Listening for the Dark Harry Nelson UCSB

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Listening for the Dark
Harry Nelson
UCSB
HNN
CDMS
Plan

Massive Dark Matter

Direct Detection

Xenon

CDMS

Future
9/15/05
Penn State Colloquium
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HNN
CDMS
0.01%
Metals (us)
0.5%
Visible Baryons
`We Declare a New Order’
(Joel Primack)
Dark Baryons
5%
Cold Dark Matter
(WIMPs?)
25%
Cosmological Constant

70%
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HNN
CDMS
r
9/15/05
v; = v/c
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HNN
9/15/05
CDMS
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CDMS
b = 0.488 ± 0.009
a  M = (1.85 ± 0.06) 1030 kg
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CDMS
Stars w/r Galaxy Center: v/c =  constant  0.7 10-3
Planets about sun
Msun = (1.85 ± 0.06) 1030 kg
Moons about Saturn
MSaturn = (5.5 ± 0.2) 1026 kg
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HNN
CDMS
Galactic Dark Matter
R is the distance from center
v
v is the speed (tangential)
R
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HNN
CDMS
What about our home galaxy (Milky Way)?
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Honma and Sofue, 1996
v
220 km/s
Without the Dark Halo
(Binney & Tremaine)
:v0=180 km/s

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Penn State Colloquium
R
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HNN
CDMS
Milky Way:
mainly a dark cloud
Bulge
Disk
Sun: moves in
plane of disk
v/c =  0.7 10-3
Particles in `halo’: 3-d
 = mc2  n  1/3 GeV/cm3
(1/2 of total mass density)
Maxwellian/Gaussian (simple)
v/c =  0.7 10-3
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HNN
CDMS
Design a Particle and an Experiment
0
v/c =  0.7 10-3
Neutral: cool particles neutral –
, n, , K0, Z0, H0…
v/c =  0.7 10-3
We use Germanium,
A=73, mc2=67.6 GeV;
others: Si, S, I, Xe, W
Massive: Mc2100 GeV hinted ER½ mGec2 2
 ½ 68 GeV  ½  10-6
at by accelerator data
 20 keV
 x-ray energy ! Easy!
`Weak Scale’
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Arguments for  characteristic
of weak interaction
CDMS
1. Particle physics… chose Mc2  100 GeV,
`Weak Scale’
2. Big Bang… independently implies weak cross
section as well…
Coincidence(s)… or Clues ???
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HNN
CDMS
What is the weak interaction cross section?
Donald H. Perkins, 1987
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HNN
Rate governed by scattering cross section, 
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CDMS
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Coherence, density of states
enormous bonus!
CDMS
Scattering off a proton….
…. Hopeless!
0

A = # neutrons + # protons
0

Indistinguishable
Density of States:
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Rate of Main Background
CDMS
Rate about 103 / (kg-day) !!!
Shield… but that radioactive too
Strategies: DAMA… huge target mass (100 kg),
look for astrophysical modulation
CDMS… small target mass (few kg)
distinguish electron from nucl. recoil
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HNN
CDMS
Signal Shape
A2
MWIMP=100 GeV
  10-42 cm2/nucleon
Silicon, Sulphur
Germanium
Iodine, Xenon
Nucleus
Recoils
Er
Slope: Maxwell-Boltzmann
Diffraction
WIMPs in Galaxy
0
9/15/05
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HNN
Catalog of Direct Detection Experiments
CDMS
Indirect Detection:
Super-Kamiokande,
Amanda, Ice-Cube,
HEAT, GLAST,
Egret…
Look for astrophysical
neutrinos, gammas
From WIMP
annihilation
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HNN
Direct Detection: Signal and Main Background
Signal
Background
Nucleus
Recoils
Electron
Recoils
Er
v/c  710-4
dense energy deposition
efficiency low
distinct energy scale
0
 (calibrate: neutron)
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CDMS

Er
v/c  0.3
Sparse Energy Deposition
Differences the
Basis of Particle ID
Penn State Colloquium
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HNN
ZEPLIN II, III, MAX,
XMAS, XENON
CDMS
IGEX,
DRIFTI, II
ionization
CDMS, EDELWEISS
Q
NAIAD, ZEPLIN I,
DAMA
CRESST II,
ROSEBUD
CRESST I,
PICASSO,
COUPP
Tim Sumner
9/15/05
Penn State Colloquium
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HNN
CDMS
Xenon – nuclear recoils give 1/7 scintillation/energy,
compared to electron recoils (``quenching’’)…. Sets recoil energy scale
– Bernabei et al.
– Arneodo et al.
– Akimov et al.
– Aprile et al.
– LIP work
Lindhard
Hitachi
Tim Sumner
9/15/05
E. Aprile et al., arXiv:astro-ph/0503621
Penn State Colloquium
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HNN
Zeplin 1 – Scintillation Alone
CDMS
Nucl. Recoil
Electron Recoil
125 keV
30 keV
3.2 kg Xe
Nuclear Recoils –
Faster Risetime…
30 keV
Risetime (ns)
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HNN
CDMS
Zeplin-I Limit- Background Weakens
300 kg-days
10-42 cm2
CDMS: 100 kg-days
9/15/05
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HNN
CDMS
2-Phase (Liquid/Gas) Noble … Ar or Xe
Nuclear Recoil
S1
S2
S2
Electron Recoil
S2
S1
S1
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HNN
Gamma + neutron source
Gamma source
Zeplin-II
9/15/05
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CDMS
Zeplin-II
25
HNN

Analysis….
Appears scalable
CDMS

However, unforeseen backgrounds are the rule as
sensitivity increases

Promising… ZEPLIN-II and Xenon-10 soon
deployed in deep sites
9/15/05
Penn State Colloquium
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HNN
CDMS
CDMS: Adapt Traditional Ionization Detector
ER10’s keV
Holes
e-
Electrode
Implants

E 1 cm
Germanium (or Silicon)
7.6 cm
¼ kg (1/10 kg)
0

9/15/05
What rate? (in, say, 1kg)
Backgrounds?
….…. Gamma rays, neutrons, surface beta-decay
Penn State Colloquium
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HNN
CDMS
Our Hunting Ground
Weakly
Interacting
Massive
Particle
Experiment
CDMS (shallow)
DAMA (old!)
1/10
9/10
Theory
SUSY,
various constraints
including Big Bang
Gaitskell/Mandic
9/15/05
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HNN
DAMA – Exploit Annual Modulation
CDMS
Signal: higher rate in June,
lower in December
Background: constant in time
9/15/05
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HNN
CDMS
CDMS Collaboration (Mar. 2002)
9/15/05
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HNN
CDMS
CDMS Collaboration
Brown University
Stanford University
M.J. Attisha, R.J. Gaitskell, J-P. F. Thompson
Case Western Reserve University
D.S. Akerib, P. Brusov, C. Bailey, M.R.
Dragowsky, D.D.Driscoll, S.Kamat, A.G.
Manalaysay, T.A. Perera, R.W.Schnee, G.Wang
University of Colorado at Denver
M. E. Huber
Fermi National Accelerator Laboratory
P.L. Brink, B. Cabrera, J.P. Castle,
C.L. Chang, J. Cooley, M. Kurylowicz,
L. Novak, R. W. Ogburn, M. Pyle, T. Saab,
A. Tomada
University of California, Berkeley
Cryogenic Fillipini, A. Lu, V. Mandic, P.Meunier, N.
Mirabolfathi, M.C.Perillo Isaac, W. Rau, B.
Dark
Sadoulet, D.N.Seitz, B. Serfass, G. Smith, A.
Spadafora, K. Sundqvist
Matter
Search University of California, Santa Barbara
D.A. Bauer, R. Choate, M.B. Crisler, R. Dixon,
M. Haldeman, D. Holmgren, B. Johnson,
W.Johnson, M. Kozlovsky, D. Kubik, L. Kula,
B. Lambin, B. Merkel, S. Morrison, S. Orr,
E.Ramberg, R.L. Schmitt, J. Williams, J. Yoo
Lawrence Berkeley National Laboratory
J. Alvaro-Dean, M.S. Armel, M. Daal, J.
R. Bunker, S. Burke, D.O. Caldwell, D.
Callahan, R.Ferril, D. Hale, S. Kyre, R.
Mahapatra, J.May, H. Nelson, R. Nelson, J.
Sander, C.Savage, S.Yellin
University of Florida
L. Baudis, S. Leclerq
J.H Emes, R. McDonald, R.R. Ross, A. Smith
Santa Clara University
B.A. Young
9/15/05
University of Minnesota
J. Beaty, P. Cushman, L. Duong, A. Reisetter
Penn State Colloquium
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HNN
CDMS
Nuclear Recoil bad at making Ionization
Holes
eGermanium
more ionization!
Both deposit, say,
0

20 keV
9/15/05

Need a second, `fair’
measure of deposited
energy… sound!
Penn State Colloquium
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HNN
CDMS
Our Detectors
Phonon D
SQUID array
R bias
`Phonon sensor (4)’ (TES)
R feedback
I bias
Array of Transition Edge Sensors
Ionization Electrodes (2)
D
A
C
B
x-y-z imaging:
Q outer
Q inner
from timing, sharing
Vqbias
Z-coordinate, Ionization, Phonons
ZIP
Operate at 0.050 Kelvin
9/15/05
Penn State Colloquium
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HNN
CDMS
The Phonon Sensor
quasiparticle
trap
W
quasiparticle
Transition-Edge
diffusion
Sensor (TES)
Al Collector
Cooper Pair
Al
Ge or Si
phonons
~ 10mK
normal
RTES ()
4
3
2
1
superconducting
Tc ~ 80mK
T (mK)
R. Schnee
9/15/05
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HNN
CDMS
Pulses
20 KeV
Phonon (4)
Charge (2)
0
30
Time (s)
300
0
Time (s)
300
-30
-30
9/15/05
30
-30
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35
HNN
CDMS
Separation of the types of recoils
(electron recoils)
Neutrons cause
(nuclear
recoils) recoils
nuclear
too!
Another
background…
Sound
9/15/05
Penn State Colloquium
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HNN
CDMS
SUF Run 21 Germanium – Low Threshold
1.3 keV xray, L-shell
Capture
Shallow Site
Neutron
Background
71Ge K-shell Capture
10.4
keV
Ga
x-rays
from
R. Bunker
9/15/05
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HNN
CDMS
Background Neutrons from Cosmic Ray Muons
Limited our earlier
results…moved to a deep mine
9/15/05
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HNN
Go Deep Underground to Evade Muons
9/15/05
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CDMS
39
HNN
CDMS
Deep Facility
Soudan Mine
Hosts: State of Minn., U Minn.,
Fermilab
690 meters underground
2090 meters water equivalent
9/15/05
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HNN
CDMS
Down deep in the Soudan mine
DAQ/Electronics
HVAC
RF-shielded
Clean room
Soudan II
Mezzanine
MINOS
connecting
tunnel
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Mezzanine
Shield
Mechanical
Pumps,
Cryogenics
Fridge
Front-end
Electronics
Icebox
Penn State Colloquium
Detector Prep
Clean Benches
41
HNN
CDMS
Outside In
lead
plastic
scintillators
outer
polyethylene
ancient
lead
9/15/05
inner
polyethylene
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HNN
CDMS
A Cold Heart
Results from first…
FET cards
SQUID cards
4K
0.6 K
0.06 K
0.04 K
ZIP 1 (Ge)
ZIP 2 (Ge)
ZIP 3 (Ge)
ZIP 4 (Si)
ZIP 5 (Ge)
ZIP 6 (Si)
Two `towers’
poorer resolution
14C
14C
14C
6 detectors…
10 cm
4 Germanium (0.25 kg each), 2 Silicon (0.1 kg each)
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HNN
 Calibration (133Barium) (e recoils)
Ionization
L. Baudis
9/15/05
CDMS
Phonons
Energy, KeV
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HNN
CDMS
Better Source, Calibration
Ionization
9/15/05
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Phonons
45
HNN
CDMS
n Calib. (252Californium) (nuclear recoils)
S. Kamat
9/15/05
Reconstructed recoil energy, KeV
Penn State Colloquium
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HNN
CDMS
Soudan Data
First Run


92 calendar days
53 live days,
1 kg Germanium
Tower 1
Second Run



140 calendar days
74 live days,
1.5 kg Germanium
0.6 kg Silicon
Double `Exposure’
9/15/05
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HNN
CDMS
Reject Multiple Interactions
FET cards
SQUID cards
WIMPs
Backgrounds
don’t
scatter
oftentwice
do
4K
0.6 K
0.06 K
0.04 K
ZIP 1 (Ge)
ZIP 2 (Ge)
ZIP 3 (Ge)
ZIP 4 (Si)
ZIP 5 (Ge)
ZIP 6 (Si)
9/15/05
14C
14C
14C
Penn State Colloquium
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
n, 
48
HNN
CDMS
First Run
Prior to timing cuts
After timing cuts, which
reject external electrons
10.4 keV Gallium line
External e
(address with timing cuts)
B. Cabrera
9/15/05
Nuclear Recoils
induced
by a neutron source
Penn
State Colloquium
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HNN
CDMS
External e : surface events, ionization missed
External e
 decay contamination,
escaping compton recoils
Ionization not collected
z
Electrode
Germanium
Implants

E
`ZIP’ : `reconstruct’ z with start time, risetime
9/15/05
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HNN
CDMS
External e
 decay contamination,
Edge
Induces
escaping compton
recoils
Phonon Energy
Downshift
Phonon Sensors
Distinct Sensor
Sharing
0
9/15/05
Primary Phonons
Lower Energy
Eventually
energy low,
`High Energy,’
Phonons Have
pathlength
long,
`Rayleigh
Scatter’
Longer Pathlength,
`phonons
ballistic’
so theygodiffuse
Diffuse More Promptly
+ energy downshift
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HNN
Timing rejects surface/external e
CDMS
Nuclear Recoils
e
External e
9/15/05
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HNN
CDMS
WIMP search data with Ge detectors
Z2, Z3, Z5
Prior to timing cuts
After timing cuts, which
reject external electrons
10.4 keV Gallium line
B. Cabrera
9/15/05
(yellow points are from neutron calibration)
State Colloquium
Nuclear RecoilsPenn
induced
by a neutron source
53
HNN
CDMS
All the features on one plot
Z2, Z3, Z5
10.4 keV Gallium line
Surface
Rejection:
Omitted
Applied

10 keV
threshold
(1 20 keV)
9/15/05
0.7  0.35 external e,
0.07 recoils from neutrons expected
2/3 event expected from Barium calib
Penn State Colloquium
Energy
Estimate
Corrected
(non-blind)
54
HNN
CDMS
Second Run – twice the exposure
After timing cuts, which
reject most electron recoils
Prior to timing cuts
1.5
1.5
Z2/Z3/Z5/Z9/Z11
Ionization Yield
Ionization Yield
10.4 keV Gallium line
1.0
1.0
0.5
0.5
1 candidate
(barely)
0.0
0
Z2/Z3/Z5/Z9/Z11
10
20
30
40 50
60
70
80
Recoil Energy (keV)
9/15/05
90 100
0.0
0 10
20
30 40
1 near-miss
50 60 70
80 90 100
Recoil Energy (keV)
ESTIMATE: 0.37 0.20 (sys.)  0.15 (stat.) surface
electron recoils,
0.05 recoils from neutrons expected
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HNN
CDMS
Limits
DAMA
9/15/05
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HNN
CDMS
The Near Future
Installed 3 additional
towers November
2004

Improvements



30 detectors in 5 towers of 6


9/15/05
Cryogenics, backgrounds,
DAQ
Currently commissioning
4.75 kg of Ge, 1.1 kg of Si to
run through 2006
Improve sensitivity x10
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HNN
CDMS
Sensitivity Expectations: Distant Future
9/15/05
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HNN
CDMS
Projected Sensitivies
9/15/05
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HNN
CDMS
CDMS Collaboration(March 2002)
9/15/05
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HNN
DAMA – 100 kg of NaI
CDMS
Sodium, A=23
Eobs(KeVee)0.25 Erecoil (KeV)
Erecoil  Light
Iodine, A=127
Eobs(KeVee)0.09 Erecoil (KeV)
Copper
9/15/05
NaI
Lead
PMT
PMT
vk = 15 km/s
Poly
Penn State Colloquium
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HNN
CDMS
DAMA Background and Signal
0.01950.031
-0.00010.019
cpd/kg/keV
Energy Spectrum
Bkgd  1 cpd/kg/keV
2-6 KeV
8-24 KeV Na(23)
20-70 KeV I(127)
through
through2000
2003…
…4
6.3 
Bernabei et al., astro-ph/0307403
9/15/05
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HNN
Similar Exposure… Stanford Site
Surface electrons
 Z1 () or Z5 (+)
Nuclear Recoils
9/15/05
Penn State Colloquium
CDMS
Neutrons!!
Soudan rock
filters the muons
that make them
(but not WIMPS)
63
HNN
CDMS
Limits
DAMA 1-4
58,000 kg-days
CDMS
Stanford
Edelweiss
Non-blind
blind
(10’s of
kg-days)
Various Models
9/15/05
Penn State Colloquium
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