1. Introduction
Diagnostic assessment of the posterior fossa using non-contrast head computed tomography (CT) remains challenging because of beam-hardening artifacts originating from the dense skull base. These artifacts arise when lower-energy photons are preferentially absorbed by the petrous temporal bones, resulting in distortion of attenuation values, increased image noise, and reduced grey–white matter differentiation in the posterior fossa [
1,
2]. The resulting degradation of image quality may limit visualization of the brainstem and cerebellum, particularly in routine emergency CT examinations.
Although magnetic resonance imaging (MRI) provides superior assessment of posterior fossa pathology, including ischemia, inflammatory disease, and neoplasms, MRI is often unavailable in the acute setting, requires substantially longer examination times, and may be contraindicated in some patients [
3,
4]. Consequently, optimizing the image quality of routine head CT remains clinically relevant, even when MRI is ultimately performed.
Dual-energy CT (DECT) enables material-specific image reconstruction and generation of virtual monoenergetic images (VMIs), which simulate images acquired using monochromatic X-ray beams at selectable energy levels. Depending on the acquisition technology—including rapid kV switching, dual-source systems, or dual-layer detector CT—VMIs can reduce beam-hardening artifacts while simultaneously influencing image noise, tissue contrast, and contrast-to-noise ratio [
5,
6]. Dual-layer spectral CT is particularly attractive because spectral information is acquired simultaneously without changes to routine scanning protocols or additional radiation exposure [
7].
Previous studies have demonstrated that VMIs improve image quality in unenhanced head CT, including reduced posterior fossa artifacts and improved grey–white matter differentiation [
8,
9,
10]. However, these studies have generally been limited by relatively small patient cohorts, evaluation of a restricted number of monoenergetic reconstructions, or both. Consequently, the optimal reconstruction energy and the robustness of these findings across a larger patient population remain incompletely established.
Accordingly, we performed a comprehensive quantitative and qualitative evaluation of posterior fossa image quality across the monoenergetic reconstruction spectrum using dual-layer spectral CT in a large cohort of normal non-contrast head CT examinations. By isolating the effect of reconstruction energy in examinations without intracranial pathology, we aimed to characterize how VMIs influence beam-hardening artifacts, image noise, signal-to-noise ratio, contrast-to-noise ratio, and subjective image quality, thereby providing further evidence to guide image optimization in spectral head CT.
2. Materials and Methods
2.1. Study Population
We retrospectively included consecutive adult patients (≥18 years) who underwent non-contrast head CT using a dual-layer spectral CT scanner (IQon Spectral CT, Philips Healthcare, Best, The Netherlands) between 1 October and 30 November 2018. Only examinations reported as normal, without evidence of ischemia, intracranial hemorrhage, mass lesion, or other structural pathology, were included.
Restricting the study population to examinations without intracranial pathology allowed for assessment of reconstruction-dependent changes in attenuation, image noise, and beam-hardening artifacts without confounding from lesion-related alterations in tissue attenuation or image interpretation.
The Swedish Ethical Review Authority approved the study and waived individual informed consent (reference number 2019-02225).
Generative AI (ChatGPT version 1.2026183, OpenAI Inc., San Francisco, CA, USA) was used for language editing. All edits were reviewed and approved by the authors.
2.2. Image Acquisition and Reconstruction Parameters
All examinations were acquired using the institutional standard non-contrast head CT protocol: tube voltage 120 kilovolt (kV), tube current modulation (DoseRight, DoseRight Index 37, Philips Healthcare, Best, The Netherlands), collimation 64 × 0.625, pitch 0.36 and rotation time 0.33 s. The dose length product (DLP) was noted for each patient, and the effective dose was calculated by multiplying DLP with a conversion factor of 0.0024 mSv/mGycm [
11] to characterize the radiation exposure associated with the acquisition protocol.
For this study, the spectral image file for each patient was then transferred to IntelliSpace Portal (ISP) (Philips Healthcare, Best, The Netherlands) v. 10.1.4.21403 software, where axial CIs of 4 mm slice thickness, as per local routine, were reconstructed and all subsequent image measurements performed.
2.3. Quantitative Analysis Method
Quantitative image analysis was performed using standardized regions of interest (ROIs) positioned in predefined posterior fossa and supratentorial reference locations to evaluate both local artifact behavior and unaffected reference tissue.
Five predefined circular ROIs (10 ± 1 mm diameter) were manually positioned on the coventional image series by a single observer using standardized anatomical landmarks. The ROIs were subsequently propagated automatically by the spectral analysis software to all monoenergetic reconstructions, ensuring identical anatomical sampling across all energy levels. These ROIs were as follows:
cerebellar grey matter,
cerebellar white matter,
the interpetrous portion of the pons,
thalamic grey matter (reference), and
supratentorial white matter (reference).
Reference ROIs were included to distinguish reconstruction-related image changes specific to the posterior fossa from global changes in image characteristics (
Figure 1).
Mean and standard deviation (SD) attenuation values measured in Hounsfield units (HU) were noted for each ROI in the CIs and retrieved through spectral diagrams using the ISP software for the corresponding ROIs in VMIs at 40–200 keV in 10 keV intervals.
The standard deviation of attenuation within each ROI was used as a surrogate measure of image noise. The SD of the ROI in the interpetrous pons was used as a surrogate measure of beam-hardening artifact severity (Posterior Fossa Artifact Index, PFAI), in accordance with previous studies [
8,
9].
The SNR was calculated using previously described formulas HU/SD where HU indicates the mean attenuation of the tissue in Hounsfield units and SD the standard deviation (image noise) of the tissue within the ROI.
The contrast-to-noise ratio (CNR) was calculated for reference GM–WM and cerebellar GM–WM as (HU
1 − HU
2)/√ (SD
1 + SD
2), where HU_1 and HU_2 represent the mean attenuation of the two tissues and SD_1 and SD_2 their corresponding standard deviations. This CNR formulation has been used in previous spectral head CT studies [
12,
13] and was selected to maintain methodological comparability with previous work. The difference in mean attenuation (ΔHU) was calculated for cerebellar WM–interpetrous pons as previously described [
10].
2.4. Qualitative Analysis Method
Forty consecutive examinations from the study cohort were included in the qualitative analysis. Conventional images (CIs) and virtual monoenergetic images (VMIs) reconstructed at 40–200 keV (10 keV increments) were independently reviewed by two interventional neuroradiologists with 20 and 8 years of experience, respectively. Only Reviewer 1 repeated the qualitative assessment after a three-week washout period; therefore, intra-reader agreement was calculated only for Reviewer 1.
The readers were blinded to the reconstruction energy level and independently evaluated all image series. Before the independent assessments, both reviewers jointly calibrated the scoring system using image sets not included in the study. The individual assessment and grading were performed using Viewdex (Viewer for Digital Evaluation of X-ray images) version 3.0 software [
14], which allows for visualization of an axial CT stack with standard window settings (width = 65, level = 35). The readers were allowed to adjust window settings. VMIs and CIs were randomly presented to the reviewers for grading using the Viewdex software. All images were displayed on standard diagnostic monitors (Coronis
® Fusion MDCC-6430 6MP, Barco, Kortrijk, Belgium). CIs and VMIs at 40, 50, 60, 70, 80, 100, 120, 140 and 200 keV were included in the qualitative analysis based on both previous work [
8,
9,
10] and visual assessment of the graphs of the quantitative part of this study.
Images were assessed using a five-point Likert scale for:
overall image quality;
grey–white matter differentiation in the cerebellum;
grey–white matter differentiation in the supratentorial brain;
severity of artifacts in the temporal cerebellum;
severity of artifacts in the interpetrous pons; and
severity of supratentorial subcalvarial artifacts.
In addition, the readers recorded whether they considered each image series to provide sufficient image quality to allow for confident exclusion of major posterior fossa or supratentorial pathology. This assessment reflected subjective reader confidence rather than diagnostic accuracy because only examinations without intracranial pathology were included.
Higher scores indicated better image quality, improved grey–white matter differentiation, and less severe artifacts.
2.5. Statistical Analysis
Continuous data are presented as mean ± SD, or mean with 95% confidence interval, and nominal and ordinal data as mean ± SD or quantity (%). A paired sample t-test was used to compare paired, parametric, continuous data (values of the same ROI but different reconstructions) and an unpaired sample t-test compared unpaired, parametric, continuous data (for example comparing values of different ROIs or CNR for reference/cerebellar tissue). A Wilcoxon signed rank test was used to compare paired ordinal data (such as values from the same task of the subjective analysis but for different reconstructions), assuming equal steps within the ranking scale.
p values ≤0.05 were considered statistically significant. Because the analyses were primarily exploratory and aimed to characterize reconstruction-dependent changes across the monoenergetic spectrum, no formal adjustment for multiple comparisons was applied. Results should therefore be interpreted with emphasis on the magnitude, consistency, and biological plausibility of the observed effects rather than isolated
p-values. Statistical calculations were performed using IBM SPSS Statistics for Windows, version 28.0 (IBM Corp., Armonk, NY, USA). Intra- and interrater agreement was calculated as a weighted Cohen’s kappa coefficient using MedCalc v. 22.023 software (MedCalc, Ostend, Belgium) and interpreted as suggested by Altman [
15].
4. Discussion
This study demonstrates that virtual monoenergetic images (VMIs) reconstructed from dual-layer detector spectral CT substantially reduce posterior fossa beam-hardening artifacts while preserving, and in several respects improving, overall image quality compared with conventional images. Quantitative analyses showed that image noise and posterior fossa artifact severity decreased progressively with increasing VMI energy, whereas tissue attenuation and the contrast-to-noise ratio (CNR) were the highest at lower energy levels. Qualitative assessment by two neuroradiologists consistently identified VMIs reconstructed at approximately 50–70 keV as providing the best overall image quality. No single reconstruction energy was optimal for every image quality metric. Rather, lower-energy VMIs improved tissue contrast, whereas progressively higher energies reduced image noise and beam-hardening artifacts. Intermediate-energy reconstructions (approximately 50–70 keV) achieved the most favorable overall balance between these competing properties and therefore received the highest overall qualitative ratings.
The assessment of diagnostic adequacy should be interpreted cautiously because only examinations without intracranial pathology were included. Consequently, this endpoint reflects reader confidence in image quality rather than true diagnostic performance. Whether the observed improvements translate into improved lesion detection requires dedicated diagnostic accuracy studies including patients with posterior fossa pathology. The qualitative assessment demonstrated only fair inter-reader agreement for several subjective endpoints, reflecting the inherent subjectivity of image quality assessment and the absence of universally accepted criteria for grading posterior fossa artifacts. Importantly, despite differences in absolute scoring between readers, both observers consistently identified VMIs reconstructed between approximately 50 and 70 keV as providing the most favorable overall balance between artifact reduction and image quality. Thus, the principal qualitative conclusions were supported despite variability in individual scoring behavior. Taken together, these findings indicate that intermediate-energy VMIs achieve the most favorable balance between artifact suppression and preservation of tissue contrast.
Since all examinations were acquired on a single first-generation dual-layer detector spectral CT system using a standardized institutional protocol. Although the physical principles underlying monoenergetic reconstruction are common across spectral CT technologies, different implementations—including dual-source CT, rapid kV-switching systems, and photon-counting CT—differ in spectral separation, reconstruction methodology, and noise optimization. Consequently, while the overall trends observed in this study are likely to be broadly applicable, the precise reconstruction energy providing the optimal balance between artifact suppression, image noise, and tissue contrast may differ between vendors, scanner generations, and acquisition protocols. The present recommendation of approximately 50–70 keV should therefore be interpreted as specific to the investigated dual-layer detector platform until validated on other systems.
The quantitative results illustrate the fundamental trade-off inherent to monoenergetic CT reconstruction. Lower-energy VMIs increase tissue attenuation and improve tissue contrast through greater photoelectric absorption, thereby increasing CNR. However, these benefits are accompanied by increased image noise and more pronounced beam-hardening artifacts. Conversely, increasing the monoenergetic reconstruction energy progressively suppresses beam-hardening artifacts and reduces image noise but at the expense of tissue contrast. These findings are fully consistent with the physical principles underlying dual-energy CT and virtual monoenergetic image reconstruction [
5,
7].
Interestingly, the attenuation difference between cerebellar white matter and the interpetrous pons crossed zero between 60 and 70 keV. This observation reflects the opposing attenuation trends of normal brain tissue and beam-hardening artifacts with increasing monoenergetic energy and provides a quantitative explanation for why intermediate-energy VMIs achieved the highest qualitative ratings.
Our findings are consistent with previous studies demonstrating improved posterior fossa image quality using virtual monoenergetic reconstructions. Investigations using both dual-layer detector CT and rapid kVp-switching DECT have similarly reported reductions in beam-hardening artifacts and improvements in overall image quality compared with conventional images [
8,
9,
10,
16,
17]. However, these studies generally included smaller patient cohorts and evaluated fewer monoenergetic reconstructions than the present study. Compared with previous studies, the present work combines the largest reported patient cohort with comprehensive quantitative measurements across the full clinically relevant monoenergetic spectrum, enabling characterization of how competing image-quality metrics together determine the optimal reconstruction energy.
The quantitative findings also closely paralleled previous observations. As reported by Neuhaus et al. and Pomerantz et al., the posterior fossa artifact index decreased rapidly with increasing monoenergetic energy before reaching a plateau above approximately 100 keV [
8,
9]. In contrast to Neuhaus et al., we observed significant differences between conventional images and VMIs, which likely reflects the greater statistical power afforded by our larger study population.
The attenuation difference between cerebellar white matter and the interpetrous pons crossed zero at slightly lower energies than previously reported by Zhao et al., who observed this transition between 75 and 80 keV [
10]. Given the relatively small attenuation differences involved, together with differences in ROI placement, reconstruction parameters, and post-processing software, these findings are nevertheless highly consistent.
From a clinical perspective, the present findings suggest that routine reconstruction of VMIs at approximately 60 keV may improve evaluation of the posterior fossa without compromising supratentorial image quality. This may be particularly relevant in emergency neuroradiology, where beam-hardening artifacts may obscure small hemorrhages or early posterior circulation infarction and MRI is often unavailable or delayed [
3,
4].
Although our study assessed image quality rather than diagnostic accuracy, the qualitative assessments indicate that intermediate-energy VMIs may increase diagnostic confidence during routine evaluation of the posterior fossa.
Diagnostic performance cannot be established from a cohort consisting exclusively of normal examinations. Nevertheless, the improved image quality observed in the present study is consistent with previous work suggesting improved detection of posterior fossa infarction using VMIs. Hixon et al. reported higher sensitivity for posterior circulation infarction using VMIs than conventional images, although the difference did not reach statistical significance, likely because of the relatively small study population [
18]. Similar improvements have also been shown by using iterative reconstruction algorithms [
19].
Strengths and Limitations
The principal strengths of this study are its comparatively large cohort, comprehensive quantitative evaluation across the full monoenergetic spectrum, and independent qualitative assessment by two experienced neuroradiologists. Together, these enabled evaluation of not only individual image-quality metrics but also the balance between artifact suppression and preservation of tissue contrast that determines overall diagnostic image quality.
There are several limitations of this study.
First, this was a retrospective single-center study performed using a standardized imaging protocol at one tertiary referral center. Although this ensured a homogeneous study population and minimized technical variability, it may limit the generalizability of the findings to institutions using different patient populations, imaging protocols, or scanner settings. Prospective multicenter studies would be valuable to confirm the optimal reconstruction energy across a broader range of clinical settings.
Second, only examinations without intracranial pathology were included. This design allowed for evaluation of reconstruction-dependent image quality without confounding from lesion-related attenuation changes but precludes assessment of diagnostic accuracy. Consequently, although VMIs improved objective and subjective image quality, the present study cannot determine whether these improvements translate into improved detection of posterior fossa infarction, hemorrhage, tumors, or other pathological conditions. Future studies should evaluate diagnostic performance in clinically relevant patient cohorts.
Third, qualitative image assessment was based on subjective Likert-scale ratings. Although this reflects routine clinical image interpretation, subjective image-quality assessment inevitably introduces reader variability. Indeed, the two reviewers differed considerably in their absolute scoring, particularly regarding diagnostic acceptability, despite demonstrating similar trends across reconstruction energies. This suggests that the observed differences primarily reflect individual thresholds for image quality rather than disagreement regarding the optimal reconstruction energy.
Fourth, the study involved multiple comparisons across reconstruction energies and imaging metrics without formal adjustment for multiplicity. Although this increases the possibility of type I error, the principal conclusions were supported by consistent quantitative and qualitative findings across multiple independent image-quality measures.
Fifth, ROI placement was performed manually on the conventional images before automatic propagation to all monoenergetic reconstructions. Although this ensured identical ROI locations across reconstruction energies within each examination, reproducibility of the initial ROI placement was not formally evaluated and may have contributed to measurement variability.
Finally, all examinations were performed on a single dual-layer detector CT platform. Although the physical principles of virtual monoenergetic imaging are shared across DECT technologies, the optimal reconstruction energy may vary somewhat between vendors and reconstruction algorithms. The examinations were acquired using a first-generation dual-layer spectral CT platform and reconstructed using the software version available at the time of the study. Subsequent advances in reconstruction algorithms, iterative reconstruction techniques, and spectral post-processing may alter image noise characteristics and potentially shift the precise reconstruction energy providing the optimal balance between noise and artifact reduction. Nevertheless, the fundamental relationship between monoenergetic reconstruction energy and beam-hardening artifact suppression is expected to remain similar, although confirmation on newer software generations would be valuable.