WP2 Background simulations: progress of the work.

Slides:



Advertisements
Similar presentations
TIERRAS: an AIRES package to simulate high energy cosmic ray showers underground and underwater Matías Tueros Instituto de Física La Plata – Universidad.
Advertisements

Stefan Roesler SC-RP/CERN on behalf of the CERN-SLAC RP Collaboration
Antonis Leisos KM3NeT Collaboration Meeting the calibration principle using atmospheric showers the calibration principle using atmospheric showers Monte.
Plastic Scintillator Option for DB a simulation study by Maxim Gonchar, Yury Gornushkin and Dmitry Naumov JINR, Dubna, Russia Collaboration Meeting January.
Atmospheric Neutrinos Barry Barish Bari, Bologna, Boston, Caltech, Drexel, Indiana, Frascati, Gran Sasso, L’Aquila, Lecce, Michigan, Napoli, Pisa, Roma.
Institut für Kernphysik Markus Horn ILIAS-N3, BSNS-working group meeting Valencia, Forschungszentrum Karlsruhe in der Helmholtz-Gemeinschaft.
Activity for the Gerda-specific part Description of the Gerda setup including shielding (water tank, Cu tank, liquid Nitrogen), crystals array and kapton.
WP2 Background simulations Outline Execution plan for the third year Progress of the work Activities and news.
13/12/2004Vitaly Kudryavtsev - LRT20041 Simulation of backgrounds for particle astrophysics experiments V. A. Kudryavtsev Department of Physics and Astronomy.
Development of a standard library of background simulation codes JRA1WP2 Gloria Luzon, Canfranc Underground Laboratory.
Neutron energy spectrum from U and Th traces in the Modane rock simulated with SOURCES (full line). The fission contribution is also shown (dashed line).
Modane, 12/01/2005 Vitaly Kudryavtsev - JRA1 meeting 1 Background simulations: testing Monte Carlo codes V. A. Kudryavtsev Department of Physics and Astronomy.
JRA1 meeting - 10/07/2006Vitaly Kudryavtsev1 Muon-induced neutrons: how deep should we go to get rid of them? V. A. Kudryavtsev Department of Physics and.
N3-BSNS/JRA1-WP2 - Valencia, 15 April 2005Vitaly Kudryavtsev 1 Monte Carlo codes: MUSIC, MUSUN, SOURCES Vitaly Kudryavtsev Department of Physics and Astronomy.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
21-25 January 2002 WIN 2002 Colin Okada, LBNL for the SNO Collaboration What Else Can SNO Do? Muons and Atmospheric Neutrinos Supernovae Anti-Neutrinos.
MUON FLUX MEASUREMENTS AT THE LSC JRA1-N2 Meeting, Zaragoza, Nov 23 rd 2007 Héctor Gómez Maluenda, University of Zaragoza.
Simulations with MEGAlib Jau-Shian Liang Department of Physics, NTHU / SSL, UCB 2007/05/15.
Luciano Pandola, INFN Gran Sasso Luciano Pandola INFN Gran Sasso Valencia, April 14 th, 2005 Geant4 and the underground physics community.
GLAST LAT Project Test Beam Meeting, June 6, 2006 S. Funk 1/6 PS Positron Simulations Stefan Funk June 6, 2006.
Atmospheric Neutrino Oscillations in Soudan 2
EHE Search for EHE neutrinos with the IceCube detector Aya Ishihara for the IceCube collaboration Chiba University.
Study of plastic scintillator quenching factors Lea Reichhart, IOP Glasgow, April /17.
Medium heavy Λ hyper nuclear spectroscopic experiment by the (e,e’K + ) reaction Graduate school of science, Tohoku University Toshiyuki Gogami for HES-HKS.
Preliminary MC study on the GRAND prototype scintillator array Feng Zhaoyang Institute of High Energy Physics, CAS, China GRAND Workshop, Paris, Feb. 015.
Neutron scattering systems for calibration of dark matter search and low-energy neutrino detectors A.Bondar, A.Buzulutskov, A.Burdakov, E.Grishnjaev, A.Dolgov,
NESTOR SIMULATION TOOLS AND METHODS Antonis Leisos Hellenic Open University Vlvnt Workhop.
Properties of giant air showers and the problem of energy estimation of initial particles M.I. Pravdin for Yukutsk Collaboration Yu.G. Shafer Institute.
G4GeneralParticleSource Class: Developed by ESA as the space radiation environment is often quite complex in energy and angular distribution, and requires.
Detector Monte-Carlo ● Goal: Develop software tools to: – Model detector performance – Study background issues – Calculate event rates – Determine feasibility.
What is MaGe? MJ outputGERDA output MaGe is a Monte Carlo simulation package dedicated to experiments searching for 0 2  decay in 76 Ge. Created by the.
Cosmic rays at sea level. There is in nearby interstellar space a flux of particles—mostly protons and atomic nuclei— travelling at almost the speed of.
Hadronic interaction studies with the ARGO-YBJ experiment (5,800 m 2 ) 10 Pads (56 x 62 cm 2 ) for each RPC 8 Strips (6.5 x 62 cm 2 ) for each Pad ( 
1 NaI calibrationneutron observation NaI calibration and neutron observation during the charge exchange experiment 1.Improving the NaI energy resolution.
MaGe framework for Monte Carlo simulations MaGe is a Geant4-based Monte Carlo simulation package dedicated to experiments searching for 0 2  decay of.
Status of neutron simulations Piotr Mijakowski (Warsaw) ArDM meeting, 2010/12/03 1.
In high energy astrophysics observations, it is crucial to reduce the background effectively to achieve a high sensitivity, for the source intensity is.
Radiation study of the TPC electronics Georgios Tsiledakis, GSI.
Luciano Pandola, INFN Gran Sasso Luciano Pandola INFN Gran Sasso Genova, July 18 th, 2005 Geant4 and the underground physics community.
Geant4 and the Underground Physics Community Luciano Pandola INFN, Laboratori Nazionali del Gran Sasso for the ILIAS JRA1 and N3 Monte Carlo groups Geant4.
Marina Golubeva, Alexander Ivashkin Institute for Nuclear Research RAS, Moscow AGeV simulations with Geant4 and Shield Geant4 with Dpmjet-2.5 interface.
NEVOD-DECOR experiment: results and future A.A.Petrukhin for Russian-Italian Collaboration Contents MSU, May 16, New method of EAS investigations.
Alex Howard PH-SFT LCG-PV 10 th May 2006 Neutron Benchmark for Geant4 using TARC – initial status 1)TARC – experimental set-up and aims 2)Geant4 Simulation.
September 10, 2002M. Fechner1 Energy reconstruction in quasi elastic events unfolding physics and detector effects M. Fechner, Ecole Normale Supérieure.
1 Study of Data from the GLAST Balloon Prototype Based on a Geant4 Simulator Tsunefumi Mizuno February 22, Geant4 Work Shop The GLAST Satellite.
A New Upper Limit for the Tau-Neutrino Magnetic Moment Reinhard Schwienhorst      ee ee
Muon-induced neutron background at Boulby mine Vitaly A. Kudryavtsev University of Sheffield UKDMC meeting, ICSTM, London, 27 June 2002.
Alex Howard, CERN Slide 1 Simulating Dark Matter Detectors (a.k.a. DMX Underground Advanced Example) 1.Dark Matter detectors 2.Implementation within Geant4.
Muon Flux Measurements and Simulation at CJPL Zhi ZENG CDEX Collaboration Symposium of the Sino-German GDT Cooperation Tübingen, Apr
Geant4 Simulation for KM3 Georgios Stavropoulos NESTOR Institute WP2 meeting, Paris December 2008.
1 Cosmic Ray Physics with IceTop and IceCube Serap Tilav University of Delaware for The IceCube Collaboration ISVHECRI2010 June 28 - July 2, 2010 Fermilab.
EHE Search for EHE neutrinos with the IceCube detector Aya Ishihara Chiba University.
 CC QE results from the NOvA prototype detector Jarek Nowak and Minerba Betancourt.
Alex Howard, Imperial College Slide 1 July 2 nd 2001 Underground Project UNDERGROUND PROJECT – Overview and Goals Alex Howard Imperial College, London.
Report (2) on JPARC/MLF-12B025 Gd(n,  ) experiment TIT, Jan.13, 2014 For MLF-12B025 Collaboration (Okayama and JAEA): Outline 1.Motivation.
Comparisons of neutron production by muons in GEANT4 and toy model
Cosmogenic Muon Background
Fast neutron flux measurement in CJPL
Muons in IceCube PRELIMINARY
Update on Muon Flux Underground Using Geant4 Simulation
Simulation for DayaBay Detectors
Neutron and 9Li Background Calculations
Summary of hadronic tests and benchmarks in ALICE
Gamma-ray Albedo of the Moon Igor V. Moskalenko (Stanford) & Troy A
Development of a standard library of background simulation codes
BACKGROUND STUDY IN CRESST
The Hadrontherapy Geant4 advanced example
Beam Dump Experiments with Photon and Electron Beams
Development of a standard library of background simulation codes
Development of a standard library of background simulation codes
Presentation transcript:

WP2 Background simulations: progress of the work

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 JRA1-WP2 N3-BSNS JRA2(IDEA)WP3-B1 Development of a standard library of background simulation codes BackgroundSimulation,Neutron-Shield and Muon-Vetos and Muon-Vetos Study on Cosmogenic Induced Activity Induced Activity

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 General issues

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Planning for this third year Analysis of data collected in the background monitoring campaign with MC codes Optimisation of the codes Tasks Design and implementation of the library –Standard codes for specific task –End-to-end simulation tool for experiments. Milestones and deliverables

Analysis of collected data and optimisation of codes

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Muon simulations and MUSUN Muon backgrounds at Super-Kamiokande, KamLAND and CHOOZ are calculated using MUSIC (hep-ph/ ) –Use of digital maps and mountain profile –Real composition of the rock (approximate in CHOOZ) –Modified Gaisser atmospheric muon parametrization in the large angle and small energy regimes –Well tested Monte Carlo integration method

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Average muon intensity versus depth: experimental and simulated (standard and modified Gaisser parametrization)

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Perfect agreement simulation/experiment (Cherenkov detector covering the entire solid angle) Exp Stand. rock

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Not so good agreement simulation/experiment (Two RPC plates) Better agreement in the simulated experiment

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June x10 -5 Quite good agreement regarding fluxes

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 G4 muon simulation and LSC measurements GOAL To help in the understanding and interpretation of muon measurements in Zaragoza and Canfranc FEATURES Code: GEANT4 simulation, including standard electromagnetic processes for muons (Multiple Scattering, Ionisation, Bremsstrahung, Pair production,  - Capture) Geometry: two plastic scintillators 40x80x5.08 cm 3 (BC408) with different air separations, according to measurements Primary particles: muons with energy spectrum and angular distribution corresponding to Zaragoza (sea level) and Canfranc depth Output: energy deposits in each of the two detectors registered to perform off- line coincidence analysis with ROOT

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 RESULTS: Zaragoza Angular distribution: I α cos 2  Energy spectrum: mean energy ~4 GeV, f(E)=N 0 if E E 0 Detector configuration: without air between them

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Registered energy spectra in top and bottom detectors energy (MeV)

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 RESULTS: Zaragoza Angular distribution: I α cos 2  Energy spectrum: mean energy ~4 GeV, f(E)=N 0 if E E 0 Detector configuration: without air between them ~91% of detected muons produce coincidences ~2.5% of muons give energy deposits under 3 MeV in coincidence spectra ratio of muons below and above the peak energy: ~0.064 in coincidence spectra This ratio is in quite good agreement with experimental data Detector configuration: 95 cm air between them only ~16% of detected muons produce coincidences This reduction is in good agreement with experimental data

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 RESULTS: Canfranc Angular distribution: I α cos 3.6 , corresponding to a depth of ~850 m of standard rock C. T. Stockel, J. Phys. A (Gen. Phys.) 1969, vol. 2 p. 639 Energy spectrum: sampled from Lipari distribution for the Canfranc depth, mean energy 216 GeV P. Lipari and T. Stanev, Phys. Rev. D 44 (1991) 3543

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 RESULTS: Canfranc Angular distribution: I α cos 3.6 , corresponding to a depth of ~850 m of standard rock C. T. Stockel, J. Phys. A (Gen. Phys.) 1969, vol. 2 p. 639 Energy spectrum: sampled from Lipari distribution for the Canfranc depth, mean energy 216 GeV P. Lipari and T. Stanev, Phys. Rev. D 44 (1991) 3543 Detector configuration: 1 cm air between them

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Registered energy spectra in top and bottom detectors energy (MeV)

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 RESULTS: Canfranc Angular distribution: I α cos 3.6 , corresponding to a depth of ~850 m of standard rock C. T. Stockel, J. Phys. A (Gen. Phys.) 1969, vol. 2 p. 639 Energy spectrum: sampled from Lipari distribution for the Canfranc depth, mean energy 216 GeV P. Lipari and T. Stanev, Phys. Rev. D 44 (1991) 3543 Detector configuration: 1 cm air between them ~92% of detected muons produce coincidences ~2% of muons give energy deposits under 3 MeV in coincidence spectra ratio of muons below and above the peak: ~0.058 in coincidence spectra This ratio is lower than in preliminary experimental data: to be understood

Design of specific codes

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Zeplin III Its performance have been studied using an end-to-end simulation tool based on G4 code To appear in Astroparticle Phys.

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 ZEPLIN-III Software It models the instrument response to radioactive backgrounds and calibration sources –Generation –Ray tracing and detection –Processing by data acquisition electronics The package builds upon previous G4 advanced example “Underground Physics” by A. Howard and H. Araújo.

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 S1 and S2 energy spectra in the inner 8 kg from collimated 57Co source located above the detector. S2 (shaded) is scaled down by a factor of The contribution of the individual energies (122.1 keV and keV) is also shown. Calibration

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Discrimination power S2/S1 distributions for electrons (upper population) and nuclear recoils (lower population). The thick lines represent the boundaries for a given -ray discrimination efficiency.

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 With a WIMP-nucleon cross-section sensitivity of ~ 5 × 10−9 ZEPLIN-III would compete favourably with much larger targets and more expensive technologies being considered around the world. Results

Activities and news

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Reports and presentations Technical report on WP1 included in the JRA1 annual report and presented in the Third ILIAS General Meeting (Gran Sasso, 29 February 2006)

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Publications A. Tang et al, Muon Simulations for Super-Kaiokande, KamLAND and CHOOZ, hep-ph/ H. Araújo et al., The ZEPLIN-III dark matter detector: performance study using an end-to-end simulation tool, to appear in Astroparticle Phys.

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 Letter to G4 team In collaboration with the MaGe group –Long-standing bugs have gone unfixed: the Inelastic/ CrossSection/ 32_70|72|73|74|76_Ge have been removed Bug 799 describes an inelastic interaction between a proton and an alpha in which 55 MeV goes "missing" Apparent non-generation of residuals for Ge(n,2n) reactions, which leads to discrepancies in the statistics of inelastic recoils … –We ask them to change the “priority code” of our problems offering them our help.

G. Luzón, JRA1 Meeting, Zaragoza,10-11 June 2006 News Released of G4 8.1 (June 2006). Changes: –New data G4EMLOW 4.0 –Old data does not reproduce detection in gas at atomic shell edges (Rob Veenhof) (¿new?) G4NDL 3.9 –Added data for Antimony, Hafnium, Technetium, Samarium, Neodymium and Gadolinium. –Updated inelastic data for 17_nat_Chlorine, 28_62_Nickel and removed data for 32_70/2/3/4/6_Germanium.