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Accuracy and precision of zero-echo-time, single- and multi-atlas attenuation correction for dynamic [11C]PE2I PET-MR brain imaging

EJNMMI Physics volume 7, Article number: 77 (2020) Cite this article

Abstract

Background

A valid photon attenuation correction (AC) method is instrumental for obtaining quantitatively correct PET images. Integrated PET/MR systems provide no direct information on attenuation, and novel methods for MR-based AC (MRAC) are still under investigation. Evaluations of various AC methods have mainly focused on static brain PET acquisitions. In this study, we determined the validity of three MRAC methods in a dynamic PET/MR study of the brain.

Methods

Nine participants underwent dynamic brain PET/MR scanning using the dopamine transporter radioligand [11C]PE2I. Three MRAC methods were evaluated: single-atlas (Atlas), multi-atlas (MaxProb) and zero-echo-time (ZTE). The 68Ge-transmission data from a previous stand-alone PET scan was used as reference method. Parametric relative delivery (R1) images and binding potential (BPND) maps were generated using cerebellar grey matter as reference region. Evaluation was based on bias in MRAC maps, accuracy and precision of [11C]PE2I BPND and R1 estimates, and [11C]PE2I time-activity curves. BPND was examined for striatal regions and R1 in clusters of regions across the brain.

Results

For BPND, ZTE-MRAC showed the highest accuracy (bias < 2%) in striatal regions. Atlas-MRAC exhibited a significant bias in caudate nucleus (− 12%) while MaxProb-MRAC revealed a substantial, non-significant bias in the putamen (9%). R1 estimates had a marginal bias for all MRAC methods (− 1.0–3.2%). MaxProb-MRAC showed the largest intersubject variability for both R1 and BPND. Standardized uptake values (SUV) of striatal regions displayed the strongest average bias for ZTE-MRAC (~ 10%), although constant over time and with the smallest intersubject variability. Atlas-MRAC had highest variation in bias over time (+10 to − 10%), followed by MaxProb-MRAC (+5 to − 5%), but MaxProb showed the lowest mean bias. For the cerebellum, MaxProb-MRAC showed the highest variability while bias was constant over time for Atlas- and ZTE-MRAC.

Conclusions

Both Maxprob- and ZTE-MRAC performed better than Atlas-MRAC when using a 68Ge transmission scan as reference method. Overall, ZTE-MRAC showed the highest precision and accuracy in outcome parameters of dynamic [11C]PE2I PET analysis with use of kinetic modelling.

Introduction

In positron emission tomography (PET), photon attenuation correction (AC) is a prerequisite for obtaining dependable images and quantifications. Photon attenuation is the largest correction required in PET imaging as photon attenuation is inhomogeneous across tissues [1]. The amount of attenuation depends on spatially varying electron density. PET AC routines therefore require knowledge about the spatial distribution of attenuation coefficients within the field of view (FOV) of the scanner, represented as an attenuation map whose voxel values denote linear attenuation coefficients [2,3,4].

Stand-alone PET systems are most often equipped with rotating 68Ge/68Ga transmission sources [5, 6]. This method is usually regarded as the gold standard for AC [7] as it measures 511 keV photon attenuation directly, however not without some drawbacks like noise and poor resolution. In PET/computed tomography (CT) systems, AC is based on low-dose CT scanning [8], with CT images converted from Hounsfield units to linear attenuation coefficients at 511 keV to obtain a suitable AC map for PET correction [9].

Integrated PET/magnetic resonance imaging (MRI) systems offer new opportunities and challenges. Neurological disorders are key applications with a long clinical tradition of combining functional information from nuclear medicine images with structural information from magnetic resonance imaging (MRI) to allow adequate quantification across the brain. However, MRI provides no direct information on electron density that can be used for AC [10, 11]. Instead, MRI can supply proton density, but its correlation with gamma photon attenuation is highly nonlinear: the bone, in particular, has low proton density and high electron density [12, 13]. Additional efforts are needed to determine which AC method can be implemented as a routine in an image reconstruction process.

Several approaches have been reported for MR-based attenuation correction (MRAC) of PET brain data. Initially, a Dixon-based approach was implemented for PET MRAC. This method is based on segmentation into tissue classes (i.e. air, lung, fat and soft tissue) to which fixed attenuation coefficients are assigned [14,15,16]. As the Dixon-based approach is primarily intended for whole-body PET-MR, the skull is not considered. As a consequence, this MRAC method is a source of a substantial bias in brain studies, especially for cortical regions [17,18,19]. In parallel, various atlas-based MRAC approaches were developed and evaluated. In this broad class of methods, a single atlas [20, 21] or multiple atlases [22, 23] are applied to incorporate the bone in the MRAC map. As no direct relationship exists between MRI and CT [3], various statistical methods have been applied to convert MR intensities to a pseudo-CT with Hounsfield units for discrimination of soft tissue, air and bone [24]. Generally, atlas-based MRAC methods improve accuracy by including the skull and seem to perform within acceptable quantitative limits [11, 25]. Most recently, segmentation of a zero-echo-time (ZTE) MRI sequence [12, 26, 27] has been suggested for MRAC. With some resemblance to ultrashort echo time (UTE) [28] and more recently RESOLUTE [29], ZTE was designed to obtain signal from cortical bone with both lower acoustic noise and reduced sensitivity to gradient fidelity artefacts [26, 30, 31]. As such, ZTE could be used to incorporate the bone in a MRAC map [10, 12, 26]. Several clinical evaluations demonstrated for static PET-data acquisitions that ZTE-based MRAC accomplished quantification with smaller errors than a single-atlas approach, both with CT-AC [10, 32,33,34,35,36,37] or 68Ge-AC as reference [38]. Another rapidly emerging field is the use of neural-networks to incorporate the bone in MRAC [39,40,41,42] but these approaches are not considered here.

Until now, evaluations of various MRAC methods have mainly focused on static brain PET, showing merely the tracer uptake or target-to-reference ratios. In an independent multi-centre study where eleven MRAC methods were applied to a large cohort data set of static fluorodeoxyglucose (FDG) PET/MR data, the average performance in PET tracer uptake was generally within ± 5% of CT-AC [25]. However, dynamic brain PET holds the compelling promise of in vivo functional imaging, i.e. following physiological processes over time, or obtaining quantitative measures by means of tracer kinetic modelling. Several recent studies have reported results for dynamic PET data using two scanners, MRAC methods and radiotracers as well as different kinetic modelling approaches depending on the tracer kinetics [43,44,45,46]. To date, no study has compared the multi-atlas method maximum probability algorithm (MaxProb) [43], favoured by Ladefoged et al. [25], the single-atlas method and ZTE using the gold standard 68Ge-AC as a reference, in a dynamic setting. MaxProb-MRAC builds on a database of brain MR/CT image pairs and an application of a novel maximum probability method. In a dynamic setting with the serotonergic 1a tracer [18F]MPPF, an acceptable amount of bias in the estimated binding potential (BPND) was seen using CT-AC as reference.

In this study, we used 11C-labelled PE2I (N-(3-iodoprop-2E-enyl)-2β-carbomethoxy-3β-(4-methyl-phenyl) nortropane), a radiotracer with high affinity to dopamine transporters (DAT), especially in the striatum [47]. Kinetic modelling of dynamic [11C]PE2I imaging data is able to determine both BPND, proportional to DAT availability, and relative delivery (R1) reflecting relative cerebral blood flow, from one single brain scan [48, 49]. These quantitative outcome measures are particularly important for the differential diagnosis in patients with Parkinsonism [50] and used in clinical routine at our centre. Despite the promising evaluation reports of novel MRAC methods, it is still unclear how these approaches might perform in a dynamic dataset with a specific dopamine tracer and use of a kinetic modelling approach.

The aim of this study was to determine the validity of three different MRAC methods in a setting with a dynamic [11C]PE2I PET brain scan on a PET-MR system, using 68Ge-transmission AC as a reference method. We evaluated (1) a single-atlas method (Atlas-MRAC) [11], (2) an MR sequence-based method (ZTE-MRAC) [12, 26, 27] and (3) a multiple-atlas method (MaxProb-MRAC) [43, 51] in a dynamic [11C]PE2I PET dataset acquired on an integrated digital time-of-flight PET-MR system. Individual transmission scans acquired on a stand-alone PET system were used as the reference method (68Ge-MRAC), directly measuring attenuation at 511 keV.

Methods

Participants and data acquisition

The participants and data acquisition have previously been described [38]. This study was approved by the Regional Board of Medical Ethics in Uppsala as well as the Radiation Ethics Committee of Uppsala University Hospital, and all participants consented in writing to take part in the study before inclusion. The study comprised nine patients with Parkinsonism (5 females, 4 males; median age 72 years, range 49–82). Previously, each participant had undergone a 10-min transmission scan using three rotating 68Ge rod sources on an ECAT Exact HR+ scanner (Siemens, Knoxville, USA), prior to injection of any radioactivity. Participants then underwent a dynamic brain PET scan using 11C-PE2I on a 3-T time-of-flight (TOF) PET/MR (SIGNA PET/MR, GE Healthcare, Waukesha, USA) system.

An 80-min PET scan was acquired in list mode, starting simultaneously with intravenous bolus administration of 5 MBq/kg [11C]PE2I using an infusion pump, and divided into 22 time frames of increasing duration (4 × 60s, 2 × 120 s, 4 × 180 s, 12 × 300 s). Relevant MR sequences were acquired during the first five minutes of the [11C]PE2I PET scan to avoid misalignment due to head movements. Three MR sequences were acquired during the [11C]PE2I PET scan: (1) a T1w 3D LAVA Flex that was later used for Atlas-MRAC (duration 18 s, 1 number of excitations (NEX), FOV 500 mm, slice thickness 5.2 mm, overlap 2.6 mm, matrix 256 × 256 and 5° flip angle); (2) a proton-density ZTE sequence (duration 153 s, 4 NEX, FOV 260 mm, slice thickness 1.4 mm, no slice gap, matrix 192 × 192, flip angle 0.8°); and (3) a 3D T1w brain volume imaging sequence that was later used for definition of regions of interest and as the target for MaxProb-MRAC registration (gradient-echo, duration 272 s, 1 NEX, FOV 250 mm, slice thickness 1 mm, matrix 256 × 256, flip angle 12°, TI 450 ms).

Generation of MR attenuation correction maps

For each participant, the following MR attenuation correction maps (MRAC) were produced:

Atlas-MRAC—The single-atlas-based method [11, 20] consisted of three steps: (1) application of a Hessian matrix to enhance bone structures in the T1w image, (2) pseudo-CT generation by registration of the enhanced image to a head atlas based on CT scans of 50 participants, and (3) standard energy conversion and resampling of the pseudo-CT, resulting in an AC map with dimensions of 128 × 128 × 89 voxels (4.68 × 4.68 × 2.78 mm). This method was vendor-provided (software version MP26) as a standard application for our PET/MR system when the study was initiated.

ZTE-MRAC—In this procedure, an intensity equalization to a ZTE image was followed by logarithmic image rescaling to enhance bone tissue. Next, a mask was used to isolate the brain data, thus removing bed and coil information. A sequence of thresholding operations was then applied to the subject’s brain image to segment the bone and air regions by fitting a Gaussian to the main image histogram peaks. Remaining internal air compartments were further segmented by means of histogram thresholding. ZTE bone voxels are assigned continuous attenuation coefficients using a ZTE-intensity HU calibration curve as described in [10, 12, 26, 33]. Finally, the resulting MRAC image was co-registered and resampled to the subjects’ individual Atlas-MRAC by applying 6-parameter rigid-body registration creating the ZTE-MRAC map. This method is also a vendor-implemented process (GE PET Reconstruction Toolbox MP26), but during data acquisition still under development [12, 26, 27].

MaxProb-MRAC—This method utilized a database of 40 corresponding MR and CT images [43, 51]. Processing steps were executed using an in-house MATLAB pipeline (MATLAB R2017a, Mathworks Inc., Natick, MA, USA). Each MR image from the database was paired with the participant’s high-resolution T1w image, and masking was applied to both images to reduce extraneous image information. In the following registration steps, the masked MR image pair was aligned by means of affine registration followed by non-rigid registration using normalized mutual information as the similarity measure (register github.com/BioMedIA/MIRTK). Subsequently, the transformation matrices acquired from the non-rigid registration of MR images were applied to the corresponding CT images, yielding a database of co-registered MR/CT image pairs. In the next step, the co-registered CTs were segmented into three tissue classes defined by intensity thresholds (air: < − 500 HU, soft tissue: − 500–300 HU, bone: > 300 HU [20]. Each voxel tissue class of the target subject space was then assigned to a tissue class by majority voting of tissue class labels across the registered CT database. Finally, a voxel-wise pseudo-CT was generated by averaging CT Hounsfield values of atlases belonging to the majority class for the corresponding voxel. A bilinear energy conversion [52] was performed as the last step of attenuation map computation. The resulting MRAC image was rigidly co-registered and resampled to the participant’s individual Atlas-MRAC. Thereafter, the MaxProb-MRAC image was completed by adding, from the Atlas-MRAC map, the neck information missing due to differences in axial FOV between the images retrieved from the MR/CT database (216 mm) and the PET/MR scanner (250 mm).

68Ge-AC—Attenuation maps were reconstructed from the 68Ge transmission scan using ordered subset expectation maximisation (OSEM) with 6 iterations, 8 subsets and a 4 mm Hanning post-filter, dimensions 128 × 128 × 63 voxels (5.15 × 5.15 × 2.43 mm). Thereafter, a mask was applied to strip the AC map from the bed and head support as well as noise surrounding the head, followed by rigid co-registration and resampling to the participant’s individual Atlas-MRAC map. As the axial FOV differed between the stand-alone PET (155 mm) and PET/MR scanner (250 mm), the 68Ge-AC map was completed with the corresponding information concerning the neck and top of the head from the Atlas-MRAC map.

As a common step for all generated MRAC maps, coil and bed AC map templates were then incorporated, applying an in-house MATLAB pipeline (MATLAB R2017a, Mathworks Inc., Natick, MA, USA).

Image reconstruction

The dynamic [11C]PE2I PET data were reconstructed using time-of-flight OSEM with 2 iterations, 28 subsets, 5 mm Gaussian post-filter, 128 × 128 reconstruction matrix and 300 mm FOV. MRAC was performed in four ways as described in the previous section. Further, all appropriate corrections for quantitative image reconstruction were applied.

[11C]PE2I image analysis

The methodology and validation for voxel-level analysis of dynamic [11C]PE2I scans have been previously reported [48, 49].

Following this approach, the reconstructed [11C]PE2I PET images were realigned to correct for interframe patient movements using an early (0–3 min) [11C]PE2I summed image as reference using an in-house MATLAB 2018 script. Interframe motion was estimated in this way for the PET images corrected for AC using 68Ge-AC, and the same transformation were applied to the other three dynamic data sets. Subsequently, the same summed image was used for co-registration of the 3D T1w MRI scan based on a 6-parameter rigid transformation, to achieve positional alignment. Then, MR images were segmented into grey matter, white matter, and cerebrospinal fluid using Statistical Parametric Mapping (SPM12; Wellcome Trust Center for Neuroimaging, University College London, UK). Grey matter volumes of interest (VOI) were established on the T1w structural MR images using an automated probabilistic template as implemented in the PVElab software [53] for cortical and limbic regions. For striatal regions, MAPER [54], a technique optimized for segmentation of atrophic brains, was used to achieve a more accurate delineation. All VOIs were projected over the dynamic scans to generate time-activity curves (TACs).

Parametric images were generated from the [11C]PE2I scan using receptor parametric mapping (RPM) with cerebellar grey matter as a reference region [55]. RPM is an implementation of the simplified reference tissue model, SRTM [56], with a set of predefined basis functions to linearize the model and estimate voxel-wise R1 and BPND that can be applied to [11C]PE2I. The parametric [11C]PE2I BPND images demonstrate specific binding of [11C]PE2I to DAT directly proportional to DAT density (availability) and therefore mainly show the deep grey matter of the striatum. The parametric [11C]PE2I R1 images display relative cerebral blood flow, which reveals overall brain functional activity. This procedure was repeated for all four [11C]PE2I PET data sets. Finally, the grey matter VOIs on the co-registered MR images were projected on the various parametric [11C]PE2I R1 and BPND images from all four datasets.

Volumes of interest

Quantification of BPND was evaluated separately for the caudate nucleus and putamen as well as for the whole dorsal striatum (volume-weighted average of the putamen and caudate). These regions normally have high DAT availability, but a pronounced reduction is often observed in persons with Parkinsonism [49].

Evaluation of the quantification of R1 was based on four clusters of VOIs across the brain: anterior cortical regions (cingulate, frontal gyrus), posterior cortical regions (occipital cortex, parietal cortex, somatosensory-motor cortex), dorsal striatal regions (caudate nucleus, putamen) and limbic regions (amygdala, hippocampus, hypothalamus, thalamus) [49]. In addition, whole-brain grey matter (WB) was determined as an overall measure.

Evaluation of MRAC maps

All participants’ MRAC maps were converted to MNI space using SPM12. Mean MRAC images for all four methods were calculated, and bias compared to 68Ge-AC was calculated at the voxel level as follows:

$$ {Bias}_i={MRAC}_i-{}^{68} GeAC $$
(1)

where i refers to the three MRAC methods being compared to 68Ge-AC.

Attenuation maps were assessed on soft tissue and bone compartments. A large VOI was drawn over the 68Ge-AC map soft tissue and copied to the other AC methods. A bone mask was created by simple segmentation of the ZTE map followed by 2-pixel erosion to reduce the probability of coinciding with other tissues. The bone mask was then transferred to all other AC methods. Mean bias values were calculated for both soft tissue and bone.

Evaluation of [11C]PE2I BPND and R1 estimates

[11C]PE2I BPND and R1 images for each subject were converted to MNI space using SPM12. Mean [11C]PE2I BPND and R1 images for all four methods were calculated, and bias (Eq. 1) compared to 68Ge was calculated at the voxel level for the defined VOIs.

For quantitative assessment, we used relative differences (% bias; see Eq. 2) in BPND and R1 as a measure of accuracy, while standard deviation of the bias was taken as a measure of precision.

$$ {Bias}_i\left(\%\right)=\frac{PET_{MRAC_i}-{PET}_{68 Ge- AC}}{PET_{68 Ge- AC}}\times 100\kern0.75em $$
(2)

with i referring to the three evaluated MRAC methods.

Correlation analysis (Spearman) and Deming regression were used to assess the degree of agreement between BPND and R1 values obtained using each of the evaluated MRAC methods and the reference method (68Ge-AC).

Statistical analysis was performed using GraphPad Prism 6 (GraphPad Software, La Jolla, CA, USA). Significant differences in bias (p < 0.05) between each evaluated MRAC method and 68Ge-AC as reference method were assessed using a Friedman test with post-hoc tests (comparison to 68Ge-AC) and Dunn’s correction.

Evaluation of time-activity curves

Previous reports indicate that effects of attenuation correction on uptake over time can be inhomogeneous [29, 43, 44, 57] and may potentially affect the accuracy and precision of the parameters estimated by kinetic modelling. We therefore examined relative bias and its SD in [11C]PE2I standardized uptake values (SUV) over time. This was done for striatal regions with a high DAT density and the reference region (cerebellum) used after implementation of Atlas-, ZTE- and MaxProb-MRAC.

Results

MRAC maps

The MRAC maps for 68Ge, Atlas, ZTE and MaxProb of a representative subject are presented in Fig. 1. Each MRAC map exhibited distinct qualitative features mainly inherent to how the maps were generated. The 68Ge-AC map displayed images with heterogeneous signal in the soft tissue due to noise as a result of low-count statistics. The ZTE-MRAC map based on MRI methodology had the highest resolution, although the sinus regions are not well defined. The Atlas- and MaxProb-MRAC maps were qualitatively similar. Furthermore, 68Ge and MaxProb-MRAC maps were completed with Atlas-based information.

Fig. 1
figure 1

Typical MRAC maps-based on 68Ge, Atlas, ZTE and MaxProb approaches. Neck completion was required for 68Ge-AC and MaxProb-MRAC and was based on Atlas-MRAC

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Figure 2 shows the mean bias across all participants in brain attenuation maps for the evaluated MRAC methods. In brain soft tissue, the smallest mean bias was found for ZTE-MRAC (2.9 · 10−4 cm−1) and MaxProb-MRAC (3.0 · 10−4 cm−1) closely followed by Atlas-MRAC (3.3 · 10−4 cm−1). In the bone, Atlas-MRAC yielded the lowest mean bias (5.6 · 10−4 cm−1) compared with an approximately two times higher bias for MaxProb-MRAC (13 · 10−4 cm−1) and three times higher bias for ZTE-MRAC (18 · 10−4 cm−1). In the sinus region, an evident bias was detected in all maps where the highest overestimation was noticed for ZTE-MRAC.

Fig. 2
figure 2

Mean absolute and relative bias across participants in Atlas-, ZTE- and MaxProb-MRAC maps. Positive bias in red and negative in blue

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Binding potential

Mean parametric BPND images were similar for all MRAC methods (Fig. 3a). Mean bias images of BPND displayed an obvious negative bias in the striatum in case of Atlas-MRAC while these images pointed to a relatively small striatal bias for ZTE- and MaxProb-MRAC (Fig. 3b). Various bias patterns between MRAC methods were found for extrastriatal regions but this might also be due to low DAT density (see Fig. 3b).

Fig. 3
figure 3

a Mean BPND images using 68Ge- and Atlas-, ZTE- and MaxProb-MRAC showing striatal DAT density. b Mean bias images of BPND illustrating voxel-wise differences in BPND between each MRAC method and 68Ge-MRAC

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The relative bias of the striatal BPND estimates is presented in Fig. 4a. Atlas-MRAC resulted in a substantial negative relative bias for the caudate and the entire striatum, but only a small bias for the putamen. For ZTE, a minor relative bias in BPND with a low variability was observed for the putamen and striatum, whereas a greater variability between participants was noted for the caudate. For all regions, MaxProb showed considerable variability with both positive and negative bias percentages. There was no obvious relationship between the magnitude of the reference values (BPND based on 68Ge-AC) and bias percentages.

Fig. 4
figure 4

a Relative differences in BPND (% bias) plots of BPND when comparing Atlas-, ZTE- or MaxProb-MRAC to 68Ge-AC (gold standard) for striatal brain regions. b Relationship between BPND using various MRAC methods and 68Ge-AC as reference, where solid lines represent Deming regressions and dashed line identity

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The Deming regression lines demonstrated a high degree of agreement for ZTE- and MaxProb-MRAC compared to the reference method in all brain regions (Fig. 4b). In contrast, the regression lines for Atlas-MRAC exhibited a deviation from the identity line, indicating a negative bias compared to the reference method.

Table 1 lists quantitative values related to accuracy (% bias) and precision (SD of % bias) for estimated BPND values as well as measures of consistency between evaluated and reference MRAC (correlations, regression parameters). ZTE-MRAC results showed little bias for all regions (< 2%) with a generally high precision. The highest bias was found for Atlas-MRAC in the caudate (approximately − 12%) which differed significantly from 68Ge-AC (p < 0.05). MaxProb also showed a relatively large mean bias in the putamen (about 9%) but did not deviate significantly from 68Ge-MRAC. MaxProb-MRAC showed the lowest precision in all regions. Only the bias obtained for the caudate with the Atlas approach was statistically significant.

Table 1 BPND–mean % bias and precision (SD of % bias) as well as correlation coefficient (r) for striatal regions when comparing Atlas-, ZTE- and MaxProb-MRAC against 68Ge-AC. Additionally, the slope and intercept of Deming regression lines are given
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In general, strong correlations with 68Ge-AC were established for all three evaluated MRAC- methods in all regions (r ≥ 0.95).

Estimated BPND values and relative bias for the evaluated MRAC methods are illustrated with boxplots in Fig. 5. The median BPND of the investigated brain regions differed only modestly within regions (Fig. 5a). The relative bias was low for ZTE-MRAC while MaxProb-MRAC showed the lowest precision indicated by the size of the boxes and bars (Fig. 5b).

Fig. 5
figure 5

Boxplots for estimated BPND (a) and % bias (b) in BPND when comparing Atlas-, ZTE- or MaxProb-MRAC to 68Ge-AC for the caudate (CN), putamen (PUT), and entire striatum (STR). Bars and whiskers represent median and first and third quartile. * p value < 0.05

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Relative delivery

Mean parametric R1 images, representing relative cerebral blood flow and overall brain activity, are presented in Fig. 6a and show similar patterns for all four MRAC methods. Mean bias images of R1 indicated mostly a positive bias throughout the brain regardless of the MRAC method used (Fig. 6b). Further, these images pointed to a distinct positive bias in the anterior part of the brain for Atlas-MRAC and especially MaxProb-MRAC. Negative bias was evident in the posterior part of the brain for Atlas-MRAC and to a lesser degree for ZTE.

Fig. 6
figure 6

a Mean parametric R1 images using 68Ge- and Atlas-, ZTE- and MaxProb-MRAC. b Mean bias images of R1 illustrating voxel-wise differences in R1 between each MRAC method and 68Ge-AC

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The relative bias of R1 estimates for various clusters of brain regions is displayed in Fig. 7a. Generally, the relative bias of R1 was within a range of −/+ 5%. However, for all brain clusters, the variability was greater for MaxProb-MRAC compared to the other MRAC methods. R1 estimates of WB had a small bias and variability for all MRAC methods. The individual regional R1 bias values were generally in the range of − 5 to 15%. Striatal R1 estimates contained mainly a positive bias, while the other regions contained both positive and negative % bias.

Fig. 7
figure 7

a Relative differences in R1 (% bias) plots of R1 when comparing Atlas-, ZTE- or MaxProb-MRAC to 68Ge-AC as gold standard for different clusters of brain regions. b Relationship between R1 values derived using various MRAC methods and 68Ge-AC as reference, where solid lines represent Deming regressions and dashed line identity

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Strong and similar relationships were found between the R1 estimates from the investigated MRAC methods and the reference method (Fig. 7b). All Deming regression lines were close to the line of identity, displaying a high degree of agreement.

The outcome of the evaluation of R1 estimates (accuracy, precision and degree of agreement) is given for various clusters of brain regions in Table 2. For all investigated MRAC methods, the mean bias percentages were low and within a range of − 1.0 to + 3.5%. A modest negative mean bias was found for posterior cortical regions using Atlas- or ZTE-MRAC, whereas all other mean bias values were positive. Based on the SD of the mean bias percentages, ZTE-MRAC showed the highest precision and MaxProb-MRAC the lowest precision, which was consistent for most clusters of brain regions. High correlations between the evaluated MRAC methods and the reference method were attained for all brain regions (0.92–1.00).

Table 2 R1 mean % bias, precision (SD of % bias) and correlation coefficient (r) for all clusters of brain regions when comparing Atlas-, ZTE- and MaxProb-MRAC against 68Ge-MRAC. Additionally, slope and intercept of Deming regression lines are given
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Boxplots for estimated R1 values and relative bias are given for all MRAC methods used in Fig. 8. Only minor differences in median and the variability of R1 estimates were found between the four MRAC methods within each brain cluster (Fig. 8a). Significant differences in relative bias were noted in the striatum for all three MRAC methods relative to 68Ge-MRAC, in anterior cortical regions for Atlas- and MaxProb-MRAC and in limbic regions for Atlas and ZTE, Table 2 and Fig. 8b.

Fig. 8
figure 8

Estimated R1 (a) and % bias (b) using Atlas-, ZTE- or MaxProb-MRAC compared to 68Ge-AC for different clusters of brain regions. Bars and whiskers are median, first and third quartile. ACR anterior cortical regions, PCR posterior cortical regions, STR striatal regions, LR limbic regions, WB whole brain. *p value < 0.05

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Evaluation of time-activity curves

Figure 9 shows the bias and its SD over time in SUV for the three evaluated MRAC methods compared to 68Ge-MRAC, in striatal regions and cerebellum. Particularly, in the caudate, the biases on TACs had variable shapes: a strong and slightly decreasing bias over time for ZTE-MRAC (+ 10% to7%), a relatively low bias for MaxProb-MRAC (+ 5 to − 5%) for MaxProb-MRAC and a strong and highly variable bias over time for Atlas-MRAC (+ 10 to − 7%). In cerebellum, a consistent bias over time was found for both Atlas- and ZTE-MRAC but not for MaxProb-MRAC. Intersubject variability was smallest for ZTE-MRAC and largest for MaxProb-MRAC in all considered regions.

Fig. 9
figure 9

Relative bias and standard deviation on time-activity curves for striatal regions with high binding of [11C]PE2I (caudate nucleus, putamen and whole striatum) and cerebellum with negligible binding which was used as a reference region

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Discussion

Significance

This study evaluated bias in estimated attenuation maps as well as accuracy, precision and degree of agreement of [11C]PE2I BPND and R1 estimates for three different MRAC methods using a 68Ge transmission scan as reference method. The main differences with most other reported MRAC evaluation studies are three-fold: (1) use of individual 68Ge-transmission AC maps with a direct measurement of 511 keV AC as reference method in contrast to CT-AC, (2) acquisition of dynamic data instead of static data and (3) quantification based on a kinetic modelling approach versus SUV. Reliable MRAC methods are prerequisites for both dynamic PET/MR imaging in research and clinical practice using dynamic [11C]PE2I PET examinations for differential diagnosis in patients with Parkinsonism [49].

Results

MRAC maps—The evaluation of attenuation maps did not reveal any MRAC approach being obviously superior. ZTE- and MaxProb-MRAC agreed best with 68Ge-AC in brain soft tissue. In the bone, Atlas-MRAC showed the lowest and ZTE-MRAC the highest bias. While absolute differences were small in soft tissue (less than 10%), they were larger in the bone (up to 16%), with Atlas-AC showing the lowest and ZTE-MRAC the highest bias. The bias in the bone may in part be due to the spatial resolution of the different AC images, with the skull being more smoothed in the Atlas- and 68Ge-AC images than in the Maxprob- and ZTE-AC images. Since the bone VOI was based on ZTE, it inherently showed lower AC values in Atlas and 68Ge-AC maps.

For BPND in striatal regions, mean bias across AC methods ranged from about − 12 to + 9%. For R1, the mean bias ranged from about + 1 to + 3% in various clusters of regions across the brain for all methods. Values within limits of −/+ 5% are generally regarded as acceptable. Importantly, differences in accuracy and precision between MRAC data sets can in part be explained by differences in shapes of the time-activity curves and their SDs.

Binding potential and relative delivery—Based on a full quantitative analysis of the dynamic [11C]PE2I PET data, ZTE-MRAC showed low BPND bias for all striatal regions (− 0.9 to 1.8%). The vendor-provided Atlas-MRAC method appeared to perform well for estimation of BPND values in the putamen, but a severe and significant underestimation was found in BPND values in the caudate (12.1%). In contrast, for MaxProb-MRAC, the mean bias was also relatively low in the caudate (2.1%) while a substantial, but non-significant, bias was observed in the putamen (9.2%). For R1, the mean bias ranged from about + 1 to + 3% in various clusters of regions across the brain for all methods. However, MaxProb-MRAC showed higher variability in bias for both BPND and R1 in all regions indicating a lower precision than ZTE- and Atlas-MRAC. Methods with both a high accuracy and precision are most desirable as this will lead to more robust and reproducible outcome parameters, and this will favour ZTE-MRAC as the most appropriate MRAC in this study.

Relatively few dynamic brain PET/MRI studies have investigated the effects of MRAC methods on accuracy and precision using kinetic analysis for quantification of outcome parameters [36, 39, 43, 45, 46]. Schramm et al. [36] evaluated ZTE-MRAC and Atlas-MRAC compared to CT-based AC in eight healthy volunteers using a SIGNA PET/MRI scanner and [18F]PE2I. BPND in striatal regions was estimated using SRTM with cerebellum as reference region. In the striatum, the mean bias was 1.5% for ZTE-MRAC and 3.8% for Atlas-MRAC. These results are in line with our study for ZTE-MRAC, but not for Atlas-MRAC where we found a bias of − 5.4%. Our Atlas-MRAC results revealed that especially in the caudate, the BPND values were severely underestimated for all participants, leading to a range of individual biases from − 11.0 to − 1.0% compared to − 1.0 versus + 9.4 reported by Schramm et al. [36]. The discrepancy in results might be due to differences in the type of participants (patients vs healthy subjects), methodological aspects such as tracer properties ([11C]PE2I vs [18F]FE-PE2I), definition of brain regions (using Hammers maximum probability atlas in PMOD [58, 59]) and most importantly the reference standard used (68Ge vs CT). However, both studies point out distinctly that ZTE-MRAC performed better than Atlas-MRAC.

Merida et al. [43] assessed the value of a multi-atlas approach (MaxProb-MRAC) compared to a single atlas with CT-based AC as reference method. The study used dynamic PET data from seven healthy participants acquired on a PET/CT scanner without TOF and using the serotonin 5-HT1A receptor tracer [18F] MPPF. SRTM was used for estimation of BPND across the brain, with cerebellar grey matter defined with the Hammers maximum probability atlas [58, 59] and excluding cerebellar vermis which may contain 5-HT1A receptors. Overall, bias of BPND ranged from − 2.5 to 5.0% for MaxProb-MRAC and from − 9.3 to 3.3% for their single-atlas MRAC. For MaxProb, the range of the bias was in good agreement with our results, as was the substantial increase in bias when using a single-atlas MRAC. Furthermore, their single-atlas MRAC caused a severe underestimation of BPND values, as seen for Atlas-MRAC in our study. However, these comparisons between studies need to be interpreted with care because of differences in data acquisition, tracer kinetics and specified VOIs. It should also be noted that that study’s single-atlas MRAC implementation is different from the Atlas-MRAC in the present work.

Evaluation of time-activity curves—The relative bias on TACs and its SD demonstrated that the effect of the applied MRAC methods varied over time between regions and methods, especially in the caudate and consequently striatum. These findings are in line with the hypothesis that various MRAC methods are affected differently by the radioactivity distribution in the brain at different time points [43, 44, 57]. For example, for MaxProb, the bias curves for the cerebellum and striatum have similar shapes, and bias in the resulting BPND is low (2.1%). On the other hand, relative bias on TACs in the putamen and cerebellum have different shapes, resulting in a larger bias in BPND for the putamen (9.2%) despite the bias for the putamen in the TACs themselves being much lower than that of the other two methods. Similarly, for ZTE, substantial but constant biases over time were found (around 10% for the striatum and 5% for the cerebellum). These quantification errors are then compensated when using cerebellum as the reference region in kinetic modelling, and even when using SUV ratios with target region over the cerebellum. It is noteworthy that the constant-but-high biases on ZTE TACs could have even a higher impact when kinetic modelling is performed with an arterial input functions as the error compensation between two regions may not take place. In that case, MaxProb-MRAC may be the optimal method because of its lower absolute bias. Scatter correction might also contribute to the bias; however, previous reports [43, 60, 61] indicate errors produced by incorrect attenuation correction to be more significant.

Implications—Based on our comparisons and evaluation of the results, we suggest that the choice of MRAC method may depend on the aim of the PET examinations, tracer and quantification method. The aim of the study determines the requested accuracy and precision of the quantification method. When considering absolute values in quantitative evaluation models, MaxProb’s low absolute bias may be particularly important. For ratio or reference region-based methods, ZTE’s consistent bias over time with a low variability will be advantageous, despite a higher absolute bias compared to MaxProb-MRAC. In case of participants with an abnormal anatomy, e.g. post-trauma or post-operative patients, subjects-specific acquisition-based methods like ZTE-MRAC should be preferred. In contrast to stand-alone PET and PET/CT systems, it seems to be difficult to develop a standard MRAC routine for AC in integrated PET/MR systems suitable for all circumstances and tracers. Instead, the choice of MRAC method for a specific investigation might be based on balancing the pros and cons of each approach.

Methodological considerations

There are some methodological considerations which need to be addressed as they might affect comparisons between MRAC methods and other studies. First, we used 68Ge-transmission AC maps with a direct voxel-wise measurement of AC, whereas CT-AC requires a conversion from Hounsfield units to 511 keV attenuation coefficients. Hence, the 68Ge-AC attenuation maps can be regarded as the true reference standard for AC. A comparison of 68Ge-AC and CT-AC demonstrated slightly higher radioactivity concentrations in PET images corrected with CT-AC: however, this increase is consistent and significant [8]. This bias should be noted when making comparisons across different imaging modalities.

In our previous study with static [11C]PE2I PET data [38], the effect of different AC values was investigated. The AC of 0.097 cm−1 measured for soft tissue for 68Ge-MRAC is modestly lower than that for the other investigated MRAC methods, i.e. 0.100 cm−1. The latter value was the same as used in clinical practice for CT-AC. In the present study, outcome parameters were normalized to the cerebellum, but we cannot exclude entirely a possible bias on BPND and R1 estimates due to differences in AC values.

AC of sinus regions is vulnerable to misclassification of tissue types and inaccurate registrations of templates/atlas as they are composed of the bone, soft tissue, and air [3, 32]. In theory, biased AC in sinus regions could therefore have affected the accuracy of the estimated R1 and BPND values in various regions. However, we believe this effect is modest. Accurate registration of templates/atlases might also be hampered by the difficulty of matching skull boundaries in sinus regions. Furthermore, the interindividual variability is large for sinus regions. Inaccurate registrations might confound parameter estimations, particularly in subcortical regions. The issues dealing with sinus segmentation have been addressed by the manufacturer [32, 62] but after the completion of the data acquisition in this work.

Like 68Ge-transmission AC maps, ZTE-MRAC is based on an individual scan in contrast to single- and multiple-atlas MRAC approaches. One advantage of a specific AC map for every individual is that it does not depend on a priori anatomical information and assumptions [10, 36]. Multiple atlases are expected being more reliable than a single atlas, as shown earlier by Merida et al. [43] and also found in our comparison of Atlas- and MaxProb-MRAC. However, methods based on an individual scan are likely to be suitable even for patients with an abnormal brain anatomy (e.g. brain cyst or hydrocephalus) or after surgery (e.g. patients with epilepsy surgery or traumatic brain injury).

MRI acquisitions are prone to susceptibility artefacts when the patient owns metallic implants, which could impact the performance of ZTE. However, Chiba et al. [31] reported that the magnetic susceptibility is minimal for ZTE, even at high magnetic fields (7 T MRI), due to the extremely short echo time. Hence, the risk for disturbing artefacts would be negligible. In our study, we had no patients with metallic implants as it was an exclusion criterion.

Finally, the vendor-provided ZTE- and Atlas-MRAC are under continuous development and reflected the state of the art at the time when the study was conducted. The version of ZTE-MRAC as used in the present work (MP26) is commercially available with small modifications mainly in terms of image resolution [27], but further developments have already been proposed [40] and may be implemented in forthcoming upgrades.

Limitations

A limitation related to the design was that the results were based on data from only nine patients with Parkinsonism and this might have affected the robustness of our results. Some patients had even severe atrophy. In this case, MaxProb-MRAC may mislabel cerebral spinal fluid as the bone, which could cause a positive bias in the cerebellum as a result of inaccurate bone estimation [19], but this positive bias was not observed in our results. It might have been beneficial to study a healthy cohort in addition to the patient cohort, as effects of MRAC method and disease were entangled in the current design.

In the analysis, we had to deal with differences in axial FOV between scanners, and the MRAC maps for 68Ge and MaxProb were completed with corresponding information from the Atlas-AC map. Consequently, the lines of response associated with the added parts might have introduced a bias towards Atlas-MRAC, though more in regions outside than inside the brain. Head movements during the entire dynamic [11C]PE2I PET scan might also have affected the results as MRI sequences for AC are acquired during the first five minutes. Frame by frame motion correction was applied post reconstruction using identical transformation parameters for all four dynamic datasets, and thus, any remaining movement-induced errors should be the same for all four AC methods. However, the AC maps could be not corrected for any motion-induced errors, and the consequences might differ between AC methods.

Despite these limitations, this study provides important information on the accuracy and precision of four MRAC methods in a clinical setting with use of dynamic data.

Future developments

For the future development of MRAC methods in dynamic brain PET, it will be important to consider diverse neurological applications in larger patient cohorts with specific tracers. The current data did not allow subgrouping based on, e.g. the magnitude of accuracy and precision, subtypes of Parkinsonian disorders. Application to more complex cases will show whether the developed MRAC methods are likely to perform well in clinical practice. For example, differential diagnosis of Parkinsonian disorders might be extremely challenging at an early stage due to the difficulty of distinguishing typical Parkinson’s disease and the atypical subtypes, and the confounding effect of comorbidity with other neurodegenerative and chronic diseases (e.g. dementia and diabetes). For this, it is essential that quantitative values are accurate and precise.

Another promising direction is the further development of an individual mapping of linear attenuation coefficients, as suggested by Visvikis et al. [3]. Like CT-AC, most of the reported MRAC methods disregarded possible heterogeneity in tissue by using AC maps with fixed values assigned to a limited number of tissue types. More detailed attenuation maps may be developed by optimizing the simultaneous acquired information from MRI and PET combined with templates/atlas and machine learning [39, 40, 42, 45, 63].

Conclusions

ZTE-MRAC showed a high accuracy and precision for both BPND and R1 estimates. MaxProb-MRAC had statistically a similar accuracy, but a lower precision than ZTE-MRAC. Differences in accuracy and precision between MRAC methods were in part explained by differences in activity concentration bias over time. MaxProb-MRAC showed the lowest absolute bias over time which might be important when considering absolute activity concentration or SUV values in quantitative evaluation models. On the other hand, ZTE’s higher but consistent bias over time in target and reference regions seemed to be most advantageous for quantification using ratio or reference region-based evaluations.

Availability of data and materials

João M. Sousa (joao.sousa@surgsci.uu.se) is the corresponding author for the data used in this manuscript.

Abbreviations

AC:

Attenuation correction

BPND :

Binding potential (non-displaceable)

CT:

Computer tomography

DAT:

Dopamine transporter

FDG:

Fluorodeoxyglucose

FOV:

Field of view

MaxProb:

Maximum probability algorithm

MRAC:

MR-based attenuation correction

MRI:

Magnetic resonance imaging

NEX:

Number of excitations

OSEM:

Ordered subset expectation maximisation

PET:

Positron emission tomography

R1 :

Relative delivery

RPM:

Receptor parametric mapping

SRTM:

Simplified reference tissue model

T:

Tesla

TOF:

Time of flight

UTE:

Ultrashort echo time

VOI:

Volume of interest

ZTE:

Zero echo time

3D:

Three-dimensional

References

  1. Chen Y, An H. Attenuation correction of PET/MR imaging. Magn Reson Imaging Clin N Am. 2017;25:245–55 Available from: http://www.ncbi.nlm.nih.gov/pubmed/28390526. NIH Public Access.

  2. Keereman V, Mollet P, Berker Y, Schulz V, Vandenberghe S. Challenges and current methods for attenuation correction in PET/MR. Magn Reson Mater Physics, Biol Med. 2013;26:81–98 Available from: http://link.springer.com/10.1007/s10334-012-0334-7.

    Article  Google Scholar 

  3. Visvikis D, Monnier F, Bert J, Hatt M, Fayad H. PET/MR attenuation correction: where have we come from and where are we going? Eur J Nucl Med Mol Imaging. 2014;41:1172–5 Available from: http://link.springer.com/10.1007/s00259-014-2748-0. Springer Berlin Heidelberg.

  4. Bezrukov I, Mantlik F, Schmidt H, Schölkopf B, Pichler BJ. MR-based PET attenuation correction for PET/MR Imaging. Semin Nucl Med. 2013;43:45–59 Available from: http://linkinghub.elsevier.com/retrieve/pii/S0001299812000785. Elsevier Inc.

    Article  Google Scholar 

  5. Carson RE, Daube-Witherspoon ME, Green MV. A method for postinjection PET transmission measurements with a rotating source. J Nucl Med. 1988;29:1558–67. Available from: http://www.ncbi.nlm.nih.gov/pubmed/3261786.

  6. Bailey DL. Transmission scanning in emission tomography. Eur J Nucl Med Mol Imaging. 1998;25:774–87. Available from: http://link.springer.com/10.1007/s002590050282.

  7. Eldib M, Bini J, Faul DD, Oesingmann N, Tsoumpas C, Fayad ZA. Attenuation correction for magnetic resonance coils in combined PET/MR imaging. PET Clin. 2016;11:151–60. Available from: https://linkinghub.elsevier.com/retrieve/pii/S1556859815001170. W.B. Saunders.

  8. Nakamoto Y, Osman M, Cohade C, Marshall LT, Links JM, Kohlmyer S, et al. PET/CT: comparison of quantitative tracer uptake between germanium and CT transmission attenuation-corrected images. J Nucl Med. 2002;43:1137–43. Available from: http://www.ncbi.nlm.nih.gov/pubmed/12215550. Society of Nuclear Medicine.

  9. Mackewn JE, Stirling J, Jeljeli S, Gould SM, Johnstone RI, Merida I, et al. Practical issues and limitations of brain attenuation correction on a simultaneous PET-MR scanner. EJNMMI Phys. 2020;7:24 Available from: https://ejnmmiphys.springeropen.com/articles/10.1186/s40658-020-00295-x.

    Article  CAS  Google Scholar 

  10. Sekine T, ter Voert EEGW, Warnock G, Buck A, Huellner M, Veit-Haibach P, et al. Clinical evaluation of zero-echo-time attenuation correction for brain 18F-FDG PET/MRI: comparison with atlas attenuation correction. J Nucl Med. 2016;57:1927–32 Available from: https://www.ncbi.nlm.nih.gov/pubmed/27339875%5Cn. http://jnm.snmjournals.org/content/57/12/1927.full.pdf.

    Article  CAS  Google Scholar 

  11. Sekine T, Buck A, Delso G, ter Voert EEGW, Huellner M, Veit-Haibach P, et al. Evaluation of atlas-based attenuation correction for integrated PET/MR in human brain: application of a head atlas and comparison to true CT-based attenuation correction. J Nucl Med. 2016;57:215–20 Available from: http://jnm.snmjournals.org/cgi/doi/10.2967/jnumed.115.159228.

    Article  CAS  Google Scholar 

  12. Wiesinger F, Sacolick LI, Menini A, Kaushik SS, Ahn S, Veit-Haibach P, et al. Zero TE MR bone imaging in the head. Magn Reson Med. 2016;75:107–14. Available from. https://doi.org/10.1002/mrm.25545.

    Article  PubMed  Google Scholar 

  13. Du J, Borden K, Diaz E, Bydder M. Imaging of metallic implant using 3D ultrashort echo time (3D UTE) pulse sequence. Proc Intl Soc Mag Reson Med. 2010;18:132.

  14. Martinez-Moller A, Souvatzoglou M, Delso G, Bundschuh RA, Chefd’hotel C, Ziegler SI, et al. Tissue classification as a potential approach for attenuation correction in whole-body PET/MRI: evaluation with PET/CT Data. J Nucl Med. 2009;50:520–6 Available from: http://jnm.snmjournals.org/cgi/doi/10.2967/jnumed.108.054726.

    Article  Google Scholar 

  15. Beyer T, Lassen ML, Boellaard R, Delso G, Yaqub M, Sattler B, et al. Investigating the state-of-the-art in whole-body MR-based attenuation correction: an intra-individual, inter-system, inventory study on three clinical PET/MR systems. Magn Reson Mater Physics, Biol Med. 2016;29:75–87. Available from: http://link.springer.com/10.1007/s10334-015-0505-4. Springer Berlin Heidelberg.

  16. Teuho J, Torrado-Carvajal A, Herzog H, Anazodo U, Klén R, Iida H, et al. Magnetic resonance-based attenuation correction and scatter correction in neurological positron emission tomography/magnetic resonance imaging—current status with emerging applications. Front Phys. 2020;7:243.

  17. Keereman V, Van Holen R, Mollet P, Vandenberghe S. The effect of errors in segmented attenuation maps on PET quantification. Med Phys. 2011;38:6010–6019. Available from: https://doi.org/10.1118/1.3651640. American Association of Physicists in Medicine.

  18. Dickson JC, O’Meara C, Barnes A. A comparison of CT- and MR-based attenuation correction in neurological PET. Eur J Nucl Med Mol Imaging. 2014;41:1176–89. Available from: http://link.springer.com/10.1007/s00259-013-2652-z. Springer Berlin Heidelberg.

  19. Andersen FL, Ladefoged CN, Beyer T, Keller SH, Hansen AE, Højgaard L, et al. Combined PET/MR imaging in neurology: MR-based attenuation correction implies a strong spatial bias when ignoring bone. Neuroimage. 2014;84:206–16 Elsevier Inc.

    Article  Google Scholar 

  20. Wollenweber SD, Ambwani S, Delso G, Lonn AHR, Mullick R, Wiesinger F, et al. Evaluation of an atlas-based PET head attenuation correction using PET/CT & MR patient data. IEEE Trans Nucl Sci. 2013;60:3383–90 Available from: http://ieeexplore.ieee.org/document/6583257/.

    Article  Google Scholar 

  21. Koesters T, Friedman KP, Fenchel M, Zhan Y, Hermosillo G, Babb J, et al. Dixon Sequence with superimposed model-based bone compartment provides highly accurate PET/MR attenuation correction of the brain. J Nucl Med. 2016;57:918–24. Available from: http://www.ncbi.nlm.nih.gov/pubmed/26837338. Society of Nuclear Medicine.

  22. Burgos N, Cardoso MJ, Thielemans K, Modat M, Pedemonte S, Dickson J, et al. Attenuation correction synthesis for hybrid PET-MR scanners: application to brain studies. IEEE Trans Med Imaging. 2014;33:2332–41. Available from: http://ieeexplore.ieee.org/lpdocs/epic03/wrapper.htm?arnumber=6858020.

  23. Burgos N, Cardoso MJ, Thielemans K, Modat M, Dickson J, Schott JM, et al. Multi-contrast attenuation map synthesis for PET/MR scanners: assessment on FDG and Florbetapir PET tracers. Eur J Nucl Med Mol Imaging. 2015;42:1447–58. Available from: http://link.springer.com/10.1007/s00259-015-3082-x. Springer Berlin Heidelberg.

  24. Huynh T, Gao Y, Kang J, Wang L, Zhang P, Lian J, et al. Estimating CT image from MRI data using structured random forest and auto-context model. IEEE Trans Med Imaging. 2016;35:174–83. Available from: http://www.ncbi.nlm.nih.gov/pubmed/26241970. NIH Public Access.

  25. Ladefoged CN, Law I, Anazodo U, St. Lawrence K, Izquierdo-Garcia D, Catana C, et al. A multi-centre evaluation of eleven clinically feasible brain PET/MRI attenuation correction techniques using a large cohort of patients. Neuroimage. 2017;147:346–59. Available from: http://linkinghub.elsevier.com/retrieve/pii/S1053811916307170.

  26. Delso G, Wiesinger F, Carl M, McKinnon G, Khalighi M, ter Voert E, et al. ZTE-based clinical bone imaging for PET/MR. J Nucl Med. 2015;56:1806. Available from: http://jnm.snmjournals.org/cgi/content/short/56/supplement_3/1806. Society of Nuclear Medicine.

  27. Wiesinger F, Bylund M, Yang J, Kaushik S, Shanbhag D, Ahn S, et al. Zero TE-based pseudo-CT image conversion in the head and its application in PET/MR attenuation correction and MR-guided radiation therapy planning. Magn Reson Med. 2018;80:1440–51. Available from:. https://doi.org/10.1002/mrm.27134.

    Article  PubMed  Google Scholar 

  28. Delso G, Carl MC, Wiesinger F, Sacolick L, Huellner M, Kuhn F, et al. Evaluation of 2D and 3D UTE for PET/MR attenuation correction in the head. J Nucl Med. 2013;54:2108 Available from: http://jnm.snmjournals.org/content/54/supplement_2/2108.short.

    Google Scholar 

  29. Ladefoged CN, Benoit D, Law I, Holm S, Kjær A, HØjgaard L, et al. Region specific optimization of continuous linear attenuation coefficients based on UTE (RESOLUTE): application to PET/MR brain imaging. Phys Med Biol. 2015;60:8047–65. Available from: http://stacks.iop.org/0031-9155/60/i=20/a=8047?key=crossref.734635890123afb79cc9eb94d2b0cd10. IOP Publishing.

  30. Larson PEZ, Han M, Krug R, Jakary A, Nelson SJ, Vigneron DB, et al. Ultrashort echo time and zero-echo-time MRI at 7 T. Magn Reson Mater Physics, Biol Med. 2016;29:359–70 NIH Public Access; Available from: http://www.ncbi.nlm.nih.gov/pubmed/26702940.

  31. Chiba Y, Murakami H, Sasaki M, Endo H, Yamabe D, Kinno D, et al. Quantification of metal-induced susceptibility artifacts associated with ultrahigh-field magnetic resonance imaging of spinal implants. JOR spine. 2019;2:e1064 Available from: https://onlinelibrary.wiley.com/doi/abs/10.1002/jsp2.1064.

    Article  Google Scholar 

  32. Yang J, Wiesinger F, Kaushik S, Shanbhag D, Hope TA, Larson PEZ, et al. Evaluation of sinus/edge-corrected zero-echo-time–based attenuation correction in brain PET/MRI. J Nucl Med. 2017;58:1873–9. Available from: http://jnm.snmjournals.org/content/early/2017/05/03/jnumed.116.188268.full.pdf.

  33. Delso G, Wiesinger F, Sacolick LI, Kaushik SS, Shanbhag DD, Hullner M, et al. Clinical evaluation of zero-echo-time MR imaging for the segmentation of the skull. J Nucl Med. 2015;56:417–22 Available from: http://jnm.snmjournals.org/cgi/doi/10.2967/jnumed.114.149997.

    Article  Google Scholar 

  34. Khalife M, Fernandez B, Nioche C, Soussan M, Buvat I, Brulon V. Exploring the relation between MR ZTE intensity and tissue density: application to MR attenuation correction in PET/MR. In: 2016 IEEE Nuclear Science Symposium, Medical Imaging Conference and Room-Temperature Semiconductor Detector Workshop: IEEE; 2016. p. 1–4. Available from: http://ieeexplore.ieee.org/document/8069588/.

  35. Khalifé M, Fernandez B, Jaubert O, Soussan M, Brulon V, Buvat I, et al. Subject-specific bone attenuation correction for brain PET/MR: can ZTE-MRI substitute CT scan accurately? Phys Med Biol. 2017;62:7814–32 Available from: http://stacks.iop.org/0031-9155/62/i=19/a=7814?key=crossref.eadca1ee04a8c704ffada57c864b9f19.

    Article  Google Scholar 

  36. Schramm G, Koole M, Willekens SMA, Rezaei A, Van Weehaeghe D, Delso G. et al, Regional accuracy of ZTE-based attenuation correction in static and dynamic brain PET/MR. 2018;211. Available from: http://arxiv.org/abs/1806.03481.Front Phys. 2019;7:211.

  37. Sgard B, Khalifé M, Bouchut A, Fernandez B, Soret M, Giron A, et al. ZTE MR-based attenuation correction in brain FDG-PET/MR: performance in patients with cognitive impairment. Eur Radiol. 2020;30:1770–9. Available from: http://link.springer.com/10.1007/s00330-019-06514-z. Springer Berlin Heidelberg.

  38. Sousa JM, Appel L, Engström M, Papadimitriou S, Nyholm D, Larsson E-M, et al. Evaluation of zero-echo-time attenuation correction for integrated PET/MR brain imaging—comparison to head atlas and 68Ge-transmission-based attenuation correction. EJNMMI Phys. 2018;5:20 Available from: https://ejnmmiphys.springeropen.com/articles/10.1186/s40658-018-0220-0.

    Article  Google Scholar 

  39. Spuhler KD, Gardus J, Gao Y, DeLorenzo C, Parsey R, Huang C. Synthesis of patient-specific transmission data for PET attenuation correction for PET/MRI neuroimaging using a convolutional neural network. J Nucl Med. 2019;60:555–60.

    Article  CAS  Google Scholar 

  40. Blanc-Durand P, Khalife M, Sgard B, Kaushik S, Soret M, Tiss A, et al. Attenuation correction using 3D deep convolutional neural network for brain 18F-FDG PET/MR: Comparison with Atlas, ZTE and CT based attenuation correction. Ginsberg SD, editor. PLoS One. 2019;14:1–12. Available from: https://dx.plos.org/10.1371/journal.pone.0223141.

  41. Gong K, Yang J, Kim K, El Fakhri G, Seo Y, Li Q. Attenuation correction for brain PET imaging using deep neural network based on Dixon and ZTE MR images. Phys Med Biol. 2018;63(12).

  42. Ladefoged CN, Marner L, Hindsholm A, Law I, Højgaard L, Andersen FL. Deep learning based attenuation correction of PET/MRI in pediatric brain tumor patients: evaluation in a clinical setting. Front Neurosci. 2018;12:1005 Available from: https://www.frontiersin.org/article/10.3389/fnins.2018.01005/full.

    Article  Google Scholar 

  43. Mérida I, Reilhac A, Redouté J, Heckemann RA, Costes N, Hammers A. Multi-atlas attenuation correction supports full quantification of static and dynamic brain PET data in PET-MR. Phys Med Biol. 2017;62:2834–58.

    Article  Google Scholar 

  44. Mansur A, Newbould R, Searle GE, Redstone C, Gunn RN, Hallett WA. PET-MR Attenuation correction in dynamic brain PET Using [ 11 C]Cimbi-36: a direct comparison with PET-CT. IEEE Trans Radiat Plasma Med Sci. 2018;2:483–9. Available from: https://ieeexplore.ieee.org/document/8402147/.

  45. Rischka L, Gryglewski G, Berroterán-Infante N, Rausch I, James GM, Klöbl M, et al. Attenuation correction approaches for serotonin transporter quantification with PET/MRI. Front Physiol. 2019;10:1–11 Available from: https://www.frontiersin.org/article/10.3389/fphys.2019.01422/full.

    Article  Google Scholar 

  46. Cabello J, Avram M, Brandl F, Mustafa M, Scherr M, Leucht C, et al. Impact of non-uniform attenuation correction in a dynamic [18F]-FDOPA brain PET/MRI study. EJNMMI Res. 2019;9:77. Available from: https://ejnmmires.springeropen.com/articles/10.1186/s13550-019-0547-0. SpringerOpen.

  47. Emond P, Guilloteau D, Chalon S. PE2I: A radiopharmaceutical for in vivo exploration of the dopamine transporter. CNS Drug Rev. 2008;14:47–64. Available from: http://doi.wiley.com/10.1111/j.1527-3458.2007.00033.x. Blackwell Publishing Inc.

  48. Jonasson M, Appel L, Engman J, Frick A, Nyholm D, Askmark H, et al. Validation of parametric methods for [11C]PE2I positron emission tomography. Neuroimage. 2013;74:172–8 Available from: http://linkinghub.elsevier.com/retrieve/pii/S1053811913001493.

    Article  Google Scholar 

  49. Appel L, Jonasson M, Danfors T, Nyholm D, Askmark H, Lubberink M, et al. Use of 11C-PE2I PET in differential diagnosis of Parkinsonian disorders. J Nucl Med. 2015;56:234–42 Available from: http://jnm.snmjournals.org/cgi/doi/10.2967/jnumed.114.148619.

    Article  Google Scholar 

  50. Brooks DJ. Molecular imaging of dopamine transporters. Ageing Res Rev. 2016;30:114–21. Available from: https://linkinghub.elsevier.com/retrieve/pii/S156816371530043X. Elsevier Ireland Ltd.

  51. Merida I, Costes N, Heckemann R, Hammers A. Pseudo-CT generation in brain MR-PET attenuation correction: comparison of several multi-atlas methods. EJNMMI Phys. 2015;2:A29. Available from. https://doi.org/10.1186/2197-7364-2-S1-A29.

    Article  PubMed  PubMed Central  Google Scholar 

  52. Carney JPJ, Townsend DW, Rappoport V, Bendriem B. Method for transforming CT images for attenuation correction in PET/CT imaging. Med Phys. 2006;33:976–83.

    Article  Google Scholar 

  53. Svarer C, Madsen K, Hasselbalch SG, Pinborg LH, Haugbøl S, Frøkjær VG, et al. MR-based automatic delineation of volumes of interest in human brain PET images using probability maps. Neuroimage. 2005;24:969–79. Available from: http://www.ncbi.nlm.nih.gov/pubmed/15670674.

  54. Heckemann RA, Keihaninejad S, Aljabar P, Rueckert D, Hajnal JV, Hammers A. Improving intersubject image registration using tissue-class information benefits robustness and accuracy of multi-atlas based anatomical segmentation. Neuroimage. 2010;51:221–7 Available from: https://linkinghub.elsevier.com/retrieve/pii/S1053811910000947.

    Article  Google Scholar 

  55. Gunn RN, Lammertsma AA, Hume SP, Cunningham VJ. Parametric imaging of ligand-receptor binding in PET using a simplified reference region model. Neuroimage. 1997;6:279–87 Available from: https://linkinghub.elsevier.com/retrieve/pii/S1053811997903037.

    Article  CAS  Google Scholar 

  56. Lammertsma AA, Hume SP. Simplified reference tissue model for PET receptor studies. Neuroimage. 1996;4:153–8 Available from: http://linkinghub.elsevier.com/retrieve/pii/S105381199690066X.

    Article  CAS  Google Scholar 

  57. Lassen ML, Muzik O, Beyer T, Hacker M, Ladefoged CN, Cal-González J, et al. Reproducibility of quantitative brain imaging using a PET-only and a combined PET/MR system. Front Neurosci. 2017;11:396. Available from: http://journal.frontiersin.org/article/10.3389/fnins.2017.00396/full. Frontiers Media S.A.

  58. Hammers A, Allom R, Koepp MJ, Free SL, Myers R, Lemieux L, et al. Three-dimensional maximum probability atlas of the human brain, with particular reference to the temporal lobe. Hum Brain Mapp. 2003;19:224–47. Available from: https://onlinelibrary.wiley.com/doi/full/10.1002/hbm.10123. John Wiley & Sons, Ltd.

  59. Gousias IS, Rueckert D, Heckemann RA, Dyet LE, Boardman JP, Edwards AD, et al. Automatic segmentation of brain MRIs of 2-year-olds into 83 regions of interest. Neuroimage. 2008;40:672–84. Available from: https://pubmed.ncbi.nlm.nih.gov/18234511/. Neuroimage.

  60. Burgos N, Thielemans K, Cardoso MJ, Markiewicz P, Jiao J, Dickson J, et al. Effect of scatter correction when comparing attenuation maps: application to brain PET/MR. In: 2014 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC) 2014; 2016.

    Google Scholar 

  61. Teuho J, Saunavaara V, Tolvanen T, Tuokkola T, Karlsson A, Tuisku J, et al. Quantitative evaluation of 2 scatter-correction techniques for 18F-FDG brain PET/MRI in regard to MR-based attenuation correction. J Nucl Med. 2017;58:1691–8.

    Article  CAS  Google Scholar 

  62. Delso G, Kemp B, Kaushik S, Wiesinger F, Sekine T. Improving PET/MR brain quantitation with template-enhanced ZTE. Neuroimage. 2018;181:403–13 Available from: https://linkinghub.elsevier.com/retrieve/pii/S105381191830644X.

    Article  Google Scholar 

  63. Kläser K, Varsavsky T, Markiewicz P, Vercauteren T, Atkinson D, Thielemans K, et al. Improved MR to CT synthesis for PET/MR attenuation correction using imitation learning; 2019. p. 13–21. Available from: http://link.springer.com/10.1007/978-3-030-32778-1_2.

    Google Scholar 

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Acknowledgements

The authors would like to express their gratitude to Anders Lundberg and Marie Åhlman, Uppsala University, for the image acquisition and support with data handling, and to the patients for participation in this study. Further, we would like to thank Dr. Gaspar Delso and Dr. Florian Wiesinger, GE Healthcare, Waukesha, for software support.

Funding

This work was supported by the Swedish Research Council, grant no. 2011-6269 and the Regional Medical Training and Research Agreement (Avtal om Läkarutbildning och Forskning, ALF) between Uppsala County and Uppsala University Hospital. Open Access funding provided by Uppsala University.

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Author notes

  1. João M. Sousa and Lieuwe Appel contributed equally to this work.

Authors and Affiliations

  1. Department of Surgical Sciences, Uppsala University, Uppsala, Sweden

    João M. Sousa, Lieuwe Appel, Håkan Ahlström & Mark Lubberink

  2. Medical Imaging Centre, Uppsala University Hospital, Uppsala, Sweden

    Lieuwe Appel & Håkan Ahlström

  3. CERMEP, Lyon, France

    Inés Merida & Nicolas Costes

  4. Department of Radiation Physics, Sahlgrenska Academy, University of Gothenburg, Gothenburg, Sweden

    Rolf A. Heckemann

  5. GE Healthcare, Waukesha, USA

    Mathias Engström

  6. Department of Neurology, Uppsala University Hospital, Uppsala, Sweden

    Stergios Papadimitriou & Dag Nyholm

  7. Department of Neurosciences, Uppsala University, Uppsala, Sweden

    Dag Nyholm

  8. King’s College London & Guy’s and St Thomas’ PET Centre, King’s College, London, UK

    Alexander Hammers

  9. Medical Physics, Uppsala University Hospital, Uppsala, Sweden

    Mark Lubberink

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Contributions

ML, LA and HA did the concept, design and ethical application. SP, DN and LA recruited the patients. JMS, LA and ML are responsible for the acquisition of data. JMS, ME, ML, IM, NC and RAH did the data analysis. JMS, IM, ML, LA and AH interpreted the data. JMS, IM, LA and ML did the draft of the manuscript. All authors reviewed the manuscript. The authors read and approved the final manuscript.

Corresponding author

Correspondence to João M. Sousa.

Ethics declarations

Ethics approval and consent to participate

All procedures performed in studies involving human participants were in accordance with the ethical standards of the institutional and/or national research committee and with the 1964 Helsinki Declaration and its later amendments or comparable ethical standards. Informed consent was obtained from all individual participants included in the study.

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Not applicable.

Competing interests

ME is an employee of GE Healthcare. HA and ML receive research support and speaker fees from GE Healthcare. The other authors declare that they have no competing interest.

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Sousa, J.M., Appel, L., Merida, I. et al. Accuracy and precision of zero-echo-time, single- and multi-atlas attenuation correction for dynamic [11C]PE2I PET-MR brain imaging. EJNMMI Phys 7, 77 (2020). https://doi.org/10.1186/s40658-020-00347-2

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