Building an Experiment at the Bottom of the Sea to Detect
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Search for Neutrinos from TANAMI Observed AGN Using Fermi
Search for neutrinos from TANAMI observed AGN using Fermi lightcurves with ANTARES Suche nach Neutrinos von TANAMI-AGN unter Verwendung von Fermi-Lichtkurven mit ANTARES Der Naturwissenschaftlichen Fakultät der Friedrich-Alexander-Universität Erlangen-Nürnberg zur Erlangung des Doktorgrads Dr. rer. nat. vorgelegt von Kerstin Fehn Als Dissertation genehmigt von der Naturwissenschaftlichen Fakultät der Friedrich-Alexander Universität Erlangen-Nürnberg Tag der mündlichen Prüfung: 24.03.2015 Vorsitzender des Promotionsorgans: Prof. Dr. Jörn Wilms Gutachter/in: Prof. Dr. Gisela Anton Prof. Dr. Ulrich Katz ν Abstract Active galactic nuclei (AGN) are promising candidates for hadronic acceleration. The combination of radio, gamma ray and neutrino data should give information on their properties, especially concerning the sources of the high-energetic cosmic rays. Assuming a temporal correlation of gamma and neutrino emission in AGN the background of neutrino telescopes can be reduced using gamma ray lightcurves. Thereby the sensitivity for discovering cosmic neutrino sources is enhanced. In the present work a stacked search for a group of AGN with the ANTARES neutrino telescope in the Mediterranean is presented. The selection of AGN is based on the source sample of TANAMI, a multiwavelength observation program (radio to gamma rays) of extragalactic jets southerly of −30◦ declination. In the analysis lightcurves of the gamma satellite Fermi are used. In an unbinned maximum likelihood approach the test statistic in the background only case and in the signal and background case is determined. For the investigated 10% of data of ANTARES within the measurement time between 01.09.2008 and 30.07.2012 no significant excess is observed. -
Panel 1: 3-Flavor Neutrino Oscillation
Panel 1: 3-flavor Neutrino Oscillation Marcos Dracos,1 Mark Hartz,2, 3 Patrick Huber,4 Ryan Patterson,5 Serguey Petcov,6 and Ewa Rondio7 1IPHC, Universit´ede Strasbourg, CNRS/IN2P3, F-67037 Strasbourg, France 2TRIUMF, Canada 3Kavli IPMU (WPI), University of Tokyo 4Center for Neutrino Physics, Virginia Tech, Blacksburg, USA 5California Institute of Technology, Pasadena, USA 6SISSA/INFN, Trieste, Italy, and Kavli IPMU (WPI), University of Tokyo, Kashiwa, Japan 7National Centre for Nuclear Research (NCBJ), Warsaw, Poland (Dated: November 6, 2018) PREAMBLE tence of new fundamental symmetry in the lepton sector. The most distinctive feature of the symmetry approach to In this brief document we will focus on experimental neutrino mixing are the predictions of the values of some programs and ideas which have at some level been rec- of the neutrino mixing angles and leptonic CP phases, ognized by funding agencies, either by outright funding and/or of existence of correlations between the values of them or by at least providing significant support for the at least some the neutrino mixing angles and/or between R&D for the neutrino oscillation related aspects of the the values of the neutrino mixing angles and the Dirac program. CP phase in the PMNS matrix, etc. This implies that a sufficiently precise measurement of the Dirac phase δ of the PMNS neutrino mixing matrix in current and future neutrino oscillation experiments, combined with planned INTRODUCTION improvements of the precision on the neutrino mixing an- gles, might provide unique information about the possible The discovery of neutrino oscillation dates back two discrete symmetry origin of the observed pattern of neu- decades and to this day is the most direct laboratory ev- trino mixing and, correspondingly, about the existence of idence for the existence of physics beyond the Standard new fundamental symmetry in the lepton sector. -
The ANTARES and Km3net Neutrino Telescopes: Status and Outlook for Acoustic Studies
EPJ Web of Conferences 216, 01004 (2019) https://doi.org/10.1051/epjconf/201921601004 ARENA 2018 The ANTARES and KM3NeT neutrino telescopes: Status and outlook for acoustic studies Véronique Van Elewyck1,2, for the ANTARES and KM3NeT Collaborations 1APC, Université Paris Diderot, CNRS/IN2P3, CEA/Irfu, Observatoire de Paris, Sorbonne Paris Cité, France 2Institut Universitaire de France, 75005 Paris, France Abstract. The ANTARES detector has been operating continuously since 2007 in the Mediterranean Sea, demonstrating the feasibility of an undersea neutrino telescope. Its superior angular resolution in the reconstruction of neutrino events of all flavors results in unprecedented sensitivity for neutrino source searches in the southern sky at TeV en- ergies, so that valuable constraints can be set on the origin of the cosmic neutrino flux discovered by the IceCube detector. The next generation KM3NeT neutrino telescope is now under construction, featuring two detectors with the same technology but different granularity: ARCA designed to search for high energy (TeV-PeV) cosmic neutrinos and ORCA designed to study atmospheric neutrino oscillations at the GeV scale, focusing on the determination of the neutrino mass hierarchy. Both detectors use acoustic devices for positioning calibration, and provide testbeds for acoustic neutrino detection. 1 Introduction Neutrinos have long been proposed as a complementary probe to cosmic rays and photons to explore the high-energy (HE) sky, as they can emerge from dense media and travel across cosmological dis- tances without being deflected by magnetic fields nor absorbed by inter- and intra-galactic matter and radiation. HE (>TeV) neutrinos are expected to be emitted in a wide range of astrophysical objects. -
Neutrino Telescopes
Neutrino Telescopes Gisela Anton Erlangen Centre for Astroparticle Physics, University Erlangen-Nürnberg, Erwin–Rommel-Str. 1, 91058 Erlangen, Germany [email protected] This paper addresses the working principle of neutrino telescopes, im- portant detector parameters as well as the layout and performance of current and future neutrino telescopes. It was prepared for the book "Probing Particle Physics with Neutrino Telescopes", C. Pérez de los Heros, editor, 2020 (World Scientific) in 2018. 1 Introductory considerations Usual astronomical telescopes determine the intensity respectively the spectral density of light arriving from a certain direction at Earth. The analogue task of a neutrino telescope is the detection of neutrinos determining their direction and energy. While visible photons can be collected and directed with mirrors no analogue mechanism exists for neutrinos. This implies that the phase space (area and direction) of neutrinos cannot be changed. So, the strategy is to detect single neutrinos and for each single neutrino to determine its direction and energy from the interaction characteristics and from energy and momenta of secondary particles produced in the neutrino interaction. Neutrinos only feel the weak force resulting in a rather low probability of interaction with matter. For a large energy regime the neutrino-nucleon cross section increases linearly with energy E while for most of the expected neutrino sources the emitted flux decreases with energy as E−2 or even steeper. This implies that a neutrino telescope needs the more target mass the higher the envisaged neutrino energy regime is. To give a rough orientation, usual neutrino detectors employ a Megaton target mass for the GeV energy regime and a Gigaton mass for the TeV energy regime. -
Methods and Problems in Low Energy Neutrino Experiments (Solar, Reactors, Geo-)
Methods and problems in low energy neutrino experiments (solar, reactors, geo-) I G. Ranucci ISAPP 2011 International School on Astroparticle physics THE NEUTRINO PHYSICS AND ASTROPHYSICS July 26th - August 5th, 2011 Varenna - Italy Summary of the topics -Neutrino detection overview -Radiochemical methodology -Scintillation methods -Cerenkov approach -Low background implications in low energy neutrino search With examples of applications taken from experiments and geo-neutrinos (anti-ν)ν)ν) (not discussed here) fundamental Neutrino production in the Sun In our star > 99% of the energy is created in this reaction The pp chain reaction The CNO cycle In the Sun < 1% More important in heavier stars There are different steps in which energy (and neutrinos) are produced pp ν νν from: Monocrhomatic ν’s (2 bodies in the final state) pp pep CNO ννν from: 7Be 13 N 8B 15 O hep 17 F Rome - 3 July, 2009 Gioacchino Ranucci - I.N.F.N. Sez. di Milano Neutrino production in the Sun Neutrino energy spectrum as predicted by the Solar Standard Model (SSM) John Norris Bahcall (Dec. 30 , 1934 – Aug. 17 , 2005 ) 7Be: 384 keV (10%) 862 keV (90%) Pep: 1.44 MeV Rome - 3 July, 2009 Gioacchino Ranucci - I.N.F.N. Sez. di Milano Solar neutrino experiments: a more than four decades long saga Radiochemical experiments Homestake (Cl) Gallex/GNO (Ga) Sage (Ga) Real time Cherenkov experiments Kamiokande/Super-Kamiokande SNO Scintillator experiments Borexino Rome - 3 July, 2009 Gioacchino Ranucci - I.N.F.N. Sez. di Milano This is equivalent to find a needle in a haystack -
Acoustic Particle Detection – from Early Ideas to Future Benefits
Nuclear Instruments and Methods in Physics Research A ] (]]]]) ]]]–]]] Contents lists available at ScienceDirect Nuclear Instruments and Methods in Physics Research A journal homepage: www.elsevier.com/locate/nima Acoustic particle detection – From early ideas to future benefits Rolf Nahnhauer n Deutsches Elektronen-Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, Germany article info abstract The history of acoustic neutrino detection technology is shortly reviewed from the first ideas 50 years ago Keywords: to the detailed R&D programs of the last decade. The physics potential of ultra-high energy neutrino Cosmogenic neutrinos interaction studies is discussed for some examples. Ideas about the necessary detector size and suitable Ultra-high energy neutrino detection design are presented. Acoustic detection technology & 2010 Elsevier B.V. All rights reserved. 1. The dawn of neutrino astroparticle physics 2. First ideas about ‘‘particle sound’’ Very soon after the 1956 Science publication of Cowan et al. [1] Fifty years ago a well developed method to observe elementary about the discovery of neutrino interactions at the Savannah River particles in accelerator and cosmic ray experiments was to look for light reactor first ideas about experiments detecting neutrinos produced in they produced through Cherenkov radiation or scintillation effects the Earth atmosphere or in distant astrophysical sources appeared. In when passing transparent media. At accelerators bubble chambers his talk ‘‘On high energy neutrino physics’’ at the 1960 Rochester started their two decades lasting successful application, having their conference [2] Markov stated: ‘‘in papers by Zhelesnykh1 and myself working principle still under study. In this context Askaryan [6] (1958, 1960) possibilities of experiments with cosmic ray neutrinos published in 1957 a paper about ‘‘Hydrodynamic radiation from the are analyzed. -
The ANTARES Collaboration
PROCEEDINGS OF THE 31st ICRC, ŁOD´ Z´ 2009 1 The ANTARES Collaboration: contributions to the 31st International Cosmic Ray Conference (ICRC 2009), Lodz, Poland, July 2009 Abstract The Antares neutrino telescope, operating at 2.5 km depth in the Mediterranean Sea, 40 km off the Toulon shore, represents the world’s largest operational underwater neutrino telescope, optimized for the detection of Cerenkov light produced by neutrino-induced muons. The main goal of Antares is the search of high energy neutrinos from astrophysical point or transient sources. Antares is taking data in its full 12 lines configuration since May 2008: in this paper we collect the 16 contributions by the ANTARES collaboration that were submitted to the 31th International Cosmic Ray Conference ICRC 2009. These contributions includes the detector performances, the first preliminary results on neutrino events and the current physics analysis including the sensitivity to point like sources, the possibility to detect high energy neutrinos in coincidence with GRB, the search for dark matter or exotic particles. arXiv:1002.0701v1 [astro-ph.HE] 3 Feb 2010 2 THE ANTARES COLLABORATION ANTARES Collaboration J.A. Aguilar1, I. Al Samarai2, A. Albert3, M. Anghinolfi4, G. Anton5, S. Anvar6, M. Ardid7, A.C. Assis Jesus8, T. Astraatmadja8; a, J.J. Aubert2, R. Auer5, B. Baret9, S. Basa10, M. Bazzotti11; 12, V. Bertin2, S. Biagi11; 12, C. Bigongiari1, M. Bou-Cabo7, M.C. Bouwhuis8, A. Brown2, J. Brunner2; b, J. Busto2, F. Camarena7, A. Capone13; 14, C.C^arloganu15, G. Carminati11; 12, J. Carr2, E. Castorina16; 17, V. Cavasinni16; 17, S. Cecchini12; 18, Ph. -
ANNUAL REPORT (APRIL 2016 – MARCH 2017) Editorial Board MIYOKI, Shinji YOSHIKOSHI, Takanori TAKENAGA, Yumiko FUKUDA, Hironobu
INSTITUTE FOR COSMIC RAY RESEARCH THE UNIVERSITY OF TOKYO ANNUAL REPORT (APRIL 2016 – MARCH 2017) Editorial Board MIYOKI, Shinji YOSHIKOSHI, Takanori TAKENAGA, Yumiko FUKUDA, Hironobu c Institute for Cosmic Ray Research, The University of Tokyo 5-1-5, Kashiwanoha, Kashiwa, Chiba 277-8582, Japan Telephone: (81) 4-7136-3102 Facsimile: (81) 4-7136-3115 WWW URL: http://www.icrr.u-tokyo.ac.jp/ TABLE OF CONTENTS Preface Research Divisions ......................................................................................... 1 Neutrino and Astroparticle Division 2 High Energy Cosmic Ray Division 28 Astrophysics and Gravity Division 52 Observatories and a Research Center ......................................................................... 65 Norikura Observatory 66 Akeno Observatory 72 Kamioka Observatory 75 Kagra Observatory 76 Research Center for Cosmic Neutrinos 77 Appendix A. ICRR Workshops and Ceremonies ............................................................. 79 Appendix B. ICRR Seminars .............................................................................. 82 Appendix C. List of Publications .......................................................................... 82 (a) Papers Published in Journals (b) Conference Papers (c) ICRR Reports Appendix D. Doctoral Theses ............................................................................. 89 Appendix E. Public Relations ............................................................................. 89 (a) ICRR News (b) Public Lectures (c) Visitors Appendix F. Inter-University -
A Deep Ocean Anti-Neutrino Detector Near Hawaii
Part I: Project Summary A Deep Ocean Anti-Neutrino Detector near Hawaii In Response to: CEROS-CORE-05-01 The National Defense Center of Excellence for Research in Ocean Sciences (CEROS) 73-4460 Queen Kaahumanu Highway, Suite 111 Kailua-Kona, Hawaii 96740 Objectives/Result: Design and initial component testing of a deep ocean anti-neutrino detector for the presence of both natural and man-made nuclear activity. Period of Performance: 12 months (June 2005 - May 2006) Funding Requirements: $686,000 Subcontractors: University of Hawaii, Manoa High Energy Physics Principal Investigator: Dr. Joseph Van Ryzin, President Makai Ocean Engineering, Inc. [email protected] Co-Principal Investigator: Dr. John Learned, Professor Department of Physics and Astronomy University of Hawaii, Manoa [email protected] Administrative Contact: Dr. Michael Nedbal Makai Ocean Engineering, Inc. [email protected] Contact Address: Makai Ocean Engineering, Inc. PO Box 1206 Kailua, Hawaii 96734 [email protected] Phone: (808) 259-8871 Fax (808) 259-8238 January 26, 2005 Project Summary A Deep Ocean Anti-Neutrino Detector near Hawaii Summary, Proposed Effort We propose to initiate a project to build a deep ocean detector to measure low energy anti-neutrinos from radioactive decays. These anti-neutrinos arise from decays throughout the Earth, from a theoretical natural reactor at the Earth's core, and from man-made nuclear reactors or nuclear weapon testing. Such a detector has great value for both geophysical science and nuclear proliferation deterrence. A proposed initial detector is conceptually shown in Figure 1; it is 20m in diameter. Subsequent nuclear deterrent detectors would most likely be even larger. -
Arxiv:1806.05058V1 [Hep-Ph] 13 Jun 2018
Prospects of indirect searches for dark matter annihilations in the earth with ICAL@INO Deepak Tiwari,1, ∗ Sandhya Choubey,1, 2, y and Anushree Ghosh3, z 1Harish-Chandra Research Institute (HBNI), Chhatnag Road, Jhunsi, Allahabad 211 019, India 2Department of Physics, School of Engineering Sciences, KTH Royal Institute of Technology, AlbaNova University Centre, 106 91 Stockholm, Sweden 3Universidad Tecnica Federico Santa Maria - Departamento de Fisica Casilla 110-V, Avda. Espana 1680, Valparaiso, Chile Abstract We study the prospects of detecting muon events at the upcoming Iron CALorimeter (ICAL) detector to be built at the proposed India-based Neutrino Observatory (INO) facility due to neutrinos arising out of annihilation of Weakly Interactive Massive Particles (WIMP) in the centre of the earth. The atmospheric neutrinos coming from the direction of earth core presents an irreducible background. We consider 50kt × 10 years of ICAL running and WIMP masses between 10-100 GeV and present 90 % C.L. exclusion sensitivity limits on σSI which is the WIMP-nucleon Spin Independent (SI) interaction cross-section. The expected sensitivity limits calculated for ICAL for the WIMP annihilation in the earth are more stringent than the limits obtained by any other indirect detection experiment. For a WIMP mass of 52:14 GeV, where the signal fluxes are enhanced due to resonance capture of WIMP in earth due to Fe nuclei, the sensitivity −44 2 + − limits, assuming 100% branching ratio for each channel, are : σSI = 1:02 × 10 cm for the τ τ −44 2 ¯ channel and σSI = 5:36 × 10 cm for the b b channel. arXiv:1806.05058v1 [hep-ph] 13 Jun 2018 ∗Electronic address: [email protected] yElectronic address: [email protected] zElectronic address: [email protected] 1 I. -
History of High-Energy Neutrino Astronomy
History of high-energy neutrino astronomy C. Spiering DESY, Platanenallee 6, D-15738 Zeuthen, Germany This talk sketches the main milestones of the path towards cubic kilometer neutrino telescopes. It starts with the first conceptual ideas in the late 1950s and describes the emergence of concepts for detectors with a realistic discovery potential in the 1970s and 1980s. After the pioneering project DUMAND close to Hawaii was terminated in 1995, the further development was carried by NT200 in Lake Baikal, AMANDA at the South Pole and ANTARES in the Mediterranean Sea. In 2013, more than half a century after the first concepts, IceCube has discovered extraterrestrial high-energy neutrinos and opened a new observational window to the cosmos { marking a milestone along a journey which is far from being finished. 1 From first concepts to the detection of atmospheric neutrinos The initial idea of neutrino astronomy beyond the solar system rested on two arguments: The first was the expectation that a supernova stellar collapse in our galaxy would be accompanied by an enormous burst of neutrinos in the 5-10 MeV range. The second was the expectation that fast rotating pulsars must accelerate charged particles in their Tera-Gauss magnetic fields. Either in the source or on their way to Earth they must hit matter, generate pions and neutrinos as decay products of the pions. The first ideas to detect cosmic high energy neutrinos underground or underwater date back to the late fifties (see 1 for a detailed history of cosmic neutrino detectors). In the 1960 Annual Review of Nuclear Science, K. -
Neutrino Astrophysics Astrophysics and Astronomy
Neutrino Astrophysics and Astronomy Madhurima Pandey Astroparticle Physics and Cosmology Division Saha Institute of Nuclear Physics, HBNI, Kolkata WHEPP XVI, IIT Guwahati Wednesday, December 4, 2019 WHEPP XVI 1 Wednesday, December 4, 2019 WHEPP XVI 2 Solar Neutrino Wednesday, December 4, 2019 WHEPP XVI 3 Solar Neutrino Neutrino and antineutrino production mechanism [1] Rates proportional to , and - depend on specific processes, and - effective coupling constants for vector and axial – vector interaction. Antineutrinos can be probed at the Earth detector in KeV energy range. [1] E. Vitagliano et al., JCAP 12, 010 (2017) Wednesday, December 4, 2019 WHEPP XVI 4 Solar Neutrino sterile neutrinos in KeV range - 1. capture on a stable isotope of dysprosium if > 2.83 KeV [2] 2. slightly heavier sterile neutrinos include unstable isotopes[3] coherent inelastic scattering on atoms [4] and electron scattering [5] CP violation MSW effect [2] T. Lasserre et al., arXiv:1609.04671, [3] Y.F. Li et al., Phys. Lett. B 695 (2011) 205, [4] S. Ando et al., Phys. Rev. D 81 (2010) 113006, [5] M.D. Campos et al., Phys. Rev. D 94 (2016) 095010 Wednesday, December 4, 2019 WHEPP XVI 5 Atmospheric(ATM) Neutrino ATM neutrinos at Super Kamiokande (SK) experiment confirmed neutrino flavour oscillation – established the existence of neutrino masses and mixing Discovery of flavour oscillation of ATM neutrinos in 2015 Cosmic ray particles collide with the nuclei in the Earth’s atmosphere, producing pions and kaons which decay into neutrinos First observations of ATM neutrinos in 1965 at kolar Gold experiment in India and simultaneously led by Fred Reines in South Africa – looking for proton decay – the discrepancy was resolved by the SK experiments Wednesday, December 4, 2019 WHEPP XVI 6 ATM Neutrino ATM neutrino detector – 1.