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Research ArticleBasic Science Investigations

Multimodal Partial-Volume Correction: Application to 18F-Fluoride PET/CT Bone Metastases Studies

Elisabetta Grecchi, Jim O’Doherty, Mattia Veronese, Charalampos Tsoumpas, Gary J. Cook and Federico E. Turkheimer
Journal of Nuclear Medicine September 2015, 56 (9) 1408-1414; DOI: https://doi.org/10.2967/jnumed.115.160598
Elisabetta Grecchi
1Centre for Neuroimaging, Institute of Psychiatry, Psychology and Neuroscience King’s College London, London, United Kingdom
2Division of Imaging Sciences & Biomedical Engineering, King's College London, London, United Kingdom
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Jim O’Doherty
3PET Imaging Centre, Division of Imaging Sciences and Biomedical Engineering, King’s College London, King’s Health Partners, St. Thomas’s Hospital, London, United Kingdom; and
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Mattia Veronese
1Centre for Neuroimaging, Institute of Psychiatry, Psychology and Neuroscience King’s College London, London, United Kingdom
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Charalampos Tsoumpas
2Division of Imaging Sciences & Biomedical Engineering, King's College London, London, United Kingdom
4Division of Biomedical Imaging, University of Leeds, Leeds, United Kingdom
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Gary J. Cook
2Division of Imaging Sciences & Biomedical Engineering, King's College London, London, United Kingdom
3PET Imaging Centre, Division of Imaging Sciences and Biomedical Engineering, King’s College London, King’s Health Partners, St. Thomas’s Hospital, London, United Kingdom; and
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Federico E. Turkheimer
1Centre for Neuroimaging, Institute of Psychiatry, Psychology and Neuroscience King’s College London, London, United Kingdom
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  • FIGURE 1.
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    FIGURE 1.

    Graphical representation of SFS-RR algorithm. (A) Structural reference image required by SFS-RR algorithm is computed from CT and PET images. (B) Wavelet decomposition of functional and structural images. (C) Functional and structural wavelet coefficients are combined to get new high-resolution PET coefficients. (D) Inverse wavelet transform of coefficients obtained from step C resulting in the new high-resolution SFS-RR PET image. For detailed mathematic formulation, refer to supplemental materials.

  • FIGURE 2.
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    FIGURE 2.

    18F-fluoride PET/CT transaxial images of 3 different phantom experiment acquisitions (1 for each line). Alongside CT image (first column) are 3 different types of functional images: standard PET images (second column), images resulting from inclusion of PSF model into reconstruction (third column), and images resulting after application of SFS resolution recovery algorithm (fourth column). For detailed information on lesion volume, CM, and 18F-FDG concentrations, refer to Table 1. Green markers highlight sphere 2, blue markers highlight sphere 4, and red markers highlight sphere 6.

  • FIGURE 3.
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    FIGURE 3.

    RMSE and noise analysis. For each sphere (S1–S6), 3 values corresponding to images obtained with different modalities are reported: standard PET (dashed circle), PET with PSF reconstruction (white triangle), and PET corrected with SFS-RR algorithm (black diamond). (A) RMSE for 6 spheres obtained as average among 3 phantom experiments. (B and C) CNR computed for each sphere against uniform region in phantom background. Only experiments 1 and 2 are reported for consistency reasons (in experiment 3, three spheres have zero activity).

  • FIGURE 4.
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    FIGURE 4.

    Maximum-intensity projection and transaxial views of representative subject (patient 01). (Left) Standard PET. (Right) PET corrected with SFS-RR algorithm. Red and blue markers highlight 2 representative lesions (spine and rib, respectively) that appear sharper in PET-SFS image than in standard PET 1. Dashed lines indicate slice position of transaxial views reported below maximum-intensity projection.

  • FIGURE 5.
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    FIGURE 5.

    Bland–Altman plots showing differences in MATV and activity quantification when estimates are computed in images obtained with standard PET and PET corrected with SFS-RR algorithm. Each gray circle represents specific lesion; all lesions of all patients are reported. Differences between estimates for SUVmean (A), SUVmax (B), and SUVpeak (C) are reported as relative percentage difference. MATV (D) is reported as absolute difference in cm3.

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    TABLE 1

    CT Contrast Medium and PET Radiotracer Concentrations

    Experiment 1Experiment 2Experiment 3
    Phantom compartmentsIodine contrast medium (mg/mL)18F-FDG (kBq/mL)Iodine contrast medium (mg/mL)18F-FDG (kBq/mL)Iodine contrast medium (mg/mL)18F-FDG (kBq/mL)Sphere volume (mL)
    Background1.08*4.56*1.20*5.29*1.20*5.70*9,700
    S16.00†53.20†6.00†66.50†1.20*5.70*26.52
    S26.00†53.20†42.00‡187.00‡41.20‡227.00‡11.49
    S36.00†53.20†6.00†66.50†1.20*5.70*5.57
    S41.00*148.50‡42.00‡187.00‡41.20‡227.00‡2.57
    S51.00*148.50‡6.00†66.50†1.20*5.70*1.15
    S61.00*148.50‡42.00‡187.00‡41.20‡227.00‡0.52
    • ↵* Concentration resulting in image contrast comparable to normal soft tissue.

    • ↵† Concentration resulting in image contrast comparable to normal bone.

    • ↵‡ Concentration resulting in image contrast comparable to metastatic bone.

    • Concentrations of iodine (from Omnipaque300) and 18F-FDG injected in all phantom compartments for each experiment. Compartment volumes are also reported. Spheres 4–6, experiment 1, and spheres 1, 3, and 5, experiment 3, are filled with same radioactivity concentration as background; as a result they are indiscernible in PET image.

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    TABLE 2

    Quantitative Results of Phantom Experiments

    SUVmean (g/mL)SUVmax (g/mL)SUVpeak (g/mL)MATV (cm3)
    ExperimentPETPETPSFPETSFSPETPETPSFPETSFSPETPETPSFPETSFSGround truth (g/mL)PETPETPSFPETSFSGround truth
    1
     S15.665.956.448.458.8410.038.038.178.199.6032.2230.8130.4426.52
     S25.295.646.288.509.0010.698.508.87.889.6013.8413.2012.4711.49
     S34.545.015.737.738.589.377.737.877.979.607.466.726.755.57
     S410.2212.2513.1718.6422.1222.1118.6416.2518.2424.873.522.863.332.57
     S57.729.5112.6014.8218.5523.5614.8110.9113.7524.871.981.561.371.15
     S64.215.278.508.1910.5216.924.7710.5111.9624.871.341.100.830.52
    2
     S14.654.875.166.857.087.786.626.696.548.6734.2832.9631.0326.52
     S210.4011.1111.5516.2816.8317.1615.6315.8714.9224.3814.0613.5413.5211.49
     S33.874.254.606.747.257.576.096.616.398.677.536.896.535.57
     S49.9311.4212.4017.5720.2119.7613.9515.9017.2024.383.353.033.202.57
     S52.493.084.024.976.057.713.143.574.768.672.321.711.371.15
     S64.566.168.578.7911.7616.145.027.6010.0324.381.390.980.860.52
    3
     S224.5925.9526.6338.1138.0137.9037.2036.8234.8740.6113.5213.4213.5911.49
     S416.6819.0820.7429.9234.1233.9723.7826.8929.1940.613.353.083.252.57
     S67.369.7813.6113.7718.3325.528.0214.0819.1540.611.250.900.790.52
    • SUVmean, SUVmax, SUVpeak, and MATV estimates computed for phantom spheres after automated segmentation for all experiments 1–3. Values are reported for estimates obtained with 3 different modalities (standard PET, PET reconstructed with a PSF model, and PET corrected with SFS-RR algorithm) alongside corresponding ground truth values.

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Journal of Nuclear Medicine: 56 (9)
Journal of Nuclear Medicine
Vol. 56, Issue 9
September 1, 2015
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Multimodal Partial-Volume Correction: Application to 18F-Fluoride PET/CT Bone Metastases Studies
Elisabetta Grecchi, Jim O’Doherty, Mattia Veronese, Charalampos Tsoumpas, Gary J. Cook, Federico E. Turkheimer
Journal of Nuclear Medicine Sep 2015, 56 (9) 1408-1414; DOI: 10.2967/jnumed.115.160598

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Multimodal Partial-Volume Correction: Application to 18F-Fluoride PET/CT Bone Metastases Studies
Elisabetta Grecchi, Jim O’Doherty, Mattia Veronese, Charalampos Tsoumpas, Gary J. Cook, Federico E. Turkheimer
Journal of Nuclear Medicine Sep 2015, 56 (9) 1408-1414; DOI: 10.2967/jnumed.115.160598
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Keywords

  • 18F-fluoride
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