A Search for Astrophysical Tau Neutrinos with Icecube Using an Advanced Statistical Approach
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Snowmass 2021 Letter of Interest: Ultra-High-Energy Neutrinos
Snowmass 2021 Letter of Interest: Ultra-High-Energy Neutrinos Markus Ahlers,1 Jaime Alvarez-Mu~niz,´ 2 Rafael Alves Batista,3 Luis Anchordoqui,4 Carlos A. Arg¨uelles,5 Jos´e Bazo,6 James Beatty,7 Douglas R. Bergman,8 Dave Besson,9, 10 Stijn Buitink,11 Mauricio Bustamante,1, 12, ∗ Olga Botner,13 Anthony M. Brown,14 Washington Carvalho Jr.,15 Pisin Chen,16 Brian A. Clark,17 Amy Connolly,7 Linda Cremonesi,18 Cosmin Deaconu,19 Valentin Decoene,20 Paul de Jong,21, 22 Sijbrand de Jong,23, 22 Peter B. Denton,24, y Krijn De Vries,25 Michele Doro,26 Michael A. DuVernois,27 Ke Fang,28 Christian Glaser,13 Peter Gorham,29 Claire Gu´epin,30 Allan Hallgren,13 Jordan C. Hanson,31 Tim Huege,32, 11 Martin H. Israel,33 Albrecht Karle,27 Spencer R. Klein,34, 35 Kumiko Kotera,20 Ilya Kravchenko,36 John Krizmanic,30, 37 John G. Learned,29 Olivier Martineau-Huynh,38 Peter M´esz´aros,39 Thomas Meures,27 Miguel A. Mostaf´a,39, 40 Katharine Mulrey,11 Kohta Murase,39, 40, 41 Jiwoo Nam,16 Anna Nelles,42, 43 Eric Oberla,44 Foteini Oikonomou,45 Angela V. Olinto,44 Yasar Onel,46 A. Nepomuk Otte,47 Sergio Palomares-Ruiz,48 Alex Pizzuto,27 Steven Prohira,7 Brian Rauch,49 Mary Hall Reno,46 Juan Rojo,50, 51 Andr´esRomero-Wolf,52 Ibrahim Safa,5, 27 Olaf Scholten,53, 25 Frank G. Schr¨oder,54, 32 Wayne Springer,55 Irene Tamborra,1, 12 Charles Timmermans,51, 23 Diego F. Torres,56 Jo~aoR. -
Neutrino Astrophysics
Neutrino Astrophysics Ryan Nichol UK Input to European Strategy Neutrino Astrophysics Ryan Nichol UK Input to European Strategy Highly cited papers • Higgs Discovery (2012) • Z discovery (1983) –1500+ – 8000+ citations –2000+ • SN1987a neutrinos (1987) • Atmospheric neutrino • Positron excess –1500+ oscillations (1998) [PAMELA] (2008) • Weak neutral current –5000+ citations –1900+ (1973) • Top quark discovery • Reactor neutrino theta_13 –1500+ (1995) (2012) • Charmomium (2003) –3000+ citations –1900+ –1400+ • Solar neutrino oscillations • b-quark discovery (1977) • B-Bbar oscillation (1987) (2002) –1900+ –1300+ –3000+ citations • W-discovery (1983) • nu_mu -> nu_e (2011) • Kaon CP violations (1964) –1800+ –1300+ –3000+ citations • Z width (2005) • Accelerator neutrino • Reactor antineutrino –1700+ oscillation (2002) [KamLAND] (2003) • Proton spin crisis (1989) –1100+ –2000+ citations –1700+ • Muon neutrino discovery • Gravitational Waves • LSND anomaly (2001) (1962) (2016) –1700+ –1100+ –2000+ citations • Parity non conservation • DAMA/Libra (2008-) • c-quark discovery (1974) (1957) –1000+ –2000+ citations –1600+ • Pentaquark [LEPS] (2003) • Solar neutrino • LUX Dark Matter (2013) –1000+ [Homestake] (1968-1998) –1500+ • Neutron EDM (2006) !3 –2000+ • g-2 (2006) –1000+ Highly cited papers • Higgs Discovery (2012) • Z discovery (1983) –1500+ – 8000+ citations –2000+ • SN1987a neutrinos (1987) • Atmospheric neutrino • Positron excess –1500+ oscillations (1998) [PAMELA] (2008) • Weak neutral current –5000+ citations –1900+ (1973) • Top quark -
The Gran Sasso Underground Laboratory Program
The Gran Sasso Underground Laboratory Program Eugenio Coccia INFN Gran Sasso and University of Rome “Tor Vergata” [email protected] XXXIII International Meeting on Fundamental Physics Benasque - March 7, 2005 Underground Laboratories Boulby UK Modane France Canfranc Spain INFN Gran Sasso National Laboratory LNGSLNGS ROME QuickTime™ and a Photo - JPEG decompressor are needed to see this picture. L’AQUILA Tunnel of 10.4 km TERAMO In 1979 A. Zichichi proposed to the Parliament the project of a large underground laboratory close to the Gran Sasso highway tunnel, then under construction In 1982 the Parliament approved the construction, finished in 1987 In 1989 the first experiment, MACRO, started taking data LABORATORI NAZIONALI DEL GRAN SASSO - INFN Largest underground laboratory for astroparticle physics 1400 m rock coverage cosmic µ reduction= 10–6 (1 /m2 h) underground area: 18 000 m2 external facilities Research lines easy access • Neutrino physics 756 scientists from 25 countries Permanent staff = 66 positions (mass, oscillations, stellar physics) • Dark matter • Nuclear reactions of astrophysics interest • Gravitational waves • Geophysics • Biology LNGS Users Foreigners: 356 from 24 countries Italians: 364 Permanent Staff: 64 people Administration Public relationships support Secretariats (visa, work permissions) Outreach Environmental issues Prevention, safety, security External facilities General, safety, electrical plants Civil works Chemistry Cryogenics Mechanical shop Electronics Computing and networks Offices Assembly halls Lab -
Radiochemical Solar Neutrino Experiments, "Successful and Otherwise"
BNL-81686-2008-CP Radiochemical Solar Neutrino Experiments, "Successful and Otherwise" R. L. Hahn Presented at the Proceedings of the Neutrino-2008 Conference Christchurch, New Zealand May 25 - 31, 2008 September 2008 Chemistry Department Brookhaven National Laboratory P.O. Box 5000 Upton, NY 11973-5000 www.bnl.gov Notice: This manuscript has been authored by employees of Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy. The publisher by accepting the manuscript for publication acknowledges that the United States Government retains a non-exclusive, paid-up, irrevocable, world-wide license to publish or reproduce the published form of this manuscript, or allow others to do so, for United States Government purposes. This preprint is intended for publication in a journal or proceedings. Since changes may be made before publication, it may not be cited or reproduced without the author’s permission. DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, nor any of their contractors, subcontractors, or their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or any third party’s use or the results of such use of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof or its contractors or subcontractors. -
The Compact Program Booklet
- 1 - MONDAY, 5 SEPTEMBER 2011 WELCOME TO 12th International Conference on Topics in Astroparticle and Underground Physics 5 – 9 September 2011, Munich, Germany - 2 - structure of The ConferenCe SUNDAY, 4 SEP 2011 WEDNesDAY, 7 SEP 2011 Page 11 17:00 - 21:00 Registration/Reception 09:00 - 10:45 Plenary: Neutrinos 11:15 - 13:00 Plenary: Neutrinos MONDAY, 5 SEP 2011 Page 3 14:30 - 16:10 DM AM DBD/NM LE 09:00 - 10:10 Plenary: Cosmology 16:50 - 18:30 DM AM NO C 10:10 - 10:45 Plenary: Dark Matter 20:00 - 23:30 Conference Dinner 11:15 - 11:50 Plenary: Dark Matter 11:50 - 12:25 Plenary: Astrophysical Messengers THURSDAY, 8 SEP 2011 Page 14 12:25 - 13:00 Plenary: Underground Physics 09:00 - 10:45 Plenary: Astrophysical Messengers 14:30 - 16:10 DM AM DBD/NM LE 11:15 - 13:00 Plenary: Astrophysical Messengers 16:50 - 18:30 DM AM NO C 14:30 - 16:10 DM AM DBD/NM GW 16:50 - 18:30 DM LE DBD/NM GW TUesDAY, 6 seP 2011 Page 6 09:00 - 10:50 Plenary: Dark Matter FRIDAY, 9 seP 2011 Page 17 11:15 - 13:00 Plenary: Dark Matter 09:00 - 09:35 Plenary: Underground Physics 14:30 - 16:10 DM AM DBD/NM LE 09:35 - 10:45 Plenary: Astrophysical Messengers 16:50 - 18:30 DM AM NO C 11:15 - 12:25 Plenary: Astrophysical Messengers 18:30 - 20:00 Poster Session 12:25 - 13:00 Concluding Session DM Dark Matter NO Neutrino Oscillations AM Astrophysical Messengers DBD/NM Double Beta Decay, Neutrino Mass C Cosmology LE Low-Energy Neutrinos GW Gravitational Waves - 3 - MONDAY, 5 SEPTEMBER 2011 PLENARY SessION: CosmoloGY I Festsaal 09:00 CMB and Planck Francois Bouchet (IAP Paris) -
Science Case for the Giant Radio Antenna Neutrino Detector
Science Case for the Giant Radio Antenna Neutrino Detector Kumiko Kotera — Institut d’Astrophysique de Paris, UMR 7095 - CNRS, Université Pierre & Marie Curie, 98 bis boulevard Arago, 75014, Paris, France ; email: [email protected] “The title [of this book] is more of an expression of hope than a de- scription of the book’s contents [...]. As new ideas (theoretical and experimental) are explored, the observational horizon of neutrino as- trophysics may grow and the successor to this book may take on a different character, perhaps in a time as short as one or two decades.” John N. Bahcall, Neutrino Astrophysics, Cambridge University Press, 1989 igh-energy (> 1015 eV) neutrino as- progress in the fields of high-energy astro- tronomy will probe the working of physics and astroparticle physics. Addi- Hthe most violent phenomena in the tionally, they should contribute to unveil Universe. When most of the information fundamental neutrino properties. we have on the Universe stems from the observation of light, one essential strategy to undertake is to diversify our messengers. 1 Why neutrinos? The most energetic, mysterious and hardly understood astrophysical sources or events Neutrinos are unique messengers that let (fast-rotating neutron stars, supernova ex- us see deeper in objects, further in dis- plosions and remnants, gamma-ray bursts, tance, and pinpoint the exact location of outflows and flares from active galactic nu- their sources. clei, ...) are expected to be producers Neutrinos can escape much denser as- of high-energy non-thermal hadronic emis- trophysical environments than light, hence sion. Hence they should produce copious they enable us to explore processes in the amounts of high-energy neutrinos. -
Astrophysical Neutrinos at the Low and High Energy Frontiers by Lili Yang A
Astrophysical neutrinos at the low and high energy frontiers by Lili Yang A Dissertation Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy Approved November 2013 by the Graduate Supervisory Committee: Cecilia Lunardini, Chair Ricardo Alarcon Igor Shovkovy Francis Timmes Tanmay Vachaspati ARIZONA STATE UNIVERSITY December 2013 ABSTRACT For this project, the diffuse supernova neutrino background (DSNB) has been calcu- lated based on the recent direct supernova rate measurements and neutrino spectrum from SN1987A. The estimated diffuse n¯ flux is 0.10 – 0.59 cm 2s 1 at 99% confi- e ⇠ − − dence level, which is 5 times lower than the Super-Kamiokande 2012 upper limit of 3.0 2 1 cm− s− , above energy threshold of 17.3 MeV. With a Megaton scale water detector, 40 events could be detected above the threshold per year. In addition, the detectability of neutrino bursts from direct black hole forming col- lapses (failed supernovae) at Megaton detectors is calculated. These neutrino bursts are energetic and with short time duration, 1s. They could be identified by the time coin- ⇠ cidence of N 2 or N 3 events within 1s time window from nearby (4 – 5 Mpc) failed ≥ ≥ supernovae. The detection rate of these neutrino bursts could get up to one per decade. This is a realistic way to detect a failed supernova and gives a promising method for studying the physics of direct black hole formation mechanism. Finally, the absorption of ultra high energy (UHE) neutrinos by the cosmic neutrino background, with full inclusion of the effect of the thermal distribution of the back- ground on the resonant annihilation channel, is discussed. -
THE BOREXINO IMPACT in the GLOBAL ANALYSIS of NEUTRINO DATA Settore Scientifico Disciplinare FIS/04
UNIVERSITA’ DEGLI STUDI DI MILANO DIPARTIMENTO DI FISICA SCUOLA DI DOTTORATO IN FISICA, ASTROFISICA E FISICA APPLICATA CICLO XXIV THE BOREXINO IMPACT IN THE GLOBAL ANALYSIS OF NEUTRINO DATA Settore Scientifico Disciplinare FIS/04 Tesi di Dottorato di: Alessandra Carlotta Re Tutore: Prof.ssa Emanuela Meroni Coordinatore: Prof. Marco Bersanelli Anno Accademico 2010-2011 Contents Introduction1 1 Neutrino Physics3 1.1 Neutrinos in the Standard Model . .4 1.2 Massive neutrinos . .7 1.3 Solar Neutrinos . .8 1.3.1 pp chain . .9 1.3.2 CNO chain . 13 1.3.3 The Standard Solar Model . 13 1.4 Other sources of neutrinos . 17 1.5 Neutrino Oscillation . 18 1.5.1 Vacuum oscillations . 20 1.5.2 Matter-enhanced oscillations . 22 1.5.3 The MSW effect for solar neutrinos . 26 1.6 Solar neutrino experiments . 28 1.7 Reactor neutrino experiments . 33 1.8 The global analysis of neutrino data . 34 2 The Borexino experiment 37 2.1 The LNGS underground laboratory . 38 2.2 The detector design . 40 2.3 Signal processing and Data Acquisition System . 44 2.4 Calibration and monitoring . 45 2.5 Neutrino detection in Borexino . 47 2.5.1 Neutrino scattering cross-section . 48 2.6 7Be solar neutrino . 48 2.6.1 Seasonal variations . 50 2.7 Radioactive backgrounds in Borexino . 51 I CONTENTS 2.7.1 External backgrounds . 53 2.7.2 Internal backgrounds . 54 2.8 Physics goals and achieved results . 57 2.8.1 7Be solar neutrino flux measurement . 57 2.8.2 The day-night asymmetry measurement . 58 2.8.3 8B neutrino flux measurement . -
The History of Neutrinos, 1930 − 1985
The History of Neutrinos, 1930 − 1985. What have we Learned About Neutrinos? What have we Learned Using Neutrinos? J. Steinberger Prepared for “25th International Conference On Neutrino Physics and Astrophysics”, Kyoto (Japan), June 2012 1 2 3 4 The detector of the experiment of Conversi, Pancini and Piccioni, 1946, 5 which showed that the mesotron is not the Yukawa particle. Detector with 80 Geiger counters. The muon decay spectrum is continuous. My thesis experiment, under Fermi, which showed that the muon decays into two neutral particles, plus the electron. Fermi, myself and others, in 1954, at a summer school in Varenna, lake Como, a few months before Fermi’s untimely disappearance. 6 Demonstration of the Neutrino In 1956 Cowan and Reines detected antineutrinos from a nuclear reactor, reacting with protons in liquid scintillator which also contained cadmium, observing the positron as well as the scattering of the neutron on cadmium. 7 The Electron and Muon Neutrinos are Different. 1. G. Feinberg, 1958. 2. B. Pontecorvo, 1959. 3. M. Schwartz (T.D. Lee), 1959 4. Higher energy accelerators, Courant, Livingston and Snyder. Pontecorvo 8 9 A C B D Spark chamber and counter arrangement. A are triggering counters, Energy spectra of neutrinos B, C and D are anticoincidence counters from pion and kaon decays. 10 Event with penetrating muon and hadron shower 11 The group of the 2nd neutrino experiment in 1962: J.S., Goulianos, Gaillard, Mistry, Danby, technician whose name I have forgotten, Lederman and Schwartz. 12 Same group, 26 years later, at Nobel ceremony in Stockholm. 13 Discovery of partons, nucleon structure, scaling, in deep inelastic scattering of electrons on protons at SLAC in 1969. -
Probing Light Gauge Bosons in Tau Neutrino Experiments
Probing Light Gauge Bosons in Tau Neutrino Experiments Felix Kling∗ SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA The tau neutrino is probably the least studied particle in the SM, with only a handful of interaction events being identified so far. This can in part be attributed to their small production rate in the SM, which occurs mainly through Ds meson decay. However, this also makes the tau neutrino flux measurement an interesting laboratory for additional new physics production modes. In this study, we investigate the possibility of tau neutrino production in the decay of light vector bosons. We consider four scenarios of anomaly-free U(1) gauge groups corresponding to the B−L, B−Lµ−2Lτ , B − Le − 2Lτ and B − 3Lτ numbers, analyze current constraints on their parameter spaces and explore the sensitivity of DONuT and as well as the future emulsion detector experiments FASERν, SND@LHC and SND@SHiP. We find that these experiments provide the leading direct constraints in parts of the parameter space, especially when the vector boson's mass is close to the mass of the ! meson. I. INTRODUCTION other neutrino flavors. This small SM production rate makes the tau neutrino flux measurement an interesting The standard model (SM) consist of 17 particles, out laboratory for additional beyond the SM (BSM) produc- tion modes. of which the tau neutrino ντ is the least experimentally constrained one. To detect the rare tau neutrino interac- One example of such new physics are light vector tions, an intense neutrino beam with a sufficiently large bosons V associated with additional gauge groups. -
Pos(ICRC2021)048
ICRC 2021 THE ASTROPARTICLE PHYSICS CONFERENCE ONLINE ICRC 2021Berlin | Germany THE ASTROPARTICLE PHYSICS CONFERENCE th Berlin37 International| Germany Cosmic Ray Conference 12–23 July 2021 Rapporteur ICRC 2021: Neutrinos and Muons PoS(ICRC2021)048 0,1, Anna Nelles ∗ 0DESY, Platanenallee 6, 15738 Zeuthen, Germany 1ECAP, Friedrich-Alexander-University Erlangen-Nuremberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany E-mail: [email protected] This contribution attempts to summarize the status of the field of neutrinos from the cosmos as presented at the ICRC 2021, the first online-only edition of this conference. This rapporteur report builds on 212 contributions with pre-recorded talks and posters, as well as 11 discussion sessions. Furthermore, many of the session conveners provided valuable input to this summary. 37th International Cosmic Ray Conference (ICRC 2021) July 12th – 23rd, 2021 Online – Berlin, Germany ∗Presenter © Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License (CC BY-NC-ND 4.0). https://pos.sissa.it/ Rapporteur: Neutrinos and Muons Anna Nelles The field of neutrino astronomy already provides exciting results, however,it is still dominated by very low statistics in astrophysical neutrino detections. The most transformative results have been discussed in the multi-messenger context [1] and clearly neutrinos are becoming a target of opportunity for all experiments with a potential sensitivity to them. The neutrino field itself is booming with new ideas for detectors and has reached a maturity in which detailed data analysis and systematic detector calibration are the order of business. To summarize the sentiment: the community is doing their homework to get ready for many more neutrinos, which the broader community is excited about. -
Measurement of Muon Neutrino Disappearance with the Nova Experiment Luke Vinton
Measurement of Muon Neutrino Disappearance with the NOvA Experiment Luke Vinton Submitted for the degree of Doctor of Philosophy University of Sussex 14th February 2018 Declaration I hereby declare that this thesis has not been and will not be submitted in whole or in part to another University for the award of any other degree. Signature: Luke Vinton iii UNIVERSITY OF SUSSEX Luke Vinton, Doctor of Philosophy Measurement of muon neutrino disappearance with the NOvA experiment Abstract The NOvA experiment consists of two functionally identical tracking calorimeter detectors which measure the neutrino energy and flavour composition of the NuMI beam at baselines of 1 km and 810 km. Measurements of neutrino oscillation parameters are extracted by comparing the neutrino energy spectrum in the far detector with predictions of the oscil- lated neutrino energy spectra that are made using information extracted from the near detector. Observation of muon neutrino disappearance allows NOvA to make measure- 2 ments of the mass squared splitting ∆m32 and the mixing angle θ23. The measurement of θ23 will provide insight into the make-up of the third mass eigenstate and probe the muon-tau symmetry hypothesis that requires θ23 = π=4. This thesis introduces three methods to improve the sensitivity of NOvA's muon neut- rino disappearance analysis. First, neutrino events are separated according to an estimate of their energy resolution to distinguish well resolved events from events that are not so well resolved. Second, an optimised neutrino energy binning is implemented that uses finer binning in the region of maximum muon neutrino disappearance. Third, a hybrid selection is introduced that selects muon neutrino events with greater efficiency and purity.