the drift dark matter experiment

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The DRIFT Dark Matter Experiment Jennie Davies University of Sheffield (UK) IoP HEPP Conference - Dublin 21st - 23rd March 2005

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The DRIFT Dark Matter Experiment. Jennie Davies University of Sheffield (UK) IoP HEPP Conference - Dublin 21st - 23rd March 2005. Outline. Why? Dark matter Who? What? Where? When? How? The detector Recent developments. DRIFT... Why?. - PowerPoint PPT Presentation

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Page 1: The DRIFT Dark Matter Experiment

The DRIFTDark Matter Experiment

The DRIFTDark Matter Experiment

Jennie Davies University of Sheffield (UK)

IoP HEPP Conference - Dublin21st - 23rd March 2005

Jennie Davies University of Sheffield (UK)

IoP HEPP Conference - Dublin21st - 23rd March 2005

Page 2: The DRIFT Dark Matter Experiment

OutlineOutline

Why?

Dark matter

Who? What?

Where? When?

How?

The detector

Recent developments

Why?

Dark matter

Who? What?

Where? When?

How?

The detector

Recent developments

Page 3: The DRIFT Dark Matter Experiment

DRIFT... Why?DRIFT... Why?

To search for dark matter and identify a signal of galactic origin using directional information from nuclear recoil tracks.

To search for dark matter and identify a signal of galactic origin using directional information from nuclear recoil tracks.

Page 4: The DRIFT Dark Matter Experiment

DRIFT... Why?Dark Matter: The

Evidence

DRIFT... Why?Dark Matter: The

EvidenceObservational evidence

Rotational curves of galaxies

Gravitational lensing

Theoretical support

Supersymmetry

Observational evidence

Rotational curves of galaxies

Gravitational lensing

Theoretical support

Supersymmetry

Page 5: The DRIFT Dark Matter Experiment

DRIFT... Why?Dark Matter: The

Candidates

DRIFT... Why?Dark Matter: The

CandidatesBaryonic particle candidates

Non-baryonic particle candidates

Neutrinos

Weakly Interacting Massive Particles (WIMPs) - The stable LSP (neutralino)

Axions

Dark Energy

Baryonic particle candidates

Non-baryonic particle candidates

Neutrinos

Weakly Interacting Massive Particles (WIMPs) - The stable LSP (neutralino)

Axions

Dark Energy

Page 6: The DRIFT Dark Matter Experiment

DRIFT... Why?Dark Matter: WIMPs

DRIFT... Why?Dark Matter: WIMPs

Cold Dark Matter

Neutral

High mass (10 -1000 GeV)

Interact only very weakly

Postulated ‘WIMP Wind’

Daily fluctuations due to the Earth’s rotation

Cold Dark Matter

Neutral

High mass (10 -1000 GeV)

Interact only very weakly

Postulated ‘WIMP Wind’

Daily fluctuations due to the Earth’s rotation

Page 7: The DRIFT Dark Matter Experiment

DRIFT... Who?The DRIFT

Collaboration

DRIFT... Who?The DRIFT

CollaborationUK Dark Matter Collaboration

University of SheffieldUniversity of EdinburghImperial College, LondonRutherford Appleton Laboratory

Occidental College, Los Angeles, USATemple University, Philadelphia, USAUniversity of New Mexico, USAUniversity of Boston, USAUniversity of Thessaloniki, GreeceUniversity of Darmstadt, Germany

UK Dark Matter CollaborationUniversity of SheffieldUniversity of EdinburghImperial College, LondonRutherford Appleton Laboratory

Occidental College, Los Angeles, USATemple University, Philadelphia, USAUniversity of New Mexico, USAUniversity of Boston, USAUniversity of Thessaloniki, GreeceUniversity of Darmstadt, Germany

Page 8: The DRIFT Dark Matter Experiment

DRIFT... What?DRIFT... What?

DirectionalRecoilIdentificationFromTracks

DirectionalRecoilIdentificationFromTracks

Page 9: The DRIFT Dark Matter Experiment

DRIFT... What?DRIFT... What?

Negative Ion TimeProjection Chamber (NITPC)

Two back-to-back field cageswith a shared central cathode

Two readout planes - Multi-Wire Proportional Chambers (MWPCs)

Filled with CS2 gas at low pressure

Negative Ion TimeProjection Chamber (NITPC)

Two back-to-back field cageswith a shared central cathode

Two readout planes - Multi-Wire Proportional Chambers (MWPCs)

Filled with CS2 gas at low pressureMartoff et al. NIM-A 440 (2000) 355

Page 10: The DRIFT Dark Matter Experiment

DRIFT... Where?DRIFT... Where?

Boulby mineBoulby mine

Cleveland Potash Ltd.

Page 11: The DRIFT Dark Matter Experiment

DRIFT... When?DRIFT... When?

DRIFT-I

Underground in 2001

Data taking 2001-2004

Shielding installed 2004

Decommissioned 2004

DRIFT-I

Underground in 2001

Data taking 2001-2004

Shielding installed 2004

Decommissioned 2004

Page 12: The DRIFT Dark Matter Experiment

DRIFT... When?DRIFT... When?

DRIFT-IIUnderfloor shielding Autumn 20041st vessel u/g December 20041st detector u/g February 2005Further modules to go u/g throughout 2005 and on

DRIFT-IIUnderfloor shielding Autumn 20041st vessel u/g December 20041st detector u/g February 2005Further modules to go u/g throughout 2005 and on

Page 13: The DRIFT Dark Matter Experiment

DRIFT... How?DRIFT... How?

Nuclear recoils (elastic scattering)

Low energy ionisation

0.01 - 1 kg-1 day-1

Directionally sensitive

IMPORTANT:

Background reduction

gammas, alphas, neutrons etc.

require << 1 recoil per year

Nuclear recoils (elastic scattering)

Low energy ionisation

0.01 - 1 kg-1 day-1

Directionally sensitive

IMPORTANT:

Background reduction

gammas, alphas, neutrons etc.

require << 1 recoil per year

Page 14: The DRIFT Dark Matter Experiment

Carson et al. Astrop. Phys. 21 (2004) 667Carson et al. hep-ex/0503017 (accepted to

NIM-A)

SimulationsSimulations

Using SOURCES, GEANT4 and FLUKA

Neutron energy spectra (U & Th contamination)

Muon-induced neutrons

Geometry and particle tracking

Using SOURCES, GEANT4 and FLUKA

Neutron energy spectra (U & Th contamination)

Muon-induced neutrons

Geometry and particle tracking

Page 15: The DRIFT Dark Matter Experiment

SimulationsSimulations

Single and grouped DRIFT modules

Hydrocarbon neutron shielding

Reduce recoils due to neutron background to < 1 per year per module

Single and grouped DRIFT modules

Hydrocarbon neutron shielding

Reduce recoils due to neutron background to < 1 per year per module

SourceRecoil rate per

module per year (10-50 keV)

Recoil rate per 20 modules per year (10-50 keV)

Recoil rate per 10 kg per year

(10-50 keV)

Rock (40 g/cm2 CH2) 0.01 0.2 0.6

Detector components 0.06 1.3 3.8

Muon-induced 0.12 2.4 7.2

TOTAL 0.19 3.9 11.6

Page 16: The DRIFT Dark Matter Experiment

Data AnalysisData Analysis

DRIFT-IDRIFT-I

Snowden-Ifft et al. NIM-A 498 (2003) 155

Alner et al. NIM-A 535 (2004) 644

Page 17: The DRIFT Dark Matter Experiment

Data AnalysisData Analysis

Commissioning of the first DRIFT-II detector has been performed at Occidental College, L.A.

Initial calibration and background runs successful

Data analysis software is progressing as early data is being taken

Waveform plotting and data reduction

Parameter calculation and plotting

Software cuts in progress

Commissioning of the first DRIFT-II detector has been performed at Occidental College, L.A.

Initial calibration and background runs successful

Data analysis software is progressing as early data is being taken

Waveform plotting and data reduction

Parameter calculation and plotting

Software cuts in progress

55Fe gamma55Fe gamma

Cosmic neutronCosmic neutron

AlphaAlpha

Page 18: The DRIFT Dark Matter Experiment

Looking ahead ...Looking ahead ...

DRIFT-II

In progress

DRIFT-III

towards 1000 kg

target mass

Plus

Further improved simulations

Charge readout R & D

Much data taking and analysis

DRIFT-II

In progress

DRIFT-III

towards 1000 kg

target mass

Plus

Further improved simulations

Charge readout R & D

Much data taking and analysis