MIcro-tpc Matrix of Cells of He3

Slides:



Advertisements
Similar presentations
MACHe3: Prototype of a bolometric detector based on superfluid 3 He for the search of non-baryonic Dark Matter C. Winkelmann J. Elbs E. Collin Yu. Bunkov.
Advertisements

Beijing, August 18, 2004 P. Colas - Micromegas for HEP 1 Recent developments of Micromegas detectors for High Energy Physics Principle of operationPrinciple.
Comprehensive Analysis on the Light Higgs Scenario in the Framework of Non-Universal Higgs Mass Model M. Asano (Tohoku Univ.) M. Senami (Kyoto Univ.) H.
Neutral Particles. Neutrons Neutrons are like neutral protons. –Mass is 1% larger –Interacts strongly Neutral charge complicates detection Neutron lifetime.
Susy05, Durham 21 st July1 Split SUSY at Colliders Peter Richardson Durham University Work done in collaboration with W. Kilian, T. Plehn and E. Schmidt,
Looking for SUSY Dark Matter with ATLAS The Story of a Lonely Lepton Nadia Davidson Supervisor: Elisabetta Barberio.
Paris 22/4 UED Albert De Roeck (CERN) 1 Identifying Universal Extra Dimensions at CLIC  Minimal UED model  CLIC experimentation  UED signals & Measurements.
Proportional Light in a Dual Phase Xenon Chamber
P. Gorodetzky PCC-Collège de France XIII ISVHECRI Pylos September NOSTOS a new low energy neutrino experiment Detect low energy neutrinos from.
SUSY Dark Matter Collider – direct – indirect search bridge. Sabine Kraml Laboratoire de Physique Subatomique et de Cosmologie Grenoble, France ● 43. Rencontres.
I. Giomataris Large TPCs for low energy rare event detection NNN05 Next Generation of Nucleon Decay and Neutrino Detectors 7-9 April 2005 Aussois, Savoie,
Measurement of gas gain fluctuations M. Chefdeville, LAPP, Annecy TPC Jamboree, Orsay, 12/05/2009.
I. Giomataris NOSTOS Neutrino studies with a tritium source Neutrino Oscillations with triton neutrinos The concept of a spherical TPC Measurement of.
A Direction Sensitive Dark Matter Detector
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.
Masato Yamanaka (Saitama University) collaborators Shigeki Matsumoto Joe Sato Masato Senami arXiv: [hep-ph]Phys.Lett.B647: and Relic abundance.
LRT2004 Sudbury, December 2004Igor G. Irastorza, CEA Saclay NOSTOS: a spherical TPC to detect low energy neutrinos Igor G. Irastorza CEA/Saclay NOSTOS.
DARK MATTER CANDIDATES Cody Carr, Minh Nguyen December 9 th, 2014.
Neutron scattering systems for calibration of dark matter search and low-energy neutrino detectors A.Bondar, A.Buzulutskov, A.Burdakov, E.Grishnjaev, A.Dolgov,
Dark matter in split extended supersymmetry in collaboration with M. Quiros (IFAE) and P. Ullio (SISSA/ISAS) Alessio Provenza (SISSA/ISAS) Newport Beach.
Stanford, Mar 21, 2005P. Colas - Micromegas TPC1 Results from a Micromegas TPC Cosmic Ray Test Berkeley-Orsay-Saclay Progress Report Reminder: the Berkeley-Orsay-
Geant4 Simulation of Neutrons interaction with GEM-foil and gas Gabriele Croci, Matteo Alfonsi, Serge Duarte Pinto, Leszek Ropelewski, Marco Villa (CERN)
HEP-Aachen/16-24 July 2003 L.Chabert IPNL Latest results ot the EDELWEISS experiment : L.Chabert Institut de Physique Nucléaire de Lyon ● CEA-Saclay DAPNIA/DRECAM.
NEWAGE Hironobu Nishimura ( Kyoto University) K. Miuchi T. Tanimori, H. Kubo, S. Kabuki, A. Takada, K. Hattori, K. Ueno, S. Kurosawa, T.Ida, S.Iwaki A.
IDM 2000, September, 2000 Joakim Edsjö, Paolo Gondolo, Joakim Edsjö, Lars Bergström, Piero Ullio and Edward A. Baltz.
Digital primary electron counting: W, Fano Factor, Polya vs Exponential M. Chefdeville, NIKHEF, Amsterdam RD51, Paris, October 2008.
Underground Laboratories and Low Background Experiments Pia Loaiza Laboratoire Souterrain de Modane Bordeaux, March 16 th, 2006.
A Lightning Review of Dark Matter R.L. Cooper
I. Giomataris NOSTOS a new low energy neutrino experiment Detect low energy neutrinos from a tritium source using a spherical gaseous TPC Study neutrino.
WIMP search Result from KIMS experiments Kim Seung Cheon (DMRC,SNU)
? At Yangyang beach, looking for something in the swamp of particles and waves. 1 The recent results from KIMS Seung Cheon Kim (Seoul National University)
NEMO3 experiment: results G. Broudin-Bay LAL (CNRS/ Université Paris-Sud 11) for the NEMO collaboration Moriond EW conference La Thuile, March 2008.
Goddard February 2003 R.Bellazzini - INFN Pisa A new X-Ray Polarimeter based on the photoelectric effect for Black Holes and Neutron Stars Astrophysics.
D. Santos Large TPC Workshop – LPNHE 21/12/2004 Daniel Santos & Emmanuel Moulin Laboratoire de Physique Subatomique et de Cosmologie Grenoble MIMAC-He3.
Kamioka Kyoto We feel WIMP wind on the earth NEWAGE Direction-sensitive direct dark matter search with μ-TPC * 1.Dark.
DARK MATTER SEARCH Carter Hall, University of Maryland.
Ray Bunker (UCSB) – APS – April 17 th, 2005 CDMS SUF Run 21 Low-Mass WIMP Search Ray Bunker Jan 17 th -DOE UCSB Review.
Neutrons in gases Mary Tsagri CERN PH / SFT Tuesday, 23 February 2010 RD51 mini week.
I. Giomataris, CEA-Irfu-France
J. KalinowskiDark matter in U(1) extended SUSY1 Dark matter in the U(1) extended supersymmetric model Jan Kalinowski S.Y. Choi, H.E. Haber and P.M. Zerwas,
Identification of Dark Matter with Directional Detection Julien Billard, F. Mayet, D. Santos, O. Guillaudin, C. Grignon (MIMAC Collaboration) Laboratoire.
Elba -- June 7, 2006 Collaboration Meeting 1 CDF Melisa Rossi -- Udine University On behalf of the Multilepton Group CDF Collaboration Meeting.
Energy resolution results for Microbulk MICROMEGAS at high energy and pressure. Alfredo Tomás Alquézar Universidad de Zaragoza on behalf of the collaboration.
Slides for IG NewS : GG – analysis june juin 2016 Spherical detector: recent developments I. Giomataris, CEA-Irfu-France Spherical detector at.
A portable and directional fast neutron detector MIMAC FASTn Nadine Sauzet Laboratoire de Physique Subatomique et de Cosmologie (LPSC-Grenoble) (UJF Grenoble.
From Edelweiss I to Edelweiss II
Low Energy Gamma Rejection
MIMAC MIcro-tpc MAtrix of Chambers ( 3He + CF4) A Large TPC for non baryonic Dark Matter search Daniel Santos Laboratoire de Physique Subatomique et.
Keiko Nagao (National Institute of Technology, Niihama College, Japan)
Direct Search for Dark Matter with XENON100
Elettra Sincrotrone Trieste
Dark Matter Search With an Ultra-low Threshold Germanium Detector proposed by Tsinghua University Seoul National University Academia Sinica Qian Yue.
An interesting candidate?
UK Dark Matter Collaboration
The Heidelberg Dark Matter Search Experiment
Development of Hard X-ray Detector with GEM
Irina Bavykina, MPI f. Physik
XAX Can DM and DBD detectors combined?
Non-Baryonic Dark Matter: From the CMB and axial direct detection
Dark Matter Phenomenology of the GUT-less CMSSM
John Kelley IceCube Journal Club 27 February 2008
The MICROMEGAS detector in CAST
Neutral and charged Higgsino as carriers of residual SUSY effects.
Supersymmetric Dark Matter
LUX: Shedding Light on Dark Matter
Detecting WIMPs using Au-DNA Microarrays
Yue, Yongpyung, Korea Prospects of Dark Matter Search with an Ultra-Low Threshold Germanium Detector Yue, Yongpyung, Korea
SUSY SEARCHES WITH ATLAS
The Estimated Limits For A 5g LE-Ge Detector
Dark Matter Detection,Models and Constraints
Presentation transcript:

MIcro-tpc Matrix of Cells of He3 MIMAC-He3 MIcro-tpc Matrix of Cells of He3 A new He3 detector for non-baryonic dark matter search Daniel Santos & Emmanuel Moulin Laboratoire de Physique Subatomique et de Cosmologie Grenoble

(MIcroTPC MAtrix of Chambers MIMAC-He3: (MIcroTPC MAtrix of Chambers Of Helium 3) LPSC (Grenoble) : G. Bosson, V. Comparat, G.Duhamel, J. Genevey, R. Guglielmini, O. Guillaudin, T. Lamy, E. Moulin, J.A. Pinston, D. Santos, P. Sortais Dapnia-Saclay: S. Aune, I. Giomataris CPPM (Marseille): J. Bustó, C. Cerna CdF (Paris): J. Dolbeau, Ph. Gorodetzky, T. Patzak, P. Salin GPS (Paris) + LSBB (Rustrel): G. Waysand

of non-baryonic dark matter 3He for axial detection of non-baryonic dark matter spin 1/2 nucleus  axial interaction with high signal/noise ratio : energy range ~ 2-5 keV sensitive to M (WIMP) > 5 GeV neutron capture signature: n + 3He  p + 1H + 764 keV very low sensivity to -rays no intrinsic X-rays

Recoil energy range for a 3He detector Energy threshold for 3He detector: 1keV 194.1 keV 117.8 keV 4.8 keV  It must be convoluted by the QF(E) !

Background in the cell without source 57Co source in MACHe3 (LPSC+CRTBT) E. Moulin, C. Winkelmann, J.Macias-Perez, Y. Bunkov, H. Godfrin, D. Santos,( to be published) Background in the cell without source 5.5 keV 7.3 keV 13.6 keV 14.4 keV 21.7 keV 27.9 keV 12.8 keV

Expected electron spectrum from 57Co source (in a volume with 0.0013 mol) conversion electrons : 7.3 keV (K shell) 13.6 keV (L shell) 14.4 keV (M shell) auger electrons : 5.5 keV (K ~ 35.2%) 0.6-1.8 keV (L ~ 0.6%) pile-up : 12.8 keV (ecK + eAK) 14.2-15.4 keV (ecL + eAL) 21.7 keV (gold eAL + ecK) 27.9 keV (gold eAL + ecL) 25 m thick gold foil 100 m thick copper box from 122 keV  interaction in gold

(MIcroTPC MAtrix of Cells of He 3) MIMAC-He3: (MIcroTPC MAtrix of Cells of He 3) spatial High temporal resolution energetic recoil track projection energy threshold < 1 keV electron/recoil discrimination

Distribution of energy depositions from 6.4 keV X-rays Argon escape peak (operating gas: Ar/isobutane 95/5) X-ray detection threshold: 0.6 keV CAST collaboration

Low energy spectrum from Micromegas in CAST Fe escape Cu Ar escape Fe

Pixels (anode) in CAST Pitch: 350 μm

Range of recoils (He3) vs. Recoil Energy (SRIM-2003)

Diffusion & Charge collection D~ 200μm √ L[cm] => D~800 μm => 30 pixels ( L ~15 cm and pixels~250 μm ) He => 41 eV/ pair (e-ion) => 25 pairs/keV With a gain G~3000 => 75000 e-/keV over 30 pixels => threshold ~ 2500e- “gassiplex” does the job…but we’ll try to do better !

Drift velocity vs. Pressure

a/b ratio simulation (Geant 4) a: major axis b: minor axis of the trajectory projection Isotropically emitted at 10 cm of the anode E. Moulin (LPSC)

Two-elastic interactions distance in He3 (2 atm) for a 8 keV neutron

Elastic-capture distance distribution in He3(2 atm) for a 8 keV neutron

Recoil Source : 3He2+ in the keV range

Source + filter : 3He2+ ( 6 to 50 KV) Magnétron 300W

Recoil energy distribution after a polypropilene foil of 0 Recoil energy distribution after a polypropilene foil of 0.44μg/cm2 for acceleration energies of 45 and 50 keV

The lightest neutralino lowest mass linear superposition of superpartners of the gauge and higgs bosons: ~ ~ ~ ~ ~ = a1B + a2W3 + a3H1 + a4H2 neutral, colorless, only weak interaction stable with R-parity conservation non-relativistic at decoupling  CDM relic density can be compatible with cosmological observations

Light neutralinos ? (1) in universal models: M1 , M2 gaugino mass unification at MGUT  standard relation at EW scale (after RGE): M1 = 5/3 tan2 W  0.5 M2 -   M1,M2 : m ~ M1 neutralino and chargino m± ~ M2 mass matrix: -   M1,M2 : m ~  m± ~  LEP2 constraint on ± mass: m± > 103 GeV  M2,  103 GeV  m  50 GeV

Light neutralinos ? (2) in non-universal models: masses M1 , M2 non unified at MGUT M1  M2/2 at EW scale  LEP2 constraint not valid on neutralino mass M1 = R M2 , R free parameter (constraint at EW scale relaxed) constraint on the neutralino mass in non-universal models: m  6 GeV A. Bottino et al, PRD69:037302,2004 G. Belanger et al, JHEP0403:012,2004 … …

Axial cross section 3He- and rate in 10 kg 3He detector M  6 GeV   0.3 Exclusion curve for 0.01 day-1 background

Complementarity with scalar detection CDMS 2004 Edelweiss 2003 Rate  0.01 day-1 Rate < 0.01 day-1

Summary We have learned a lot with Mache3 (on simulations and interactions with muons, gammas, electrons and neutrons) MIMAC-He3 prototype designed He3 source for QF measurements designed and under construction New electronic design in progress First results of the prototype for the next IDM !! Complementarities with the scalar experiments (Ge, Xe,..)