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

Similar documents
The XENON1T experiment

Technical Specifications and Requirements on Direct detection for Dark Matter Searches

The Direct Search for Dark Matter

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

Status of Dark Matter Detection Experiments

Direct Search for Dark Matter

Down-to-earth searches for cosmological dark matter

Introduction to Class and Dark Matter

Direct dark matter search using liquid noble gases

Direct Dark Matter Search with Noble Liquids

Enectalí Figueroa-Feliciano

The Search for Dark Matter with the XENON Experiment

Direct detection: results from liquid noble-gas experiments

Direct Dark Matter Searches

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

Dark Matter Search * in China

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

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

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

SuperCDMS SNOLAB: A G2 Dark Matter Search. Ben Loer, Fermilab Center for Particle Astrophysics On behalf of the SuperCDMS Collaboration

Dark Matter, Low-Background Physics

A survey of recent dark matter direct detection results

Status of the XENON100 Dark Matter Search

Darkside and the future Liquid Argon Dark Matter program

Direct dark matter search using liquid noble gases

Precision Measurement Of Nuclear Recoil Ionization Yields For Low Mass Wimp Searches

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

Direct Detection Lecture 2: Current Results

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

Direct Search for Dark Matter

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

Direct Detection of Dark Matter with LUX

WIMP Dark Matter Search with XENON and DARWIN

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

Dark Matter Searches. Marijke Haffke University of Zürich

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

DarkSide new results and prospects

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

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

Background and sensitivity predictions for XENON1T

WIMP Direct Detection: an outlook

PandaX Dark Matter Search

Recent results from the second CDMSlite run and overview of SuperCDMS SNOLAB project

Esperimenti bolometrici al Gran Sasso: CUORE e CRESST

Direct Search for Dark Matter

Dark Matter Direct Detection

Prospects for WIMP Dark Matter Direct Searches with XENON1T and DARWIN

LZ and Direct Dark Matter Detection

Dark Matter. and TPC Technologies

DARWIN. Marc Schumann Physik Institut, Universität Zürich. Aspera Technology Forum 2010, October 21-22, 2010

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

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

Measurement of 39 Ar in Underground Argon for Dark Matter Experiments

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

Chapter 12. Dark Matter

COUPP: Bubble Chambers for Dark Matter Detection

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

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

Outline. Dark Matter Physics at SNOLAB: And Future Prospects. Overview of SNOLAB DarkMatter Program. Status of Current Experiments

DARWIN: dark matter WIMP search with noble liquids

Effective theory of dark matter direct detection. Riccardo Catena. Chalmers University of Technology

Axion search with Dark Matter detector

Direct Detection in the next five years: Experimental challenges and Phonon Mediated Detectors

Quest for Dark Matter by direct detection experiments with noble liquids

Dark Matter Search with XENON

Current status of LUX Dark Matter Experiment

The Search for Dark Matter, and Xenon1TP

Direct Detection: Liquid Nobles

Future DM Direct Detection Experiments

Dark Matter Searches WIMPs

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

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

Latest Results on Direct Detection of Dark Matter WIMPs - CDMS & SuperCDMS

Week 3 - Part 2 Recombination and Dark Matter. Joel Primack

Dark Matter Direct Detection: the state-of-the-art KMI School, Nagoya, Japan February 28, 2018

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

Looking for WIMPs A Review

Overview of Direct Detection Dark Matter Experiments

Sensitivity and Backgrounds of the LUX Dark Matter Search

Neutrino mass and neutrino dark matter. Do non-relativistic neutrinos constitute the dark matter? Europhysics Letters 86 (2009) 59001

SuperCDMS: Recent Results for low-mass WIMPS

Recent Results from the PandaX Experiment

DEAP & CLEAN Detectors for the Direct Detection of Dark Matter

Dark Matter and the XENON Experiment

Direct Detection of Dark Matter: Not Noble Gases

Bubble Chambers for Direct Dark Matter Searches in COUPP

XMASS: a large single-phase liquid-xenon detector

Dark Matter - III. Workshop Freudenstadt September 30, GRK 1694: Elementarteilchenphysik bei höchster Energie und höchster Präzision

The LZ Experiment Tom Shutt SLAC. SURF South Dakota

The XENON1T Experiment

China JinPing underground Laboratory (CJPL) and China Darkmatter Experiment (CDEX) Qian Yue Tsinghua University Mar.24, 2011

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

Review of dark matter direct detection experiments

Supernova Neutrino Physics with XENON1T and Beyond

Dark matter search with the SABRE experiment

Dark Matter Detection with XENON100 Accomplishments, Challenges and the Future

Direct Detection of! sub-gev Dark Matter

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

Search for Inelastic Dark Matter with the CDMS experiment. Sebastian Arrenberg Universität Zürich Doktorierendenseminar 2010 Zürich,

Cryodetectors, CRESST and Background

Transcription:

Status of DM Direct Detection Ranny Budnik Weizmann Institute of Science

DM evidence on one slide

Thermal freeze out of dark matter in the standard cosmological model Weakly Interacting Massive Particles (WIMPs) were produced in Big Bang The equilibrium abundance is maintained by pair annihilation and vice versa Production suppressed (T<mχ) Being produced and annihilating (T mχ) Freeze out Due to the expansion of the Universe, the rate of the annihilation goes down and freezes. e.g. Bertone, Hooper, Silk (2005) But there are other ways as well Timeline of Universe since big bang Fig.: Jungman, Kamionkowski & Griest, PR 96

A short reminder, how to look for WIMPs Directly Indirectly Accelerators χ χ χ q q χ q q χ q- q- χ

A complementary approach Directly Indirectly Accelerators - Local DM distribution - Backgrounds - Limited mass range - Strong astrophysical uncertainties - Distribution in centers of halos - Product propagation - Can only produce candidates - Model dependence: p-p and operators χ χ χ q q χ q q χ q- q- χ

Galactic DM Our Galaxy is rotating at ~200 km/s at the Sun's orbit DM is standing still Hence, there is a constant flux of DM through Earth! Velocities are non-relativistic, β~10-3 <v2dm> v2sun (or close to it)

Principles of Direct Detection Movement with respect to the galactic frame imply DM flux, (for ~100 GeV particle) DM recoils off a target material, leaving some energy in the form of: - Ionized electrons. - Scintillation light. - Heat/phonons. Signal is collected and the recoil energy is extracted.

Dark Matter Direct Detection Goal: Observe WIMP interactions with some target material Expected interaction rate Number of targets WIMP mass WIMP density χ Nuclear Form factor N Interaction cross section WIMP velocity distribution χ Elastic scattering Inelastic scattering Only those WIMPs with velocity above threshold will contribute to that energy For Spin Independent interactions the cross section is enhanced by a factor A2 (coherent scattering)

Dark matter and Earth dynamics: Annual modulation In general, the higher vmin, the stronger the relative modulation, but... About 7% modulation on <v>, can be much higher in signal

Direct Detection Techniques PICASSO SIMPLE COUPP PICO HEAT CDMS I-II supercdms EDELWEISS I-II WIMP Detector CRESST -II ROSEBUD +time measurement IONIZATION HPGe exp. IGEX GEDEON GERDA GENIUS CoGeNT WIMP SCINTILLATION ZEPLIN II-III XMASS II XENON LUX/LZ PandaX WARP, ArDM DarkSide ZEPLIN I CLEAN DEAP XMASS DAMA / LIBRA KIMS SABRE

Underground facilities: A must

Fighting backgrounds - UG External γ Shielding and self shielding Multiple scattering Discrimination ER/NR Internal α, β Neutrons: Fission, μ-generated, α-n Cleaning, discrimination Multiple scattering, moderators, n-veto ν s: Don t know yet... Plus, each detector carries extra unique backgrounds (instrumental, unknown source)

Fast progress over ~2 decades

Let neutrinos set the stage! Threshold 8 B DSNB Size Atm. ν

The Size Frontier Target mass is #1 priority Currently led by liquid noble elements: However: backgrounds, threshold play a role Xenon: Xenon LUX/LZ, PandaX-II, XENON1T/nT Argon: DEAP3600, DarkSide, ArDM If looking at non-trivial interaction (e.g. SpinDependent), other targets get the lead (e.g. PICO, 19F)

The leading tech: Dual Phase Xenon TPC S1: Prompt scintillation Gaseous Xenon Top PMTs Anode mesh S2 Ground mesh E ~0.53kV/cm S2: Proportional scintillation after e- drift and extraction into gas Nuclear Recoil χ/n Drift time S1 S2 Discrimination by S2/S1 ee- e- S1 γ/β Cathode mesh Bottom PMTs Liquid Xenon Electronic Recoil Interaction vertex reconstruction: Horizontal from top PMT array Vertical from drift time Drift time S1 S2

LUX Forerunner Summer 2016 From Gaitskell, TAUP

LZ- LUX+Zeplin To start 2020 @SURF Use of n-veto, 7-ton TPC, 5 year run

XENON1T/nT Swift upgrade to XENONnT within 18 months, equivalent to LZ Arxiv:1705:06655

DARWIN The ultimate LXe exp? Can we reach the ν floor? Would require O(50t) Xe Backgrounds at unprecedented levels Technology stretching to the end: HV, purity, calibration, stability Probably means cooperation between long-time competitors SI 1606:07001 WIMP-n

PandaX-II hot from the oven 3 days ago Combining all runs, 54 ton-day Reduced Kr background, plus under-fluctuation Future plans for PandaX-4t and PabdaX-III (2ν0β)

DarkSide50 and 20k

Single phase - DEAP3600 3.6t of LAr Low radioactivity underground Ar Great discrimination, LY, purity Has great potential at high masses Future prospects for >100t global experiment (with DS, ArDM, CLEAN)

PICO Bubble chambers back in the biz Using bubble nucleation plus acoustic (to reject α s) PICO60 best in proton cross section PICO500 to begin construction 2018 Fight with n-background, water background

The Low Mass Frontier Name of the game Lower threshold, control backgrounds Main competitors: Crystals with all channels Ongoing R&D efforts for low noise, low T, low background, low threshold

CRESST-III: Lowest achieved threshold

SuperCDMS Ge and Si crystals at 10s of mk using TES for phonons, plus ionization The old-time leader, re-invented to lead in the low mass range Will start data taking 2020 @SNOLAB Charge signal HV izip Electron recoils: background Nuclear recoils: signal Phonon signal HV may come at the expense of backgrounds and discrimination

EDELWEISS-III

- DAMIC e recoil

Can someone finally solve the DAMA/LIBRA conundrum? Can we resolve a two decade old puzzle of disagreement with so many experiments? SABRE ANAIS DM-ICE PICOLON COSINE-100 COSINUS Efforts should yield an answer is a few years...

And more, Off the mainstream: SD, EFT, axions, inelastic, e- scattering... Annual modulation Crazy technologies for future detectors Ptolemy, Sensei Experiments skipped today, but not forgotten XMASS, KIMS, CDEX, CUORE... How to battle the backgrounds? New ideas are required!

Conclusions The direct detection field keeps growing in sensitivity is both major directions: size and threshold Competitiveness is very high, backgrounds are low but should be lower! Search for crazier technologies ongoing Many windows still closed, and the neutrino floor is coming for us! What is the step beyond? How about directionality?