Abstract
The x-ray detector is a fundamental component of a CT system that determines image quality and dose efficiency. Until the approval of the first clinical photon-counting-detector (PCD) system in 2021, all clinical CT scanners used scintillating detectors, which do not capture information about individual photons in the two-step detection process. In contrast, PCDs use a one step process whereby x-ray energy is converted directly into electrical signal. This preserves information about individual photons such that the numbers of x-rays in different energy ranges can be counted. Primary advantages of PCDs include the absence of electronic noise, improved radiation dose efficiency, increased iodine signal and the ability to use lower doses of iodinated contrast material, and better spatial resolution. PCDs with more than one energy threshold can sort the detected photons into two or more energy bins, making energy resolved information available for all acquisitions. This allows for material classification or quantitation tasks to be performed in conjunction with high spatial resolution, and in the case of dual-source CT, high pitch or high temporal resolution acquisitions. Some of the most promising applications of PCD-CT involve imaging of anatomy where exquisite spatial resolution adds clinical value. These include imaging of the inner ear, bones, small blood vessels, heart, and lung. This review describes the clinical benefits observed to date and future directions for this technical advance in CT imaging.
MeSH key terms: Tomography, X-Ray Computed, Radiation Dosage, Humans, Photons, Iodine
Introduction
The beneficial characteristics of photon-counting detectors (PCDs) relative to energy-integrating detectors (EIDs) include the absence of electronic noise, increased iodine signal-to-noise-ratio (SNR) due to equivalent weighting of low- and high-energy photons, the ability to decrease detector pixel size without loss of radiation dose efficiency, the ability to bin photons according to their respective energies to facilitate multi-energy applications, and the ability to differentiate high atomic number contrast agents having sufficiently different k-edges (e.g., iodine versus gadolinium or bismuth). These and other technical characteristics are reviewed in part one of this review [1], which explains the physical basis for the improvements in image quality and dose efficiency. In this work, we review how the technical characteristics of PCDs have been translated into the clinic to improve diagnostic capabilities, improve radiologist confidence, and benefit patients.
The first human images from PCD-CT were acquired in 2007 using a proof-of-concept PCD-CT system manufactured by General Electric [2]. In 2015, human studies commenced on an investigational dual-source CT system manufactured by Siemens Healthcare [3–5]. The focus of these early clinical studies was to demonstrate the hypothesized benefits of PCD-CT in humans. An investigational human system was developed by Philips Healthcare [6], as well as a second research system from Siemens [7; 8]. Collectively, the studies performed using these systems provided convincing evidence that the anticipated benefits to CT imaging from the use of PCDs could be realized in patients.
In 2021, the first PCD-CT system approved for clinical use was released (NAEOTOM Alpha, Siemens Healthcare) [9]. In 2022, Neurologica announced U.S. FDA 510k clearance of a PCD system for head scanning, the OmniTom Elite. Other CT manufacturers have presented data from prototype PCD systems, which are still in the development or evaluation phase.
Improved Image Quality and Associated Clinical Benefits
Noise
Electronic noise, which can become significant when the signal to the detector is very low, is absent in PCD-CT [1; 10]. This is particularly beneficial for low-dose and quantitative applications. For example, using low-dose PCD-CT, Symons et al. found increased CT number accuracy and stability [11] and lower image noise compared with EID-CT performed using the same radiation dose, while achieving better diagnostic quality and lung nodule contrast-to-noise ratio (CNR) [12].
Radiation dose
Because PCDs do not require septa within the detector layer, as do EIDs, they are inherently more dose efficient. Leng et al. [13] demonstrated that PCD-CT can achieve the same spatial resolution (slice thickness and in-plane resolution) and image noise as EID-CT using a lower radiation dose, as have other investigators [14–18].
Iodine enhancement
The increased enhancement of iodine that occurs with PCD-CT allows for lower volumes of iodinated contrast. This is due to photon counting’s equal weighting of all photon energies (as compared to EID-CT, where the iodine-information-carrying lower-energy photons produce lower detector signal than the higher-energy photons that carry little iodine information). Sawall et al. estimated that a reduction in iodinated contrast volume of up to 13–37% is feasible, with the greatest reduction seen in larger patient sizes [19]. Further, low-energy virtual monoenergetic images (VMIs), which are available for any PCD-CT acquisition using 2 or more energy thresholds, increase iodine signal, enable use of lower doses of iodinated contrast media, and can help salvage suboptimal enhanced vascular studies due to the higher iodine signal [20]. In the absence of reduced doses of iodinated contrast, subtle CT number differences between pathologies are better demonstrated with PCDs owing to the increased iodine signal associated with the equal weighting of low energy photons.
Spatial resolution
The increased spatial resolution of PCD-CT is attractive for most organ systems and radiology subspecialities, including
Multi-energy imaging
In EID-CT, quantitative imaging is available using dual-energy acquisitions in specific modes or configurations [34; 35]. PCDs with more than one energy threshold can sort the detected photons into two or more energy bins, making energy-resolved information available for all acquisitions. This multi-energy information can be used to produce images that help distinguish material types and quantify their mass densities. For instance, multi-energy PCD-CT data can be decomposed into iodine maps to quantitate iodine concentrations [36], e.g., within hyper-enhancing lesions [37]. In addition, the x-ray energy discriminating capabilities of PCDs allow for K-edge imaging of high-atomic-number contrast agents (e.g., bismuth, tungsten, gadolinium) by setting the acquisition energy thresholds around the k-edge energies [38].
While many multi-energy applications are similar to dual-energy CT, dual-source PCD-CT permits multi-energy imaging at high pitch (e.g., 3.2) or high temporal resolution (e.g., 66 ms), which are not possible with dual-source EID-CT. However, as high spatial resolution image reconstruction kernels increase image noise, multi-energy reconstructions with these kernels may be of limited value due to the increased noise associated with multi-energy processing.
Metal artifacts and beam hardening
Higher-energy x-rays better penetrate metal and are subject to less beam hardening and scatter. Thus, PCD-CT’s ability to produce images derived from only the higher energies of the x-ray beam (e.g., high-energy threshold images) allows for decreased metal artifacts and beam hardening, which is advantageous for imaging around dense structures or devices such as stents, coils, dental amalgam, or orthopaedic hardware [18]. When combined with dedicated x-ray beam shaping techniques such as pre-patient filtration (e.g., 0.4 mm tin), the low-energy photons that are most affected by beam hardening are filtered out of the x-ray spectrum while also increasing the dose efficiency of the acquisition [39].
VMIs and material decomposition are alternative multi-energy visualization techniques that may result in effective correction of metal artifacts. Importantly, these multi-energy methods are fully compatible with sinogram-based metal artifact reduction algorithms [40].
Organ-system-specific benefits
The body of literature demonstrating clinical benefits from PCD-CT for specific imaging tasks continues to grow. The following sections highlight studies specific to various organ systems.
Neurologic imaging
Using theoretical simulations and benchtop experiments with an anthropomorphic cerebral angiographic phantom, Harvey et al. demonstrated that compared with EID-CT, PCD-CT provided superior vessel conspicuity and reduced artifactual stenoses [21]. In human studies, Symons et al. performed vascular imaging of the head and neck [22] on sixteen asymptomatic subjects using both EID-CT and PCD-CT. PCD-CT image quality scores were significantly higher compared to EID-CT and PCD-CT demonstrated lower image noise and less image artifacts.
In high-spatial-resolution, non-contrast imaging of the temporal bones, both cadaveric and human subject studies demonstrated superior visualization of critical anatomic structures [23; 24]. For example, stapes prostheses that were barely visible at EID-CT were well visualized at PCD-CT. Further, the addition of a tin filter in the beam resulted in dose reductions of up to 85% for imaging of the temporal bone and sinuses [17; 18]. While the use of a tin filter is not unique to PCD-CT, it is synergistic with PCD’s equal weighting of all photon energies; the lower energy photons that are detected are not “down-weighted” as they are in EID-CT. Campeau et al. have recently demonstrated that PCD-CTA can display many small periorbital vessels, which are difficult to appreciate at conventional CT [41].
Thoracic imaging
In a study by Inoue et al., who assessed 30 patients with known or suspected interstitial lung disease (ILD) with both an EID-CT system and a PCD-CT, PCD-CT significantly increased reader confidence for the presence or absence of imaging findings of reticulation, ground-glass opacity and mosaic attention, all of which contributed to more accurate categorization of ILD [42]. The use of smaller detector pixels on PCD-CT has been shown to improve the conspicuity of ILD and small bronchi. Alternatively, Jungblut et al. have shown that sensitivity for ILD detection can be maintained despite substantial radiation dose reduction [15]. Similarly, PCD-CT permits radiation dose reduction for contrast-enhanced chest CT while improving contrast-to noise ratio for vessels, pulmonary parenchyma, and pulmonary metastases [14].
With the simultaneous acquisition of high spatial resolution and multi-energy data, PCD-CT allows quantitative display of pulmonary blood pool within the lungs as a complement to the high-resolution anatomical information in patients with suspected acute or chronic pulmonary embolism [43]. As the size of the detector readout pixel is decreased, the rate of data coming from the detector increases, requiring higher data transfer speeds. In some cases, if the maximum bandwidth is exceeded, trade-offs may be required in other aspects of the acquisition, such as longitudinal beam coverage.
Cardiovascular imaging
PCD-CT is particularly advantageous in cardiovascular imaging for the visualization of small vessels [27; 28]. The improved spatial resolution also reduces calcium blooming artifact [29], improving luminal assessment adjacent to dense calcifications and within stents (Fig. 3a–b) [28; 30]. It is anticipated that this will help in the characterization of atherosclerotic plaques [28; 44].
Dual-source CT with EIDs permits either dual-energy or 66 ms temporal resolution imaging; they cannot, however, be performed simultaneously. In dual-source PCD-CT, 66 msec, multi-energy scanning is possible, which allows for material decomposition to remove calcium signal [45] (Fig. 3c–d) to help improve luminal assessment in the presence of dense calcium. High-energy VMIs, e.g., 100 keV, can also be used to decrease artifacts such as from calcium blooming, beam hardening, or metal [46]. Simultaneous use of multi-energy information is also useful in cardiac CT to generate iodine maps reflecting parenchymal perfusion, e.g., delayed iodine CT for myocardial scar, or to calculate extracellular volume [27]. Finally, in work by Symons et al, multi-contrast imaging of the heart has been investigated [47] in a canine model.
Abdominopelvic imaging
In Decker et al., 20 patients with clinically indicated low-dose CT were scanned on a PCD-CT and their images compared with those from a BMI-matched EID-CT-cohort [48]. Image noise was found to be significantly lower and iodine SNR was significantly higher at PCD-CT. Subjective image quality was substantially higher and conspicuity better for the renal pelvis, ureters, and mesenteric vessels on the PCD-CT. There was no significant difference in the conspicuity of the adrenal glands [48]. Higashigaito et al. showed that PCD-CT low energy (50 keV) VMIs resulted in higher iodine CNRs at similar subjective image quality as compared to EID-CT using identical radiation doses [49]. Similar results have been attained within other abdominal tasks, such as detection of peritoneal carcinomatosis where visualization of small peritoneal or serosal deposits is enhanced using PCD-CT (Fig. 4a–c). Through the substantial increase in iodine CNR, PCD-CT has notable relevance in efforts to achieve similar diagnostic-quality images with reduced radiation [48] or iodine doses.
PCD-CT also holds potential for improved urolithiasis detection and characterization. Marcus et al. [50] showed that PCD-CT improved the detection and characterization of stones smaller than 3 mm compared to dual-energy EID-CT. These results can have clinical management implications, e.g., when an apparent single stone at EID dual-energy CT was instead shown to be two smaller stones when imaged using PCD-CT (Fig. 4d–e). Mergen et al. have demonstrated reasonable diagnostic quality in virtual non-contrast (VNC) images relative to true non-contrast images and suggest the elimination of true non-contrast phases in the abdomen and pelvis [51].
An important consequence of multi-energy imaging is the availability of VMIs; not only can the iodine signal be increased but the CT numbers can be standardized. This may be of benefit for follow up studies, where use of the same photon-energy-level VMI can standardize the iodine enhancement, regardless of scanner make, model, or scan acquisition parameters, in addition to highlighting key imaging findings for many tasks in abdominopelvic CT due to improved iodine signal (Fig. 4f–g), similar to the use of VMIs at dual energy CT [52–55]. Because abdominopelvic CT is generally performed within a single breathhold, PCD-CT acquisition is more difficult at the thinnest collimation (120 × 0.2 mm) on the Siemens scanner, so it is generally performed with a more routine collimation (144 × 0.4 mm).
Musculoskeletal imaging
Bette et al. compared the visualization of bone details in mice specimens between PCD-CT and EID-CT [32]. In dose-matched scans, PCD-CT showed significantly lower image noise, higher bone SNR, and higher edge sharpness than EID-CT [32]. Similar results have been observed in human specimens [16; 33] and patients [16; 31] demonstrating improved visualization of cortical and trabecular architecture (Fig. 5). Some conventional EID-CT systems use dose-inefficient comb- or grid-filter based techniques for acquiring high-resolution images [56]; however, high resolution images of larger joints such as the shoulder and hips are not possible due to tube power limits and the dose penalty of these modes. With PCD-CT, ultra-high spatial resolution (e.g., 125 microns) CT images can be obtained of large body parts such as the shoulders, pelvis, and spine [31]. For smaller body parts, radiation dose will be substantially decreased owing to acquisition of images without the post-patient comb- or grid-filter [16]. The improved spatial resolution of PCD-CT has been shown to result in improved confidence in evaluation of critical anatomic strictures for large and small joints, as well as multiple myeloma lesions [16; 31; 57].
With EID dual-source CT systems, the user must choose between obtaining a high-resolution image in single-energy mode to detect subtle fractures or operating the scanner in dual-energy mode to generate virtual non-calcium images, which allow visualization of bone marrow edema that may signal an acute/subacute fracture [58]. Dual-source PCD-CT eliminates this quandary. Concurrent high spatial resolution imaging with multi-energy data is also beneficial in the work up of intraarticular and periarticular pathology with CT arthrography. With one CT acquisition, high-resolution VNC images can be generated to develop 3D bone models, without the need for a non-contrast CT arthrographic exam. PCD-CT may also be of value in the quantitative assessment of cartilage health [59] or bone mineral density [60]. Improved assessment of bone lesions has also been shown [61; 62].
Pediatric imaging
Cao at el. [63] published clinical examples of the use of PCD-CT in children, demonstrating the ability to reduce both radiation [64] and iodine doses. High pitch (e.g., 3.2) dual-source CT for scanning of pediatric patients has previously been shown to result in acceptable image quality without the need for sedation [65]. With dual-source PCD CT, high pitch imaging can be performed for multi-energy applications, making VMIs available at energy levels selected to match the diagnostic task. One promising application of ultra-low dose CT is in the work-up of non-accidental trauma. Currently, the guidelines for the imaging work-up of non-accidental trauma set by the American College of Radiology and Society for Pediatric Radiology offer chest CT as a secondary tool when there is high clinical suspicion for abuse, but the radiographic skeletal survey is negative for fracture [66]. Fractures related to abuse can be missed on radiographs, as they are often subtle and equivocal in appearance. PCD-CT may help to detect these fractures at effective dose levels similar to a two-view chest radiograph (Supplemental Fig. 1). The use of PCD-CT to quantify cystic fibrosis in children has also been suggested [67].
Future Directions
Ultra-high-resolution imaging of the breast (e.g., breast microcalcifications)
Dedicated breast CT systems are commercially available, although their use is relatively limited at this time. One such system (nu:view; AB-CT GmbH) uses a photon counting detector [68; 69]. However, breast CT performed with whole-body CT scanners has generally not been used for diagnostic breast imaging due to limitations in spatial resolution, excessive image noise, and radiation dose considerations. With the advent of whole body PCD-CT, ultra-high-resolution breast CT imaging may be possible using whole-body systems with radiation doses similar to a chest CT exam [70]. With addition of dedicated deep learning-based CT image denoising algorithm, breast microcalcifications can be visualized (Fig. 6). The use of intravenous contrast allows assessment of iodine distribution within the breast tissue and can identify abnormal areas of breast enhancement. With the ultra-high spatial resolution mode, architectural distortion, masses, and microcalcifications can be potentially visualized at higher spatial resolution and specificity than seen on breast MR.
Quantitative CT
The ability of PCD-CT to quantify the mass densities of native tissue types and novel contrast agents based on their x-ray attenuation characteristics could enable a range of novel diagnostic and theragnostic applications. In a preclinical study, Cormode et al. [71] showed the utility of a macrophage-targeted gold-core nanoparticle (Au-HDL) to image the composition of atherosclerotic plaque in a mouse model. The authors were able to distinguish Au-HDL nanoparticles from iodine, soft tissue and calcium and confirm Au-HDL uptake in the plaque region with high macrophage activity. While dual-contrast techniques and targeted nanoparticle-based imaging using high-atomic-number contrast agents and PCD-CT are exciting, there are considerable challenges that need to be addressed before such techniques become clinically adopted. The largest barrier to clinical use is the lack of FDA-cleared high-atomic-number contrast agents other than iodine and gadolinium.
Simultaneous multi-contrast imaging
Simultaneous imaging of two or more contrast agents using one single multi-energy acquisition has been proposed for PCD-CT [47; 72–77] to generate a quantitative map of each contrast agent that corresponds to a particular physiological contrast phase. One example is to acquire bi-phase liver images in one single PCD-CT scan after sequential injection of iodine and gadolinium-based agents [73; 74]. With appropriate injection and scan timing, iodine enhancement can correspond to the late arterial phase and gadolinium enhancement can correspond to the portal-venous phase. Simultaneous imaging of iodine and gadolinium has also been proposed in biphasic kidney imaging [76], CT colonography [78], or cardiac imaging [47]. Another example is small bowel imaging using both intravascular iodine for arterial enhancement in the vascularized bowel wall and enteric bismuth for enhancement of the intestinal lumen [75]. However, the dose efficiency of simultaneous imaging of multiple contrast agents has been shown to be worse than that of a two-scan bi-phase exam due to the substantial increase in image noise from the material decomposition process [79]. This decreased dose efficiency is partially due to spectral distortions caused by many physical non-idealities of the PCD [80]. Charge summing [81], coincidence counting [82; 83], or software corrections [84; 85] for these non-ideal effects may further improve the material-specific imaging performance and improve the radiation dose efficiency. In addition, many noise reduction algorithms have been developed for material decomposition, which may also be used to control the noise and improve the quantitative results.
Summary and conclusions
PCD-CT offers numerous technical advantages over conventional EID-CT systems, fundamentally due to its different approach to x-ray detection. The promising early investigations into PCDs have led to the culmination of clinical PCD-CT systems, with high-spatial resolution, improved contrast-to-noise ratio, improved radiation dose efficiency, and the routine availability of multi-energy capabilities as notable technical features that can substantially enhance diagnostic CT. While conventional EID systems offer high spatial resolution imaging for smaller body parts, PCD-CT extends this benefit to all body parts and across a range of diagnostic tasks. Similarly, the benefits of multi-energy imaging can now be combined with dual-source high temporal resolution and high pitch imaging. High spatial resolution combined with multi-energy imaging at PCD-CT can be used to reduce calcium bloom and metallic artifacts, which often limit diagnostic assessment. We anticipate that in coming years, the improved visualization of key anatomic features, reduction of artifacts, and simultaneous multi-energy capabilities will result in improved clinical outcomes for specific diagnostic tasks. The improved diagnostic information available with higher spatial resolution at lower radiation doses is expected to expand the information provided by these exams and result in new types of exams performed routinely with CT.
Supplementary Material
Key points:
Beneficial characteristics of photon-counting detectors include absence of electronic noise, increased iodine signal-to-noise-ratio, improved spatial resolution, and full-time multi-energy imaging.
Promising applications of PCD-CT involve imaging of anatomy where exquisite spatial resolution adds clinical value and applications requiring multi-energy data simultaneous with high spatial and/or temporal resolution.
Future applications of PCD-CT technology may include extremely high spatial resolution tasks, such as detection of breast micro-calcifications, and quantitative imaging of native tissue types and novel contrast agents.
Abbreviations:
- PCD
photon counting detector
- EID
energy integrating detector
- SNR
signal to noise ratio
- CTA
CT angiography
- VMI
virtual monoenergetic image
- VNC
virtual non-contrast
- ILD
Interstitial lung disease
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