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Dark Matter Search with Stilbene Scintillator

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constellation Cygnus. (R.A. 21h12.0', Dec 48.19 ) WIMP ... ( Cygnus )and the galactic center ( Sagittarius ). Set the crystals on the. driving system like ... – PowerPoint PPT presentation

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Title: Dark Matter Search with Stilbene Scintillator


1
Dark Matter Search with Stilbene Scintillator
  • 9th ICEPP Symposium in Hakuba
  • 20 Feb 2003
  • Hiroyuki Sekiya
  • University of Tokyo

2
Dark Matter in the Universe
Flat Universe O OM O? 1
3
Results of WMAP
2/12 Asahi.com
4
COBE WMAP
Accurate measurements of CBR anisotropies reveals
Otot 1
O? 0.73 OM 0.27
Obaryonic 0.04 Onon baryonic 0.23
5
Neutralino as Dark Matter
Non Baryonic Cold Dark Matter Candidate
  • DM Axion ( KSVZ, DFSZ )
  • SUSY WIMPs ( LSP neutralino )

Leading candidate
Neutralino
Lowest mass, linear superposition of Photino,
zino, higgsino
Various implementation of MSSM leads to various
Mass window GeV lt lt TeV
6
DM Neutralino Search
  • Looking for antiprotons, positrons, gamma
    raysproduced by WIMP annihilation in the
    GALACTIC HALO.

BESS, GLAST, ISS,
  • Looking for high energy neutrinos as final
    products of WIMP annihilation in the celestial
    bodies (EARTH, SUN).

SK, AMANDA, MACRO,
  • Measuring the nuclear recoil produced by the
    elastic scattering of WIMP by the DETECTOR nuclei.

Direct Search
DAMA, CDMS, UKDMC, TOKYO,
7
Signal of WIMPs
Earth motion through the galactic halo produce
asymmetries distinctive of WIMPs.
  • Earth orbital motion around
  • the Sun (15 km/s)

Annual modulation of the WIMP interaction rate.
8
Directional Signal
  • Earth motion around the
  • Galactic Center (230 km /s)

Directional asymmetry of the recoil nucleus.
WIMP halo manifests as WIMP wind with halo model
dependent directional signature.
isothermal halo
  • Directional sensitivity is indispensable for
    identifying Galactic WIMP signature.
  • Potential for distinguishing different halo model.

WIMP astronomy
9
Organic Crystal Scintillator
Scintillation efficiency depends on direction of
nuclear recoils with respect to crystal axes.
anthracene
stilbene
monoclinic system
Interesting recoil energy region ( below 100 keV
) had not been investigated.
10
Carbon Recoils in Stilbene
Recoil energies of protons given by WIMPs are
too small!
We had measured scintillation efficiency of
Carbon recoils in a stilbene single crystal.
  • Light yield 30 of NaI
  • ?max 410 nm
  • Decay time 5 ns

2cm x 2cm x 2cm Amcrys-H _at_Ukraine
11
Calibration with Neutrons
?N
Recoil energy ER Recoil angle ?N
?n
neutron
target crystal
are uniquely determined.
neutron counter
Evisible
  • Quenching Factor (ER, ?N)

ER
Performed at 3.2 MV Pelletron accelerator
(??? ???????? ???)
  • Pulsed proton beam (2 MHz 1.5ns width)
  • Li(p,n) Be (Q -1.6MeV) reaction

7
8
12
A Birds Eye View
13
Li Target
14
The Detectors
15
Results
252
  • Cf run was also performed.
  • Depends on
  • the angle with
  • respect to
  • c axis.
  • Variation of
  • the scintillation
  • response is
  • about 7.

16
Application to Dark Matter Detector
Scattered WIMP
VE
Recoil directions show a peak at ? 180
WIMP wind
?
Nuclear Recoil
Light outputs should be
  • minimum at c // VE.
  • maximum at c - VE.

See the difference in light output spectra.
17
Possible Measurements 1
Setting on the ground
WIMP wind
6to c
The earth moves toward constellation Cygnus.
(R.A. 21h12.0, Dec 48.19)
36
42
VE
42to the earths axis
78to c
WIMP incident angle with respect to c axis
modulates 72over 12 sidereal hours at
N36(KAMIOKA)
18
Possible Measurements 2
c axis maintained to the direction of the
galactic rotation ( Cygnus )and the galactic
center ( Sagittarius ).
Set the crystals on the driving system like
19
Expected Spectra
Assuming spherical isothermal halo.
  • Resemble the annual
  • modulation of the
  • count rate.
  • The measurements
  • can be achieved
  • more robustly.
  • 100 kg 100 days!
  • (Zero BG)

?00.3 GeV/cm, v0220 km/s, vE232km/s
20
Ability to set an upper limit
Assuming 1 counts/keV/day/kg
Directional sensitivity also has the advantage of
exclusion the parameter space.
  • More important is
  • the sensitivity for an actual positive WIMP
    detection!

21
Plans
  • Stilbene 5cmf x 5cm (100g) x 3
  • Low background PMTs R8778 MOD-ASSY
  • Background measurement
  • _at_Kamioka underground
    laboratory
  • Settings on the turntable or on the ground??

Stronger directional dependency is favorable!
naphthalene
22
Naphthalene
50 anisotropy
  • Yield 12 of NaI
  • ?max 348 nm
  • Decay time 96 ns

Available from Ukraine
Z. phys. 165 (1961) 1
23
Summary
  • The variation of the quenching factor of the
    stilbene crystal is 7.
  • That could produce the possible dark matter
    signal.
  • Pilot run with 300g stilbene will be performed at
    Kamioka underground lab.
  • Naphthalene crystals which show more anisotropic
    scintillation response will be ready.
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