Current status of LUX Dark Matter Experiment

Similar documents
LARGE UNDERGROUND XENON

Background Modeling and Materials Screening for the LUX and LZ Detectors. David Malling Brown University LUX Collaboration AARM Meeting February 2011

After LUX: The LZ Program. David Malling, Simon Fiorucci Brown University APS DPF Conference August 10, 2011

Sensitivity and Backgrounds of the LUX Dark Matter Search

The LZ Experiment Tom Shutt SLAC. SURF South Dakota

Background Characterization and Rejection in the LZ Detector. David Malling Brown University IDM 2012 July 25, 2012

LUX-ZEPLIN (LZ) Status. Attila Dobi Lawrence Berkeley National Laboratory June 10, 2015 WIN Heidelberg

UCLA Dark Matter 2014 Symposium. Origins and Distributions of the Backgrounds. 15 min

Direct Detection of Dark Matter with LUX

The LUX Dark Matter Search Objectives and Status

Studies of the XENON100 Electromagnetic Background

XENON100. Marc Schumann. Physik Institut, Universität Zürich. IDM 2010, Montpellier, July 26 th,

LUX. Some thoughts on large detectors. Comments on Xe microphysics. Tom Shutt Case Western Reserve University

Axion search with Dark Matter detector

The XENON100 Dark Matter Experiment at LNGS: Status and Sensitivity

The XENON1T experiment

Backgrounds and Sensitivity Expectations for XENON100

The Search for Dark Matter with the XENON Experiment

Measurement of 39 Ar in Underground Argon for Dark Matter Experiments

XENONNT AND BEYOND. Hardy Simgen. WIN 2015 MPIK Heidelberg. Max-Planck-Institut für Kernphysik Heidelberg

Direct dark matter search using liquid noble gases

Recent results from PandaX- II and status of PandaX-4T

Down-to-earth searches for cosmological dark matter

The XENON Dark Matter Project: Status of the XENON100 Phase. Elena Aprile Columbia University

DarkSide-50: performance and results from the first atmospheric argon run

Background and sensitivity predictions for XENON1T

LUX: A Large Underground Xenon detector. WIMP Search. Mani Tripathi, INPAC Meeting. Berkeley, May 5, 2007

Measurements of liquid xenon s response to low-energy particle interactions

Light Dark Matter and XENON100. For the XENON100 Collaboration Rafael F. Lang Columbia University

PANDA-X A New Detector for Dark Matter Search. Karl Giboni Shanghai Jiao Tong University

Recent Results from the PandaX Experiment

A survey of recent dark matter direct detection results

Searching for Dark Matter From XENON10 to LUX. Luiz de Viveiros

The Large Underground Xenon (LUX) Dark Matter Experiment

arxiv:astro-ph/ v1 15 Feb 2005

Paolo Agnes Laboratoire APC, Université Paris 7 on behalf of the DarkSide Collaboration. Dark Matter 2016 UCLA 17th - 19th February 2016

Nuclear Recoil Scintillation and Ionization Yields in Liquid Xenon

DARWIN. Marc Schumann. U Freiburg PATRAS 2017 Thessaloniki, May 19,

Recent results from the UK Dark Matter Search at Boulby Mine.

DarkSide new results and prospects

TWO-PHASE DETECTORS USING THE NOBLE LIQUID XENON. Henrique Araújo Imperial College London

Dark Matter Detection with XENON100 Accomplishments, Challenges and the Future

Dark Matter Detection and the XENON Experiment. 1 Abstract. 2 Introduction

LZ and Direct Dark Matter Detection

Background Studies for the XENON100 Experiment. Alexander Kish Physics Institute, University of Zürich Doktorandenseminar August 30, 2010 UZH

DarkSide-20k and the future Liquid Argon Dark Matter program. Giuliana Fiorillo Università degli Studi di Napoli Federico II & INFN Napoli

The XENON1T Experiment

PoS(EPS-HEP2017)074. Darkside Status and Prospects. Charles Jeff Martoff Temple University

XMASS: a large single-phase liquid-xenon detector

The next generation dark matter hunter: XENON1T status and perspective

The XENON Project. M. Selvi The XENON project

DarkSide. Bianca Bottino Università di Genova and INFN Sezione di Genova on behalf of the DarkSide collaboration 1

Background simulations and shielding calculations

Status of the XENON100 Dark Matter Search

The XENON100 Dark Matter Experiment

The XENON dark matter search. T. Shutt CWRU

DARWIN. Marc Schumann. U Freiburg LAUNCH 17 Heidelberg, September 15,

DarkSide-20k and the Darkside Program for Dark Matter Searches

LZ and Direct Dark Matter Detection. Kimberly J. Palladino May 1, 2018

Prospects for WIMP Dark Matter Direct Searches with XENON1T and DARWIN

DARK MATTER SEARCH AT BOULBY MINE

SIGN: A Pressurized Noble Gas Approach to WIMP Detection

The Neutron/WIMP Acceptance In XENON100

Scintillation Efficiency of Nuclear Recoils in Liquid Xenon. T. Wongjirad, L. Kastens, A. Manzur, K. Ni, and D.N. McKinsey Yale University

Study well-shaped germanium detectors for lowbackground

Search for Dark Matter with Liquid Argon and Pulse Shape Discrimination

Darkside-50, DarkSide-20k and the Global Collaboration to reach the Neutrino Floor with liquid argon

LUX: The next stage(s) Multi-tonne LXe TPC s (DM08, Marina del Rey, 21 Feb 08)

Technical Specifications and Requirements on Direct detection for Dark Matter Searches

Direct dark matter search using liquid noble gases

PandaX Dark Matter Search

XMASS 1.5, the next step of the XMASS experiment

Direct Dark Matter Searches with LUX

Par$cle and Neutrino Physics. Liang Yang University of Illinois at Urbana- Champaign Physics 403 April 15, 2014

DARWIN: dark matter WIMP search with noble liquids

the DarkSide project Andrea Pocar University of Massachusetts, Amherst

Neutrino coherent scattering in Liquid Xenon

LOW ENERGY SOLAR NEUTRINOS WITH BOREXINO. Lea Di Noto on behalf of the Borexino collaboration

Low Energy Particles in Noble Liquids

DARK MATTER SEARCHES AT CANFRANC: ANAIS AND ROSEBUD: an update INTRODUCTION AND EXPERIMENTAL GOALS SUMMARY OF RECENT ACHIEVEMENTS AND EFFORTS

The relevance of XENON10 constraints in this low-mass region has been questioned [15] C.E. Aalseth et al. arxiv: v1

The Direct Search for Dark Matter

Detectors for astroparticle physics

First Results from the XENON10 Dark Matter Search at Gran Sasso. Elena Aprile Columbia University for the XENON Collaboration

Rivelazione di neutrini solari - Borexino Lino Miramonti 6 Giugno 2006 Gran Sasso

XENON1T: opening a new era in the search for Dark Matter. Elena Aprile, Columbia University on behalf of the Collaboration, UCLA, February 17, 2016

1. Brief Introduction 2. Direct Detection 3. The ZEPLIN II Detector 4. Performance and Results 5. The LUX Detector

Status and Sensitivity Projections for the XENON100 Dark Matter Experiment

Darkside and the future Liquid Argon Dark Matter program

Direct detection: results from liquid noble-gas experiments

The XMASS Experiment. Jing LIU Kavli IPMU, Univ. of Tokyo PPC2013, Jul Deadwood, SD, USA

Direct Dark Matter Searches. General Overview LUX-ZEPLIN Hans Kraus, Oxford

Liquid Xenon Scintillator for Dark Matter Detection

New Physics Results from DarkSide-50. Masayuki Wada Princeton University on behalf of the DarkSide-50 Collaboration Feb

Backgrounds in PICO. Eric Vázquez Jáuregui SNOLAB. AARM Meeting Fermilab; Batavia IL, USA; March 19, 2014

Towards One Tonne WIMP Direct Detectors: Have we got what it takes?

arxiv: v1 [physics.ins-det] 31 Oct 2015 Alden Fan 1

Direct dark matter search with XMASS. K. Abe for the XMASS collaboration

Recent Progress from the DEAP-3600 Dark Matter Direct Detection Experiment

Shedding Light on Dark Matter from Deep Underground with XENON. Kaixuan Ni (Columbia)

Transcription:

Current status of LUX Dark Matter Experiment by A. Lyashenko Yale University On behalf of LUX collaboration

LUX Large Underground Xenon experiment LUX Collaboration: Yale, CWRU, UC Santa Barbara, Brown, TAMU, UC Davis, Harvard, LLNL, LIPP Coimbra, Rochester, LBNL, Maryland, South Dakota SMT

WIMP Dark matter Assuming Ω DM = Ω χ WIMP DM WIMP: stable, non-barionic, non-relativistic, el. neutral m χ =10 GeV-few TeV scatter preferably from nuclei Local Milky Way DM density: ρ χ =0.3±0.1GeV cm -3 ~3 WIMPs in 1L Xe Low Energy Threshold is vital 0-80keV R Recoil Energy

WIMP direct detection: two phase Xe Top PMT Array Gamma Drift time Bottom PMT Array S2/S1 Gamma >>S2/S1 WIMP WIMP

Water Tank LUX Detector Titanium Cans Thermosyphon Top PMT Array Detector Stand 59cm 49cm Field Cage and Teflon Reflector Panels 350 kg LXe (100 kg fiducial) E d =2kV/cm, E extr =5kV/cm, E sc =10kV/cm 122 PMTs (QE~30% @ 175nm) Low Radioactivity Materials >1kW Cooling Power (Thermosyphons) Bottom PMT Array 2 Hamamatsu R8778 PMTs

Challenge: Backgrounds Sea level total muon flux: 55.2 m -2 sec -1 (threshold 300 MeV) Ambient radioactivity: ~100 evts/kg/sec Where is WIMP? Human gamma activity 40 K: ~4000 gammas/sec Walls (U/Th/K): - concrete 25/5.5/640 Bq/kg - rhyolite rock 100/45/900 Bq/kg Internal radioactivity WIMP Goal: few events/100kg/year!!!

Trickery: Going Deep Sanford Underground Research Facility (SURF) LUX 4850 feet (1478 m) underground Homestake Mine ~10 7 fold muon flux suppression 55.2 m -2 sec -1 10-5 m -2 sec -1

Trickery: Water Shield d = 8 m 6 m 20 Tonnes inverted steel pyramid 300 Tonnes of Water Cherenkov Muon Veto 20 Ø10 PMTs Gamma suppression: ~10-7 Neutron suppression (>10 MeV): ~10-3 Neutron suppression (<10 MeV): <10-9

Trickery: Understanding internal backgrounds X 122 PMTs: 10/2/65 mbq/pmt (U/Th/K) and 2 n/year/pmt Dominant source of background!!! Titanium cryostat: <0.4 mbq/kg U+Th (very low!) Cu: 10 ppt U / 12 ppt Th / 18 ppb K [~1% of ER BG budget] Radon: Cleanroom reduces levels to <40 Bq/m 3, Radon Cowl Kr: present in Xe at ppm level <2 ppt level with charcoal column PTFE: U/Th/K < 0.004/<0.001/0.053 mbq/kg 6 10-8 events/kevee/kg/day [~1% of ER BG budget]

Trickery: Xe self shielding PMT gammas PMTs are dominant background source 10 kg Fiducial volume 300 kg PMT neutrons We benefit a lot from scaling up Expect <0.5 nuclear/electron-recoils in 100 days

Trickery: ER/NR Discrimination WIMP region XENON10 data Electron Recoils Cut 2-3 kevee Nuclear Recoils High energies 99.5% Low energies 99.9%

External Sources LUX calibration Internal Sources 83m Kr (half-life 1.86 hours) 9.4 kev 32.1 kev S1 L. Kastens et al., Phys. Rev. C80: 045809,2009, A. Manalaysay et al., Rev. Sci. Instr. 81, 073303 (2010) alpha source S1 LY and kevee, e - lifetime Fills entire fiducial volume 133 Ba, 137 Cs, 22 Na, 208 Tl (collimated): S1 LY, ER energy bands, e - lifetime 241 Am/Be: NR band Tritium (half-life 12.3 yrs) Injected as CH 3 T Beta source, up to 18.6 kev Removed by purification system S2/S1 ER band Fills entire fiducial volume

LUX Program Timeline LUX Surface Run LUX DM Search Run LUX 0.1 2007-2009 2010-2011 NOW!!! 2012+

Sanford Lab Surface Facility

May 2011 first cooldown Held Target Temperature 180K Flexible Temperature Control

Expectations LUX 4000 kg-days (MC simulation) LUX ~2days LUX ~60days LUX ~300days WIMP events Targeting at 7 10-46 cm 2 (@ 100GeV) LUX strong emphasis on WIMP discovery

Future Plans: LZS/LZD Projects LZ = joint collaboration of LUX and ZEPLIN LZS (Sanford) =1500 kg (1200 kg fiducial) LUX infrastructure designed to accommodate LZ Liquid scintillator veto Construction 2012 2013, operation 2014-2015 σ χ = 2x10-47 cm 2 in 2 years LZD = 20 ton concept 2 m diameter x 2 m height Will be in a deeper site, possibly 8000 feet Construction 2014 2016, operation 2017 2020 σ χ = 10-48 cm 2 in 3 years LZD LUX

Summary Dark Matter puzzle convergence of astronomy and particle physics Evidences point to WIMPs waiting to be discovered LUX experiment uses proven liquid Xe technology to reach σ χ = 7x10-46 cm 2 Surface operation is in progress Dark Matter search run will start in 2012 Just when the LHC will be searching for New Physics LZS/LZD will push the sensitivity to 10-48 cm 2 by 2020 We may know what Dark Matter is within this decade!!!

Extra Slides

Xe signal generation

Why WIMPs?

NR scintillation efficiency E ee A. Manzur et al., arxiv:0909.1063v4 and references therein

Tritiated methane (CH 3 T) removal experiment Gaseous proportional tube counter Univ. of Maryland Xe proportional tube for CH 3 T counting Xe purifier CH 3 T storage bottle FE-55 x-ray calibration > 99.9% of CH 3 T removed from proportional tube in one pass through the purifier. Liquid xenon removal test @ UMD this spring.

Case Western Reserve University 15

New analytic technique to detect krypton at the part-per-trillion level arxiv:1103.2714v1 LN 2 Residual Gas Analyzer mass spectrometer GOAL: O(10) ppt 85 Kr - Leads to an event rate of O(0.1) events in the 2-10 kev ee regime after 10 4 kgdays and 99.5% rejection of e - recoils 1.5 ppt Kr open leak valve 16