status r&d of directional dm search with nuclear...
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Status R&D of directional DM search with Nuclear Emulsion
Tatsuhiro Naka
Mitsuhiro Nakamura, Toshiyuki Nakano, Osam Sato, Kimio NiwaNagoya University Fundamental Particle Lab.
Yuzuru TawaraNagoya University, Ecotopia Lab.
Kenichi KugeChiba University
Hiroaki Misawa, Kose UenoHokkaido University
Masashi IwasakiKyoto Kogei-Seni University
CYGNUS2009 09.June.11-13 @MIT,USA
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600keV Kr 3D image of optical microscope
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Test of automatic readout of expanded track
-Neutron source : DD neutron (2.5MeV)
Test of automatic readout of expanded track
Neutron Intensity: (2~3)×107n/secExposure time :9.5h
4μm 4μm 2μm
Cross section image of Expanded track (original range<1μm)
Such tracks were been object of automatic scanning R&D.
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UTS
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•Take 16 tomographic images by microscope.
•Shift images aiming an angle
•Sum up all images to examine coincidence
•Appear tracks as peaks
Repeat on angle space
Track recognition algorithm
Number of hit in 16 tomographic image : pulse height (ph)
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Ex image)
3grain track (4.56μm range)
Scanning R&D status for NIT
data
・light field (transmission) -> dark field・10μm thick scan per 1view・ checked scanning data by manual check every 5 view scanning⇒recognize the track
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track up ph:100099down ph:130250
fog ph:100097
Ph>7 Ph>8
Ph>9 Ph>10
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Noise
Tracknoise
Ph>9 cut may be good.
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ResultTracking efficiencyscanning data →confirmed by manual check
ph>10 39ph 9 15ph 8 2
Number of found track 56
ph>9 cut 86+-11%
ph>10 cut 81+-13%
Tracking efficiency
5view scanning area : 3450μm2 ×10μm thick
⇒scanning volume 1.9×106μm3
small grain
large angleThe tracks that couldn’t detect by track selector [9 track ]
・improvement of image processing ⇒ improvement of measurement accuracy of angle ・improvement of development treatment and sensitivity of NIT
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Background rejection by development treatment
Generation of latent image is needed for AgBr that particle
penetrated is developed.Possibility of generation of latent image depends on dE/dx of particle.
MIP
In the case of nuclear recoil track and BG track..-Difference is very large of dE/dx between nuclear recoil and BG track(γ, e)-dE/dx process of nuclear recoil is Lindhard-Sharf region and nuclear stopping power diminant.
You can expect there is difference of generated mechanism of latent image.
Ex.) α ray electron(MIP)
20μm
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Separation of dE/dx between Nuclear and electron stopping power
Nuclear Stopping PowerIt is expected that Lattice Defect is generated into the AgBr crystal.
Electron Stopping PowerIt is expected as normal ionization. Then latent image is generated on the surface of AgBr crystal.
AgBr crystal
Latent Image
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Background track discrimination
Nuclear recoil track Background track (γ, β)
Ionization dominantNuclear stooping power dominant
There may be difference between nuclear recoil and background track from the place of generated latent image and size of latent image.
By preceding development of internal latent image, signal/BG efficiency may be improved.
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Recognize of the place of latent image
Dissolution Physics Development Physics Development
This can develop while AgBr is dissolved.
internal latent image is able to be developed.
Only surface latent image is developed because AgBr is not dissolved.
αray test
Grain density < 1.0grain/μm Grain density = 2.5grain/μmDistinguish track is difficult.
10μm10μm
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Kr test
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0 5 10 15 20 25
Kr
sign
al d
en
sity
[/μ
m^2
]
MF dev time [min] (PD time: 5min)
MF->PDとPD->APD現像比較(MF time parameter: PD 5min)
HA sensitized PD->APD
Both surface and internal
Only surface
At least, Internal latent image is generated for nuclear recoil track and only surface latent image is generated for the track that ionization process dominant.
From now on, I will measure the background rejection ratio for this method.
(low alpha sensitivity)
(lhigh alpha sensitivity)
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600 650 700 750 800
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
R
wavelength (nm)
Nuclear recoil
Noise
No wavelength shift
FDTD simulation
parallel
perpendicular
20 nm gap L & T mode
4 6 8 10 12 14 16 18 20 22
640
660
680
700
720
740
760
780
800
820
m
ax (
nm
)
gap (nm)
Further large volume readout plan
Condition: 100nm Ag into the gelatine
With Pro. Misawa and Dr.Ueno @ Hokkaido Univ.
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200nm
200nm
Normal development treatment
Grains grow up as filament
Dissolution Physics development
Grains grow up as sphere.
200nm
200nm
This can’t use because grain is anisotropic.
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Concept of the next generation emulsion readoutOptics Technology transfer from photo lithographic system
Imager Mosaic CMOS imager (multiple 4k2k imager)
Effective FOV 21.55×20.9 mm2×0.28 (1450×1100mm2×80)
Effective pixel size 0.35-0.5mm
Repetition time 1.5 sec /16depth/fullarea (4 steps/view)
Max. scan speed 12000cm2/h (150cm2/h×80)
20mm
Current system : 0.2mm
FOV comparison New vs. Present
IC-Stepper (Lithographic system)
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第9回X線結像光学シンポジウム2007.11.2@Nagoya
19
Example of the system
Imaging fluorescence X-ray
microscope
X-ray specimen
CCD
Multilayer coated Wolter I
Mirror
with Prof. Tawara
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X-ray microscope for Dark matterparticle search
X-ray Generat
or
Condenser mirror
Objective mirror
Optical microsc
ope
Specimens (Nuclearemulsion
X-raymicroscope
Specimensscannningsysytem
PC control
CCDcontrol
X-ray CCD
System Plan
Large sampleOptical alignmentFast processing
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Conclusion
• Automatic scanning system
- developed 100 times speed track selector
- developed readout system of short range track
• Development treatment for background rejection
- using the difference of generated process of latent image
- possibility of head-tail discrimination
• New tracking system
- using the wavelength shift by direction of polarized light
• Xray microscope