into account the expected background and the detector response.

Journal ArticleDOI
TL;DR: In this article, the authors presented a measurement of the combined neutrino + ε-charge-averaged charged-current inclusive cross section on argon using data from the MicroBooNE liquid argon time projection chamber (LArTPC) at Fermilab.
Abstract: We present a measurement of the combined $ u_e$ + $\bar{ u}_e$ flux-averaged charged-current inclusive cross section on argon using data from the MicroBooNE liquid argon time projection chamber (LArTPC) at Fermilab. Using the off-axis flux from the NuMI beam, MicroBooNE has reconstructed 214 candidate $ u_e$ + $\bar{ u}_e$ interactions with an estimated exposure of 2.4$\times10^{20}$ protons on target. Given the estimated purity of 38.6\%, this implies the observation of 80 $ u_e$ + $\bar{ u}_e$ events in argon, the largest such sample to date. The analysis includes the first demonstration of a fully automated application of a dE/dx-based particle discrimination technique of electron and photon induced showers in a LArTPC neutrino detector. We measure the $ u_e + \bar{ u}_e$ flux-averaged charged-current total cross section to be ${6.84\pm\!1.51~\textrm{(stat.)}\pm\!2.33~\textrm{(sys.)}\!\times\!10^{-39}~\textrm{cm}^{2}/~\textrm{nucleon}}$, for neutrino energies above 250 MeV and an average neutrino flux energy of 905 MeV when this threshold is applied. The measurement is sensitive to neutrino events where the final state electron momentum is above 48 MeV/c, includes the entire angular phase space of the electron, and is in agreement with the theoretical predictions from \texttt{GENIE} and \texttt{NuWro}. This measurement is also the first demonstration of electron neutrino reconstruction in a surface LArTPC in the presence of cosmic ray backgrounds, which will be a crucial task for surface experiments like those that comprise the Short-Baseline Neutrino (SBN) Program at Fermilab.

Journal ArticleDOI
TL;DR: In this paper, neutrino signals from core-collapse supernova (CCSN) are computed using axisymmetric CCSN simulations that cover the post-bounce phase up to
Abstract: We study theoretical neutrino signals from core-collapse supernova (CCSN) computed using axisymmetric CCSN simulations that cover the post-bounce phase up to $\sim 4$~s. We provide basic quantities of the neutrino signals such as event rates, energy spectra, and cumulative number of events at some terrestrial neutrino detectors, and then we discuss some new features in the late phase that emerge in our models. Contrary to popular beliefs, neutrino emissions in the late phase are not always quiet, but rather have temporal fluctuations, the vigor of which hinges on the CCSN model and neutrino flavor. We find that the temporal variations are not primarily driven by proto-neutron star (PNS) convection, but by fallback accretion flows in explosion models. We assess the detectability of these temporal variations, and conclude that IceCube is the most promising detector with which to resolve them. We also update fitting formulae first proposed in our previous paper for which total neutrino energy (TONE) emitted at the CCSN source is estimated from the cumulative number of events at each detector. This will be very powerful in the data analysis of real observations, in particular for low-statistics data. As an interesting demonstration, we apply our fitting formulae to a real observation, that of SN 1987A at Kamiokande-II. The TONE is estimated as $\sim 2 \times 10^{53}$~erg. By combining the recent constraints on the equation-of-state, we further estimate the gravitational mass of PNS in the remnant of SN 1987A, which is $\sim 1.2~M_{\sun}$.

Journal ArticleDOI
TL;DR: A review and summarise a number of these Liquid Argon Time Projection Chamber (LArTPC) experiments, and briefly describe the specific technologies that they currently employ can be found in this paper.
Abstract: Liquid Argon (LAr) is one of the most widely used scintillators in particle detection, due to its low cost, high availability and excellent scintillation properties. A large number of experiments in the neutrino sector are based around using LAr in one or more Time Projection Chambers (TPCs), leading to high resolution three-dimensional particle reconstruction. In this paper, we review and summarise a number of these Liquid Argon Time Projection Chamber (LArTPC) experiments, and briefly describe the specific technologies that they currently employ. This includes single phase LAr experiments (ICARUS T600, MicroBooNE, SBND, LArIAT, DUNE-SP, ProtoDUNE-SP, ArgonCube and Vertical Drift) and dual phase LAr experiments (DUNE-DP, WA105, ProtoDUNE-DP and ARIADNE). We also discuss some new avenues of research in the field of LArTPC readout, which show potential for wide-scale use in the near future.

Journal ArticleDOI
TL;DR: In this article, a detailed modeling and computation methodology is presented to determine the optical Cherenkov signals produced by upward-moving extensive air showers (EASs) induced by tau and muon initiated EASs.
Abstract: We present a detailed modeling and computation methodology to determine the optical Cherenkov signals produced by upward-moving extensive air showers (EASs) induced by $\ensuremath{\tau}$-leptons and muons, sourced from the interaction of high-energy astrophysical neutrinos interacting in the Earth. Following and extending the physics modeling and Cherenkov signal simulations performed in M. H. Reno et al. [Phys. Rev. D 100, 063010 (2019)], this scheme encompasses a new, state-of-the-art computation of the muon neutrino propagation inside the Earth and the contribution to the $\ensuremath{\tau}$-lepton muon decay channel. The modeling takes into account all possible $\ensuremath{\tau}$-lepton decay and muon energy loss channels that feed the optical Cherenkov emission, produced by both tau and muon initiated EASs. The EAS modeling uses the electron energy, angular, and lateral distributions in the EAS and their evolution as well as the wavelength dependence of the Cherenkov emission and its atmospheric attenuation. The results presented here are focused on the detection capabilities of suborbital (balloon-borne) and orbital (satellite) based instruments. The latter case was calculated for POEMMA [The Probe Of Extreme MultiMessenger Astrophysics] to compare to that presented in M. H. Reno et al. [Phys. Rev. D 100, 063010 (2019)], specifically including the muon-decay channel of $\ensuremath{\tau}$-leptons and the muonic EAS Cherenkov signal from muon neutrino interactions in the Earth. By detailing all these individual contributions to the optical Cherenkov emission and detection, we show how the ensemble that includes muonic channels provides a large detection capability for space-based, high-energy cosmic neutrino detection. Specifically, we show that for neutrino energies $\ensuremath{\lesssim}10\text{ }\text{ }\mathrm{PeV}$, the upward-EAS sensitivity due to muon neutrino interactions in the Earth begin to dominate over that for tau neutrino interactions, effectively extending the neutrino sensitivity to lower energies.

Journal ArticleDOI
TL;DR: In this article, the authors revisit the production of millicharged particles in these atmospheric showers and provide new constraints for XENON1T and Super-Kamiokande and new sensitivity estimates of current and future detectors, such as JUNO.
Abstract: For nearly a century, studying cosmic-ray air showers has driven progress in our understanding of elementary particle physics. In this work, we revisit the production of millicharged particles in these atmospheric showers and provide new constraints for XENON1T and Super-Kamiokande and new sensitivity estimates of current and future detectors, such as JUNO. We discuss distinct search strategies, specifically studies of single-energy-deposition events, where one electron in the detector receives a relatively large energy transfer, as well as multiple-scattering events consisting of (at least) two relatively small energy depositions. We demonstrate that these atmospheric search strategies — especially the multiple-scattering signature — provide significant room for improvement beyond existing searches, in a way that is complementary to anthropogenic, beam-based searches for MeV-GeV millicharged particles. Finally, we also discuss the implementation of a Monte Carlo simulation for millicharged particle detection in large-volume neutrino detectors, such as IceCube.

Journal ArticleDOI
TL;DR: The SoLid experiment as mentioned in this paper is a new generation neutrino experiment which tries to address the key challenges for high precision reactor neutrinos measurements at very short distances from a reactor core and with little or no overburden.
Abstract: The SoLid experiment, short for Search for Oscillations with a Lithium-6 detector, is a new generation neutrino experiment which tries to address the key challenges for high precision reactor neutrino measurements at very short distances from a reactor core and with little or no overburden. The primary goal of the SoLid experiment is to perform a precise measurement of the electron antineutrino energy spectrum and flux and to search for very short distance neutrino oscillations as a probe of eV-scale sterile neutrinos. This paper describes the SoLid detection principle, the mechanical design and the construction of the detector. It then reports on the installation and commissioning on site near the BR2 reactor, Belgium, and finally highlights its performance in terms of detector response and calibration.

Journal ArticleDOI
TL;DR: In this article, the multi-azimuthal angle (MAA) effect on collective neutrino oscillation was investigated by considering the three-dimensional Neutrino momentum distribution in a realistic electron-capture supernova model with an $8.8$ progenitor.
Abstract: We investigate the multi-azimuthal angle (MAA) effect on collective neutrino oscillation by considering the three-dimensional neutrino momentum distribution in a realistic electron-capture supernova model with an $8.8\text{ }\text{ }{M}_{\ensuremath{\bigodot}}$ progenitor. We find that the MAA effect induces collective flavor conversions at epochs when it is completely suppressed under the axial-symmetric approximation. This novel activity is switched on/off by the growth of the MAA instability and imprints additional time evolution in the expected neutrino event rate. We validate our results by extending the linear stability analysis into the three-flavor scheme including mixing angles, and confirm that the onset of collective neutrino oscillation matches the steep growth of flavor instability. We discuss how the MAA effect alters neutrino detection at Super-Kamiokande and DUNE.

Journal ArticleDOI
Arnauld Albert1, Michel André, M. Anghinolfi, Gisela Anton, M. Ardid, J. J. Aubert, Julien Aublin, Bruny Baret, S. Basa, B. Belhorma, V. Bertin, S.F. Biagi, M. Bissinger, Jihad Boumaaza, M. Bouta, M.C. Bouwhuis, H. Brânzaş, R. Bruijn, J. Brunner, J. Busto, Alessia Capone, L. Caramete, J. Jeffrey Carr, S. Cecchini, Silvia Celli, Mohamed Chabab, T. N. Chau, R. Cherkaoui El Moursli, Tommaso Chiarusi, M. Circella, Alexis Coleiro, M. Colomer-Molla, R. Coniglione, P. Coyle, A. Creusot, Antonio F. Díaz, G. de Wasseige, Anne Deschamps, C. Distefano, I. Di Palma, Alba Domi, C. Donzaud2, D. Dornic, D. Drouhin1, Thomas Eberl, N. El Khayati, A. Enzenhöfer, A. Ettahiri, Paolo Fermani, Giovanna Ferrara, F. Filippini, Luigi Antonio Fusco, Hervé Glotin, R. Gozzini, Kay Graf, C. Guidi, Steffen Hallmann, H. van Haren, A.J. Heijboer, Yann Hello, J.J. Hernández-Rey, J. Hößl, J. Hofestädt, F. Huang, Giulia Illuminati, C. W. James, M. de Jong, P. de Jong, M. Jongen, Matthias Kadler, O. Kalekin, U. Katz, N.R. Khan-Chowdhury, Antoine Kouchner3, I. Kreykenbohm, Vladimir Kulikovskiy, R. Lahmann, R. Le Breton, Dominique Lefèvre, Emanuele Leonora, Giuseppe Levi, Massimiliano Lincetto, D. Lopez-Coto, S. Loucatos, J. Manczak, M. Marcelin, Annarita Margiotta, A. Marinelli, J.A. Martínez-Mora, S. Mazzou, Karel Melis, P. Migliozzi, Michael Moser, Abdelilah Moussa, R. Muller, L. Nauta, S. Sánchez Navas, E. Nezri, A. Nuñez-Castiñeyra, B. O'Fearraigh, M. Organokov, G.E. Păvălaş, C. Pellegrino, M. Perrin-Terrin, P. Piattelli, C. Poirè, V. Popa, Thierry Pradier, N. Randazzo, S. Reck, G. Riccobene, F. Salesa, A. Sánchez-Losa, D. F. E. Samtleben, Matteo Sanguineti, Paolo Sapienza, Jutta Schnabel, F. Schüssler, Maurizio Spurio, Th. Stolarczyk, B. Strandberg, M. Taiuti, Yahya Tayalati, T. Thakore, Steven Tingay, B. Vallage, V. Van Elewyck3, Federico Versari, S. Viola, Daniele Vivolo, Jörn Wilms, A. Zegarelli, J.D. Zornoza, J. Zúñiga 
TL;DR: In this paper, Monte Carlo simulations are used to check the response of a deep-sea neutrino detector and to monitor its performance, in addition to a reliable description of active parts of the detector and features of physics events.
Abstract: Monte Carlo simulations are a unique tool to check the response of a detector and to monitor its performance. For a deep-sea neutrino telescope, the variability of the environmental conditions that can affect the behaviour of the data acquisition system must be considered, in addition to a reliable description of the active parts of the detector and of the features of physics events, in order to produce a realistic set of simulated events. In this paper, the software tools used to produce neutrino and cosmic ray signatures in the telescope and the strategy developed to represent the time evolution of the natural environment and of the detector efficiency are described.

Journal Article
TL;DR: The ProtoDune-SP detector as discussed by the authors is a prototype for the first far detector module of the Deep Underground Neutrino Experiment (DUNE), which will be constructed at the Sandford Underground Research Facility (SURF) in Lead, South Dakota, USA.
Abstract: The ProtoDUNE-SP detector is a single-phase liquid argon time projection chamber (LArTPC) that was constructed and operated in the CERN North Area at the end of the H4 beamline. This detector is a prototype for the first far detector module of the Deep Underground Neutrino Experiment (DUNE), which will be constructed at the Sandford Underground Research Facility (SURF) in Lead, South Dakota, USA. The ProtoDUNE-SP detector incorporates full-size components as designed for DUNE and has an active volume of $7\times 6\times 7.2$~m$^3$. The H4 beam delivers incident particles with well-measured momenta and high-purity particle identification. ProtoDUNE-SP's successful operation between 2018 and 2020 demonstrates the effectiveness of the single-phase far detector design. This paper describes the design, construction, assembly and operation of the detector components.

Journal ArticleDOI
TL;DR: In this article, the authors evaluate the detectability of neutrinos from nearby bright Seyfert galaxies identified by X-ray measurements and find that NGC 1068 is the most promising galaxy in the Northern sky.
Abstract: Particles may be accelerated in magnetized coronae via magnetic reconnections and/or plasma turbulence, leading to high-energy neutrinos and soft gamma rays. We evaluate the detectability of neutrinos from nearby bright Seyfert galaxies identified by X-ray measurements. In the disk-corona model, we find that NGC 1068 is the most promising Seyfert galaxy in the Northern sky, where IceCube is the most sensitive, and show prospects for the identification of aggregated neutrino signals from Seyfert galaxies bright in X-rays. Moreover, we demonstrate that nearby Seyfert galaxies are promising targets for the next generation of neutrino telescopes such as KM3NeT and IceCube-Gen2. For KM3NeT, Cen A can be the most promising source in the Southern sky if a significant fraction of the observed X-rays come from the corona, and it could be identified in few years of KM3NeT operation. Our results reinforce the idea that hidden cores of supermassive black holes are the dominant sources of the high-energy neutrino emission and underlines the necessity of better sensitivity to medium-energy ranges in future neutrino detectors for identifying the origin of high-energy cosmic neutrinos.

Journal ArticleDOI
Arnauld Albert1, Arnauld Albert2, S. Alves3, Michel André4, M. Anghinolfi, Gisela Anton5, M. Ardid6, J-J. Aubert7, Julien Aublin8, B. Baret8, S. Basa7, B. Belhorma, M. Bendahman8, V. Bertin7, S.F. Biagi, M. Bissinger5, Jihad Boumaaza, M. Bouta, M.C. Bouwhuis, H. Brânzaş, R. Bruijn9, J. Brunner7, Jose Busto7, Alessia Capone10, L. Caramete, J. Carr7, V. Carretero3, Silvia Celli10, Mohamed Chabab11, T. N. Chau8, R. Cherkaoui El Moursli, Tommaso Chiarusi, M. Circella, Alexis Coleiro8, M. Colomer-Molla8, M. Colomer-Molla3, R. Coniglione, P. Coyle7, A. Creusot8, Antonio F. Díaz12, G. de Wasseige8, Anne Deschamps13, C. Distefano, I. Di Palma10, Alba Domi, C. Donzaud14, C. Donzaud8, Damien Dornic7, D. Drouhin2, D. Drouhin1, Thomas Eberl5, N. El Khayati, A. Enzenhöfer7, Paolo Fermani10, Giovanna Ferrara, F. Filippini, L. Fusco7, L. Fusco8, R. García, Y. Gatelet8, Hervé Glotin7, R. Gozzini3, R. Gozzini5, Kay Graf5, C. Guidi, Steffen Hallmann5, H. van Haren, A.J. Heijboer, Yann Hello13, J.J. Hernández-Rey3, J. Hößl5, J. Hofestädt5, F. Huang1, G. Illuminati8, C. W. James15, B. Jisse-Jung, M. de Jong16, P. de Jong, M. Jongen, Matthias Kadler17, O. Kalekin5, U. Katz5, N.R. Khan-Chowdhury3, Antoine Kouchner8, I. Kreykenbohm5, Vladimir Kulikovskiy18, Robert Lahmann5, R. Le Breton8, Dominique Lefèvre7, Dominique Lefèvre13, Emanuele Leonora, Giuseppe Levi, Massimiliano Lincetto7, D. Lopez-Coto12, S. Loucatos8, S. Loucatos19, L. Maderer8, J. Manczak3, M. Marcelin7, Annarita Margiotta, A. Marinelli, J.A. Martínez-Mora6, Karel Melis9, P. Migliozzi, Michael Moser5, Abdelilah Moussa, R. Muller, L. Nauta, S. Sánchez Navas12, E. Nezri7, A. Nuñez-Castiñeyra7, B. O'Fearraigh, M. Organokov1, G.E. Păvălaş, C. Pellegrino, M. Perrin-Terrin7, P. Piattelli, C. Pieterse3, C. Poirè6, V. Popa, Thierry Pradier1, N. Randazzo, S. Reck5, G. Riccobene, F. Salesa Greus3, D. F. E. Samtleben16, A. Sánchez-Losa, Matteo Sanguineti, Paolo Sapienza, Jutta Schnabel5, J. Schumann5, F. Schüssler19, Maurizio Spurio, Th. Stolarczyk19, M. Taiuti, Yahya Tayalati, T. Thakore3, Steven Tingay15, B. Vallage8, B. Vallage19, V. Van Elewyck20, V. Van Elewyck8, F. Versari8, S. Viola, Daniele Vivolo, Joern Wilms5, A. Zegarelli10, J.D. Zornoza3, J. Zúñiga3 
TL;DR: In this paper, a combined measurement of the energy spectra of atmospheric ν e and ν μ in the energy range between ∼100 GeV and ∼50 TeV with the ANTARES neutrino telescope is presented.

Journal ArticleDOI
C. Ahdida1, A. Akmete2, Raffaele Albanese, A. Alexandrov  +357 moreInstitutions (51)
TL;DR: In this paper, the authors study the potential of the SHiP experiment to detect such elusive particles through its Scattering and Neutrino detector (SND), and they find that SHIP will improve the current limits in the mass range for the dark matter from about 1 MeV to 300 MeV.
Abstract: Dark matter is a well-established theoretical addition to the Standard Model supported by many observations in modern astrophysics and cosmology. In this context, the existence of weakly interacting massive particles represents an appealing solution to the observed thermal relic in the Universe. Indeed, a large experimental campaign is ongoing for the detection of such particles in the sub-GeV mass range. Adopting the benchmark scenario for light dark matter particles produced in the decay of a dark photon, with $\alpha_D=0.1$ and $m_{A'}=3m_{\chi}$, we study the potential of the SHiP experiment to detect such elusive particles through its Scattering and Neutrino detector (SND). In its 5-years run, corresponding to $2\cdot 10^{20}$ protons on target from the CERN SPS, we find that SHiP will improve the current limits in the mass range for the dark matter from about 1 MeV to 300 MeV. In particular, we show that SHiP will probe the thermal target for Majorana candidates in most of this mass window and even reach the Pseudo-Dirac thermal relic.

Journal ArticleDOI
TL;DR: In this paper, the neutrino detection capability of the KM3NeT project is estimated from detailed analyses of background data from the first KM3NET detection units and simulations of neutrinos signal.
Abstract: The KM3NeT research infrastructure is under construction in the Mediterranean Sea. It consists of two water Cherenkov neutrino detectors, ARCA and ORCA, aimed at neutrino astrophysics and oscillation research, respectively. Instrumenting a large volume of sea water with $\sim$ 6,200 optical modules comprising a total of $\sim$ 200,000 photomultiplier tubes, KM3NeT will achieve sensitivity to $\sim$ 10 MeV neutrinos from Galactic and near-Galactic core-collapse supernovae through the observation of coincident hits in photomultipliers above the background. In this paper, the sensitivity of KM3NeT to a supernova explosion is estimated from detailed analyses of background data from the first KM3NeT detection units and simulations of the neutrino signal. The KM3NeT observational horizon (for a $5\,\sigma$ discovery) covers essentially the Milky-Way and for the most optimistic model, extends to the Small Magellanic Cloud ($\sim$ 60 kpc). Detailed studies of the time profile of the neutrino signal allow assessment of the KM3NeT capability to determine the arrival time of the neutrino burst with a few milliseconds precision for sources up to 5$-$8 kpc away, and detecting the peculiar signature of the standing accretion shock instability if the core-collapse supernova explosion happens closer than 3$-$5 kpc, depending on the progenitor mass. KM3NeT's capability to measure the neutrino flux spectral parameters is also presented.

Journal ArticleDOI
TL;DR: The eHWC J1825-134 source is located in the southern sky and has been recently detected by the HAWC observatory as discussed by the authors, and it is the most luminous in the multi-TeV domain and therefore is one of the first that should be searched for with a neutrino telescope in the northern hemisphere.
Abstract: The eHWC J1825-134 source is located in the southern sky and has been recently detected by the HAWC observatory. It presents an hard spectral index and its gamma-ray flux extends up to energies close to 100 TeV without significant suppression. Amongst the HAWC sources, it is the most luminous in the multi-TeV domain and therefore is one of the first that should be searched for with a neutrino telescope in the northern hemisphere. Using an updated effective area for the forthcoming KM3NeT detector, we study the possibility to detect this source within ten years of its running time. We show how the Fermi-LAT data could help in providing a morphology information on the source region. We conclude that, considering a neutrino energy threshold around 10 TeV, about a four to five sigma detection has to be expected after ten years of observations, depending on the details of the considered scenario. Finally, we also consider the case in which the emission from the HWC J1825-134 source is only partially hadronic and show that in 20 years of running time a three sigma detection is feasible.

Journal ArticleDOI
TL;DR: The developed neural network has been trained and tested on diverse neutrino interaction samples, showing very promising results: the classification of particle track voxels produced in the detector can be done with efficiencies and purities of 94-96% per event and most of the ambiguities can be identified and rejected, while being robust against systematic effects.
Abstract: Deep-learning tools are being used extensively in high energy physics and are becoming central in the reconstruction of neutrino interactions in particle detectors. In this work, we report on the performance of a graph neural network in assisting with particle set event reconstruction. The three-dimensional reconstruction of particle tracks produced in neutrino interactions can be subject to ambiguities due to high multiplicity signatures in the detector or leakage of signal between neighboring active detector volumes. Graph neural networks potentially have the capability of identifying all these features to boost the reconstruction performance. As an example case study, we tested a graph neural network, inspired by the graphsage algorithm, on a novel 3D-granular plastic-scintillator detector, that will be used to upgrade the near detector of the T2K experiment. The developed neural network has been trained and tested on diverse neutrino interaction samples, showing very promising results: the classification of particle track voxels produced in the detector can be done with efficiencies and purities of 94%--96% per event and most of the ambiguities can be identified and rejected, while being robust against systematic effects.

Posted Content
TL;DR: The Jiangmen Underground Neutrino Observatory (JUNO) is a 20 kton LS detector at 700-m underground as mentioned in this paper, which has excellent energy resolution and a large fiducial volume offer exciting opportunities for addressing many important topics in neutrino and astroparticle physics.
Abstract: The Jiangmen Underground Neutrino Observatory (JUNO) is a 20 kton LS detector at 700-m underground. An excellent energy resolution and a large fiducial volume offer exciting opportunities for addressing many important topics in neutrino and astro-particle physics. With 6 years of data, the neutrino mass ordering can be determined at 3-4 sigma and three oscillation parameters can be measured to a precision of 0.6% or better by detecting reactor antineutrinos. With 10 years of data, DSNB could be observed at 3-sigma; a lower limit of the proton lifetime of 8.34e33 years (90% C.L.) can be set by searching for p->nu_bar K^+; detection of solar neutrinos would shed new light on the solar metallicity problem and examine the vacuum-matter transition region. A core-collapse supernova at 10 kpc would lead to ~5000 IBD and ~2000 (300) all-flavor neutrino-proton (electron) scattering events. Geo-neutrinos can be detected with a rate of ~400 events/year. We also summarize the final design of the JUNO detector and the key R&D achievements. All 20-inch PMTs have been tested. The average photon detection efficiency is 28.9% for the 15,000 MCP PMTs and 28.1% for the 5,000 dynode PMTs, higher than the JUNO requirement of 27%. Together with the >20 m attenuation length of LS, we expect a yield of 1345 p.e. per MeV and an effective energy resolution of 3.02%/\sqrt{E (MeV)}$ in simulations. The underwater electronics is designed to have a loss rate <0.5% in 6 years. With degassing membranes and a micro-bubble system, the radon concentration in the 35-kton water pool could be lowered to <10 mBq/m^3. Acrylic panels of radiopurity <0.5 ppt U/Th are produced. The 20-kton LS will be purified onsite. Singles in the fiducial volume can be controlled to ~10 Hz. The JUNO experiment also features a double calorimeter system with 25,600 3-inch PMTs, a LS testing facility OSIRIS, and a near detector TAO.