Down-to-earth searches for cosmological dark matter

Similar documents
Axion search with Dark Matter detector

Technical Specifications and Requirements on Direct detection for Dark Matter Searches

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

LARGE UNDERGROUND XENON

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

Low Background Experiments and Material Assay. Tessa Johnson NSSC Summer School July 2016

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

Direct dark matter search using liquid noble gases

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

Current status of LUX Dark Matter Experiment

Status of Dark Matter Detection Experiments

Status of DM Direct Detection. Ranny Budnik Weizmann Institute of Science

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

XMASS: a large single-phase liquid-xenon detector

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

Measurement of 39 Ar in Underground Argon for Dark Matter Experiments

Direct Search for Dark Matter

Low Energy Particles in Noble Liquids

The Search for Dark Matter with the XENON Experiment

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

Sensitivity and Backgrounds of the LUX Dark Matter Search

Do WIMPs Rule? The LUX & LZ Experiments and the Search for Cosmic Dark Matter

Background and sensitivity predictions for XENON1T

DarkSide new results and prospects

The Search for Dark Matter, and Xenon1TP

LZ and Direct Dark Matter Detection

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

The Neutron/WIMP Acceptance In XENON100

Direct Detection of Dark Matter with LUX

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

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

The XENON1T experiment

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

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

A survey of recent dark matter direct detection results

Dark Matter. and TPC Technologies

Chapter 12. Dark Matter

Direct detection: results from liquid noble-gas experiments

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

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

DARWIN: dark matter WIMP search with noble liquids

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

Dark Matter Searches. Marijke Haffke University of Zürich

Direct dark matter search using liquid noble gases

Whither WIMP Dark Matter Search? Pijushpani Bhattacharjee AstroParticle Physics & Cosmology Division Saha Institute of Nuclear Physics Kolkata

Recent Results from the PandaX Experiment

Direct Detection of Dark Matter. Lauren Hsu Fermilab Center for Particle Astrophysics TRISEP Summer School, June 10, 2014

Detectors for astroparticle physics

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

The Direct Search for Dark Matter

Neutrino and Dark Matter Detections via Atomic Ionizations at sub-kev Sensitivities

Esperimenti bolometrici al Gran Sasso: CUORE e CRESST

DARK MATTER SEARCH AT BOULBY MINE

Direct Search for Dark Matter

The next generation dark matter hunter: XENON1T status and perspective

Cryogenic Detectors Direct Dark Matter Search. Dark Matter

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

XMASS 1.5, the next step of the XMASS experiment

Neutrinos. Why measure them? Why are they difficult to observe?

Direkte Suche nach Dark Matter

Measuring Dark Matter Properties with High-Energy Colliders

Solar and atmospheric neutrinos as background for direct dark matter searches

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

=> Ωmatter >> Ωbaryon

CMB constraints on dark matter annihilation

Studies of the XENON100 Electromagnetic Background

FURTHER COSMOLOGY Book page T H E M A K E U P O F T H E U N I V E R S E

The LUX Dark Matter Search Objectives and Status

Nuclear Recoil Scintillation and Ionization Yields in Liquid Xenon

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

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

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

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

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

Threshold optimization and Bayesian inference on the XENON1T experiment

Search for double electron capture on 124 Xe with the XMASS-I detector

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

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

Axion and axion-like particle searches in LUX and LZ. Maria Francesca Marzioni

The Search for Dark Matter. Jim Musser

The XENON Project. M. Selvi The XENON project

Dark Matter Search at Boulby Mine I. Liubarskyy 1, T. Aliz, G. J. Alnerx, B. Ahmedz, G. T. J. Arnisonx, J. C. Bartoní, A. Bewickz, D. Davidgez, G. J.

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

David Reyna Belkis Cabrera-Palmer AAP2010, Japan

Introduction to Class and Dark Matter

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

Dark Matter, Low-Background Physics

Direct Dark Matter and Axion Detection with CUORE

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

BubXe: a liquid xenon bubble chamber for Dark Matter detection!

arxiv:astro-ph/ v1 15 Feb 2005

Neutrino coherent scattering in Liquid Xenon

Nucleosíntesis primordial

arxiv:astro-ph/ v1 24 Jun 2004

Direct Dark Matter Searches

Darkside and the future Liquid Argon Dark Matter program

Recent Discoveries in Neutrino Physics

Recent results and status of the XENON program

Astronomy 182: Origin and Evolution of the Universe

Transcription:

Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Astrophysical evidence for dark matter Galaxy cluster collisions Rotation curves Ω

380,000 years after the big bang 13.9 billion years Today Credit: Andrey Kravtsov, KICP, U. Chicago 1970 s - 1980 s: Cold dark matter is needed to seed the formation of galaxy clusters 3

Temperature and density fluctuations are 1 part in 10 5. The cosmic microwave background anisotropy imaged Planck (2014). 4

CMB multipole expansion - measured by Planck (2014) ~ 1 Prominent 3 rd peak indicates presence of matter which did not rebound. ~ 1/2 ~ 1/3 5

Neutrinos? not heavy enough generalize Weakly Interacting Massive Particle

The thermal hypothesis: Was the dark matter an interacting component in the very early universe? Early universe plasma Dark matter annihilation Dark matter Normal matter? Age of universe ~ 1 nanosecond; Temperature ~ 100 GeV Dark matter Dark matter creation Normal matter

The thermal hypothesis: Was the dark matter an interacting component in the very early universe? Small annihilation cross section Typical weak nuclear force cross sections Correct dark matter abundance Large annihilation cross section J. Feng, Annu. Rev. Astron. Astrophys. 2010. 48:495 545

The Milky Way s dark matter halo Typical orbital vel. = 230 km/sec ~ 0.1% speed of light Density: ~ 300 m proton / liter WIMPs (~100 GeV): 3 per liter debroglie wavelength: WIMPs: larger than a nucleus. Coherent scalar scattering on ordinary nuclear matter, σ ~ A 2 Production: WIMPs: thermal

Dark matter annihilation Dark matter Normal matter? Dark matter Normal matter Dark matter creation

HAWC projected five-year sensitivity (start 2015)

Direct detection Dark matter Normal matter? Dark matter Normal matter

Direct Detection WIMP nuclear recoil signal γ,β electron recoil background

The parameter space of direct detection & XENONNT

Nuclear recoil energy spectra A 2 dependence From: arxiv:1107.1295

Calibration of LUX: Beta spectrum of Carbon-14 Carbon-14 beta decay Detector threshold = 1.3 kev Xenon-131 Gamma line (164 kev) 1-8 kev: x-ray region

Detection modes for ionizing radiation Nuclear recoils vs. electron recoils "Division of energy "Timing "Stopping power Two-phase noble liquids (PandaX, XENON, LUX) Ionization Target WIMP Cryogenic semiconductors (CDMS) Phonons/heat 100% energy slowest cryogenics Single-Phase noble liquids (XMASS, DEAP/CLEAN) Light WIMP scintillating bolometers (CRESST) 20

Typical Event in LUX S1 S2 22

Strong background rejection from kinematics ~ kev deposition must cross full volume without interacting again ~ MeV γ forward scattering 23

Simulation of self-shielding in liquid xenon Volume cut rejects most gamma backgrounds. 24

Particle ID: recoil discrimination in LUX Charge/Light Electron recoils (background) Charge/Light Nuclear recoils (signal) Charge/Light Difference Electron recoil rejection factor: 200-500 Light 25

LUX assembly 2010-2011 370 kg of liquid xenon 26

27

Sanford Underground Research Facility Davis Cavern 1480 m (4200 mwe) LUX Water Tank South Dakota USA 28

Davis Cavern @ SURF, March 2011 29

Davis Campus dedication, May 30, 2012 Davis Campus water tank, home of LUX Ana Davis, widow of Ray Davis 30

On top of the water shield, Sept. 2012 31

LUX installed underground, Sept. 2012 32

LUX recoil bands and energy scales electron recoil band less charge recombination nuclear recoil band more charge recombination 33

2.6 2.4 LUX WIMP search data (2013) 1.3 kev ee 1.8 160 events observed 85.3 days 118.3 kg = 10,090 kgdays Charge Light log 10 (S2 b /S1) x,y,z corrected 2.2 2 1.8 1.6 1.4 3.5 4.6 5.9 7.1 1.2 3 6 9 12 15 18 21 24 27 30 kevnr 1 0 10 20 30 40 50 S1 x,y,z corrected (phe) Light 2013 initial results (Run 3): Phys.Rev.Lett. 112 (2014) 091303. 2015 re-analysis of Run 3: Phys.Rev.Lett. 116 (2016) 161301. 34

October 30, 2013

Calibration: external gamma sources ( 137 Cs) Calibration source guide tubes Self-shielding makes external gamma sources mostly ineffectual

Tritium: an ideal electron-recoil band calibration source Tritium Beta Spectrum (Q=18.6 kev, T1/2=12.3 years) 2 Counts/keV/day/100000 atoms 1.5 1 0.5 WIMP search range H H C T H 0 0 2 4 6 8 10 12 14 16 18 20 Electron Kinetic Energy [kev] 37

Injection and removal of tritium from LUX, August 2013 10 0 10 1 Fiducial S1 count <150 [Phe]. rate Fiducial for S1 Volume < 150 PE Rate τ 1 =6.0 ±0.5Hours τ 2 =6.4 ±0.1 Hours August 8, 2013 Rate (Hz) 10 2 Success 10 3 10 4 10/21/16 300 200 100 0 100 200 300 400 500 Time (hours) 38

Tritium event locations in LUX August 2013 y (cm) 25 20 15 10 5 0 5 10 15 20 25 20 10 0 10 20 x (cm) drift time (µs) 0 50 100 150 200 250 300 0 100 200 300 400 500 600 radius squared (cm 2 ) 39

Charge vs Light from tritium in LUX at 170 V/cm 10/21/16 178,000 fiducial tritium events 40

Tritium combined-energy spectrum 178,000 fiducial tritium events 41

Light yield of liquid xenon LUX tritium (100 & 180 V/cm)

Nuclear-recoil calibration w/mono-energetic neutrons D + D n + 3 He E n = 2.45 MeV

Nuclear-recoil calibration of LUX Neutron scattering with a neutron generator

LUX final WIMP search results Run 3 & 4 combined, 2013-2016 LUX Run 3 & 4 (2016): arxiv:1608.07648

LUX -> LZ (2020) Scale up LUX fiducial mass by x40 LZ: Total Xe - 10 Ton Ac5ve Xe 7 Ton Fiducial Xe 5.6 Ton LUX LUX 46

The LZ Experiment coming in 2020 Xe TPC existing LUX water shield 50 kv high voltage Gd-doped liquid scintillator outer detector 47

LZ Sensitivity (5.6 Tonnes, 1000 live days) 2.5 10-48 cm 2 48

History of WIMP sensitivity @ 50 GeV Ge, NaI no discrimination Ge, w/discrim. ZEPLIN XENON100 LXe, w/discrim. LUX (2013) LUX & PandaX-II (2016) LZ XENON 1T

Uranium-238 decay chain start Thorium-232 decay chain start gamma sources end end 51

Ordinary radioactive decay here on earth K-40 Bi-214 (U-238) Tl-208 (Th-232) WIMP scattering ββ0ν Q values: Ge-76 Xe-136 Te-130 52

Two problems from particle physics 1) Why is the weak scale so light? è New weak physics? è WIMPs 2) Why no CP violation in QCD? è Peccei-Quinn symmetry?è Axions

Electron-recoil and nuclear-recoil calibration data 54

Is LUX a success?

July 22, 2016