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First results in the application of Silicon Photomultiplier matrices to ...

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<strong>First</strong> <strong>results</strong> <strong>in</strong> <strong>the</strong> <strong>application</strong> <strong>of</strong> <strong>Silicon</strong><br />

<strong>Pho<strong>to</strong>multiplier</strong> <strong>matrices</strong> <strong>to</strong> small<br />

animal PET<br />

G. Llosá, N. Belcari, M. G. Bisogni, G. Collazuol, A. del Guerra, S.<br />

Marcatili<br />

University <strong>of</strong> Pisa -INFN Pisa, Italy.<br />

M. Boscard<strong>in</strong>, M. Melchiorri, A. Tarolli, C. Piemonte, N. Zorzi<br />

FBK-irst, Tren<strong>to</strong>, Italy.<br />

P. Barrillon, S. Bondil-Bl<strong>in</strong>, V. Chaumat, C. de la Taille, N. D<strong>in</strong>u,<br />

V. Puill, J-F Vagnucci<br />

Labora<strong>to</strong>ire de l'Accélérateur L<strong>in</strong>éaire, IN2P3-CNRS, Orsay, France.<br />

This work is partially supported by <strong>the</strong> European Commision's Sixth<br />

Framework Program through a Marie Curie Intra-European Fellowship<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 1


High resolution small animal PET<br />

! A high resolution small animal PET scanner with <strong>Silicon</strong><br />

<strong>Pho<strong>to</strong>multiplier</strong>s as pho<strong>to</strong>detec<strong>to</strong>rs is under development at <strong>the</strong><br />

University <strong>of</strong> Pisa.<br />

! <strong>Silicon</strong> pho<strong>to</strong>multiplier <strong>matrices</strong> from <strong>the</strong> Center from Scientific<br />

and technological research (FBK-irst , Tren<strong>to</strong>, Italy) will be<br />

employed.<br />

! The use <strong>of</strong> SiPM <strong>matrices</strong> has significant advantages <strong>in</strong> <strong>the</strong><br />

design <strong>of</strong> a detec<strong>to</strong>r head for a small animal PET <strong>to</strong>mograph wrt<br />

arrays <strong>of</strong> s<strong>in</strong>gle SiPMs:<br />

High pho<strong>to</strong>detec<strong>to</strong>r sensitivity: SiPM <strong>matrices</strong> leave low dead area<br />

wrt arrays <strong>of</strong> s<strong>in</strong>gle SiPMs.<br />

Small pitch: high spatial resolution.<br />

Ma<strong>in</strong> drawback: high number <strong>of</strong> output channels<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 2


PET detec<strong>to</strong>r head<br />

! Use <strong>of</strong> cont<strong>in</strong>uous sc<strong>in</strong>tilla<strong>to</strong>r slabs + f<strong>in</strong>ely pixellated SiPM<br />

matrix can provide better performance than pixellated sc<strong>in</strong>tilla<strong>to</strong>r<br />

blocks:<br />

- Very good spatial resolution with maximum likelihood<br />

algorithms.<br />

- high efficiency : no light losses due <strong>to</strong> small pixel size.<br />

- lower cost.<br />

• Stack <strong>of</strong> several detec<strong>to</strong>r layers:<br />

– Discrete DOI <strong>in</strong>formation that reduces<br />

parallax error => higher spatial<br />

resolution.<br />

– High efficiency: <strong>in</strong>creased sc<strong>in</strong>tilla<strong>to</strong>r<br />

thickness.<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 3


Detec<strong>to</strong>r head performance<br />

• Optimized geometry and performance estimated with GEANT4<br />

simulations.<br />

• Head geometry: stack <strong>of</strong> three detec<strong>to</strong>r layers (4 cm x 4 cm x 5 mm).<br />

– Cont<strong>in</strong>uous slab <strong>of</strong> LYSO, 5 mm thick=>15 mm <strong>to</strong>tal thickness.<br />

– SiPM matrix with 1.5 mm pitch elements as pho<strong>to</strong>detec<strong>to</strong>r.<br />

• Head performance:<br />

– About 70% efficiency for 511 keV pho<strong>to</strong>ns.<br />

– Intr<strong>in</strong>sic spatial resolution – 0.3 mm <strong>in</strong> <strong>the</strong> center <strong>of</strong> <strong>the</strong> crystal;<br />

< 1mm <strong>in</strong> <strong>the</strong> edges.<br />

• Center-<strong>of</strong>-gravity position determ<strong>in</strong>ation algorithms worsen resolution and<br />

displacement errors <strong>to</strong>wards <strong>the</strong> edges.<br />

• ML methods (skeweness and barycenter based) reduce error <strong>to</strong>wards <strong>the</strong><br />

edges.<br />

S. Moehrs et al. A detec<strong>to</strong>r head design for small-animal PET with silicon pho<strong>to</strong>multipliers (SiPM).<br />

Phys. Med. Biol. 51 (2006) 1113-1127.<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 4


PET <strong>application</strong>s: rotat<strong>in</strong>g <strong>to</strong>mograph<br />

4-head <strong>to</strong>mograph (same concept as YAP(S)-PET):<br />

– 2(4) rotat<strong>in</strong>g detec<strong>to</strong>r heads at 10-15 cm distance.<br />

– FOV 4 cm axial, 4 cm transaxial.<br />

– efficiency around 4%<br />

– Spatial resolution better than 1 mm 3 for a po<strong>in</strong>t source <strong>in</strong> <strong>the</strong> CFOV.<br />

– low cost.<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 5


MR compatible r<strong>in</strong>g <strong>to</strong>mograph<br />

• R<strong>in</strong>g <strong>to</strong>mograph <strong>to</strong> be <strong>in</strong>serted <strong>in</strong> a<br />

magnet bore <strong>of</strong> an MR system.<br />

• 16 detec<strong>to</strong>r heads, 7 cm x 2.4 cm;<br />

• FOV axial 7 cm, transaxial FOV ~6 cm.<br />

• Spatial resolution: 0.76 mm 3 for a 18 F po<strong>in</strong>t source<br />

<strong>in</strong> <strong>the</strong> CFOV with FBP.<br />

• efficiency around 11% for 250 keV energy<br />

threshold.<br />

Tests with SiPMs <strong>in</strong> MR system show no degradation <strong>of</strong> <strong>the</strong> data<br />

gradients <strong>of</strong>f<br />

gradients on<br />

gradients <strong>of</strong>f<br />

gradients on<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 6


SiPM <strong>matrices</strong> from FBK-irst<br />

Composed <strong>of</strong> 16 pixel elements <strong>in</strong> a common substrate<br />

1 mm pixels <strong>in</strong> 1.06 mm pitch<br />

• Structure: n + -p-! -p + optimized for blue light:<br />

Shallow n + layer + specific antireflective coat<strong>in</strong>g.<br />

• 625 (25 x 25) microcells, 40 "m x 40 "m size.<br />

• Polysilicon quench<strong>in</strong>g resistance.<br />

• Fill fac<strong>to</strong>r (GF) 30 – 35%.<br />

• PDE 8 % at #V=3.5V for $ = 420 nm.<br />

4 mm<br />

1 mm<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 7


<strong>First</strong> <strong>results</strong><br />

• Data acquisition system<br />

• Characterization<br />

• Measurements with pixellated crystals.<br />

• Measurements with cont<strong>in</strong>uous crystals.<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 8


Readout: MAROC2 (LAL Orsay)<br />

• 64 channels (only 16 used)<br />

• Variable ga<strong>in</strong> (6 bits), low noise preamplifier<br />

• Slow shaper (~20-150 ns, adjustable)<br />

• Fast shaper (15 ns) + 3 discrim<strong>in</strong>a<strong>to</strong>rs=> trigger signal<br />

• Designed for MAPMT – not optimized for SiPMs, but<br />

allows us <strong>to</strong> make <strong>the</strong> first tests satisfac<strong>to</strong>rily.<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 9


Readout: Test board<br />

• Altera FPGA<br />

• USB Port<br />

• ADC<br />

• ASIC calibration <strong>in</strong>put.<br />

• LabVIEW s<strong>of</strong>tware for<br />

data acquisition<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 10


MAROC2 calibration<br />

• Calibration at m<strong>in</strong>imum preamplifier ga<strong>in</strong>: two l<strong>in</strong>ear ranges<br />

before saturation.<br />

• Good uniformity: % = 0.9 % at 7 pC; % = 1.5 % at 94 pC;<br />

• SiPM signals with pixellated crystals at high overvoltage (>2V)<br />

saturate <strong>the</strong> amplifier.<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 11


Characterization<br />

• Very good uniformity<br />

• Breakdown voltage variations %= 0.3%<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 12


Results with pixellated crystals<br />

Holder for precise position<strong>in</strong>g:<br />

Error < 50 "m.<br />

LYSO crystal array: 16 (4x4)<br />

crystals <strong>of</strong> 0.96 mm x 0.96 mm<br />

x 10 mm separated by 100 "m<br />

<strong>of</strong> white epoxy res<strong>in</strong>.<br />

Perfect match <strong>to</strong> <strong>the</strong> SiPM matrix<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 13


Results with pixellated crystals<br />

NO COINCIDENCE<br />

BACKGROUND<br />

DUE TO 176 Lu<br />

– One SiPM pixel <strong>in</strong> <strong>the</strong> matrix<br />

– Na-22 energy spectra<br />

acquired with <strong>the</strong><br />

oscilloscope (no amplifier)<br />

– 3V overvoltage.<br />

COINCIDENCE WITH<br />

PMT + YAP crystal<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 14


Results with pixellated crystals<br />

• Na-22 spectra from all channels with MAROC2 board<br />

• Co<strong>in</strong>cidence with 1x1x10 mm LSO crystal + s<strong>in</strong>gle SiPM<br />

• Peak position variation %=4.4%<br />

2 V overvoltage<br />

peak position variation Na spectrum all channels<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 15


Results with cont<strong>in</strong>uous crystals<br />

• Crystal 4 mm x 4 mm x 5 mm cover<strong>in</strong>g<br />

<strong>the</strong> whole matrix.<br />

• Na-22 spectrum summ<strong>in</strong>g signals from<br />

all channels.<br />

4 V overvoltage<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 16<br />

4 mm<br />

4 mm


Position determ<strong>in</strong>ation<br />

~35 mm 5 mm<br />

• Co<strong>in</strong>cidence with a 2 nd detec<strong>to</strong>r: 1 mm x 1 mm x<br />

1 mm crystal coupled <strong>to</strong> a SiPM<br />

• Source close <strong>to</strong> <strong>the</strong> matrix, far from 2 nd detec<strong>to</strong>r<br />

• Move <strong>to</strong>ge<strong>the</strong>r source and 2 nd detec<strong>to</strong>r <strong>in</strong> 0.5 mm<br />

steps.<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 17


Position determ<strong>in</strong>ation<br />

Hitmap for different source position with crystal array<br />

+ 1 mm + 2 mm<br />

+ 0.5 mm + 1.5 mm<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 18


Future work<br />

• Position determ<strong>in</strong>ation with cont<strong>in</strong>uous<br />

crystal<br />

• Tim<strong>in</strong>g measurements<br />

• <strong>First</strong> test pro<strong>to</strong>type<br />

– 2 rotat<strong>in</strong>g heads<br />

– Pixellated crystals<br />

– New readout system<br />

• Matrices 64 pixels will soon be fabricated.<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 19


Conclusions<br />

• FBK-irst has developed SiPM <strong>matrices</strong> with 16 SiPM pixels<br />

<strong>in</strong> a common substrate. The first <strong>results</strong> obta<strong>in</strong>ed are very<br />

good and lead <strong>to</strong> <strong>the</strong> fabrication <strong>of</strong> SiPM <strong>matrices</strong> with 64<br />

pixels.<br />

•A very high resolution PET <strong>to</strong>mograph for small animals<br />

employ<strong>in</strong>g SiPMs as pho<strong>to</strong>detec<strong>to</strong>rs is under development<br />

at <strong>the</strong> University <strong>of</strong> Pisa. A spatial resolution <strong>of</strong> 0.76 mm<br />

FWHM is expected for a 18 F po<strong>in</strong>t source <strong>in</strong> water <strong>in</strong> <strong>the</strong><br />

centre <strong>of</strong> <strong>the</strong> FOV, employ<strong>in</strong>g FBP for image reconstruction,<br />

accord<strong>in</strong>g <strong>to</strong> GEANT4 simulations.<br />

• The first tests <strong>to</strong>wards <strong>the</strong> PET scanner construction are<br />

ongo<strong>in</strong>g with good <strong>results</strong>. Tests with both pixellated and<br />

cont<strong>in</strong>uous crystals are be<strong>in</strong>g carried on.<br />

• A first pro<strong>to</strong>type with two rotat<strong>in</strong>g heads is be<strong>in</strong>g<br />

assembled, employ<strong>in</strong>g pixellated crystals.<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 20


<strong>Silicon</strong> <strong>Pho<strong>to</strong>multiplier</strong>s<br />

SiPM : Multicell Avalanche Pho<strong>to</strong>diode work<strong>in</strong>g <strong>in</strong> limited Geiger mode<br />

- 2D array <strong>of</strong> microcells: structures <strong>in</strong> a common bulk.<br />

-Vbias > Vbreakdown: high field <strong>in</strong> mult. region.<br />

- Microcells work <strong>in</strong> Geiger mode: <strong>the</strong> signal is <strong>in</strong>dependent <strong>of</strong> <strong>the</strong> particle energy<br />

- The SiPM output is <strong>the</strong> sum <strong>of</strong> <strong>the</strong> signals produced <strong>in</strong> all microcells fired.<br />

! Significant advantages wrt o<strong>the</strong>r pho<strong>to</strong>detec<strong>to</strong>rs:<br />

• High Ga<strong>in</strong><br />

• Fast tim<strong>in</strong>g<br />

• High PDE<br />

• High S/N ratio<br />

• Insensitive <strong>to</strong> magnetic fields<br />

• Low operat<strong>in</strong>g voltage<br />

• Potential low cost<br />

n + cathode +VGM h&<br />

p high-electric field<br />

multiplication region<br />

! epilayer<br />

p + substrate<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 21<br />

4 µm<br />

oxide<br />

e -<br />

hole


New detec<strong>to</strong>rs<br />

• Different geometry, size, microcell size and GF.<br />

40x40!m => GF 44%<br />

50x50!m => GF 50%<br />

100x100!m => GF 76%<br />

• Matrices 16 elements (4x4)<br />

4 mm<br />

4 mm<br />

IV CURVES OF 9<br />

MATRICES. VERY<br />

UNIFORM<br />

BREAKDOWN<br />

POINT<br />

N41-2: C. Piemonte. Recent Progress <strong>in</strong> <strong>the</strong><br />

Performance <strong>of</strong> <strong>Silicon</strong> <strong>Pho<strong>to</strong>multiplier</strong>s<br />

produced at FBK-irst.<br />

circular (1mm diam) 1x1mm 2x2mm 3x3mm (3600 cells) 4x4mm (6400 cells)<br />

gabriela.llosa@pi.<strong>in</strong>fn.it NDIP08 Aix les Ba<strong>in</strong>s 15-20 June 2008 22

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