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Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford ORNL Physics Division
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Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

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Page 1: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

Digital Signal Processing

for

HPGe Detectors

July 28, 2012

David Radford ORNL Physics Division

Page 2: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

2 Managed by UT-Battelle for the U.S. Department of Energy

•  Hyper-Pure Ge (HPGe) detectors are the “gold standard” for gamma-ray spectroscopy −  Unsurpassed energy resolution

−  Indispensible to in-beam nuclear structure studies for many decades

•  Made from a single large crystal pulled from molten hyper-pure Ge •  Operated as a large reverse-biased diode; up to 5 kV bias

•  No current flows until a gamma ray interacts with an electron in the Ge, lifting its energy above the band gap of the Ge semiconductor

•  This electron scatters off other electrons, creating many electron-hole pairs; each pair takes ~ 3 eV in energy

•  The electrons and holes separate in the strong electric field and are collected at the electrodes

•  The resulting charge pulse is proportional to the deposited gamma-ray energy, and is amplified and digitized

•  Operated at cryogenic temperatures to prevent thermal generation of electron-hole pairs

HPGe Detectors

Page 3: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

3 Managed by UT-Battelle for the U.S. Department of Energy

Closed-end coaxial

n+

p+ p

n+

p

Planar

HPGe Detectors Historically, there have been two designs, both cylindrical:

Coaxial and Planar.

Later we will discuss a new design, “Point Contact” detectors

p+

Page 4: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

4 Managed by UT-Battelle for the U.S. Department of Energy

Closed-end coaxial

n+

p+ p

n+

p

Planar

HPGe Detectors Historically, there have been two designs, both cylindrical:

Coaxial and Planar.

p+

~ 3 kV

+

Page 5: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

5 Managed by UT-Battelle for the U.S. Department of Energy

HPGe Detectors

Electric potential

Drift paths of electrons and holes

Closed-end coaxial

Fast ADC Charge-integrating pre-amp

Page 6: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

Signal Processing

Once the preamplifier signal/waveform has been digitized, need to process the data to extract interesting numbers, e.g. •  Amplitude

•  Gives energy, so we want it to be as accurate as possible

•  Timing •  Pulse-shape analysis to select specific types of

events •  Noise filtering and/or reduction •  Pile-up rejection and/or correction

Page 7: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

Extracting Signal Amplitude

Height of signal is proportional to

detected energy

Preamp signal •  Decays exponentially with

~ 50µs time constant

Time

Volta

ge

Page 8: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

Extracting Signal Amplitude

But the signal has noise… •  Need to integrate signal for several microseconds

to determine amplitude more precisely •  Use “Trapezoid Filter”

Page 9: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

Extracting Signal Amplitude

Output of Trapezoid Filter

Undershoot due to exponential decay of signal

Page 10: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

Extracting Signal Amplitude

•  Need to correct for signal decay time •  “Pole-zero” correction

Page 11: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

Trapezoid and P/Z Correction •  Need to know the baseline (asymptote)

and signal decay time constant tau •  E ~ S2’ – S1’

Baseline

S1’  

S2   S2’  

S1  

Page 12: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

14 Managed by UT-Battelle for the U.S. Department of Energy

P-type Coaxial P-type Point Contact

p p+

n+ n+

p+

p

Point Contact Detectors •  No deep hole; small point-like central contact •  Length is shorter than standard coaxial detector •  Excellent discrimination between single-interaction and multiple-

interaction events •  Excellent resolution at low energies

Page 13: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

Pulse-Shape Response Point Contact detectors are ideal for discrimination between single-site and multi-site events (or determining the number of interactions)

0

100

200

300C

harg

e Si

gnal

0

20

40

60

Cur

rent

Sig

nal

200 600 1000 1400Time (ns)

0

100

200

300

400

0

20

40

60

80

200 600 1000 1400Time (ns)

a) Single-site b) Multi-site

Page 14: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

16 Managed by UT-Battelle for the U.S. Department of Energy

Pulse-Shape Response

9/30/09 Radford, RedTeam Review

Red: all events Blue: PSA-selected events

Th source

95% efficiency for double-escape peak = single-site events 99% rejection of single-escape peak = multi-site events

Page 15: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

17 Managed by UT-Battelle for the U.S. Department of Energy

“Inverted-Coaxial” Point-Contact Detector •  Designed and developed here at ORNL •  Drift of charges is radically different from a normal coaxial detector •  Very long drift times, ~ 2 µs •  A segmented prototype has recently been produced by Canberra France

Page 16: Digital Signal Processing for HPGe Detectorsfribusers.org/documents/2014/ebssLectures/EBSS_activity_3.pdf · Digital Signal Processing for HPGe Detectors July 28, 2012 David Radford

19 Managed by UT-Battelle for the U.S. Department of Energy

Am “SuperPulses” •  Finely collimated Am source,

directed at known location on the detector surface

•  Select events with 60 keV in a single hit segment

•  Use PSA to select only single-site events

•  Time-align events to a common time

•  Take average signal to reduce noise to negligible level

RadWaresig2sp.ps, created 08-Apr-13 03:18:08

Cha

rge

1 1 1 10 2 2 2 2Time ( s)

Superpulse

Singleevent

PC Seg1 Seg2 Seg3