Literature DB >> 27295658

Improving Depth, Energy and Timing Estimation in PET Detectors with Deconvolution and Maximum Likelihood Pulse Shape Discrimination.

Eric Berg, Emilie Roncali, Will Hutchcroft, Jinyi Qi, Simon R Cherry.   

Abstract

In a scintillation detector, the light generated in the scintillator by a gamma interaction is converted to photoelectrons by a photodetector and produces a time-dependent waveform, the shape of which depends on the scintillator properties and the photodetector response. Several depth-of-interaction (DOI) encoding strategies have been developed that manipulate the scintillator's temporal response along the crystal length and therefore require pulse shape discrimination techniques to differentiate waveform shapes. In this work, we demonstrate how maximum likelihood (ML) estimation methods can be applied to pulse shape discrimination to better estimate deposited energy, DOI and interaction time (for time-of-flight (TOF) PET) of a gamma ray in a scintillation detector. We developed likelihood models based on either the estimated detection times of individual photoelectrons or the number of photoelectrons in discrete time bins, and applied to two phosphor-coated crystals (LFS and LYSO) used in a previously developed TOF-DOI detector concept. Compared with conventional analytical methods, ML pulse shape discrimination improved DOI encoding by 27% for both crystals. Using the ML DOI estimate, we were able to counter depth-dependent changes in light collection inherent to long scintillator crystals and recover the energy resolution measured with fixed depth irradiation (~11.5% for both crystals). Lastly, we demonstrated how the Richardson-Lucy algorithm, an iterative, ML-based deconvolution technique, can be applied to the digitized waveforms to deconvolve the photodetector's single photoelectron response and produce waveforms with a faster rising edge. After deconvolution and applying DOI and time-walk corrections, we demonstrated a 13% improvement in coincidence timing resolution (from 290 to 254 ps) with the LFS crystal and an 8% improvement (323 to 297 ps) with the LYSO crystal.

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Year:  2016        PMID: 27295658      PMCID: PMC5119913          DOI: 10.1109/TMI.2016.2577539

Source DB:  PubMed          Journal:  IEEE Trans Med Imaging        ISSN: 0278-0062            Impact factor:   10.048


  12 in total

1.  Depth-of-interaction measurement in a single-layer crystal array with a single-ended readout using digital silicon photomultiplier.

Authors:  Min Sun Lee; Jae Sung Lee
Journal:  Phys Med Biol       Date:  2015-08-06       Impact factor: 3.609

2.  Depth of interaction resolution measurements for a high resolution PET detector using position sensitive avalanche photodiodes.

Authors:  Yongfeng Yang; Purushottam A Dokhale; Robert W Silverman; Kanai S Shah; Mickel A McClish; Richard Farrell; Gerald Entine; Simon R Cherry
Journal:  Phys Med Biol       Date:  2006-04-10       Impact factor: 3.609

3.  Depth of interaction decoding of a continuous crystal detector module.

Authors:  T Ling; T K Lewellen; R S Miyaoka
Journal:  Phys Med Biol       Date:  2007-03-29       Impact factor: 3.609

4.  Maximum likelihood positioning in the scintillation camera using depth of interaction.

Authors:  D Gagnon; N Pouliot; L Laperriere; M Therrien; P Olivier
Journal:  IEEE Trans Med Imaging       Date:  1993       Impact factor: 10.048

5.  DOI Determination by Rise Time Discrimination in Single-Ended Readout for TOF PET Imaging.

Authors:  R I Wiener; S Surti; J S Karp
Journal:  IEEE Trans Nucl Sci       Date:  2013-06       Impact factor: 1.679

6.  Timing properties of phosphor-coated polished LSO crystals.

Authors:  Jeffrey P Schmall; Emilie Roncali; Eric Berg; Varsha Viswanath; Junwei Du; Simon R Cherry
Journal:  Phys Med Biol       Date:  2014-07-22       Impact factor: 3.609

7.  Pulse shape discrimination and classification methods for continuous depth of interaction encoding PET detectors.

Authors:  Emilie Roncali; Jennifer E Phipps; Laura Marcu; Simon R Cherry
Journal:  Phys Med Biol       Date:  2012-09-25       Impact factor: 3.609

8.  Calibration Method for ML Estimation of 3D Interaction Position in a Thick Gamma-Ray Detector.

Authors:  William C J Hunter; Harrison H Barrett; Lars R Furenlid
Journal:  IEEE Trans Nucl Sci       Date:  2009-02-10       Impact factor: 1.679

9.  Continuous depth-of-interaction encoding using phosphor-coated scintillators.

Authors:  Huini Du; Yongfeng Yang; Jarek Glodo; Yibao Wu; Kanai Shah; Simon R Cherry
Journal:  Phys Med Biol       Date:  2009-03-03       Impact factor: 3.609

10.  Maximum-Likelihood Methods for Processing Signals From Gamma-Ray Detectors.

Authors:  Harrison H Barrett; William C J Hunter; Brian William Miller; Stephen K Moore; Yichun Chen; Lars R Furenlid
Journal:  IEEE Trans Nucl Sci       Date:  2009-06-01       Impact factor: 1.679

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  4 in total

Review 1.  Innovations in Instrumentation for Positron Emission Tomography.

Authors:  Eric Berg; Simon R Cherry
Journal:  Semin Nucl Med       Date:  2018-03-12       Impact factor: 4.446

2.  Reaching 200-ps timing resolution in a time-of-flight and depth-of-interaction positron emission tomography detector using phosphor-coated crystals and high-density silicon photomultipliers.

Authors:  Sun Il Kwon; Alessandro Ferri; Alberto Gola; Eric Berg; Claudio Piemonte; Simon R Cherry; Emilie Roncali
Journal:  J Med Imaging (Bellingham)       Date:  2016-11-23

3.  Using convolutional neural networks to estimate time-of-flight from PET detector waveforms.

Authors:  Eric Berg; Simon R Cherry
Journal:  Phys Med Biol       Date:  2018-01-11       Impact factor: 3.609

4.  Dynamic cardiac PET imaging: Technological improvements advancing future cardiac health.

Authors:  Grant T Gullberg; Uttam M Shrestha; Youngho Seo
Journal:  J Nucl Cardiol       Date:  2018-01-31       Impact factor: 5.952

  4 in total

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