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Duallayer spectral computed tomography: measuring relative electron density
European Radiology Experimental volume 2, Article number: 20 (2018)
Abstract
Background
Xray and particle radiation therapy planning requires accurate estimation of local electron density within the patient body to calculate dose delivery to tumour regions. We evaluate the feasibility and accuracy of electron density measurement using duallayer computed tomography (DLCT), a recently introduced dualenergy CT technique.
Methods
Two calibration phantoms were scanned with DLCT and virtual monoenergetic images (VMIs) at 50 keV and 200 keV were generated. We investigated two approaches to obtain relative electron densities from these VMIs: to fit an analytic interaction crosssectional model and to empirically calibrate a conversion function with one of the phantoms. Knowledge of the emitted xray spectrum was not required for the presented work.
Results
The results from both methods were highly correlated to the nominal values (R > 0.999). Except for the water and lung inserts, the error was within 1.79% (average 1.53%) for the crosssectional model and 1.61% (average 0.87%) for the calibrated conversion. Different radiation doses did not have a significant influence on the measurement (p = 0.348, 0.167), suggesting that the methods are reproducible. Further, we applied these methods to routine clinical data.
Conclusions
Our study shows a high validity of electron density estimation based on DLCT, which has potential to improve the procedure and accuracy of measuring electron density in clinical practice.
Key points

Duallayer spectral CT provides accurate electron density estimation (error rate < 1.75%)

Virtual monoenergetic images from duallayer CT allow direct calculation of electron densities

Electron densities generated via dualenergy CT have the potential to improve clinical practice
Background
Prior to receiving xray or particle radiation therapy, it is a crucial step for the patient to undergo computed tomography (CT) so that the optimal dose delivery to the tumour can be calculated while reducing unnecessary radiation exposure to surrounding healthy and critical tissue. This treatment planning is generally achieved by the estimation of the corresponding particle and xray absorption properties of the tissue, such as in the form of relative electron density, which is the ratio of electron densities of given materials to the electron density of water.
Conventional singleenergy CT can provide a raw estimation of electron density by simply applying its correlations with Hounsfield units (HU), then categorising the values to electron densities [1, 2]. However, this method is not accurate, because conventional HU values, which are defined by the linear attenuation coefficient, also depend on the effective atomic number and the xray spectrum. Dualenergy CT (DECT), such as dualsource CT (DSCT) or twinbeam CT, improve this estimation by using two different energy spectra [3]. Various studies have demonstrated the accuracy of measuring electron density using DECT [4,5,6,7]. Recently, a detectorbased spectral DECT technique, namely duallayer CT (DLCT), was introduced [8]. This technology allows the acquisition of energyselective projection data in the two detection layers simultaneously and therefore directly generating spectral information for each CT scan without the need to select specific protocols [8]. Compared with DSCT, DLCT seems to be superior in generating highly accurate virtual monoenergetic images (VMIs) [9, 10] to recognise different materials and to quantitate elemental decompositions, such as intravenous contrast agents or bone mineral density [11,12,13], which may be of great benefit when estimating electron densities.
There are several ways to approximate electron density. With DECT, the physical interaction crosssectional model has been applied to dualenergy data [4,5,6,7], resulting in a significant improvement in accuracy compared with singleenergy CT [3]. However, these methods require exact knowledge of the spectra of the two xray beams in the DECT scanner to parameterise the physical interaction mechanisms, so that the accuracy relies largely on the precision of the assumed xray spectra. Conversely, calibration methods generate a specific empirical conversion function from measured HU values at two xray spectra to relative electron densities by fitting data from known phantoms to their known electron densities [14]. This method does not require beam spectra, but is limited to a specific calibrated scanner model and acquisition protocol.
In this article, we describe both methods, fitting crosssectional models and phantomcalibrated conversion functions to DLCT. Our aim was to access relative electron densities from VMIs of DLCT and to quantify their accuracy.
Methods
CT phantoms, scan protocols and image reconstruction
Two different CT phantoms were used: a Gammex phantom (467TOMO; Gammex RMI, Middleton WI, USA) (Fig. 1) and a Catphan phantom (Catphan 504; The Phantom Laboratory, Salem NY, USA) (Fig. 2). The Gammex phantom contains 12 inserts representing tissueequivalent materials with various known electron densities. Each insert is cylindrical, with a diameter of 30 mm and a length of 70 mm. The Catphan phantom has six homogeneous regions consisting of common materials with known electron densities; each region is a cylinder with a 12.5mm diameter and a length of 25 mm.
Scans were conducted with a DLCT unit, the IQon Spectral CT (Philips Healthcare, Best, the Netherlands). Similarly to the acquisition protocols applied in clinical routine, Gammex and Catphan phantoms were scanned with an xray source voltage of 120 peak kilovoltage (kVp), a collimation width of 0.625 mm, a revolution time of 1.5 s and a spiral pitch factor of 0.983. We made four levels of xray tube currents, which were 229, 153, 77 and 56 mA, resulting in xray exposures of 350, 234, 117 and 86 mA, respectively, and the corresponding volume CT dose index (CTDI_{vol}) of 30, 20, 10 and 7.5 mGy was recorded in the dose reports.
The spectral data were reconstructed with an iterative reconstruction at vendorspecific level 2 and a standard filter B, according to the settings used in most clinical abdominal examinations. The field of view was 360 mm, and the slice thickness was 0.8 mm. Corresponding VMIs were generated by using vendorspecific spectral software (IntelliSpace Portal v10.1; Philips Healthcare) at 50 and 200 keV. We used these two monoenergetic levels because at 50 keV the photoelectric effect and at 200 keV the Compton effect are the dominant xray interactions with matter. Regions of interest were drawn as cylinders with half of the radius and height of the actual insert dimension, and the mean HU values were measured. Regions of interest were synchronised between VMIs, and the measurements were repeated using imageprocessing software (ImageJ v1.50f; National Institutes of Health, Bethesda, MD, USA) [15].
Electron density estimation using crosssectional model
In order to obtain electron density values using the crosssectional model, the energydependent CT numbers HU(E) in the corresponding VMI were firstly converted into the massattenuation coefficients μ(E)/ρ at the specific energy using the following equation:
where μ_{w}(E)/ρ_{w} is constant representing massattenuation coefficient of water at energy E, which can be referenced from the National Institute of Standards and Technology database [16].
In an ideal case of a narrow beam of monoenergetic photons in the range of clinical CT (E < 511 keV), the massattenuation coefficient μ(E)/ρ can be attributed to three physical interaction mechanisms: photoelectric absorption, incoherent (Compton) scattering and coherent (Rayleigh) scattering. For the energy range used in clinical CT, coherent scattering can often be neglected for standard body tissues, resulting in the wellknown twodimensional parameterisation for the massattenuation coefficient [17, 18]:
where a_{p} and a_{c} are characteristic parameters for the different materials in the image. f_{p} and f_{c} are the energy dependencies of photoelectric absorption and Compton scattering. The photoelectric absorption part is approximated as:
where ρ_{e} is the absolute electron density (e/cm^{3}), and Z is the effective atomic number. C_{p} is constant and equals 9.8 × 10^{− 24} [18]. E is the energy of the xray beam measured in kiloelectron volts. For a numerical fit of the experimental data, m is between 3 and 4, and n is between 3 and 3.5. In this study, we use m = 3.8, n = 3.2 [4].
The Compton effect can be approximated with electron density and the total KleinNishina crosssection [19]:
where E is the xray energy and has the unit of kiloelectron volts, and r_{0} is the classical electron radius, which equals to 2.818 × 10^{− 13} cm.
If we substitute Eqs. (3)–(5) into Eq. (2), we obtain:
The two unknown variables ρ_{e} and Z in Eq. (7) can be obtained by the acquisition of two VMIs at distinct energy levels and then analytically solving the resulting set of equations. To maximise the difference between two VMIs and thus improve the accuracy of the solution, we use energy levels at 50 keV and 200 keV. Absolute electron densities can then be converted to relative electron density using known water electron density (3.343 × 10^{23} e/cm^{3}).
Electron density estimation using calibrated conversion function
We used the Gammex phantom to fit a conversion function from HU values measured in two VMIs to relative electron densities. A scan is taken using a relatively high radiation exposure (30 mGy) to acquire almost noisefree calibration images of the phantom at 50 keV and 200 keV. HU values at these two energies are used to fit Saito’s conversion function [14]:
where ρ_{e} is the actual relative electron density taken from the phantom’s data sheet, HU_{H} and HU_{L} are HU values in the VMIs at 50 keV and 200 keV, and a, b, α are parameters specific to the scanner.
The Gammex phantom consists of twelve materials with known pairs of (ρ_{e}, HU_{H}, HU_{L}), and there were three unknown parameters (a, b, α) in the equation; this fitting was computed using MATLAB software (v9.2; MathWorks, Natick MA, USA) and a surfacefitting algorithm. The fitting results were then used to compute relative electron densities of the Catphan phantom containing six materials in varied dose scans.
Error measurement
To describe measurement errors, we computed the percentage error (%Error) as the ratio of the difference of the estimated value (ρ_{e}) to the nominal value of the relative electron density (ρ_{n}):
and ρ_{e} − ρ_{n} is noted as absolute error. The overall estimation error is assessed using root mean square error (RMSE) and normalised root mean square error (NRMSE):
To assess correlations between the estimated values and the nominal values, the Pearson correlation R was used. In addition, linear regression analysis was performed as fitting:
where β and ϵ are regression coefficients (slope and intercept). Coefficient of determination, which describes the goodness of the fit, is noted as R^{2}. Analysis of covariance (ANCOVA) was performed for the measurement against the group where \( {\rho}_e^{\prime }={\rho}_n \), which indicates an ideal measurement. Moreover, a paired t test was performed for the measurement against the nominal values.
In order to assess the reproducibility of the estimation and the influence of different radiation exposures, Pearson correlation, RMSE, and NRMSE between measurements and nominal values were computed. A paired t test was performed for measurements between the highest dose (30 mGy) and lowest dose (7.5 mGy). All error estimation and statistical analyses were performed using MATLAB software.
Results
For Lehmann’s crosssectional model, relative electron densities estimated for the Gammex phantom and the Catphan phantom were highly correlated to the nominal values (R = 0.9993, p < 0.001) in the scan with a standard dose (20 mGy) (Tables 1 and 2; Fig. 3). Linear regression analysis also suggested that the result was very close to nominal value: with the slope β and goodness of fit R^{2} very close to 1, and intercept ϵ very close to 0: β = 1.0028, ϵ = 0.0063, R^{2} = 0.9986. ANCOVA suggested the measurement had no statistically significant difference from an ideal measurement (p = 0.768 for β; p = 0.557 for ϵ). The overall NRMSE was 1.53%. The maximum increase related to water is + 0.021 (cortical bone), and the maximum decrease was − 0.036 (water). If we exclude one of the lungequivalent inserts (LN 300) and the water insert, all percentage errors are less than 1.79%. The largest percentage error (− 6.82%) was found in the LN300; owing to the low attenuation of this insert, the small actual electron density (0.264) resulted in larger percentage errors. Nevertheless, the absolute error for LN300 was − 0.020 and was actually comparable to that of the other inserts. The water insert had the largest absolute error (+ 0.036) compared with all the measurements. A paired t test showed the difference between measured electron densities from Lehmann’s model, and nominal values for the Gammex phantom were not statistically significant (p = 0.212). The relative electron densities for the Catphan phantom obtained with Lehmann’s model were all higher than their nominal values (p = 0.001) (Table 1).
For Saito’s calibrated conversion function, the fitting result from a single scan of the Gammex phantom (n = 12) at a relatively high radiation dose (30 mGy) was a = 0.9704, b = 0.9874 and α = − 0.02104 for Eq. (8). To validate this fitted conversion function, we computed the relative electron densities for the Gammex and Catphan phantom scans at a standard radiation dose (20 mGy). In Fig. 4, strong correlation to the exact values was observed (R = 0.9997, p < 0.001). Regression analysis also indicated that the measurements were quite accurate (β = 0.9952, ϵ = 0.0016, R^{2} = 0.9995). ANCOVA also suggested that the measurement showed no significant difference from an ideal measurement (p = 0.412 for β, p = 0.813 for ϵ). The overall error was 0.87%. Compared with the results of the fitted crosssectional model, a higher error was also observed in the case of water (+ 1.92%) and lung inserts (− 3.41%). If we exclude these inserts, the fitted percentage errors are all under 1.61% (see Table 1). Similar to the crosssectional model, the measured electron densities with Saito’s method for the Gammex phantom showed no significant difference from the nominal values (p = 0.969). The relative electron densities for the Catphan phantom obtained with Saito’s method were all below the nominal value provided by the manufacturer (p = 0.015) (Table 1).
Only subtle influences from different radiation exposures were observed in the measurement. Table 2 shows the RMSE, NRMSE and correlation coefficients between the nominal values and the estimated values for all exposures (30, 20, 10 and 7.5 mGy). The computed relative electron densities between the highest and lowest doses did not show significant changes (p = 0.348 for Lehmann’s model, p = 0.167 for Saito’s function). On this note, the relatively small effect of different radiation dose levels can also be accounted for by the size of the employed phantoms.
A patient scan applying the relative electron density estimations with Lehmann’s crosssectional model and Saito’s conversion function is shown in Fig. 3. Both methods have no significant visual differences when depicting tissue with different electron densities.
Discussion
In this paper, we have illustrated that it is feasible to compute relative electron densities from DLCT acquisitions and that the results for two different phantoms are accurate and reliable. In both methods, we used VMIs while actual xray source spectra and detector response information were not required. The measured and nominal values were highly statistically correlated.
For both methods, we observed that a relatively high error appeared in two lung inserts and in the water insert of the Gammex phantom. Previous studies have observed similar inconsistencies with lung inserts and recommended to exclude them [20]. This may be caused by the inhomogeneity of the phantom composition, which is actually thin plastic with small air bubbles as compared with other phantoms based on uniform resin. In our study, higher discrepancy of relative electron density for the water insert was also observed. It is highly likely that in contrast to pure water, which contains mainly hydrogen and oxygen, the material used in the phantom also included certain other substances for solidification. Therefore, manufacturing tolerances may need to be considered. Interestingly, discrepancy in previous studies involving oldergeneration Gammex phantoms for the brain and adipose phantom was not observed [14].
DECT offers VMIs, which mimic CT images as if the xray source is monochromatic. However, real monoenergetic images could be generated only via more advanced image equipment such as a synchrotron [21, 22], which is currently not realistic in a clinical environment. As a result, the crosssectional model and the VMIs are only approximations. Nevertheless, VMIs estimated from DLCT illustrated much higher accuracy than other DECT solutions [10]. On this note, the application of the crosssectional model used in DECT was limited to a certain range of atomic numbers of the materials and could introduce errors for hydrogen (Z = 1) and higherdensity elements (Z > 30) [4, 5]. In previous studies with DSCT, the estimation of electron density with images at two energies based on a crosssectional model was not simple, because it involved a lot of data, such as xray beam spectrum and detector corrections. The errors ranged between 1.8% ± 1.6% [5] and 2.3% [6], which are slightly higher than our result (1.53%). The highly correlated result for relative electron density approximation in our study showed that the fitting crosssectional model is feasible and that the VMIs are highly reliable.
Recently, Almeida et al. [20] investigated the accuracy of relative electron density calculations for DSCT and twinbeam CT, showing high correlations. Similar to our work, Saito’s conversion method was applied for multiple scanners. The investigators observed percentage errors of 1.2% for DSCT and 3.2% for a twinbeam scanner, excluding lung inserts. In contrast to their approach of excluding inhomogeneous lung phantom for calibrating, we also included these materials in our calibration. Nevertheless, in our study we observed that relative electron densities could be measured within 1.61%.
Saito’s conversion function was originally proposed for DSCT with dualkVp scans. In our study, we applied this method directly to VMIs from DLCT without additional modifications. This conversion method has the advantage that no exact spectral information of the xray source is required, meaning that any VMIs in two different energies can be directly applied. According to the original author, a larger spectral separation between the dualkVp scans led to a smaller α. In our case, we used very low and very high VMIs (50 and 200 keV, respectively), instead of two energy scans in DSCT (xray source peaks at 80 kV and 140 kV). We found an extremely low α (− 0.02104) compared with 0.778 and 0.35 in previous studies [14, 20]. This illustrates the highly competitive spectral performance of the DLCT.
Our study has limitations. First, we did not investigate the effect of different reconstruction methods. We assumed that image filters and advanced iterative reconstruction algorithms can only improve the appearance of the image, but not change the quantitative HU values. Instead, we made scans with different radiation exposures and proved that the methods were still reliable and reproducible across different scans. Second, our study was limited to some degree to the actual phantoms and manufacturing errors needed to be considered. The actual resinbased materials used in the phantom were different from the actual composition of human organs or were insufficient to represent biological materials. Nevertheless, we compared phantoms from two independent manufacturers and showed that the electron density estimation was reliable.
In conclusion, we report an experimental evaluation of relative electron density estimations in DLCT. Our investigation demonstrates that DLCTbased VMIs can be used to estimate relative electron density and that the results are accurate. In the future, DLCT can potentially enhance the workflow of radiation therapy planning by providing spectral data for every scan.
Abbreviations
 ANCOVA:

Analysis of covariance
 CDTI_{vol} :

Volume computed tomography dose index
 CT:

Computed tomography
 DECT:

Dualenergy computed tomography
 DLCT:

Duallayer computed tomography
 DSCT:

Dualsource computed tomography
 HU:

Hounsfield units
 kVp:

Peak kilovoltage
 LDPE:

Lowdensity polyethylene
 NRMSE:

Normalised root mean square error
 PMP:

Polymethylpentene
 RMSE:

Root mean squared error
 VMI:

Virtual monoenergetic image
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Data obtained or analysed during this study are included in this published article.
Funding
We acknowledge the support provided by the German Research Foundation (DFG) within the Research Training Group GRK 2274 and by the German Department of Education and Research (BMBF) under grant IMEDO (13GW0072C).
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All authors contributed to the literature research. KM, SE, DP, AAF, FP, SEC, JJW, EJR and PBN conceived of and designed the study. KM, SE, MO and FKK performed the experiments. KM, SE and FKK performed the statistical analysis. All authors edited the manuscript. KM, SE and PBN are guarantors of the integrity of the entire study. All authors reviewed and approved the final manuscript.
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Institutional Review Board approval was obtained (Ethikkommission der Fakultät für Medizin der Technischen Universität München, Munich, Germany). Written informed consent was obtained from the patient in this study.
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Mei, K., Ehn, S., Oechsner, M. et al. Duallayer spectral computed tomography: measuring relative electron density. Eur Radiol Exp 2, 20 (2018). https://doi.org/10.1186/s4174701800518
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DOI: https://doi.org/10.1186/s4174701800518