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Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 3 Dark Matter WIMPs The Science –Scientific case compelling for dark matter WIMPs both from particle physics side and astrophysics side Galaxy formed in dark matter gravitational potential –Our solar system rotates through swarm of WIMPs 10 9 /cm 2 /s –These would only interact with nuclei not electrons ~ (m N /m e ) 2 –Nearly all backgrounds interact with e’s produced by gammas CDMS II detectors and program –Tower 1 (4 Ge and 2 Si detectors) at SUF (neutron limited) –Same Tower 1 at Soudan - PRL 93, (2004) best by x4 –Towers 1& 2 (2004) and Towers 1-5 (2005) - x20 (n limited) SuperCDMS detectors and program –Development Project - 5 kg Ge new detectors run at Soudan –Phase A (25 kg Ge) & Phase B (150 kg Ge) run at SNOLab –Can run 1000 kg Ge at SNOLab before neutron limited Conclusions: to succeed need SLAC technical and management experience
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Blas Cabrera - Stanford University SLAC Experimental Seminar Page 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search) Extending the search for dark matter WIMPs beyond CDMS-II with SuperCDMS SLAC Experimental Seminar November 17, 2004 Blas Cabrera CDMS Collaboration At Stanford: Paul Brink, Laura Baudis (now at U Florida), Jodi Cooley, Clarence Chang, Walter Ogburn, Matt Pyle, Daniel Soto, Betty Young (SCU),
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Page 1: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 1

The Search for Dark Matter in the form of WIMPs:CDMS (Cryogenic Dark Matter Search)

Extending the search for dark matter WIMPsbeyond CDMS-II with SuperCDMS

SLAC Experimental SeminarNovember 17, 2004

Blas Cabrera

CDMS Collaboration

At Stanford: Paul Brink, Laura Baudis (now at U Florida), Jodi Cooley,Clarence Chang, Walter Ogburn, Matt Pyle, Daniel Soto, Betty Young (SCU),

Pat Castle, Astrid Tomada and Larry Novak

Page 2: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 2

CDMS Collaboration

UC Berkeley, Stanford, LBNL, UC Santa Barbara,Case Western Reserve U, FNAL, Santa Clara U, NIST, U Colorado Denver, Brown U, U Minnesota,U Florida, Princeton

Page 3: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 3

Dark Matter WIMPs• The Science

– Scientific case compelling for dark matter WIMPs both from particle physics side and astrophysics side

• Galaxy formed in dark matter gravitational potential– Our solar system rotates through swarm of WIMPs 109/cm2/s– These would only interact with nuclei not electrons ~ (mN/me)2

– Nearly all backgrounds interact with e’s produced by gammas• CDMS II detectors and program

– Tower 1 (4 Ge and 2 Si detectors) at SUF (neutron limited)– Same Tower 1 at Soudan - PRL 93, 211301 (2004) best by x4– Towers 1& 2 (2004) and Towers 1-5 (2005) - x20 (n limited)

• SuperCDMS detectors and program– Development Project - 5 kg Ge new detectors run at Soudan– Phase A (25 kg Ge) & Phase B (150 kg Ge) run at SNOLab– Can run 1000 kg Ge at SNOLab before neutron limited

• Conclusions: to succeed need SLAC technical and management experience

Page 4: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 4

timeThe BIG questions

?What is the

Origin of the Universe?

What role did Quantum Gravity play in the birth of the Universe?

The fabric of Space & Time: Was Einstein right?

How did Black Holes form in the early Universe?; Are Gamma Ray Bursts related to Black Holes?

What is Dark Matter? Does Dark Energy really exist?

How did Galaxies form? Which came first, Black Holes or Galaxies?

How does our star work? Is Life in our galaxy unique?

What is the ultimate fate of the Universe?

Page 5: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 5

Expanding universe - simulations and data

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

Page 6: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 6

Concordance Model of Cosmology

• Supernovae + Cosmic Microwave Background + Large Scale Structure

• Great overall success!

• However raises even more questions about origin of dark energy

Dark Energy density

Matter density

WMAP + flat : Ωm = 0.27 ± 0.04 ΩΛ = 0.73 ± 0.04

Page 7: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 7

Composition of the Cosmos

WIMPs

WMAP best fit

Page 8: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 8

Strong motivation• Cosmology

– Theory:– Observation:

• Nuclear Physics: baryons - p, n, e– Theory of formation of H, D, He, Li– Observations:

• Astronomy: luminous matter– Stars & gas

• Baryonic dark matter is necessary: MACHOs at most 20% of halo mass

• Non-baryonic dark matter dominates universe hot cold

axionsneutrinosmonopolesWIMPs

X√

√√

Supersymmetry LSP

~1√?X√ √

best DMcandidates

ρ ρcrit = Ωm; Ωm + ΩΛ =1; ΩΛ ≠ 0 still ugly!

0.25 ≤ Ωm < 0.30

lum ≈ 0.005 0.01 0.1 1

lumDM, B

B DM, ≠B

m Λ

But favored bysupernova data

0.03 < ΩB < 0.05

χ =N10* ˜ B + N20

* ˜ W 3 + N30* ˜ H 1

0 + N40* ˜ H 2

0

Page 9: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 9

The Signal and Backgrounds

χ0

v/c 710-4

NucleusRecoils

Er 10’s KeVphonons

Signal (WIMPs)

Er

v/c 0.3

ElectronRecoils

Background (gammas)

Er

ionization

Surface electrons from beta decay can mimic nuclear recoils

Neutrons also interact with nuclei, but mean free path a few cms

Page 10: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 10

Direct Detection of Neutralinos

• [e. g., Lewin & Smith; and Jungman, Kamionkowski & Griest]

• The observed differential rate of events is given by

• For a Maxwell distribution of incident velocities

dRdQ

=σ0 ρ0

π v0 m χ mρ2 F

2 Q( )T Q( )η Q( )

T Q( ) =exπ −vmin v0( )2

[ ] wηeρe vmin = Qm N mρ

η Q( ) is the detector efficiency as a function of Q

R in evts/kg - d, typically σ 0, scalar >> σ 0, spin; ρ 0 WIMP (χ ) at earth, ~ 0.3 GeV/cm3

v0 velocity of sun around galaxy, ~ 220 km/s

mχ , mN mass of neutralino & nucleus, mr =mχ mN

mχ + mN

; recoil energy Q = mr2 v2

mN

1− cosθ *( )

Page 11: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 11

• To compare the coherent rates of different materials

• We define the fundamental WIMP-nucleon cross section

• Two target materials such as Si and Ge very powerful

mχ =40 GeV

σ0,σχalaρ=5×10−42 χm2neutronbackground

σ0 scalar =4mχ

2 mN4

π mχ + mN( )2

fn

mn

⎛ ⎝ ⎜ ⎞

⎠ ⎟2

, where fn ≅ fp is the WIMP - nucleon coupling

σ0 W n

mrχ n2 =

fn2 =

σ 0 scalar

A2 mrχ N

2 , which gives σ 0 Wn in terms of σ 0 scalarwith A ≅ mN mn

Spin independent scalar cross section

Page 12: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 12

Nuclear form factor suppression

• For spin-independent or coherent interactions the form factor F2(Q) suppression is shown below and results in suppressed rates for heavy nuclei

50 keV true nuclear recoil threshold is equivalent to about 5 keVee recoil

F Q( ) =3

j1 Qρn / ηχ( )Qρn /ηχ

exπ −Qσ/ηχ( )2 /2[ ], wηeρe ρn ≈ 0.89A1 3 + 0.3( ) fm and σ~1 fm

Page 13: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 13

Summary and bold future visionLimit at SUF 2002(during CDMS II)

Development Project 5 kg of Ge 2008

SuperCDMS Phase C 1000 kg of Ge

World-best limit today

SuperCDMS Phase A 25 kg of Ge 2011

CDMS II goal 2006

SuperCDMS Phase B 150 kg of Ge 2014

Page 14: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 14

CDMS ZIP Detectors (Ge/Si)

Qinner

Q outer

A

B

D

C

Rbias

Ibias

SQUID array Phonon D

Rfeedback

Vqbias

Phonon sensors (4) (TES)

Ionization Electrodes (2)x-y-z imaging:

from timing, sharing

WIMPs: σ(Ge) >> σ(Si)

Neutrons: σ(Ge) ~ σ(Si)

Page 15: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 15

380 mm Al fins

60 mm wide

~25% QP collection eff.

o TES’s patterned on the surface measure the full recoil energy of the interaction

o Phonon pulse shape allows for rejection of surface recoils (with suppressed charge)

o 4 phonon channels allow for event position reconstruction

ZIP detector phonon sensor technology

Page 16: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 16

The ZIP Detector Signal• Charge & Phonon signals occur on a similar timescale• Phonon pulse time of arrival allows for event position

reconstruction• 20 keV event in a Si & Ge ZIP

Si ZIP Ge ZIP

(EXCELLENT S/N FOR 20 KeV TRUE RECOIL ENERGY)

Page 17: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 17

Am241 : 14, 18, 20, 26, 60 kev

Cd109 + Al foil : 22 kev

ZIP Phonon Position Sensitivity

Delay Plot

A D

CB

Page 18: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 18

First operate at SUF (17 mwe)• At SUF

– 17 mwe– 0.5 n/d/kg

• At Soudan– 2090 mwe– 0.8 n/y/kg

• At SNOLab– 6060 mwe– 1 n/y/ton

Log 1

0(Muo

n Fl

ux) (

m-2s-1

)

Depth (meters water equivalent)

Page 19: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 19

ZIP 1 (Ge)ZIP 2 (Ge)ZIP 3 (Ge)ZIP 4 (Si)ZIP 5 (Ge)ZIP 6 (Si)

SQUID cards

FET cards

4 K

0.6 K0.06 K0.02 K

The shallow Stanford Underground Facility (SUF)

• Tower 1 operated at SUF during calendar 2002 at a depth of 17 mwe sufficient to eliminate the hadronic component of cosmic rays

Page 20: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 20

Recoil [keV] vs Charge [keVee]

Yellow252Cf

Blueµ coin

Redµ anti

Page 21: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 21

Tower 1 (4 Ge and 2 Si detectors) at SUF

• SUF Run 21– Calendar 2002– 52.6 kg-d of Ge after

cuts• Saw 19 nuclear recoils

– clean separation of gamma & beta events

– See 10 keV and 67 keV lines for energy calibration

• All consistent with neutrons– Consistent ratio of Ge

singles to Ge multiples

– Consistent ratio of Ge events to Si events

– Only gain as sqrt(MT)• TO DO BETTER NEED TO GO

DEEPER

Page 22: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 22

Now operate at Soudan (2090 mwe)

• At SUF– 17 mwe– 0.5 n/d/kg

• At Soudan– 2090 mwe– 0.8 n/y/kg

• At SNOLab– 6060 mwe– 1 n/y/ton

Log 1

0(Muo

n Fl

ux) (

m-2s-1

)

Depth (meters water equivalent)

Page 23: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 23

Outside of the Experiment

plasticscintillators

outerpolyethylene

lead

ancientlead inner

polyethylene

Page 24: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 24

Run 118 (1T) & Run 119 (2T) in Soudan

Page 25: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 25

Phonon energy (prg) in keVPhonon energy (prg) in keV

Excellent agreement between data and Monte CarloExcellent agreement between data and Monte Carlo

Energy calibration of Ge ZIP with 133Ba source

Ionization energy in keVIonization energy in keV

Page 26: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 26

Nuclear recoil calibration of Ge & Si ZIPs with 252Cf

Nuclear recoils in Ge ZIPNuclear recoils in Ge ZIP Nuclear recoils in Si ZIPNuclear recoils in Si ZIP

Excellent agreement between data and Monte CarloExcellent agreement between data and Monte Carlo

Page 27: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 27

252Cf Neutron & Gamma calibration data

• Upper red dashed line are +/- 2 σ gamma band

• Lower red dashed line are +/- 2 σ nuclear recoil band

• Separate high statistics calibrations with 133Ba gamma source

• Determined with calibration data as was the analysis threshold energy

Page 28: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 28

133Ba gamma & 252Cf neutron calibrations• Use phonon

risetime and charge to phonon delay for discrimination of surface electrons “betas”

• Cuts and analysis thresholds determined entirely from calibration data with WIMP search data blinded until after the cuts and thresholds were set.

gammas

neutrons

ejectrons

Page 29: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 29

Example of setting cut with calibration

Calibration - Gaussiandistribution 1000 evts

Data - samedistribution100 evts

Datax10

Calx10

Cut atlast event

Probability0.1 of eventpast cut

On averagearea beyondlast event = 1

On averagearea beyondcut = 0.1

Page 30: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 30

• In 92 days between October 11, 2003 and January 11, 2004, we collected 52.6 live days - a net exposure of 22 kg-d after cuts

• Below data are shown before (left) and after (right) timing cuts

WIMP search data with Ge detectors

(yellow points are from neutron calibration)

Page 31: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 31

CDMS-II Reach with five Towers• We have begun to

explore MSSM cross section range

• DAMA largely ruled out for spin independent scalar interactions (see Gelmini & Gondolo hep-ph/0405278)

• Light mass region suggested by Bottino (hep-ph/0307303) largely ruled out

• Another factor of 3-5 improvement at Soudan past CDMS-II (neutrons)

• THEN MUST GO DEEPER - exploring SNOLab in Canada

EGRET gammas asDM annihilation

astro-ph/0408272

Page 32: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 32

Cryocooler Improvements

• Sumitomo (SHI) RDK415D cryocooler head & compressor

• 1.5 W at 4.2 K• 45 W at 50 K• Cost $50k• First use in dewar

(reduce boiloff)• Second use in Estem

(colder 4 K stage)

Page 33: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 33

Now installing Towers 3, 4 and 5 in Soudan

Page 34: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 34

Completed fabrication & testing of T3-5

Page 35: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 35

Propose to operate at SNOLab (6060 mwe)

• At SUF– 17 mwe– 0.5 n/d/kg

• At Soudan– 2090 mwe– 0.8 n/y/kg

• At SNOLab– 6060 mwe– 1 n/y/ton

Log 1

0(Muo

n Fl

ux) (

m-2s-1

)

Depth (meters water equivalent)

Page 36: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 36

SuperCDMS Roadmap to SNOLAB

Page 37: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 37

Possible SLAC roles• At Stanford we know how to fabricate detectors for 25 kg experiment, but for 150 kg and 1000 kg we need to mass produce the fabrication/mounting

• SLAC could take central responsibility for fabrication with a combination of in house facilities (radon suppression) and commercial production.

• Other major areas include electronics (custom boards), DAQ (with digitizers for 10k channels readout at a 50 Hz for calibrations), computing (first pass data reduction, data analysis and Monte Carlo simulations).

• With Spokesperson for SuperCDMS at Stanford, SLAC could & should take the lead role in project management

Page 38: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 38

Detector development (Paul)• Existing ZIPs3” dia x 1 cm thick

• Thicker ZIPs3” dia x 1” thick(base detector)

• Explore larger ZIPs to 4” dia and up to 4 cm thick

Page 39: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 39

Detector development plans

Page 40: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 40

05

1015

02

46

810-1

-0.5

0

0.5

1

X Position [mm]Z Position [mm]

Interleaved Ionization electrodes concept

• Alternative method to identify near-surface events– Phonon sensors on both sides are virtual ground reference.– Bias rails at +3 V connected to one Qamp– Bias rails at -3 V connected to other Qamp– Signals coincident in both Qamps correspond to events drifted out of the bulk.

– Events only seen by one Qamp are < 1.0 mm of the surface.

Page 41: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 41

Interleaved Ionization electrode design• Design details

– To maintain ~60 pF of capacitance requires keeping bias and ground rails ~ 1 mm apart.

– Phonon sensors ‘contained’ within the (200 mm wide)ground rails.

– First mask-layout recently completed:

Ground ring around side to define the ‘Qouter’ volume containing all surfaces

Page 42: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 42

New Read-out schemes• Two-stage SQUIDs for reading out new phonon sensors

– Allows lower Rn, more TESs, better phonon sensor surface area coverage.• Will improve effectiveness of present phonon risetime cut even further.

– Allows move to Al-Mn TESs to overcome W Tc variability• Resitivity of Al-Mn < W, hence risk /design constraint of electro-thermal oscillation if change-over to two-stage SQUIDs not implemented.

– Commensurate with NIST-style time-domain multiplexing.• ZIP detector phonon pulses are probably sufficiently slow to utilize this scheme effectively to reduce the readout wiring to room temperature that would otherwise be required.

Page 43: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 43

• Two-stage SQUID configuration – Ionization detector transformer-coupled to first-stage SQUID

– Eliminate potential microphonic read-out issues associated with FET readout

– Eliminate IR photon leakage

– Eliminate heated FET load on 4 K

– Transformer ~ 12 mm x 6 mmchip, fabricated at NIST.

– Critically damped circuit, ~1 MHz sampling required.

– Simulations give 0.4 keVee FWHM

Ionization read-out using SQUIDs

Page 44: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 44

How to build a 1000 kg experiment in stages

Page 45: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 45

Schematic of new ‘SNObox’

x3

x3

Exploring cryocooler system with little or no cryogen servicing

Page 46: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 46

Summary and bold future visionLimit at SUF 2002(during CDMS II)

Development Project 5 kg of Ge 2008

SuperCDMS Phase C 1000 kg of Ge

World-best limit today

SuperCDMS Phase A 25 kg of Ge 2011

CDMS II goal 2006

SuperCDMS Phase B 150 kg of Ge 2014

Page 47: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 47

Conclusion• Excellent scientific reach for 1000 kg Ge experiment at SNOLAB with three phases

• SuperCDMS Development Project continues to run Towers 1-5, develops 0.6 kg ZIP detectors, and operates one SNOLAB Tower at Soudan in 2008

• Start SNOLAB installation in 2007 so that detectors can be operated starting in 2009

• SLAC could & should take leadership role in SuperCDMS

Page 48: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 48

Identify and Reduce 210Pb, 14C & 40K

• Use Van de Graaff to attract positive ion radon daughters 222Rn -> 218Po -> 214Pb -> 214Bi -> 214Po -> 210Pb

• Run VdG for 2 hrs• Wipe surface & count

QuickTime™ and aTIFF (Uncompressed) decompressorare needed to see this picture.

QuickTime™ and aTIFF (Uncompressed) decompressorare needed to see this picture.

3.8d 3.1m 27m 20m .16ms

250kV

ground

Page 49: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 49

Quantum Universe• Question 6:

– WHAT IS DARK MATTER?– HOW CAN WE MAKE IT IN

THE LABORATORY?

• “…We need to study dark matter directly by detecting relic dark matter particles in an underground detector and by creating dark matter particles at accelerators, where we can measure their properties and understand how they fit into the cosmic picture.”

Page 50: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 50

Quantum Universe - CDMS!

Page 51: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 51

Quntum Universe - direct detection

• “… The particle nature of dark matter can be verified by finding the rare events they would produce in a sensitive underground dark matter detector such as CDMS. …”

• “However, to understand the true nature of dark matter particles, particle physics experiments must produce them at accelerators and study their quantum properties. Physicists need to discover how they fit into a coherent picture of the universe. Suppose experimenters detect WIMPs streaming through an underground detector. What are they? Are they the lightest supersymmetric particle? The lightest particle moving in extra dimensions? Or are they something else?”

• Did not go the final step of saying that if supersymmetry discovered at an accelerator then we must see if it is the dark matter with direct detection experiments.

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Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 52

Earlier MSSM

Baltz & Gondolo PRD67 065503 (2003)Kim,Nihei,Roszkowski, hep-ph/0208069

Baltz & Gondolo hep-ph/0102147

Page 53: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 53

mSUGRA and relax GUTs

Baer et al, hep-ph/0305191Chattopadhyay et. al, hep-ph/0407039Ellis et al, hep-ph/0306219

Bottino, et al hep-ph/0307303

Page 54: Blas Cabrera - Stanford UniversitySLAC Experimental SeminarPage 1 The Search for Dark Matter in the form of WIMPs: CDMS (Cryogenic Dark Matter Search)

Blas Cabrera - Stanford UniversitySLAC Experimental Seminar Page 54

mSUGRA and Split Supersymmetry

Baltz & Gondolo hep-ph/0407039A. Pierce, hep-ph/0406144 &G. F. Giudice and A. Romaninohep-ph/0406088


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