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Optimized filter functions for filtered back projection reconstructions

  • *Corresponding author: Judith Nickel

    *Corresponding author: Judith Nickel

The authors are listed in alphabetical order. This work was supported by the Deutsche Forschungsgemeinschaft (DFG) - project numbers 530863002 and 281474342/GRK2224/2 - as well as the Bundesministerium für Bildung und Forschung (BMBF) - funding code 03TR07W11A.

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  • The method of filtered back projection (FBP) is a widely used reconstruction technique in X-ray computerized tomography (CT), which is particularly important in clinical diagnostics. To reduce scanning times and radiation doses in medical CT settings, enhancing the reconstruction quality of the FBP method is essential. To this end, this paper focuses on analytically optimizing the applied filter function. We derive a formula for the filter that minimizes the expected squared $ {\mathrm L}^2 $-norm of the difference between the FBP reconstruction, given infinite noisy measurement data and the true target function. Additionally, we adapt our derived filter to the case of finitely many measurements. The resulting filter functions have a closed-form representation, do not require a training dataset, and, thus, provide an easy-to-implement, out-of-the-box solution. Our theoretical findings are supported by numerical experiments based on both simulated and real CT data.

    Mathematics Subject Classification: 44A12, 65R32, 4A12.

    Citation:

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  • Figure 1.  Selection of classical low-pass filters used in our numerical experiments

    Figure 2.  Phantoms used in our numerical experiments along with their sinograms (Radon data)

    Figure 3.  Noisy sinograms of the Shepp-Logan phantom with different noise levels

    Figure 4.  Plots of the MSE and SSIM of FBP reconstructions for the Shepp-Logan phantom

    Figure 5.  Plots of the optimized filter functions $ A_{L,D}^\ast $, $ A_{L,D}^\varepsilon $ and $ \hat{A}_{L,D}^\varepsilon $ for the noisy Shepp-Logan sinogram with $ N_\varphi \in \{90,180,360\} $ and $ p_{\mathrm{noise}} \in \{0.05, \, 0.1, \, 0.15\} $

    Figure 6.  Reconstructions of Shepp-Logan phantom from noisy Radon data ($ p_\mathrm{noise} = 0.1 $, $ N_\varphi = 360 $)

    Figure 7.  Plots of the MSE and SSIM of FBP reconstructions for the modified Shepp-Logan phantom

    Figure 8.  Reconstructions of modified Shepp-Logan phantom from noisy Radon data ($ p_\mathrm{noise} = 0.1 $, $ N_\varphi = 360 $)

    Figure 9.  2DeteCT slice 1942 (mode 1) sinogram with target reconstruction

    Figure 10.  Reconstructions of 2DeteCT slice 1942 (mode 1)

    Figure 11.  Zoomed-in reconstructions of 2DeteCT slice 1942 (mode 1)

    Figure 12.  Plots of the MSE and SSIM of FBP reconstructions with the three best filter functions for the Shepp-Logan phantom

    Figure 13.  Plots of the MSE and SSIM of FBP reconstructions with the three best filter functions for the modified Shepp-Logan phantom

    Table 1.  Window functions of classical low-pass filters, where $ W(\sigma) = 0 $ for all $ |\sigma| > 1 $ in all cases

    Name $ W(\sigma) $ for $ |\sigma|\leq 1 $ Parameter
    Ram-Lak 1 -
    Shepp-Logan $ {\rm{sinc}}(\tfrac{\pi \sigma}{2}) $ -
    Cosine $ \cos(\tfrac{\pi \sigma}{2}) $ -
    Hamming $ \beta + (1-\beta) \cos(\pi \sigma) $ $ \beta \in [\tfrac{1}{2},1] $
     | Show Table
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    Table 2.  MSE of FBP reconstructions for the 2DeteCT slice 1942 (mode 1)

    Filter MSE Filter MSE Filter MSE
    Ram-Lak $ 1.0703 \cdot 10^{-5} $ MR-FBP $ 1.2231 \cdot 10^{-5} $ $ \bar{A}_{L,D}^\ast $ $ 8.7733 \cdot 10^{-6} $
    Shepp-Logan $ 9.1803 \cdot 10^{-6} $ MR-FBP$ _\mathrm{GM} $ $ 9.8905 \cdot 10^{-6} $ $ \hat{A}_{L,D}^\varepsilon $ $ 9.1616 \cdot 10^{-6} $
    Cosine $ 9.5116 \cdot 10^{-6} $ SIRT-FBP $ 9.2900 \cdot 10^{-6} $ $ A_{L,D}^\varepsilon $ $ 9.0792 \cdot 10^{-6} $
     | Show Table
    DownLoad: CSV
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