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Systems Biology and Emerging Technologies |
1 Department of Radiology, Maastricht University Hospital, 2 Cardiovascular Research Institute Maastricht (CARIM), Departments of 3 Biomedical Engineering, 4 Biochemistry, and 5 Physiology, and 6 Research Institute GROW, Maastricht University, Maastricht, the Netherlands; and 7 Department of Biomedical Engineering, Eindhoven University of Technology, Eindhoven, the Netherlands
Requests for reprints: Walter H. Backes, Maastricht University Hospital, Department of Radiology, P.Debyelaan 25, 6229 HX, Maastricht, the Netherlands. Phone: 0031-43-3876948; Fax: 0031-43-3876909; E-mail: wbac{at}rdia.azm.nl.
| Abstract |
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| Introduction |
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Currently, molecular imaging techniques are being developed that allow direct visualization and characterization of cellular or molecular activation of angiogenesis-related pathways (5). More specifically, molecular imaging uses contrast agents that home to up-regulated biomolecules (e.g., receptors, enzymes) via interaction with high-affinity ligands coupled to the contrast agent. Ideally, this results in an altered signal intensity at the location of these molecules. Of the different imaging modalities, magnetic resonance imaging (MRI) may be the most desirable for molecular imaging due to its excellent spatial resolution and soft tissue contrast. Moreover, molecular MRI potentially allows direct covisualization of tumor angiogenic activity with anatomy. However, the inherently low sensitivity of MRI is a problem due to the typically low abundance of up-regulated biomolecules. This can be overcome by large molecular weight constructs carrying a high payload of gadolinium or iron, and multiple targeting ligands to enhance the relaxivity and targeting efficacy, respectively, of the particle (6).
One of the best-defined ligands for molecular imaging of angiogenesis is the cyclic Arg-Gly-Asp (cRGD) peptide, which binds specifically to the
vβ3-integrin (7, 8). However, for the cyclic Asn-Gly-Arg (cNGR) motif, the tumor-homing capability was shown to be 3-fold higher compared with cRGD (9). The clinical applicability of cNGR as a tumor-homing ligand was previously shown by conjugating cNGR to tumor necrosis factor
(TNF
). Compared with unlabeled TNF
, cNGR-TNF
displayed a significantly increased antitumor activity with similar systemic toxicity (10–12).
The vascular address of cNGR is a specific isoform of CD13 (aminopeptidase N), a transmembrane glycoprotein involved in cancer angiogenesis, tumor invasion, and metastasis, which is overexpressed by activated endothelial cells (ECs) of tumor vasculature (9, 13, 14). CD13 is not required for vessel growth during embryonic development and normal adult function, as shown in CD13-null mice (15). In a model of retinal neovascularization, these mice had significantly decreased vessel growth, suggesting that CD13 is important in pathologic neovascularization. In addition, fluorophore-conjugated cNGR allowed detection of the in vivo expression of CD13 in tumors and infarcted myocardium (16, 17). Competition with unconjugated cNGR significantly decreased the fluorescence signal, indicating high specificity of cNGR for CD13 (16, 17).
Despite the aforementioned high tumor-homing capability of cNGR, its potency as a targeting ligand for molecular imaging of tumor angiogenesis is currently unknown. Therefore, the objective of this study was to explore cNGR-labeled paramagnetic quantum dots (cNGR-pQDs) for the noninvasive and selective in vivo detection of tumor neovascularization using quantitative molecular MRI. QDs were chosen as contrast agent scaffolds because of their excellent photophysical properties, i.e., broad excitation, small emission spectra, and limited photobleaching (18, 19). Furthermore, QDs enabled binding of multiple targeting ligands and gadolinium chelates. The bimodal nature of the particle (i.e., paramagnetic and fluorescent) allowed validation of the results with ex vivo two-photon laser scanning microscopy (TPLSM). With TPLSM, three-dimensional contrast agent localization can be obtained at subcellular resolution with a penetration depth reaching 250 µm in tumors.
MRI data were analyzed via absolute quantification of contrast agent induced changes in the longitudinal relaxation rate R1 (1/T1) of the tissue, which is proportional to contrast agent concentration, and proton visibility. The latter expectedly decreases at high densities of paramagnetic contrast material. Quantitative analysis requires acquisition of a series of images and may provide improved sensitivity of molecular MRI. Theoretically, the used inversion recovery (IR) technique has an inherent 2-fold higher sensitivity than spin echo pulse sequences and by measuring a series of images it potentially allows detection of smaller changes in R1 than a single image.
Both MRI and TPLSM showed specific binding of cNGR-pQDs to ECs in the angiogenic tumor rim but not in tumor core or muscle tissue. Furthermore, a significantly lower quantitative contrast was found with unlabeled pQDs, indicating a high specificity of the cNGR-labeled contrast agent for angiogenic ECs. To our knowledge, this is the first noninvasive in vivo application of cNGR as a targeting ligand for molecular MRI of tumor angiogenesis.
| Materials and Methods |
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-amino group to obtain biotinylated peptide-resin, the peptide was deprotected and cleaved from the resin using anhydrous hydrogen fluoride for 1 h at 0°C with 4% p-cresol as scavenger and lyophilized. Electrospray ionization mass spectrometry (ESI-MS) revealed a mass of 1,287.4, corresponding well to the theoretical average mass (1,288.7) of the reduced biotinylated Nac-Cys-Asn-Gly-Arg-Cys-Gly-Gly-Lys(biotin)-NH2 peptide. Oxidative folding of the crude product in 0.1 mol/L Tris (pH 8), 1 mol/L guanidin at 4°C for 16 h yielded the internal disulfide bridged biotin-cyclic NGR, which was high performance liquid chromatography (HPLC)-purified (C18 RP-HPLC) and lyophilized. ESI-MS confirmed a mass decrease of 2, representing the loss of 2 protons from the cystein side chains due to the generation of 1 disulfide bond (S-S). Biotinylated poly(lysine) dendritic wedge, a construct comprising 8 Gd-diethylenetriaminepentaacetic acid (DTPA) moieties, was synthesized and purified similarly (21, 22).
Curnis and colleagues (23) previously showed that cNGR spontaneously converts into isoDGR by asparagine deamidation at slightly basic pH, generating an
vβ3-integrin ligand. Using a combination of HPLC and mass spectrometry up to 24 h after dissolving cNGR in water (pH 6.0) and 1 µmol/L borate buffer (pH 8.3; supplemented with 0.05% NaN3), respectively, it was found that this process did not occur in the time-period of the experiments (data not shown).
Bimodal, multivalent contrast agent was prepared as follows. Streptavidin-conjugated QDs [1 µmol/L in borate buffer (pH 8.3), emission at 585 nm] were purchased from Invitrogen. QDs were composed of a CdSe core with a ZnS shell and covered with polyethyleneglycol-2000. Each QD holds
10 surface-bound streptavidins, allowing 30 biotinylated compounds to bind on average.8 For each experiment, cNGR-pQDs were prepared freshly at room temperature by sequential mixing of 100 µL QD solution with biotin-cNGR and biotin-poly(lysine) dendritic wedge, both dissolved in HBSS (pH 7.4; Invitrogen), in a molar ratio of 1:6:24 to a total volume of
120 µL. Samples were mildly vortexed during each preparation step to ensure a homogeneous distribution of biotin-cNGR and biotin-poly(lysine) dendritic wedge over the QD surface. Overall, each QD carried a maximum of 192 Gd ions and 6 cNGR peptides. Unlabeled pQDs carried the same number of Gd constructs but no cNGR. A schematic representation of the cNGR-pQD particle is shown in Fig. 1
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15-wk-old male Swiss nu/nu mice (Charles River). Mice were subjected to the MRI examination when the tumor diameter was >1.0 cm, which was
16 d after LS174T injection. For in vivo MRI, mice were anesthetized using 1.5% to 2.0% isoflurane (Abbott Laboratories Ltd) in medical air and were placed prone in a dedicated animal holder with built-in mask for anesthesia gas supply. An infusion line was placed in the jugular vein for contrast agent administration during the MRI experiment. A heating pad was placed over the mice to maintain normothermic conditions. Respiration rate and body temperature were continuously monitored via a balloon sensor and rectal temperature probe, respectively, interfaced to an MR compatible small animal monitoring system (SA Instruments, Inc.).
Mice were randomly selected for injection with either cNGR-labeled or unlabeled pQDs. Seven mice were included for each contrast agent group. Mice were kept inside the magnet during the entire MRI experiment to preserve their position.
MRI Protocol
All MRI experiments were performed on a 7 T Bruker Biospec 70/30 USR MRI system, interfaced to an AVANCE II console (Bruker Biospin GmbH). The BGA12-S mini imaging gradient (maximum gradient strength, 720 mTm–1; slew rate, 6,000 Tm–1s–1) and a 3.5-cm inner diameter quadrature volume resonator were used.
Molecular MRI. Tumors were localized using T2-weighted anatomic images (TR, 4,200 ms; TE, 37.4 ms). Next, precontrast R1 values were determined using a series of IR measurements with increasing inversion times (TR, 4,000 ms; TE, 8.4 ms; TI, 500, 1,000, 1,500, 2,000, 2,500, and 3,500 ms; total scan time, 18 min). Subsequently, mice were injected with 120 µL of cNGR-labeled or unlabeled pQDs, followed by a 50 µL saline flush. IR experiments were repeated
30 min postcontrast to ensure adequate contrast agent circulation and a reduced level of intravascular contrast agent. Images were recorded using a field of view (FOV) of 4.0 x 4.0 cm2, a 192 x 192 acquisition matrix interpolated to 256 x 256 by means of zero-filling, and a slice thickness of 1.2 mm, resulting in 0.16 x 0.16 x 1.2-mm3-sized voxels. On average, 15 contiguous slices were recorded in multislice mode (range, 11–22 slices; depending on tumor size and orientation). After MRI, mice were euthanized by cervical dislocation.
Competition experiment. Four tumor-bearing mice were randomly selected for a competition experiment of cNGR-pQDs with unconjugated cNGR, i.e., nonbiotinylated, nonparamagnetic, and nonfluorescent. Imaging was performed as described above, except that 525 µg per mouse of unconjugated cNGR, i.e., a 1,000-fold excess compared with QD-bound cNGR, was injected i.v. 10 min after administration of cNGR-pQDs.
Biodistribution. Healthy Swiss mice (Charles River) were injected with either cNGR-pQDs, unlabeled pQDs, or no contrast agent. After
1 h circulation time, mice were sacrificed and whole body T1-weighted spin echo images were recorded (TR, 1,100 ms; TE, 8.5 ms; FOV, 4.0 x 6.0 cm2; matrix, 256 x 512; resolution, 0.16 x 0.12 x 1.2 mm3). Two mice were included per group.
Tissue harvesting. After MRI, tumor, spleen, liver, kidney, hind limb muscle, heart, and lung were excised and embedded in optimal cutting temperature (OCT) compound (Sakura Finetek Europe). Next, tissues were snapfrozen in cold 2-methylbutane (Acros Organics) for
2 min and subsequently transferred to liquid nitrogen. Tissues were stored at –80°C until TPLSM measurements.
Contrast agent relaxivity. T1 relaxivity (r1) was determined by diluting cNGR-pQDs in HBSS in 9 steps to concentrations of 0 to 0.001 mmol/L (corresponding gadolinium concentrations, 0–0.192 mmol/L). The R1 of each sample was determined using the IR series as described above. Absolute gadolinium concentrations were measured using Inductively Coupled Plasma Mass Spectrometry. Longitudinal relaxivity was determined by the slope of a linear fit of R1 versus gadolinium concentration.
MRI Data Analysis
All data processing was performed in Matlab (The Mathworks), unless stated otherwise. IR images were first spatially coregistered using the mutual information algorithm in the MIRIT software package (24) to correct for possible animal motion in the images with different T1 contrast, and smoothed with a three dimensional Gaussian kernel with a full-width-at-half-maximum of 0.4 x 0.4 x 3.0 mm3. Regions of interest (ROI) were drawn manually in MRIcro (25) to define tumor and muscle tissue. Both T1- and T2-weighted images were used to accurately delineate tumors from surrounding tissue and edema.
Precontrast and postcontrast R1 values were determined on a voxel-by-voxel basis by nonlinear curve fitting of the IR signal intensity function (26):
![]() | (1) |
The detection limit for changes in R1 (
R1 = R1,post – R1,pre) was determined with a Monte Carlo simulation using Eq. 1, in vivo relaxation rates, and representative noise levels as derived from the in vivo experiments. A voxel was considered significantly enhanced when
R1 was >1.96 (i.e., 95% confidence interval) times higher than the detection limit of 0.005 s–1. We defined the Quantitative Contrast derived from the
R1 measurements (QCR1) as the product of the mean
R1 and the percentage of significantly enhanced voxels for each tissue type, i.e., tumor rim and core, and muscle tissue. QCR1 indicates both the level and spatial extent of contrast agent binding. Changes in S0 (
S0 = S0,post – S0,pre) were also evaluated, and the Quantitative Contrast from S0 (QCS0) was defined analogously to QCR1 to yield a quantity that reflects proton visibility (27).
Tumor rim/core analysis. To investigate the differences between tumor rim, i.e., the region with the highest expected angiogenic activity, and core, the tumor rim was first defined as a
1-mm thick peripheral zone with the strongest R1 enhancement, in accordance with the approach taken by others (28, 29). Using this thickness, the difference between cNGR-labeled and unlabeled pQDs was maximal (Fig. 3C). The rim comprised 29.0% ± 5.8% and 31.6% ± 3.5% of all tumor voxels for mice injected with cNGR-labeled and unlabeled pQDs, respectively. The tumor core was defined as the difference between whole tumor and tumor rim ROIs. Second, a contour was drawn to calculate the number of voxels with a significantly increased
R1 as a function of the distance to the tumor rim. As an empirical measure of spatial heterogeneity in angiogenic tumor activity, the half-value-depth was defined as the distance from the rim at which the percentage of enhanced voxels has decreased by 50% compared with its value at zero distance, i.e., the rim. The half-value-depth was calculated by fitting the group-averaged data presented in Fig. 3C with a monoexponential decay function.
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Statistical analysis. Statistical analysis of paired samples was performed using a nonparametric Wilcoxon signed-rank test in SPSS 14.0 (SPSS).
As both QCR1 and QCS0 represent contrast agent presence, QCR1 and QCS0 were combined to a summary value according to O'Brien and Läuter (30, 31), which is more sensitive to contrast effects than the individual measures. Therefore, QCR1 and QCS0 were first standardized by z = [QC – mean(QC)/sd(QC)]. Subsequently, the absolute values of zQCR1 and zQCS0 were averaged per animal. The resulting summary measure was tested using a nonparametric Mann-Whitney U test. P < 0.05 was considered statistically significant.
TPLSM Data Acquisition
Tissue samples were thawed and washed with HBSS to remove OCT compound. Except for the spleen and liver, tissues were incubated with 25-fold diluted
CD31-FITC (0.5 mg/mL; BD Biosciences PharMingen) to fluorescently label ECs. Next, tissues were embedded in 2 w% agarose gel (Invitrogen), with their rim upwards. For measurements in the tumor core, tumors were cut transversally to resemble the slice orientation of the MRI measurements.
TPLSM imaging was performed using a Nikon Eclipse E600FN upright microscope, incorporated in the Bio-Rad Radiance 2100MP imaging system and operated by Lasersharp2000 V6.0 (Bio-Rad). Tissue samples were excited by the Tsunami Ti:sapphire laser (Spectra-Physics), which was pumped by a Millennia Vs 5 W pump laser (Spectra-Physics) and mode locked at 800 nm, with a 82.5 MHz repetition rate and 100 fs pulse width. Tissues were observed through a water dipping 60 x fluor objective with a 1.00 numerical aperture (Nikon). Photomultiplier tubes (PMTs 9108B02 and 9136B05; Electron Tubes Limited) were used to acquire fluorescence photons in three spectral regions: 420 to 470 nm (autofluorescence), 520 to 560 nm, (FITC) and 570 to 600 nm (QD). Each PMT was tuned for minimal bleed through of the fluorescent markers to adjacent PMTs. Images, color coded blue, green, and red, respectively, were subsequently merged into a single image. The in-plane pixel dwell time was 11.8 µs, which, together with a 2-fold Kalman averaging, resulted in an imaging speed of 0.16 Hz. The FOV was 179 x 179 µm2 with a matrix size of 512 x 512, resulting in 0.35 x 0.35 µm2 sized pixels.
TPLSM Data Analysis
Data were analyzed with Image-Pro Plus 6.0 (MediaCybernetics) and ImageJ 1.35 (NIH). Image quality was improved by convolution with a 1.05 x 1.05 µm2 Gaussian filter. Spatial distribution of pQDs was classified into four groups: intravascular, intracellular, colocalized with the EC membrane, or extravasated to the interstitium.
| Results |
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For both cNGR-labeled and unlabeled pQDs, changes in R1 (
R1) were spatially heterogeneous throughout the tumor and were most pronounced at the tumor rim (Fig. 2A
). Averaged over all mice, the
R1 induced by cNGR-pQDs ranged up to
0.3 s–1, which was considerably larger than the intrinsic variation in precontrast tumor R1 of 0.1 s–1. Furthermore, the range in
R1 was relatively large compared with the precontrast tumor R1 of 0.8 s–1. Administration of unlabeled pQDs resulted in a 3-fold lower response range (
R1 < 0.1 s–1) compared with cNGR-pQDs.
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Further evidence for the specificity of cNGR was provided by
R1 in hind limb muscle. Here, average
R1 upon administration of cNGR-pQDs was considerably lower than in the tumor and ranged up to 0.05 s–1. TPLSM did not display colocalization of cNGR-pQD with ECs of muscle vasculature. However, the incidence of cNGR-pQDs in the muscle vascular lumen was almost 2-fold higher than for unlabeled pQDs (Fig. 2D).
S0-effect. For both cNGR-labeled and unlabeled pQDs, changes in the scaling factor S0 colocalized strongly with
R1 (Fig. 2B). The S0-effect is likely caused by field inhomogeneities (T2*-effect) in the vicinity of the contrast agent, induced by the magnetic properties of QDs (33) and the dense gadolinium concentration on the particle. Analogous to iron oxide particles, such properties result in locally reduced transverse relaxation times T2 and T2*, a shift in local resonance frequency and a broader water resonance line, which is reflected by a decrease in S0, i.e., a reduced proton visibility (27, 34). Therefore,
R1 and
S0 both represent contrast agent presence.
Spatial heterogeneity. To explore the absolute differences between tumor rim, tumor core, and muscle, QCR1 and QCS0 were determined for each tissue type for cNGR-labeled and unlabeled pQDs (Fig. 3A and B
). Administration of cNGR-pQDs resulted in an
50-fold increase in QCR1 in the angiogenic rim compared with tumor core or muscle tissue. For unlabeled pQDs, significant differences were also found between tumor rim and core, and tumor rim and muscle tissue, although the net increase in QCR1 was lower than for cNGR-pQDs. The decreases in S0 showed the same trend as the increases in R1 (cf. Fig. 3A and B).
For each of the three tissue types, no significant differences in QCR1 or QCS0 were found between cNGR-labeled and unlabeled pQDs. Because
R1 and
S0 were shown to accurately colocalize (Fig. 2), QCR1 data were combined with QCS0 to a summary measure as described above. This resulted in a statistically significant difference between cNGR-labeled and unlabeled pQDs for the tumor rim only (Fig. 3A and B).
To further investigate the spatial distribution of angiogenic activity in the tumor, the percentage of significantly enhanced voxels was calculated as a function of the distance to the tumor rim (Fig. 3C). Although the highest signal increase was found at the tumor rim for both contrast agents, more than twice as many rim voxels were enhanced for cNGR-pQDs than for unlabeled pQDs. In the tumor core, similar enhancements were found for both contrast agents. These findings qualitatively concur with previous findings showing that angiogenic activity is most pronounced at the tumor rim for this tumor model (7, 35).
Subsequently, half-value-depths were calculated for both cNGR-labeled and unlabeled pQDs. High values indicate a more homogeneous distribution of enhanced voxels over the entire tumor and thus a low spatial heterogeneity, whereas low values indicate a high spatial variation. For cNGR-labeled and unlabeled pQDs, the half-value-depths were 0.6 and 1.1 mm, respectively, indicating a stronger contrast between tumor rim and core for cNGR-pQDs, which suggests that cNGR-pQDs allow a better differentiation between tumor rim and core than unlabeled pQDs.
Competition experiment. I.v. injection of a 1,000-fold excess of unconjugated cNGR 10 min after administration of cNGR-pQDs resulted in a statistically significant decrease in QCR1 and QCS0 for the tumor rim (Fig. 3A and B). With TPLSM, cNGR-pQDs were barely detected in the tumor rim, which confirmed the MRI results (data not shown). These results therefore indicate that binding of cNGR-pQDs to tumor ECs is specific, reversible, and can be competed with unconjugated cNGR.
Biodistribution. Figure 4
shows the relative MRI signal intensities for the blood and major organs recorded
1 hour after the administration of cNGR-pQDs, unlabeled pQDs, or no contrast agent. No differences were found between cNGR-labeled and unlabeled pQDs. Both contrast agents accumulated mainly in the spleen, liver, and kidneys (Fig. 4), which was confirmed by TPLSM and corresponds to previous findings (36). Due to the i.v. administration, pQDs were also expected to accumulate in the lung. However, MRI has only limited signal sensitivity in the lung due to the inherently low signal intensity and air-tissue interfaces. With TPLSM, pQDs could be clearly detected in the lung (Fig. 4), although microscopic imaging was hampered by tissue movement caused by heating of the sample during excitation, resulting in expansion of air in the pulmonary alveoli.
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| Discussion |
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In correspondence with other studies (7, 35), our results indicate that angiogenic activity is highest at the tumor rim, which was reflected by a high QCR1 and a strongly negative QCS0 for cNGR- pQDs. This was supported by the statistically significant difference between cNGR-labeled and unlabeled pQDs found using the summary value. Unlabeled pQDs also showed differences between tumor rim versus core and muscle, albeit smaller than for the cNGR-pQDs. This is likely due to the intrinsically higher vascular density of the tumor rim and corresponding blood pool fraction, resulting in a larger amount of circulating contrast agent compared with tumor core or muscle tissue (35). Additionally, heterogeneous blood flow and long wash-in and wash-out times of macromolecular contrast agents, which was previously described for dendritic agents (38), may have contributed to a prolonged retention of unlabeled pQDs in the tumor peripheral vasculature.
Methodologic considerations. Nonlinear fitting of the IR signal over a range of inversion times provided a sensitive and reliable method for detecting R1 changes induced by contrast agent binding. Compared with signal intensity measurements, it is relatively independent of technical settings, e.g., repetition time, echo time, and flip angle, thereby allowing objective comparison between different subjects, both spatially and temporally. A disadvantage of the quantitative approach is the lengthy acquisition time because an adequate number of data points is required for accurate fitting of the IR curve. Although prolonged precontrast and postcontrast acquisition of a single image at a fixed inversion time may also allow accurate detection of changes in signal intensity, this will not provide quantitative information on R1 and S0. In our quantitative approach, coregistration of these variables ensured increased sensitivity to detect differences between cNGR-labeled and unlabeled pQDs and is therefore preferred over acquisition of a single image.
Theoretically, the measured longitudinal relaxation rates and contrast agent relaxivity allow estimation of local contrast agent concentration and might be used to gain insight in the density of the molecular target. However, the conditions under which the relaxivity was determined differ strongly from the in vivo situation. Not only is the relaxivity affected by the chemical environment of the particle, i.e., aqueous buffer versus blood plasma (39), specific binding to vascular endothelium reduces its tumbling rate, thereby increasing the relaxivity. Taken together, this would lead to an overestimation of the local concentration in vivo. Unfortunately, accurate measurements of in vivo relaxivity are currently unavailable.
Contrast agent. Quantum dots were chosen as scaffold to enable bimodal, i.e., MRI and TPLSM, visualization of tumor angiogenic activity, which is an essential step in the characterization and validation of cNGR as a targeting ligand. Furthermore, streptavidin-coated QDs provide a suitable and versatile research scaffold to identify and test other potential targeting ligands. In addition, QDs show minimal extravasation, both from healthy and hyperpermeable tumor vasculature,9 which is beneficial for EC targeting. However, QDs may pose serious health limitations due to the potential release of toxic cadmium ions. Although this can be prevented by effective shielding of the core (40, 41), QDs are not cleared from the body and accumulate in spleen, liver, and kidneys. Cadmium-based QDs will therefore not be approved for clinical application. Recently developed nontoxic and renally excretable QDs may provide a potential solution for this problem (42, 43). Nevertheless, once a robust MRI method has been accepted in clinical practice, validation with luminescent particles is no longer necessary and clinically more suitable particles may be applied.
The magnetic and semiconductive properties of QDs give increase to field inhomogeneities when placed inside a magnetic field (33), which likely result in a local decrease of the transverse relaxation times T2 and T2*. In addition, T2 contrast becomes more effective at high field strength, whereas T1 contrast decreases. Using a standard multislice multiecho spin echo sequence, an average R2 increase of 5.7 s–1 upon cNGR-pQD injection was detected in the tumor rim at a mean tumor precontrast R2 of
27 s–1. However, the percentage of significantly enhanced voxels in the tumor rim was only 4%, which is considerably lower than the 42% found for R1. This shows that T2 changes did not interfere with the effects on T1 and S0. Consequently, the T1 and S0 quantification was more sensitive in discriminating between angiogenic activity in the tumor rim, tumor core, and muscle tissue than T2.
Clinical perspectives. Regarding the potential clinical applicability, quantitative molecular MRI with a suitable contrast agent has a number of advantages over the currently used immunohistochemical methods to quantify tumor angiogenic activity. First, molecular MRI is noninvasive and does not interfere with tissue integrity. Second, it can probe the entire tumor, whereas immunohistochemistry requires biopsies at one or multiple selected locations. Third, it allows covisualization of angiogenic activity with local anatomy. Fourth, tumor status or therapeutic response may be objectively monitored over time due to the absolute quantification methodology. Finally, molecular MRI allows direct detection of activated endothelium in functional vasculature, whereas immunohistochemistry measures both perfused and nonperfused vessels.
With respect to the applied tumor model, a human colorectal adenocarcinoma, MRI is clinically important for local T-staging of rectal cancer and for the identification of tumors close to or invading the mesorectal fascia (44). On diagnostic T2-weighted images, however, it remains difficult to differentiate between fibrotic tissue and viable tumor cells. Molecular MRI of angiogenesis may facilitate this demarcation because only viable tumor cells induce angiogenesis, which may be visualized upon administration of the targeted contrast agent.
Besides the availability of suitable contrast agents, clinical implementation of quantitative molecular MRI requires rapid imaging techniques. Possible sequences that allow fast quantification of relaxation times are Look-Locker (45), IR-true-FISP (46), and the recently described QRAPTEST (47). However, these methods are relatively sensitive to subject movement and field inhomogeneities, although the Look-Locker method was recently modified to allow in vivo T1-mapping of the heart (48). Thus, the development of fast quantification of relaxation rates seems to support future clinical application of quantitative molecular MRI.
In summary, we have shown that cNGR-labeled paramagnetic quantum dots are suitable for the noninvasive visualization and quantification of tumor angiogenic activity using in vivo molecular MRI. These results provide a promising basis for further developments in contrast agent design and synthesis, data acquisition, and postprocessing techniques, which may be valuable for future clinical applications to pathologies in which abnormal vessel growth plays a pivotal role.
| Disclosure of Potential Conflicts of Interest |
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| Acknowledgments |
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The costs of publication of this article were defrayed in part by the payment of page charges. This article must therefore be hereby marked advertisement in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
We thank Remco Foppen and Stephen H. Chamberlain from Invitrogen for providing detailed information on quantum dot composition; Sander Langereis, Jeannette Smulders, and Thea Haex from Philips Research, Eindhoven, the Netherlands for performing the ICP-MS measurements; and Ludwig Dubois for the in vitro growth of the LS174T tumor cell line.
| Footnotes |
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8 Personal communication with Invitrogen. ![]()
Received 2/25/08. Revised 6/12/08. Accepted 6/13/08.
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M. Oostendorp, M. J. Post, and W. H. Backes Vessel Growth and Function: Depiction with Contrast-enhanced MR Imaging Radiology, May 1, 2009; 251(2): 317 - 335. [Abstract] [Full Text] [PDF] |
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