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

Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

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Page 1: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Down-to-earth searches for cosmological dark matterCarter Hall, University of Maryland

October 19, 2016

Page 2: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Astrophysical evidence for dark matter

Ω Galaxy cluster collisions Rotation curves

Page 3: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

3 3

380,000 years after the big bang

Today

1970’s - 1980’s: Cold dark matter is needed to seed the formation of galaxy clusters

13.9 billion years

Credit: Andrey Kravtsov, KICP, U. Chicago

Page 4: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

4

Temperature and density fluctuations are 1 part in 105.

The cosmic microwave background anisotropy imaged Planck (2014).

Page 5: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

5

CMB multipole expansion - measured by Planck (2014)

Prominent 3rd peak indicates presence of matter which did not rebound.

~ 1°

~ 1/2°~ 1/3°

Page 6: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Neutrinos? – not heavy enough

‘Weakly Interacting Massive Particle’

generalize

Page 7: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Early universe plasma

Age of universe ~ 1 nanosecond;Temperature ~ 100 GeV

?

Dark matter

Dark matter

Normalmatter

Normal matter

Dark matter annihilation

Dark matter creation

The thermal hypothesis:Was the dark matter an interacting component in the very early universe?

Page 8: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Correct dark

matter abundance

Large annihilation cross section

Small annihilation cross section

Typical weak nuclear force cross sections

J. Feng, Annu. Rev. Astron. Astrophys. 2010. 48:495–545

The thermal hypothesis:Was the dark matter an interacting component in the very early universe?

Page 9: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

The Milky Way’s dark matter halo

•  Typical orbital vel. = 230 km/sec~ 0.1% speed of light

•  Density: ~ 300 mproton / liter•  WIMPs (~100 GeV): 3 per liter

•  deBroglie wavelength:•  WIMPs: larger than a nucleus.

Coherent scalar scattering on ordinary nuclear matter, σ ~ A2

•  Production: •  WIMPs: thermal

Page 10: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

?

Dark matter

Dark matter

Normalmatter

Normal matter

Dark matter annihilation

Dark matter creation

Page 11: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016
Page 12: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

HAWC projected five-year sensitivity (start 2015)

Page 13: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016
Page 14: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016
Page 15: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

?

Dark matter

Dark matter

Normalmatter

Normal matter

‘Direct detection’

Page 16: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

WIMP γ,β

‘Direct Detection’

nuclear recoil signal

electron recoil background

Page 17: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

The parameter space of direct detection

& XENONNT

Page 18: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Nuclear recoil energy spectra

From: arXiv:1107.1295

A2 dependence

Page 19: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Calibration of LUX: Beta spectrum of Carbon-14

Carbon-14 beta decay

Xenon-131 Gamma line

(164 keV)

Detector threshold = 1.3 keV

1- 8 keV: x-ray region

Page 20: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

20 20

Target

scintillating bolometers (CRESST)

Cryogenic semiconductors

(CDMS)

Light

Phonons/heat 100% energy slowest cryogenics

Ionization

WIMP

WIMP

• Nuclear recoils vs. electron recoils ◆ "Division of energy ◆ "Timing ◆ "Stopping power

Two-phase noble liquids (PandaX, XENON, LUX)

Detection modes for ionizing radiation

Single-Phase noble liquids (XMASS, DEAP/CLEAN)

Page 21: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016
Page 22: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

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Typical Event in LUX

S1S2

Page 23: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

23

Strong background rejection from kinematics

~ MeV γ

must cross

full volume without

interacting again

~ keV deposition

forward scattering

Page 24: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

24

Simulation of self-shielding in liquid xenon

Volume cut rejects most gamma backgrounds.

Page 25: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

25

Particle ID: recoil discrimination in LUX

Light

Charge/Light

Charge/Light

Charge/Light

Electron recoils (background)

Nuclear recoils (signal)

Difference

Electron recoil rejection factor:

200 -500

Page 26: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

26

LUX assembly – 2010 - 2011

370 kg of liquid xenon

Page 27: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

27

Page 28: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Sanford Underground Research Facility

Davis Cavern 1480 m (4200 mwe)

LUX Water Tank South Dakota USA

28

Page 29: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

29

Davis Cavern @ SURF, March 2011

Page 30: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

30 30

Davis Campus dedication, May 30, 2012

Ana Davis, widow of Ray Davis

Davis Campus water tank, home of LUX

Page 31: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

31

On top of the water shield, Sept. 2012

Page 32: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

32

LUX installed underground, Sept. 2012

Page 33: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

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LUX recoil bands and energy scales

more charge recombination

less charge recombination

electron recoil band

nuclear recoil band

Page 34: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

34

0 10 20 30 40 501

1.2

1.4

1.6

1.8

2

2.2

2.4

2.6

log 10

(S2 b/S

1) x

,y,z

cor

rect

ed

S1 x,y,z corrected (phe)

3 6 9 12 15 18 21 24 27 30 keVnr

1.3

1.8

3.5

4.65.9

7.1

keVee

LUX WIMP search data (2013) 160 events observed 85.3 days × 118.3 kg = 10,090 kg�days

2013 initial results (Run 3): Phys.Rev.Lett. 112 (2014) 091303. 2015 re-analysis of Run 3: Phys.Rev.Lett. 116 (2016) 161301.

Light

Charge Light

_______

Page 35: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

October 30, 2013

Page 36: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Calibration: external gamma sources (137Cs)

Calibration source guide tubes

Self-shielding makesexternal gamma sources

mostly ineffectual

Page 37: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

37

Tritium: an ideal electron-recoil band calibration source

0 2 4 6 8 10 12 14 16 18 200

0.5

1

1.5

2

Electron Kinetic Energy [keV]

Coun

ts/k

eV/d

ay/1

0000

0 at

oms

Tritium Beta Spectrum (Q=18.6 keV, T1/2=12.3 years)

WIMP search range

C

H

H H

T

Page 38: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

38

Injection and removal of tritium from LUX, August 2013

−300 −200 −100 0 100 200 300 400 500

10−4

10−3

10−2

10−1

100

Time (hours)

Rat

e (H

z)

S1 <150 [Phe]. Fiducial Volume

Rateτ 1=6.0 ±0.5Hoursτ 2=6.4 ±0.1 Hours

August 8, 2013

Success

10/21/16

Fiducial count rate for S1 < 150 PE

Page 39: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

0 100 200 300 400 500 600

0

50

100

150

200

250

300

radius squared (cm2)

drift

tim

e (µ

s)

−20 −10 0 10 20−25

−20

−15

−10

−5

0

5

10

15

20

25

x (cm)

y (c

m)

Tritium event locations in LUX – August 2013

39

Page 40: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Charge vs Light from tritium in LUX at 170 V/cm

178,000 fiducial tritium events 10/21/16 40

Page 41: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Tritium “combined-energy” spectrum

178,000 fiducial tritium events 41

Page 42: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Light yield of liquid xenon

LUX – tritium (100 & 180 V/cm)

Page 43: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Nuclear-recoil calibration w/mono-energetic neutronsD + D → n + 3He En = 2.45 MeV

Page 44: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

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

Page 45: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

LUX final WIMP search results – Run 3 & 4 combined, 2013 - 2016

LUX Run 3 & 4 (2016): arXiv:1608.07648

Page 46: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

LUX -> LZ (2020) Scale up LUX fiducial mass by x40

46

LUX

LZ:TotalXe-10TonAc5veXe–7TonFiducialXe–5.6Ton

LUX

Page 47: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

47

Xe TPC

Gd-doped liquid

scintillator outer

detector

50 kV high voltage

existing LUX water shield

The LZ Experiment – coming in 2020

Page 48: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

LZ Sensitivity (5.6 Tonnes, 1000 live days)

48

2.5×10-48cm2

Page 49: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

History of WIMP sensitivity @ 50 GeV

LUX & PandaX-II (2016) LZ

Ge, NaI no discrimination

Ge, w/discrim.

LXe, w/discrim. ZEPLIN

XENON 1T

XENON100

LUX (2013)

Page 50: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016
Page 51: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

51

Uranium-238 decay chain

Thorium-232 decay chain

end end

start

start

gamma sources

Page 52: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

52

Tl-208 (Th-232) Bi-214

(U-238) K-40

Ge-76

Xe-136 Te-130

ββ0ν Q values:

Ordinary radioactive decay here on earth

WIMP scattering

Page 53: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

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

Page 54: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

54

Electron-recoil and nuclear-recoil calibration data

Page 55: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

Is LUX a success?

Page 56: Down-to-earth searches for cosmological dark matter · 2016. 10. 21. · Down-to-earth searches for cosmological dark matter Carter Hall, University of Maryland October 19, 2016

July 22, 2016