Sterile Neutrino Experiments at Accelerator
|
|
- Emerald Lambert
- 5 years ago
- Views:
Transcription
1 Sterile Neutrino Experiments at Accelerator Takeo Kawasaki Kitasato University Rencontres du Vietnam, Neutrinos, Quy Nhon, July 16-22,2017 1
2 Outline Neutrino oscillation Sterile neutrino 3+1 model Neutrino oscillation experiments at accelerator Indication of sterile neutrino LSND MiniBooNE Sterile neutrino search at accelerator experiment JSNS 2 SBN NuPRISM Summary 2
3 Matrix elements Neutrino mixing matrix (3 flavors) ν e ν μ ν τ = U e1 U μ1 U τ1 U e2 U μ2 U τ2 U e3 U μ3 U τ3 ν 1 ν 2 ν 3 Ex) P ν μ ν μ Monochromatic energy case 1/Δm 2 ν oscillation is explained by mixing matrix elements and mass difference. Most Exp. Results are consistent with 3 neutrino mixing model. 3
4 Neutrino mixing matrix (4 or more flavors) If there are more generations, it affect to the oscillation ν e ν μ ν τ ν s = U e1 U μ1 U τ1 U s1 U e2 U μ2 U τ2 U s2 U e3 U μ3 U τ3 U s3 U e4 U μ4 U τ4 U s4 ν 1 ν 2 ν 3 ν 4 m 4 2 m 2 ν e ν μ ν τ ν S 2 Δm new For 3(n a ) + 1(n s ) & m 4 >> m 1~3 case, 0 P ν e ν e 1 4 U S4 2 U e4 2 sin 2 m 4 2 L 4E ν P ν μ ν e 4 U μ4 2 Ue4 2 sin 2 m 4 2 L 4E ν P ν μ ν μ 1 4 U S4 2 U μ4 2 sin 2 m 4 2 L 4E ν n e disappearance n m n e appearance n m disappearance Reactor &source Exp. Accelerator Exp. can measure n s may be detected by n oscillations 4
5 Reactor/RI source Accelerator Exp. E-L relation of n oscillation experiments Suekane@HINT2016 P ν α ν β = sin 2 2θ sin 2 Δm ij 2 L 4E ν There are indications of 3 rd Dm 2 which requires 4 or more n s. 2 Dm 2 s are confirmed Solar n 5
6 Reactor/RI source Accelerator Exp. E-L relation of n oscillation experiments Suekane@HINT2016 P ν α ν β = sin 2 2θ sin 2 Δm ij 2 L 4E ν There are indications of 3 rd Dm 2 which requires 4 or more n s. SBN NuPRISM 2 Dm 2 s are confirmed JSNS2 Solar n 6
7 How to make neutrino beam Decay in Flight Proton beam Target π π ± π + Horn magnet Choose flavor K + π ± (in flight) μ ± + ν μ μ + Decay volume ν μ Off-Axis On-Axis ν e ~0.5% contamination Decay at Rest Proton beam π ± ν μ π + μ + νμ Stopper π and μ captured in the beam stopper material ν e 7
8 Indications of Sterile neutrinos Experiment ν source Mode Significance LSND Decay-At-Rest ν μ ν e 3.8σ MiniBooNE Decay-In-Flight ν μ ν e 3.4σ νμ νe 2.8σ combined 3.8σ Ga-Solar e capture n e n x 2.7σ Reactor b-decay n e n x 3.0σ Strong indication at Appearance modes at Accelerator experiment Reactor/source experiments show indication at Disappearance mode. However, no positive result at Dis-appearance mode at Accelerator Exp. 8
9 LSND experiment The most significant indication of the sterile n Decay At Rest 800MeV, proton beam 120Hz, 600ms Duty factor= 6% Inverse b decay (ν e only) Neutron capture Liquid Scintillator π ± produced at the water Target 9
10 LSND Results Phys. Rev. D64, (2001) Oscillation Parameter νe excess = 87.9 ± 22.4 ± 6.0 events To reject beam/cosmic related BG, many complicated cut were applied. Unknown systematics may have been introduced. 10
11 MiniBooNE experiment MiniBooNE Detector Placed at 500m to preserve LSND results with similar L/E 800-ton mineral oil Cherenkov/Scintillation Ring topology to separate e, μ and π 0 Can t distinguish e from γ π ± (in flight) μ ± + ν μ ν μ energy 400/600MeV Oscillation ν μ ν e νμ νe Detection mode: ν e + n e + p νe + p e + + n 11
12 MiniBooNE results Phys. Rev. Lett.110, (2013) 2.8σ Event excess ν mode: 78.4 ± σ ν mode: ± σ 3.4σ ν mode case; Large excess at low energy <475MeV But no excess at higher energy. The fit result doesn t explain it? Due to miss-id γ as electron? 12
13 MiniBooNE/LSND Results Comparison Phys Rev. D80, (2009) Phys. Rev. Lett.110, (2013) MiniBooNE ν mode is more compatible with LSND result compared with ν mode. How the difference is explained? 13
14 Short baseline accelerator experiments in preparation LSND/MiniBooNE results should be checked by accelerator experiment for Appearance/Dis-Appearance mode. J-PARC(Japan Accelerator Research Complex) Fermilab Booster n beam NuPrism SBN program JSNS 2 n Beam To Kamioka JSNS DAR/Appearance SBN program@fermilab BNB NuPrism@J-PARC /n -beam line DIF/Appearance/Dis-appearance 14
15 Direct test of LSND result JSNS Life science Facility Stage-1 approved. Funded for 1 detector TDR released on May 2017 arxiv: Members experienced at Reactor Exps. (Daya-Bay, DoubleChooz,RENO) Consists of -21 institutes -53 collaborators -Japan/US/Korea MLF Exp. Hall JSNS 2 : J-PARC Sterile Neutrino Search at J-PARC Spallation Neutron Source. 15
16 Experimental site: J-PARC MLF Use existing building and beam facility Detector positon : 3 rd floor (L=24m) Mercury target (neutron&neutrino source) p + Hg π ± + X π + stop μ + + ν μ (t=2.2ms) μ + stop e + + ν e + νμ n source and oscillation mode are same as LSND Oscillation 3GeV, 1MW Proton beam νe Thanks to high-z of Hg, νe from μ decays are suppressed to 1/1,
17 ν beam DT=40ms(25Hz) Expected spectrum observed for L=24m 0.5eV 2 Δm 2 = 2.5eV 2 3.5eV 2 4.5eV 2 n from p & K decays n from m decay. n timing window =1~10ms - Signal - νefrom μ (normalized) Pulsed beam can reduce beam BKG and accidental BKG drastically Cosmic-ray and accidental BG: suppression factor= 9ms/40ms~2x
18 JSNS 2 :Detector Gd-loaded Liq. Scintillator 17 tons 2 (Established for reactor Exp.) νe + p n + e + (prompt) Depends on Gd concentration n Gd 158 Gd + γs (delayed; Q~8MeV, t cap ~30ms) 253,000b for thermal n Delayed coincidence Prompt; t e =1~10ms, E e =20~60MeV Delayed; t g =t p ~100ms, E g =7~12MeV Surface level without overburden Further BG suppression with PSD (Pulse shape discrimination) Use 2 of them. (1 detector funded) 18
19 JSNS 2 :Detector Normal LS Gd-LS 3 rd Floor for MLF maintenance work Use 2 of them. The detector size is limited by Facility requirement. Well established technology for reactor experiments. Gd loaded LS in transparent Acrylic tank Normal LS in Stainless Tank inch PMTs to ensure good Energy resolution Huge cosmic induced BG at surface level. LS region is divided to make Veto region. Neutron beam lines 19
20 Comparison with LSND Neutrino beam Detector Facility Beam Pow. [MW] Rep. Rate [Hz] Pulse Width [ns] Duty Factor JSNS 2 J-PARC/MLF e-5 LSND LANL/LAMPF e Type Mass [t] L [m] JSNS 2 Gd-LS with PSD LSND LS JSNS 2 : S/N > 1,000 LSND 20
21 JSNS 2 sensitivity (3y, 1 MW, 17 tons) Expected spectrum Case Δm 2 = 2.5eV 2, sin 2 2θ = Case Δm 2 = 1.2eV 2, sin 2 2θ =
22 Schedule for the 1st Detector (17-ton) JSNS2 group is now preparing for the 1 st detector construction Japan Fiscal Year (April March) JFY S.S/Acrylic Tank PMT install LS production Dry run LS filling Start Exp. Run Now Continuous work for 2 nd detector (17t) for increase of statistics and measurement with different baseline. The bidding of Stainless tank was started on June, 2017! 22
23 JSNS 2 status We have experiences at reactor Expetiments Work for Detector construction (from TDR) Stainless/Acrylic Tank design (inner)pmt location Consideration on Acrylic tank and PMTinstallation to S.S tank. 23
24 Compatibility tests of material inside Liquid Scintillators. It is Important to chose the material installed into LS (LAB Check attenuation length of the liquids and the condition of the material surface/weight after long soak. FINEMET for PMT magnetic shield LUIREMIRROR for light reflection at veto region 24
25 PMT Gain and P/V ratio were measured for PMT candidate. 25
26 SBN Address MiniBooNE anomaly Funded Booster neutrino Beam ~700MeV L/E ~ 1km/GeV Use 3 Liquid Argon TPCs( t) Good separation e/γ Study ν-lar cross section Further development for DUNE Sensitive to sterile oscillation ν μ ν e appearance ν μ ν μ dis-appearance I borrowed the slides from * Neutrino2016 arxive:
27 n-beam penetrates 3 LAr TPCs (soon) (running) 27
28 28
29 Sensitivities for sterile ν oscillations(3yrs) 29
30 neutrino beamline Stage1 approved ~10m Use movable detector in a shaft hole Water Cherenkov, ~1000 ton (depends on baseline) Baseline :1-2km (not fixed yet) Study ν nuclear interaction with various energy ~15m It is sensitive to sterile ν oscillation Both appearance/dis-appearance mode 30
31 θ OA = 4.0 θ OA = 2.5 With Off-axis beam technique. Large angle gives sharp E ν distribution. θ OA = 1.0 Change Off-Axis angle by moving detector in a shaft, 31
32 NuPRISM: sterile n sensitivity T2K II exposure(2e21 POT) ν e appearance mode 32
33 Comparison of the future projects JSNS2 SBND/mBooN/ICARUS nuprism Accelerator J-PARC/MLF Fermilab BnB J-PARC/n E n [MeV] ~50 ~ ~1500 n source m + DAR p + DIF p + DIF L[m] /470/ ~2000 (-) (-) (-) (-) Osc. mode νμ νe n m n e, n m n m n m n e, n m n m Detector Gd-LS LAr-TPC Water Cherenkov Fid. Mass(t) 17(phase0) 112/87/ (depnds on L) Characteristic Status Direct Test of LSND funded for 1detector Full n-ar interaction reconstruction. Near/Far cancellation funded Commissioning 2018~9 2018~9/2015/ Cost $ $$$ $$$ Wide range semimonochromatic n stage-1 approval 33
34 Summary There are some indications of sterile neutrinos Significant at LSND/MiniBooNE: Δm 2 ~O(eV) at ν e appearance mode Reactor/Source Exp. also show it in ν e dis-appearance mode SBL Accelerator experiments are sensitive to ν μ ν e and ν μ ν x Experiments are in preparation JSNS2@J-PARC is funded for 1 detector SBN@FermiLAB is funded and will start soon Those are complementary to the reactor/source experiments The interesting results will appear in a few years. 34
Bari Osmanov, University of Florida. OscSNS - proposal for neutrino experiment at ORNL SNS facility
, University of Florida OscSNS - proposal for neutrino experiment at ORNL SNS facility 1 of 19 Outline ORNL SNS facility Neutrino production at SNS Neutrino detection at SNS Event reconstruction and particle
More informationThe Hunt for Sterile Neutrinos. H. Ray, University of Florida
The Hunt for Sterile Neutrinos 1 Particle Physics is Over!..finding the Higgs arguably the most important discovery in more than a generation has left physicists without a clear roadmap of where to go
More informationThe Double Chooz Project
The Double Chooz Project Progress and Expected Sensitivity David McKee, KSU 13 17 July 2009 TeVPA @ SLAC Outline I. Neutrino mixing and θ 13 II. Existing θ 13 measurements III. This is hard with a single
More informationNeutrino Experiments with Reactors
Neutrino Experiments with Reactors 1 Ed Blucher, Chicago Lecture 2 Reactors as antineutrino sources Antineutrino detection Reines-Cowan experiment Oscillation Experiments Solar Δm 2 (KAMLAND) Atmospheric
More informationDaya Bay and joint reactor neutrino analysis
Daya Bay and joint reactor neutrino analysis Logan Lebanowski (Tsinghua University) on behalf of the Daya Bay collaboration 2016/11/4 - NNN16, Beijing 1 Contents Daya Bay Reactor Neutrino Experiment Introduction
More informationOak Ridge and Neutrinos eharmony forms another perfect couple
Oak Ridge and Neutrinos eharmony forms another perfect couple H. Ray University of Florida 05/28/08 1 Oak Ridge Laboratory Spallation Neutron Source Accelerator based neutron source in Oak Ridge, TN 05/28/08
More informationThe Short Baseline Neutrino Program at Fermilab
Yale University E-mail: serhan.tufanli@cern.ch The Short-Baseline Neutrino (SBN) program at Fermilab is a short-baseline neutrino experiment with the main goal of performing definitive search for neutrino
More informationTakasumi Maruyama (KEK) 2018/June/21
Takasumi Maruyama (KEK) 2018/June/21 Sterile neutrinos Sterile neutrinos could give an insight for the questions beyond the standard model; (E.g.; PLB 631, 151 (2005)) No strong, electro-magnetic, weak
More informationWei Wang University of Wisconsin-Madison. NNN09, Estes Park, Colorado, Oct 8, 2009
The Hunt for at Daya Bay University of Wisconsin-Madison NNN09, Estes Park, Colorado, Oct 8, 2009 Outline Neutrino oscillation and the search for θ 13 The Daya Bay neutrino experiment - Design of the Daya
More informationOak Ridge National Laboratory, TN. K. Scholberg, Duke University On behalf of the COHERENT collaboration August 2, 2017 DPF 2017, Fermilab
Oak Ridge National Laboratory, TN K. Scholberg, Duke University On behalf of the COHERENT collaboration August 2, 2017 DPF 2017, Fermilab Coherent elastic neutrino-nucleus scattering (CEvNS) n + A n +
More informationObservation of Reactor Antineutrinos at RENO. Soo-Bong Kim for the RENO Collaboration KNRC, Seoul National University March 29, 2012
Observation of Reactor Antineutrinos at RENO Soo-Bong Kim for the RENO Collaboration KNRC, Seoul National University March 29, 2012 Outline Introduction Experimental setup & detector Data-taking & data
More informationCorrelated Background measurement in Double Chooz experiment
Correlated Background measurement in Double Chooz experiment Guillaume Pronost (Supervisor : Frederic Yermia) SUBATECH Journe es de Rencontres des Jeunes Chercheurs 2013 OUTLINE 1 - Neutrino Physics 2
More informationNeutrino Experiments: Lecture 3 M. Shaevitz Columbia University
Neutrino Experiments: Lecture 3 M. Shaevitz Columbia University 1 Outline 2 Lecture 1: Experimental Neutrino Physics Neutrino Physics and Interactions Neutrino Mass Experiments Neutrino Sources/Beams and
More informationThe Daya Bay Reactor Neutrino Experiment
The Daya Bay Reactor Neutrino Experiment Ming-chung Chu The Chinese University of Hong Kong, Hong Kong On behalf of the Daya Bay Collaboration Partial support: CUHK VC Discretionary Fund, RGC CUHK3/CRF/10R
More informationMiniBooNE, LSND, and Future Very-Short Baseline Experiments
1 MiniBooNE, LSND, and Future Very-Short Baseline Experiments Mike Shaevitz - Columbia University BLV2011 - September, 2011 - Gatlinburg, Tennessee Neutrino Oscillation Summary 2! µ "! Sterile "! e New
More informationNeutrino Experiments: Lecture 2 M. Shaevitz Columbia University
Neutrino Experiments: Lecture 2 M. Shaevitz Columbia University 1 Outline 2 Lecture 1: Experimental Neutrino Physics Neutrino Physics and Interactions Neutrino Mass Experiments Neutrino Sources/Beams and
More informationThe Daya Bay Reactor Neutrino Oscillation Experiment
The Daya Bay Reactor Neutrino Oscillation Experiment Measurement of θ 13 Mixing Parameter Viktor Pěč for the Daya Bay Experiment Collaboration Charles University in Prague EPS HEP09, Neutrino Physics,
More informationNeutrino Experiment. Wei Wang NEPPSR09, Aug 14, 2009
Search for at the Daya Bay Neutrino Experiment, Aug 14, 2009 Outline Neutrino oscillation and the search for θ 13 The Daya Bay neutrino experiment - Design of the Daya Bay detector - Systematic uncertainty
More informationStatus and Neutrino Oscillation Physics Potential of the Hyper-Kamiokande Project in Japan
Status and Neutrino Oscillation Physics Potential of the Hyper-Kamiokande Project in Japan Gianfranca De Rosa Univ. Federico II and INFN Naples On behalf of Hyper-Kamiokande Collaboration Hyper-Kamiokande:
More informationarxiv:hep-ex/ v1 15 Aug 2006
The Double Chooz Experiment 1 Daniel M. Kaplan (for the Double Chooz Collaboration) Illinois Institute of Technology, 3101 South Dearborn Street, Chicago, Illinois, USA arxiv:hep-ex/0608040v1 15 Aug 2006
More informationKamLAND. Studying Neutrinos from Reactor
KamLAND : Studying Neutrinos from Reactor Atsuto Suzuki KEK : High Energy Accelerator Research Organization KamLAND Collaboration Outline 1. KamLAND Overview 2. Reactor Neutrinos 3. e Detection in Liquid
More informationNeutrino oscillation physics potential of Hyper-Kamiokande
Neutrino oscillation physics potential of Hyper-Kamiokande on behalf of the Hyper-Kamiokande Collaboration Queen Mary University of London E-mail: l.cremonesi@qmul.ac.uk Hyper-Kamiokande (Hyper-K) is a
More informationAn Underground Laboratory for a Multi-Detector Experiment. Karsten Heeger Lawrence Berkeley National Laboratory
Measuring sin 2 2θ 13 with Reactor Antineutrinos at Daya Bay An Underground Laboratory for a Multi-Detector Experiment Karsten Heeger Lawrence Berkeley National Laboratory On behalf of the Daya Bay collaboration
More information500m. 1000m. /POT/GeV/cm 2. (GeV) E ν 10-14
1 The Future of the Short-Baseline Neutrino Oscillation Experiments in the US: MiniBooNE and ORLaND Ion Stancu a a Department of Physics, University of California, Riverside, CA 92521, USA E-mail: ion.stancu@ucr.edu
More information章飞虹 ZHANG FeiHong INTERNATIONAL SCHOOL OF SUBNUCLEAR PHYSICS Ph.D. student from Institute of High Energy Physics, Beijing
章飞虹 ZHANG FeiHong zhangfh@ihep.ac.cn Ph.D. student from Institute of High Energy Physics, Beijing INTERNATIONAL SCHOOL OF SUBNUCLEAR PHYSICS 2012 Erice, 23 June 2 July 2012 1 Before Hunting Introduction
More informationThe COHERENT Experiment: Overview and Update of Results
The COHERENT Experiment: Overview and Update of Results for the COHERENT Collaboration 2016 Fall Meeting of the APS Division of Nuclear Physics, Vancouver, B.C. ORNL is managed by UT-Battelle for the US
More informationParticle Physics: Neutrinos part I
Particle Physics: Neutrinos part I José I. Crespo-Anadón Week 8: November 10, 2017 Columbia University Science Honors Program Course policies Attendance record counts Up to four absences Lateness or leaving
More informationMeasurement of q 13 in Neutrino Oscillation Experiments. Stefan Roth, RWTH Aachen Seminar, DESY, 21 st /22 nd January 2014
Measurement of q 13 in Neutrino Oscillation Experiments Stefan Roth, RWTH Aachen Seminar, DESY, 21 st /22 nd January 2014 Overview Experiments with neutrinos Neutrino oscillations Reactor and accelerator
More informationDaya Bay Neutrino Experiment
Daya Bay Neutrino Experiment Jun Cao Institute of High Energy Physics, Beijing 3rd International Conference on Flavor Physics, Oct. 3-8, 2005 National Central University Chung-li, Taiwan Neutrino Oscillation
More informationRecent results from Super-Kamiokande
Recent results from Super-Kamiokande ~ atmospheric neutrino ~ Yoshinari Hayato ( Kamioka, ICRR, U-Tokyo ) for the Super-Kamiokande collaboration 1 41.4m Super-Kamiokande detector 50000 tons Ring imaging
More informationThe Double Chooz reactor neutrino experiment
The Double Chooz reactor neutrino experiment Christian Buck, MPIK Heidelberg MPIK July, 30th 2009 Overview Motivation Double Chooz concept and design Status of experiment MPIK activities Summary Neutrino
More informationAccelerator Neutrino Experiments News from Neutrino 2010 Athens
Accelerator Neutrino Experiments News from Neutrino 2010 Athens Ed Kearns Boston University Outline Quick overview New result 1: OPERA tau appearance New result 2: MINOS nu- e appearance Looking forward
More informationProspects for Measuring the Reactor Neutrino Flux and Spectrum
Prospects for Measuring the Reactor Neutrino Flux and Spectrum Karsten Heeger Yale University as a member of the Daya Bay and PROSPECT collaborations INT, Seattle, November 8, 2013 ν e /MeV/fisson Reactor
More informationNeutrino mixing II. Can ν e ν µ ν τ? If this happens:
Can ν e ν µ ν τ? If this happens: Neutrino mixing II neutrinos have mass (though there are some subtleties involving the MSW mechanism) physics beyond the (perturbative) Standard Model participates Outline:
More informationK2K and T2K experiments
K2K and T2K experiments Issei Kato TRIUMF, Canada for the K2K and T2K collaborations Neutrino Oscillation Workshop 2006 at Conca Specchiulla,, Otranto, Italy Outline K2K experiment, shortly What s updated
More informationNeutrino Oscilla8ons
Neutrino Oscilla8ons Kathleen Tatem Columbia University Neutrino oscilla8on experiments may be seeing signs of a new fundamental par8cle, the sterile neutrino! 1 Outline Neutrinos Proper8es Sources Neutrino
More informationθ13 Measurements with Reactor Antineutrinos
θ13 Measurements with Reactor Antineutrinos and the KASKA experiment WIN 05 Neutrino Working Group Delphi Greece on June 8 th, 2005 Y.Fukuda for the KASKA collaboration Miyagi University of Education Understanding
More information- ICARUS status and near future
Journal of Physics: Conference Series PAPER OPEN ACCESS ICARUS status and near future Related content - ICARUS status and near future Filippo Varanini and ICARUS Collaboration To cite this article: Filippo
More informationNeutrino Physics. Neutron Detector in the Aberdeen Tunnel Underground Laboratory. The Daya Bay Experiment. Significance of θ 13
Neutrino Physics Neutron Detector in the Aberdeen Tunnel Underground Laboratory John K.C. Leung Department of Physics, HKU On behalf of CUHK, LBL & IHEP Presented to HKRPS on June 21, 2007 Neutrinos have
More informationEXPLORING PARTICLE-ANTIPARTICLE ASYMMETRY IN NEUTRINO OSCILLATION. Atsuko K. Ichikawa, Kyoto University
EXPLORING PARTICLE-ANTIPARTICLE ASYMMETRY IN NEUTRINO OSCILLATION Atsuko K. Ichikawa, Kyoto University Got PhD by detecting doubly-strange nuclei using emulsion After that, working on accelerator-based
More informationNeutrino Experiments with Reactors
Neutrino Experiments with Reactors 1 Ed Blucher, Chicago Reactors as antineutrino sources Antineutrino detection Reines-Cowan experiment Oscillation Experiments Solar Δm 2 (KAMLAND) Atmospheric Δm 2 --
More informationRecent results from MiniBooNE on neutrino oscillations
Recent results from MiniBooNE on neutrino oscillations Alexis [for the MiniBooNE collaboration] IX International Symposium on High Energy Physics 1 SILAFAE 2012,, December 10 14, 2013 Outline LSND and
More informationThe Daya Bay Reactor Neutrino Experiment
The Daya Bay Reactor Neutrino Experiment Lisa Whitehead Brookhaven National Laboratory for the Daya Bay Collaboration APS Meeting, Washington, D.C. Measuring 13 at a Reactor S jk =sin jk C jk =cos jk Neutrino
More informationPoS(NOW2016)003. T2K oscillation results. Lorenzo Magaletti. INFN Sezione di Bari
INFN Sezione di Bari E-mail: lorenzo.magaletti@ba.infn.it The TK (Tokai-to-Kamioka) experiment is a second generation long baseline neutrino oscillation experiment that probes physics beyond the Standard
More informationNEUTRINOS II The Sequel
NEUTRINOS II The Sequel More About Neutrinos Ed Kearns Boston University NEPPSR V - 2006 August 18, 2006 Ed Kearns Boston University NEPPSR 2006 1 There is something unusual about this neutrino talk compared
More informationThe Search for θ13 : First Results from Double Chooz. Jaime Dawson, APC
The Search for θ13 : First Results from Double Chooz Jaime Dawson, APC Contents Brief reminder θ13 current knowledge Reactor experiments Double Chooz Far detector Calibration Neutrinos & Backgrounds Oscillation
More informationThe Nucifer Experiment: Non-Proliferation with Reactor Antineutrinos
The Nucifer Experiment: Non-Proliferation with Reactor Antineutrinos Andi S. Cucoanes1 for the Nucifer Collaboration* * V.M.Bui2, M.Cribier1, A.S.Cucoanes1, M.Fallot2, M.Fechner1, J.Gaffiot1, L.Giot2,
More informationarxiv: v1 [hep-ex] 14 May 2015
arxiv:1505.03641v1 [hep-ex] 14 May 2015 Recent Results from Daya Bay Reactor Neutrino Experiment B. Z. HU on behalf of the Daya Bay collaboration Department of Physics, National Taiwan University, No.
More informationSuper-K Gd. M.Ikeda(ICRR) for Super-K collaboration Workshop for Neutrino Programs with facilities in Japan
Super-K Gd M.Ikeda(ICRR) for Super-K collaboration 20150804@JPARC Workshop for Neutrino Programs with facilities in Japan 1 Contents Introduction to SK-Gd Physics motivations Study of Gd effect to SK Plan
More informationRecent Results from Alysia Marino, University of Colorado at Boulder Neutrino Flux Workshop, University of Pittsburgh, Dec 6 8,2012
Recent Results from Alysia Marino, University of Colorado at Boulder Neutrino Flux Workshop, University of Pittsburgh, Dec 6 8,2012 Outline T2K Beamline and Detectors Uncertainties from prior measurements
More informationRecent T2K results on CP violation in the lepton sector
Recent T2K results on CP violation in the lepton sector presented by Per Jonsson Imperial College London On Behalf of the T2K Collaboration, December 14-20 2016, Fort Lauderdale, USA. Outline Neutrino
More informationStatus of The Daya Bay Reactor Neutrino Experiment
Mary Bishai, BNL 1 p.1/29 Status of The Daya Bay Reactor Neutrino Experiment Neutrino Frontiers 2008, 10/23/2008 Mary Bishai (for the Daya Bay Collaboration) mbishai@bnl.gov Brookhaven National Lab. Mary
More informationRecent Discoveries in Neutrino Physics
Recent Discoveries in Neutrino Physics Experiments with Reactor Antineutrinos Karsten Heeger http://neutrino.physics.wisc.edu/ Karsten Heeger, Univ. of Wisconsin NUSS, July 13, 2009 Standard Model and
More informationStatus Report: A Search for Sterile Neutrino at J-PARC MLF (E56, JSNS 2 )
Status Report: A Search for Sterile Neutrino at J-PARC MLF (E56, JSNS 2 ) July 8, 2015 M. Harada, S. Hasegawa, Y. Kasugai, S. Meigo, K. Sakai, S. Sakamoto, K. Suzuya JAEA, Tokai, JAPAN E. Iwai, T. Maruyama
More informationNeutrino Masses and Mixing
Neutrino Masses and Mixing < Why so different??? (Harrison, Perkins, Scott 1999) The Mass Puzzle Seesaw mechanism L R m m D m 2 D M m D M m D L R M Heavy Majorana Neutrino Connection with high mass scales
More informationJonathan Asaadi Syracuse University
Future prospects of electron/photon 0 separation & Neutral Current π measurements with Liquid Argon TPCs and other methods ν e candidate ArgoNeuT Data ArgoNeuT Data γ candidate ArgoNeuT Data Neutral Current
More informationParticle Physics: Neutrinos part II
Particle Physics: Neutrinos part II José I. Crespo-Anadón Week 9: November 18, 2017 Columbia University Science Honors Program 3 evidences for 3 neutrinos 2 3 neutrinos: 3 charged leptons Neutrinos are
More informationParticle Physics: Neutrinos part II
Particle Physics: Neutrinos part II José I. Crespo-Anadón Week 9: April 1, 2017 Columbia University Science Honors Program Course Policies Attendance Up to four absences Send email notifications of all
More information- Future Prospects in Oscillation Physics -
Measuring θ 13 and the Search for Leptonic CP Violation - Future Prospects in Oscillation Physics - Karsten M. Heeger Lawrence Berkeley National Laboratory ν e flux θ 13 =? P ee, (4 MeV) 1/r 2 Evidence
More informationPoS(FPCP2017)024. The Hyper-Kamiokande Project. Justyna Lagoda
National Centre for Nuclear Research Otwock-Swierk, Poland E-mail: justyna.lagoda@ncbj.gov.pl The Hyper-Kamiokande is a project of a large water Cherenkov detector to be built in Japan. The design allows
More informationSensitivity to sterile ν mixings at a ν Factory --Side business of a ν Factory --
Sensitivity to sterile ν mixings at a ν Factory --Side business of a ν Factory -- Osamu Yasuda Tokyo Metropolitan University 009-1-18 @ Miami009 1 1. Introduction. Light sterile neutrinos 3. Summary 1.
More informationMeasuring Neutrino Proper0es with Liquid Argon TPCs
Measuring Neutrino Proper0es with Liquid Argon TPCs Oxford Seminar 13 October 2015 MaE Bass INTRODUCTION 2 Outline Open ques0ons in Neutrino Physics Liquid Argon Time Projec=on Chambers LAr TPC Experiments
More informationThe reactor antineutrino anomaly & experimental status of anomalies beyond 3 flavors
The reactor antineutrino anomaly & experimental status of anomalies beyond 3 flavors G. Mention CEA Saclay / Irfu / SPP Rencontres IPhT-SPP, 24 janvier 2012 Overview List of anomalies: LSND MB, anti- Gallium
More informationMiniBooNE Progress and Little Muon Counter Overview
MiniBooNE Progress and Little Muon Counter Overview Neutrino Introduction and MiniBooNE Motivation MiniBooNE Detector and LMC Calibration and Performance Progress Toward Physics Results Terry Hart, University
More informationPoS(NEUTEL2017)007. Results from RENO. Soo-Bong Kim. for the RENO collaboration Seoul National University, Republic of Korea
for the RENO collaboration Seoul National University, Republic of Korea E-mail: sbk@snu.ac.kr The Reactor Experiment for Neutrino Oscillation (RENO) has been taking data near the Hanbit nuclear power plant
More informationThe OscSNS White Paper
The OscSNS White Paper October 8, 2013 arxiv:1307.7097v3 [physics.ins-det] 7 Oct 2013 M. Elnimr, I. Stancu University of Alabama, Tuscaloosa, AL 35487 M. Yeh Brookhaven National Laboratory, Upton, NY 11973
More informationHow large is the "LSND anomaly"?
How large is the "LSND anomaly"? Andrey Elagin on behalf of the HARP-CDP group HEP lunch, UChicago, March 12, 2012 Outline 3.8 σ LSND Final Paper PRD 64, 112007 3.8 σ 2.9 σ HARP-CDP Paper I arxiv:1110.4265
More informationMINOS. Luke A. Corwin, for MINOS Collaboration Indiana University XIV International Workshop On Neutrino Telescopes 2011 March 15
MINOS Luke A. Corwin, for MINOS Collaboration Indiana University XIV International Workshop On Neutrino Telescopes 2011 March 15 2 Overview and Current Status Beam Detectors Analyses Neutrino Charged Current
More informationNeutrino Oscillations
1. Introduction 2. Status and Prospects A. Solar Neutrinos B. Atmospheric Neutrinos C. LSND Experiment D. High-Mass Neutrinos 3. Conclusions Plenary talk given at DPF 99 UCLA, January 9, 1999 Introduction
More informationBNL Very Long Baseline Neutrino Oscillation Expt.
Mary Bishai, BNL 1 p.1/36 BNL Very Long Baseline Neutrino Oscillation Expt. Next Generation of Nucleon Decay and Neutrino Detectors 8/04/2005 Mary Bishai mbishai@bnl.gov Brookhaven National Lab. Mary Bishai,
More informationGadolinium Doped Water Cherenkov Detectors
Gadolinium Doped Water Cherenkov Detectors David Hadley University of Warwick NuInt-UK Workshop 20th July 2015 Water Cherenkov Detector Super-Kamiokande 22.5 kt fiducial mass 2 Physics with Large Scale
More informationN u P J-PARC Seminar August 20, 2015
Confronting Neutrino-Nucleus Interactions at Eν~1 GeV with the Detector Mark Hartz Kavli IPMU (WPI), University of Tokyo and TRIUMF N u P August 20, 2015 R I S M Outline Long baseline neutrino experiments
More informationStatus Report: A Search for Sterile Neutrino at J-PARC MLF (E56, JSNS 2 )
Status Report: A Search for Sterile Neutrino at J-PARC MLF (E56, JSNS 2 ) July 8, 2015 arxiv:1507.07076v1 [physics.ins-det] 25 Jul 2015 M. Harada, S. Hasegawa, Y. Kasugai, S. Meigo, K. Sakai, S. Sakamoto,
More informationLong Baseline Neutrinos
Long Baseline Neutrinos GINA RAMEIKA FERMILAB SLAC SUMMER INSTITUTE AUGUST 5-6, 2010 Lecture 1 Outline Defining Long Baseline Experiment Ingredients Neutrino Beams Neutrino Interactions Neutrino Cross
More informationThe ultimate measurement?
Reactor neutrinos θ13 The ultimate measurement? Pau Novella CNRS/APC 1 Overview Neutrino oscillations and the last mixing angle Reactor neutrinos as a probe to θ13 Unrevealing θ13 with reactor neutrino
More informationAndrey Formozov The University of Milan INFN Milan
T h e i nv e s t i g a t i o n of l i q u i d s c i n t i l l a t o r p ro p e r t i e s, e n e r g y a n d s p a t i a l re s o l u t i o n fo r JUNO re a c t o r n e u t r i n o e x p e r i m e n t Andrey
More informationSTATUS OF THE J-PARC FACILITY
STATUS OF THE J-PARC FACILITY Shoji Nagamiya, J-PARC Center, 2-4 Shirakata Shirane, Tokai-Mura, Ibaraki 319-1195, Japan Abstract J-PARC (Japan Proton Accelerator Research Complex) consists of three accelerators
More informationNeutrinos. Why measure them? Why are they difficult to observe?
Outline What is a neutrino? Why do we want to study them? Building a detector to detect the undetectable What does a neutrino detector see? How do you seperate a neutrino signal from the background? Neutrinos
More informationNeutrino Physics with Short Baseline Experiments
XXVI Physics in Collision, Bu zios, Rio de Janeiro, 6-9 July 2006 Neutrino Physics with Short Baseline Experiments E. D. Zimmerman University of Colorado, Boulder, Colo. 80309 USA Neutrino physics with
More informationRecent Results from RENO & Future Project RENO-50
Recent Results from RENO & Future Project RENO-50 Sunny (Seon-Hee) Seo Seoul National University Feb. 15, 2014 KIAS- NCTS Joint Workshop 2014 @High1 Neutrino Oscillation Pontecorvo 1957 MNS 1967 Solar
More informationKamLAND. Introduction Data Analysis First Results Implications Future
KamLAND Introduction Data Analysis First Results Implications Future Bruce Berger 1 Tohoku University, Sendai, Japan University of Alabama University of California at Berkeley/LBNL California Institute
More informationSearching for Sterile Neutrinos with an Isotope β-decay Source: The IsoDAR Experiment
1 Searching for Sterile Neutrinos with an Isotope β-decay Source: The IsoDAR Experiment Mike Shaevitz - Columbia University Aspen Winter Workshop--New Directions in Neutrino Physics February 8, 2013 Where
More informationHow J-PARC recovered from the big earthquake
How J-PARC recovered from the big earthquake KEK / Fujio Naito Outline About J-PARC The earthquake Damage on J-PARC Recovery plan Beam study results Summary J-PARC (Japan Proton Accelerator Research Complex)
More informationarxiv: v1 [hep-ex] 11 May 2017
LATEST RESULTS FROM TK arxiv:1705.0477v1 [hep-ex] 11 May 017 Marcela Batkiewicz a, for the TK collaboration Institute of Nuclear Physics Polish Academy of Sciences, Cracow, Poland Abstract. The TK (Tokai
More informationNew Results for ν µ ν e oscillations in MINOS
New Results for ν µ ν e oscillations in MINOS Jelena Ilic Rutherford Appleton Lab 4/28/10 RAL PPD Seminar 1 Neutrino Mixing Mass eigenstates flavour eigenstates Maki-Nakagawa-Sakata: Flavour composition
More informationSterile Neutrinos. Carlo Giunti
C. Giunti Sterile Neutrinos PPC07 6 May 07 /5 Sterile Neutrinos Carlo Giunti INFN, Torino, Italy XI International Conference on Interconnections between Particle Physics and Cosmology Corpus Christi, Texas,
More informationRecent Results from T2K and Future Prospects
Recent Results from TK and Future Prospects Konosuke Iwamoto, on behalf of the TK Collaboration University of Rochester E-mail: kiwamoto@pas.rochester.edu The TK long-baseline neutrino oscillation experiment
More informationReactor-based Neutrino Experiment
Reactor-based Neutrino Experiment Haoqi Lu Institute of High Energy physics, China Member of the Daya Bay collaboration 2013PIC, Beijing 1 Outline Introduction Reactor-based neutrino experiment Results
More informationJelena Maricic Drexel University. For Double Chooz Collaboration. Spain. France. Germany U.S.A. Japan Russia. Brazil U.K. Courtesy of T.
Jelena Maricic Drexel University For Double Chooz Collaboration France Spain Germany U.S.A Japan Russia Brazil U.K. http://doublechooz.in2p3.fr/ J. Maricic, Drexel U 1 Courtesy of T. Lasserre ν e ν μ ν
More informationShort baseline neutrino oscillation experiments at nuclear reactors
Short baseline neutrino oscillation experiments at nuclear reactors Christian Buck, MPIK Heidelberg Erice School, Sicily Sept, 17th 2017 Neutrino oscillations = 3 2 1 3 2 1 3 2 1 3 2 1 ν ν ν ν ν ν τ τ
More informationNEW νe Appearance Results from the. T2K Experiment. Matthew Malek Imperial College London. University of Birmingham HEP Seminar 13 June 2012
NEW νe Appearance Results from the T2K Experiment Matthew Malek Imperial College London University of Birmingham HEP Seminar 13 June 2012 Outline Physics motivation: Neutrinos & Oscillations Overview of
More informationResults from T2K. Alex Finch Lancaster University ND280 T2K
Results from T2K Alex Finch Lancaster University ND280 T2K 1 Contents T2K Overview Tokai Kamioka Neutrino Oscillations Results Muon neutrino disappearance Electron neutrino appearance Charged Current inclusive
More informationA Trial of Neutrino Detection from Joyo Fast Research Reactor
A Trial of Neutrino Detection from Joyo Fast Research Reactor F.Suekane Tohoku University For KASKA group, made up of; Tohoku Univ., Tokyo Inst. of Tech., Niigata Univ., Tokyo Metropolitan Univ., Tohoku
More informationThe SOX experiment. Stefano Davini (on behalf of the Borexino-SOX collaboration) Brussels, December 1 st 2017
The SOX experiment Stefano Davini (on behalf of the Borexino-SOX collaboration) Brussels, December 1 st 2017 Beyond the Standard model with Neutrinos Neutrino masses call for physics beyond Standard model
More informationThe LENA Neutrino Observatory
The LENA Neutrino Observatory for the LENA Collaboration 1 Consortium of European science institutions and industry partners Design studies funded by the European Community (FP7) LAGUNA: detector site,
More informationDouglas Michael California Institute of Technology RPIA 2002 KEK, Oct. 29, 2002
Neutrino Oscillations The Fermilab Complex Mini-BooNE/BooNE MINOS NuMI Off-Axis and Beyond Conclusions Douglas Michael California Institute of Technology RPIA 2002 KEK, Oct. 29, 2002 Flavor Eigenstates
More informationT2K and other long baseline experiments (bonus: reactor experiments) Justyna Łagoda
T2K and other long baseline experiments (bonus: reactor experiments) Justyna Łagoda Neutrino mixing and oscillations mixing of flavor and mass eigenstates PMNS matrix parametrized as ( )( cxy = cosθxy
More informationCurrent Results from Reactor Neutrino Experiments
Current Results from Reactor Neutrino Experiments Soo-Bong Kim (KNRC, Seoul National University) Tsukuba Global Science Week (TGSW015), Tsukuba, Sep. 8-30, 015 Neutrino Physics with Reactor 1956 Discovery
More informationν e Neutrino Oscillation Experiments National Nuclear Physics Summer School MIT July 29, 2016 Janet Conrad
ν e Neutrino Oscillation Experiments ν µ National Nuclear Physics Summer School MIT July 29, 2016 Janet Conrad Introduction to this class What do I hope to do with this class? Paint a quick picture of
More informationNew results from RENO and prospects with RENO-50
New results from RENO and prospects with RENO-50 Soo-Bong Kim KNRC, Department of Physics and Astronomy, Seoul National University, Seoul 151-742, South Korea Abstract RENO (Reactor Experiment for Neutrino
More information