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DMTPC: A Dark Matter Detector with Directional Sensitivity Shawn Henderson on behalf of the DMTPC Collaboration TeVPA 2009 July 12, 2009
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DMTPC: A Dark Matter Detector with Directional Sensitivity

Shawn Henderson

on behalf of the DMTPC Collaboration

TeVPA 2009 July 12, 2009

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Dark Matter Time Projection Chamber

Boston UniversityS. Ahlen (PI), A. Inglis, H. Tomita

Brandeis UniversityA. Dushkin, S. Goyal, F. Golub, B. N. Skvorodnev, H. Wellenstein (PI)

Massachusetts Institute of TechnologyP. Fisher (PI), G. Sciolla, R. Yamamoto, D. Dujmic, R. Vanderspek, J. Battat, J. Monroe, S. Henderson, A. Kaboth, J. Lopez, T. Caldwell,

A. Lee, T. Sahin, I. Wolfe, H. Yegorian

Detector PapersD. Dujmic et al. [DMTPC] NIMA 584 (2007)A. Kaboth et al. [DMTPC] NIMA 592 (2008)D. Dujmic et al. [DMTPC] Astropart. Phys 30 (2008)T. Caldwell et al. [DMTPC] arXiv:0905.2549 (2009)

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Time Projection Chamber

Side View

GND

+V

-V

Drift 5kV

20 cm

Amplify0.7 kV0.5 mm

Low pressure gas

CF4

~0.1 atm

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GND

+V

-V

Drift 5kV

20 cm

Amplify0.7 kV0.5 mm

Recoil(few mm long)

ER

χ

χ

PMT PMTCamera

photons electrons 9

GND

+V

-V

Drift 5kV

20 cm

Amplify0.7 kV0.5 mm

χ

χPMT PMTCamera

electrons 10

GND

+V

-V

Drift 5kV

20 cm

Amplify0.7 kV0.5 mm

χ

χPMT PMTCamera

photons electrons 11

15.5

cm

15.5 cm

We Measure E

recoil from total light

Direction of track

Sense of direction

For nuclear recoils,

dE/dx DECREASES

along track

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θ

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Reconstructing the Sense

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Particle Identification

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DMTPC 10-liter detector

Dual TPC

Mesh-amplification region (2-D readout)

10-L fiducial volume 20 cm drift 3g at 75 Torr

Charge readout

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BackgroundStudy

Detector stability

Surface (basement) lab Remote operation5-second exposures (shutter-less) Without trigger - every image saved Daily gas refill70% live time 1% gain stability/day 6 and 3 week long datasets 20

( )Energy VS Range No Cuts

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Alphas

Worms

Pro

ject

ed R

ange

(mm

)

α Backgrounds

Some are contained in the view field; cut on energy VS range

Little impact on detector efficiency

Most likely from U, Th chains and Rn

Particularly large background because detector materials were not chosen for radiopurity

Most come from the sides and can be identified by edge crossing

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WormsAny event with one or a few localized very bright pixels

CCD-specific background

Probable origin: n's, 's, radioactivity in CCDμ

Rate ~ 7-10 mHz

Cut on high energy densities

Better software/hardware solutions are on the way

Going underground could help

μ

?

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Analysis energy range: 110-200 keV Measured # BG events: 7 Expected # BG events: 21 Detector live time: 10.8 days Active detector mass: 0.0033 kgThis exposure: 0.036 kg*days

After Cuts

LimitCalculation

PRELIMINARY

PRELIMINARY

PRELIMINARY

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Expected Sensitivity

DMTPC10Lsurface estimate for 7 observed events, 20 bkg expected, 44g-day,E>110keV

PRELIMINARY

KIMS (2007)

COUPP (2008)

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W aste I solation P ilot PlantLow radon level < 7 Bq/m3 1600m water equivalent < 1 event/yr neutron background

Site ofDMTPC

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DMTPC 10-liter detector SD-proton,

50 keV threshold, 365 days

underground @ 100 torr

KIMS (2007)COUPP (2008)

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Looking Ahead: A 1-m3 DetectorG. Sciolla arXiv:0805.2431

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Heavier Targets/Inelastic DM?

D. Finkbeiner arXiv:0906.0002

Heavier targets than CF4 are sensitive to inelastic dark

matter models

Could reconcile DAMA and other SI results

Signal is VERY directional

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