IEEE 2026 NSS MIC RTSD

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Quantitative imaging, image assessment and standardization

Session chair: Lerche, ChristophW., Dr. (Forschungszentrum Jülich GmbH, Institut für Neurowissenschaften, Jülich, Germany); Roser, Jorge, Dr. (University of Lübeck, Lübeck, Germany)
 
Shortcut: MIC-04
Date: Wednesday, 11 November, 2026, 15:00 - 17:00
Location: MANUEL DE FALLA
Session type: MIC Session

Contents

Click on an contribution to preview the abstract content.

The underlined authors are the presenters. The authors in bold are the main authors.

15:00 MIC-04-01

Single-Source Cross-Tracer Brain PET Attenuation Correction via Anchored Flow Matching with Attenuation Maps from Simultaneous Reconstruction (#1516)

M.J. Cho1, 2, S.K. Kang3, J.S. Lee4, 5

1 Seoul National University, Interdisciplinary Program of Bioengineering, Seoul, Republic of Korea
2 Seoul National University, Integrated Major in Innovative Medical Science, Seoul, Republic of Korea
3 Samsung Ventures, Seoul, Republic of Korea
4 Seoul National University, Department of Nuclear Medicine, Seoul, Republic of Korea
5 Brightonix Imaging Inc., Seoul, Republic of Korea

Abstract

Accurate attenuation correction (AC) is essential for quantitative PET imaging, but CT-free AC across diverse radiotracers remains challenging. MLAA-derived μ-maps are useful inputs for deep learning-based AC. However, tracer-dependent biodistribution introduces domain shifts that limit the generalizability of models trained only on ¹⁸F-FDG. We propose a single-source cross-tracer CT-free AC framework that combines tracer-robust U-Net regression with anchored flow matching. Local Gamma Field augmentation is used during U-Net training to mimic anatomy-preserving regional intensity and contrast variations in MLAA μ-maps, encouraging tracer-independent MLAA-to-CT mapping. The U-Net output is then used as an anchor for an unconditional flow-matching model trained on CT μ-maps, enabling generative refinement from a reliable deterministic estimate. The proposed method achieved the highest PSNR across all evaluated tracers and reduced MLAA noise, tracer-specific artifacts, and U-Net over-smoothing. AC PET analysis showed strong agreement with CT-based AC PET, with regional uptake correlations closest to the identity line. These results demonstrate that the proposed framework enables accurate and structurally faithful μ-map estimation across multiple tracers using only FDG training data.

AcknowledgmentThis research was supported by the AI Computing Infrastructure Enhancement (GPU Rental Support) User Support Program funded by the Ministry of Science and ICT (MSIT), Republic of Korea. (No. RQT-25-090157)
References
[1] Hwang, D., Kang, S. K., Kim, K. Y., Seo, S., Paeng, J. C., Lee, D. S., & Lee, J. S. (2019). Generation of PET attenuation map for whole-body time-of-flight 18F-FDG PET/MRI using a deep neural network trained with simultaneously reconstructed activity and attenuation maps. Journal of Nuclear Medicine, 60(8), 1183-1189.
[2] Lipman, Y., Chen, R. T., Ben-Hamu, H., Nickel, M., & Le, M. Flow Matching for Generative Modeling. In The Eleventh International Conference on Learning Representations.
Keywords: Attenuation correction, cross-tracer generalization, CT-free PET, flow matching, maximum-likelihood reconstruction of attenuation and activity
15:15 MIC-04-02

High-Energy Penetration Correction in Multi-Aperture SPECT Using Aperture–Plate Ray Decomposition (#1606)

Y. Li1, Q. Wang2, L. He1, H. Li1

1 United Imaging Healthcare North America, MI, Houston, Texas, United States of America
2 United Imaging Healthcare, MI, Shanghai, China

Abstract

Multi-aperture single-photon emission computed tomography (SPECT) at <sup>131</sup>I (364&nbsp;keV) exhibits a detector-wide plate-penetration halo: a 1.8&nbsp;cm tungsten plate transmits ~4 &times; 10<sup>&minus;4</sup> at &mu;<sub>W</sub> = 4.4&nbsp;cm<sup>&minus;1</sup>. Prior corrections perform the aperture/plate split at the photon level via effective-radius point-spread function enlargement, or at the system-matrix level via per-ray full-physics tracing; both merge the two components at storage time, inflating memory by one to two orders of magnitude. We propose a <em>storage-agnostic</em> per-ray partition: a topological rule on the source-to-detector intersection list separates the response into a sparse, peaked aperture component <em>A</em> and a slowly varying plate halo <em>B</em>, upstream of any representation choice. The rule is mutually exclusive and jointly exhaustive, so <em>A</em><sub>ij</sub> + <em>B</em><sub>ij</sub> = <em>C</em><sub>ij</sub> holds bit-exactly against the unsplit baseline for any per-ray contribution functional; the plate path length is a closed-form slab chord minus an analytic aperture chord at O(<em>N</em><sub>ap</sub>) per ray. On a 34-module multi-aperture SPECT ring (small-aperture configuration), the identity holds bit-exactly across three projection modes (collimator-path, sensitivity, counts) for a centered single-photon source and across every pixel of 34 Jaszczak hot-rod <sup>131</sup>I views, with per-pixel plate intensity ~10<sup>&minus;4</sup>&ndash;10<sup>&minus;3</sup> of the aperture peak. OSEM correction with a lagged plate estimate will be presented at the conference.

References
[1] K. van Audenhaege, R. Van Holen, S. Vandenberghe, C. Vanhove, S. D. Metzler, and S. C. Moore, “Review of SPECT collimator selection, optimization, and fabrication for clinical and preclinical imaging,” Med. Phys., vol. 42, no. 8, pp. 4796–4813, 2015. [Online]. Available: https://doi.org/10.1118/1.4927061
[2] M. F. Smith and R. J. Jaszczak, “An analytic model of pinhole aperture penetration for 3D pinhole SPECT image reconstruction,” Phys. Med. Biol., vol. 43, no. 4, pp. 761–775, 1998. [Online]. Available: https://doi.org/10.1088/0031-9155/43/4/006
[3] S. D. Metzler and S. C. Moore, “Analytic determination of rectangular-pinhole sensitivity with penetration,” IEEE Trans. Med. Imag., vol. 39, no. 4, pp. 833–843, Apr. 2020. [Online]. Available: https://doi.org/10.1109/TMI.2019.2936187
[4] K. Vunckx, J. Nuyts, H. Vanbilloen, M. De Saint-Hubert, D. Vanderghinste, D. Rattat, F. M. Mottaghy, and M. Defrise, “Optimized multipinhole design for mouse imaging,” IEEE Trans. Nucl. Sci., vol. 56, no. 5, pp. 2696–2705, 2009. [Online]. Available: https://doi.org/10.1109/TNS.2009.2030194
[5] H. M. Hudson and R. S. Larkin, “Accelerated image reconstruction using ordered subsets of projection data,” IEEE Trans. Med. Imag., vol. 13, no. 4, pp. 601–609, 1994. [Online]. Available: https://doi.org/10.1109/42.363108
[6] Y. Li and H. Li, “Minkhole collimators for SPECT: Minkowski-sum aperture geometry and closed-form ray tracing,” in Proc. IEEE Nucl. Sci. Symp. Med. Imag. Conf. (NSS/MIC) RTSD, 2026, submitted.
Keywords: Single-photon emission computed tomography (SPECT), penetration correction, pinhole collimator, aperture--plate decomposition, ordered-subsets expectation-maximization (OSEM).
15:30 MIC-04-03

Improving Lutetium Background Radiation-based Attenuation Correction for CT-less PET Using Singles-derived Randoms (#2103)

B. Dai1, S. C. Moore1, M. E. Daube-Witherspoon1, F. M. Muller1, 2, J. S. Karp1

1 University of Pennsylvania, Department of Radiology, Philadelphia, Pennsylvania, United States of America
2 Ghent University, Faculty of Engineering and Architecture, Ghent, Belgium

Abstract

Lutetium background radiation in modern PET scanners enables activity- and tracer-independent transmission measurement for attenuation correction (AC) without CT scans. However, quantitative accuracy of attenuation maps (µ-maps) derived from lutetium transmission (Lu-Tx) is limited by low transmission statistics and noisy randoms estimation from delayed coincidences (DE). In this work, we investigate the use of singles-derived randoms (RS) to improve Lu-Tx-based AC for CT-less PET. Emission and Lu-Tx data were acquired simultaneously on the PennPET Explorer, a 142-cm long axial field-of-view (LAFOV) scanner. µ-maps were reconstructed using maximum-likelihood transmission reconstruction with randoms estimated from either delayed coincidences or singles data, then used for attenuation and scatter correction during PET image reconstruction. The methods were evaluated using physical phantoms, including uniform cylinders, a 190-cm pipe phantom, cylinders with non-uniform axial activity distributions, and an image quality (IQ) phantom. Data were subsampled to simulate low-count short clinical scans. RS produced substantially smoother sinograms while maintaining agreement with DE in total randoms counts. Incorporation of RS improved axial uniformity, reduced noise, and mitigated emission contamination-induced bias in µ-maps, particularly under low-count conditions and non-uniform activity distributions. In IQ phantom studies, AC PET images reconstructed using RS demonstrated contrast comparable to CT-AC PET, whereas DE led to reduced contrast and increased bias, especially for short scans. These results demonstrate that RS improves the quantitative accuracy of Lu-Tx-based AC and support the proposed method as a practical pathway towards CT-less PET for both long dynamic imaging and short clinical scans.

AcknowledgmentThis work was supported by NIH CA-113941. FMM acknowledges support from the Research Foundation Flanders (11P0E24N0). Authors thank S McDonald for phantom experiments.
References
[1] Sari H, Teimoorisichani M, Viscione M, et al. Feasibility of an Ultra-Low-Dose PET Scan Protocol with CT-Based and LSO-TX–Based Attenuation Correction Using a Long–Axial-Field-of-View PET/CT Scanner. Journal of Nuclear Medicine. 2025. doi:10.2967/jnumed.124.268380
[2] Daube-Witherspoon ME, Moore SC, Karp JS. Randoms Estimation for Long Axial Field-of-View PET. IEEE Transactions on Radiation and Plasma Medical Sciences. 2025:1-1. doi:10.1109/TRPMS.2025.3591035
[3] Dai B, Daube-Witherspoon ME, McDonald S, et al. Performance evaluation of the PennPET explorer with expanded axial coverage. Physics in Medicine & Biology. 2023;68(9):095007. doi:10.1088/1361-6560/acc722
[4] Li Y, Matej S, Karp JS. Practical joint reconstruction of activity and attenuation with autonomous scaling for time-of-flight PET. Phys Med Biol. 2020;65(23):235037. doi:10.1088/1361-6560/ab8d75
Keywords: Lutetium background radiation, attenuation correction, randoms estimation, CT-less PET
15:45 MIC-04-04

Estimation of random events in PET imaging using the time differences of uncorrelated singles (#2578)

M. Toussaint1, T. Carlier1, 2, S. Stute1, 2

1 Nantes Université, Laboratoire CRCI2NA, INSERM, CNRS, Nantes, France
2 Nantes University Hospital, Nuclear Medicine Department, Nantes, France

Abstract

Correction of random coincidences is required in clinical PET imaging. Several methods have been proposed to estimate their distributions in a PET acquisition and they mostly use singles detection and/or a delayed coincidence window (DCW). We propose a new approach to achieve this task, which uses the differences in arrival times between consecutive single events that are greater than the coincidence window. This approach is thus less susceptible to bias induced by true coincidences and has more statistics than a DCW. As a proof of concept, a first implementation of this approach was compared to the classic methods using simulations from a small-sized PET scanner. The acquisition of four phantoms, each with different challenges in terms of randoms estimation, were simulated over a range of activities. Overall, the proposed method was less biased than the classical methods while also being more precise than DCW.

AcknowledgmentThis work has been funded by the French INCA-DGOS-INSERM/ITMO Cancer 18011 (SIRIC ILIAD).
References
[1] T. Carlier et al., “Assessment of acquisition protocols for routine imaging of Y-90 using PET/CT,” EJNMMI research, vol. 3, no. 1, p. 11, 2013
[2] S. R. Cherry et al., Physics in nuclear medicine. Saunders, 2003, vol. 3.
[3] M. Conti, “Effect of randoms on signal-to-noise-ratio in tof pet,” in IEEENuclear Science Symposium Conference Record, 2005, vol. 3.IEEE, 2005,pp. 6–pp.
[4] J. F. Oliver et al., “Improving the singles rate method for modeling accidentalcoincidences in high-resolution pet,” Physics in Medicine & Biology, vol. 55,no. 22, pp. 6951–6971, 2010.
[5] J. F. Oliver et al., “Modelling random coincidences in positron emission tomography byusing singles and prompts: a comparison study,” PloS one, vol. 11, no. 9, p.e0162096, 201
[6] D. Sarrut et al., “The opengate ecosystem for monte carlo simulation inmedical physics,” PMB, vol. 67, no. 18, p. 184001, sep 2022.
[7] C. C. Watson, “A hybrid algorithm for randoms variance reduction,” in 2009IEEE Nuclear Science Symposium Conference Record (NSS/MIC). IEEE,2009, pp. 3882–3885.
Keywords: Positron emission tomography (PET), Randoms correction, Monte-Carlo simulation, Delay window, Singles rate
16:00 MIC-04-05

Quantitative Activities Evaluation of Ac-225 and Daughter Nuclides Using the Alpha-SPECT Mini System (#3094)

W. Zhao1, X. Luo1, L.-J. Meng2, Y. Du1

1 Johns Hopkins University School of Medicine, Baltimore, Maryland, United States of America
2 University of Illinois at Urbana and Champaign , Champaign Il, Champaign, Illinois, United States of America

Abstract

The Alpha-SPECT Mini system integrates SPECT imaging with CT-based attenuation correction, providing a platform for quantifying in vivo distributions of alpha-emitting radiopharmaceuticals and daughter radionuclides. In this study, three Ac-225 filled syringes with different volumes, 0.5, 4.2, and 18.0 mL, respectively, were scanned with Alpha-SPECT Mini. The ground truth activities were[YD1] 26.12 µCi, 21.62 µCi, and 18.80 µCi from the smallest to the largest syringe, respectively. SPECT listmode acquisition was performed for 20 minutes for each syringe, together with an 80 kV CT scan for attenuation correction. SPECT images were reconstructed for the following photopeaks: 100 keV for Ac-225, 218 keV for Fr-221, 440 keV for Bi-213, and 117 keV for Tl-209. Activities of Ac-225 and these daughter radionuclides, were then estimated from SPECT images using CT defined ROIs and compared with ground truth.

The results showed that quantification accuracy varied with the radionuclides and syringe sizes. Fr-221 and Bi-213 showed relatively lower errors (<5%), while Ac-225 and Tl-209 exhibited larger deviations. The higher errors likely due to the low abundance of low energy (100 keV for Ac-225 and 117 keV for Tl-209) photopeaks and interference from downscatter and collimator penetration from high energy photons. Tl-209 also exhibited larger deviations with a size-dependent trend, suggesting sensitivity to source geometry and scatter correction. Overall, the Alpha-SPECT Mini system showed potential for quantitative imaging of Ac-225 and daughter radionuclides. Future work includes further calibration and implementation of scatter correction.

AcknowledgmentThis research was funded by National Institutes of Health, grant number S10OD038221. The content is solely the responsibility of the authors and does not necessarily represent the official views of the National Institutes of Health.
Keywords: SPECT, Ac-225, Daughter nuclides, Activity quantification, Quantitative imaging
16:15 MIC-04-06

Physics-Driven Methods for Standardizing Radiomics Features in CT Data (#2771)

H. Din1, Y. Yuan2, G. H. Kim3, M. F. McNitt-Gray3, J. W. Stayman2, G. J. Gang1

1 University of Pennsylvania, Radiology, Philadelphia, Pennsylvania, United States of America
2 Johns Hopkins University, Biomedical Engineering, Baltimore, Maryland, United States of America
3 University of California, Los Angeles, Radiology, Los Angeles, California, United States of America

Abstract

Radiomics have demonstrated potential in numerous clinical applications. However, feature variability resulting from different scanner hardware and image processing degrades predictive ability and reduces model generalizability. We present a novel physics-driven framework for radiomics standardization. Assuming a linear, shift-invariant image formation model, we developed an analytical method to remove the dependency of radiomics features classes on known spatial resolution and noise properties. The method consists of two deconvolution operations: deconvolving the system blur from the reconstructed image, then deconvolving the noise probability density function from radiomics feature distributions. This approach is applicable to multiple feature classes. We further developed a workflow to implement this framework on a clinical CT scanner. The method was evaluated on an anthropomorphic lung phantom imaged at five dose levels and reconstructed using eight kernels. Results demonstrate that the standardization method effectively improves the consistency of radiomics features value with those at reference imaging conditions. As expected, standardizing from smoother kernels to sharp kernels is more challenging than the reverse. The proposed standardization method is a promising tool for improving the robustness and generalizability of radiomics models.

AcknowledgmentThis work was supported, in part, by the NIH Grant R01EB031592.
References
[1] D. Mackin, X. Fave, L. Zhang, J. Yang, A. K. Jones, C. S. Ng and L. Court, "Harmonizing the pixel size in retrospective computed tomography radiomics studies," PLoS One, vol. 13, no. 1, 2017.
[2] Mackin D, Ger R, Gay S, Dodge C, Zhang L, Yang J and Jones AK 2019. Matching and homogenizing convolution kernels for quantitative studies in computed tomography Investigative Radiol. 54 288–95
[3] H. Um, F. Tixier, D. Bermudez, J. O. Deasy, R. J. Young and H. Veeraraghavan, "Impact of image preprocessing on the scanner dependence of multi-parametric MRI radiomic features and covariate shift in multi-institutional glioblastoma datasets," Phys. med. Biol., vol. 64, 2019.
[4] W. E. Johnson, C. Li and A. Rabinovic, "Adjusting batch effects in microarray expression data using empirical Bayes," Biostatistics, vol. 8, no. 1, pp. 118-127, 2007.
[5] G. J. Gang, R. Deshpande and J. W. Stayman, "Standardization of histogram- and gray-level co-occurrence matrices-based radiomics in the presence of blur and noise," Phys Med Biol., 2021.
[6] G. J. Gang, W. Zbijewski, J. W. Stayman and J. H. Siewerdsen, "Cascaded systems analysis of noise and detectability in dual-energy cone-beam CT," Med. Phys, vol. 39, no. 8, pp. 5145-5156, 2012.
Keywords: radiomics, hardmonization, calibration
16:30 MIC-04-07

Uncertainty estimation for 123I-DaTSCAN (#2802)

K. M. Ferreira1, 3, A. P. Robinson3, K. M. Bradley1, 4, D. R. McGowan1, 2

1 Oxford University Hospitals NHS Foundation Trust, Department of Medical Physics and Clinical Engineering, Oxford, United Kingdom
2 National Physical Laboratory (NPL), Teddington, United Kingdom
3 University of Oxford, Department of Oncology, Oxford, United Kingdom
4 University Hospital of Wales, Wales Research and Diagnostic Positron Emission Tomography Imaging Centre (PETIC), Wales, United Kingdom

Abstract

123I-DaTSCAN is used to aid diagnosis of Parkinsonism. Visual analysis of 123I-DaTSCAN is used in conjunction with patient clinical history and semi-quantification. Specific Binding Ratios (SBR) are commonly estimated for the right and left putamen and caudate using commercially available software. The estimation of uncertainties is not common for this clinical study; however, the benefits of estimating uncertainties have been recognised for other clinical applications. In this work, a method to evaluate the uncertainty associated with SBR is developed using phantom data and then applied to estimate uncertainties for imaging data from a cohort of patients. List mode data was acquired and bootstrapped to create equivalent sinograms. The sinograms were reconstructed and processed using BRASS software to obtain the distribution of SBR and respective standard deviations were estimated. The impact of estimating uncertainties in patient classification is also considered.
For the patient data, the estimated standard uncertainties varied between 2.8 % and 19 %. The correlation of SBR uncertainty with patient classification within the cohort is presented. Initial analysis suggests the patient classification does not change when considering uncertainty, but does provide confidence in the results. 
This is the first time that uncertainties on SBR values are used to evaluate impact on patient classification. Future work will include analysing additional patient data to further investigate the impact of uncertainties in patient classification. Analysis to understand if the uncertainties can be reduced is also planned.

Acknowledgment

The National Physical Laboratory is operated by NPL Management Ltd, a wholly owned company of the UK Department for Science, Innovation and Technology (DSIT).

References
[1] JCGM, “Evaluation of measurement data-guide to the expression of uncertainty in measurement évaluation des données de mesure-guide pour l’expression de l’incertitude de mesure,” Tech. Rep., 2008. [Online]. Available: www.bipm.org.
[2] A. Possolo, “Simple guide for evaluating and expressing the uncertainty of NIST measurement results NIST technical note 1900,” National Institute of Standards and Technology, vol. 1297, pp. 1–20, 2015. [Online]. Available: http://dx.doi.org/10.6028/NIST.TN.1900.
[3] L. Mari et al. “Measurement fundamentals: A pragmatic view,” IEEE Transactions on Instrumentation and Measurement, vol. 61, pp. 2107–2115,
2012.
[4] S. Morbelli et al. “EANM practice guideline/SNMMI procedure standard for dopaminergic imaging in parkinsonian syndromes 1.0,” European Journal of Nuclear Medicine and Molecular Imaging, vol. 47, pp. 1885–1912, 2020.
[5] I. Buvat, “A non-parametric bootstrap approach for analysing the statistical properties of SPECT and PET images,” Physics in Medicine and Biology, vol. 47, pp. 1761–1775, 2002.
Keywords: 123I-DaTSCAN, SPECT/CT, Uncertainty
16:45 MIC-04-08

Towards Absolute Resolution Characterization in OSEM Reconstructed Images without Ground Truth: Using FBP Reconstructed Images as the Bridge (#2809)

Y. Hu1, L. Guo2, T. Mulnix1, T. Marin1, R. E. Carson1, 2

1 Yale University, Department of Radiology and Biomedical Imaging, New Haven, Connecticut, United States of America
2 Yale University, Department of Biomedical Engineering, New Haven, United States of America

Abstract

Absolute resolution characterization of OSEM-reconstructed images is challenging because the OSEM algorithm is nonlinear and its resolution strongly depends on the activity distribution and the number of iterations. In contrast, the linear FBP algorithm provides a more consistent resolution, albeit with higher noise. In this work, we propose using FBP-reconstructed images as a bridge to estimate the absolute resolution of OSEM images without requiring ground truth. Two FBP-bridge approaches are investigated: an image-domain Gaussian fitting method and a frequency-domain modulation transfer function (MTF) ratio method. Hoffman phantom experimental results show that the Gaussian fitting approach has better agreement with the reference FWHM obtained using the known phantom ground truth. Both methods are further applied to human brain PET scans. This method also allows pixel-wise visualization of spatially variant image resolution. Future work will investigate the effects of noise and FBP filter selection.

Keywords: OSEM, FBP, resolution characterization, Gaussian fitting, modulation transfer function


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