1 MEMPHYS Simulation & Performance A. Tonazzo, N. Vassilopoulos * / APC for MEMPHYS ECFA Review Panel, Dansbury May 2011 * now at IPHC, Strasbourg.

Slides:



Advertisements
Similar presentations
EuroNu CERN February 5, 2008 Marco Zito Super-Beam work package Marco Zito Dapnia-Saclay On behalf of the SB w2 team EuroNu 5/2/2008 Thanks to M. Dracos.
Advertisements

NDVCS measurement with BoNuS RTPC M. Osipenko December 2, 2009, CLAS12 Central Detector Collaboration meeting.
CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
Trigger issues for KM3NeT the large scale underwater neutrino telescope the project objectives design aspects from the KM3NeT TDR trigger issues outlook.
HARP Anselmo Cervera Villanueva University of Geneva (Switzerland) K2K Neutrino CH Meeting Neuchâtel, June 21-22, 2004.
A long-baseline experiment with the IHEP neutrino beam Y. Efremenko detector Presented by.
Super-Kamiokande Introduction Contained events and upward muons Updated results Oscillation analysis with a 3D flux Multi-ring events  0 /  ratio 3 decay.
03 Aug NP041 KOPIO Experiment Measurement of K L    Hideki Morii (Kyoto Univ.) for the KOPIO collaborations Contents Physics Motivation.
Is B s 0 production by neutrino interactions interesting? Presented at the Super-B factory workshop as an alternative approach Nickolas Solomey 21 April.
Off-axis Simulations Peter Litchfield, Minnesota  What has been simulated?  Will the experiment work?  Can we choose a technology based on simulations?
How to Build a Neutrino Oscillations Detector - Why MINOS is like it is! Alfons Weber March 2005.
A Search for Point Sources of High Energy Neutrinos with AMANDA-B10 Scott Young, for the AMANDA collaboration UC-Irvine PhD Thesis:
Liquid Scintillation Detectors for High Energy Neutrinos John G. Learned Department of Physics and Astronomy, University of Hawaii See: arXiv:
Basic Measurements: What do we want to measure? Prof. Robin D. Erbacher University of California, Davis References: R. Fernow, Introduction to Experimental.
Energy Reconstruction Algorithms for the ANTARES Neutrino Telescope J.D. Zornoza 1, A. Romeyer 2, R. Bruijn 3 on Behalf of the ANTARES Collaboration 1.
INDIA-BASED NEUTRINO OBSERVATORY (INO) STATUS REPORT Naba K Mondal Tata Institute of Fundamental Research Mumbai, India NUFACT Scoping Study Meeting at.
Zhihong Ye Hampton University Feb. 16 th 2010, APS Meeting, Washington DC Data Analysis Strategy to Obtain High Precision Missing Mass Spectra For E
A feasibility study for the detection of SuperNova explosions with an Undersea Neutrino Telescope A. Leisos, A. G. Tsirigotis, S. E. Tzamarias Physics.
New results from K2K Makoto Yoshida (IPNS, KEK) for the K2K collaboration NuFACT02, July 4, 2002 London, UK.
Coincidence analysis in ANTARES: Potassium-40 and muons  Brief overview of ANTARES experiment  Potassium-40 calibration technique  Adjacent floor coincidences.
A. Blondel, M.Campanelli, M.Fechner Energy measurement in quasi-elastics Unfolding detector and physics effects Alain Blondel Mario Campanelli Maximilien.
A Reconstruction Algorithm for a RICH detector for CLAS12 Ahmed El Alaoui RICH Workchop, Jefferson Lab, newport News, VA November th 2011.
PINGU – An IceCube extension for low-energy neutrinos Uli Katz on behalf of the PINGU Collaboration European Strategy for Neutrino Oscillation.
NNN /10/07 1 MEMPHYS MEgaton Mass PHYSics Detector N. Vassilopoulos / LAL on behalf of MEMPHYS Collaboration without LAGUNA aspects (L.Mosca) without.
Recent results from the K2K experiment Yoshinari Hayato (KEK/IPNS) for the K2K collaboration Introduction Summary of the results in 2001 Overview of the.
Feb 10, 2005 S. Kahn -- Pid Detectors in G4MicePage 1 Pid Detector Implementation in G4Mice Steve Kahn Brookhaven National Lab 10 Feb 2005.
Status of the NO ν A Near Detector Prototype Timothy Kutnink Iowa State University For the NOvA Collaboration.
The Earth Matter Effect in the T2KK Experiment Ken-ichi Senda Grad. Univ. for Adv. Studies.
2 Atmospheric Neutrinos Atmospheric neutrino detector at Kolar Gold Field –1965.
1 Realistic top Quark Reconstruction for Vertex Detector Optimisation Talini Pinto Jayawardena (RAL) Kristian Harder (RAL) LCFI Collaboration Meeting 23/09/08.
Long Baseline Experiments at Fermilab Maury Goodman.
Large area photodetection for Water Cerenkov detectors PMm 2 proposal: Front End Electronics MAROC ASIC Pierre BARRILLON, Sylvie BLIN, Jean-Eric CAMPAGNE,
MiniBooNE Michel Sorel (Valencia U.) for the MiniBooNE Collaboration TAUP Conference September 2005 Zaragoza (Spain)
Gavril Giurgiu, Carnegie Mellon, FCP Nashville B s Mixing at CDF Frontiers in Contemporary Physics Nashville, May Gavril Giurgiu – for CDF.
NESTOR SIMULATION TOOLS AND METHODS Antonis Leisos Hellenic Open University Vlvnt Workhop.
Counting Electrons to Measure the Neutrino Mass Hierarchy J. Brunner 17/04/2013 APC.
1 MEMPHYS Safety at the Fréjus site Jean-Luc Borne – June Summary of MEMPHYS Studies Nikos Vassilopoulos, IPHC, CNRS.
Hyper-Kamiokande project and R&D status Hyper-K project Motivation Detector Physics potential study photo-sensor development Summary Kamioka.
1 水质契仑科夫探测器中的中子识别 张海兵 清华大学 , 南京 First Study of Neutron Tagging with a Water Cherenkov Detector.
Detection of electromagnetic showers along muon tracks Salvatore Mangano (IFIC)
CEA DSM Irfu Reconstruction and analysis of ANTARES 5 line data Niccolò Cottini on behalf of the ANTARES Collaboration XX th Rencontres de Blois 21 / 05.
1 MEMPHYS Simulation & Performance A. Tonazzo, N. Vassilopoulos * / APC for MEMPHYS N. WP5 EUROnu RAL 2011 * now at IPHC, Strasbourg.
The ORCA Letter of Intent Oscillation Research with Cosmics in the Abyss ORCA Antoine Kouchner University Paris 7 Diderot- AstroParticle and Cosmology.
NuFact02, July 2002, London Takaaki Kajita, ICRR, U.Tokyo For the K2K collab. and JHF-Kamioka WG.
Nucleon Decay Search in the Detector on the Earth’s Surface. Background Estimation. J.Stepaniak Institute for Nuclear Studies Warsaw, Poland FLARE Workshop.
Neutrino Oscillations at Super-Kamiokande Soo-Bong Kim (Seoul National University)
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.
CP violation in B decays: prospects for LHCb Werner Ruckstuhl, NIKHEF, 3 July 1998.
Accelerator-based Long-Baseline Neutrino Oscillation Experiments Kam-Biu Luk University of California, Berkeley and Lawrence Berkeley National Laboratory.
2 July 2002 S. Kahn BNL Homestake Long Baseline1 A Super-Neutrino Beam from BNL to Homestake Steve Kahn For the BNL-Homestake Collaboration Presented at.
CP phase and mass hierarchy Ken-ichi Senda Graduate University for Advanced Studies (SOKENDAI) &KEK This talk is based on K. Hagiwara, N. Okamura, KS PLB.
An experiment to measure   with the CNGS beam off axis and a deep underwater Cherenkov detector in the Gulf of Taranto CNGS.
1 Limitations in the use of RICH counters to detect tau-neutrino appearance Tord Ekelöf /Uppsala University Roger Forty /CERN Christian Hansen This talk.
Cherenkov Tracking Calorimeters D. Casper University of California, Irvine.
P.F.Ermolov SVD-2 status and experimental program VHMP 16 April 2005 SVD-2 status and experimental program 1.SVD history 2.SVD-2 setup 3.Experiment characteristics.
September 10, 2002M. Fechner1 Energy reconstruction in quasi elastic events unfolding physics and detector effects M. Fechner, Ecole Normale Supérieure.
MIND Systematic Errors EuroNu Meeting, RAL 18 January 2010 Paul Soler.
Geant4 Simulation for KM3 Georgios Stavropoulos NESTOR Institute WP2 meeting, Paris December 2008.
Observation Gamma rays from neutral current quasi-elastic in the T2K experiment Huang Kunxian for half of T2K collaboration Mar. 24, Univ.
Open and Hidden Beauty Production in 920 GeV p-N interactions Presented by Mauro Villa for the Hera-B collaboration 2002/3 data taking:
 13 Readout Electronics A First Look 28-Jan-2004.
23/11/05BENE meeting at CERN1 (22-25 November 2005) L. Mosca (CEA-Saclay) The MEMPHYS project MEgaton Mass PHYSics in a Large International Underground.
Marcos DRACOS IPHC-IN2P3/CNRS Université de Strasbourg
IPHC-IN2P3/CNRS Strasbourg
EURONu Collaboration Board,
Results from OPERA Pablo del Amo Sánchez for the OPERA collaboration
Physics with the ICARUS T1800 detector
A First Look J. Pilcher 12-Mar-2004
Impact of neutrino interaction uncertainties in T2K
Presentation transcript:

1 MEMPHYS Simulation & Performance A. Tonazzo, N. Vassilopoulos * / APC for MEMPHYS ECFA Review Panel, Dansbury May 2011 * now at IPHC, Strasbourg

2  underground water Cherenkov at Laboratoire Souterrain de Modane Fréjus at 4800 m.w.e.  total fiducial volume: up to 400 kton: 3 x 65mX60 modules could be designed up to 572kton: 3 x 65mX80m size, shape limited by light attenuation length (λ~80m) and pressure on PMTs size, shape limited by light attenuation length (λ~80m) and pressure on PMTs readout : ~3 x 81k 12″ (alternatively 8″, 10″) PMTs, 30% cover readout : ~3 x 81k 12″ (alternatively 8″, 10″) PMTs, 30% cover  PMT R&D + detailed study on excavation existing & ongoing + prototype Cherenkov detector MEMPHYNO  underground water Cherenkov at Laboratoire Souterrain de Modane Fréjus at 4800 m.w.e.  total fiducial volume: up to 400 kton: 3 x 65mX60 modules could be designed up to 572kton: 3 x 65mX80m size, shape limited by light attenuation length (λ~80m) and pressure on PMTs size, shape limited by light attenuation length (λ~80m) and pressure on PMTs readout : ~3 x 81k 12″ (alternatively 8″, 10″) PMTs, 30% cover readout : ~3 x 81k 12″ (alternatively 8″, 10″) PMTs, 30% cover  PMT R&D + detailed study on excavation existing & ongoing + prototype Cherenkov detector MEMPHYNO MEMPHYS: Underground Laboratory and Detector ECFA Review Panel, Dansbury May 2011 one possible design at LSM (by Lombardi SA Inagenieurs – Conseils) (by Lombardi SA Inagenieurs – Conseils)

3 MEMPHYS physics goals  Proton decay sensitivity: up to yrs in 10y from the "golden" channel: p  e + π 0 up to yrs in 10y from the "golden" channel: p  e + π 0 up to 2x10 34 yrs in 10y from p  K + + anti- up to 2x10 34 yrs in 10y from p  K + + anti-  SuperNova core collapse: huge statistics from galactic SN => spectral analysis in E,t, flavour -> access SN collapse mechanism / neutrino oscillation parameters huge statistics from galactic SN => spectral analysis in E,t, flavour -> access SN collapse mechanism / neutrino oscillation parameters sensitivity up to ~1 Mpc sensitivity up to ~1 Mpc possibility of early SN trigger (from event coincidence) up to ~5 Mpc possibility of early SN trigger (from event coincidence) up to ~5 Mpc  SuperNova relic neutrinos: observable in few years with significant statistics, according to most of existing models observable in few years with significant statistics, according to most of existing models direct measurement of emission parameters possible direct measurement of emission parameters possible  and, of course... NEUTRINO BEAMS (EUROnu WP2, WP4) ECFA Review Panel, Dansbury May 2011

4 CERN-MEMPHYS: Oscillation measurements with beams  θ 13 discovery reach and sensitivity to CP Violation CERN Fréjus Campagne, Maltoni, Mezzeto, Schwertz hep-ph/ ECFA Review Panel, Dansbury May 2011

CERN-MEMPHYS: Oscillation measurements Studies with beams good sensitivity of θ 13 and δ CP for super- beams (   e ) & beta-beams ( e   )  good sensitivity of θ 13 and δ CP for super- beams (   e ) & beta-beams ( e   )  improved performance with the 2 beams combined Campagne, Maltoni, Mezzeto, Schwertz hep-ph/ βB beam’s ions/year reduced by 2: performance is strongly depended on ion production 5 ECFA Review Panel, Dansbury May 2011

Latest Results from WP2 SuperBeam Studies ECFA Review Panel, Dansbury May  Graphite Solid target, 2λ I  Hg, 2λ I  Integrated target, 2λ I  excellent performance of packed bed Ti, d= 74%d Ti any density reduction of packed could be recuperated increasing the horn current by 50, 100 kA

Campagne, Maltoni, Mezzeto, Schwertz hep-ph/ CERN-MEMPHYS: mass hierarchy and degeneracies addition of ATM data leads to a sensitivity to the neutrino mass hierarchy at 2σ CL for sin 2 2θ 13 ≥ for βB and SPL  addition of ATM data leads to a sensitivity to the neutrino mass hierarchy at 2σ CL for sin 2 2θ 13 ≥ for βB and SPL  the optimal hierarchy sensitivity is obtained from combining βB + SPL + atmospheric data  beta beam + ATM can not solve degeneracies (no  and insufficient spectral info)  super beam + ATM: degeneracies lifted without ATM data for large sin 2 2θ 13 degeneracies and mass hierarchy is possible to be resolved: 7 ECFA Review Panel, Dansbury May 2011

8 R&D towards MEMPHYS : PMm2: “Innovative electronics for array of photodetectors used in High Energy Physics and Astroparticles”. R&D program funded by French national agency for research (LAL, IPNO, LAPP and Photonis) ( ) Basic concept: very large photodetection surface  macropixels of PMTs connected to an autonomous front- end electronics. Replace large PMTs (20”) by groups of 16 smaller ones (12”, 8”) with central ASIC : Independent channelsIndependent channels charge and time measurementcharge and time measurement water-tight, common High Voltagewater-tight, common High Voltage Only one wire out (DATA + VCC)Only one wire out (DATA + VCC) I.studies on 12" 8" PMTs design -parameter correlation -potting -pressure resistance (collaboration with BNL since NNN07) II.PArISROC readout chip -complete front-end chip with 16 channels -testboard now in layout, soon available detailed description of the R&D: pmm2.in2p3.fr ECFA Review Panel, Dansbury May 2011 installed at APC, Paris

MEMPHYNO at APC & Demonstrator 9 ECFA Review Panel, Dansbury May 2011 M. Marafini’s talk at NNN10

10  Event Generator: GENIE for beam newGENIE for beam new  MEMPHYS Full Simulation (M. Fechner, J.E. Campagne, N. Vassilopoulos) : Interface with the OpenScientist v16r0 framework (G. Barrand/LAL) using distribution kits as Geant4 & CLHEP & AIDA-IO implementation to Rio (also HDF5, XML)Interface with the OpenScientist v16r0 framework (G. Barrand/LAL) using distribution kits as Geant4 & CLHEP & AIDA-IO implementation to Rio (also HDF5, XML) 3 modes of running in the same framework:3 modes of running in the same framework: Interactive Viewing, Batch processing, AIDA_ROOT analysis Interactive Viewing, Batch processing, AIDA_ROOT analysis primary + secondary + Optical Photon info, modular detector geometry, ntuples’ storage, etc...primary + secondary + Optical Photon info, modular detector geometry, ntuples’ storage, etc...  MEMPHYS Event Reconstruction, Analyses (N. Vassilopoulos, A. Tonazzo, M. Marafini) : interactive ROOT- cintinteractive ROOT- cint Solo C++ for complex/high stats using ROOT + AIDA librariesSolo C++ for complex/high stats using ROOT + AIDA libraries MEMPHYS: Full Simulation Present Status ECFA Review Panel, Dansbury May 2011

11 MEMPHYS v7 atmospheric (1-10GeV) atmospheric (1-10GeV) transparency by J. E. Campagne ECFA Review Panel, Dansbury May 2011

ns  →  - →e -  →  - →e - MEMPHYS v7 Interactive histogram to identify the e Michel optical photons… Only detected op. photons transparency by J. E. Campagne ECFA Review Panel, Dansbury May 2011

MEMPHYS: GUI / Event Reconstruction 13 MEMPHYS GUI MEMPHYS: interactive μ MeV ECFA Review Panel, Dansbury May 2011  main task using all the available tools evaluate detector performance evaluate detector performance extract energy resolutions and lepton efficiencies migration matrices extract energy resolutions and lepton efficiencies migration matrices

Attenuation length studies 14 attenuation length in water as a function of the wavelength in MEMPHYS simulation  correct modelling of light propagation looks comparable to SK data looks comparable to SK data ECFA Review Panel, Dansbury May 2011

MEMPHYS Single ring studies, electrons  single e- events from 1 to 25 MeV (FC): PMTs and PE infos 15 Number of PMTs with at least one photoelectron as a function of electron energy ECFA Review Panel, Dansbury May 2011 * * * * * * * * 27% more FV without light reduction 65mX60m * 65mX80m 65mX60m * 65mX80m

MEMPHYS Single ring studies electrons, muons  single e-, μ+ (no decays) events from 200 to 1000 MeV: PMTs and PE infos 16 Number of PMTs with at least one photoelectron as a function of lepton energy Number of detected photoelectrons per MeV as a function of lepton energy ECFA Review Panel, Dansbury May 2011 e- e- μ+μ+μ+μ+ μ+μ+μ+μ+

Single rings: electrons primary vertex fit  pick up a 400 MeV electron (FC), assume point like track length  primary vertex fit based only on each PMT’s timing info: t i PMT = t i + TOF i => t i = t i PMT – TOF i, where TOF i = (n / c) x D, D = distance between each PMT and grid’s coordinates  maximize estimator E a la SK to find the true vertex of electron : 17 e- vertex random point fit estimator ECFA Review Panel, Dansbury May 2011

Single rings: particle direction, outer ring edge  keep the 400 MeV e-  calculate roughly the direction: t  θ edge θ edge > θ peak θ edge > θ peak d 2 PE(θ) / d 2 (θ) = 0 d 2 PE(θ) / d 2 (θ) = 0 18 θ peak = 42 0 θ edge θ edge > θ peak d 2 PE(θ) / d 2 (θ) = 0 ECFA Review Panel, Dansbury May 2011

Single rings (FC): e-, μ+ 200MeV to 1000MeV ring direction  find the best direction maximizing : 19 ECFA Review Panel, Dansbury May 2011 e- θ edge Q(θ edge ) PEs angular distribution seen at best vertex and with respect to true direction. Different shapes μ+μ+μ+μ+ θ edge Q(θ edge ) spread e’ s rings sharper μ’ s rings θ edge θ peak = 42 0 θ mean = 44 0 θ peak = 42 0 θ mean = 38 0

Single rings: e-, μ+ 200MeV to 1000MeV pid  use PEs (PMT) angular distribution from best reconstructed vertex and best direction as fast pid variable  full detector simulation  20 ECFA Review Panel, Dansbury May 2011 e- PEs angular distribution seen at best vertex and with respect to best direction. Different shapes μ+μ+μ+μ+ pid spread e’ s rings sharper μ’ s rings pid number of PEs as a function of the PMT distance to the best vertex and with respect to best direction dPE(θ) / d (θ) θ peak = 42 0 θ mean = 44 0 θ peak = 40 0 θ mean = 37 0

Single rings: e-, μ+ up to 1 GeV/c momentum resolution (magnitude)  R tot, to correlate momentum with measured charged  full detector simulation but low statistics 21 ECFA Review Panel, Dansbury May 2011 resolutions in between to SK-I, SK-II: higher energies higher statistics of collected charge lower energies small degradation due to detector size e- μ+μ+μ+μ+

Single rings: e-, μ+ up to 1 GeV/c momentum resolution (direction)  make the difference of true and reconstructed: resolution in degrees at 68% of events  full detector simulation but low statistics 22 ECFA Review Panel, Dansbury May 2011 comparable to SK e- μ+μ+μ+μ+

MEMPHYS energy reconstruction  momentum resolution could be be applied to any beam design to derive efficiencies, bdg. contamination and migration matrices  e.g. true versus reconstructed  uniform neutrino, antinuetrino samples up to 1 GeV, interactions in water simulated with GENIE 23 gaussian peak due to QE’s smearing of Fermi motion and experimental resolution tail due to no-QE events, increasing with ν ‘s energy νμνμ νμνμ ECFA Review Panel, Dansbury May 2011 νμνμ

24 conclusions, next steps conclusions so far: MEMPHYS detector performance:  primary vertex reconstruction, ring direction  excellent single-ring identification as e or μ (low stats)  single-ring momentum and direction resolution: energy reconstruction  detector optimisation: no light reduction when moving from 65mx60m to 65mx80m detector (+27% FV): similar results are expected in event reconstruction. next steps:  optimisation of vertex reconstruction, ring counting  background: π 0 for SB and single π +- for βB analyses  high statistical neutrino samples to extract migration matrices (in progress)  volume vs. performance studies: more detailed THANKS THANKS ECFA Review Panel, Dansbury May 2011