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Digital Pulse-Shape Discrimination

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Pacific Northwest National Laboratory. U.S. Department of Energy ... Pacific Northwest National Laboratory. 2. 8/21/09. Majorana Overview (http://majorana.pnl.gov) ... – PowerPoint PPT presentation

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Title: Digital Pulse-Shape Discrimination


1
Digital Pulse-Shape Discrimination Detector
Segmentation for the Majorana Project
  • C. E. Aalseth
  • National Security Division,
  • Radiological Chemical Sciences Group
  • Pacific Northwest National Laboratory

2
Majorana Overview(http//majorana.pnl.gov)
  • 0nbb decay of 76Ge potentially measured at 2039
    keV
  • Sensitive to effective Majorana n mass as low as
    0.02-0.07 eV
  • Based on well-known 76Ge detector technology
    plus
  • Pulse-shape analysis
  • Detector segmentation
  • Ready to begin now
  • Requires
  • Deep underground location
  • 500 kg enriched 85 76Ge
  • 210 crystals, 8 segments each
  • Advanced signal processing
  • Special materials (low bkg)

Baseline Concept
3
Physics Motivation for Background Rejection
  • Interaction multiplicity varies with energy, type
    of radiation
  • Multiple interactions change shape of induced
    detector current
  • Multi-site events
  • Full-energy gamma signals gt500 keV
  • Sum-energy peak signals
  • Single-site events
  • Gamma signals lt150 keV
  • 72Ge(n, n e-) fast neutrons
  • Double-escape peaks
  • Internal beta-decay (no g) events

G. F. Knoll. Radiation detection and measurement.
John Wiley Sons, Inc., second edition, 1989.
4
Why Now is a good time for PSD.
  • Commercial digital spectroscopy hardware is
    available with fast (40 MHz), high-resolution
    (14-bit) digitization
  • Significant developments in pulse-shape
    discrimination techniques for HPGe have been made
    in the past 10 years and are ready to apply to
    new hardware

Full-energy 1621-keV g (top) and 1592-keV DEP
(bottom) reconstructed current pulses from 120
P-type Ortec HPGe detector (experimental data)
5
Starting Background Estimate
  • International Germanium Experiment (IGEX)
    achieved between 0.1-0.3 cts/keV/kg/y
  • Documented experiences with cosmic secondary
    neutron production of isotopes

Calculated Experimental
6
Low-Background Electroformed CopperKey
Technologies
  • Semiconductor-grade acids
  • Glassware-free handling
  • Copper sulfate purified by recrystallization
  • Baths circulated with continuous microfiltration
    to remove oxides and precipitates
  • Continuous barium scavenge removes radium
  • Cover gas in plating tanks reduces oxide
    formation
  • Periodic surface machining during production
    minimizes dendritic growth

Low-background detector and electroformed
cryostat during assembly
7
Low-Background Electroformed Copper Examples
  • Purity established with International Germanium
    Experiment (IGEX) experience
  • Strength equal to OFHC
  • Can be easily formed into thin, low-mass parts
  • Parts shown are for the MEGA array

Electroformed cups shown have wall thickness of
only 250 mm!
8
Backgrounds 68Ge
9
Backgrounds 60Co
10
Single-site interaction example
Monte-Carlo 2038-keV deposition from 0n bb-decay
of 76Ge
11
Multiple-site interaction example
Monte-Carlo 2038-keV deposition from
multi-Compton of 2615-keV 208Tl g
12
PNNLMulti-parametric Discriminator
  • Extracts key parameters from each preamplifier
    output pulse
  • Sensitive to radial location of interactions and
    interaction multiplicity
  • Self-calibrating allows optimal discrimination
    for each detector
  • Discriminator can be recalibrated for changing
    bias voltage or other variables
  • Method is computationally cheap, requiring no
    computed libraries-of-pulses

13
PSD can reject multiple-site backgrounds (like
68Ge and 60Co)
Keeps 80 of the single-site DEP (double escape
peak)
Experimental Data
Rejects 74 of the multi-site backgrounds (use
212Bi peak as indicator)
Original spectrum
Scaled PSD result
Improves T1/2 limit by 56
14
Fast Neutron Signature
  • Reaction of interest is 72Ge(n,ne-)
  • Signature is single-site (electron nuclear
    recoil)
  • Sensitive to useful range of fast-neutron energies

15
252Cf data result
  • Result is virtually free of gamma interference
  • Efficiency of PSD for the fast neutron signal is
    91
  • Fast neutron peak/continuum ratio improved by a
    factor of 11
  • Sensitivity increase of 300

total
Final result
16
Detector Segmentation
  • Sensitive to axial and azimuthal separation of
    depositions
  • Perkin-Elmer design with six azimuthal and two
    axial contacts
  • Projected efficacy of this design is excellent
    with expected backgrounds

17
Monte-Carlo Example
Segment multiplicity at 2039 keV
Sensitive to z and phi separation of depositions
0nbb efficiency 91 internal 60Co efficiency
14 Improves T1/2 limit by 140
18
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19
Projected Sensitivity
  • GIVEN
  • Background at 2038 keV 0.2 cts/keV/kg/y
  • 68Ge decay 10x reduction
  • 60Co decay/self shielding/less copper mass 2x
    reduction
  • 500 kg 86 76Ge x 10 years
  • PSDSegmentation FOM 1.6 x 2.4 3.8
  • RESULT
  • 0n T½ 4.0 x 1027 y
  • ltmngt 0.020 0.068 eV

20
Conclusions
  • Unprecedented confluence
  • Krasnoyarsk availability/Neutrino mass interest/
    Underground development/Crystal capacity
  • High Density
  • reduced shielding and footprint
  • Low Risk
  • proven technology / modular instrument /
    relocatable
  • Experienced Collaboration
  • long bb track record
  • Neutrino mass sensitivity
  • potential for discovery
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