Groupe Neutrino
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In the Light of LSND, Miniboone and Other Data
DAPNIA-SPhT Joint Seminar, 21 May 2007 Exotic Neutrino Physics in the light of LSND, MiniBooNE and other data Marco Cirelli + Stéphane Lavignac SPhT - CEA/Saclay Introduction CDHSW Neutrino Physics (pre-MiniBooNE): CHORUS NOMAD NOMAD NOMAD 0 KARMEN2 CHORUS Everything fits in terms of: 10 LSND 3 neutrino oscillations (mass-driven) Bugey BNL E776 K2K SuperK CHOOZ erde 10–3 PaloV Super-K+SNO Cl +KamLAND ] 2 KamLAND [eV 2 –6 SNO m 10 Super-K ∆ Ga –9 10 νe↔νX νµ↔ντ νe↔ντ νe↔νµ 10–12 10–4 10–2 100 102 tan2θ http://hitoshi.berkeley.edu/neutrino Particle Data Group 2006 Introduction CDHSW Neutrino Physics (pre-MiniBooNE): CHORUS NOMAD NOMAD NOMAD 0 KARMEN2 CHORUS Everything fits in terms of: 10 LSND 3 neutrino oscillations (mass-driven) Bugey BNL E776 K2K SuperK Simple ingredients: CHOOZ erde 10–3 PaloV νe, νµ, ντ m1, m2, m3 Super-K+SNO Cl +KamLAND ] θ12, θ23, θ13 δCP 2 KamLAND [eV 2 –6 SNO m 10 Super-K ∆ Ga –9 10 νe↔νX νµ↔ντ νe↔ντ νe↔νµ 10–12 10–4 10–2 100 102 tan2θ http://hitoshi.berkeley.edu/neutrino Particle Data Group 2006 Introduction CDHSW Neutrino Physics (pre-MiniBooNE): CHORUS NOMAD NOMAD NOMAD 0 KARMEN2 CHORUS Everything fits in terms of: 10 LSND 3 neutrino oscillations (mass-driven) Bugey BNL E776 K2K SuperK Simple ingredients: CHOOZ erde 10–3 PaloV νe, νµ, ντ m1, m2, m3 Super-K+SNO Cl +KamLAND ] θ12, θ23, θ13 δCP 2 KamLAND Simple theory: [eV 2 –6 SNO m 10 |ν! = cos θ|ν1! + sin θ|ν2! Super-K ∆ −E1t −E2t |ν(t)! = e cos θ|ν1! + e sin θ|ν2! Ga 2 Ei = p + mi /2p 2 –9 ν ↔ν m L 10 e X 2 2 ∆ ν ↔ν P ν → ν θ µ τ ( α β) = sin 2 αβ sin ν ↔ν E e -
Km3net/ORCA Telescopes
Search for light sterile neutrinos with ANTARES and KM3NeT/ORCA telescopes A. Domi1,2, J. A. B. Coelho3, T. Thakore4, for the ANTARES and KM3NeT Collaborations 1 Università degli Studi di Genova, Genoa (Italy) - [email protected] 2 INFN-Genova, Genoa (Italy) 3 LAL, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, Orsay (France) - [email protected] 4 University of Cincinnati, Ohio (United States) - [email protected] VLVnT Workshop - 19/05/2021 1 Where are we with light sterile neutrinos? • Majority of experiments have confirmed the 3 flavour neutrino oscillations. • In parallel, anomalies observed in some oscillation experiments: Anomalies in Short baseline (SBL) Ref: Prog.Part.Nucl.Phys. 111 (2020) 103736 experiments •LSND: �� -> �e •MINIBooNE: �� -> �e / �� -> �e Gallium Anomalies: �e disappearance Reactor anomalies: e disappearance � Disagreement between appearance and disappearance NO ANOMALIES observed in / disappearance. Further observations needed! �� �� 2 Where are we with light sterile neutrinos? Cosmology • Constrains the effective number of relativistic species (Neff) in our universe. • A SBL neutrino would require Neff=4. • Measured Neff compatible with 3. -> Tension with SBL anomalies. • Tension relaxes when cosmological data are combined with astrophysical data. • Cosmological data alone can be compatible with • an eV-mass sterile neutrino only if its contribution to Neff is very small, • a larger Neff only if it comes from a nearly massless sterile particle. We need further observations: neutrino telescopes make it possible! 3 Sterile Neutrinos • Oscillations in the presence of sterile neutrinos are solutions of: 2 • Adding one sterile neutrino introduces 6 more free parameters: �m41 , 3 mixing angles (�14,�24,�34) and 2 more CP phases (�14, �24). -
A Survey of the Physics Related to Underground Labs
ANDES: A survey of the physics related to underground labs. Osvaldo Civitarese Dept.of Physics, University of La Plata and IFLP-CONICET ANDES/CLES working group ANDES: A survey of the physics related to underground labs. – p. 1 Plan of the talk The field in perspective The neutrino mass problem The two-neutrino and neutrino-less double beta decay Neutrino-nucleus scattering Constraints on the neutrino mass and WR mass from LHC-CMS and 0νββ Dark matter Supernovae neutrinos, matter formation Sterile neutrinos High energy neutrinos, GRB Decoherence Summary The field in perspective How the matter in the Universe was (is) formed ? What is the composition of Dark matter? Neutrino physics: violation of fundamental symmetries? The atomic nucleus as a laboratory: exploring physics at large scale. Neutrino oscillations Building neutrino flavor states from mass eigenstates νl = Uliνi i X Energy of the state m2c4 E ≈ pc + i i 2E Probability of survival/disappearance 2 ′ −i(Ei−Ep)t/h¯ ∗ P (νl → νl′ )= | δ(l, l )+ Ul′i(e − 1)Uli | 6 Xi=p 2 2 4 (mi −mp )c L provided 2Ehc¯ ≥ 1 Neutrino oscillations The existence of neutrino oscillations was demonstrated by experiments conducted at SNO and Kamioka. The Swedish Academy rewarded the findings with two Nobel Prices : Koshiba, Davis and Giacconi (2002) and Kajita and Mc Donald (2015) Some of the experiments which contributed (and still contribute) to the measurements of neutrino oscillation parameters are K2K, Double CHOOZ, Borexino, MINOS, T2K, Daya Bay. Like other underground labs ANDES will certainly be a good option for these large scale experiments. -
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. -
Pos(ICHEP2020)886
The Outer Detector (OD) system for the Hyper-Kamiokande experiment PoS(ICHEP2020)886 Stephane Zsoldos0,1,2,∗ 0Department of Physics, King’s College London, Strand, London WC2R 2LS, United Kingdom 1Department of Physics, University of California, Berkeley, CA 94720, Berkeley, USA 2Lawrence Berkeley National Laboratory, 1 Cyclotron Road, Berkeley, CA 94720-8153, USA E-mail: [email protected], [email protected] Hyper-Kamiokande, scheduled to begin construction as soon as 2020, is a next generation under- ground water Cherenkov detector, based on the highly successful Super-Kamiokande experiment. It will serve as a far detector, 295 km away, of a long baseline neutrino experiment for the upgraded J-PARC beam in Japan. It will also be a detector capable of observing — far beyond the sensitivity of the Super-Kamiokande detector — proton decay, atmospheric neutrinos, and neutrinos from astronomical sources. An Outer Detector (OD) consisting of PMTs mounted behind the inner detector PMTs and facing outwards to view the outer shell of the cylindrical tank, would provide topological information to identify interactions originating from particles outside the inner detector. Any optimization would lead to a significant improvement for the physics goals of the experiment, which are the measurement of the CP leptonic phase and the determination of the neutrino mass hierarchy. An innovative new setup using small 3" PMTs is being proposed for the Hyper-Kamiokande OD. They would give better redundancy, spatial, and angular resolution, as there would be twice or three times more photosensors that the original 8" design proposal of the experiment, and for a reduced cost. -
Realization of the Low Background Neutrino Detector Double Chooz: from the Development of a High-Purity Liquid & Gas Handling Concept to first Neutrino Data
Realization of the low background neutrino detector Double Chooz: From the development of a high-purity liquid & gas handling concept to first neutrino data Dissertation of Patrick Pfahler TECHNISCHE UNIVERSITAT¨ MUNCHEN¨ Physik Department Lehrstuhl f¨urexperimentelle Astroteilchenphysik / E15 Univ.-Prof. Dr. Lothar Oberauer Realization of the low background neutrino detector Double Chooz: From the development of high-purity liquid- & gas handling concept to first neutrino data Dipl. Phys. (Univ.) Patrick Pfahler Vollst¨andigerAbdruck der von der Fakult¨atf¨urPhysik der Technischen Universit¨atM¨unchen zur Erlangung des akademischen Grades eines Doktors des Naturwissenschaften (Dr. rer. nat) genehmigten Dissertation. Vorsitzender: Univ.-Prof. Dr. Alejandro Ibarra Pr¨uferder Dissertation: 1. Univ.-Prof. Dr. Lothar Oberauer 2. Priv.-Doz. Dr. Andreas Ulrich Die Dissertation wurde am 3.12.2012 bei der Technischen Universit¨atM¨unchen eingereicht und durch die Fakult¨atf¨urPhysik am 17.12.2012 angenommen. 2 Contents Contents i Introduction 1 I The Neutrino Disappearance Experiment Double Chooz 5 1 Neutrino Oscillation and Flavor Mixing 6 1.1 PMNS Matrix . 6 1.2 Flavor Mixing and Neutrino Oscillations . 7 1.2.1 Survival Probability of Reactor Neutrinos . 9 1.2.2 Neutrino Masses and Mass Hierarchy . 12 2 Reactor Neutrinos 14 2.1 Neutrino Production in Nuclear Power Cores . 14 2.2 Energy Spectrum of Reactor neutrinos . 15 2.3 Neutrino Flux Approximation . 16 3 The Double Chooz Experiment 19 3.1 The Double Chooz Collaboration . 19 3.2 Experimental Site: Commercial Nuclear Power Plant in Chooz . 20 3.3 Physics Program and Experimental Concept . 21 3.4 Signal . 23 3.4.1 The Inverse Beta Decay (IBD) . -
Ankur Sharma
Ankur Sharma Date of Birth 2nd August 1991 Gender Male Nationality Indian Phone +46 76 447 51 45 Address Eklundshovsvägen 4B, Lgh 1104 Email [email protected] 752 37, Uppsala, Sweden [email protected] Research Interests Phenomenological studies of VHE emission from jets of AGNs; multi-messenger and multi-wavelength connection in blazars with neutrino, gamma-ray and X-ray data; gamma-ray astronomy; observability of point sources with Cherenkov neutrino telescopes; detection strategies for ultra-high energy neutrinos Education Jan 2017 - PhD in Physics - University of Pisa (Italy) Present Area of study - Astroparticle Physics, Neutrino Astrophysics - Astroparticles, Experimental Astrophysics & Astroparticle Physics - High Energy Experimental Physics Thesis Title - Analyzing the high energy activity of candidate blazars to constrain their observability by neutrino telescopes Supervisor - Dr. Antonio Marinelli ([email protected]) Aug 2009 - Integrated M.Sc. (M.Sc. + B.Sc.) in Applied Physics - Indian Institute of Technology (ISM), Dhanbad Feb 2015 Area of study - Applied Physics - Nuclear & Particle Physics, Classical Mechanics, Quantum Mechanics, Electrodynamics - Computer Networks, Microprocessors, C++, ForTran Sept 2013 - Erasmus Mundus India4EU II Exchange Mobility - University of Porto (Portugal) July 2014 Area of study - Master Thesis, Astronomy - Stellar Structure & Evolution, Cosmology - Optical Communication, Measurement Techniques & Instrumentation Thesis Title - Constraining the Parameter Space of Dynamical -
Geo-Neutrino Program at Baksan Neutrino Observatory Geoneutrino
Neutrino Geoscience 2019 Prague / Book of Abstracts The deep-sea neutrino detector KM3NeT/ORCA, currently being built in the Mediterranean Seanear Toulon (France), is optimized for the study of oscillations of atmospheric neutrinos in the few-GeV energy range, with the main goal to determine the neutrino mass hierarchy. This is possible due to matter effects that modify the probability of neutrino oscillations along their path through theEarth. Measuring the energy and angular distributions of neutrinos with ORCA can therefore also provide tomographic information on the Earth’s interior and more specifically on the electron density along the trajectory of the detected neutrino, complementary to standard geophysics methods. In this contribution the latest results of a study of the potential of ORCA for Earth tomography are presented. They are based on a full Monte Carlo simulation of the detector response and including systematic effects. It is shown that after ten years of operation ORCA can measure the electron density in both the lower mantle and the outer core with a precision of a few percent in the case of normal neutrino mass hierarchy. 40 Geo-neutrino program at Baksan Neutrino Observatory Authors: Albert Gangapshev1 ; Andrey Sidorenkov2 ; Bayarto Lubsandorzhiev2 ; Daniil Kudrin2 ; Dmitry Voronin2 ; Evgeny Veretenkin2 ; Evgeny Yanovich2 ; Galina Novikova2 ; Makhti Kochkarov2 ; Nikita Ushakov2 ; Tatiana Ibragimova2 ; Valery Kuzminov1 ; Valery Petkov3 ; Vladimir Gavrin2 ; Vladimir Kazalov2 ; Yury Gavrilyuk2 ; Yury Malyshkin4 1 INR RAS, KBSU 2 INR RAS 3 INR RAS, IA RAS 4 INR RAS, INFN A new neutrino program has been recently lunched at Baksan Neutrino Observatory. It is planned to deploy a 10-kiloton scale detector based on liquid scintillator in the existing shaft at a depth of 4800 m.w.e. -
Sensitivity to Light Sterile Neutrino Mixing Parameters with Km3net/ORCA
Sensitivity to light sterile neutrino mixing parameters with KM3NeT/ORCA S. Aielloa, A. Albertbb,b, M. Alshamsic, S. Alves Garred, Z. Alye, A. Ambrosonef,g, F. Amelih, M. Andrei, G. Androulakisj, M. Anghinolfik, M. Anguital, G. Antonm, M. Ardidn, S. Ardidn, J. Aublinc, C. Bagatelasj, B. Baretc, S. Basegmez du Preeo, M. Bendahmanc,p, F. Benfenatiq,r, E. Berbeeo, A. M. van den Bergs, V. Bertine, S. Biagit, M. Bissingerm, M. Boettcheru, M. Bou Cabov, J. Boumaazap, M. Boutaw, M. Bouwhuiso, C. Bozzax, H.Br^anza¸sy, F. Bretaudeauz, R. Bruijno,aa, J. Brunnere, R. Brunoa, E. Buisab, R. Buompanef,ac, J. Bustoe, B. Caiffik, D. Calvod, S. Campionad,h, A. Caponead,h, V. Carreterod, P. Castaldiq,ae, S. Celliad,h, M. Chababaf, N. Chauc, A. Chenag, S. Cherubinit,ah, V. Chiarellaai, T. Chiarusiq, M. Circellaaj, R. Cocimanot, J. A. B. Coelhoc,˚, A. Coleiroc, M. Colomer Mollac,d, R. Coniglionet, P. Coylee, A. Creusotc, A. Cruzak, G. Cuttonet, R. Dallierz, B. De Martinoe, M. De Palmaaj,al, I. Di Palmaad,h, A. F. D´ıazl, D. Diego-Tortosan, C. Distefanot, A. Domik,am,˚, C. Donzaudc, D. Dornice, M. D¨orran, D. Drouhinbb,b, T. Eberlm, A. Eddyamouip, T. van Eedeno, D. van Eijko, I. El Bojaddainiw, D. Elsaesseran, A. Enzenh¨ofere, V. Espinosan, P. Fermaniad,h, G. Ferrarat,ah, M. D. Filipovi´cao, F. Filippiniq,r, L. A. Fuscoe, T. Galm, J. Garc´ıaM´endezn, A. Garcia Sotoo, F. Garufif,g, Y. Gateletc, N. Geißelbrechtm, L. Gialanellaf,ac, E. Giorgiot, S. R. Gozziniad,h, R. Graciao, K. Grafm, G. Grellaap, D. -
The Hyper-Kamiokande Experiment Francesca Di Lodovico Queen Mary University of London
The Hyper-Kamiokande Experiment Francesca Di Lodovico Queen Mary University of London On behalf of the Hyper-K UK collaboration PPAP Meeting July 26, 2016 A Multi-purpose Experiment Comprehensive study of oscillation • CPV Supernova • Mass hierarchy with beam+atmosph. • 23 octant • Test of exotic scenarios Nucleon decay discovery potential Sun • All visible modes including p → 푒+ 0 + Accelerator and p→휈 퐾 can be advanced beyond (J-PARC) SK. • Reaching 1035yrs sensitivity Unique Astrophysics T2HK • Precision measurement of solar • High statistics Supernova with pointing capability and energy info. • Supernova relic (non-burst ) Proton observation is also possible decay Earth core's chemical composition Etc. 2 Inaugural Symposium of the HK proto- collaboration@Kashiwa, Jan-2015 12 countries, ~250 members and growing KEK-IPNS and • Proto-collaboration formed. UTokyo-ICRR • International steering group signed a MoU for • International conveners cooperation • International chair for international on the Hyper- board of representative (IBR) Kamiokande project. 26/July/2016 The Hyper-Kamiokande Experiment 3 Proto-Collaboration IRFU, CEA Saclay (France) Gifu University (Japan) Laboratoire Leprince-Ringuet, Ecole Polytechnique (France) High Energy Accelerator Research Organization (KEK) (Japan) Lancaster University (UK) Kobe University (Japan) Los Alamos National Laboratory (USA) Kyoto University (Japan) Louisiana State University (USA) Miyagi University of Education (Japan) National Centre for Nuclear Research (Poland) Nagoya University -
Icecube and Km3net: Lessons and Relations
Elsevier Science 1 Journal logo IceCube and KM3NeT: Lessons and Relations Christian Spiering DESY, Platanenallee 6, Zeuthen, 15738 Germany Elsevier use only: Received date here; revised date here; accepted date here Abstract This talk presents conclusions for KM3NeT which may be drawn from latest IceCube results and from optimization studies of the IceCube configuration. It discusses possible coordinated efforts between IceCube and KM3NeT (or, for the time being, IceCube and ANTARES). Finally, it lists ideas for formal relations between neutrino telescopes on the cubic kilometer scale. © 2001 Elsevier Science. All rights reserved Keywords: Neutrino Telescopes 1. Introduction The IceCube neutrino telescope at the South Pole Assuming one detector on the Southern is approaching its completion and meanwhile has hemisphere (IceCube) and one or more detectors at provided first results from data taken with initial the Northern hemisphere (by now ANTARES [10] configurations [1]. KM3NeT will act as IceCube’s and NT200 [11], in the future KM3NeT [12] and counterpart on the Northern hemisphere, with a GVD [13]), various possibilities for coordinated sensitivity “substantially exceeding that of all physics programs and analyses open up. They are existing neutrino telescopes including IceCube” [2]. discussed in sections 3 and 4. KM3NeT is just finishing its design phase [3], but Finally, section 5 lists formal and procedural has not yet converged to a final configuration. The possibilities of cooperation between KM3NeT and cited sensitivity requirement results not only from IceCube. gamma ray observations and their phenomenological interpretation (see e.g. [4-9]), but also from early IceCube data. The first section of this paper is 2. -
Muon Spallation in Double Chooz
Muon Spallation in Double Chooz Claire Thomas∗ REU, Columbia University and MIT (Dated: August 10, 2009) This report presents my work for Double Chooz at MIT during the 2009 Summer REU program, funded by Columbia University. Double Chooz is a reactor neutrino experiment that aims to measure the mixing parameter θ13. The experiment detects electron antineutrinos via inverse beta decay. Neutrons and light nuclei made in muon spallation are a major background to the experiment. The delayed neutron emitter 9Li is especially problematic because it mimics the inverse beta decay signal. For this reason I studied muon spallation in Double Chooz, focusing on the production and subsequent decay of 9Li. There are two key differences between 9Li decay and inverse beta decay. The first is that 9Li is a β− decay, so it emits an electron, whereas inverse beta decay emits a positron. The second difference is the energy of the neutrons emitted. In 9Li decay the neutron energy is on the order of MeV, whereas the inverse beta decay neutron has a negligible kinetic energy. Since Double Chooz does not distinguish charge, the positrons and electrons are not easy to distinguish. First, I ran simulations of electrons and positrons in the Double Chooz detector and constructed a late light variable to distinguish them from electrons. This proved insufficient, so I wrote general software to simulate radioactive decays in the Double Chooz detector. In this report I present the deposited energy spectra of a few important decays. 1. INTRODUCTION The consequence of neutrino oscillation is that an ex- periment that is sensitive to only one of the three neu- 1.1.