Purpose <p>Time-of-flight (TOF) capability of positron emission tomography (PET) can improve the signal-to-noise ratio (SNR) in the image reconstruction. A new high-density and compact front-end electronics design for TOF-enabled and position sensitive PET detectors was proposed and evaluated.</p> Purpose <p>The proposed readout scheme employs radio frequency (RF) amplifiers for timing readout and an FPGA-based dual-polarity charge-to-digital converter (FPGA-dQDC) for energy readout. The PET detector consists of a <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(15 \times 15\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>15</mn> <mo>×</mo> <mn>15</mn> </mrow> </math></EquationSource> </InlineEquation> array of <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(1 \times 1 \times 10~{\text {mm}}^3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>×</mo> <mn>1</mn> <mo>×</mo> <mn>10</mn> <mspace width="3.33333pt" /> <msup> <mrow> <mtext>mm</mtext> </mrow> <mn>3</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> LYSO crystals coupled to a <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(5 \times 5\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>5</mn> <mo>×</mo> <mn>5</mn> </mrow> </math></EquationSource> </InlineEquation> array of <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(3 \times 3~{\text {mm}}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>3</mn> <mo>×</mo> <mn>3</mn> <mspace width="3.33333pt" /> <msup> <mrow> <mtext>mm</mtext> </mrow> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> SiPMs through a light guide. All crystals are separated by enhanced specular reflector (ESR) films. The timing signals from the SiPM array are amplified and multiplexed with a 25:1 ratio, while the energy signals are multiplexed by row/column summation to form a "<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(5+5\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>5</mn> <mo>+</mo> <mn>5</mn> </mrow> </math></EquationSource> </InlineEquation>" readout configuration. The FPGA-dQDC system consists of an analog board implementing the dQDC circuit and a digital board based on a Cyclone V FPGA for discharge control, data buffering, and digital processing.</p> Results <p>The system was evaluated using a dual-detector coincidence setup consisting of a single-crystal reference detector and the "<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(5+5\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>5</mn> <mo>+</mo> <mn>5</mn> </mrow> </math></EquationSource> </InlineEquation>" PET detector. The average coincidence time resolution (CTR) obtained from the CTR map was measured to be <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(381.68 \pm 9.80\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>381.68</mn> <mo>±</mo> <mn>9.80</mn> </mrow> </math></EquationSource> </InlineEquation> ps full width at half maximum (FWHM). After saturation correction, the average energy resolution of all crystals was <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(10.83 \pm 0.68\%\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>10.83</mn> <mo>±</mo> <mn>0.68</mn> <mo>%</mo> </mrow> </math></EquationSource> </InlineEquation>.</p> Conclusion <p>The proposed RF-amplifier-based timing readout and FPGA-dQDC energy readout scheme enables compact and power-efficient front-end electronics for TOF-PET detector prototype development.</p>

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FPGA-based dual-polarity charge readout with fast timing for small-animal PET applications

  • Bo Wang,
  • Chuijiang Meng,
  • Xiaohan Sun,
  • Kun Hu

摘要

Purpose

Time-of-flight (TOF) capability of positron emission tomography (PET) can improve the signal-to-noise ratio (SNR) in the image reconstruction. A new high-density and compact front-end electronics design for TOF-enabled and position sensitive PET detectors was proposed and evaluated.

Purpose

The proposed readout scheme employs radio frequency (RF) amplifiers for timing readout and an FPGA-based dual-polarity charge-to-digital converter (FPGA-dQDC) for energy readout. The PET detector consists of a \(15 \times 15\) 15 × 15 array of \(1 \times 1 \times 10~{\text {mm}}^3\) 1 × 1 × 10 mm 3 LYSO crystals coupled to a \(5 \times 5\) 5 × 5 array of \(3 \times 3~{\text {mm}}^2\) 3 × 3 mm 2 SiPMs through a light guide. All crystals are separated by enhanced specular reflector (ESR) films. The timing signals from the SiPM array are amplified and multiplexed with a 25:1 ratio, while the energy signals are multiplexed by row/column summation to form a " \(5+5\) 5 + 5 " readout configuration. The FPGA-dQDC system consists of an analog board implementing the dQDC circuit and a digital board based on a Cyclone V FPGA for discharge control, data buffering, and digital processing.

Results

The system was evaluated using a dual-detector coincidence setup consisting of a single-crystal reference detector and the " \(5+5\) 5 + 5 " PET detector. The average coincidence time resolution (CTR) obtained from the CTR map was measured to be \(381.68 \pm 9.80\) 381.68 ± 9.80 ps full width at half maximum (FWHM). After saturation correction, the average energy resolution of all crystals was \(10.83 \pm 0.68\%\) 10.83 ± 0.68 % .

Conclusion

The proposed RF-amplifier-based timing readout and FPGA-dQDC energy readout scheme enables compact and power-efficient front-end electronics for TOF-PET detector prototype development.