Background
Hepatocellular carcinoma (HCC) is the most common primary liver cancer that develops from liver cells. It is the seventh most common cause of cancer worldwide and the second most common cause of cancer death [
1]. Many treatments are used (from surgery to palliative treatment), selected according to the BCLC (Barcelona Clinic Liver Cancer) recommendations. Radioembolization is one option for treatment that has recently been introduced in the BCLC classification for early-stage patients [
2].
The products currently approved for clinical use are glass microspheres (TheraSphere®, Boston Scientific), resin microspheres (SIR-Sphere®, SIRTEX Medical), both labeled with yttrium-90 (
90Y), and polyglycolic acid-co-dl-lactic acid) (PGLA) microspheres labeled with holmium-166 (
166Ho) (QuiremSpheres™, Terumo). The physicochemical characteristics of these different microspheres vary very slightly in diameter, but their main difference is their range of activity per microsphere, which is summarized in Table
1.
Table 1
Characteristics of products based on radioactive microspheres available in Europe for the treatment of liver tumors as of the first quarter of 2023
Microsphere diameter | 15–35 µm | 20–60 µm | 15–60 µm |
Material | Glass | Resin | Poly(glycolic acid-co-dl-lactic acid) |
Isotope | Yttrium-90 | Yttrium-90 | Holmium-166 |
Activity per microsphere | 70–2500 Bq | 50–150 Bq | 450 Bq |
Approved area | Asia, Australia, Canada, Europe, USA | | Europe |
The quantity of microspheres injected varies according to the activity to deliver and the calibration of the delivered vial. Indeed, TheraSphere® can be injected with varying activity per sphere, from a maximum of 2500 Bq per microsphere at the time of calibration, down to 70 Bq at the expiration date (15 days after calibration). For SIR-Spheres®, the activity per vial orderable is between 3 and 10 GBq with a fixed number of microspheres, which leads to an activity per sphere between 50 and 150 Bq. This results in different biodistributions, which were described in the liver parenchyma [
3] and impacts the acceptable dose limit in the healthy liver [
3‐
5]. The impact on the tumor is also suspected to result in a different dose–response profile according to the microsphere load as suggested by Romanò et al. [
6].
An alternative to the use of microspheres is to inject radiolabeled Lipiodol® ultra-fluid. This method was originally developed with Iodine-131 (
131I) [
7,
8] and was commercially available in the 2000s as Lipiocis® (CIS BIO International, Gif-Sur-Yvette, France). Radiolabeling of Lipiodol® ultra-fluid was also proposed with a rhenium-containing ligand dissolved in Lipiodol® ultra-fluid, the complex SSS, which stands for “Super-Six sulfur”. A Lipiodol® labeled with rhenium-188 (
188Re) has been proposed [
9].
The benefit of Lipiodol® ultra-fluid is that its biodistribution in the hepatic tumor has been described for years in the context of trans-arterial embolization. Its penetration to the venous sinuses, its extravasation, and its intra-cellular internalization give it a very high tumor coverage [
10,
11]. The accumulation of Lipiodol® ultra-fluid in the tumor results from the specific characteristics of the tumor microenvironment described by Folkman [
12]. The lack of contractility of the neovessel, the very slow blood flow [
13,
14], and the increase in vascular permeability lead to an accumulation in the extracellular space.
Several radionuclides have been selected as candidates for radioembolization with Lipiodol® ultra-fluid [
15] and are summarized in Table
2. They are all beta emitters and have a relatively long half-life (> 10 h). The value Δ
β/λ is the ratio of Δ
β the average energy released per β disintegration and λ the physical decay constant of the radionuclide, which stands as the total energy releasable for a source of 1 Bq. For a given radionuclide, the β radiation-absorbed dose D
β can be calculated according to this value, with the assumption of low penetrating particles and high retention over time:
$${D}_{\upbeta }=\frac{{\Delta }_{\upbeta }/\uplambda \times A}{m}$$
(1)
with
A being the activity administered in the target and
m the mass of the target. Depending on the radionuclide, the activity leading to a given absorbed dose can go from 1 to 20-fold (see Table
2). In addition, the continuous slowing-down approximation (CSDA), i.e., the range of the β particles goes from 0.4 to 4 mm. These differences can have an impact on therapeutic effect. Indeed, for a given average absorbed dose, differences in the micro-scale absorbed dose distribution can cause variations in the anti-tumor effect.
Table 2
Radionuclides characteristics used in SIRT, data taken from [
16] and NIST ESTAR Program [
17]
Phosphorus-32 (32P) | 343 | 696 keV (2.8 mm) | 198 |
Yttrium-90 (90Y) | 64 | 933 keV (4 mm) | 49.6 |
IODINE-131 (131I) | 192 | 182 keV (0.4 mm) | 29.0 |
Holmium-166 (166Ho) | 27 | 665 keV (2.6 mm) | 14.9 |
Lutetium-177 (177Lu) | 160 | 451 keV (1.5 mm) | 59.8 |
Rhenium-188 (188Re) | 17 | 762 keV (3.1 mm) | 10.8 |
We propose to study these effects according to the radioembolization agent type and radionuclide using dosimetry and radiobiological modeling, to consider micro-scale heterogeneities and dose-rate effects. To this aim, we compared the biodistribution of Lipiodol® ultra-fluid with those of microspheres comparable in the rabbit hepatocarcinoma model (VX2). For each explant, the dosimetry was modeled for the following radionuclides: 32P, 90Y, 131I, 166Ho, 177Lu, and 188Re.
Materials and methods
Animals
All animal experiments were conducted in compliance with European Union Directive 2010/63/EU on the protection of animals used for scientific purposes. The protocol was approved by the local animal research ethics committee. All surgeries were performed under general anesthesia and aseptic conditions and were supplemented by appropriate analgesic programs.
The VX2 rabbit tumor is a commonly used animal model for translational research on HCC in interventional radiology [
18]. Implantation of a VX2 fragment was performed in healthy New Zealand white rabbits (Charles River Laboratories, Saint-Germain-Nuelles, France).
VX2 well-vascularized tumor fragments (25 mg) were sampled from a carrier animal and immediately implanted in the left median lobe of the exposed liver of the recipient rabbits. One donor was used for 3–6 receivers. Tumor growth lasted at least 19 days after implantation. Ultrasound imaging was performed to ensure that the tumor had reached a length of at least 10 mm (major axis); otherwise, the animal was kept until the tumor was workable. Nineteen to twenty days after tumor induction, the population was divided into 3 groups: L for Lipiodol®, M for microspheres, and C for control.
Interventional procedure
The rabbits of the L and M groups received buprenorphine (Buprecare® 0.14 mL/kg) 1 h before surgery and were hydrated with 50 mL of saline subcutaneously in the flank. Then, they received an intravenous injection of heparin diluted to 1/10 at a dose of 50 IU/kg in the ear. A pediatric valve introducer 4F (Radifocus® TERUMO™) was inserted into the femoral vein and a 1.7F catheter (Microcatheter 1.7F angle 90° - ECHELON™ - MEDTRONIC EV3) was guided under x-ray angiography (Philips Veradius®) to the feeding artery of the tumor at the level of the left hepatic artery. After removal of the catheter, the skin and muscle planes were sutured at the paw level.
Injection
The L group received an adjusted dose of Lipiodol® ultra-fluid into the left common hepatic artery up to reflux or pulmonary passage and to a maximum volume of 0.4 mL. The Lipiodol® ultra-fluid (Guerbet) injection liquid contains per 1 ampoule of 10 mL ethyl esters of iodized fatty acids of poppy seed oil, equivalent to 4.8 g of iodine (480 mgI/mL).
The M group received a fixed volume of 0.3 mL of microspheres in the same injection site. The radiopaque microspheres used in this study were made polyethylene glycol methacrylate (PEGMA) resin microspheres and were sieved to obtain an average diameter of 33 µm. They were made by Guerbet Research representative of approved microspheres in terms of size, which have been customized to make them radiopaque for the purpose of the study. Just before injection, 300 µL of microspheres were taken from the vial and suspended in 3 mL of saline water. The total amount of this suspension was injected slowly (about 0.1 mL∙min−1).
The C group received nothing.
Imaging
Different time intervals were studied to investigate the distribution kinetics of the products. Because of its ability to extravasate leading to a possible modification of distribution during the first hours after injection, the pharmacokinetics of Lipiodol® ultra-fluid (L group) was studied at different timepoints (15 min (D0), 1, 2, 6, 9 and 12 days). For microspheres (M group) which are known to stay several months in the intravascular compartment, only the following delays were studied: 15 min (D0) and 12 days (D12) after injection. The C group was imaged at 15 min, 6 days, and 9 days. At studied time-points, the rabbits were euthanized by an intravenous injection of pentobarbital at a dose of 1 mL/kg under general anesthesia. The liver was explanted, and the tumor was isolated for high resolution 3D X-ray micro-computerized tomography (µCT). A Quantum GX2 (Perkin-Elmer) was used with the following parameters 90 kV, 88 µA, and a CuAl filter, and an acquisition time of 14 min. The field of view diameter was 72 mm or 86 mm depending on the size of the tumor, leading to a voxel side of 0.144 mm or 0.172 mm.
Histology
For the L group, as soon as the µCT image was acquired, the tumor was cut into slices of up to one centimeter, frozen (− 80 °C) and sent for analysis to Oncovet Clinical Research (Clinical Research, Loos, France). Frozen samples of liver with tumor were cut into sections of 12 µm thick. The sections were stained with Hemalum-Eosin after a previous silver staining (2.5%, 60 min, 4 °C) allowing the detection of Lipiodol® ultra-fluid. Assessments from the resulting histologic slides were performed by a veterinary pathologist blinded to sample. The Lipiodol® ultra-fluid and microspheres distributions were studied in the vascular network and in the parenchyma of the tumors.
Imaging analysis
To compare Lipiodol® ultra-fluid and microspheres capabilities to penetrate into tumor tissues, we applied a set of first-order radiomic features on the µCT images. To do so, the tumors were segmented manually using the software tool 3DSlicer [
19]. The radiomics features were extracted using the SlicerRadiomics extension based on PyRadiomics [
20]. A Spearman correlation test was done between time delay, tumor volume, and each radiomic feature. For these variables, the 3 groups were compared using the non-parametric Wilcoxon test. The statistical significance was considered to be achieved for a
p value below 0.05.
Dosimetry
Tri-dimensional (3D) dosimetry was modelized based on the Lipiodol® and microspheres distribution deduced from the µCT images. The tumor contours previously defined for the radiomic analysis were used. The distribution volume of iodine was segmented by manual thresholding. All voxels belonging to this structure were scaled so that the values were ranging from 0 to 1. The resulting image templates were then used to generate the activity maps so that the total activity within the tumors was equal to 1 MBq.
The activity in voxels was converted to time-integrated activity, which is also referred as the total number of disintegrations over the course of the treatment. In radioembolization, the calculation is simplified by the fact that the biological half-life is far greater than the physical half-life of the radionuclides used. Thus, time-integrated activity
Ã(s) in each source voxels was calculated as
$$\widetilde{A}(s)=\frac{A(s,t=0)}{\lambda }$$
(2)
with
A(
s,
t = 0) being the initial activity in the voxel and
λ the decay constant of the radionuclide.
The absorbed dose was calculated in water using dose-point kernel (DPK) convolution implemented in a previous study [
21,
22]. Water DPKs had a resolution of 0.1 mm. The dose
D(x) at position
x was calculated as
$$D\left(x\right)=\iiint \widetilde{A}\left(s\right){k}_{w}\left(\left|s-x\right|\right)\mathrm{d}s$$
(3)
with
s being the position of the source,
\(\widetilde{A}\left(s\right)\) the time-integrated activity, and
kw the kernel in water.
The absorbed dose by tumor was calculated for each radionuclide in Gy per MBq administered to the tumor, which equals the ratio of
S factor over the radionuclide decay constant
λ. Indeed, according to the medical internal radiation dose (MIRD) formalism [
23, p. 21], the tumor-absorbed dose is expressed as:
$$D=\widetilde{A}\times S$$
(4)
Hence, knowing that for radioembolization
\(\widetilde{A}=\frac{A}{\lambda }\), the tumor absorbed dose over the administered activity within the tumor can expressed as:
$$\frac{D}{A}=\frac{{S}}{\lambda }$$
(5)
To compare the biological efficacy between absorbed dose distributions, the biological effective dose (BED) was calculated according to the linear-quadratic model applied to radioembolization [
24] as:
$$\mathrm{BED}=D\left(1+\frac{\lambda }{\lambda +\mu }\times \frac{1}{\alpha /\beta }\times D\right)$$
(6)
with μ the DNA repair constant, α and β are the linear and quadratic cell killing constants. We set the value of μ to 0.46 h
−1 as reported by Cremonesi et al. for tumors [
25], and α and β values to, respectively, 0.037 Gy
−1 and 0.0028 Gy
−2, as reported by van Leeuwen et al
. [
26].
To consider the heterogeneity of absorbed dose distribution, we implemented the equivalent uniform dose (EUD) concept of Jones and Hoban [
27] to the BED leading to the EUBED:
$$\mathrm{EUBED}=-\frac{1}{\alpha }\mathrm{ln}\left({\sum }_{i=1}^{N}{e}^{-\alpha \times {\mathrm{BED}}_{i}}\times {v}_{i}\right)$$
(7)
with BED
i being the histogram
ith bin,
vi the volume fraction, and
N the number of histogram bins. EUBEDs were calculated for absorbed doses ranging from 1 to 1000.
Statistics
Mean and standard deviation were calculated for the following variables for each radionuclide: tumor volume V,
S/
λ, EUBED(D = 100 Gy). The L and M groups were compared for each variable using the Kruskal–Wallis test by ranks. The statistical significance was set for a
p value < 0.05. All statistics and graphics were processed using RStudio 2022.12.0.353 [
28] and R 4.2.2 [
29].
Discussion
Radioembolization of liver tumors is a well-established treatment strategy for HCC [
2]. Currently, there are 3 major options that are based on microspheres [
30]:
90Y-resin-microspheres,
90Y-glass-microspheres, and
166Ho-PLGA-microspheres. As reported by Bouvry et al. [
15], other compounds based on Lipiodol® ultra-fluid were developed and evaluated, but to date no direct comparison is available in terms of biodistribution and dosimetry.
This study aimed at comparing the biodistributions of Lipiodol® and microspheres in a VX2 tumor model implanted in rabbits. The biodistributions were assessed though histology and µCT, and absorbed dose distributions were simulated for radionuclides of interest in radioembolization, i.e., 32P, 90Y, 131I, 166Ho, 177Lu, and 188Re. The distributions were analyzed visually and using first-order radiomics, while the absorbed dose distributions were completed by radiobiological modeling to compare biological effective dose (BED).
The analysis of the µCT images showed that the Lipiodol® ultra-fluid perfused the large and small vessels, feeding the tumor parenchyma but also diffuses in the extravascular compartment, while the microspheres stay strictly intravascular. This observation of Lipiodol® ultra-fluid being a more penetrative agent (confirmed by the histology) was consistent with the radiomic analysis showing a significantly greater entropy in the Lipiodol® ultra-fluid group (4.06, n = 14) compared to the microspheres (2.67, n = 6).
The dosimetry analysis showed that the absorbed dose per activity administered to the tumor (S/λ) was higher for the M group than for the L group, but without statistical significance. The highest average values were found for 32P with 86.3 Gy∙MBq−1 in M group and 62.8 Gy∙MBq−1 in L group, which was significantly higher than 90Y with 19.9 Gy∙MBq−1 and 14.9 Gy∙MBq−1, respectively. All other radionuclide S/λ values were below that of 90Y. The lowest values were found for 188Re with 4.67 Gy∙MBq−1 and 3.43 Gy∙MBq−1 for M and L groups, respectively.
In order to simulate the biological efficacy of radionuclides, we calculated the equivalent uniform biological effective dose (EUBED), using radiobiological parameters found in the literature. The values of
α and
β were issued from clinical data [
26]. We found that the mean EUBED values for a tumor-absorbed dose of 100 Gy were systematically higher for the L group than for the M group. This suggests that the more distal penetration of Lipiodol® ultra-fluid should have an impact on tumor treatment efficacy, which may be expected superior to that of microspheres. Regarding the comparison between radionuclides, EUBED values were significantly higher for
90Y than all other radionuclides but
188Re. The lowest EUBED values were found for
131I and
177Lu.
Aside from these differences, the Lipiodol® ultra-fluid does not remain in the healthy liver parenchyma [
13,
31,
32] contrary to microspheres that are blocked by microvessels, regardless of being tumoral or healthy tissue feeders. This could be an advantage for Lipiodol® ultra-fluid as a radionuclide carrier for radioembolization treatments where more than a single segment of the liver needs to be treated. Different retention mechanisms are currently evoked in the tumor (accumulation of the product in the peri-tumoral sinuses by an embolization mechanism [
27], modification of the membrane potential or of the permeability of the tumor vessels [
31], slower elimination linked to a deficiency in Küpffer cells and lymphatic vessels in the tumor, membrane and then intra-cellular fixation, pinocytosis of Lipiodol® ultra-fluid droplets in HepG2 cells). While the microspheres remain blocked in the microvessels with heterogeneity in targeting the tumor, the slow infusion of radiolabeled Lipiodol® ultra-fluid in the tumor may offer potential for better biological effectiveness while preserving the healthy liver tissues.
This study clearly shows that there are some trends toward a better penetration of Lipiodol® ultra-fluid that may translate into a better radiation efficacy. The comparison of various radionuclides on such a dataset had never been done before. One interesting result is that at an absorbed dose of 100 Gy, the greatest simulated biological efficacy was obtained with 90Y and 188Re, while the lowest was obtained for 131I and 177Lu. This can be explained by the longest beta radiation range of 90Y and 188Re, but also their shortest half-life resulting in a higher dose-rate for a given absorbed dose delivered. Indeed, at higher dose-rate, the cell-killing effect is higher due to lack of reparation capabilities. In between, we found 32P, 166Ho, whose EUBED values are not statistically different but remain one-third below those of 90Y.
Our study has several limitations. First, the number of animals differ between groups and the imaging points are not equal in each group. This is due to the primary endpoint, which was to study the biodistribution kinetic of Lipiodol® ultra-fluid in VX2 tumors, which limits the interpretation of these results. Another limitation is the choice of model since there is no HCC model in rabbits. Nevertheless, although not of hepatic origin, the VX2 model is commonly used as an alternative for interventional radiotherapy studies [
33].
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