the majorana demonstratorpotato/artfest/talks/major... · 2014. 5. 30. · the majorana...
TRANSCRIPT
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THE MAJORANA DEMONSTRATOR
Ryan Martin, University of South Dakota (Art’s last PhD student)
ArtFest Symposium,Queen’s University, Kingston, Canada
30th May 2014
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Outline
• Neutrinoless double-beta decay• Germanium detectors• The MAJORANA DEMONSTRATOR
experiment• Anecdote about Art
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Neutrinos in the standard model
• 3 “flavors” of neutrinos• Interact only through the Weak
interaction• Lepton number to distinguish
neutrinos and anti-neutrinos
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What we don’t know about neutrinos
0νββ experiments can address!
• CP violating?• Steriles?• Mass (only differences are known)• Hierarchy (which is heaviest?)• Dirac or Majorana (are they their own anti-particle?)
∆m2(solar)
∆m2(atmospheric)ν3
ν1
ν2
ν3
ν1
ν2mass
or“normal” “inverted”?
?
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(Neutrinoless) double beta decay
• Double-beta decay possible in a handful of isotopes
• Energy of electrons can be detected
Electron energy
Look for this (tiny) peak!
2 neutrinos no neutrinos
Isotope Q (MeV) Abundance (%)48Ca→48Ti 4.3 0.276Ge→76Se 2.0 7.882Se→82Kr 3.0 9.296Zr→96Mo 3.4 2.8100Mo→100Ru 3.0 9.6110Pd→110Cd 2.0 11.8116Cd→116Sn 2.8 7.5124Sn→124Te 2.2 5.6130Te →130Xe 2.5 34.5136Xe →136Ba 2.5 8.9150Nd →150Sm 3.4 5.6
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Experimental searches for neutrinoless double beta decay
background rateenergy resolution
mass live-timeabundance
Detect eff.
• Perform a “counting experiment”:o If no counts are seen, the half-life is at least as long as…
Sensitivity:
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Semiconductor detectors
Q
Qγ γ
GeEgE
nerg
y C.B
V.Be-
e-
Measure total Q to get Energy:
• Number of electron-hole pairs:
• Energy resolution:εγE
N =
FNE ∝∆
For Ge:
• For 2MeV:
1.0,95.2 ≈= FeVε
000,700≈N
%1.0≈∆
EEFWHM
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Semiconductor detectors
Ge
• Apply E-field to collect charges• Low noise preamp to measure charge and obtain good energy resolution
E
HV
Charge sensitive preamp
EgEne
rgy C.B
V.Bh
e-
_ _ _ + + +_ _ _
+ + +
t
Q~ E
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+Vb(-Vb)
planar
Coaxial
p (n)p+ (n+)
n+ (p+)
“Classic” germanium detectors
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“PPC” detectors• P-type Point Contact HPGe
detectors• “Novel” technology• Small point contact to readout
charge, low capacitance, low noise
• Thick outer contact (n+, lithium diffused), strongly attenuates alphas
Semi coaxial detector
Point contact detector
Weightingpotential
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Properties of PPCs
• Sharp weighting potential allows multi-site events to be identified
• Gamma rays at 2MeV typically scatter more than once
• Small capacitance results in low noise and excellent performance at low energies
1332 keVmulti-site event in a PPC detector
PRL 101 251301 (2008)
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Germanium for neutrinoless double-beta decay experiments
Germanium detectors
• Source is detector• Good energy resolution• Well established technology• Intrinsically ultra-clean (high-
purity germanium)
76Ge isotope for 0νββ
• Q-value of 2039keV above most backgrounds
• Can be enriched to >86% in 76Ge (nat. abundance ~ 8%)
• Slow 2νββ rate (1021 yr)
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The MAJORANA DEMONSTRATOR
• An R&D project towards a tonne scale neutrinoless double-beta decay germanium experiment
• Goals:• Demonstrate backgrounds low enough to justify building a tonne
scale experiment• Establish feasibility to deploy a modular Ge array• Search for additional physics beyond the Standard Model (e.g. Dark
Matter, axions, etc.)• Have agreement to work with GERDA on optimal design of tonne scale
experiment
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The MAJORANA DEMONSTRATOR
• 40kg of PPC detectors, up to 30kg enriched to >86% 76Ge• 2 cryostats made of copper electroformed underground, 7
strings of 3-5 detectors per cryostat• Low-background passive Cu and Pb shield with active muon
veto
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MJD Schedule
MJD is proceeding in 3 phases• Prototype Module (Nov 2013):
o Commercial copper, 2 strings natGeTest mechanical designTest detector performance
• Module 1 (Summer 2014):o Electroformed copper, 20kg of enrG
• Module 2 (Summer 2015):o Electroformed copper, 10kg of enrG
Prototype cryostat
Cryostat 1 and 2
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Aside: Schedule for finishing a thesis
Art’s last 3 (inherited) PhD students. All “encouraged” to finish up their thesis in a timely manner…
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MJD status and technologies
• Enriched detector
processing
• Electroformed copper
• Electronics readout
• Underground lab and status
• Simulation and backgrounds
The Sanford Underground Research Facility, in Lead, SD
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Enriched germanium processing
Enrichment to >86% at Electro-Chemical Plant (ECP) in Russia
Reduction to Ge metal at Electrochemical Systems Inc. (ESI)
Zone-refinement by commercial vendor
Detector fabricationPull crystal by commercial vendor
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Status of enriched detectors• Have produced 30 enriched
detectors, 25kg.• These are underground and
have been tested• Performance of detectors is
excellent so far• Enrichment nearly 88% 76Ge
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Enriched detector P42575B
SignalBackground
Detector performance
232Th calibration data from enriched detector shows that with pulse shape analysis cut:• Remove 90% of multi-site events (full energy peaks), background-like• Retain 90% of single-site events (208Tl double escape peak), 0νββ-like
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The cleanest copper in the world
The temporary clean room at SURF (4850)
Copper being electroformed on a stainless steel mandrel
A clean machine shop underground
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Instrumenting germanium detectors
Detector unit from first underground string
JFET
aGe resistorcapacitor“pico coax”
Det.
LMFE Cable Preamp
• Developed ultra-low background low noise readout
~2cm
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Underground lab
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MJD Simulations
• Detailed Monte Carlo model to simulate backgrounds from 3800 components and detailed verification campaign
• ~60kCPU hours of simulations (PDSF)• U, Th, K chains for all components and 68Ge, 60Co for select components• Dominant contribution at Qββ is from multi-site events from U and Th (214Bi,
208Tl)
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Summary
o Very exciting time!o Started taking data
undergroundo Will start assembly of
the enriched detector array soon
o Rich physics program with Ge detectors
The MAJORANA Collaboration, April 2013 at SURF
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The MAJORANA Collaboration
Black Hills State University, Spearfish, SDKara Keeter
Duke University, Durham, North Carolina , and TUNLMatthew Busch, James Esterline, Gary Swift, Werner Tornow
Institute for Theoretical and Experimental Physics, Moscow, RussiaAlexander Barabash, Sergey Konovalov, Vladimir Yumatov
Joint Institute for Nuclear Research, Dubna, RussiaViktor Brudanin, Slava Egorov, K. Gusev,
Oleg Kochetov, M. Shirchenko, V. Timkin, E. Yakushev
Lawrence Berkeley National Laboratory, Berkeley, California andthe University of California - Berkeley
Nicolas Abgrall, Mark Amman, Paul Barton, Yuen-Dat Chan, Paul Luke, Susanne Mertens, Alan Poon, Kai Vetter, Harold Yaver
Los Alamos National Laboratory, Los Alamos, New MexicoMelissa Boswell, Steven Elliott,, Johnny Goett, Keith Rielage, Larry
Rodriguez, Harry Salazar, Wenqin Xu
North Carolina State University, Raleigh, North Carolina and TUNLDustin Combs, Lance Leviner, David G. Phillips II, Albert Young
Oak Ridge National Laboratory, Oak Ridge, TennesseeFred Bertrand, Kathy Carney, Alfredo Galindo-Uribarri,
Matthew P. Green, Monty Middlebrook, David Radford, Elisa Romero-Romero,Robert Varner, Brandon White, Timothy Williams, Chang-Hong Yu
Osaka University, Osaka, JapanHiroyasu Ejiri, Ryuta Hazama, Masaharu Nomachi, Shima Tatsuji
Pacific Northwest National Laboratory, Richland, WashingtonJim Fast, Eric Hoppe, Richard T. Kouzes, Brian LaFerriere, John Orrell, Nicole Overman
Shanghai Jiaotong University, Shanghai, ChinaJames Loach
South Dakota School of Mines and Technology, Rapid City, South DakotaAdam Caldwell, Cabot-Ann Christofferson, Stanley Howard,
Anne-Marie Suriano, Jared Thompson
Tennessee Tech University, Cookeville, TennesseeMary Kidd
University of Alberta, Edmonton, AlbertaAksel Hallin
University of North Carolina, Chapel Hill, North Carolina and TUNLGraham K. Giovanetti, Reyco Henning, Mark Howe, Jacqueline MacMullin, Sam Meijer, Benjamin Shanks, Christopher O’Shaughnessy, Jamin Rager, Jim Trimble, Kris Vorren,
John F. Wilkerson
University of South Carolina, Columbia, South CarolinaFrank Avignone, Vince Guiseppe, David Tedeschi, Clint Wiseman
University of South Dakota, Vermillion, South DakotaDana Byram, Ben Jasinski, Ryan Martin, Nathan Snyder
University of Tennessee, Knoxville, TennesseeYuri Efremenko, Sergey Vasilyev
University of Washington, Seattle, WashingtonTom Burritt, Micah Buuck, Clara Cuesta, Jason Detwiler, Peter J. Doe, Julieta Gruszko,
Ian Guinn, Greg Harper, Jonathan Leon, David Peterson, R. G. Hamish Robertson, Tim Van Wechel
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Thank you!
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MJD Sensitivity
30 kg y