Low Energy Neutrinos Neutrino Luminosity of the Sun & LENS Neutrino Oscillation Workshop Conca Specchiulla, September 11, 2006 Christian Grieb Virginia.

Slides:



Advertisements
Similar presentations
Standard Solar Model Calculation of Neutrino Fluxes Aldo Serenelli Institute for Advanced Study NOW 2006 Conca Specchiulla 11-Sept-2006.
Advertisements

Status of XMASS experiment Shigetaka Moriyama Institute for Cosmic Ray Research, University of Tokyo For the XMASS collaboration September 10 th, 2013.
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%
Stockholm, May 2-6, 2006 SNOW Sub-MeV solar neutrinos: experimental techniques and backgrounds Aldo Ianni Gran Sasso Laboratory, INFN.
Prospects for 7 Be Solar Neutrino Detection with KamLAND Stanford University Department of Physics Kazumi Ishii.
A Search for Point Sources of High Energy Neutrinos with AMANDA-B10 Scott Young, for the AMANDA collaboration UC-Irvine PhD Thesis:
Experimental Status of Geo-reactor Search with KamLAND Detector
CHARM 2007, Cornell University, Aug. 5-8, 20071Steven Blusk, Syracuse University D Leptonic Decays near Production Threshold Steven Blusk Syracuse University.
October 3, 2003IFIC, UVEG-CSIC A road map to solar fluxes, osc. param., and test for new physics Carlos Pena Garay IAS ~
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%
Special Issues on Neutrino Telescopy Apostolos G. Tsirigotis Hellenic Open University School of Science & Technology Particle and Astroparticle Physics.
The Importance of Low-Energy Solar Neutrino Experiments Thomas Bowles Los Alamos National Laboratory Markov Symposium Institute for Nuclear Research 5/13/05.
LENA Low Energy Neutrino Astrophysics L. Oberauer, Technische Universität München LENA Delta EL SUD Meeting.
李玉峰 中科院高能所 JUNO中微子天文和天体物理学研讨会
Solar Neutrinos Perspectives and Objectives Mark Chen Queen’s University and Canadian Institute for Advanced Research (CIFAR)
1 LENA Low Energy Neutrino Astronomy NOW 2010, September 6, 2010 Lothar Oberauer, TUM, Physik-Department.
Measuring the Low Energy Solar Neutrino Spectrum LENS-Sol SNOLAB Workshop, Sudbury, Aug 15, 2005 R. S. Raghavan Virginia Tech.
LENS-CAL I. Barabanov, V. Gurentsov, V. Kornoukhov Institute for Nuclear Research, Moscow and R. S. Raghavan, Virginia Tech LONU-LENS Blacksburg, Oct 15,
Blacksburg - October 14, 2006 LENS - The Lattice Architecture Jeff Blackmon (ORNL) on behalf of LENS Collaboration 8% Indium-loaded liquid scintillator.
LAGUNA Large Apparatus for Grand Unification and Neutrino Astrophysics Launch meeting, Heidelberg, March 2007, Lothar Oberauer, TUM.
Methods and problems in low energy neutrino experiments (solar, reactors, geo-) I G. Ranucci ISAPP 2011 International School on Astroparticle physics THE.
KamLAND : Studying Neutrinos from Reactor Atsuto Suzuki KamLAND Collaboration KEK : High Energy Accelerator Research Organization.
9-June-2003NDM2003 M. Nomachi M. Nomachi OSAKA University and MOON collaboration MOON (Mo Observatory Of Neutrinos) for double beta decay Photo by
SNS2 Workshop August 28-29, 2003 Richard Talaga, Argonne1 Calibration of the OMNIS-LPC Supernova Neutrino Detector Outline –OMNIS Experiment and Detectors.
Yasuhiro Kishimoto for KamLAND collaboration RCNS, Tohoku Univ. September 12, 2007 TAUP 2007 in Sendai.
Present and future detectors for Geo-neutrinos: Borexino and LENA Applied Antineutrino Physics Workshop APC, Paris, Dec L. Oberauer, TU München.
LSc development for Solar und Supernova Neutrino detection 17 th Lomonosov conference, Moscow, August 2015 L. Oberauer, TUM.
The Standard Solar Model and Experiments Predictions versus experiments Uncertainties in predictions Challenges and open questions BP00: astro-ph/
NESTOR SIMULATION TOOLS AND METHODS Antonis Leisos Hellenic Open University Vlvnt Workhop.
Future solar neutrino projects Value for neutrino oscillations Value for astrophysics Current status of future solar neutrino projects Conclusions Neutrino.
LENS: Measuring the Neutrino Luminosity of the Sun R. S. Raghavan Virginia Tech Henderson Capstone DUSEL Workshop Stony Brook University May 5, 2006.
Kopylov A.V. Erice School/Workshop 2009 on Neutrinos in Cosmology, in Astro, in Particle and in Nuclear Physics in Erice/Trapani/Sicily/Italy on September.
1 IDM2004 Edinburgh, 9 september 2004 Helenia Menghetti Bologna University and INFN Study of the muon-induced neutron background with the LVD detector.
Neutron detector developments at LPC Caen  -delayed neutron detectors  current limitations  future issues Search for new solid scintillators (Neutromania)
TUNL R. B. Vogelaar March 1, 2007 Measuring the complete Solar neutrino spectrum E th =114 keV (95% of pp spectrum) Measure pp- 3% Determine CNO-fraction.
MINILENS - A Scalable Prototype Detector for LENS LONU-LENS: Mini-Workshop on Low-Energy Solar Neutrinos and LENS Blacksburg, VA, October Mark Pitt.
LENS—Overview R. S. Raghavan Virginia Tech LONU-LENS Mini Workshop Oct 14, 2006.
Masatoshi Koshiba Raymond Davis Jr. The Nobel Prize in Physics 2002 "for pioneering contributions to astrophysics, in particular for the detection of cosmic.
Nd double beta decay search with SNO+ K. Zuber, on behalf of the SNO+ collaboration.
LENS:  LENS Simulations, Analysis, and Results B. Charles Rasco Louisiana State University on behalf of the LENS Collaboration.
Calorimetry for Deeply Virtual Compton Scattering in Hall A Alexandre Camsonne Hall A Jefferson Laboratory Workshop on General Purpose High Resolution.
Karsten Heeger Beijing, January 18, 2003 Design Considerations for a  13 Reactor Neutrino Experiment with Multiple Detectors Karsten M. Heeger Lawrence.
Daya Bay Reactor Neutrino Experiment On behalf of the DayaBay collaboration Virginia Polytechnic Institute and State University Joseph ykHor YuenKeung,
Davide Franco – NOW C measurement and the CNO and pep fluxes in Borexino Davide Franco NOW2004 Conca Specchiulla September 2004.
00 Cooler CSB Direct or Extra Photons in d+d  0 Andrew Bacher for the CSB Cooler Collaboration ECT Trento, June 2005.
Medium baseline neutrino oscillation searches Andrew Bazarko, Princeton University Les Houches, 20 June 2001 LSND: MeVdecay at rest MeVdecay in flight.
1 Muon Veto System and Expected Backgrounds at Dayabay Hongshan (Kevin) Zhang, BNL DayaBay Collaboration DNP08, Oakland.
Raghavan—TAUP LENS, MINILENS STATUS R. S. Raghavan Virginia Tech For The LENS Collaboration TAUP 07 Sendai, Japan Sep 13, 2007.
An experiment to measure   with the CNGS beam off axis and a deep underwater Cherenkov detector in the Gulf of Taranto CNGS.
Solar Neutrinos By Wendi Wampler. What are Neutrinos? Neutrinos are chargeless, nearly massless particles Neutrinos are chargeless, nearly massless particles.
 0 life time analysis updates, preliminary results from Primex experiment 08/13/2007 I.Larin, Hall-B meeting.
Solar Neutrino Results from SNO
Second Workshop on large TPC for low energy rare event detection, Paris, December 21 st, 2004.
October 14th, 2006LONU-LENS, Virginia Tech Solar Luminosity by Neutrinos Solar Luminosity by Neutrinos Carlos Pena Garay IFIC, Valencia ~
5th June 2003, NuFact03 Kengo Nakamura1 Solar neutrino results, KamLAND & prospects Solar Neutrino History Solar.
Forschungszentrum Karlsruhe Erice, 7th July th International School for Cosmic Rays Astrophysics Motivation Energy Reconstruction Air Fluorescence.
DPF-JPS 2006 Oct 31, Hawaii 1 CANDLES system for the study of 48-Ca double beta decay T. Kishimoto Osaka Univ.
09/04/2006NDM061 CANDLES for the study of 48 Ca double beta decay OGAWA Izumi ( 小川 泉 ) Osaka Univ. ( 大阪大学 )
Double Chooz Experiment Status Jelena Maricic, Drexel University (for the Double Chooz Collaboration) September, 27 th, SNAC11.
Solar neutrino physics The core of the Sun reaches temperatures of  15.5 million K. At these temperatures, nuclear fusion can occur which transforms 4.
Active-Sterile Neutrino Oscillations in LENS
SoLid: Recent Results and Future Prospects
Progress Towards Low Energy Neutrino Spectroscopy (LENS)
Simulation for DayaBay Detectors
Presented by S. Derek Rountree – Project Manager
SOLAR ATMOSPHERE NEUTRINOS
Search for sterile neutrinos with SOX: Monte Carlo studies of the experiment sensitivity Davide Basilico 1st year Workshop – 11/10/17 Tutors: Dott. Barbara.
Signal and Background in LENS
Davide Franco for the Borexino Collaboration Milano University & INFN
Low Energy Neutrino Astrophysics
Presentation transcript:

Low Energy Neutrinos Neutrino Luminosity of the Sun & LENS Neutrino Oscillation Workshop Conca Specchiulla, September 11, 2006 Christian Grieb Virginia Tech

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 LENS-Sol Signal = SSM(low CNO) + LMA x Detection Efficiency   Rate: pp 40 pp ev. /y /t In  2000 pp ev./ 5y/10t In  ±2.5%  Design Specification: S/N ≥ 3 LENS Expected Result: Low Energy Solar -Spectrum Access to pp spectral shape for the first time Signal (  = 4.76 µs) >98% Flux <2MeV pp:  = 64% 7 Be:  = 85% pep:  = 90%

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Test of Solar Models Solar models predict relative intensities in the pp-chain Reaction rates depend on temperature profile and abundances Cross check with measured fluxes (using neutrino oscillation physics) Data taken from John N. Bahcall, M.H. Pinsonneault, Phys.Rev.Lett.92, (2004) Solar Neutrino fluxes at the earth according to SSM

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Neutrino Inferred Solar Luminosity Nuclear fusion reactions in the solar core pp-chain + CNO cycle H.A. Bethe Phys.Rev.55, 434 (1939) No solar model needed J. N. Bahcall and R. Ulrich, Rev. Mod. Phys. 60, No. 2, p. 297 (1988) Nuclear reactions in the pp-chain:

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Solar Luminosity: Neutrino vs. photon Will be met under these conditions: 1.Fusion reactions are the sole source of energy production in the sun 2.The sun is in a quasi-steady state (change in 40,000 years is negligible) 3.The neutrino oscillation model is correct & no other physics involved; From a single detector: Test of astrophysics, solar model (absolute fluxes); Test of neutrino physics (LMA-MSW at low E, NSI, mass-varying s, CPT invariance,  13, …) (relative fluxes) Measured neutrino fluxes at earth + oscillation physics nuclear reaction rates energy release in the sun Solar luminosity as measured by photon flux = ? Energy Balance:

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Main contributions:pp Be0.074 (CNO0.014) 8 B Neutrino inferred Luminosity of the Sun - Experimental Status Measured neutrino fluxes at the earth: 8 B(SK, SNO) known very well 7 Be + 8 B (Cl) sensitive mostly to 8 B pp + 7 Be + 8 B (Ga) 7 Be (Borexino, Kamland – in the future)  in principle can deduce pp- flux Problem: disentangling fluxes from individual neutrino sources Predicted relative neutrino fluxes at the sun (SSM): Experimental status – No useful constraint! R.G.H.Robertson, Prog. Part. Nucl. Phys. 57, 90 (2006) J.N.Bahcall and C.Peña-Garay, JHEP 0311, 4 (2003)

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Temperature in the Solar Core impacts Neutrino Spectra, not just relative fluxes Neutrino Production Temperature Profile J. N. Bahcall and R. Ulrich, Rev. Mod. Phys. 60, No. 2, p. 297 (1988)

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 hep: Relative kinetic particle energies add to the Q-value of capture and fusion reactions. Not all energies contribute evenly: Temperature in the Solar Core impacts Neutrino Energies, not just relative fluxes C. Grieb and R.S. Raghavan, hep-ph/ (2006) E0E0 pep pp pp- and pep neutrino production temperature and related Gamow peak energy: 7 Be electron capture: maxwellian energy distribution shifts mean energy of 7 Be line by  ~ 1.29 keV pp-fusion: Gamow Peak at pp endpoint shifted up by ~5.2keV Maxwellian energy distribution X Tunneling probability J.N. Bahcall, Phys. Rev. D 44(6), 1644(1991) pep: combination, delta  ~ 6.6 keV J.N. Bahcall, Phys. Rev. D 49(8), 3923 (1994)

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Measurement of the Gamow Energy of pp- fusion in the sun with (improved) LENS C. Grieb and R.S. Raghavan, hep-ph/ (2006) Top:pp- spectrum with/without Gamow shift Bottom: Signal spectrum in LENS with/without Gamow shift 12t Indium - 6years -  E/E=6% at 300keV Measured Gamow shift in improved LENS: simulations with ~3000 pp events each  =1.62keV Conclusion: Slightly improved LENS can detect the predicted Gamow shift in the pp- endpoint  E=5.2keV with 95% confidence.

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Background Challenge: Indium-target is radioactive! (t = 6x10 14 y) 115 In β-spectrum overlaps pp- signal Basic background discriminator: Time/space coincidence tag Tag energy: E -tag = E βmax +116 keV Requires good spacial resolution 7 Be, CNO & LENS-Cal signals not affected by Indium-Bgd! LENS-Indium: Foundations CC -capture in 115 In to excited isomeric level in 115 Sn Tag: Delayed emission of (e/  )+  Threshold: 114 keV  pp- ’s 115 In abundance: ~ 96%

 Luminosity and LENS Christian Grieb, Virginia Tech, September Indium concentration ~8%wt (higher may be viable) 2. Scintillation signal efficiency (working value): 9000 h /MeV 3. Transparency at 430 nm: L(1/e) (working value): 10m 4. Chemical and Optical Stability: at least 1 year 5. InLS Chemistry - Robust Basic Bell Labs Patent, filed 2001, awarded % InLS (PC:PBD/MSB) hν / MeV BC505 Std h /MeV In 8%-photo Light Yield from Compton edges of 137 Cs  -ray Spectra (nm) Norm. Absorbance in 10 cm L(1/e)(InLS 8%) ~ L(PC Neat) ! ZVT39: Abs/10cm ~0.001;  L(1/e)(nominally) >>20 m InLS PC Neat Indium Liquid Scintillator Status Milestones unprecedented in metal LS technology LS technique relevant to many other applications

 Luminosity and LENS Christian Grieb, Virginia Tech, September D Digital Localizability of Hit within one cube  ~75mm precision vs. 600 mm (±2σ) by TOF in longitudinal modules  x8 less vertex vol.  x8 less random coinc.  Big effect on Background  Hit localizability independent of event energy Test of double foil mirror in New Detector Technology - The Scintillation Lattice Chamber Light propagation in GEANT4 Concept

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Indium  - -Background Topology – Space / Time coincidence Background Signal E( ) -114 keV 116 keV 498 keV 115 In 115 Sn e/    =4.76  s Background: Random time and space coincidence between two  -decays ( ); Extended shower ( ) can be created by: a)498 keV  from decay to excited state; b)Bremsstrahlungs  -rays created by  ; c)Random coincidence (~10 ns) of more  -decays; Or any combination of a), b) and c). Signal Signature: Prompt e - ( ) followed by low energy (e - /  ) ( ) and Compton-scattered  ( ) 115 In β 0 + n  (BS) (E max = 499 keV) 498 keV *Cattadori et al: 2003 β 1 (E max < 2 keV) (b = 1.2x10 -6 )* 115 Sn 

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Results of GEANT4 Monte Carlo simulation (cell size = 7.5cm, S/N=3) Signal (pp) y -1 t In) -1 Bgd (In) y -1 (t In) -1 RAW rate x A. Tag in Space/Time delayed coincidence with prompt event in vertex x 10 5 B. + ≥3 Hits in tag shower x 10 4 C. +Tag Energy = 614 keV44306 D. +Tag topology4013 ± 0.6 Background rejection steps: A.Time/space coincidence in the same cell required for trigger; B.Tag requires at least three ‘hits’; C.Narrow energy cut; D.A tag topology: multi-  vs. Compton shower; Classification of events according to hit multiplicity; Cut parameters optimized for each event class improved efficiency; Reduction by ~ through time/space coincidence Indium  - -Background Discrimination

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Test all the concepts and the technology developed so far & demonstrate Indium solar signal detection: MINI-LENS liter InLS scintillation lattice detector Summary ● Indium liquid scintillator synthesis ● New detector technology (Scintillation Lattice Chamber) ● GEANT4 Simulation of Indium  - background  Basic feasibility of In-LENS-Sol secure (10t In, 125t In-LS) Major breakthroughs in LENS: Science in LENS: Measure solar -spectrum below 2MeV  Luminosity of the sun  Gamow shift of pp- spectrum probes the T profile  Test of Astrophysics & physics in one experiment Next Step:

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Russia: INR (Moscow):I. Barabanov, L. Bezrukov, V. Gurentsov, V. Kornoukhov, E. Yanovich; INR (Troitsk):V. Gavrin et al., A. Kopylov et al.; U. S.: BNL:R. L. Hahn, M. Yeh; U. N. Carolina:A. Champagne; ORNL:J. Blackmon, C. Rascoe, A. Galindo-Uribarri, Q. Zeng; Princeton U. :J. Benziger; Virginia Tech:Z. Chang, C. Grieb, M. Pitt, R.S. Raghavan, D. Rountree, R.B. Vogelaar; LENS-Sol / LENS-Cal Collaboration (Russia-US: 2004-) New collaborators cordially invited!

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Additional Slides

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Signal Reconstruction Event localization relies on PMT hit pattern (NOT on signal timing) Algorithm finds best solution for event pattern to match PMT signal pattern System is overdetermined, hardly affected by unchannelled light Timing information + position  shower structure

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Data: Main Simulation of Indium Events with GEANT4 ~ 4x10 6 In decays in one cell centered in ~3m 3 volume (2-3 days PC time) Analysis trials with choice of pe/MeV and cut parameters (5’ /trial) Indium Background Simulations and Analysis Analysis Strategy Primary selection - tag candidate shower events with Nhit ≥ 3 Classify all eligible events (Nhit ≥ 3) according to Nhit Optimize cut conditions individually for each Nhit class Main Cuts Total energy: g2+g3 Tag topology: Distance of lone  from shower

 Luminosity and LENS Christian Grieb, Virginia Tech, September ”PMT Passive Shield Mirror 5”PMT Passive Shield Mirror Opt segmentation cage InLS 500 mm InLS LS Envelope 500 mm InLS : 128 L PC Envelope : 200 L 12.5cm pmt’s : 108 MINILENS Final Test detector for LENS

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 MINILENS: Global test of LENS R&D Test detector technology  Large Scale InLS  Design and construction Test background suppression of In radiations by Demonstrate In solar signal detection in the presence of high background Direct blue print for full scale LENS

 Luminosity and LENS Christian Grieb, Virginia Tech, September 2006 Proxy pp nu events in MINILENS from cosmogenic 115 In(p,n) 115 Sn isomers Pretagged via , p tracks Post tagged via n and 230  s delay  Gold plated 100 keV events (proxy pp), Tagged by same cascade as In- events  Demonstrate In- Signal detection even in MINILENS Proxy pp- events in MINILENS