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Showing papers on "Neutrino detector published in 2013"


Journal ArticleDOI
M. G. Aartsen1, Rasha Abbasi2, Y. Abdou3, Markus Ackermann, Jenni Adams4, Juanan Aguilar5, Markus Ahlers2, D. Altmann6, J. Auffenberg2, X. Bai, Michael J. Baker2, S. W. Barwick7, V. Baum8, R. C. Bay9, J. J. Beatty10, S. Bechet11, J. Becker Tjus12, K.-H. Becker13, M. L. Benabderrahmane, Segev BenZvi2, P. Berghaus, D. Berley14, Elisa Bernardini, A. Bernhard, D. Bertrand11, D. Z. Besson15, Gary Binder9, Gary Binder16, Daniel Bindig13, M. Bissok17, E. Blaufuss14, J. Blumenthal17, D. J. Boersma18, S. Bohaichuk19, C. Bohm20, D. Bose21, S. Böser22, Olga Botner18, L. Brayeur21, H.-P. Bretz, A. M. Brown4, R. Bruijn23, Jürgen Brunner, M. J. Carson3, J. Casey24, M. Casier21, Dmitry Chirkin2, A. Christov5, B. Christy14, K. Clark25, F. Clevermann26, S. Coenders17, Seth M. Cohen23, D. F. Cowen25, A. H. Cruz Silva, M. Danninger20, J. Daughhetee24, J. C. Davis10, M. Day2, C. De Clercq21, S. De Ridder3, Paolo Desiati2, K. D. de Vries21, Tyce DeYoung25, Juan Carlos Diaz-Velez2, Matt Dunkman25, R. Eagan25, B. Eberhardt8, B. Eichmann12, J. Eisch2, R. W. Ellsworth14, S. Euler17, Paul Evenson, O. Fadiran2, A. R. Fazely27, Anatoli Fedynitch12, J. Feintzeig2, T. Feusels3, Kirill Filimonov9, Chad Finley20, T. Fischer-Wasels13, S. Flis20, A. Franckowiak22, K. Frantzen26, T. Fuchs26, Thomas K. Gaisser, J. C. Gallagher2, L. Gerhardt9, L. Gerhardt16, L. Gladstone2, Thorsten Glusenkamp, A. Goldschmidt16, G. Golup21, J. G. Gonzalez, J. A. Goodman14, Dariusz Gora, Dylan T. Grandmont19 
20 Nov 2013-Science
TL;DR: The presence of a high-energy neutrino flux containing the most energetic neutrinos ever observed is revealed, including 28 events at energies between 30 and 1200 TeV, although the origin of this flux is unknown and the findings are consistent with expectations for a neutRino population with origins outside the solar system.
Abstract: We report on results of an all-sky search for high-energy neutrino events interacting within the IceCube neutrino detector conducted between May 2010 and May 2012. The search follows up on the previous detection of two PeV neutrino events, with improved sensitivity and extended energy coverage down to about 30 TeV. Twenty-six additional events were observed, substantially more than expected from atmospheric backgrounds. Combined, both searches reject a purely atmospheric origin for the 28 events at the 4 sigma level. These 28 events, which include the highest energy neutrinos ever observed, have flavors, directions, and energies inconsistent with those expected from the atmospheric muon and neutrino backgrounds. These properties are, however, consistent with generic predictions for an additional component of extraterrestrial origin.

1,490 citations


Journal ArticleDOI
M. G. Aartsen1, Rasha Abbasi2, Y. Abdou3, Markus Ackermann  +279 moreInstitutions (37)
TL;DR: A search for muon neutrinos from dark matter annihilation in the center of the Sun with the 79-string configuration of the IceCube neutrino telescope is performed, lowering the energy threshold and extending the search to the austral summer.
Abstract: We have performed a search for muon neutrinos from dark matter annihilation in the center of the Sun with the 79-string configuration of the IceCube neutrino telescope. For the first time, the DeepCore subarray is included in the analysis, lowering the energy threshold and extending the search to the austral summer. The 317 days of data collected between June 2010 and May 2011 are consistent with the expected background from atmospheric muons and neutrinos. Upper limits are set on the dark matter annihilation rate, with conversions to limits on spin-dependent and spin-independent scattering cross sections of weakly interacting massive particles (WIMPs) on protons, for WIMP masses in the range 20-5000 GeV=c(2). These are the most stringent spin-dependent WIMP-proton cross section limits to date above 35 GeV=c(2) for most WIMP models.

408 citations


Journal ArticleDOI
TL;DR: In this article, the authors considered the implications of the IceCube signal for hadronuclear ($pp$) scenarios of neutrino sources such as galaxy clusters/groups and star-forming galaxies.
Abstract: We consider implications of the IceCube signal for hadronuclear ($pp$) scenarios of neutrino sources such as galaxy clusters/groups and star-forming galaxies. Since the observed neutrino flux is comparable to the diffuse $\ensuremath{\gamma}$-ray background flux obtained by Fermi, we place new, strong upper limits on the source spectral index, $\ensuremath{\Gamma}\ensuremath{\lesssim}2.1--2.2$. In addition, the new IceCube data imply that these sources contribute at least 30%--40% of the diffuse $\ensuremath{\gamma}$-ray background in the 100 GeV range and even $\ensuremath{\sim}100%$ for softer spectra. Our results, which are insensitive to details of the $pp$ source models, are one of the first strong examples of the multimessenger approach combining the measured neutrino and $\ensuremath{\gamma}$-ray fluxes. The $pp$ origin of the IceCube signal can further be tested by constraining $\ensuremath{\Gamma}$ with sub-PeV neutrino observations, by unveiling the sub-TeV diffuse $\ensuremath{\gamma}$-ray background and by observing such $pp$ sources with TeV $\ensuremath{\gamma}$-ray detectors. We also discuss specific $pp$ source models with a multi-PeV neutrino break/cutoff, which are consistent with the current IceCube data.

392 citations


Journal ArticleDOI
TL;DR: In this article, the authors review sub-leading effects in neutrino flavor transitions known as non-standard Neutrino interactions (NSIs), which is currently the most explored description for effects beyond the standard paradigm of neutrinos oscillations and report on the phenomenology of NSIs and their experimental and phenomenological bounds.
Abstract: The phenomenon of neutrino oscillations has been established as the leading mechanism behind neutrino flavor transitions, providing solid experimental evidence that neutrinos are massive and lepton flavors are mixed. Here we review sub-leading effects in neutrino flavor transitions known as non-standard neutrino interactions (NSIs), which is currently the most explored description for effects beyond the standard paradigm of neutrino oscillations. In particular, we report on the phenomenology of NSIs and their experimental and phenomenological bounds as well as an outlook for future sensitivity and discovery reach.

342 citations


Journal Article
C. Adams1, David H. Adams2, T. Akiri3, T. Alion4  +478 moreInstitutions (66)
TL;DR: The Long-Baseline Neutrino Experiment (LBNE) as mentioned in this paper is an extensively developed plan for a world-class experiment dedicated to addressing the early evolution of our universe, its current state and its eventual fate.
Abstract: The preponderance of matter over antimatter in the early Universe, the dynamics of the supernova bursts that produced the heavy elements necessary for life and whether protons eventually decay --- these mysteries at the forefront of particle physics and astrophysics are key to understanding the early evolution of our Universe, its current state and its eventual fate. The Long-Baseline Neutrino Experiment (LBNE) represents an extensively developed plan for a world-class experiment dedicated to addressing these questions. LBNE is conceived around three central components: (1) a new, high-intensity neutrino source generated from a megawatt-class proton accelerator at Fermi National Accelerator Laboratory, (2) a near neutrino detector just downstream of the source, and (3) a massive liquid argon time-projection chamber deployed as a far detector deep underground at the Sanford Underground Research Facility. This facility, located at the site of the former Homestake Mine in Lead, South Dakota, is approximately 1,300 km from the neutrino source at Fermilab -- a distance (baseline) that delivers optimal sensitivity to neutrino charge-parity symmetry violation and mass ordering effects. This ambitious yet cost-effective design incorporates scalability and flexibility and can accommodate a variety of upgrades and contributions. With its exceptional combination of experimental configuration, technical capabilities, and potential for transformative discoveries, LBNE promises to be a vital facility for the field of particle physics worldwide, providing physicists from around the globe with opportunities to collaborate in a twenty to thirty year program of exciting science. In this document we provide a comprehensive overview of LBNE's scientific objectives, its place in the landscape of neutrino physics worldwide, the technologies it will incorporate and the capabilities it will possess.

328 citations


Journal ArticleDOI
TL;DR: In this article, the current status of liquid noble gas radiation detectors with energy threshold in the keV range, which are of interest for direct dark matter searches, measurement of coherent neutrino scattering and other low energy particle physics experiments is reviewed.
Abstract: We review the current status of liquid noble gas radiation detectors with energy threshold in the keV range, which are of interest for direct dark matter searches, measurement of coherent neutrino scattering and other low energy particle physics experiments. Emphasis is given to the operation principles and the most important instrumentation aspects of these detectors, principally of those operated in the double-phase mode. Recent technological advances and relevant developments in photon detection and charge readout are discussed in the context of their applicability to those experiments.

294 citations


Journal ArticleDOI
TL;DR: In this paper, the authors present the results of global analyses of short-baseline neutrino oscillation data in 3 + 1, 3 + 2 and 3+ 1 + 1 mixing schemes.
Abstract: We present the results of global analyses of short-baseline neutrino oscillation data in 3 + 1, 3 + 2 and 3 + 1 + 1 neutrino mixing schemes. We show that the data do not allow us to abandon the simplest 3 + 1 scheme in favor of the more complex 3 + 2 and 3 + 1 + 1 schemes. We present the allowed region in the 3 + 1 parameter space, which is located at Delta m(41)(2) between 0.82 and 2.19 eV(2) at 3 sigma. The case of no oscillations is disfavored by about 6 sigma, which decreases dramatically to about 2 sigma if the Liquid Scintillating Neutrino Detector (LSND) data are not considered. Hence, new high-precision experiments are needed to check the LSND signal.

226 citations


Journal ArticleDOI
K. Abe1, N. Abgrall2, Hiroaki Aihara1, T. Akiri3  +355 moreInstitutions (50)
TL;DR: In this article, a FLUKA and GEANT3-based simulation was used to model the physical processes involved in neutrino production, from the interaction of primary beam protons in the T2K target, to the decay of hadrons and muons that produce neutrinos.
Abstract: The Tokai-to-Kamioka (T2K) experiment studies neutrino oscillations using an off-axis muon neutrino beam with a peak energy of about 0.6 GeV that originates at the Japan Proton Accelerator Research Complex accelerator facility. Interactions of the neutrinos are observed at near detectors placed at 280 m from the production target and at the far detector—Super-Kamiokande—located 295 km away. The flux prediction is an essential part of the successful prediction of neutrino interaction rates at the T2K detectors and is an important input to T2K neutrino oscillation and cross section measurements. A FLUKA and GEANT3-based simulation models the physical processes involved in the neutrino production, from the interaction of primary beam protons in the T2K target, to the decay of hadrons and muons that produce neutrinos. The simulation uses proton beam monitor measurements as inputs. The modeling of hadronic interactions is reweighted using thin target hadron production data, including recent charged pion and kaon measurements from the NA61/SHINE experiment. For the first T2K analyses the uncertainties on the flux prediction are evaluated to be below 15% near the flux peak. The uncertainty on the ratio of the flux predictions at the far and near detectors is less than 2% near the flux peak.

205 citations


Journal ArticleDOI
TL;DR: The current status of solar neutrino measurements and of the theory employed in interpreting measurements are described in this paper, where a decadal evaluation of the nuclear physics of the pp chain and CNO cycle defining best values and uncertainties in the nuclear microphysics input to solar models are discussed.
Abstract: We describe the current status of solar neutrino measurements and of the theory—both neutrino physics and solar astrophysics—employed in interpreting measurements. Important recent developments include Super-Kamiokande's determination of the ν−e elastic scattering rate for 8B neutrinos to 3%; the latest Sudbury Neutrino Observatory (SNO) global analysis in which the inclusion of low-energy data from SNO I and II significantly narrowed the range of allowed values for the neutrino mixing angle θ12; Borexino results for both the 7Be and proton-electron-proton (pep) neutrino fluxes, the first direct measurements constraining the rate of proton-proton (pp) I and pp II burning in the Sun; global reanalyses of solar neutrino data that take into account new reactor results on θ13; a new decadal evaluation of the nuclear physics of the pp chain and CNO cycle defining best values and uncertainties in the nuclear microphysics input to solar models; recognition of an emerging discrepancy between two tests of solar me...

200 citations


Journal ArticleDOI
TL;DR: In this article, the distance, extinction, and magnitude probability distributions of a successful core-collapse supernova (ccSN), its shock breakout radiation, and its massive star progenitor were modeled.
Abstract: No supernova (SN) in the Milky Way has been observed since the invention of the optical telescope, instruments for other wavelengths, neutrino detectors, or gravitational wave observatories. It would be a tragedy to miss the opportunity to fully characterize the next one. To aid preparations for its observations, we model the distance, extinction, and magnitude probability distributions of a successful Galactic core-collapse supernova (ccSN), its shock breakout radiation, and its massive star progenitor. We find, at very high probability ( 100%), that the next Galactic SN will easily be detectable in the near-IR and that near-IR photometry of the progenitor star very likely ( 92%) already exists in the Two Micron All Sky Survey. Most ccSNe (98%) will be easily observed in the optical, but a significant fraction (43%) will lack observations of the progenitor due to a combination of survey sensitivity and confusion. If neutrino detection experiments can quickly disseminate a likely position (~3°), we show that a modestly priced IR camera system can probably detect the shock breakout radiation pulse even in daytime (64% for the cheapest design). Neutrino experiments should seriously consider adding such systems, both for their scientific return and as an added and internal layer of protection against false triggers. We find that shock breakouts from failed ccSNe of red supergiants may be more observable than those of successful SNe due to their lower radiation temperatures. We review the process by which neutrinos from a Galactic ccSN would be detected and announced. We provide new information on the EGADS system and its potential for providing instant neutrino alerts. We also discuss the distance, extinction, and magnitude probability distributions for the next Galactic Type Ia supernova (SN Ia). Based on our modeled observability, we find a Galactic ccSN rate of per century and a Galactic SN Ia rate of per century for a total Galactic SN rate of per century is needed to account for the SNe observed over the last millennium, which implies a Galactic star formation rate of M ☉ yr–1.

162 citations


Journal ArticleDOI
TL;DR: In this article, the authors show that fitting short-baseline datasets to a 3 + 3 (3 + 2) model, defined by three active and three (two) sterile neutrinos, results in an overall goodness of fit of 67% (69%) and good compatibility between data sets.
Abstract: This paper reviews short-baseline oscillation experiments as interpreted within the context of one, two, and three sterile neutrino models associated with additional neutrino mass states in the ~1 eV range. Appearance and disappearance signals and limits are considered. We show that fitting short-baseline datasets to a 3 + 3 (3 + 2) model, defined by three active and three (two) sterile neutrinos, results in an overall goodness of fit of 67% (69%) and good compatibility between data sets—to be compared to a 3 + 1 model with a 55% goodness of fit. While the (3 + 3) fit yields the highest quality overall, it still finds inconsistencies with the MiniBooNE appearance datasets; in particular, the global fit fails to account for the observed MiniBooNE low-energy excess. Given the overall improvement, we recommend using the results of (3 + 2) and (3 + 3) fits, rather than (3 + 1) fits, for future neutrino oscillation phenomenology. These results motivate the pursuit of further short-baseline experiments, such as those reviewed in this paper.

Journal ArticleDOI
TL;DR: In this article, the distance, extinction, and magnitude probability distributions of a successful core-collapse supernova (ccSN), its shock breakout radiation, and its massive star progenitor are modeled.
Abstract: We model the distance, extinction, and magnitude probability distributions of a successful Galactic core-collapse supernova (ccSN), its shock breakout radiation, and its massive star progenitor. We find, at very high probability (~100%), that the next Galactic SN will easily be detectable in the near-IR and that near-IR photometry of the progenitor star very likely (~92%) already exists in the 2MASS survey. Most ccSNe (~98%) will be easily observed in the optical, but a significant fraction (~43%) will lack observations of the progenitor due to a combination of survey sensitivity and confusion. If neutrino detection experiments can quickly disseminate a likely position (~3 deg), we show that a modestly priced IR camera system can probably detect the shock breakout radiation pulse even in daytime (~64% for the cheapest design). Neutrino experiments should seriously consider adding such systems, both for their scientific return and as an added and internal layer of protection against false triggers. We find that shock breakouts from failed ccSNe of red supergiants may be more observable than those of successful SNe. We review the process by which neutrinos from a Galactic ccSN would be detected and announced. We provide new information on the EGADS system and its potential for providing instant neutrino alerts. We also discuss the distance, extinction, and magnitude probability distributions for the next Galactic Type Ia SN. Based on our modeled observability, we find a Galactic ccSN rate of 3.2 (+7.3/-2.6) per century and a Galactic Type Ia SN rate of 1.4 (+1.4/-0.8) per century for a total Galactic SN rate of 4.6 (+7.4/-2.7) per century is needed to account for the SNe observed over the last millennium.

Journal ArticleDOI
TL;DR: In this paper, the expected sensitivity of neutrino magnetic moment, electroweak mixing angle, and couplings to axial and vector currents were analyzed for three possible different phases of the Borexino experiment.
Abstract: The very low radioactive background of the Borexino detector, its large size, and the well proved capability to detect both low energy electron neutrinos and antineutrinos make an ideal case for the study of short distance neutrino oscillations with artificial sources at Gran Sasso. This paper describes the possible layouts of 51Cr (ν e ) and 144Ce-144Pr $$ \left( {{{\overline{ u}}_e}} \right) $$ source experiments in Borexino and shows the expected sensitivity to eV mass sterile neutrinos for three possible different phases of the experiment. Expected results on neutrino magnetic moment, electroweak mixing angle, and couplings to axial and vector currents are shown too.

Journal ArticleDOI
TL;DR: In this paper, a detailed analysis using the recent Super-Kamiokande data in the few tens of MeV range was performed to set limits on the WIMP-nucleon scattering cross section for dierent annihilation channels and computing the evaporation rate of WIMPs from the Sun for all values of the scattering cross-section in a consistent way.
Abstract: Annihilation of dark matter particles accumulated in the Sun would produce a flux of high-energy neutrinos whose prospects of detection in neutrino telescopes and detectors have been extensively discussed in the literature. However, for annihilations into Standard Model particles, there would also be a flux of neutrinos in the MeV range from the decays at rest of muons and positively charged pions. These low-energy neutrinos have never been considered before and they open the possibility to also constrain dark matter annihilation in the Sun into e + e , + or light quarks. Here we perform a detailed analysis using the recent Super-Kamiokande data in the few tens of MeV range to set limits on the WIMP-nucleon scattering cross section for dierent annihilation channels and computing the evaporation rate of WIMPs from the Sun for all values of the scattering cross section in a consistent way.

Journal ArticleDOI
K. Abe1, J. Adam2, Hiroaki Aihara1, T. Akiri3  +339 moreInstitutions (29)
TL;DR: The T2K Collaboration reports a precision measurement of muon neutrinos disappearance with an off-axis neutrino beam with a peak energy of 0.6 GeV, corresponding to the maximal oscillation disappearance probability.
Abstract: The T2K collaboration reports a precision measurement of muon neutrino disappearance with an off-axis neutrino beam with a peak energy of 0.6 GeV. Near detector measurements are used to constrain the neutrino flux and cross section parameters. The Super-Kamiokande far detector, which is 295 km downstream of the neutrino production target, collected data corresponding to 3.01×1020 protons on target. In the absence of neutrino oscillations, 205±17 (syst.) events are expected to be detected and only 58 muon neutrino event candidates are observed. A fit to the neutrino rate and energy spectrum assuming three neutrino flavors, normal mass hierarchy and θ23≤π/4 yields a best-fit mixing angle sin2(2θ23)=1.000 and mass splitting |Δm232|=2.44×10−3 eV2/c4. If θ23≥π/4 is assumed, the best-fit mixing angle changes to sin2(2θ23)=0.999 and the mass splitting remains unchanged.

Journal ArticleDOI
M. G. Aartsen1, Rasha Abbasi2, Y. Abdou3, Markus Ackermann  +280 moreInstitutions (39)
TL;DR: In this article, the authors report on the observation of anisotropy in the arrival direction distribution of cosmic rays at PeV energies using data taken between 2009 and 2012 with the IceTop air shower array at the south pole.
Abstract: We report on the observation of anisotropy in the arrival direction distribution of cosmic rays at PeV energies. The analysis is based on data taken between 2009 and 2012 with the IceTop air shower array at the south pole. IceTop, an integral part of the IceCube detector, is sensitive to cosmic rays between 100 TeV and 1 EeV. With the current size of the IceTop data set, searches for anisotropy at the 10(-3) level can, for the first time, be extended to PeV energies. We divide the data set into two parts with median energies of 400 TeV and 2 PeV, respectively. In the low energy band, we observe a strong deficit with an angular size of about 30 degrees and an amplitude of (-1.58 +/- 0.46(stat) +/- 0.52(sys)) x 10(-3) at a location consistent with previous observations of cosmic rays with the IceCube neutrino detector. The study of the high energy band shows that the anisotropy persists to PeV energies and increases in amplitude to (-3.11 +/- 0.38(stat) +/- 0.96(sys)) x 10(-3).

Posted Content
TL;DR: The Princeton Tritium Observatory for Light, Early-Universe, Massive-Neutrino Yield (PTOLEMY) experiment as mentioned in this paper was designed to achieve the sensitivity required to detect the relic neutrino background through a combination of a large area surface-deposition tritium target, MAC-E filter methods, cryogenic calorimetry, and RF tracking and time of flight systems.
Abstract: The PTOLEMY experiment (Princeton Tritium Observatory for Light, Early-Universe, Massive-Neutrino Yield) aims to achieve the sensitivity required to detect the relic neutrino background through a combination of a large area surface-deposition tritium target, MAC-E filter methods, cryogenic calorimetry, and RF tracking and time-of-flight systems. A small-scale prototype is in operation at the Princeton Plasma Physics Laboratory with the goal of validating the technologies that would enable the design of a 100 gram PTOLEMY. With precision calorimetry in the prototype setup, the limitations from quantum mechanical and Doppler broadening of the tritium target for different substrates will be measured, including graphene substrates. Beyond relic neutrino physics, sterile neutrinos contributing to the dark matter in the universe are allowed by current constraints on partial contributions to the number of active neutrino species in thermal equilibrium in the early universe. The current PTOLEMY prototype is expected to have unique sensitivity in the search for sterile neutrinos with electron-flavor content for masses of 0.1--1keV, where less stringent, 10eV, energy resolution is required. The search for sterile neutrinos with electron-flavor content with the 100g PTOLEMY is expected to reach the level $|U_{e4}|^2$ of $10^{-4}$--$10^{-6}$, depending on the sterile neutrino mass.

Journal ArticleDOI
TL;DR: It is shown that the diffuse isotropic neutrinos background from many distant sources can be consistent with the neutrino events recently detected by the IceCube experiment, and the narrow spectrum around 1 PeV implies that some active galactic nuclei can accelerate protons to EeV energies.
Abstract: The observed very high energy spectra of distant blazars are well described by secondary gamma rays produced in line-of-sight interactions of cosmic rays with background photons. In the absence of the cosmic-ray contribution, one would not expect to observe very hard spectra from distant sources, but the cosmic ray interactions generate very high energy gamma rays relatively close to the observer, and they are not attenuated significantly. The same interactions of cosmic rays are expected to produce a flux of neutrinos with energies peaked around 1 PeV. We show that the diffuse isotropic neutrino background from many distant sources can be consistent with the neutrino events recently detected by the IceCube experiment. We also find that the flux from any individual nearby source is insufficient to account for these events. The narrow spectrum around 1 PeV implies that some active galactic nuclei can accelerate protons to EeV energies.

Journal ArticleDOI
S. Adrián-Martínez1, I. Al Samarai2, A. Albert, Michel André3  +166 moreInstitutions (26)
TL;DR: In this paper, a search for high-energy neutrinos coming from the direction of the Sun has been performed using the data recorded by the ANTARES neutrino telescope during 2007 and 2008.
Abstract: A search for high-energy neutrinos coming from the direction of the Sun has been performed using the data recorded by the ANTARES neutrino telescope during 2007 and 2008. The neutrino selection criteria have been chosen to maximize the selection of possible signals produced by the self-annihilation of weakly interacting massive particles accumulated in the centre of the Sun with respect to the atmospheric background. After data unblinding, the number of neutrinos observed towards the Sun was found to be compatible with background expectations. The $90\%$ CL upper limits in terms of spin-dependent and spin-independent WIMP-proton cross-sections are derived and compared to predictions of two supersymmetric models, CMSSM and MSSM-7. The ANTARES limits are competitive with those obtained by other neutrino observatories and are more stringent than those obtained by direct search experiments for the spin-dependent WIMP-proton cross-section.

Journal ArticleDOI
TL;DR: In this article, the neutrino mass hierarchy was determined using a nuclear neutrinos experiment at ∼60 km, and the standard χ^2 method was compared with a proposed Fourier transformation method.
Abstract: Determination of the neutrino mass hierarchy using a reactor neutrino experiment at ∼60 km is analyzed. Such a measurement is challenging due to the finite detector resolution, the absolute energy scale calibration, and the degeneracies caused by current experimental uncertainty of |Δm_(32)^2|. The standard χ^2 method is compared with a proposed Fourier transformation method. In addition, we show that for such a measurement to succeed, one must understand the nonlinearity of the detector energy scale at the level of a few tenths of percent.

Journal ArticleDOI
TL;DR: In this paper, the physics potential of multi-megaton scale ice or water Cherenkov detectors with low (~ 1 GeV) threshold is explored, and the significance of the measurements of the neutrino parameters and the dependence of this significance on the accuracy of reconstruction of the Neutrino energy and direction is explored.
Abstract: We explore the physics potential of multi-megaton scale ice or water Cherenkov detectors with low (~ 1 GeV) threshold. Using some proposed characteristics of the PINGU detector setup we compute the distributions of events versus neutrino energy E ν and zenith angle θz , and study their dependence on yet unknown neutrino parameters. The (E ν − θz) regions are identified where the distributions have the highest sensitivity to the neutrino mass hierarchy, to the deviation of the 2-3 mixing from the maximal one and to the CP-phase. We evaluate significance of the measurements of the neutrino parameters and explore dependence of this significance on the accuracy of reconstruction of the neutrino energy and direction. The effect of degeneracy of the parameters on the sensitivities is also discussed. We estimate the characteristics of future detectors (energy and angle resolution, volume, etc.) required for establishing the neutrino mass hierarchy with high confidence level. We find that the hierarchy can be identified at 3σ-10σ level (depending on the reconstruction accuracies) after 5 years of PINGU operation.

Journal ArticleDOI
M. G. Aartsen1, Rasha Abbasi2, Y. Abdou3, Markus Ackermann  +284 moreInstitutions (38)
TL;DR: The first statistically significant detection of neutrino oscillations in the high-energy regime (>20 GeV) from an analysis of IceCube Neutrino Observatory data collected in 2010 and 2011 is presented.
Abstract: We present the first statistically significant detection of neutrino oscillations in the high-energy regime (> 20 GeV) from an analysis of IceCube Neutrino Observatory data collected in 2010 and 2011. This measurement is made possible by the low-energy threshold of the DeepCore detector (similar to 20 GeV) and benefits from the use of the IceCube detector as a veto against cosmic-ray-induced muon background. The oscillation signal was detected within a low-energy muon neutrino sample (20-100 GeV) extracted from data collected by DeepCore. A high-energy muon neutrino sample (100 GeV-10 TeV) was extracted from IceCube data to constrain systematic uncertainties. The disappearance of low-energy upward-going muon neutrinos was observed, and the nonoscillation hypothesis is rejected with more than 5 sigma significance. In a two-neutrino flavor formalism, our data are best described by the atmospheric neutrino oscillation parameters vertical bar Delta m(32)(2)vertical bar = (2.3(-0.5)(+0.6)) x 10(-3) eV(2) and sin(2) (2 theta(23)) > 0.93, and maximum mixing is favored.

Journal ArticleDOI
TL;DR: In this paper, the phase II data of the Mainz Neutrino Mass Experiment have been analyzed searching for a possible contribution of a fourth light neutrino mass state.
Abstract: The recent analysis of the normalization of reactor antineutrino data, the calibration data of solar neutrino experiments using gallium targets, and the results from the neutrino oscillation experiment MiniBooNE suggest the existence of a fourth light neutrino mass state with a mass of $\mathcal{O}~(\mathrm{eV})$ , which contributes to the electron neutrino with a sizable mixing angle. Since we know from measurements of the width of the Z0 resonance that there are only three active neutrinos, a fourth neutrino should be sterile (i.e., interact only via gravity). The corresponding fourth neutrino mass state should be visible as an additional kink in β-decay spectra. In this work the phase II data of the Mainz Neutrino Mass Experiment have been analyzed searching for a possible contribution of a fourth light neutrino mass state. No signature of such a fourth mass state has been found and limits on the mass and the mixing of this fourth mass state are derived.

Journal ArticleDOI
TL;DR: In this article, a large sample of cosmic muons is identified and tracked by a muon veto detector external to the liquid scintillator, and specific light patterns observed when muons cross the scintillation volume.
Abstract: The solar neutrino experiment Borexino, which is located in the Gran Sasso underground laboratories, is in a unique position to study muon-induced backgrounds in an organic liquid scintillator. In this study, a large sample of cosmic muons is identified and tracked by a muon veto detector external to the liquid scintillator, and by the specific light patterns observed when muons cross the scintillator volume. The yield of muon-induced neutrons is found to be Yn = (3.10?0.11)?10?4?n/(??(g/cm2)). The distance profile between the parent muon track and the neutron capture point has the average value ? = (81.5?2.7) cm. Additionally the yields of a number of cosmogenic radioisotopes are measured for 12N, 12B, 8He, 9C, 9Li, 8B, 6He, 8Li, 11Be, 10C and 11C. All results are compared with Monte Carlo simulation predictions using the FLUKA and GEANT4 packages. General agreement between data and simulation is observed for the cosmogenic production yields with a few exceptions, the most prominent case being 11C yield for which both codes return about 50% lower values. The predicted ?-n distance profile and the neutron multiplicity distribution are found to be overall consistent with data.

Journal ArticleDOI
TL;DR: In this paper, the authors show that the inclusion of this correction in the analysis is expected to lead to an increase of the best oscillationmass parameters, particularly pronounced for the MiniBooNE neutrino data.
Abstract: Data on neutrino oscillation often involve reconstructed neutrino energies while the analysisimplies the real neutrino energy. The corrections corresponding to the transformation from real toreconstructed energy are discussed in the case of Cherenkov detectors where multinucleon eventsappear as quasielastic ones. These corrections show up as a tendency for the events to escapethe region of high flux, with a clear preference for the low energy side. This is an effect of themultinucleon component of the quasielastic cross section. We have applied our corrections to theT2K and MiniBooNE data for electron appearance or ν µ disappearance data. We show that theinclusion of this correction in the analysis is expected to lead to an increase of the best fit oscillationmass parameters, particularly pronounced for the MiniBooNE neutrino data. This inclusion inthe analysis of the MiniBooNE neutrino data should improve the compatibility with the existingconstraints. PACS numbers: 13.15.+g, 25.30.Pt, 14.60.Pq

Journal ArticleDOI
TL;DR: The outermost component of ND280 is a side muon range detector (SMRD) composed of scintillation counters with embedded wavelength shifting fibers and Multi-Pixel Photon Counter read-out as mentioned in this paper.
Abstract: The T2K experiment is a long baseline neutrino oscillation experiment aiming to observe the appearance ofe in a �µ beam. The �µ beam is produced at the Japan Proton Accelerator Research Complex (J-PARC), observed with the 295 km distant Super- Kamiokande Detector and monitored by a suite of near detectors at 280m from the proton target. The near detectors include a magnetized off-axis detector (ND280) which measures the un-oscillated neutrino flux and neutrino cross sections. The present paper describes the outermost component of ND280 which is a side muon range detector (SMRD) composed of scintillation counters with embedded wavelength shifting fibers and Multi-Pixel Photon Counter read-out. The components, performance and response of the SMRD are presented.

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D. Allan1, C. Andreopoulos1, C. Angelsen1, Gareth J. Barker2, G.D. Barr3, S. W. Bentham4, Iain Alexander Bertram4, S. B. Boyd2, K. Briggs2, R. G. Calland5, J. Carroll5, S. L. Cartwright6, A. Carver2, C. A. Chavez5, G. Christodoulou5, J. P. Coleman5, P.A. Cooke5, Gavin Davies4, C. Densham1, F. Di Lodovico7, J. Dobson8, T. Duboyski7, T. Durkin1, D L Evans5, Alexander Finch4, M. Fitton1, Fred Gannaway7, Alastair Grant9, N. Grant4, S Grenwood8, P. Guzowski8, D. R. Hadley2, M. D. Haigh3, Paul Fraser Harrison2, A. Hatzikoutelis4, T. D. J. Haycock6, A. Hyndman7, J. Ilic1, S. J. Ives8, A. C. Kaboth8, V. Kasey8, L. Kellet5, M. Khaleeq8, G. Kogan8, L. L. Kormos4, M. Lawe6, T. B. Lawson6, C. Lister2, R. P. Litchfield2, M. Lockwood5, M. Malek8, T. Maryon4, P. Masliah8, K. Mavrokoridis5, N. McCauley5, I. Mercer4, C. J. Metelko1, B. Morgan2, John Morris7, A. Muir9, M. Murdoch5, T. Nicholls1, M. Noy8, H. M. O'Keeffe3, R. A. Owen7, D. Payne5, G. F. Pearce1, J. D. Perkin6, E. Poplawska7, Robert D. Preece1, W. Qian1, P. N. Ratoff4, T. M. Raufer1, Michel Raymond8, Matthew T. Reeves4, D. Richards2, M. Rooney1, R. Sacco7, S. W. Sadler6, P. Schaack8, Mark Scott8, D. I. Scully2, S. Short8, M. Siyad1, Richard J.H. Smith3, B. Still7, P. Sutcliffe5, I. Taylor2, R. Terri7, Lester D.R. Thompson6, A. Thorley5, M. Thorpe1, C. N. Timis7, C. Touramanis5, M A Uchida7, Y. Uchida8, Antonin Vacheret3, J. F. van Schalkwyk8, Omar Veledar6, A. V. Waldron3, M. A. Ward6, G. P. Ward6, D. L. Wark3, D. L. Wark1, M. O. Wascko8, A. C. Weber3, A. C. Weber1, N. West3, Leigh H. Whitehead2, C. Wilkinson6, J. R. Wilson7 
TL;DR: The ND280 electromagnetic calorimeter (ECal) as mentioned in this paper is an off-axis, near detector, located 280 m downstream of the neutrino production target in order to measure the properties of the Neutrino beam and to understand better neutrinos interactions at the energy scale below a few GeV.
Abstract: The T2K experiment studies oscillations of an off-axis muon neutrino beam between the J-PARC accelerator complex and the Super-Kamiokande detector. Special emphasis is placed on measuring the mixing angle θ13 by observing νe appearance via the sub-dominant νμ → νe oscillation and searching for CP violation in the lepton sector. The experiment includes a sophisticated, off-axis, near detector, the ND280, situated 280 m downstream of the neutrino production target in order to measure the properties of the neutrino beam and to understand better neutrino interactions at the energy scale below a few GeV. The data collected with the ND280 are used to study charged- and neutral-current neutrino interaction rates and kinematics prior to oscillation, in order to reduce uncertainties in the oscillation measurements by the far detector. A key element of the near detector is the ND280 electromagnetic calorimeter (ECal), consisting of active scintillator bars sandwiched between lead sheets and read out with multi-pixel photon counters (MPPCs). The ECal is vital to the reconstruction of neutral particles, and the identification of charged particle species. The ECal surrounds the Pi-0 detector (POD) and the tracking region of the ND280, and is enclosed in the former UA1/NOMAD dipole magnet. This paper describes the design, construction and assembly of the ECal, as well as the materials from which it is composed. The electronic and data acquisition (DAQ) systems are discussed, and performance of the ECal modules, as deduced from measurements with particle beams, cosmic rays, the calibration system, and T2K data, is described.

Journal ArticleDOI
S. Adrián-Martínez1, Arnauld Albert, I. Al Samarai2, Michel André3  +154 moreInstitutions (23)
TL;DR: In this article, the authors search for muon neutrinos in coincidence with GRBs with the ANTARES neutrino detector using data from the end of 2007 to 2011.
Abstract: Aims. We search for muon neutrinos in coincidence with GRBs with the ANTARES neutrino detector using data from the end of 2007 to 2011. Methods. Expected neutrino fluxes were calculated for each burst individually. The most recent numerical calculations of the spectra using the NeuCosmA code were employed, which include Monte Carlo simulations of the full underlying photohadronic interaction processes. The discovery probability for a selection of 296 GRBs in the given period was optimised using an extended maximum-likelihood strategy. Results. No significant excess over background is found in the data, and 90% confidence level upper limits are placed on the total expected flux according to the model.

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TL;DR: In this paper, the neutrino flux in PeV energies produced by untriggered GRBs is about two times higher than that produced by triggered ones, and the total flux of triggered and untrigged GRBs can reach at most a level of ~10-9 GeV cm−2 s−1 sr−1, which is insufficient to account for the reported two PeV neutrinos.
Abstract: The IceCube Collaboration recently reported the potential detection of two cascade neutrino events in the energy range 1-10 PeV. We study the possibility that these PeV neutrinos are produced by gamma-ray bursts (GRBs), paying special attention to the contribution by untriggered GRBs that elude detection due to their low photon flux. Based on the luminosity function, rate distribution with redshift and spectral properties of GRBs, we generate, using a Monte Carlo simulation, a GRB sample that reproduces the observed fluence distribution of Fermi/GBM GRBs and an accompanying sample of untriggered GRBs simultaneously. The neutrino flux of every individual GRB is calculated in the standard internal shock scenario, so that the accumulative flux of the whole samples can be obtained. We find that the neutrino flux in PeV energies produced by untriggered GRBs is about two times higher than that produced by the triggered ones. Considering the existing IceCube limit on the neutrino flux of triggered GRBs, we find that the total flux of triggered and untriggered GRBs can reach at most a level of ~10–9 GeV cm–2 s–1 sr–1, which is insufficient to account for the reported two PeV neutrinos. Possible contributions to diffuse neutrinos by low-luminosity GRBs and the earliest population of GRBs are also discussed.

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TL;DR: The India-based Neutrino Observatory (INO) will host a 50 kt magnetized iron calorimeter (ICAL@INO) for the study of atmospheric neutrinos.
Abstract: The India-based Neutrino Observatory (INO) will host a 50 kt magnetized iron calorimeter (ICAL@INO) for the study of atmospheric neutrinos. Using the detector resolutions and efficiencies obtained by the INO collaboration from a full-detector GEANT4-based simulation, we determine the reach of this experiment for the measurement of the atmospheric neutrino mixing parameters $ \left( {\sin^2 {\theta_{23 }}\;\mathrm{and}\left| {\varDelta m_{32}^2} \right|} \right) $ . We also explore the sensitivity of this experiment to the octant of θ 23, and its deviation from maximal mixing.