Neutrino Physics with SNO+ Freija Descamps for the SNO+ collaboration

Size: px
Start display at page:

Download "Neutrino Physics with SNO+ Freija Descamps for the SNO+ collaboration"

Transcription

1 Neutrino Physics with SNO+ Freija Descamps for the SNO+ collaboration NOW 2014, Otranto, Lecce, Italy September 7-14, 2014

2 Intro Neutrino physics with the SNO+ detector 2

3 Intro What we know:! Neutrinos have mass! Neutrinos oscillate between flavour states! Squared mass differences between mass eigenstates!! Neutrino physics with the SNO+ detector 2

4 Intro What we know:! Neutrinos have mass! Neutrinos oscillate between flavour states! Squared mass differences between mass eigenstates!! Challenges:! What is their mass and what is the mass hierarchy?! Majorana vs. Dirac nature of neutrinos! What are the precise oscillation parameters?! What can ν s tell us about Earth, Sun, Universe? Neutrino physics with the SNO+ detector 2

5 Intro What we know:! Neutrinos have mass! Neutrinos oscillate between flavour states! Squared mass differences between mass eigenstates!! Challenges:! What is their mass and what is the mass hierarchy?! } Majorana vs. Dirac nature of neutrinos! What are the precise oscillation parameters?! What can ν s tell us about Earth, Sun, Universe? Neutrino physics with the SNO+ detector 2

6 SNOLAB and SNO+ SNO+ = successor to Sudbury Neutrino Observatory (SNO)! Located in SNOLAB inside the Creighton mine near Sudbury, Canada! Depth = 2070m (6000m.w.e)! ~70 muons/day in SNO+! Class-2000 clean room Neutrino physics with the SNO+ detector 3

7 SNOLAB and SNO+ Deck with DAQ SNO+ operator ~780T LAB liquid organic scintillator! + PPO acrylic vessel! 12m! 5cm thick SNO+ = successor to Sudbury Neutrino Observatory (SNO)! Located in SNOLAB inside the Creighton mine near Sudbury, Canada! Depth = 2070m (6000m.w.e)! ~70 muons/day in SNO+! Class-2000 clean room ~9500 PMTs! 54% coverage ~7kT ultrapure water shield rock Neutrino physics with the SNO+ detector 3

8 SNOLAB and SNO+ Deck with DAQ SNO+ operator ~780T LAB liquid organic scintillator! + PPO acrylic vessel! 12m! 5cm thick SNO+ = successor to Sudbury Neutrino Observatory (SNO)! Located in SNOLAB inside the Creighton mine near Sudbury, Canada! Depth = 2070m (6000m.w.e)! ~70 muons/day in SNO+! Class-2000 clean room ~9500 PMTs! 54% coverage ~7kT ultrapure water shield rock Neutrino physics with the SNO+ detector 3

9 Liquid scintillator Solvent: Linear AlkylBenzene (LAB)! Long attenuation length (~20m)! Safe: low toxicity and high flash point! Chemically compatible with acrylic! α-β separation through decay-time! 2g/L fluor 2,5 diphenyloxazole (PPO)! High light yield ~10000γ/MeV Petresa plant! Bécancour, QC NIM A640, (2011) Neutrino physics with the SNO+ detector 4

10 LAB purification plan! Multi-stage distillation! Removes heavy metals! Improves UV transparency! Dual-stream PPO distillation! N2/steam stripping! Removes Rn, Kr, Ar, O2! Water extraction! Removes Ra, K, Bi! Metal scavenging! Removes Bi, Pb! Micro-filtration! Removes dust Target levels:! 85 Kr! : g/g! 40 K! : g/g! 39 Ar! : g/g! U! : g/g! Th! : g/g Neutrino physics with the SNO+ detector 5

11 SNO+ physics goals Neutrino physics with the SNO+ detector 6

12 SNO+ physics goals Geo-neutrinos Neutrino physics with the SNO+ detector 6

13 SNO+ physics goals Geo-neutrinos Darlington reactor, Canada Reactor neutrinos Neutrino physics with the SNO+ detector 6

14 SNO+ physics goals Supernova! neutrinos Geo-neutrinos Darlington reactor, Canada Reactor neutrinos Neutrino physics with the SNO+ detector 6

15 SNO+ physics goals Supernova! neutrinos Geo-neutrinos Solar neutrinos Darlington reactor, Canada Reactor neutrinos Neutrino physics with the SNO+ detector 6

16 SNO+ physics goals Supernova! neutrinos neutrino-less double beta decay Geo-neutrinos Solar neutrinos ν e Darlington reactor, Canada Reactor neutrinos Neutrino physics with the SNO+ detector 6

17 SNO+ physics goals Supernova! neutrinos neutrino-less double beta decay Geo-neutrinos Solar neutrinos ν e Darlington reactor, Canada invisible nucleon decay Reactor neutrinos Neutrino physics with the SNO+ detector 6

18 SNO+ phases Neutrino physics with the SNO+ detector 7

19 SNO+ phases Water Nucleon spring fall 2015 Neutrino physics with the SNO+ detector 7

20 SNO+ phases Scintillator Water Solar after 0νββ Nucleon spring fall 2015 Neutrino physics with the SNO+ detector 7

21 SNO+ phases Scintillator Water Solar after 0νββ Nucleon spring fall νββ 2016 Scintillator Te Neutrino physics with the SNO+ detector 7

22 SNO+ phases Scintillator Water Solar after 0νββ Reactor Geo Supernova Background studies Nucleon spring fall νββ 2016 Scintillator Te Neutrino physics with the SNO+ detector 7

23 0νββ with the SNO+ detector Neutrino physics with the SNO+ detector 8

24 0νββ with the SNO+ detector SNO+ approach: (add 0.3% of natural Te! = ~800kg of 130 Te) Trade-off energy resolution for! Higher statistics! Low backgrounds! External shielding! Scintillator self-shielding! LAB purification by distillation! Re-use existing detector! Scalable Neutrino physics with the SNO+ detector 8

25 0νββ with the SNO+ detector Loading Te in LAB SNO+ approach: (add 0.3% of natural Te! = ~800kg of 130 Te) Trade-off energy resolution for! Higher statistics! Low backgrounds! External shielding! Scintillator self-shielding! LAB purification by distillation! Re-use existing detector! Scalable Old loading technique Neutrino physics with the SNO+ detector 8

26 0νββ with the SNO+ detector Loading Te in LAB SNO+ approach: (add 0.3% of natural Te! = ~800kg of 130 Te) Trade-off energy resolution for! Higher statistics! Low backgrounds! External shielding! Scintillator self-shielding! LAB purification by distillation! Re-use existing detector! Scalable Old loading technique Dissolve telluric acid (H6 O 6 Te) in water! Combine with LAB using a surfactant! Good optical properties! Stable > 1 year explicitly demonstrated for 0.3% loading Neutrino physics with the SNO+ detector 8

27 0νββ with the SNO+ detector Loading Te in LAB SNO+ approach: (add 0.3% of natural Te! = ~800kg of 130 Te) Trade-off energy resolution for! Higher statistics! Low backgrounds! External shielding! Scintillator self-shielding! LAB purification by distillation! Re-use existing detector! Scalable Old loading technique Dissolve telluric acid (H6 O 6 Te) in water! Combine with LAB using a surfactant! Good optical properties! Stable > 1 year explicitly demonstrated New loading technique (M. Yeh et al., for 0.3% loading paper in progress) Neutrino physics with the SNO+ detector 8

28 130 Te advantages 34% natural abundance! Load high amount of natural isotope! Relatively inexpensive compared to enriched isotope! 2νββ rate is relatively low (~100 times lower than 150 Nd)! Lower background! Less sensitive to poor energy resolution! Improved optical properties! No inherent optical absorption lines! Higher intrinsic light yield! Nd-LS (0.5%): 8400γ/MeV! Te loaded LS scaled PMT response Nd loaded LS Te-LS (0.5%): 9400γ/MeV Neutrino physics with the SNO+ detector 9

29 Backgrounds Neutrino physics with the SNO+ detector 10

30 Backgrounds Cosmogenic! 60 Co, 131 I, 110m Ag, 124 Sb! 11 C Tellurium cocktail! 238 U, 232 Th, 210 Po! LAB+PPO! 238 U, 232 Th, 14 C! Thermal neutrons! Capture on H: 2.2MeV γ! Neutrino physics with the SNO+ detector 10

31 Backgrounds 8 B Solar neutrinos Tellurium 2νββ! Cosmogenic! 60 Co, 131 I, 110m Ag, 124 Sb! 11 C Tellurium cocktail! 238 U, 232 Th, 210 Po! LAB+PPO! 238 U, 232 Th, 14 C! Thermal neutrons! Capture on H: 2.2MeV γ! Neutrino physics with the SNO+ detector 10

32 Backgrounds 8 B Solar neutrinos Tellurium 2νββ! Cosmogenic! 60 Co, 131 I, 110m Ag, 124 Sb! 11 C Tellurium cocktail! 238 U, 232 Th, 210 Po! LAB+PPO! 238 U, 232 Th, 14 C! Fiducial! volume AV Thermal neutrons! Capture on H: 2.2MeV γ! Acrylic vessel (AV)! Radon daughters in AV ( 210 Pb, 210 Bi, 210 Po) PMTs External! 214 Bi and 208 Tl from AV, PMTs, H2O, ropes! Neutrino physics with the SNO+ detector 10

33 U and Th chains 2.6 MeV gamma from external 208 Tl suppressed by fiducialization! Purification techniques! LS target levels:! ~2.5 x g U /g cocktail! ~3 x g Th /g cocktail! Direct background α and β emissions! Coincidence techniques are under investigation, ex.:! β-α 214 Bi- 214 Po! β-α 212 Bi- 212 Po! α-β 212 Bi- 208 Tl Neutrino physics with the SNO+ detector 11

34 Cosmogenic isotopes Short and long living isotopes can be produced by cosmogenic activation of natural tellurium.! Isotopes (Q> 2 MeV, T1/2 > 20 days)! Rates from ACTIVIA, sea level (n,p)-flux from Armstrong and Gehrels.! For E<200 MeV: TENDL database for cross-sections. V. Lozza, J. Petzoldt, Cosmogenic activation of a natural tellurium target, Astropart. Phys. 61, Neutrino physics with the SNO+ detector 12

35 Cosmogenic isotopes Short and long living isotopes can be produced by cosmogenic activation of natural tellurium.! Isotopes (Q> 2 MeV, T1/2 > 20 days)! Rates from ACTIVIA, sea level (n,p)-flux from Armstrong and Gehrels.! For E<200 MeV: TENDL database for cross-sections. 2 stage - purification:! Above ground: 2 passes! Dissolve Te(OH) 6 in water! Re-crystalize using nitric acid! Rinse with ethanol! Below ground: 2 passes! Dissolve in 80 C water! Cool down to re-crystalize thermally! 50% yield! 3-6 months cool-down >10 4 reduction >10 2 reduction V. Lozza, J. Petzoldt, Cosmogenic activation of a natural tellurium target, Astropart. Phys. 61, Neutrino physics with the SNO+ detector 12

36 Cosmogenic isotopes Short and long living isotopes can be produced by cosmogenic activation of natural tellurium.! Isotopes (Q> 2 MeV, T1/2 > 20 days)! Rates from ACTIVIA, sea level (n,p)-flux from Armstrong and Gehrels.! For E<200 MeV: TENDL database for cross-sections. 2 stage - purification:! Above ground: 2 passes! Dissolve Te(OH) 6 in water! Re-crystalize using nitric acid! Rinse with ethanol! Below ground: 2 passes! Dissolve in 80 C water! Cool down to re-crystalize thermally! 50% yield! 3-6 months cool-down >10 4 reduction >10 2 reduction => Cosmogenic isotopes negligible V. Lozza, J. Petzoldt, Cosmogenic activation of a natural tellurium target, Astropart. Phys. 61, Neutrino physics with the SNO+ detector 12

37 SNO+ 0νββ spectrum 0 (200 mev) 2 2 Internal! U Chain U Chain Internal U chain Optimized ROI: 18.6 events/yr 2 Internal! Th Chain Internal Th chain Th Chain 5 0.3% natural Te loading! Fiducial volume cut at 3.5m (20%)! T (MeV) 212 BiPo, 214 BiPo! Optimized ROI: 18.6 events/yr 8 B ES 8 B ES (, n) U Chain Th Chain External 100% efficient tagging for separate trigger windows! x 50 for in-window! External (, n) External (, n) Cosmogenics Counts/5 y/20 kev bin (200 mev) 2 8 B ES (, n) U Chain Th Chain External T (MeV) Neutrino physics with the SNO+ detector 13

38 0.3% natural Te sensitivity Sensitivity (y) T 1/ % confidence level for! 5 years:!! T 1/2 = 9.84 x yrs!! m ββ = 66.5 mev! 1 year:!! T 1/2 = 4.27 x yrs!! m ββ = mev 90% CL 3 CL NME = 4.03 (IBM-2)! G = 3.69 x y -1! ga = Live time (y) Neutrino physics with the SNO+ detector 14

39 Conclusion SNO+: a large liquid scintillator detector with broad physics program! 0νββ = primary goal! Natural Te will be added to the liquid scintillator! 0.3% loading (~800kg 130 Te)! Possibility of increased loading in future Schedule Water level just below acrylic vessel: now.! Water running: spring 2015.! Scintillator transition: fall 2015.! Introduction of Te: start of Neutrino physics with the SNO+ detector 15

40 Back-up slides

41 Reactor and geo neutrinos ν- e Mantle geoneutrino flux ( 238 U Th) Kamioka Gran Sasso Sudbury Detection through inverse beta decay! Delayed coincidence e + annihilation and n capture! Possible in all SNO+ scintillator phases! Reactor! Geo! 3 nearby reactors dominate flux! Favourable direction and distances! U, Th and K in Earth's crust and mantle! Investigate origin of the heat produced within Earth No oscillation All reactors oscillated No Bruce All over 700km distance Geoneutrinos Eν (MeV) Neutrino physics with the SNO+ detector 17

42 Supernova neutrinos! ν-p elastic scattering events (in LAB)! SNO+ plans to be part of SuperNova Early Warning System (SNEWS) Neutrino flux on Earth! 10kpc SN, 3x10 53 erg! Quenched SN ν-p elastic scattering spectrum True SN ν-p elastic scattering spectrum Neutrino physics with the SNO+ detector 18

43 Solar Neutrinos Assuming initial Borexino-level backgrounds are reached Figure adapted from Nature , 2014 SNO SNO: LETA SNO+ Solar neutrinos probe astrophysics and elementary particle physics models:! Solar metallicity (CNO)! Neutrino oscillations (pep)! SNO+ solar neutrino goal: pep/cno solar neutrino measurement! Low 11 C background thanks to depth (100 times lower than Borexino)! Low energy threshold thanks to LAB Critically dependent on 85 Kr and 14 C background levels Neutrino physics with the SNO+ detector 19

44 Borexino / SNO+ signal/bkg comparison Borexino SNO+

45 Cosmogenics half-life ~ 106d Neutrino physics with the SNO+ detector 21

Neutrinoless double beta decay with SNO+

Neutrinoless double beta decay with SNO+ Neutrinoless double beta decay with SNO+ - 0!"" with SNO+ - Backgrounds - Schedule Freija Descamps for the SNO+ collaboration 1 SNO+ detector 6000 m.w.e Deck with DAQ SNO+ operator ~780T LAB liquid organic

More information

Neutrinoless Double Beta Decay Search with SNO+

Neutrinoless Double Beta Decay Search with SNO+ Neutrinoless Double Beta Decay Search with SNO+ Kalpana Singh for the SNO+ Collaboration University of Alberta 8th Nov. 2016 1 Location 8th Nov. 2016 2 Location, 5890 mwe 8th Nov. 2016 3 63 muons/ day

More information

Scintillator phase of the SNO+ experiment

Scintillator phase of the SNO+ experiment Mathematik und Naturwissenschaften Institut für Kern- und Teilchen Physik Scintillator phase of the experiment Valentina Lozza On behalf of Collaboration TAUP2011, 05.09.2011 Munich Outline = SNO + Liquid

More information

SNO+ ARTFEST, MAY 2014, KINGSTON DR. CHRISTINE KRAUS, LAURENTIAN UNIVERSITY

SNO+ ARTFEST, MAY 2014, KINGSTON DR. CHRISTINE KRAUS, LAURENTIAN UNIVERSITY SNO+ ARTFEST, MAY 2014, KINGSTON DR. CHRISTINE KRAUS, LAURENTIAN UNIVERSITY SNO+ IS LOCATED AT SNOLAB 300 km Canada Ontario Sudbury Creighton mine use existing SNO cavity 2 km or 6000 m.w.e. Artfest 2014,

More information

Solar Neutrinos in Large Liquid Scintillator Detectors

Solar Neutrinos in Large Liquid Scintillator Detectors Solar Neutrinos in Large Liquid Scintillator Detectors M. Chen Queen s University DOANOW March 24, 2007 Low Energy Solar Neutrinos complete our understanding of neutrinos from the Sun pep, CNO, 7 Be, pp

More information

Leaching Studies for the SNO+ Experiment

Leaching Studies for the SNO+ Experiment Leaching Studies for the SNO+ Experiment Pouya Khaghani Laurentian University SNOLAB Users Meeting Symposium September 2 nd 2016 1 SNO+ Physics SNOLAB, Creighton Mine (2070m 6000 m. w. e) Linear Alkyl

More information

Synthesis and Characterization of Organic Tellurium Compounds for SNO+ Liquid Scintillator

Synthesis and Characterization of Organic Tellurium Compounds for SNO+ Liquid Scintillator Synthesis and Characterization of Organic Tellurium Compounds for SNO+ Liquid Scintillator Lianpeng Tian Queen s University For SNO+ Collaboration LSC2017 Conference Large multi-purpose liquid scintillator

More information

Solar Neutrinos: Status and Prospects. Marianne Göger-Neff

Solar Neutrinos: Status and Prospects. Marianne Göger-Neff Solar Neutrinos: Status and Prospects Marianne Göger-Neff NIC 2014, Debrecen TU München Solar Neutrinos Objective of the first solar neutrino experiment: to see into the interior of a star and thus verify

More information

A Large Liquid Scintillator Detector for Neutrino Mass Hierarchy : RENO-50

A Large Liquid Scintillator Detector for Neutrino Mass Hierarchy : RENO-50 A Large Liquid Scintillator Detector for Neutrino Mass Hierarchy : RENO-50 International Meeting for Large Neutrino Infrastructures Ecole Architecture Paris Val de Seine, APPEC, 23-24 June, 2014 Soo-Bong

More information

Rivelazione di neutrini solari - Borexino Lino Miramonti 6 Giugno 2006 Gran Sasso

Rivelazione di neutrini solari - Borexino Lino Miramonti 6 Giugno 2006 Gran Sasso Rivelazione di neutrini solari - Borexino Lino Miramonti 6 Giugno 2006 Gran Sasso 1 RADIOCHEMICAL Integrated in energy and time CHERENKOV Less than 0.01% of the solar neutrino flux is been measured in

More information

Results on geoneutrinos at Borexino experiment. Heavy Quarks and Leptons Yamagata Davide Basilico

Results on geoneutrinos at Borexino experiment. Heavy Quarks and Leptons Yamagata Davide Basilico Results on geoneutrinos at Borexino experiment Heavy Quarks and Leptons 2018 - Yamagata Davide Basilico Outline 1. Geoneutrinos 2. Borexino 3. Analysis and results 2 What are geoneutrinos? Distribution

More information

LOW ENERGY SOLAR NEUTRINOS WITH BOREXINO. Lea Di Noto on behalf of the Borexino collaboration

LOW ENERGY SOLAR NEUTRINOS WITH BOREXINO. Lea Di Noto on behalf of the Borexino collaboration LOW ENERGY SOLAR NEUTRINOS WITH BOREXINO Lea Di Noto on behalf of the Borexino collaboration Vulcano Workshop 20 th -26 th May 2018 [cm -2 s -1 MeV -1 ] SOLAR NEUTRINOS Electrons neutrinos are produced

More information

Review of Solar Neutrinos. Alan Poon Institute for Nuclear and Particle Astrophysics & Nuclear Science Division Lawrence Berkeley National Laboratory

Review of Solar Neutrinos. Alan Poon Institute for Nuclear and Particle Astrophysics & Nuclear Science Division Lawrence Berkeley National Laboratory Review of Solar Neutrinos Alan Poon Institute for Nuclear and Particle Astrophysics & Nuclear Science Division Lawrence Berkeley National Laboratory Solar Neutrinos pp chain: 4p + 2e 4 He + 2ν e + 26.7

More information

Muons in Borexino. SFB Block Meeting. Daniel Bick Universität Hamburg. D. Bick (Uni HH) Muons in Borexino

Muons in Borexino. SFB Block Meeting. Daniel Bick Universität Hamburg. D. Bick (Uni HH) Muons in Borexino Muons in Borexino SFB Block Meeting Daniel Bick Universität Hamburg 24.03.2010 D. Bick (Uni HH) Muons in Borexino 24.03.2010 1 / 30 Overview 1 Motivation Physics at Borexino Neutrino Detection in Liquid

More information

0νββ Physics in WbLS. Andy Mastbaum University of Pennsylvania. WbLS Workshop LBNL 17 May 2014

0νββ Physics in WbLS. Andy Mastbaum University of Pennsylvania. WbLS Workshop LBNL 17 May 2014 0νββ Physics in WbLS Andy Mastbaum University of Pennsylvania WbLS Workshop LBNL 17 May 2014 Requirements Future detectors must: Reach a sensitivity of 15 mev at the 3σ CL after years of running, according

More information

can be read by PMTs w/o wave length shifter

can be read by PMTs w/o wave length shifter Liquid-Xe Solar pp 7 Be neutrino detector Y.Suzuki Kamioka Obs. ICRR, U.Tokyo @LowNu 2000-06-15 Detector 1) Liquid Xenon with 10 ton fiducial volume 2) Scintillation detector: 42,000 photons/mev similar

More information

USING NEUTRINOS TO STUDY THE EARTH. Nikolai Tolich University of Washington

USING NEUTRINOS TO STUDY THE EARTH. Nikolai Tolich University of Washington USING NEUTRINOS TO STUDY THE EARTH Nikolai Tolich University of Washington Outline Introduction Recent results The future Structure of the Earth Seismic data splits Earth into 5 basic regions: inner core,

More information

CANDLES Experiment Current Status and Future Plan. X. Li for the CANDLES Collaboration

CANDLES Experiment Current Status and Future Plan. X. Li for the CANDLES Collaboration CANDLES Experiment Current Status and Future Plan X. Li for the CANDLES Collaboration 1 Neutrinoless Double Beta Decay (0νββ) 2νββ decay 0νββ decay (A, Z) => (A, Z+2) + 2e - process beyond Standard Model

More information

Proton decay and neutrino astrophysics with the future LENA detector

Proton decay and neutrino astrophysics with the future LENA detector Proton decay and neutrino astrophysics with the future LENA detector Teresa Marrodán Undagoitia tmarroda@ph.tum.de Institut E15 Physik-Department Technische Universität München Paris, 11.09.08 Outline

More information

Scintillator Detectors for Neutrino Physics

Scintillator Detectors for Neutrino Physics Scintillator Detectors for Neutrino Physics Minfang Yeh Neutrino and Nuclear Chemistry, BNL Jinping Workshop, Tsinghua, June 5, 2015 BNL-Liquid Scintillator Development Facility A unique facility (since

More information

Aldo Ianni, LNGS for the Borexinocollaboration Sept. 29th, 2011

Aldo Ianni, LNGS for the Borexinocollaboration Sept. 29th, 2011 Aldo Ianni, LNGS for the Borexinocollaboration Sept. 29th, 2011 First Borexino proposal: 1991 Main goal: real time measurement of sub-mev solar neutrinos Why? To solve the Solar Neutrino Puzzle (missingsolarneutrinos)

More information

LENA. Investigation of Optical Scintillation Properties and the Detection of Supernovae Relic Neutrinos. M. Wurm. January 18, 2006 LENA. M.

LENA. Investigation of Optical Scintillation Properties and the Detection of Supernovae Relic Neutrinos. M. Wurm. January 18, 2006 LENA. M. Spectrum Investigation of Scintillation and the Detection of Supernovae Relic Neutrinos January 18, 2006 Outline Spectrum 1 2 3 Spectrum 4 The Spectrum Spectrum about 50 kt of liquid scintillator, so:

More information

Low Background Experiments and Material Assay. Tessa Johnson NSSC Summer School July 2016

Low Background Experiments and Material Assay. Tessa Johnson NSSC Summer School July 2016 Low Background Experiments and Material Assay Tessa Johnson NSSC Summer School July 2016 Outline How do we detect particles? Some interesting questions relating to particle physics How can particle detection

More information

Neutrino Oscillations

Neutrino Oscillations Neutrino Oscillations Supervisor: Kai Schweda 5/18/2009 Johannes Stiller 1 Outline The Standard (Solar) Model Detecting Neutrinos The Solar Neutrino Problem Neutrino Oscillations Neutrino Interactions

More information

Andrey Formozov The University of Milan INFN Milan

Andrey 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 information

1. Neutrino Oscillations

1. Neutrino Oscillations Neutrino oscillations and masses 1. Neutrino oscillations 2. Atmospheric neutrinos 3. Solar neutrinos, MSW effect 4. Reactor neutrinos 5. Accelerator neutrinos 6. Neutrino masses, double beta decay 1.

More information

Neutrino Masses and Mixing

Neutrino 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 information

arxiv: v1 [physics.ins-det] 3 Feb 2011

arxiv: v1 [physics.ins-det] 3 Feb 2011 Nuclear Instruments and Methods in Physics Research A 00 (2018) 1 5 Alogo.pdf Nuclear Instruments and Methods in Physics Research A Scintillation decay time and pulse shape discrimination in oxygenated

More information

Search for Dark Matter with Liquid Argon and Pulse Shape Discrimination

Search for Dark Matter with Liquid Argon and Pulse Shape Discrimination Search for Dark Matter with Liquid Argon and Pulse Shape Discrimination Results from DEAP-1 and Status of DEAP-3600 Pierre Gorel for the DEAP collaboration University of Alberta Dark matter Experiment

More information

GERDA experiment A search for neutrinoless double beta decay. Roberto Santorelli (Physik-Institut der Universität Zürich)

GERDA experiment A search for neutrinoless double beta decay. Roberto Santorelli (Physik-Institut der Universität Zürich) GERDA experiment A search for neutrinoless double beta decay Roberto Santorelli (Physik-Institut der Universität Zürich) on behalf of the GERDA collaboration ÖPG/SPS/ÖGAA meeting 04/09/09 Neutrinos mixing

More information

Borexino and status of the project Aldo Ianni INFN, Gran Sasso Laboratory on behalf of the Borexino collaboration

Borexino and status of the project Aldo Ianni INFN, Gran Sasso Laboratory on behalf of the Borexino collaboration Borexino and status of the project Aldo Ianni INFN, Gran Sasso Laboratory on behalf of the Borexino collaboration Moscow, 15/10/2005 Aldo Ianni, INFN LNGS 1 Outline Borexino: Italian-Russian cooperation

More information

The LENA Neutrino Observatory

The 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 information

Results from Borexino 26th Rencontres de Blois

Results from Borexino 26th Rencontres de Blois Results from Borexino 26th Rencontres de Blois - 2014 Marco G. Giammarchi Istituto Nazionale di Fisica Nucleare Via Celoria 16 20133 Milano (Italy) marco.giammarchi@mi.infn.it http://pcgiammarchi.mi.infn.it/giammarchi/

More information

Solar Neutrino Oscillations

Solar Neutrino Oscillations Solar Neutrino Oscillations ( m 2, θ 12 ) Background (aka where we were): Radiochemical experiments Kamiokande and Super-K Where we are: Recent results SNO and KamLAND Global picture Where we are going:

More information

THE CRYOGENIC UNDERGROUND OBSERVATORY FOR RARE EVENTS: STATUS AND PROSPECTS

THE CRYOGENIC UNDERGROUND OBSERVATORY FOR RARE EVENTS: STATUS AND PROSPECTS THE CRYOGENIC UNDERGROUND OBSERVATORY FOR RARE EVENTS: STATUS AND PROSPECTS Eric B. Norman Dept. of Nuclear Engineering Univ. of California, Berkeley, CA U. S. A. Recent results in n physics Neutrinos

More information

Background Characterization and Rejection in the LZ Detector. David Malling Brown University IDM 2012 July 25, 2012

Background Characterization and Rejection in the LZ Detector. David Malling Brown University IDM 2012 July 25, 2012 Background Characterization and Rejection in the LZ Detector David Malling Brown University IDM 2012 July 25, 2012 LZ Construction 2 Background Sources Ti cryostats 1500 kg

More information

Low Energy 8 B Solar Neutrinos in SNO+: Controlling and Constraining Radon Backgrounds

Low Energy 8 B Solar Neutrinos in SNO+: Controlling and Constraining Radon Backgrounds Low Energy 8 B Solar Neutrinos in SNO+: Controlling and Constraining Radon Backgrounds by Maryam Seddighin A thesis submitted to the Department of Physics, Engineering Physics and Astronomy in conformity

More information

GERDA: The GERmanium Detector Array for the search for neutrinoless decays of 76 Ge. Allen Caldwell Max-Planck-Institut für Physik

GERDA: The GERmanium Detector Array for the search for neutrinoless decays of 76 Ge. Allen Caldwell Max-Planck-Institut für Physik GERDA: The GERmanium Detector Array for the search for neutrinoless decays of 76 Ge Allen Caldwell Max-Planck-Institut für Physik What we know Mass Scale NORMAL INVERTED m 12 2 known m 13 2 known Mixing

More information

Particle Physics: Neutrinos part I

Particle 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 information

Neutrinos from the Sun and other sources: Results from the Borexino experiment

Neutrinos from the Sun and other sources: Results from the Borexino experiment Neutrinos from the Sun and other sources: Results from the Borexino experiment Marianne Göger-Neff 23.05.2014 Neutrinos from the Sun and other sources: Results from the Borexino experiment Motivation:

More information

Water-based Liquid Scintillator

Water-based Liquid Scintillator Water-based Liquid Scintillator Minfang Yeh Neutrino and Nuclear Chemistry, Brookhaven National Laboratory NNN-2014, Nov. 4-6, 2014 Liquid Scintillator Physics 0 ββ (e.g. SNO+, KamLAND-Zen) Reactor (e.g.

More information

Design, Construction, Operation, and Simulation of a Radioactivity Assay Chamber

Design, Construction, Operation, and Simulation of a Radioactivity Assay Chamber Design, Construction, Operation, and Simulation of a Radioactivity Assay Chamber Wesley Ketchum and Abe Reddy EWI Group, UW REU 2006 Outline Neutrino Physics Background Double Beta Decay and the Majorana

More information

Neutrinos. Why measure them? Why are they difficult to observe?

Neutrinos. 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 information

KamLAND. Introduction Data Analysis First Results Implications Future

KamLAND. 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 information

Dark matter search with the SABRE experiment

Dark matter search with the SABRE experiment Dark matter search with the SABRE experiment Giulia D Imperio* for the SABRE collaboration *INFN Roma 1 25-07-2017 TAUP 2017 Sudbury, Canada 1 Dark matter detection through annual modulation WIMP is one

More information

1. Introduction on Astroparticle Physics Research options

1. Introduction on Astroparticle Physics Research options Research options Large variety of topics in astro physics and particle physics Cosmic rays (sources, production and acceleration mechanisms) Stability of matter or proton decay (GUTs) Solar neutrinos (the

More information

Water Purification in Borexino

Water Purification in Borexino Water Purification in Borexino Marco G. Giammarchi Istituto Nazionale di Fisica Nucleare - Via Celoria 16 20133 Milano (Italy) marco.giammarchi@mi.infn.it http://pcgiammarchi.mi.infn.it/giammarchi/ On

More information

Recent Discoveries in Neutrino Physics

Recent 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 information

FIRST RESULT FROM KamLAND-Zen Double Beta Decay with 136 Xe

FIRST RESULT FROM KamLAND-Zen Double Beta Decay with 136 Xe FIRST RESULT FROM KamLAND-Zen Double Beta Decay with Xe A. GANDO for the KamLAND-Zen Collaboration Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan We present the first result

More information

Status of Cuore experiment and last results from Cuoricino

Status of Cuore experiment and last results from Cuoricino Status of Cuore experiment and last results from Cuoricino on behalf of the Cuore collaboration Istituto Nazionale di Fisica Nucleare, Genova E-mail: elena.guardincerri@ge.infn.it CUORE is a cryogenic-bolometer

More information

Status and Perspectives of the COBRA-Experiment

Status and Perspectives of the COBRA-Experiment Status and Perspectives of the COBRA-Experiment Jan Tebrügge for the COBRA Collaboration Status and Perspectives of the COBRA-Experiment Jan Tebrügge beta decays for thedouble COBRA Collaboration CdZnTe

More information

Questions. 1. What kind of radiation dominates the first phase of radiation emission from a nuclear fireball?

Questions. 1. What kind of radiation dominates the first phase of radiation emission from a nuclear fireball? Questions 1. What kind of radiation dominates the first phase of radiation emission from a nuclear fireball? 2. What is the ignition temperature of wood? 3. What fuels a firestorm? Natural Radioactivity

More information

Neutrino Experiments: Lecture 2 M. Shaevitz Columbia University

Neutrino 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 information

Distillation purification and radon assay of liquid xenon

Distillation purification and radon assay of liquid xenon Distillation purification and radon assay of liquid xenon Yasuo Takeuchi Kamioka Observatory, ICRR, Univ. of Tokyo, Kamioka-cho, Hida-shi, Gifu 56-125, Japan Abstract. We succeeded to reduce the Kr contamination

More information

Two Neutrino Double Beta (2νββ) Decays into Excited States

Two Neutrino Double Beta (2νββ) Decays into Excited States Two Neutrino Double Beta (2νββ) Decays into Excited States International School of Subnuclear Physics 54 th Course: The new physics frontiers in the LHC-2 era Erice, 17/06/2016 Björn Lehnert TU-Dresden,

More information

POTASSIUM GEONEUTRINOS AND THEIR DETECTION

POTASSIUM GEONEUTRINOS AND THEIR DETECTION Proceedings of the South Dakota Academy of Science, Vol. 9 (211) 13 POTASSIUM GEONEUTRINOS AND THEIR DETECTION Barbara Szczerbinska 1 *, Alyssa Day 2, and Dongming Mei 2 1 Dakota State University Madison,

More information

Low Energy Neutrino Astronomy and Results from BOREXINO

Low Energy Neutrino Astronomy and Results from BOREXINO Low Energy Neutrino Astronomy and Results from BOREXINO DESY Hamburg / DESY Zeuthen March 25 th and 26th Lothar Oberauer, Physikdepartment E15, TU München Charge 0-1 +2/3-1/3 Neutrinos as probes? Neutrinos

More information

The GERmanium Detector Array

The GERmanium Detector Array The GERmanium Detector Array n n ν=v p e - e - p Outline: Exp. issues of 0νββ-decay of 76 Ge Concept of GERDA Status of the experiment Summary and conclusions Kevin Kröninger (Max-Planck-Institut für Physik,

More information

THE BEGINNING OF THE END OF AN ERA: Analysis After the Shutdown of the Sudbury Neutrino Observatory

THE BEGINNING OF THE END OF AN ERA: Analysis After the Shutdown of the Sudbury Neutrino Observatory THE BEGINNING OF THE END OF AN ERA: Analysis After the Shutdown of the Sudbury Neutrino Observatory Introduction Highlights of SNO Results NCD Phase Update Future Analysis Plan Keith Rielage on behalf

More information

Liquid Scintillator Timing Property

Liquid Scintillator Timing Property Liquid Scintillator Timing Property Minfang Yeh Neutrino and Nuclear Chemistry, BNL MIT workshop, Dec 15, 2015 Main Neutrino Interactions in Scintillator + p ; KamLAND v e + 12 C e 12 B 12 C e v e v +

More information

LOW RADON PERMEABLE GLOVES AND LASERBALL SIMULATIONS FOR SNO+ Zachariah Carranza-Barnard

LOW RADON PERMEABLE GLOVES AND LASERBALL SIMULATIONS FOR SNO+ Zachariah Carranza-Barnard LOW RADON PERMEABLE GLOVES AND LASERBALL SIMULATIONS FOR SNO+ by Zachariah Carranza-Barnard Thesis submitted in partial fulfillment of the requirements for the degree of Master of Science (MSc) in Physics

More information

The 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 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 information

Studies of the XENON100 Electromagnetic Background

Studies of the XENON100 Electromagnetic Background Studies of the XENON100 Electromagnetic Background Daniel Mayani Physik-Institut University of Zurich PhD Seminar PSI, August 26-27, 2015 Searching for elusive particles The main challenge for experiments

More information

XMASS: a large single-phase liquid-xenon detector

XMASS: a large single-phase liquid-xenon detector XMASS: a large single-phase liquid-xenon detector Katsuki Hiraide, the university of Tokyo for the XMASS Collaboration October 3 rd, 2016 IPRD16@Siena, Italy 1 XMASS project XMASS: a multi purpose experiment

More information

Radio-chemical method

Radio-chemical method Neutrino Detectors Radio-chemical method Neutrino reactions: n+ν e => p+e - p+ν e => n+e + Radio chemical reaction in nuclei: A N Z+ν e => A-1 N(Z+1)+e - (Electron anti-neutrino, right) (Z+1) will be extracted,

More information

UCLA Dark Matter 2014 Symposium. Origins and Distributions of the Backgrounds. 15 min

UCLA Dark Matter 2014 Symposium. Origins and Distributions of the Backgrounds. 15 min S. Fiorucci Brown University UCLA Dark Matter 2014 Symposium Origins and Distributions of the Backgrounds 15 min What is a signal for LUX? Nuclear recoil Single scatter Signal Low energy, typically < 25

More information

Neutrino Geophysics at Baksan I: Possible Detection of Georeactor Antineutrinos

Neutrino Geophysics at Baksan I: Possible Detection of Georeactor Antineutrinos arxiv:hep-ph/0401221 v1 28 Jan 2004 Neutrino Geophysics at Baksan I: Possible Detection of Georeactor Antineutrinos G. Domogatski 1, V. Kopeikin 2, L. Mikaelyan 2, V. Sinev 2 1 Institute for Nuclear Research

More information

Neutrino June 29 th Neutrino Probes of Extragalactic Supernovae. Shin ichiro Ando University of Tokyo

Neutrino June 29 th Neutrino Probes of Extragalactic Supernovae. Shin ichiro Ando University of Tokyo Neutrino Workshop@ICRR June 29 th 2005 Neutrino Probes of Extragalactic Supernovae Shin ichiro Ando University of Tokyo 1. Introduction Core-Collapse Supernova and Neutrino Burst Gravitational binding

More information

Results from Borexino on solar (and geo-neutrinos) Gemma Testera

Results from Borexino on solar (and geo-neutrinos) Gemma Testera Results from Borexino on solar (and geo-neutrinos) Gemma Testera Istituto Nazionale di Fisica Nucleare (Genova) On behalf of the Borexino collaboration Scintillator: 270 t PC+PPO (1.5 g/l) in a 150 mm

More information

Search for Sterile Neutrinos with the Borexino Detector

Search for Sterile Neutrinos with the Borexino Detector Search for Sterile Neutrinos with the Borexino Detector PANIC 2014 Hamburg on behalf of the BOREXINO Collaboration Institut für Experimentalphysik (Universität Hamburg) Borexino Detector Site 1400 m of

More information

arxiv:hep-ex/ v1 15 Aug 2006

arxiv: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 information

DUSEL Initial Suite of Experiments (ISE) 1

DUSEL Initial Suite of Experiments (ISE) 1 Dark Matter (WIMPS) Sensitivity 10^-44-10^-45 Noble Liquid (2 phase) 100 250 4100 LUX 300 proposal for Sanford Lab (2008) (Xe) CDMS Experiment in Soudan (running) Low Temperature Solid State 100 250 2000

More information

Rn assay and distillation purification

Rn assay and distillation purification Rn assay and distillation purification of Lq. Xe for Kr Introduction Distillation purification of Xe for Kr Kr assay with API-MS detector Rn assay with XMASS prototype detector Summary Yasuo Takeuchi (Kamioka

More information

Neutrino 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. 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 information

Search for double electron capture on 124 Xe with the XMASS-I detector

Search for double electron capture on 124 Xe with the XMASS-I detector Search for double electron capture on 124 Xe with the XMASS-I detector KATSUKI HIRAIDE (ICRR, THE UNIVERSITY OF TOKYO) SEPTEMBER 7 TH, 2015 TAUP2015 1 124 Xe 2n double electron capture Natural xenon contains

More information

The DarkSide-50 Outer Detectors

The DarkSide-50 Outer Detectors The DarkSide-50 Outer Detectors Shawn Westerdale Princeton University (for the DarkSide Collaboration) TAUP 2015 Torino Thursday, Sept 10, 2015 The DarkSide-50 Experiment Located in Hall C of Laboratori

More information

Present and future of SNO: SNO, SNO+ and SNOLAB. Aksel Hallin,Queen s University for the SNO Collaboration NDM, Paris, September 2006

Present and future of SNO: SNO, SNO+ and SNOLAB. Aksel Hallin,Queen s University for the SNO Collaboration NDM, Paris, September 2006 Present and future of SNO: SNO, SNO+ and SNOLAB Aksel Hallin,Queen s University for the SNO Collaboration NDM, Paris, September 2006 Sudbury Neutrino Observatory 1000 tonnes D 2 O Support Structure for

More information

The dawn of neutrino geophysics. G.Gratta Physics Department Stanford University

The dawn of neutrino geophysics. G.Gratta Physics Department Stanford University The dawn of neutrino geophysics G.Gratta Physics Department Stanford University Structure 35km of the Earth 6km 6400km 2900km 2255km 1245km From seismic data 5 basic regions: - inner core, - outer core,

More information

Neutrinoless Double Beta Decay for Particle Physicists

Neutrinoless Double Beta Decay for Particle Physicists Neutrinoless Double Beta Decay for Particle Physicists GK PhD Presentation Björn Lehnert Institut für Kern- und Teilchenphysik Berlin, 04/10/2011 About this talk Double beta decay: Particle physics implications

More information

Geo-neutrinos Status and Prospects

Geo-neutrinos Status and Prospects Geo-neutrinos Status and Prospects SNOLAB Grand Opening Workshop May 2012 e+ νe W u pu Steve Dye Hawaii Pacific University d d u d n Outline Radiogenic heat/thermal evolution Radiogenic heat/geo-neutrinos

More information

Potential of the large liquid-scintillator detector LENA in particle and astrophysics

Potential of the large liquid-scintillator detector LENA in particle and astrophysics Potential of the large liquid-scintillator detector LENA in particle and astrophysics Teresa Marrodán Undagoitia tmarroda@ph.tum.de Institut E15 Physik-Department Technical University of Munich DPG Teilchenphysik

More information

BOREXINO: A MULTI-PURPOSE DETECTOR FOR THE STUDY OF SOLAR AND TERRESTRIAL NEUTRINOS

BOREXINO: A MULTI-PURPOSE DETECTOR FOR THE STUDY OF SOLAR AND TERRESTRIAL NEUTRINOS BOREXINO: A MULTI-PURPOSE DETECTOR FOR THE STUDY OF SOLAR AND TERRESTRIAL NEUTRINOS Alex Wright Princeton University University of Chicago HEP Seminar May 10 th, 2010 Solar Neutrino Production p-p Solar

More information

Neutrino detectors. V. Lozza,

Neutrino detectors. V. Lozza, Neutrino detectors, 5.10.2011 Outline - Introduction to neutrinos Sources of neutrinos Detection techniques Why we need to go underground? Background components What to do? Summary A brief of history 1914:

More information

Workshop Towards Neutrino Technologies July Prospects and status of LENA

Workshop Towards Neutrino Technologies July Prospects and status of LENA 2047-10 Workshop Towards Neutrino Technologies 13-17 July 2009 Prospects and status of LENA Lothar OBERAUER Technical University of Munich Department of Physics James-Franck-Strasse, 1 D-85747 Garching,

More information

arxiv: v1 [physics.ins-det] 1 Feb 2016

arxiv: v1 [physics.ins-det] 1 Feb 2016 arxiv:1602.00364v1 [physics.ins-det] 1 Feb 2016 Solar neutrino interactions with liquid scintillators used for double beta-decay experiments 1. Introduction Hiroyasu Ejiri 1 and Kai Zuber 2 1. Research

More information

KamLAND. Studying Neutrinos from Reactor

KamLAND. 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 information

Status of the Gadolinium project for. Super-Kamiokande. Lluís Martí Magro. Conca Specchiulla, Italy. 5 th of September, 2010.

Status of the Gadolinium project for. Super-Kamiokande. Lluís Martí Magro. Conca Specchiulla, Italy. 5 th of September, 2010. Status of the Gadolinium project for Super-Kamiokande Lluís Martí Magro. Conca Specchiulla, Italy. 5 th of September, 2010. Super-Kamiokande in the past The Super-Kamiokande collaboration had many successes

More information

SNO+ and Geoneutrino Physics

SNO+ and Geoneutrino Physics SNO+ and Geoneutrino Physics by Chunlin Lan A thesis submitted to the Department of Physics, Engineering Physics and Astronomy in conformity with the requirements for the degree of Master of Science Queen

More information

Recent results from Borexino Gemma Testera INFN Genova TAUP 2015 September 7th, 2015

Recent results from Borexino Gemma Testera INFN Genova TAUP 2015 September 7th, 2015 Recent results from Borexino Gemma Testera INFN Genova TAUP 2015 September 7th, 2015 Signals in Borexino Solar n Anti-n from the Earth (see A. Ianni talk) Anti-n (or n) from a radioactive source (SOX,

More information

Neutron background and possibility for shallow experiments

Neutron background and possibility for shallow experiments Neutron background and possibility for shallow experiments Tadao Mitsui Research Center for Neutrino Science, Tohoku University 14-16 December, 2005 Neutrino Sciences 2005, Neutrino Geophysics, Honolulu,

More information

Status of Solar Neutrino Oscillations

Status of Solar Neutrino Oscillations Status of Solar Neutrino Oscillations With many thanks to Dave Wark - RAL/ University of Sussex and Stephen Brice - Fermilab The Solar Neutrino Problem Next three plots adapted from http://www.sns.ias.edu/~jnb/

More information

Gadolinium Doped Water Cherenkov Detectors

Gadolinium 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 information

CANDLES Search for Neutrino-less Double Beta Decay of 48 Ca

CANDLES Search for Neutrino-less Double Beta Decay of 48 Ca CANDLES Search for Neutrino-less Double Beta Decay of 48 Ca S. Umehara 1, T. Kishimoto 1,2, M. Nomachi 1, S. Ajimura 1, T. Iida 1, K. Nakajima 1, K. Ichimura 1, K. Matsuoka 1, T. Ishikawa 1, D. Tanaka

More information

Underground Physics in the Pyhäsalmi mine

Underground Physics in the Pyhäsalmi mine Timo Enqvist University of Oulu, Finland Moscow, June 10, 2016 1/40 Content The Pyhäsalmi mine and Callio Lab Cosmic-ray experiment EMMA 14 C concentration in liquid scintillators Measurement of 2ν2β half-lives

More information

Searching for neutrino- less double beta decay with EXO- 200 and nexo

Searching for neutrino- less double beta decay with EXO- 200 and nexo Searching for neutrino- less double beta decay with EXO- 200 and nexo Andrea Pocar University of Massachusetts, Amherst on behalf of the EXO-200 and nexo collaborations The EXO- 200 Collaboration 2 The

More information

The Double Chooz Project

The 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 information

The NEMO experiment. Present and Future. Ruben Saakyan UCL 28 January 2004 IOP meeting on double beta decay Sussex

The NEMO experiment. Present and Future. Ruben Saakyan UCL 28 January 2004 IOP meeting on double beta decay Sussex The NEMO experiment. Present and Future. Ruben Saakyan UCL 28 January 2004 IOP meeting on double beta decay Sussex Neutrino Ettore Majorana Observatory 50 physicists and engineers 13 Laboratories/Universities

More information

GADZOOKS! project at Super-Kamiokande

GADZOOKS! project at Super-Kamiokande GADZOOKS! project at Super-Kamiokande M.Ikeda (Kamioka ICRR, U.of Tokyo) for Super-K collaboration 2015,6,9@WIN2015 Contents GADZOOKS! project Supernova Relic Neutrino search R&D status and Plan Summary

More information

Modane underground laboratory (Fréjus)

Modane underground laboratory (Fréjus) Modane underground laboratory (Fréjus) Present and Future IDM 2006, Rhodes F. Piquemal (CENBG, CNRS-IN2P3, U. Bordeaux I) Presented by G. Gerbier (CEA-Dapnia Saclay) Modane Underground Laboratory (Fréjus)

More information

Solar spectrum. Nuclear burning in the sun produce Heat, Luminosity and Neutrinos. pp neutrinos < 0.4 MeV

Solar spectrum. Nuclear burning in the sun produce Heat, Luminosity and Neutrinos. pp neutrinos < 0.4 MeV SOLAR NEUTRINOS Solar spectrum Nuclear burning in the sun produce Heat, Luminosity and Neutrinos pp neutrinos < 0.4 MeV Beryllium neutrinos 0.86 MeV Monochromatic since 2 body decay 2 kev width due to

More information