Skip to main page content
U.S. flag

An official website of the United States government

Dot gov

The .gov means it’s official.
Federal government websites often end in .gov or .mil. Before sharing sensitive information, make sure you’re on a federal government site.

Https

The site is secure.
The https:// ensures that you are connecting to the official website and that any information you provide is encrypted and transmitted securely.

Access keys NCBI Homepage MyNCBI Homepage Main Content Main Navigation
. 2020 Sep;84(3):1624-1637.
doi: 10.1002/mrm.28185. Epub 2020 Feb 21.

The 2016 QSM Challenge: Lessons learned and considerations for a future challenge design

Affiliations

The 2016 QSM Challenge: Lessons learned and considerations for a future challenge design

Carlos Milovic et al. Magn Reson Med. 2020 Sep.

Abstract

Purpose: The 4th International Workshop on MRI Phase Contrast and QSM (2016, Graz, Austria) hosted the first QSM Challenge. A single-orientation gradient recalled echo acquisition was provided, along with COSMOS and the χ33 STI component as ground truths. The submitted solutions differed more than expected depending on the error metric used for optimization and were generally over-regularized. This raised (unanswered) questions about the ground truths and the metrics utilized.

Methods: We investigated the influence of background field remnants by applying additional filters. We also estimated the anisotropic contributions from the STI tensor to the apparent susceptibility to amend the χ33 ground truth and to investigate the impact on the reconstructions. Lastly, we used forward simulations from the COSMOS reconstruction to investigate the impact noise had on the metric scores.

Results: Reconstructions compared against the amended STI ground truth returned lower errors. We show that the background field remnants had a minor impact in the errors. In the absence of inconsistencies, all metrics converged to the same regularization weights, whereas structural similarity index metric was more insensitive to such inconsistencies.

Conclusion: There was a mismatch between the provided data and the ground truths due to the presence of unaccounted anisotropic susceptibility contributions and noise. Given the lack of reliable ground truths when using in vivo acquisitions, simulations are suggested for future QSM Challenges.

Keywords: FANSI; magnetic susceptibility; quantitative susceptibility mapping; total variation.

PubMed Disclaimer

Figures

Figure 1.
Figure 1.
Single orientation acquisition (A) and background remnant models using (B) weak-harmonics (WH-QSM, with β=5, μh=0.1, the weak harmonic regularization weights) and (C) the Projection onto Dipole Fields (PDF) methods.
Figure 2.
Figure 2.
Differences between forward simulated phases and the provided single orientation acquisition (A) for: (B and E) the χ33 component, (C and F) COSMOS, and (D and G) the STI equation, including the χ13 and χ23 anisotropic components. The right column shows the same difference maps as the left column, but with a higher contrast to reveal subtle differences.
Figure 3.
Figure 3.
The χ33 (isotropic) component and correction factors, χcorr (B and C, derived from χ13 and χ23 anisotropic components) used to estimate χSTI-TKD and χSTI-L2 respectively (D and E).
Figure 4.
Figure 4.
Selected optimal reconstructions of the challenge data, based on the RMSE (left panel) and SSIM (right panel) metrics, using χ33 (A,D) and χSTI-L2 (B, E) as ground truth. (C ,F) show optimal reconstructions of the amended phase (to remove anisotropic components) and using χ33 as ground truth (χ3333).
Figure 5.
Figure 5.
Metric scores of the reconstruction using COSMOS-based forward simulations. Optimal (A) RMSE, (B) HFEN and (C) SSIM scores are presented as function of SNR. Metric scores for in vivo reconstructions using χ33 and χSTI-L2 as ground truth, along with reconstructions of the amended phase with TV-FANSI (χ3333) and WH-QSM, are also included. (D) presents the optimal regularization weight for each metric and SNR setting. Ranges for the optimal reconstructions using χ33, χSTI-L2 and χ3333 also included.
Figure 6.
Figure 6.
(A) RMSE, (B) HFEN and (C) SSIM optimal scores for reconstructions at SNR=64 and SNR=32 and their regularization weight. Simulations included the phase forward calculated using COSMOS Φ with the addition of the background remnants obtained using PDF (ΦPDF) and the anisotropic phase contributions (Φcorr) calculated from the χ13 and χ23 components of the STI tensor. (D) Shows the range span of optimal regularization weight values by the different simulations and in vivo reconstructions, for a given metric.

References

    1. Mittal S, Wu Z, Neelavalli J, Haacke EM. Susceptibility-weighted imaging: Technical aspects and clinical applications, part 2. Am J Neuroradiol. 2009;30:232–252. doi:10.3174/ajnr.A1461 - DOI - PMC - PubMed
    1. Haacke EM, Liu S, Buch S, Zheng W, Wu D, Ye Y. Quantitative susceptibility mapping: Current status and future directions. Magn Reson Imaging. 2015;33:1–25. doi:10.1016/j.mri.2014.09.004 - DOI - PubMed
    1. Salomir R, De Senneville BD, Moonen CTW. A fast calculation method for magnetic field inhomogeneity due to an arbitrary distribution of bulk susceptibility. Concepts Magn Reson. 2003;19B:26–34. doi:10.1002/cmr.b.10083 - DOI
    1. Marques JPP, Bowtell R. Application of a fourier-based method for rapid calculation of field inhomogeneity due to spatial variation of magnetic susceptibility. Concepts Magn Reson Part B Magn Reson Eng. 2005;25:65–78. doi:10.1002/cmr.b.20034 - DOI
    1. Shmueli K, de Zwart J a, van Gelderen P, Li T-Q, Dodd SJ, Duyn JH. Magnetic susceptibility mapping of brain tissue in vivo using MRI phase data. Magn Reson Med. 2009;62:1510–1522. doi:10.1002/mrm.22135 - DOI - PMC - PubMed

Publication types