Development of a Compton Camera for Prompt Gamma Imaging file2 . Symposium on Advanced Semiconductor...

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Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015 1 Motivation: need for accurate ion beam range verification Method: prompt-γ imaging via Compton scattering kinematics R&D on Compton camera (with electron tracking capability) Design, setup and characterization of prototype detector system P.G. Thirolf, LMU Munich p, C Development of a Compton Camera for Prompt Gamma Imaging

Transcript of Development of a Compton Camera for Prompt Gamma Imaging file2 . Symposium on Advanced Semiconductor...

Page 1: Development of a Compton Camera for Prompt Gamma Imaging file2 . Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015 . Prompt gamma emission

Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015 1

Motivation: need for accurate ion beam range verification

Method: prompt-γ imaging via Compton scattering kinematics R&D on Compton camera (with electron tracking capability) Design, setup and characterization of prototype detector system

P.G. Thirolf, LMU Munich

p, C

Development of a Compton Camera for Prompt Gamma Imaging

Page 2: Development of a Compton Camera for Prompt Gamma Imaging file2 . Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015 . Prompt gamma emission

Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015 2

Prompt gamma emission from proton beam on biomedical sample

irradiation of water phantom with 100 MeV protons:

4.4 MeV 12C 5.2 MeV 15N, 15O 6.1 MeV 16O C

ount

s / G

eV/ i

ncid

ent p

50 cm

Ø 10 cm

p H2O

0 2 4 6 8 10 12 14 16 18 Energy [MeV]

key issue in hadron therapy: - localization of Bragg peak within patient/sample range verification of therapeutic proton (or ion) beam

(simulation)

experimental approach: imaging via prompt γ emission from nuclear reactions

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Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015 3

(Prompt) Gamma Imaging: Compton Camera

exploit kinematics of Compton scattering:

−−=

12

2 111cosEE

cmeθ

(i) γ tracking:

-

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(Prompt) Gamma Imaging: Compton Camera

(ii) electron tracking:

advantage: - reconstruction of incompletely absorbed events increased reconstruction efficiency

Eγ ≥ 1-2 MeV

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Garching Compton Camera Prototype

C. Lang et al., JINST 9 (2014) P01008, PhD thesis in preparation

Scatterer/Tracker

Absorber

Eγ : 0.5 - 6 MeV

e-

γ

Compton camera layout:

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simulations for tracker/absorber specifications and expected performance:

nDSSSD=6 full absorption

γ tracking ; source - tracker: 50 mm

64 pixel (6x6mm2)

256 pixel (3x3mm2)

absorber:

300µm Si 500µm Si 300µm Si 500µm Si

γ + e tracking, 500 µm γ + e tracking, 300 µm γ tracking, 500 µm γ tracking, 300 µm

γ

γ +e

Compton Camera Design Simulations

- 6x6 mm2 3x3 mm2 pixel: - spatial resolution improves by ≥50 %

- d=500 µm + electron tracking: improved efficiency

- ε ≈ 10-3 – 10-5 (@ 1- 5 MeV for optimum resolution) - angular resolution ≈ 2o – 2.5o (@ 2-6 MeV)

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Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015

Compton Camera Prototype: Scatter/Tracker Array

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Scatterer/Tracker Array: 6x double-sided silicon strip detectors (DSSSD) active area 50 x 50 mm2

thickness : 500 µm 128 strips on each side pitch size 390 µm

S. Aldawood, PhD thesis, in preparation

DSSSD readout: Gassiplex (4x16 ch. ASIC): charge-sensitive preamplifier shaper digital discriminator track & hold-stage multiplexed ADC

Adapter board

1 2 3 4

DSSSD

Gassi-plex (64 ch.)

Gassi-plex

Gassi-plex

Gassi-plex

AC

AC

Wafer AC

A C

2x 64 strips/ side

VME readout controller

replacement by modern ASIC desirable: wider dynamics, trigger, more flexibility (monitor)

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Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015

Compton Camera Prototype: Scatter/Tracker Array

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S. Aldawood, PhD thesis, in preparation

- light tight enclosure - Faraday cage (+ ventilation, thermal control)

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Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015

Compton Camera Prototype

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Absorber: LaBr3 crystal: 50 x 50 x 30 mm3.

PMT: Hamamatsu H9500 (multi-anode: 16x16): .

signal processing: - 256 pixel (3x3 mm2) - individual spectroscopy electronics channels

S. Aldawood, PhD thesis, in preparation

LaBr3

PMT

256 ch.

LaBr3 PMT

fast amplifier + CFD (Mesytec MCFD-16, 16 ch.) charge-sensitive digital converter (Mesytec, 32 ch. VME-QDC)

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LaBr3 detector properties: energy / time resolution

energy resolution: <∆E/E> = 3.8% @ 662 keV (137Cs)

Pixel (x) <∆

E/E

>

<∆E

/E>

Pixel (y)

H. v.d. Kolff, Master thesis, TU Delft/LMU (2014)

time resolution: ∆t = 270 ps

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Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015

High-Energy Calibration

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Experiment at Tandetron (HZDR, Dresden/Rossendorf): - low energy (~1 MeV) protons - Eγ =4.44 MeV via 15N(p,αγ)12C

sim.: GEANT 4

4.44

MeV

3.93

MeV

3.42

MeV

validation of MC simulations

coun

ts /

keV

energy / keV

4.44

MeV

3.93

MeV

3.42

MeV

exp

S. Aldawood, PhD thesis, in preparation

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Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015

Scatter/Tracker Array

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energy deposition in 6 DSSSD layers: Eγ = 4.4 MeV - from simulation: increasing yield from front- to backside layers (accumulating contributions from Compton electrons)

GEANT 4

layer 1

layer 6

1 6

Eγ [keV]

coun

ts/ k

eV

simulations verified Eγ [ch.]

coun

ts/ c

h. Exp. layer 6

layer 1 1 6

S. Aldawood, PhD thesis, in preparation

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Symposium on Advanced Semiconductor Detectors for Medical Applications, Garching, 13.2.2015

Commissioning at Garching Tandem Accelerator

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p beam

H2O phantom

Eγ [keV]

Coun

ts /

8 k

eV

16O

*

4.44

MeV

5.11

MeV

(6

.130

– 0

.511

)

(6.1

30 –

1.0

22)

(4.4

40 –

0.5

11)

(4.4

40 –

1.0

22)

6.13

MeV

14N

*

12C

* 20 MeV protons + water phantom: prompt-γ spectrum

I. Castelhano, Master thesis, U Lisbon/LMU, 2014 sim.: GEANT 4

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LaBr3 detector properties: Spatial resolution

H. v.d. Kolff, Master thesis, TU Delft/LMU (2014)

spatial resolution: - collimated γ source (Ø 1 mm): 137Cs (662 keV, ca. 100 MBq) 2D scan of LaBr3

data analysis: - background correction - gain matching/uniformity correction: electronics, PMT “k-nearest neighbour” algorithm (TU Delft) derive position information from monolithic crystal

137Cs

automated positioning stage

Pb shield 137Cs

LaBr3 PMT

collimator

H.T. van Dam et al., IEEE TNS 58 (2011) 2139

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LaBr3 detector properties: Spatial resolution

S. Aldawood, PhD thesis, LMU, in preparation

- 2D scan with collimated 137Cs source - irradiation of 16x16 pixels (3x3 mm2)

light amplitude distribution maps:

- goal: 104 maps as reference data set (0.5 mm collimation, 0.5 mm step size) T. Marinšek, Master thesis, LMU, in preparation

γ hit position identification via ‘k-NN’: (preliminary, not yet full resolution)

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Perspective: ‘Hybrid Detector’ System

γ-PET technique: reconstruct triple-coincidences from β+γ emitters

1 tracked event: reconstructed cone segment of prompt γ

LOR of 511 keV e+ annihilation photons

prompt-γ detection during irradiation delayed photons from β+ (γ) emitters (11,10C, 15,14O, 13N) during irradiation interrupts

C. Lang et al., JINST 9 (2014) P01008, PhD thesis in preparation

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Conclusion

Compton camera prototype for prompt-gamma range monitoring: - prototype characterized off- and online: - absorber: LaBr3 with multi-anode PMT: ∆E/E = 3.8% , ∆t= 270 ps spatial characterization (k-NN method) in progress prerequisite of source reconstruction (MEGAlib)

- scatterer/tracker: 6x DSSSD (500 µm, 50x50 mm2, 2x128 ch.)

- online characterization: Garching (Ep= 20 MeV), Dresden (Eγ=4.4 MeV) - verification of model simulations

Perspective: hybrid detector system - prompt-γ detection during irradiation - delayed photons from β+ (γ) emitters (11,10C, 15,14O, 13N) during irradiation interrupts

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Thanks to …

Thank you for your attention !

LMU Munich: C. Lang, S. Aldawood, I. Castelhano, H. v.d. Kolff, S. Liprandi, B. Tegetmeyer, G. Dedes, R. Lutter, J. Bortfeldt, K. Parodi

TU Munich: L. Maier, M. Böhmer, R. Gernhäuser

TU Delft: D.R. Schaart

OncoRay/ HZDR, Dresden: G. Pausch, K. Römer, J. Petzoldt, F. Fiedler

Supported by DFG Cluster of Excellence MAP (Munich-Centre for Advanced Photonics)