Results in Neutrino Oscillations from Super-Kamiokande I

Total Page:16

File Type:pdf, Size:1020Kb

Results in Neutrino Oscillations from Super-Kamiokande I Status of the RENO Reactor Neutrino Experiment RENO = Reactor Experiment for Neutrino Oscillation (For RENO Collaboration) K.K. Joo Chonnam National University February 15, 2011 Research Techniques Seminar @FNAL Outline Experiment Goals of the RENO Exp. - Short introduction - Expected q13 sensitivity - Systematic uncertainty Overview of the RENO Experiment - Experimental Setup of RENO - Schedule - Tunnel excavation - Status of detector construction - DAQ, data analysis tools Summary Brief History of Neutrinos 1930: Pauli postulated neutrino to explain b decay problem 1933: Fermi baptized the neutrino in his weak-interaction theory 1956: First discovery of neutrino by Reines & Cowan from reactor 1957: Neutrinos are left-handed by Glodhaber et al. 1962: Discovery of nm by Lederman et al. (Brookhaven Lab) 1974: Discovery of neutral currents due to neutrinos 1977: Tau lepton discovery by Perl et al. (SLAC) 1998: Atmospheric neutrino oscillation observed by Super-K 2000: nt discovery by DONUT (Fermilab) 2002: Solar neutrino oscillation observed by SNO and confirmed by Kamland What NEXT? Standard Model Neutrinos in SM Neutrino Oscillation . Three types of neutrinos exist & mixing among them Oscillation parameters (q12 , q23 , q13) Not measured yet . Elementary particles with almost no interactions . Almost massless: impossible to measure its mass Neutrino Mixing Parameters Matrix Components: νe Ue1 Ue2 Ue3 ν1 3 Angles (θ ; θ ; θ ) 12 13 23 ν U U U ν 1 CP phase (δ) μ μ1 μ2 μ3 2 2 Mass differences ντ Uτ1 Uτ2 Uτ3 ν3 1 0 0 c 0 s ei c s 0 13 13 12 12 U 0 c23 s23 0 1 0 s12 c12 0 i 0 s23 c23 s13e 0 c13 0 0 1 atmospheric SK, K2K The Next Big Thing? SNO, solar SK, KamLAND ≈ ≈ ° q23 qatm 45 q12 ≈qsol ≈ 32° Large and maximal mixing! Reduction of reactor neutrinos due to oscillations Disappearance Reactor neutrino disappearance Prob. due 2 to q13 with the allowed 2 range in m23 2 sin 2q13 > 0.01 with 10 t •14GW •3yr ~ 400 t•GW•yr (400 t•GW•yr: a 10(40) ton far detector and a 14(3.5) GW reactor in 3 years) Experimental Method of q13 Measurement νe Oscillations observed as a νe ν e deficit of anti-neutrinos ν νe e νe 1.0 sin22θ e 13 flux before oscillation observed here 2 2 4 2 2 1.27m12L 2 2 1.27m13L Pne ne1cos q13sin 2q12sin sin 2q13sin Probabilité ν Probabilité E E n n Distance 1200 to 1800 meters Find disappearance of ne fluxes due to neutrino oscillation as a function of energy using multiple, identical detectors to reduce the systematic errors in 1% level. Expected Number of Neutrino Events at RENO • 2.73 GW per reactor ⅹ 6 reactors • 1.21x1030 free protons per targets (16 tons) • Near : 1,280/day, 468,000/year • Far : 114/day, 41,600/year 3 years of data taking with 70% efficiency Near : 9.83x105 ≈ 106 (0.1% error) Far : 8.74x104 ≈ 105 (0.3% error) RENO Expected Sensitivity New!! (full analysis) 10x better sensitivity than current limit Expected Systematic Uncertainty Systematic Source CHOOZ (%) RENO (%) Reactor antineutrino flux and 1.9 < 0.1 Reactor related cross section absolute Reactor power 0.7 0.2 normalization Energy released per fission 0.6 < 0.1 Number of protons H/C ratio 0.8 0.2 in target Target mass 0.3 < 0.1 Positron energy 0.8 0.1 Positron geode distance 0.1 0.0 Neutron capture (H/Gd ratio) 1.0 < 0.1 Detector Efficiency Capture energy containment 0.4 0.1 Neutron geode distance 0.1 0.0 Neutron delay 0.4 0.1 Positron-neutron distance 0.3 0.0 Neutron multiplicity 0.5 0.05 combined 2.7 < 0.5 Principle of Neutrino Detection γ(0.511MeV) e - Use inverse beta decay (v + p e+ + n) e + γ(0.511MeV) e ν e reaction process p prompt signal Prompt part: n subsequent annihilation of the positron Delayed signal 30μs γ to two 0.511MeV γ Delayed part: Gd neutron is captured E ~ 8MeV γ γ ~200ms w/o Gd ~ 30ms w Gd Gd has largest n absorption cross section & emits high energy Signal Property Signal from neutron capture 1~8MeV 8MeV ~2.2MeV w/o Gd 30μs ~ 8MeV w Gd t Measure prompt signal & delayed signal “Delayed coincidence” reduces backgrounds drastically World Competition in Reactor Neutrino Experiments Thermal Distances Depth Target Mass Cost # of Experiments Location Power Near/Far Near/Far (tons) (US $) Collab (GW) (m) (mwe) orators Double-CHOOZ France 8.7 410/1050 115/300 10/10 ~30M >160 RENO Korea 17.3 290/1380 120/450 16/16 ~10M 40 360(500)/1985 Daya Bay China 11.6 260/910 402/80 ~60M >230 (1613) Double-Chooz is expected to complete construction in 2012 RENO will finish its construction by Feb 2011 Daya Bay is expected to finish its construction in 2012 Reactor Neutrino Experiments Double-CHOOZ (France) Braidwood (USA) KASKA (Japan) Daya Bay (China) Near Detectors Far Detector Double-CHOOZ Double-Chooz Collaboration: France, US, Germany, Italy, Japan, Spain & Russia * Proposal (June 20, 2006) : hep-ex/0606025 Daya Bay Daya Bay Collaboration: China, US, Czech Republic, Hong Kong, Russia & Taiwan * Proposal to DOE (Jan. 15, 2007): hep-ex/0701029 RENO Collaboration (13 institutions and 40 physicists) Chonbuk National University Chonnam National University Chung-Ang University Dongshin University Gyeongsang National University Kyungpook National University Pusan National University Sejong University Seokang Information University Seokyeong University Seoul National University Sungkyunkwan University California State University Domingez Hills, USA +++ http://neutrino.snu.ac.kr/RENO International collaborators are being invited YongGwang Nuclear Power Plant Located in the west coast of southern YongGwang(靈光): part of Korea = glorious[splendid] light ~400 km from Seoul 6 reactors are lined up in roughly equal distances and span ~1.3 km Total average thermal output ~16.4GWth (2nd largest in the world) RENO Experimental Setup Google Satellite View of Experimental Site Schematic View of Underground Facility 200m high Near Detector 70m high Reactors 100m 300m 290m 1,380m Far Detector 72 188 70 89 200 1678 25,5 RENO Detector 77 3130 238 3730 76 86 66 212 212 5580 240 350 ?85 acrylic 1500 280 75 85 880 570 200 600 75 85 570 2200 4000 5400 2200 1500 Thick Mass vessel Material (cm) (tons) Acrylic Gd(0.1%) Target 140 15.4 (10mm) +LS Gamma Acrylic 60 LS 27.5 catcher (15mm) Mineral Buffer 70 SUS(5mm) 59.2 oil • Inner PMTs: 342 10” PMTs Steel • solid angle coverage = 12.6% Veto 150 water 354.7 • Outer PMTs: ~ 60 10” PMTs (15mm) total ~460 tons Schedule 2006 2007 2008 2009 2010 2011 ActivitiesActivities 3 6 9 12 3 6 9 12 3 6 9 12 3 6 9 12 3 6 9 12 3 Detector Design & Specification Geological Survey & Tunnel Design Detector Construction Excavation & Underground Facility Construction Detector Commissioning & Data Taking Tunnel facility, detector structure & buffer steel tanks completed June 2010 : Acrylic containers installed Aug. 2010 : PMT test completed Aug. ~ Dec. 2010 : Installation of PMTs and veto tyvek Jan. 2011 : Installation of DAQ & HV and detector closing Feb. 2011 : Installation of liquid handling system Apr. 2011 : Start data taking Efforts for Underground Facility • 03~08, 2006 : Project description to local government, residents, and NGO’s (endorsed by local government) • 03, 2007 : Agreement between KHNP and SNU • 03~10, 2007 : Geological survey and tunnel design are completed. • 12, 2007 : Public hearing for YG residents • 01, 2008 : Safety regulation established and accepted by the atomic energy department of MOST • 05~11, 2008 : Tunnel construction Rock sampling (DaeWoo Engineering Co.) Rock samples from boring Rock Quality Map (2007.3~2007.8) • Near detector site: - tunnel length : 110m - overburden height : 46.1m • Far detector site: - tunnel length : 272m - overburden height : 168.1m Design of Tunnel (2007.9~2007.11) Wing tunnel(L) Wing Access tunnel Experimental hall Wing tunnel(R) Wing Detector Experimental Access tunnel hall Detector Wing tunnel(R) vertical hall Tunnel Construction for Underground Facility Approval from government regulation („08. 01/05) Cleared local government regulations („08. 01∼‟08. 06) Preparation for tunnel excavation („08. 07) Tunnel Construction (2008.6~2008.12) by Daewoo Eng. Co. Korea Near & far tunnels are completed (2008.6~2009.3) by Daewoo Eng. Co. Korea Far site Near site Underground Peripheral Facility (2009. 7~12) Electric power and ground system Internet cable and mobile telephone network Experimental Hall Detector vertical halls are ready (2008.12~2009.2) Buffer steel tanks are installed (2009.6~2009.11) by NIVAK Co. Korea Acrylic vessels are made and installed (2009.7~2010.6) by KOATECH Co. Korea Acrylic Delivery Installation of Acrylic Vessels (2010. 6) Near site Near site Nov.28 (Sun) 근거리 Nov.30 (Tue) 근거리 Target 압력 Gamma catcher 압력 미압계 (mbar) Target 압력(corrected) 대기압 (mbar) 미압계 (mbar) Gamma catcher 압력(corrected) 대기압 (mbar) 4.0 1026 4.0 1019 대기압 대기압 3.0 3.0 1025 1018 2.0 2.0 1024 1017 1.0 1.0 0.0 1023 0.0 1016 10 11 12 13 14 14 15 16 17 18 19 20 21 Time (hour) Time (hour) Far site Far site Jan.10 (Mon) 원거리 Jan.13 (Thu) 원거리 Target 압력 Gamma catcher 압력 미압계 (mbar) 대기압 (mbar) 미압계 (mbar) 대기압 (mbar) Target 압력(corrected) Gamma catcher 압력(corrected) 4.0 1022 4.00 1025 대기압 대기압 3.0 3.00 1024 2.0 1021 2.00 1023 1.0 1.00 1022 0.0 1020 0.00 1021 16 17 18 19 20 21 22 17 18 19 20 21 22 23 24 Time (hour) Time (hour) Trailer Research Facility & Guest Room (2009.
Recommended publications
  • 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) .
    [Show full text]
  • Letter of Interest Forthcoming Science from The
    Snowmass2021 - Letter of Interest Forthcoming Science from the PROSPECT-I Data Set Neutrino Frontier Topical Groups: (NF02) Sterile neutrinos (NF03) Beyond the Standard Model (NF07) Applications (NF09) Artificial neutrino sources Contact Information: Nathaniel Bowden (LLNL) [[email protected]] Karsten Heeger (Yale University) [[email protected]] Pieter Mumm (NIST) [[email protected]] M. Andriamirado,6 A. B. Balantekin,16 H. R. Band,17 C. D. Bass,8 D. E. Bergeron,10 D. Berish,13 N. S. Bowden,7 J. P.Brodsky,7 C. D. Bryan,11 R. Carr,9 T. Classen,7 A. J. Conant,4 G. Deichert,11 M. V.Diwan,2 M. J. Dolinski,3 A. Erickson,4 B. T. Foust,17 J. K. Gaison,17 A. Galindo-Uribarri,12, 14 C. E. Gilbert,12, 14 C. Grant,1 B. T. Hackett,12, 14 S. Hans,2 A. B. Hansell,13 K. M. Heeger,17 D. E. Jaffe,2 X. Ji,2 D. C. Jones,13 O. Kyzylova,3 C. E. Lane,3 T. J. Langford,17 J. LaRosa,10 B. R. Littlejohn,6 X. Lu,12, 14 J. Maricic,5 M. P.Mendenhall,7 A. M. Meyer,5 R. Milincic,5 I. Mitchell,5 P.E. Mueller,12 H. P.Mumm,10 J. Napolitano,13 C. Nave,3 R. Neilson,3 J. A. Nikkel,17 D. Norcini,17 S. Nour,10 J. L. Palomino,6 D. A. Pushin,15 X. Qian,2 E. Romero-Romero,12, 14 R. Rosero,2 P.T. Surukuchi,17 M. A. Tyra,10 R. L. Varner,12 D. Venegas-Vargas,12, 14 P.B.
    [Show full text]
  • APC Scientific Board 2017 Tech
    2012-2016 APC Laboratory Technical Activities T. Zerguerras on behalf of the Technical Departments 20/11/2017 APC Scientific Board 2017 1 Technical Departments Organisation Equipment, facilities and platform Instrumentation Department (Techniques Expérimentales) Electronics and Microelectronics Department Mechanics Department IT Department Quality Unit R&D: CMB µelectronic, Compton, GAMMACUBE, Liquido Analysis & Prospects 20/11/2017 APC Scientific Board 2017 2 General organisation • 5 technical departments + Quality Unit + the FACe platform • Building an instrument => combining skills 22/09/2017 APC Scientific Board 2017 3 Technical departments organisation Matrix organisation structure: Project/Department (Assignment to a department, participation to projects) One specific skill (Mechanics, Electronics/µelectronics, Instrumentation, IT, QA/PA) Transverse activities of the Quality Unit Supervision : Head of department Project coordination: Project manager Indicator Boards for activities and assignments monitoring Project Monitoring Committee (Comité de Suivi de Projets CSP) This organisation aims to create a bond of trust with funding and tutelage agencies 20/11/2017 APC Scientific Board 2017 4 Organisation: Technical staff evolution On 31/12 Technical departments staff evolution 60 Technical departments staff - Gender 45 50 40 40 35 34 30 30 33 35 38 38 Permanent 25 MEN Fixed-term 20 38 40 39 40 39 20 WOMEN 15 10 10 15 17 13 12 12 5 10 11 9 10 11 0 0 2012 2013 2014 2015 2016 2012 2013 2014 2015 2016 Technical departments
    [Show full text]
  • 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.
    [Show full text]
  • Neutrino Oscillation Studies with Reactors
    REVIEW Received 3 Nov 2014 | Accepted 17 Mar 2015 | Published 27 Apr 2015 DOI: 10.1038/ncomms7935 OPEN Neutrino oscillation studies with reactors P. Vogel1, L.J. Wen2 & C. Zhang3 Nuclear reactors are one of the most intense, pure, controllable, cost-effective and well- understood sources of neutrinos. Reactors have played a major role in the study of neutrino oscillations, a phenomenon that indicates that neutrinos have mass and that neutrino flavours are quantum mechanical mixtures. Over the past several decades, reactors were used in the discovery of neutrinos, were crucial in solving the solar neutrino puzzle, and allowed the determination of the smallest mixing angle y13. In the near future, reactors will help to determine the neutrino mass hierarchy and to solve the puzzling issue of sterile neutrinos. eutrinos, the products of radioactive decay among other things, are somewhat enigmatic, since they can travel enormous distances through matter without interacting even once. NUnderstanding their properties in detail is fundamentally important. Notwithstanding that they are so very difficult to observe, great progress in this field has been achieved in recent decades. The study of neutrinos is opening a path for the generalization of the so-called Standard Model that explains most of what we know about elementary particles and their interactions, but in the view of most physicists is incomplete. The Standard Model of electroweak interactions, developed in late 1960s, incorporates À À neutrinos (ne, nm, nt) as left-handed partners of the three families of charged leptons (e , m , t À ). Since weak interactions are the only way neutrinos interact with anything, the un-needed right-handed components of the neutrino field are absent in the Model by definition and neutrinos are assumed to be massless, with the individual lepton number (that is, the number of leptons of a given flavour or family) being strictly conserved.
    [Show full text]
  • PROSPECT Upgrade
    Precision Reactor Upgrade significantly expands oscillation Oscillation and physics reach in unique parameter space ] prospect.yale.edu ] ] 2 2 90% CL 90% CL 2 90% CL SPECTrum Experiment: PROSPECT, 1 yr Sensitivity PROSPECT, 2 yr Optimized Sensitivity PROSPECT, 2 yr Optimized Sensitivity PROSPECT, 2 yr Sensitivity DANSS Exclusion PROSPECT, 2 yr Optimized Sensitivity, σspectrum = 5% [eV [eV PROSPECT, 2 yr Optimized Sensitivity NEOS Exclusion [eV DYB Exclusion KATRIN Exclusion 2 41 PROSPECT, Current Sensitivity 2 41 STEREO, Current Exclusion 2 41 PROSPECT-I demonstrated PROSPECT, Current Exclusion STEREO, Expected Sensitivity LBN CPV Ambiguity Limit m m 10 m SBL + Gallium Anomaly (RAA + Evolution), 95% CL Δ 10 Δ 10 Upgrade & Science Goals Δ excellent performance H. Pieter Mumm for the PROSPECT collaboration 6 Primary Physics Goals Li capture Search for sterile neutrino oscillation 1 1 1 • Nuclear recoil within unique parameter space important for the reactor anomaly and Long Baseline Electronic recoil experiments. 235 • High-resolution U spectrum and flux 10−1 10−1 10−1 measurement addresses observed shape 10−2 10−1 1 10−2 10−1 1 10−2 10−1 1 sin22θ sin22θ sin22 discrepancies 14 14 θ14 Pulse shape discrimination (PSD) PROSPECT measurement strategy capable scintillator with high light yield • Unique 6Li-doped liquid scintillator as inverse Left: Comparison of sterile oscillation sensitivities for current and projected PROSPECT-II datasets. allows for excellent background beta decay target; distinct IBD topology Center: Projected PROSPECT-II sensitivity compared to selected short-baseline reactor experiments. rejection and > 5%/ E resolution. • Highly segmented array for background Right: Overlap of three year PROSPECT-II sensitivity with relevant regions of parameter space rejection and event localization • ~ 7m baseline to very compact highly- PROSPECT-II uniquely addresses a high Δ m2 region between enriched reactor core provides unique 1 eV2 - 15 eV2, and will reach the 5o sin2(2�14) sensitivity over sensitivity at high Δ m2.
    [Show full text]
  • Double Chooz: the Show Goes On!
    Double Chooz: The Show Goes On! Lindley Winslow University of California Los Angeles On behalf of the Double Chooz Collaboration The Double Chooz Collaboration: Brazil France Germany Japan Russia Spain USA CBPF APC EKU Tübingen Tohoku U. INR RAS CIEMAT- U. Alabama UNICAMP CEA/DSM/ MPIK Tokyo Inst. Tech. IPC RAS Madrid ANL UFABC IRFU: Heidelberg Tokyo Metro. U. RRC U. Chicago SPP RWTH Aachen Niigata U. Kurchatov Columbia U. SPhN TU München Kobe U. UCDavis SEDI U. Hamburg Tohoku Gakuin U. Drexel U. SIS Hiroshima Inst. IIT SENAC Tech. KSU CNRS/IN2P3: LLNL Subatech MIT IPHC U. Notre Dame Spokesperson: U. H. de Kerret (IN2P3) Tennessee Project Manager: Ch. Veyssière (CEA-Saclay) Web Site: www.doublechooz.org/ 2 Theory favored small sin 2θ13! Model Review Theory Order of Magnitude Prediction by Albright et. al. ArXiv:0803.4176 Le-Lμ-Lτ 0.00001 SO(3) 0.00001 Neutrino Factory S3 and S4 0.001 Designs A4 Tetrahedral 0.001 Texture Zero 0.001 Reactor Experiment RH Dominance 0.01 Design SO(10) with Sym/Antisym 0.01 Contributions Limit as SO(10) with lopsided 0.1 masses of 2011 Measuring the last mixing angle: 1.0 Probability 2 2 2 P = 1 - sin 2!13 sin (1.27 "m L/E)! Distance ~1000 meters Measuring the last mixing angle: 1.0 Probability 2 2 2 P = 1 - sin 2!13 sin (1.27 "m L/E)! Distance ~1000 meters Remember: We are looking for an effect as a function of L/E. Construction Underway! Double Chooz Analysis is Unique: • Analysis uses BOTH Rate and Energy information ➙Detailed Energy Response Model • Simple Reactor Configuration ➙ Multiple analysis periods.
    [Show full text]
  • Highlight Talk from Super-Kamiokande †
    Communication Highlight Talk from Super-Kamiokande † Yuuki Nakano and on behalf of the Super-Kamiokande Collaboration Kamioka Observatory, Institute for Cosmic Ray Research, The University of Tokyo, Higashi-Mozumi 456, Kamioka-cho, Hida-city Gifu 506-1205, Japan; [email protected]; Tel.: +81-578-85-9665 † This paper is based on the talk at the 7th International Conference on New Frontiers in Physics (ICNFP 2018), Crete, Greece, 4–12 July 2018. Received: 30 November 2018; Accepted: 7 January 2019; Published: 9 January 2019 Abstract: Super-Kamiokande (SK), a 50 kton water Cherenkov detector in Japan, is observing both atmospheric and solar neutrinos. It is also searching for supernova (relic) neutrinos, proton decays and dark matter-like particles. A three-flavor oscillation analysis was conducted with the atmospheric neutrino data to study the mass hierarchy, the leptonic CP violation term, and other oscillation parameters. In addition, the observation of solar neutrinos gives precise measurements of the energy spectrum and oscillation parameters. In this proceedings, we given an overview of the latest results from SK and the prospect toward the future project of SK-Gd. Keywords: Super-Kamiokande; atmospheric neutrino; solar neutrino; neutrino oscillation; CP violation; proton decay 1. Introduction A theoretical framework of neutrino oscillation has been established in the past 50 years [1,2]. Neutrino physics has been dominated by the measurement of oscillation parameters and such measurements suggest that neutrinos are massive and mixing in the lepton sector [3]. Within the three- 2 2 flavor framework, three mixing angles (q12, q23, and q13) and two mass splittings (Dm21 and Dm32,31) are measured among neutrino experiments.
    [Show full text]
  • Overview of Hyper-Kamiokande
    Overview of Hyper-Kamiokande Masato Shiozawa ANT11 Workshop, Oct.-10-2011 Kamioka Observatory, Institute for Cosmic Ray Research, U of Tokyo, and Kamioka Satellite, Institute for the Mathematics and Physics of the Universe, U of Tokyo Establish θ13, then CP violation T2K collaboration, PRL107,041801(2011) Fogli et al., arXiv1106.6028 T2K observed indication of νμ→νe titled “Evidence of θ13>0 from global ν analysis” Data ν Osc. e CC ν ν MeV) μ+ μ CC 3 ν e CC NC 2 Nobs : 6 νe candidates Nexp : 1.5±0.3(syst) 2 for sin 2θ13=0 1 nonzero θ13 at 2.5σ Number of events /(250 Number of events 0 0 1000 2000 3000 ν Reconstructed energy (MeV) nonzero θ13 is already >3σ w/ solar and reactorν ‣T2K aims to establish nonzero θ13 and measure it w/ more data ‣reactor experiments are starting data taking (Double CHOOZ, RENO, Daya Bay) It’s now time to seriously think about next generation 2 experiments assuming θ13≠0 (sin θ13= a few %). Hyper-K WG, arXiv:1109.3262 [hep-ex] Letter of Intent: The Hyper-Kamiokande Experiment — Detector Design and Physics Potential — K. Abe,12, 14 T. Abe,10 H. Aihara,10, 14 Y. Fukuda,5 Y. Hayato,12, 14 K. Huang,4 A. K. Ichikawa,4 M. Ikeda,4 K. Inoue,8, 14 H. Ishino,7 Y. Itow,6 T. Kajita,13, 14 J. Kameda,12, 14 Y. Kishimoto,12, 14 M. Koga,8, 14 Y. Koshio,12, 14 K. P. Lee,13 A. Minamino,4 M. Miura,12, 14 S.
    [Show full text]
  • APC - Astroparticule Et Cosmologie Rapport Hcéres
    APC - Astroparticule et cosmologie Rapport Hcéres To cite this version: Rapport d’évaluation d’une entité de recherche. APC - Astroparticule et cosmologie. 2013, Université Paris Diderot - Paris 7, Commissariat à l’énergie atomique et aux énergies alternatives - CEA, Centre national de la recherche scientifique - CNRS, L’Observatoire de Paris. hceres-02031598 HAL Id: hceres-02031598 https://hal-hceres.archives-ouvertes.fr/hceres-02031598 Submitted on 20 Feb 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Department for the evaluation of research units AERES report on unit: AstroParticule et Cosmologie APC Under the supervision of the following institutions and research bodies: Université Paris 7 - Denis Diderot Centre National de la Recherche Scientifique Commissariat à l’Energie Atomique et aux Energies Alternatives Observatoire de Paris January 2013 Research Units Department The president of AERES "signs[...], the evaluation reports, [...]countersigned for each evaluation department by the relevant head of department (Article 9, paragraph 3, of french decree n°2006-1334 dated 3 november 2006, revised). Astro-Particule et Cosmologie, APC, UP7, CNRS, CEA, Observatoire de Paris, Mr Pierre BINETRUY Grading Once the visits for the 2012-2013 evaluation campaign had been completed, the chairpersons of the expert committees, who met per disciplinary group, proceeded to attribute a score to the research units in their group (and, when necessary, for these units’ in-house teams).
    [Show full text]
  • The Double Chooz Experiment
    The Double Chooz experiment M. Goger-Neff,¨ M. Franke, N. Haag, M. Hofmann, L. Oberauer, P. Pfahler, W. Potzel, S. Schonert,¨ H. TrinhThi, V. Zimmer Introduction The goal of the Double Chooz experiment is the precise determination of the neutrino mixing angle θ13. Two iden- tical detectors measure the electron antineutrinos emitted from two nuclear reactors at the Chooz nuclear power sta- tion in France. The far detector in 1 km distance from the reactor cores started data taking in April 2011. A second near detector at a distance of about 400 m from the reactors is currently under construction and will start data taking in 2014. The near detector will monitor the unoscillated neu- trino flux whereas the far detector is searching for a disap- pearance effect due to neutrino oscillations. If the electron antineutrinos change their flavor (for a nonzero value of θ13), a reduced electron antineutrino flux is observed at the far detector. Detector Setup The target of the Double Chooz detector consists of about 8 tons of a newly developed Gadolinium-loaded liq- uid scintillator. The detection reaction is the inverse beta + decay: ν¯e + p ! n + e . The positron created in this re- action provides a prompt scintillation light signal and car- ries the energy information of the neutrino. The neutron is captured with high probability on the Gd dissolved in Figure 1: Setup of the Double Chooz detectors. the target scintillator with a typical delay time of ∼ 30µs releasing gamma radiation with a total energy of about 8 MeV. This coincidence allows an efficient neutrino de- tection and background reduction.
    [Show full text]
  • Neutrino Experiments
    deconstruction: neutrino experiments Neutrinos zip straight through the Earth, while rarely leaving a trace. Yet these particles may hold answers to many of the key questions of 21st century particle physics. Around the world, scientists are creating an array of increasingly sophisticated neutrino experiments to find these answers. What do we know about neutrinos? Scientists have discovered many surprising and often puzzling things about neutrinos since 1956, when Frederick Reines and Clyde Cowan found the first experimental evidence for these elusive particles in an experiment that they referred to as Project Poltergeist. Today we know: • Neutrinos are among the most abundant types of particles in the universe. • Neutrino sources include fusion processes in the sun; the fission processes in nuclear power stations; the decays of isotopes such as tritium and germanium; the collisions of cosmic rays with atoms in Earth’s atmosphere; the collisions produced by particle accelerators; supernovae. • Neutrinos have no electric charge and are immune to the strong nuclear force. • Neutrinos have a tiny mass: the heaviest neutrino has less than a millionth the mass of an electron. • Neutrinos come in three different types, or flavors: electron, muon, and tau neutrinos. • Neutrinos can change (oscillate) from one type to another. The sun, for example, creates electron neutrinos. By the time they arrive on Earth, the majority have turned into muon and tau neutrinos. • Neutrinos are hard to detect. Because they only interact with ordinary matter via the weak nuclear force, most of them zip through the earth unscathed. MINOS MINOS ICARUS DOUBLE CHOOZ EXO SNO/SNO+ DAYA BAY Neutrino experiments address the key questions of particle physics In 2004, the Quantum Universe report, published by the U.S.
    [Show full text]