A scale space theory based motion correction approach for dynamic PET brain imaging studies

被引:1
|
作者
Gutschmayer, Sebastian [1 ]
Muzik, Otto [2 ]
Chalampalakis, Zacharias [3 ]
Ferrara, Daria [1 ]
Yu, Josef [1 ]
Kluge, Killian [4 ]
Rausch, Ivo [1 ]
Boellaard, Ronald [5 ]
Golla, Sandeep S. V. [5 ]
Zuehlsdorff, Sven [6 ]
Newiger, Hartwig [7 ]
Beyer, Thomas [1 ]
Kumar Shiyam Sundar, Lalith [1 ]
机构
[1] Med Univ Vienna, QIMP Team, Vienna, Austria
[2] Wayne State Univ, Dept Pediat, Detroit, MI 48202 USA
[3] Univ Paris Saclay, Serv Hos Frederic Joliot, Lab Imagerie Biomed Multimodale BioMaps, CEA,CNRS,Inserm, Orsay, France
[4] Med Univ Vienna, Dept Biomed Imaging & Image Guided Therapy, Div Nucl Med, Vienna, Austria
[5] Amsterdam UMC Locat Vrije Univ Amsterdam, Dept Radiol & Nucl Med, Amsterdam, Netherlands
[6] Siemens Med Solut USA Inc, Hoffman Estates, IL USA
[7] Siemens Healthineers, Erlangen, Germany
来源
FRONTIERS IN PHYSICS | 2022年 / 10卷
基金
奥地利科学基金会;
关键词
brain motion correction; scale-space; dynamic PET imaging; frame-based algorithm; gaussian pyramid algorithms; POSITRON-EMISSION-TOMOGRAPHY; HEAD MOTION; DESIGN;
D O I
10.3389/fphy.2022.1034783
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Aim/Introduction: Patient head motion poses a significant challenge when performing dynamic PET brain studies. In response, we developed a fast, robust, easily implementable and tracer-independent brain motion correction technique that facilitates accurate alignment of dynamic PET images.Materials and methods: Correction of head motion was performed using motion vectors derived by the application of Gaussian scale-space theory. A multiscale pyramid consisting of three different resolution levels (1/4x: coarse, 1/2x: medium, and 1x: fine) was applied to all image frames (37 frames, framing of 12 x 10s, 15 x 30s, 10 x 300s) of the dynamic PET sequence. Frame image alignment was initially performed at the coarse scale, which was subsequently used to initialise coregistration at the next finer scale, a process repeated until the finest possible scale, that is, the original resolution was reached. In addition, as tracer distribution changes during the dynamic frame sequence, a mutual information (MI) score was used to identify the starting frame for motion correction that is characterised by a sufficiently similar tracer distribution with the reference (last) frame. Validation of the approach was performed based on a simulated F18-fluoro-deoxy-glucose (FDG) dynamic sequence synthesised from the digital Zubal phantom. Inter-frame motion was added to each dynamic frame (except the reference frame). Total brain voxel displacement based on the added motion was constrained to 25 mm, which included both translation (0-15 mm in x, y and z) and rotation (0-0.3 rad for each Euler angle). Twenty repetitions were performed for each dataset with arbitrarily simulated motion, resulting in 20 synthetic datasets, each consisting of 36 dynamic frames (frame 37 was the reference frame). Assessment of motion correction accuracy across the dynamic sequence was performed based on the uncorrected/residual displacement remaining after the application of our algorithm. To investigate the clinical utility of the developed algorithm, three clinically cases that underwent list-mode PET imaging utilising different tracers ([18F]-fluoro-deoxy-glucose [18F]FDG [18F]-fluoroethyl-l-tyrosine [18F]FET [11C]-alpha-methyl-tryptophan [11C]AMT), each characterised by a different temporal tracer distribution were included in this study. Improvements in the Dice score coefficient (DSC) following frame alignment were evaluated as the correlation significance between the identified displacement for each frame of the clinical FDG, FET and AMT dynamic sequences.Results: Sub-millimetre accuracy (0.4 & PLUSMN; 0.2 mm) was achieved in the Zubal phantom for all frames after 5 min p. i., with early frames (30 s-180 s) displaying a higher residual displacement of & SIM;3 mm (3.2 & PLUSMN; 0.6 mm) due to differences in tracer distribution relative to the reference frame. The effect of these differences was also seen in MI scores; the MI plateau phase was reached at 35s p. i., 2.0 and 2.5 min p. i. At the coarse, medium and fine resolution levels, respectively. For the clinical images, a significant correlation between the identified (and corrected) displacement and the improvement in DSC score was seen in all dynamic studies (FET: R = 0.49, p < 0.001; FDG: R = 0.82, p < 0.001; AMT: R = 0.92, p < 0.001). Conclusion: The developed motion correction method is insensitive to any specific tracer distribution pattern, thus enabling improved correction of motion artefacts in a variety of clinical applications of extended PET imaging of the brain without the need for fiducial markers.
引用
收藏
页数:13
相关论文
共 50 条
  • [1] Motion correction in PET brain studies
    Herzog, H
    Tellman, L
    Fulton, R
    Pietrzyk, U
    [J]. FOURTH INTERNATIONAL WORKSHOP ON MULTIDIMENSIONAL SYSTEMS - NDS 2005, 2005, : 178 - 181
  • [2] Motion correction in dynamic PET/CT imaging
    Feeley, Christina
    Moore, Stephen
    Pande, Reena
    Park, Mi-Ae
    [J]. JOURNAL OF NUCLEAR MEDICINE, 2009, 50
  • [3] Accuracy of motion correction methods for PET brain imaging
    Fulton, R
    Tellmann, L
    Pietrzyk, U
    Winz, O
    Stangier, I
    Nickel, I
    Schmid, A
    Meikle, S
    Herzog, H
    [J]. 2004 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOLS 1-7, 2004, : 4226 - 4230
  • [4] Rigid motion correction of PET and CT for PET/CT brain imaging
    Bickell, Matthew
    Kim, Jung-Ha
    Rezaei, Ahmadreza
    Nuyts, Johan
    Fulton, Roger
    [J]. 2015 IEEE NUCLEAR SCIENCE SYMPOSIUM AND MEDICAL IMAGING CONFERENCE (NSS/MIC), 2015,
  • [5] Tracer kinetics driven motion correction in dynamic PET imaging
    Sun, Tao
    Wang, Ying
    Hu, Zhanli
    Li, Chenwei
    Yang, Yongfeng
    [J]. JOURNAL OF NUCLEAR MEDICINE, 2021, 62
  • [6] An adaptive motion correction method for PET/CT Brain Imaging
    Wang, Man
    Su, Yusheng
    Lu, Jie
    Liang, Zhigang
    Yang, Defu
    Lv, Yang
    Dong, Yun
    Chen, Mu
    An, Lin
    [J]. JOURNAL OF NUCLEAR MEDICINE, 2016, 57
  • [7] A volumetric approach to motion correction in dynamic N-13 ammonia PET cardiac imaging
    Nekolla, SG
    Schonauer, M
    Munz, F
    Ziegler, SI
    Schwaiger, M
    [J]. JOURNAL OF NUCLEAR MEDICINE, 1996, 37 (05) : 513 - 513
  • [8] Comparison of MR Based Attenuation Correction Methods with CT Based Attenuation Correction in Dynamic Brain PET imaging
    Firouzian, A.
    Delso, G.
    Hallett, W.
    [J]. EUROPEAN JOURNAL OF NUCLEAR MEDICINE AND MOLECULAR IMAGING, 2018, 45 : S695 - S696
  • [9] CT Based Attenuation Correction for PET Brain Imaging
    Lokitz, Stephen J.
    Coleman, R. Edward
    Yoshizumi, Terry T.
    Toncheva, Greta I.
    Daigle, Lauren T.
    Colsher, James G.
    Turkington, Timothy G.
    [J]. 2006 IEEE NUCLEAR SCIENCE SYMPOSIUM CONFERENCE RECORD, VOL 1-6, 2006, : 3320 - 3325
  • [10] Development of a Novel Respiring Phantom for Motion Correction Studies in PET Imaging
    Scott-Jackson, W.
    McQuaid, S.
    Wells, K.
    Scuffham, J.
    Lewis, E.
    [J]. MEDICAL IMAGING 2018: PHYSICS OF MEDICAL IMAGING, 2018, 10573