PSD 7, Liverpool, September 2005 Position Sensitive Detectors for Astroparticle Physics Timothy J Sumner Imperial College London.

Slides:



Advertisements
Similar presentations
Trigger issues for KM3NeT the large scale underwater neutrino telescope the project objectives design aspects from the KM3NeT TDR trigger issues outlook.
Advertisements

ICECUBE & Limits on neutrino emission from gamma-ray bursts IceCube collaboration Journal Club talk Alex Fry.
The MAGIC telescope and the GLAST satellite La Palma, Roque de los Muchacos (28.8° latitude ° longitude, 2225 m asl) INAUGURATION: 10/10/2003 LAT.
Cherenkov Detectors. Index of Refraction When light passes through matter its velocity decreases. –Index of refraction n. The index depends on the medium.
Detection of Gamma-Rays and Energetic Particles
Gamma-Ray Astronomy Call no Assoc. Prof. Markus Böttcher Clippinger # 339 Phone:
Dark Matter Searches with Dual-Phase Noble Liquid Detectors Imperial HEP 1st Year Talks ‒ Evidence and Motivation ‒ Dual-phase Noble Liquid Detectors ‒
Report from Low Background Experiments Geant4 Collaboration Workshop 10 September 2012 Dennis Wright (SLAC)
The Pierre Auger Observatory Nicolás G. Busca Fermilab-University of Chicago FNAL User’s Meeting, May 2006.
March 13thXXXXth RENCONTRES DE MORIOND 1 The Alpha Magnetic Spectrometer on the International Space Station Carmen Palomares CIEMAT (Madrid) On behalf.
The Transient Universe: AY 250 Spring 2007 New High Energy Telescopes Geoff Bower.
The Telescope Array Low Energy Extension (TALE)‏ Pierre Sokolsky University of Utah.
Large Magellanic Cloud, 1987 (51.4 kparsec) SN 1987a after before 2006 Hubble.
The XENON Project A 1 tonne Liquid Xenon experiment for a sensitive Dark Matter Search Elena Aprile Columbia University.
The Highest Energy Cosmic Rays Two Large Air Shower Detectors
TAUP 2005: Zaragoza Observations of Ultra-high Energy Cosmic Rays Alan Watson University of Leeds Spokesperson for Pierre Auger Observatory
1 Gamma-Ray Astronomy with GLAST May 24, 2008 Toby Burnett WALTA meeting.
High Energy Detection. High Energy Spectrum High energy EM radiation:  (nm)E (eV) Soft x-rays X-rays K Soft gamma rays M Hard gamma.
GLAST Simulations Theodore E. Hierath Louisiana State University August 20, 2001.
The ANTARES Neutrino Telescope Mieke Bouwhuis 27/03/2006.
30 Ge & Si Crystals Arranged in verticals stacks of 6 called “towers” Shielding composed of lead, poly, and a muon veto not described. 7.6 cm diameter.
1 Tuning in to Nature’s Tevatrons Stella Bradbury, University of Leeds T e V  -ray Astronomy the atmospheric Cherenkov technique the Whipple 10m telescope.
The Project of Space Experiment with Wide Field Gamma-Ray Telescope (“GAMMASCOPE”) Skobeltsyn Institute of Nuclear Physics, Moscow State University.
Sampling Detectors for e Detection and Identification Adam Para, Fermilab NuFact02 Imperial College Interest de jour: what is sin 2 2  13  oscillations.
Design and status of the Pierre Auger Observatory J. C. Arteaga Velázquez 1, Rebeca López 2, R. Pelayo 1 and Arnulfo Zepeda 1 1 Departamento de Física,
Applications of Micro-TPC to Dark Matter Search 1. WIMP signatures 2. Performance of the Micro-TPC 3. WIMP-wind measurement 4. Future works 5. Conclusions.
Introduction to gamma-ray astronomy GLAST-Large Area Telescope Introduction to GLAST Science New way of studying astrophysics Schedule of GLAST project.
Wednesday, Feb. 14, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #6 Wednesday, Feb. 14, 2007 Dr. Jae Yu 1.Neutrino Oscillation Formalism 2.Neutrino.
Space-based Gamma-ray Astronomy Liz Hays (NASA Goddard Space Flight Center)
Future work Kamioka Kyoto We feel WIMP wind oh the earth NEWAGE ~ Direction Sensitive Direct Dark Matter Search ~ Kyoto University Hironobu Nishimura
SNO and the new SNOLAB SNO: Heavy Water Phase Complete Status of SNOLAB Future experiments at SNOLAB: (Dark Matter, Double beta, Solar, geo-, supernova.
Lepton - Photon 01 Francis Halzen the sky the sky > 10 GeV photon energy < cm wavelength > 10 8 TeV particles exist > 10 8 TeV particles exist Fly’s.
Humberto Salazar (FCFM-BUAP) for the Pierre Auger Collaboration, CTEQ- Fermilab School Lima, Peru, August 2012 Ultrahigh Cosmic Rays: The highest energy.
Observational techniques meeting #15
HAWC Science  Survey of 2  sr (half the sky) up to 100 TeV energies Probe knee in cosmic ray spectrum Identify sources of Galactic cosmic rays  Extended.
1 João Espadanal, Patricia Gonçalves, Mário Pimenta Santiago de Compostela 3 rd IDPASC school Auger LIP Group 3D simulation Of Extensive Air.
The Auger Observatory for High-Energy Cosmic Rays G.Matthiae University of Roma II and INFN For the Pierre Auger Collaboration The physics case Pierre.
PHY418 Particle Astrophysics
High Redshift Gamma-Ray Bursts observed by GLAST Abstract The Gamma-ray Large Area Space Telescope (GLAST) is the next generation satellite for high energy.
June 6, 2006 CALOR 2006 E. Hays University of Chicago / Argonne National Lab VERITAS Imaging Calorimetry at Very High Energies.
Pheno Symposium, University of Wisconsin-Madison, April 2008John Beacom, The Ohio State University Astroparticle Physics in the LHC Era John Beacom The.
Astroparticle physics with large neutrino detectors  Existing detectors  Physics motivation  Antares project  KM3NeT proposal M. de Jong.
NEMO3 experiment: results G. Broudin-Bay LAL (CNRS/ Université Paris-Sud 11) for the NEMO collaboration Moriond EW conference La Thuile, March 2008.
Kamioka Kyoto We feel WIMP wind on the earth NEWAGE Direction-sensitive direct dark matter search with μ-TPC * 1.Dark.
05/02/031 Next Generation Ground- based  -ray Telescopes Frank Krennrich April,
High Energy cosmic-Radiation Detection (HERD) Facility onboard China’s Space Station Shuang-Nan Zhang ( 张双南 ) Center for Particle Astrophysics.
Sources emitting gamma-rays observed in the MAGIC field of view Jelena-Kristina Željeznjak , Zagreb.
What we do know about cosmic rays at energies above eV? A.A.Petrukhin Contents 4 th Round Table, December , Introduction. 2. How these.
1 CEA mercredi 26 novembre 2007 Latest news from the Pierre Auger Observatory Nicolas G. Busca - APC - Paris 7.
1 Study of Data from the GLAST Balloon Prototype Based on a Geant4 Simulator Tsunefumi Mizuno February 22, Geant4 Work Shop The GLAST Satellite.
ZEPLIN III Position Sensitivity PSD7, 12 th to 17 th September 2005, Liverpool, UK Alexandre Lindote LIP - Coimbra, Portugal On behalf of the ZEPLIN/UKDM.
Second Workshop on large TPC for low energy rare event detection, Paris, December 21 st, 2004.
Fermi Gamma-ray Space Telescope Searches for Dark Matter Signals Workshop for Science Writers Introduction S. Ritz UCSC Physics Dept. and SCIPP On behalf.
Gamma-ray Large Area Space Telescope -France -Germany -Italy -Japan -Sweden -USA Energy Range 10 keV-300 GeV. GLAST : - An imaging gamma-ray telescope.
Bianca Keilhauer for the Pierre Auger Collaboration
Detecting the Directionality of Dark Matter via “Columnar Recombination” (CR) Technique An attractive, natural candidate for Dark Matter is the WIMP –
The Large High Altitude Air Shower Observatory LHAASO.
The end of the electromagnetic spectrum
Search for Neutrinoless Double Beta Decay with NEMO-3 Zornitza Daraktchieva University College London On behalf of the NEMO3 collaboration PANIC08, Eilat,
Alex Howard, Imperial College Slide 1 July 2 nd 2001 Underground Project UNDERGROUND PROJECT – Overview and Goals Alex Howard Imperial College, London.
WIMPs Direct Search with Dual Light-emitting Crystals Xilei Sun IHEP International Symposium on Neutrino Physics and Beyond
KM3NeT P.Kooijman Universities of Amsterdam & Utrecht for the consortium.
L.L.Ma for LHAASO collaboration Beijing China
Expectation of Cosmic Ray Energy Spectrum with LHAASO
Theoretical status of high energy cosmic rays and neutrinos
Particle Physics LECTURE 7
Pierre Auger Observatory Present and Future
Neutral Particles.
XAX Can DM and DBD detectors combined?
Presentation transcript:

PSD 7, Liverpool, September 2005 Position Sensitive Detectors for Astroparticle Physics Timothy J Sumner Imperial College London

PSD 7, Liverpool, September 2005 Position Sensitivity? Imaging –Sky maps – ν/γ rays/cr? –Directionality – dm Event Characterisation –Particle identification – dm/cr –Event location (within detector) – dm, ββ –Calibration Motion Sensing –Scientific signal – gw

PSD 7, Liverpool, September 2005 Astroparticle Physics Techniques span at least 20 orders of magnitude in energy and at least 5 different ‘event’ species!!!!

PSD 7, Liverpool, September 2005 Cosmic Ray Particles AMS Goals –Detection of primary cosmic-rays below the knee [~1GeV to 1TeV] –Good energy resolution –Good particle identification –Good statistics

PSD 7, Liverpool, September 2005 TR+EMC ΔR/R ~ 1.5% & ΔE/E ~ 3% TR+TOF+RICH

PSD 7, Liverpool, September 2005

Cosmic Ray Particles Auger –Observation of ultra-high energy cosmic rays (~10 20 eV)

PSD 7, Liverpool, September 2005 Pierre Auger Observatory Array of 1600 Surface Detectors (SD) –Cylindrical water Cherenkov tanks – 1.8m diameter x 1.5m tall viewed by 3 9” photomultipliers – on 1.5km grid. –Some ability to separate the electromagnetic and muon components. Array of 4 Fluorescence Detectors (FD) –Each FD has 6 telescopes with 3.5m mirrors and 440 PMTs in the focal plane. Each PMT is viewing 1.5 o diameter and the psf is ~ 0.5 o.

PSD 7, Liverpool, September 2005 ΔE/E ~ 25% +

PSD 7, Liverpool, September 2005 γ -Rays GLAST Goals –Identify and measure the flux of gamma-rays with energy 20MeV to 300GeV - LAT –Gamma-ray burst spectra between 10keV and 30MeV - GBM Gamma-ray Large Area Space Telescope

PSD 7, Liverpool, September 2005 e+e+ e–e–  Calorimeter Grid pair conversion telescope ACD [surrounds 4x4 array of TKR towers]

PSD 7, Liverpool, September 2005

γ -Rays HESS Goals –γ-ray astronomy above 100 GeV Technique –Air Cherenkov imaging

PSD 7, Liverpool, September 2005 γ -Rays Four identical telescopes –Davies-Cotton reflector with a flat-to-flat width of 13m and a focal length of 15 m. –mirror is segmented into 382 round (60 cm diameter) front-aluminized glass mirrors. –psf (<0.1 o ) across the whole 5 o field of view. –960 photomultiplier pixels subtending 0.16 o each, with Winston cone light concentrators.

PSD 7, Liverpool, September 2005 γ -Rays Background rejection (cosmic-rays!) requires good image recovery ΔE/E ~ 15%

PSD 7, Liverpool, September 2005 Seven identical telescopes –Davies-Cotton 12m with f/1.0. –mirror is segmented into 315 hexagonal elements. –psf (<0.1 o ) across the whole 3.5 o field of view. –499 photomultiplier pixels with 0.15 o spacing.

PSD 7, Liverpool, September 2005

Neutrinos ANTARES/AMANDA/BAIKAL/ICECUBE/ NEMO/NESTOR –Measure Cherenkov light from relativistic muon created by incoming neutrino. –Arrays of photodetectors widely spaced in medium (water/ice)

PSD 7, Liverpool, September TeV  6 PeV 

PSD 7, Liverpool, September 2005 [No] Neutrinos – Double beta decays –Measure total energy spectrum of decay electrons – EXO, Majorana, Cuore, Gerda, COBRA  good spectral resolution in large mass detectors –Measure tracks of decay electrons – Super- NEMO, COBRA?

PSD 7, Liverpool, September m 4 m B (25 G) 20 sectors Talk by Fulton In this session

PSD 7, Liverpool, September 2005 Direct Dark Matter Detection Requirements –Detect rare elastic nuclear recoil scattering events with ΔE~1=10keV with expected rates to /kg/day. –Reject backgrounds from electron recoils and neutron induced nuclear recoils. –Identify signatures of Galactic particles

PSD 7, Liverpool, September 2005 Direct Dark Matter Detection Techniques –Ionisation detectors – Germanium, DRIFT –Scintillators – CRESST I, ZEPLIN I –Phonons/Ionisation – CDMS, EDELEISS –Phonons/scintillation – CRESST II –Scintillation/Ionisation – ZEPLIN II/III, XENON –Others

PSD 7, Liverpool, September 2005 CDMS Position sensitivity defines fiducial volume

PSD 7, Liverpool, September 2005 ZEPLIN III Talk by Lindote – this session Poster by Solovov Position sensitivity defines fiducial volume and gives multi-site rejection

PSD 7, Liverpool, September 2005 Ionisation electrons rapidly attach to CS 2 molecules and these are drifted to read-out plane. High-field detaches electrons which are then detected in proportional gain mode using fine wire read-out Discrimination from ‘range’ vs energy Directionality from TPC (axis) + dE/dx (sense)  x, y from crossed read-out wire grids (DRIFT I and II)  z from event time duration as it crosses readout plane DRIFT Talk by Hiroyuki – this session Poster by Ghag/Plank

PSD 7, Liverpool, September 2005 Gravitational Wave Detection Requirements –Detect waves in space-time through strain induced in measurement systems, ΔL/L. –Measure temporal behaviour of ΔL/L –Unravel signals from all sources seen together.

PSD 7, Liverpool, September x m 1x m

PSD 7, Liverpool, September 2005 The ultimate psds!! Talk by Lockerbie – this session