Solar Neutrino Results from SNO

Slides:



Advertisements
Similar presentations
Neutrinos Louvain, February 2005 Alan Martin Arguably the most fascinating of the elementary particles. Certainly they take us beyond the Standard Model.
Advertisements

Neutrino oscillations/mixing
Recent Discoveries in Neutrino Physics: Understanding Neutrino Oscillations 2-3 neutrino detectors with variable baseline 1500 ft nuclear reactor Determining.
Neutrino emission =0.27 MeV E=0.39,0.86 MeV =6.74 MeV ppI loss: ~2% ppII loss: 4% note: /Q= 0.27/26.73 = 1% ppIII loss: 28% Total loss: 2.3%
Takaaki Kajita ICRR, Univ. of Tokyo Nufact05, Frascati, June 2005.
Super-Kamiokande Introduction Contained events and upward muons Updated results Oscillation analysis with a 3D flux Multi-ring events  0 /  ratio 3 decay.
G. Sullivan - Princeton - Mar 2002 What Have We Learned from Super-K? –Before Super-K –SK-I ( ) Atmospheric Solar –SNO & SK-I Active solar –SK.
Neutrino Mass and Mixing David Sinclair Carleton University PIC2004.
From Nuclei to Neutrinos The Naming of the Denys Wilkinson Building 21 June 2002 Nick Jelley.
16 May 2002Paul Dauncey - BaBar1 Measurements of CP asymmetries and branching fractions in B 0   +  ,  K +  ,  K + K  Paul Dauncey Imperial College,
Prospects for 7 Be Solar Neutrino Detection with KamLAND Stanford University Department of Physics Kazumi Ishii.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Queen’s University, Kingston, ON, Canada
2. Present Understandings
Heavy Flavor Production at the Tevatron Jennifer Pursley The Johns Hopkins University on behalf of the CDF and D0 Collaborations Beauty University.
Experimental Status of Geo-reactor Search with KamLAND Detector
21-25 January 2002 WIN 2002 Colin Okada, LBNL for the SNO Collaboration What Else Can SNO Do? Muons and Atmospheric Neutrinos Supernovae Anti-Neutrinos.
Solar & Atmospheric. June 2005Steve Elliott, NPSS Outline Neutrinos from the Sun The neutrinos Past experiments What we know and what we want to.
October 3, 2003IFIC, UVEG-CSIC A road map to solar fluxes, osc. param., and test for new physics Carlos Pena Garay IAS ~
8/5/2002Ulrich Heintz - Quarknet neutrino puzzles Ulrich Heintz Boston University
Neutrino Physics - Lecture 3 Steve Elliott LANL Staff Member UNM Adjunct Professor ,
Chris Barnes, Imperial CollegeWIN 2005 B mixing at DØ B mixing at DØ WIN 2005 Delphi, Greece Chris Barnes, Imperial College.
Neutrino emission =0.27 MeV E=0.39,0.86 MeV =6.74 MeV ppI loss: ~2% ppII loss: 4% note: /Q= 0.27/26.73 = 1% ppIII loss: 28% Total loss: 2.3%
Neutrino Physics - Lecture 4 Steve Elliott LANL Staff Member UNM Adjunct Professor ,
Measurement of the Branching fraction B( B  D* l ) C. Borean, G. Della Ricca G. De Nardo, D. Monorchio M. Rotondo Riunione Gruppo I – Napoli 19 Dicembre.
Results and Prospects for SNO
The Importance of Low-Energy Solar Neutrino Experiments Thomas Bowles Los Alamos National Laboratory Markov Symposium Institute for Nuclear Research 5/13/05.
Solar Neutrinos Perspectives and Objectives Mark Chen Queen’s University and Canadian Institute for Advanced Research (CIFAR)
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
Latest SNO Results from Salt-Phase Data and Current NCD-Phase Status Melin Huang ● Introduction ● Results of Salt Phase (Phase II) ● Status of NCD Phase.
Solar neutrino measurement at Super Kamiokande ICHEP'04 ICRR K.Ishihara for SK collaboration Super Kamiokande detector Result from SK-I Status of SK-II.
Results from Sudbury Neutrino Observatory Huaizhang Deng University of Pennsylvania.
Neutrino Physics from SNO Aksel Hallin University of Alberta Erice, 2009.
Michael Smy UC Irvine Solar and Atmospheric Neutrinos 8 th International Workshop on Neutrino Factories, Superbeams & Betabeams Irvine, California, August.
Methods and problems in low energy neutrino experiments (solar, reactors, geo-) I G. Ranucci ISAPP 2011 International School on Astroparticle physics THE.
Monday, Feb. 24, 2003PHYS 5326, Spring 2003 Jae Yu 1 PHYS 5326 – Lecture #11 Monday, Feb. 24, 2003 Dr. Jae Yu 1.Brief Review of sin 2  W measurement 2.Neutrino.
B c mass, lifetime and BR’s at CDF Masato Aoki University of Tsukuba For the CDF Collaboration International Workshop on Heavy Quarkonium BNL.
Solar Neutrino Experiments A Review The CAP'09 Congress Moncton, 7-10 June, 2009 Alain Bellerive On behalf of the SNO Collaboration Carleton University,
Wednesday, Feb. 14, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #6 Wednesday, Feb. 14, 2007 Dr. Jae Yu 1.Neutrino Oscillation Formalism 2.Neutrino.
SNO and the new SNOLAB SNO: Heavy Water Phase Complete Status of SNOLAB Future experiments at SNOLAB: (Dark Matter, Double beta, Solar, geo-, supernova.
Latest Results from the MINOS Experiment Justin Evans, University College London for the MINOS Collaboration NOW th September 2008.
Solar neutrino results from Super-Kamiokande Satoru Yamada for the Super-Kamiokande collaboration Institute of cosmic ray research, University of Tokyo.
Tests of non-standard neutrino interactions (NSI) Cecilia Lunardini Institute for Nuclear Theory University of Washington, Seattle.
Study of solar neutrino energy spectrum above 4.5 MeV in Super-Kamiokande-I 1, Solar Neutrino Oscillation 2, Super-Kamiokande detector 3, Data set for.
New Results from the Salt Phase of SNO Kathryn Miknaitis Center for Experimental Nuclear Physics and Astrophysics, Univ. of Washington For the Sudbury.
Yoshihisa OBAYASHI, Oct. Neutrino Oscillation Experiment between JHF – Super-Kamiokande Yoshihisa OBAYASHI (Kamioka Observatory, ICRR)
Search for Electron Neutrino Appearance in MINOS Mhair Orchanian California Institute of Technology On behalf of the MINOS Collaboration DPF 2011 Meeting.
J. Goodman – January 03 The Solution to the Solar Problem Jordan A. Goodman University of Maryland January 2003 Solar Neutrinos MSW Oscillations Super-K.
Data Processing for the Sudbury Neutrino Observatory Aksel Hallin Queen’s, October 2006.
Results from RENO Soo-Bong Kim (KNRC, Seoul National University) “17 th Lomosonov Conference on Elementary Particle Physics” Moscow. Russia, Aug ,
Search for Sterile Neutrino Oscillations with MiniBooNE
J. Dunmore, University of Oxford NDM03, 10 June 2003 Event Isotropy in the Salt Phase of SNO Jessica Dunmore University of Oxford NDM03, Nara - 10 June.
Medium baseline neutrino oscillation searches Andrew Bazarko, Princeton University Les Houches, 20 June 2001 LSND: MeVdecay at rest MeVdecay in flight.
CP phase and mass hierarchy Ken-ichi Senda Graduate University for Advanced Studies (SOKENDAI) &KEK This talk is based on K. Hagiwara, N. Okamura, KS PLB.
P Spring 2002 L18Richard Kass The Solar Neutrino Problem M&S Since 1968 R.Davis and collaborators have been measuring the cross section of:
Solar Neutrinos By Wendi Wampler. What are Neutrinos? Neutrinos are chargeless, nearly massless particles Neutrinos are chargeless, nearly massless particles.
Recent Results from RENO NUFACT2014 August. 25 to 30, 2014, Glasgow, Scotland, U.K. Hyunkwan Seo on behalf of the RENO Collaboration Seoul National University.
Supernova Relic Neutrinos (SRN) are a diffuse neutrino signal from all past supernovae that has never been detected. Motivation SRN measurement enables.
5th June 2003, NuFact03 Kengo Nakamura1 Solar neutrino results, KamLAND & prospects Solar Neutrino History Solar.
Review of experimental results on atmospheric neutrinos Introduction Super-Kamiokande MACRO Soudan 2 Summary Univ. of Tokyo, Kamioka Observatory.
News from the Sudbury Neutrino Observatory Simon JM Peeters July 2007 o SNO overview o Results phases I & II o hep neutrinos and DSNB o Update on the III.
Results and Prospects with the Sudbury Neutrino Observatory Neutrinos and SNO Phase III Results Low Threshold Analysis Future (maybe) Josh Klein University.
Observation Gamma rays from neutral current quasi-elastic in the T2K experiment Huang Kunxian for half of T2K collaboration Mar. 24, Univ.
Mats Selen, HEP Measuring Strong Phases, Charm Mixing, and DCSD at CLEO-c Mats Selen, University of Illinois HEP 2005, July 22, Lisboa, Portugal.
First Results from Phase II of the Sudbury Neutrino Observatory Joshua R. Klein University of Texas at Austin  Solar Neutrinos  Review of Phase I Solar.
Solar Neutrino Problem
“Solar” Neutrino Oscillations (Dm2, q12)
Sudbury Neutrino Observatory
Davide Franco for the Borexino Collaboration Milano University & INFN
Intae Yu Sungkyunkwan University (SKKU), Korea KNO 2nd KNU, Nov
Presentation transcript:

Solar Neutrino Results from SNO Kevin Graham Carleton University

Ray Davis and John Bahcall

Solar Neutrino Measurements understanding how the sun works - solar neutrino problem - solar neutrino flux measurements - temporal/consistency evaluations neutrino physics - flavour change/oscillation - MNSP parameters - new physics? 2n oscillation probability (modified by MSW for solar)

Solar Neutrino Spectra 8B Standard Solar Model (5.69 ± 0.91)x106 cm2 s-1 18.77 MeV hep SSM (7.97 ± 1.24)x103 cm2 s-1

The SNO Detector 9438 Inward- Looking PMTs 2039 m to surface 91 Outward Looking PMTs (Veto) 12 m diameter Acrylic vessel Norite Rock PMT Support Structure (PSUP) 5300 tonnes light water ~1000 tonnes heavy water 1700 tonnes light water

cosq = 1/(index of refraction) ~420 What We Measure Cherenkov Light cosq = 1/(index of refraction) ~420 PMT Measurements position charge time Reconstructed Event -event vertex -event direction -energy -isotropy

Neutrino Reactions in SNO CC n + d  p + p + e− e Q = 1.445 MeV good measurement of ne energy spectrum some directional info  (1 – 1/3 cosq) ne only NC x n +  p d Q = 2.22 MeV measures total 8B n flux from the Sun equal cross section for all n types ES n + e−  n + e− x x low statistics mainly sensitive to ne, some n and n strong directional sensitivity

SNO Data Taking Phases Phase I (pure D2O): 306.4 live days Te > 5 MeV R < 550 cm 2928 events n capture on D Single 6.25 MeV g High CC-NC corr. Te constrained Phase II (salty D2O): 391 live days Te > 5.5 MeV R < 550 cm 4722 events n capture on Cl Multiple g’s 8.6 MeV High CC-NC corr. Te unconstrained Phase III (3He n counters): n capture on 3He n + 3He g p + t Channels indep. gno correlation Reduced NC systematics counters in and collecting data Initial Results Recent Results Now Running

Signal Extraction maximum likelihood fit of model PDF’s to data event variables R (radial position) b14(isotropy) cosqsun and E(energy) b14 CC-NC separation cosqsun CC NC ES ES separation don’t use E g “energy-unconstrained” g fit out CC spectrum!

Results from Complete Phase II CC 2176+/-78 ES 279+/-26 NC 2010+/-85 #EVENTS 4722 candidate events 391 live days a Flux Results CC Energy Spectrum Neutrino Flavour Change! no significant sterile or NSI effects Day/Night Asymmetry

Global analysis of solar and reactor data “LMA I” only allowed region Maximal mixing rejected at ~5 s Solar + KamLAND

SNO Periodicity Analysis search for sinusoidal periodicity in Phase I and Phase II data used both a Lomb-Scargle periodogram and an unbinned maximum likelihood fit. (see PRD 72 2005, 052010) event arrival times are fit to: (t) = N [1 + A cos(2pft+d)] largest peak in combined data set occurs at a period of 2.4 days, with a significance statistic of S=8.8 Monte Carlo shows that 35% of simulated data sets give a peak at least this large. No evidence for modulation in any of SNO's data.

hep < 2.3 x 104 cm-2 s-1 (90% C.L.) <2.9 SSM Preliminary Phase I hep and Diffuse Supernova Neutrino Background Observed: 2 events Expected: 3.13 ± 0.60 background 0.99 ± 0.09 signal look in ‘high’ energy windows for hep and DSNB signals 8B hep atm DSNB DSNB for 22.9 < En/MeV < 36.9 : flux limit: <70 cm-2s-1 (90%CL) predicted flux: 0.2→1.5 cm-2s-1 hep < 2.3 x 104 cm-2 s-1 (90% C.L.) <2.9 SSM

NCD Phase Data 3He + n  p + 3H + 0.76 MeV event-by-event separation (pulse shape) different systematic uncertainties precision NC measurement

Characteristic 3He(n,p)t Spectrum from Calibration Data from 3He NCD-Strings Alpha Background Next adding Pulse Shape Discrimination Fit Characteristic 3He(n,p)t Spectrum from Calibration

Summary So far: What is next: 8B neutrino results from first two phases including fluxes, spectrum, D/N asymmetry search for periodicity in data hep and diffuse SN neutrino results What is next: first results from NCD phase muon and atmospheric analysis combined phase I and II results with lower energy threshold supernova watch other results to come! flavour change MSW effect q12 and Dm2 solar physics

Solar Neutrinos 8B only tiny fraction of solar neutrinos chlorine and gallium experiments integrate over different chains no real low energy spectrum 7Be interesting but large model uncertainty pep has small uncertainty and at ‘right’ energy can provide most physics

2n oscillation probability <Ynm|Yne> Neutrino Mixing for two neutrino mixing flavour eigenstates different from mass eigenstates (like quark CKM) e,m,t 1,2,3 2n oscillation probability <Ynm|Yne> Experimental Parameters L = distance to experiment E = neutrino energy Physics Parameters Dm2=m12-m22 sin22q appearance/disappearance

3 Neutrinos + Matter Effect 3 neutrinos (at least) a4 model parameters matter enhancement modifies oscillation amplitude (MSW effect) ne e W

Vacuum vs Matter Enhanced Survival Probability start with ne in sun transition region matter enhanced oscillation vacuum oscillation ne solar pp pep 8B

What do 8B n Measurements Tell Us? Fluxes - CC/NC ratio Day/Night - asymmetry CC Energy Spectrum -shape distortion Increasing Δm2 Decreasing q No. of CC events 6 MeV 13 MeV hep-ph/0406328 July 21 2004 Bandyopadhyay, Choubey, Goswami, Petcov, and Roy

Flux Results from Complete Phase II CC 2176+/-78 ES 279+/-26 NC 2010+/-85 #EVENTS 4722 candidate events 391 live days a energy-unconstrained results Unconstrained Fit Key Systematics CC NC Energy scale -0.9% +1.0% -3.3% +3.8% β14 mean -4.0% +3.7% -3.6% +4.5% Radial scale -2.6% +2.5% -3.0% +3.3% n capture -2.3% +2.1% Total -5.4% +4.8% -6.9% +7.7% Neutrino Flavour Change!

Measured Total Flux and SSM Predictions 8B Flux experimental uncertainty smaller than theoretical for this sector of solar neutrinos

Day-Night Asymmetries ACC= -0.056 ± 0.074 (stat.) ± 0.051 (syst.) ANC= 0.042 ± 0.086(stat.) ± 0.067 (syst.) AES= 0.146 ± 0.198(stat.) ± 0.032 (syst.) Constraining ANC to be zero: ACC= -0.037 ± 0.063(stat.) ±0.032(sys.) AES= 0.153 ± 0.198(stat.) ±0.030(sys.) Combined Pure D2O and Salt No evidence for asymmetries from matter effects in the earth

2-n oscillation region defined by SNO Allowed regions

Muon and atmospheric neutrino analysis