A COMPLETE MICRO/NANOSYSTEM SOLUTION FOR ALPHA, BETA, GAMMA, AND NEUTRON DETECTION - PowerPoint PPT Presentation

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A COMPLETE MICRO/NANOSYSTEM SOLUTION FOR ALPHA, BETA, GAMMA, AND NEUTRON DETECTION

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A COMPLETE MICRO/NANOSYSTEM SOLUTION FOR ALPHA, BETA, GAMMA, AND NEUTRON DETECTION Dr. Chester Wilson Louisiana Tech University President, Cybercorps Interactive – PowerPoint PPT presentation

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Title: A COMPLETE MICRO/NANOSYSTEM SOLUTION FOR ALPHA, BETA, GAMMA, AND NEUTRON DETECTION


1
A COMPLETE MICRO/NANOSYSTEM SOLUTION FOR ALPHA,
BETA, GAMMA, AND NEUTRON DETECTION
  • Dr. Chester Wilson
  • Louisiana Tech University
  • President, Cybercorps Interactive

2
Why Is Nuclear Energy a Big Part of The Answer?
  • Decades of operational safety exceeding other
    energy producers.
  • Zero greenhouse gas emissions.
  • Fantastic power densities.
  • Domestic energy production.

3
Why Is Nuclear Energy a Big Part of The Answer?
  • Decades of operational safety exceeding other
    energy producers.
  • Zero greenhouse gas emissions.
  • Fantastic power densities.
  • Domestic energy production.
  • Around 40 of plant fuel comes from reprocessed
    ex-soviet nuclear weapons.

4
Weapons Grade Plutonium Becoming Energy
5
Other Guys Want it Too
6
Traditional Radiation Detectors
Traditional Method of Detection is Geiger
Counter. Problem Most detect Alphas, Betas,
Gammas, but not Neutrons. He3 and BF3 tubes
detect neutrons, but are toxic and expensive.
7
Traditional Radiation Detectors
Traditional Method of Detection is Geiger
Counter. Problem Most detect Alphas, Betas,
Gammas, but not Neutrons. He3 and BF3 tubes
detect neutrons, but are toxic and expensive.
Important because weapons grade plutonium emits
neutrons, not much else does
8
How do you shield neutrons?
Terrorist
Lead ?
Bomb Maker
9
Neutrons vs. Lead
  • Neutron interacting with Pb
  • Since the mass of the neutron is much smaller
    than the larger Pb atoms, the neutron recoils
    without losing much energy. The neutrons
    continuously bounce around able to exit the lead
    shielding.

10
NEED FOR DETECTORS
Terrorist
Plastic ?
Bomb Maker
11
NEED FOR DETECTORS
Neutron interacting with H
  • Since the mass of the neutron is approximately
    equal to the H atoms, the neutron can transfer up
    to its full energy. The recoil H nuclei has a
    small range losing energy quickly.

12
Nanoparticle Neutron Detection
Gadolinium oxide is opaque, but
Transparency! This scintillator is loaded with
30 gadolinium oxide, but because the
nanoparticles are too small to scatter light, it
is transparent.
And this allows a patternable film to make
imaging Arrays with better spatial resolution
and gamma selectivity.
13
Nanoparticle Neutron Detection
Neutron detection is enabled through gadolinium
nanoparticles, 255,000 barn absorption 1000X
smaller than anything else. Measurements taken at
Entergy Nuclears Grand Gulf Facility
14
Four Channel Device
  • Problem limited to the types of radiation
    detected
  • Solution dope with charge conversion
    nanoparticles

Radiation impinging on tailored nanoparticles
create electrons, which
scintillates a background matrix. WO3 Beta
Detection Pb3O4 Gamma/X-ray Detection Glass
Alpha Detection Gd2O3 Neutron Detection
15
DEVICE DESIGN
  • Four channels embedded into a sandblasted glass
    substrate
  • Optical cross talk barrier to reduce cross talk
    between detector channels

16
RESULTS
  • Gamma detection
  • 60Co emits both gammas and betas so lead sheets
    are used to block betas in order to detect only
    gammas and demonstrate the difficulty in
    shielding gammas.

Pulse height spectroscopy Tailored resins use
different conversion mechanisms producing varying
PM tube outputs
17
MULTIPLE LAYERSMORE INFORMATION
  • Varying thicknesses for top layer scintillator
    allows for different count rates
  • Energy spectroscopy capability by determining
    where the energy deposition took place as a
    function of top layer thickness

18
RESULTS
  • Bottom layer
  • With a decay constant of 285 ns, the
    created photons do not produce a ringing pulse.
  • Top layer
  • With a decay constant of 2.3 ns, the created
    photons produce a ringing pulse.

19
PRINTED CIRCUIT BOARD
  • Power
  • Converter

High Voltage
Pulse Shaping
20
PRINTED CIRCUIT BOARD
  • Design the printed circuit board using Eagle
    software.
  • Autoroute function to layout the copper traces
    after the components are placed.

21
Microscale Photomultiplier Tube
  • Photomultiplier tube components
  • Photocathode
  • Series of Dynodes
  • Anode

22
Beating the State of the Art
  • The count rates increase from non-doped
    scintillator to heavier doped scintillator.
  • Neutron sensitivity around 11 vs. around 0.2 on
    tube

23
Working Towards Cheap Pen Size Detector
  • Fully integrated radiation detector
  • Build smaller and cheaper components
  • Integrated Circuits
  • Miniaturized PM tube
  • Goal
  • Hockey puck style detector
  • Pager sized
  • Eventually pen sized

24
Thanks
  • Funding Sources
  • Entergy Nuclear
  • Department of Energy
  • National Science Foundation
  • Office of the Director of National Intelligence
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