The influence of different signal-to-background ratios on spatial resolution and F18-FDG-PET quantification using point spread function and time-of-flight reconstruction

BackgroundF18-fluorodeoxyglucose positron-emission tomography (FDG-PET) reconstruction algorithms can have substantial influence on quantitative image data used, e.g., for therapy planning or monitoring in oncology. We analyzed radial activity concentration profiles of differently reconstructed FDG-PET images to determine the influence of varying signal-to-background ratios (SBRs) on the respective spatial resolution, activity concentration distribution, and quantification (standardized uptake value [SUV], metabolic tumor volume [MTV]).MethodsMeasurements were performed on a Siemens Biograph mCT 64 using a cylindrical phantom containing four spheres (diameter, 30 to 70 mm) filled with F18-FDG applying three SBRs (SBR1, 16:1; SBR2, 6:1; SBR3, 2:1). Images were reconstructed employing six algorithms (filtered backprojection [FBP], FBP + time-of-flight analysis [FBP + TOF], 3D-ordered subset expectation maximization [3D-OSEM], 3D-OSEM + TOF, point spread function [PSF], PSF + TOF). Spatial resolution was determined by fitting the convolution of the object geometry with a Gaussian point spread function to radial activity concentration profiles. MTV delineation was performed using fixed thresholds and semiautomatic background-adapted thresholding (ROVER, ABX, Radeberg, Germany).ResultsThe pairwise Wilcoxon test revealed significantly higher spatial resolutions for PSF + TOF (up to 4.0 mm) compared to PSF, FBP, FBP + TOF, 3D-OSEM, and 3D-OSEM + TOF at all SBRs (each P < 0.05) with the highest differences for SBR1 decreasing to the lowest for SBR3. Edge elevations in radial activity profiles (Gibbs artifacts) were highest for PSF and PSF + TOF declining with decreasing SBR (PSF + TOF largest sphere; SBR1, 6.3%; SBR3, 2.7%). These artifacts induce substantial SUVmax overestimation compared to the reference SUV for PSF algorithms at SBR1 and SBR2 leading to substantial MTV underestimation in threshold-based segmentation. In contrast, both PSF algorithms provided the lowest deviation of SUVmean from reference SUV at SBR1 and SBR2.ConclusionsAt high contrast, the PSF algorithms provided the highest spatial resolution and lowest SUVmean deviation from the reference SUV. In contrast, both algorithms showed the highest deviations in SUVmax and threshold-based MTV definition. At low contrast, all investigated reconstruction algorithms performed approximately equally. The use of PSF algorithms for quantitative PET data, e.g., for target volume definition or in serial PET studies, should be performed with caution - especially if comparing SUV of lesions with high and low contrasts.

[1]  Habib Zaidi,et al.  A novel fuzzy C-means algorithm for unsupervised heterogeneous tumor quantification in PET. , 2010, Medical physics.

[2]  Christina Pfannenberg,et al.  Einfluss des Rekonstruktionsalgorithmus (UltraHD vs. OSEM3D) und der Auswertemethodik (SUV-Isokontur vs. SUV-Peak) auf die SUV-Quantifizierung am PET/CT (Siemens mCT-X4R) , 2013 .

[3]  Philippe Lambin,et al.  FDG-PET-CT reduces the interobserver variability in rectal tumor delineation. , 2012, Radiotherapy and oncology : journal of the European Society for Therapeutic Radiology and Oncology.

[4]  M. Hatt,et al.  Comparison Between 18F-FDG PET Image–Derived Indices for Early Prediction of Response to Neoadjuvant Chemotherapy in Breast Cancer , 2013, The Journal of Nuclear Medicine.

[5]  H Bergmann,et al.  Influence of PET reconstruction parameters on the TrueX algorithm. A combined phantom and patient study. , 2013, Nuklearmedizin. Nuclear medicine.

[6]  Koichiro Abe,et al.  Improvement in PET/CT Image Quality with a Combination of Point-Spread Function and Time-of-Flight in Relation to Reconstruction Parameters , 2012, The Journal of Nuclear Medicine.

[7]  D. Groheux,et al.  18F-FDG PET/CT in Staging Patients with Locally Advanced or Inflammatory Breast Cancer: Comparison to Conventional Staging , 2013, The Journal of Nuclear Medicine.

[8]  Y. Erdi,et al.  FDG-PET standardized uptake values in normal anatomical structures using iterative reconstruction segmented attenuation correction and filtered back-projection , 2001, European Journal of Nuclear Medicine.

[9]  Helmar Bergmann,et al.  PET based volume segmentation with emphasis on the iterative TrueX algorithm. , 2012, Zeitschrift fur medizinische Physik.

[10]  D Visvikis,et al.  Fuzzy hidden Markov chains segmentation for volume determination and quantitation in PET. , 2007, Physics in medicine and biology.

[11]  F Hofheinz,et al.  A volume of intersection approach for on-the-fly system matrix calculation in 3D PET image reconstruction. , 2014, Physics in medicine and biology.

[12]  Liane Oehme,et al.  Automatische Volumenabgrenzung in der onkologischen PET – Bewertung eines entsprechenden Software-Werkzeugs und Vergleich mit manueller Abgrenzung anhand klinischer Datensätze , 2012 .

[13]  Antonio Rodríguez-Fernández,et al.  Fluorine-18 fluorodeoxyglucose PET in the preoperative staging of colorectal cancer , 2007, European Journal of Nuclear Medicine and Molecular Imaging.

[14]  Shingo Baba,et al.  Influences of point-spread function and time-of-flight reconstructions on standardized uptake value of lymph node metastases in FDG-PET. , 2014, European journal of radiology.

[15]  Anne Bol,et al.  A gradient-based method for segmenting FDG-PET images: methodology and validation , 2007, European Journal of Nuclear Medicine and Molecular Imaging.

[16]  E Prieto,et al.  [Contribution of time of flight and point spread function modeling to the performance characteristics of the PET/CT Biograph mCT scanner]. , 2013, Revista espanola de medicina nuclear e imagen molecular.

[17]  D. Townsend,et al.  Impact of Time-of-Flight on PET Tumor Detection , 2009, Journal of Nuclear Medicine.

[18]  David Dagan Feng,et al.  Real-Time Volume Rendering Visualization of Dual-Modality PET/CT Images With Interactive Fuzzy Thresholding Segmentation , 2007, IEEE Transactions on Information Technology in Biomedicine.

[19]  R. Tibshirani,et al.  Generalized Additive Models , 1986 .

[20]  Vladimir Y. Panin,et al.  Fully 3-D PET reconstruction with system matrix derived from point source measurements , 2006, IEEE Transactions on Medical Imaging.

[21]  B. C. Penney,et al.  Prognostic value of metabolic tumor burden from (18)F-FDG PET in surgical patients with non-small-cell lung cancer. , 2013, Academic radiology.

[22]  Ronald Boellaard,et al.  Impact of [18F]FDG PET imaging parameters on automatic tumour delineation: need for improved tumour delineation methodology , 2011, European Journal of Nuclear Medicine and Molecular Imaging.

[23]  Gang Huang,et al.  Is 18F-FDG PET accurate to predict neoadjuvant therapy response in breast cancer? A meta-analysis , 2011, Breast Cancer Research and Treatment.

[24]  B. C. Penney,et al.  A Gaussian mixture model for definition of lung tumor volumes in positron emission tomography. , 2007, Medical physics.

[25]  K Thielemans,et al.  Image-based point spread function implementation in a fully 3D OSEM reconstruction algorithm for PET , 2010, Physics in medicine and biology.

[26]  Philippe Lambin,et al.  Effects of radiotherapy planning with a dedicated combined PET-CT-simulator of patients with non-small cell lung cancer on dose limiting normal tissues and radiation dose-escalation: a planning study. , 2005, Radiotherapy and oncology : journal of the European Society for Therapeutic Radiology and Oncology.

[27]  D. Binns,et al.  Effect of PET/CT on Management of Patients with Non–Small Cell Lung Cancer: Results of a Prospective Study with 5-Year Survival Data , 2012, The Journal of Nuclear Medicine.

[28]  Michael Casey,et al.  Clinical impact of time-of-flight and point response modeling in PET reconstructions: a lesion detection study , 2013, Physics in medicine and biology.

[29]  Cyrill Burger,et al.  Automated functional image-guided radiation treatment planning for rectal cancer. , 2005, International journal of radiation oncology, biology, physics.

[30]  W. Oyen,et al.  FDG PET and PET/CT: EANM procedure guidelines for tumour PET imaging: version 1.0 , 2009, European Journal of Nuclear Medicine and Molecular Imaging.

[31]  F Hofheinz,et al.  Effects of cold sphere walls in PET phantom measurements on the volume reproducing threshold , 2010, Physics in medicine and biology.

[32]  Dietmar Georg,et al.  Einfluss der PET-Rekonstruktionsparameter auf den TrueX-Algorithmus , 2013 .

[33]  Elena Prieto,et al.  Impact of Time-of-Flight and Point-Spread-Function in SUV Quantification for Oncological PET , 2013, Clinical nuclear medicine.

[34]  F Hofheinz,et al.  Automatic volume delineation in oncological PET , 2011, Nuklearmedizin.

[35]  E. Hewitt,et al.  The Gibbs-Wilbraham phenomenon: An episode in fourier analysis , 1979 .

[36]  B. C. Penney,et al.  Prognostic value of metabolic tumor burden on 18F-FDG PET in nonsurgical patients with non-small cell lung cancer , 2011, European Journal of Nuclear Medicine and Molecular Imaging.

[37]  Ralph A Bundschuh,et al.  Radioactive spheres without inactive wall for lesion simulation in PET. , 2008, Zeitschrift fur medizinische Physik.