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Cryogenic Dark Matter Search
Harry Nelson
UCSB
Journal Club
March 12, 2004
HNN
CDMS Collaboration
Brown University
Stanford University
M. Attisha, R.J. Gaitskell, J-P. Thompson
Case Western Reserve University
D.S. Akerib, M.R. Dragowsky,
D.Driscoll, S. Kamat, T.A. Perera, R.W.
Schnee, G.Wang
Fermi National Accelerator Laboratory
D.A. Bauer, M.B. Crisler, R. Dixon, D.
Holmgren, E. Ramberg
Lawrence Berkeley National Laboratory
J.H Emes, R.R. Ross, A. Smith
Princeton University
T. Shutt
Santa Clara University
B.A. Young
3/12/04
UCSB
Cryogenic
Dark
Matter
Search
L. Baudis, P.L. Brink, B. Cabrera,
C. Chang, W. Ogburn, T. Saab
University of California, Berkeley
M.S. Armel, A. Lu, V. Mandic,
P.Meunier, N. Mirabolfathi, W. Rau, B.
Sadoulet, D. Seitz, A. Spadafora, K.
Sundqvist
University of California, Santa Barbara
R. Bunker, D.O. Caldwell, R. Ferril, R.
Mahapatra, H. Nelson, J. Sander, C.
Savage, S. Yellin
University of Colorado at Denver
M. E. Huber
University of Minnesota
P. Cushman, L. Duong, A. Reisetter
Cornell Journal Club
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HNN
UCSB
Plan
z
Massive Dark Matter
z
Direct Detection
z
The ZIP Detector
z
Data
z
Future
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Primack Pyramid
UCSB
We are 1 in 10,000 of the
energy in Universe…
Our form of matter less than
dark matter by factor of 5 or
so in energy...
Who ordered that?
3/12/04
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Leading Thinkers
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UCSB
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z
Origin of Dark Matter
During inflation
⟩
⟩
Axion, superpartner Axino
*Zillas
→Could
⟩
z
UCSB
have only gravitational interactions!
Few constraints…
During thermal equilibration phase of Big Bang…
⟩
⟩
3/12/04
m > few keV (currently observed large scale structure)
m > 10 or so GeV (nothing new at accelerators)
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UCSB
Candidates
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UCSB
Coincidence or Clue… `WIMP’
’
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WIMP/nucleon σ≈10-42 cm
UCSB
Exper.
CDMS
DAMA
Theory
SUSY: various constraints
including Big Bang
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Galactic Dark Matter
UCSB
R is the distance from center
v
v is the speed (tangential)
R
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HNN
UCSB
The Dark Ball
Bulge
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Disk
Cornell Journal Club
Dark Matter
`Halo’ (aka Aura)
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HNN
UCSB
What about our home galaxy (Milky Way)?
χ
χ
χ
χ
χ
χ
χ
χ
χ
χχ
χ
χ
χ
χχ
χ
χ
χ
χ
χ
χ
χ
χ
χ
χ
Honma and Sofue, 1996
v
220 km/s
Without the Dark Halo
(Binney & Tremaine)
∆:v0=180 km/s
⊕
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R
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From Galactic Astrophysics…
z
Local energy density, speed of DM
MeV
ú 0 ø 300
3
cm
0? (200-2000)
z
UCSB
DM at rest:
3/12/04
km
v 0 ø 220
(ì 0 ø 7 â 10 à4)
s
(ì 20 ø 12 â 10 à6)
(170-270)
⟨vDM⟩=0 (sun plowing through at v0 ≈ 220 km/s)
2 ⟩1/2 ≈ 300 km/s… useful to approximate ≈ 0
⟨vDM
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Direct Detection: Signal and Main Background
Signal
Nucleus
Recoils
Background
Electron
Recoils
Er
v/c ≈ 7×10-4
dense energy deposition
ionization efficiency low
distinct ionization energy scale
0
χ (calibrate: neutron)
3/12/04
UCSB
γ
Er
v/c ≈ 0.3
Sparse Energy Deposition
Differences the
Basis of Particle ID
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Rate of Main Background
UCSB
≡ DRU
• Shield (shield radioactive too!)… 1 ev/(kg d keV) typical
• Reduce the background… HDMS , IGEX , Genius
• Exploit astron. properties (year cycle, directionality) DAMA, DRIFT
• Devise detectors that can distinguish nuclear recoil from electron
recoil… Edelweiss, CDMS, Xenon..
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HNN
UCSB
Nuclear Recoil – Cross Section
∝A4
`scalar’ or SI (Spin Independent)
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HNN
Nuclear Recoil – Diffraction
UCSB
Iodine
(A=127)
DAMA
0 110 220 330 keV ER
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HNN
UCSB
Nuclear Recoils from Massive Dark Matter
z
Deposit 10’s of keV; high target A favored
z
Target A<<160, dark matter velocity spectrum a
delta-function, recoil spectrum flat up to endpoint.
z
Dark matter spectrum roughly maxwellian…
recoil spectrum ends up exponentially falling
z
Form factor of nucleus directly appears in recoil
spectrum
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UCSB
Copper
NaI
Lead
PMT
DAMA – 100 kg of NaI, no particle ID
PMT
HNN
Poly
Sodium, A=23
Eobs(KeVee)≈0.25 Erecoil (KeV)
Erecoil → Light
Iodine, A=127
Eobs(KeVee)≈0.09 Erecoil (KeV)
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Annual Modulation in Rate
UCSB
• `Usual Simplification’: Halo particles are at rest, on average 2 1/2
⟨vDM⟩ =0 km/s
• Sun moves through Halo - `apparent’ wind
• Earth modulates `wind’ velocity yearly
v k = 15 km/s
2
⟨vDM⟩1/2 ≈ 300 km/s
Fig. from DRIFT
DAMA at Gran Sasso
Peak-to-peak up to 40%
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DAMA Background and Signal
UCSB
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…
…4σ
6.3 σ
Bernabei et al., astro-ph/0307403
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UCSB
DAMA
noise...
>1 pe threshold
<10-4 cpd...
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Particle ID/Discrimination (by DRIFT)
40 keV Ar in 1/20 atm Ar
UCSB
13 keV e- in 1/20 atm Ar
Ar pushes other Ar atoms,
none go very far.
Electron pushes other
electrons, all go far
5 cm
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UCSB
Discrimination Techniques
1) Time Structure of the Pulse
2) Pulse Height/Area via:
• Ionization (like Ge)
• Scintillation (like NaI)
• Heat/Phonons
• Physical Size of Ionization
Liquid Xenon
Also a scintillator
1
0.1
(Spooner)
0.01
e- recoils from γ’s
0.001
0.0001
NaI
0.00001
1
NaI
10
100
pulse time constant (ns)
1
Nuclear recoils
From neutrons
γ’s
0.1
DAMA does
not use this
10-20keV
(50-100 keV ER)
0.01
0.001
ER:
130-150 KeV (I)
⟨t⟩
0.0001
0.00001
1
1
Gerbier et al., 1998
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Width of pulse
Cornell Journal Club
10
10
pulse time constant ns
⟨t⟩ (ns)
100
100
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Catalog of Recoil Experiments
UCSB
Rick Gaitskell
3/12/04
Cornell Journal Club
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CDMS Technique: Phonons v. Ionization
Nuclear recoils
(induced by a neutron source)
UCSB
Electron recoils
(induced by a γ source)
Slope really 1!
Ionization
=1
(bkgd)
≈1/3
(sig)
Phonons
Egap = 3/4 eV
w = 3 eV
(Ge)
Shutt et al., 1992
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Our Detectors (Ge/Si 30 mK)
UCSB
Phonon D
SQUID array
Rbias
One side: `Phono cathode’
Transition Edge Sensors
Segmented for x,y imaging
Rfeedback
I bias
D
A
C
B
Q outer
Q inner
Vqbias
7.5 cm
3/12/04
Other side: charge collection
2 segments to reject edge events
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The ZIP Phono`cathode’...
1 µ tungsten
UCSB
380µ x 60µ aluminum fins
• 4 segments + timing to get x,y on the face
• rise time to get z, into the face
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UCSB
Technology of `ZIP’s (Z for z)
The `phono-cathode’…
quasiparticle
trap
W
quasiparticle
Transition-Edge
diffusion
Sensor (TES)
Al Collector
Cooper Pair
Al
Si or Ge
phonons
~ 10mK
RTES (Ω)
• Signal much faster microseconds
• 3-d imaging (Z)
4
3
2
1
superconducting
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normal
Cornell Journal Club
Tc ~ 80mK
T (mK)
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UCSB
Pulses
Charge (Q)
• Charge signals are virtually
instantaneous
20 keV
Phonons (P)
µ = 10.4 keV
σ = 0.34 keV
• Phonon start times are
measured relative to charge
signal
• Can `triangulate’ timing to
reconstruct x, y…
• Risetime gives z (along thin
direction of detector)
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Calibration Data
UCSB
1334 Photons (external source)
233 External Electrons (β)
(tagged contamination)
616 Neutrons (external source)
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Incomplete Ionization Collection...
External β
z
Electrode
Germanium
Implants
UCSB
Ionization electrons
get trapped in this
electrode
1
E
Those electrons never drift over to the
other electrode… ionization signal
reduced… but, all the phonons/heat still
present… (ionization)/(phonons) < 1
Measure z with pulse
risetime
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ZIP Surface
Electron
Rejection
UCSB
(Single-scatter)
Neutrons Surfaceelectron recoils photons from
from
(selected via nearest- 60Co Source
252Cf
neighbor multiple
source
scatters from 60Co
source)
Accept
Surface electrons
still likely to be the
limiting background
3/12/04
Reject
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UCSB
Signal Shape
∝A2
Nucleus
Recoils
MWIMP=100 GeV
σ = 10-42 cm2/nucleon
Silicon, Sulphur
Germanium
Iodine, Xenon
Er
Slope: Maxwell-Boltzmann
Diffraction off Nucleus
WIMPs in Galaxy
χ0
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UCSB
CDMS Sites
Stanford (through 2002):
• 17 mwe - shallow
• Substantial neutron flux
• Results (28 of 50 kg-d)
scintillator
veto
polyethylene
outer moderator
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outer Pb shield
detectors
Icebox
inner Pb
shield
Soudan Site (online 10/2003):
• 2100 mwe
• Neutron flux down 1/300
• 30 kg-d bkgd-free
dilution
• Mass just roughly doubled
refrigerator
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Shallow Site Data
UCSB
Just one detector hit
FET cards
SQUID cards
4K
0.6 K
0.06 K
0.02 K
ZIP 1 (Ge)
ZIP 2 (Ge)
ZIP 3 (Ge)
ZIP 4 (Si)
ZIP 5 (Ge)
ZIP 6 (Si)
Surface electrons
‹ Z1 (×) or Z5 (+)
8 cm
NR Band (22)
4 Germanium Detectors (0.66 kg total)
2 Silicon Detectors (0.2 kg total)
→ Small DM rate, high neutron rate
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CDMS: not deep… neutron background
UCSB
17 mwe
µ
µ
Active Muon Veto
Pb Shield
n
Copper
n
Fridge
Polyethylene
Detectors
Inner Pb shield
... Experiment moved to Soudan,
2100 mwe depth
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More Proof: Multiple Scattering
photons
Nonneighbor
doublescatter U
Triplescatter
z
z
z
•
3 here + MC:
16±9 single scatter
see 22-2=20
3/12/04
neutrons
Cornell Journal Club
UCSB
Size & color indicates yield in third detector
HNN
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HNN
Candidate Energy Spectrum
UCSB
Expected shape if detection
efficiencies were 100%, neutrons
Expected spectrum including
detection efficiencies, normalized
to expected # of events
(resembles 20 GeV WIMP!!)
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UCSB
Limits
90% CL upper limits assuming standard halo, A2 scaling
ZEPLIN
-I
New CDMS
limits, 28 kg-d
no bkgd sub,
w/bkgd sub,
expected
er
p
p
U
iss
e
w
×
Lim
it
el
d
E MSSM models
300X lower neutron background expected at Soudan… have 30 kg-d
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UCSB
Soudan
2341 ft of hard
rock shielding
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UCSB
More Soudan
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Soudan Calibration Data Looks Good
Californium Source (n and gamma)
UCSB
Barium Source (gamma)
… 30 kg-d `low background’ collected, processed,
blinded…. results April??
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HNN
UCSB
Where should we get?
For more limit curves, see
http://dmtools.berkeley.edu, Gaitskell & Mandic
Current CDMS Limit
eis
w
l
e
Ed
mit
i
L
sion
u
l
c
s Ex
SUSY gµ-2
(Baltz&Gondolo,
PRL 86 (2001) 5004)
No SUSY gµ-2
constraint
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Cornell Journal Club
Expected sensitivity of
completed CDMS run at
Soudan (5x better than
current limit).
Projected sensitivity for
CDMS at Soudan, with 5
towers 4 kg Ge, 1.5 kg Si:
0.1 events/kg/keV/year
(100x better than current
limit).
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Lots of competition...
UCSB
Rick Gaitskell
HNN
3/12/04
Cornell Journal Club
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HNN
Prognostication
3/12/04
Cornell Journal Club
UCSB
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