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Dr Laura HarknessBrennan Liverpool Physics’ Teachers Conference 2014 Gammaray detection & imaging in the digital world

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Dr  Laura  Harkness-­‐Brennan    

Liverpool  Physics’  Teachers  Conference  2014  

Gamma-­‐ray  detection  &  

imaging  in  the  digital  world  

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•  Gamma-­‐ray  detec,on  and  spectroscopy  

•  Going  digital  

•  Gamma-­‐ray  imaging  

•  in  medical  physics  

•  in  nuclear  security  and  decomissioning  

Outline  

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Radiation  Detection  

•  Is  there  any  radia,on?  

•  What  type  is  it?  

•  What  is  the  ac,vity  or  dose  rate?  

•  What  material  does  it  come  

from?  

•  Where  is  it  located?  

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By  measuring  the  energies  of  gamma-­‐rays,  can  understand  what  material  they  were  emi>ed  from      

Gamma-­‐ray  Spectroscopy  

511keV  

1274keV  

662keV  

137Cs  and  22Na  fingerprints  •  Characteris,c  energies  •  Probability  of  emission    

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Gamma-­‐ray  Detection  Demo  

Incident    Radia,on  

 Photoelectron     Dynodes    Anode  

Output  Voltage    Interac,on  point    

•  Gamma-­‐rays  interact  in  scin,lla,on  detector  •  Scin,lla,on  light  is  produced  (which  is  propor,onal  to  how  much  

energy  has  been  deposited)  •  Light  is  converted  into  an  electrical  signal  and  amplified  in  a  Photo  

Mul,plier  Tube  (PMT)  •  Output  signals  are  processed  into  an  energy  spectrum  

 

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•  Digital  electronics  offer  enhanced  func5onality  for  flexible  teaching  

and  research  

•  Compact  –  can  plug  directly  into  computer  or  laptop  

•  Teaching  systems  easier  to  use  

•  Complex  analogue  experiments  made  simpler  with  digital  readout  

Going  Digital:  Teaching  

•  Central  teaching  labs  have  

43  fully  digital  systems  

(semiconductor,  scin,lla,on  

and  gas  detectors),  all  on  

one  network  

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•  Standard  commercial  products    

•  1-­‐box  spectroscopy  

•  Usually  1-­‐2  channels    

•  Provides  low  and  high  voltage  

•  “User-­‐friendly”  so[ware  

•  Usually  records  only  energy  and  ,ming  

 

Going  Digital:  Teaching  

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•  Gamma-­‐ray  spectroscopy  with  

scin,llator  and  semiconductor  

detectors    

•  Coun,ng  sta,s,cs  

•  Gamma-­‐ray  a>enua,on  in  

ma>er  

•  Compton  sca>ering  

•  Half-­‐life  measurement  

•  Coincidence  coun,ng  

•  Positron  annihila,on    

Going  Digital:  Teaching  

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•  Research  grade    

•  Mul,  channel  –  modular  

•  Records  detector  signals  

•  Custom  so[ware  

Going  Digital:  Research  

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•   Informa,on  about  the  

interac,on  is  o[en  

contained  in  the  detector  

signal  shape  

•   Algorithms  process  the  

detector  signals  

•   Posi5on  of  interac5on  

within  the  detector  

Going  Digital:  Research  Pulse  Shape  Analysis  

Essen5al  in  imaging  applica5ons  and  gamma-­‐ray  spectroscopy  

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Aim:  To  improve  the  sensi,vity  of  germanium  gamma-­‐ray  detectors  for  measurement  of  low  ac,vity  nuclear  waste    Methods:  High-­‐precision  experimental  measurements  in  lab,  modeling  and  in-­‐situ  measurements    

Enhanced  Nuclear  Waste  Assay  Industrial  Partner:  Nuclear  Decommissioning  Authority  (NDA)  

Improved  Sensitivity  

Experimental  Data  

Simulated  Data  Algorithm  

Development  

Performance  Evaluation  

MDA = (2.71+ 4.65x B)εtk

B:  background  counts  ε:  efficiency  t:  measurement  8me  k:  correc8on  factor  

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Objec5ves:    1)  To  experimentally  assess  the  response  of  

detectors  for  known  posi,ons  of  single  gamma-­‐ray  interac,ons    

2)  To  use  the  database  to  validate  a  detector  modelling  code    

3)  To  op,mise  pulse  shape  analysis  algorithms  for  detectors  of  differing  geometry  

Enhanced  Nuclear  Waste  Assay  Industrial  Partner:  Nuclear  Decommissioning  Authority  (NDA)  

4)  To  conduct  realis,c  industrial  performance  tests  at  Canberra  (Harwell)  using  their  facili,es  that  include  waste  drum  analogues  and  at  the  NNL  Central  Laboratory  

NDA  

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•  Gamma-­‐ray  source  collimated  into  beam,  suspended  above  the  detector  

•  Detector  signal  stored  and  processed  by  digital  electronics  

•  Collimator  moved  across  surface,  using  an  automated  x-­‐y  posi,oning  table  

•  Calculate  average  pulse  shapes  

•  Pulse  shape  varia,on  -­‐  posi,on  of  interac,on  sensi,vity  

Time (ns)0 100 200 300 400 500 600

Nor

mal

ised

Pul

se H

eigh

t

0

0.2

0.4

0.6

0.8

1 0mm8mm16mm24mm

Enhanced  Nuclear  Waste  Assay  Industrial  Partner:  Nuclear  Decommissioning  Authority  (NDA)  

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•  Technique  used  to  detect  sources  of  gamma  

radia,on  

•  Iden5fy  what  the  source  is:  gamma-­‐ray  

spectroscopy  

•  Locate  radia,on:  imaging  methods  

Compton  Imaging  

 

•  Wide  range  of  fields  of  view–  in  a  lorry,  in  a  room  and  in  a  body  

•  Security,  nuclear  decommissioning  and  nuclear  medicine  

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•  Gamma  rays  interact  in  two  detectors  

•  The  path  of  each  gamma  ray  is  

reconstructed  as  a  cone  

•  Source  of  radia,on  located  at  max  cone  

overlap  

Compton  Imaging  

           

⎟⎟⎠

⎞⎜⎜⎝

⎛−−=

01

2 111cosEE

cmeϑθ  

θ   (E,  X,Y,Z)2  

(E,  X,Y,Z)2    

   Source  E0  

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•  Gamma  rays  interact  in  two  detectors  

•  The  path  of  each  gamma  ray  is  

reconstructed  as  a  cone  

•  Source  of  radia,on  located  at  max  cone  

overlap  

Compton  Imaging  

           

⎟⎟⎠

⎞⎜⎜⎝

⎛−−=

01

2 111cosEE

cmeϑθ  

θ   (E,  X,Y,Z)2  

(E,  X,Y,Z)2    

   Source  E0  

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•  Gamma  rays  interact  in  two  detectors  

•  The  path  of  each  gamma  ray  is  

reconstructed  as  a  cone  

•  Source  of  radia,on  located  at  max  cone  

overlap  

Compton  Imaging  

           

⎟⎟⎠

⎞⎜⎜⎝

⎛−−=

01

2 111cosEE

cmeϑθ  

θ   (E,  X,Y,Z)2  

(E,  X,Y,Z)2    

   Source  E0  

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•  Gamma  rays  interact  in  two  detectors  

•  The  path  of  each  gamma  ray  is  

reconstructed  as  a  cone  

•  Source  of  radia,on  located  at  max  cone  

overlap  

Compton  Imaging  

           

⎟⎟⎠

⎞⎜⎜⎝

⎛−−=

01

2 111cosEE

cmeϑθ  

θ   (E,  X,Y,Z)2  

(E,  X,Y,Z)2    

   Source  E0  

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Medical  Physics  -­‐  SPECT  

•  Single  Photon  Emission  Computed  Tomography  

(SPECT)  

•  Diagnosis/monitoring  of  cancer  and  neurological  

condi,ons  

•  Biological  informa,on  complements  MRI  structural  

informa,on  

•  Mechanical  collimator  1  x  10  -­‐4  

•  Scin,llator  detector  with  photomul,plier  tubes  

Pa,ent  injected  with  radiopharmaceu,cal  

Radiopharmaceu,cal  accumulates  in  organ  

of  interest      

Gamma-­‐rays    emi>ed  from  organ  and  detected  outside  body  by  gamma  camera  

Medical  Imaging  SPECT:  Single  Photon  Emission  Computed  Tomography  

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•   £1.1  million  project    

•   Prototype  system  

•   High-­‐sensi,vity  alterna,ve  to  

SPECT  

•   Different  method  of  imaging  the  

gamma  radia,on  

•   Semiconductor  detectors  

 

Medical  Physics  -­‐  SPECT  Medical  Imaging  SPECT:  Single  Photon  Emission  Computed  Tomography  

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Conventional  SPECT  

•  Use  1  gamma  ray  in  every  3000    

•  Incompa,ble  with  MRI  

ProSPECTus  

•  Use  1  gamma  ray  in  every  30  •  Compa,ble  with  MRI  •  Mul,-­‐isotope  imaging  Lower  dose  

to  pa,ent  or  shorter  data  acquisi,on  ,mes  

θ

θ (E, X,Y,Z)2

(E, X,Y,Z)2

   Source  E0  

Medical  Physics  -­‐  SPECT  Medical  Imaging  ProSPECTus:  Next  Generation  SPECT  

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Criteria  •  Prototype  system  for  use  with  current  

medical  radionuclides  •  High  sensi,vity    •  Excellent  image  quality    •  MRI  compa,bility  

Final  Design  •  Op,mised  for  imaging  gamma  rays  

from  99mTc    •  Si(Li)  sca>er  detector  and  a  HPGe  

absorber  detector    •  Custom  –built  cryostat    •  Digital  electronics  

Medical  Physics  -­‐  SPECT  Medical  Imaging  ProSPECTus:  Next  Generation  SPECT  

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•  Planar  Si(Li)  (60  x  60  x  9)  mm  detector  

•  16  strips  on  each  face,  4mm  pitch  

Photo  

Courtesy  of  Semikon  

•   Planar  HPGe  (60  x  60  x  20)  mm  detector  

•   12  strips  on  each  face,  5mm  pitch  

Photo  

Courtesy  of  ORTEC  

Medical  Physics  -­‐  SPECT  Medical  Imaging  ProSPECTus:  Next  Generation  SPECT  

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Medical  Physics  -­‐  SPECT  Medical  Imaging  ProSPECTus:  Next  Generation  SPECT  

•  Preclinical  trials  in  progress  

•  Compara,ve  imaging  of  phantoms  against  clinical  scanners  

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Medical  Physics  -­‐  SPECT  Nuclear  Security  and  Decomissioning  Industrial  Partner:  National  Nuclear  Laboratory  (NNL)  

•  Radia,on  map  of  source  •  Op,cal  image  •  Stereoscopic  image  “3D”  

•  Nuclear  decommissioning  •  Remote  response  

•  High  sensi,vity  and  good  image  quality  essen,al  

 •  2  semiconductor  detectors,  which  

measure  posi,on  and  energy  of  

gamma-­‐ray  interac,ons  

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Medical  Physics  -­‐  SPECT  Nuclear  Security  and  Decomissioning  PorGamRays:  Portable  Gamma-­‐ray  Spectroscopy  

•   PorGamRays  –  room  temperature,  small  

area,  semiconductor  detectors  portable  for  

“in  the  field”  measurements  

•   Pixelated  CZT  detectors  with  ASIC  readout  

•   Imaging  demonstrated:  e.g.  133Ba  source  

located  at  100  mm  then  120  mm  

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Medical  Physics  -­‐  SPECT  Nuclear  Security  and  Decomissioning  Industrial  Partner:  AWE  

•   Compton  imaging  data  acquired  at  

Liverpool  using  various  gamma-­‐ray  sources  

•   Successful  trials  AWE  to  iden,fy  “unknown”  

sources,  at  rela,vely  far  stand  off  distance  

and  when  “concealed”  by  various  absorbing  

materials  

 57Co  122keV   137Cs  662keV   137Cs  662keV  

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•   Useful  to  iden,fy  specific  materials,  e.g.  drugs  and  explosives  

•   Research  at  UoL  Physics  Dept:  Detec,on  of  gamma-­‐rays  from  neutron  

ac,vated  materials  

•   Can  both  form  an  image  and  produce  a  gamma-­‐ray  spectrum  

•   The  peaks  in  the  gamma-­‐ray  spectrum  contain  elemental  informa,on:  

what  is  inside?  

•   Explosives  and  drugs  contain  combina,ons  of  light  elements  e.g.  

Oxygen  (6.1  MeV),  carbon,  (4.4  MeV)  

nitrogen  (1.64,  2.31,  5.11  MeV)  

*  *    *  

*  *  

Medical  Physics  -­‐  SPECT  Nuclear  Security  DISTINGUISH  

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14MeV  pulsed  neutrons.    

Inelastic  scattering.  

Characteristic  gamma  rays  emitted  

Detection  &  imaging    (Compton  Camera)  

Neutron  detector  

Neutron  generator  

Medical  Physics  -­‐  SPECT  Nuclear  Security  DISTINGUISH  

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•  Gamma-­‐ray  detec,on  and  spectroscopy  

•  Going  digital  

•  Gamma-­‐ray  imaging  

•  in  medical  physics  

•  in  nuclear  security  

Summary  

Contact:  [email protected]