Abstract
Purpose
To investigate the utility of inversion recovery with ON-resonant water suppression (IRON) to create positive signal in normal lymph nodes after injection of super-paramagnetic nanoparticles.
Materials and Methods
Experiments were conducted on six rabbits, which received a single bolus injection of 80 µmol Fe/kg monocrystalline iron oxide nanoparticle (MION-47). Magnetic resonance imaging (MRI) was performed at baseline, 1 day, and 3 days after MION-47 injection using conventional T1- and T2*-weighted sequences and IRON. Contrast-to-noise ratios (CNR) were measured in blood and in paraaortic lymph nodes.
Results
On T2*-weighted images, as expected, signal attenuation was observed in areas of paraaortic lymph nodes after MION-47 injection. However, using IRON the paraaortic lymph nodes exhibited very high contrast enhancement, which remained 3 days after injection. CNR with IRON was 2.2 ± 0.8 at baseline, increased markedly 1 day after injection (23.5 ± 5.4, P < 0.01 vs. baseline), and remained high after 3 days (21.8 ± 5.7, *P < 0.01 vs. baseline). CNR was also high in blood 1 day after injection (42.7 ± 7.2 vs. 1.8 ± 0.7 at baseline, P < 0.01) but approached baseline after 3 days (1.9 ± 1.4, P = NS vs. baseline).
Conclusion
IRON in conjunction with superparamagnetic nanoparticles can be used to perform ‘positive contrast’ MR-lymphography, particularly 3 days after injection of the contrast agent, when signal is no longer visible within blood vessels. The proposed method may have potential as an adjunct for nodal staging in cancer screening.
Keywords: inversion recovery with ON-resonant water suppression (IRON), off-resonance imaging, monocrystalline iron oxide nanoparticle (MION-47), magnetic resonance lymphography
Contrast-enhanced magnetic resonance (MR)-lymphography is a potential noninvasive method for the evaluation of the lymphatic system and in particular for nodal staging (1–10). The most widely evaluated intravenous contrast agents for MR-lymphography are superparamagnetic nanoparticles, which accumulate slowly in macrophages of the lymph nodes and show maximum lymphographic effects 24 hours after injection. Several experimental (1–5) and clinical studies (6–10) have demonstrated the accuracy for lymph node evaluation after the administration of superparamagnetic nanoparticles for the evaluation of pelvic, abdominal, thoracic, head, and neck tumors.
Conventional strategies for MR-lymphography take advantage of magnetic susceptibility artifacts, creating negative signal in normal lymph nodes, which accumulate superparamagnetic nanoparticles, while the signal in metastatic lymph nodes remains unchanged (1–10). However, negative signal may arise from many other sources such as the absence of tissue, motion, or calcifications. This may hamper the ability of conventional methods to discriminate between normal lymph nodes with low signal and other sources of signal loss (4,9).
Recently, spectrally selective radiofrequency (RF) pulses have been reported to create positive signal using superparamagnetic materials (11–15). This positive signal is a result of off-resonance effects in areas of superparamagnetic particles. Inversion recovery with ON-resonant water suppression (IRON) is a new approach which creates positive signal in areas of superparamagnetic nanoparticles and simultaneously suppresses signal from tissues which do not contain iron (16). The purpose of the present study was to test the hypothesis whether IRON can create positive signal in normal lymph nodes after the systemic administration of superparamagnetic nanoparticles. This hypothesis was tested in a rabbit model at 3T.
MATERIALS AND METHODS
Animals and Imaging Agent
The studies were approved by the Institutional Animal Care and Use Committee. Experiments were conducted on six male rabbits (2.5–3.2 kg). The animals were sedated with acepromazine (1 mg/kg I.M.) and ketamine (40 mg/kg I.M.), and general anesthesia was maintained with intravenous thiopental. Monocrystalline iron oxide nanoparticle (MION)-47 was administrated as a single bolus injection of 80 µmol Fe/kg in all six rabbits. The physical, chemical, and MR properties of MION-47 are described elsewhere (17,18).
MR Imaging
All animals were imaged in the supine position using a commercial 3T whole body scanner (Achieva, Philips Medical Systems, Best, the Netherlands) and a 4-element human carotid receiver coil (Pathway MRI, Seattle, WA). Imaging was performed at baseline and 1 day and 3 days after MION-47 injection.
Conventional T1- and T2*-Weighted Imaging
For T1-weighted imaging, 3D gradient-echo images of the abdomen were obtained using the following parameters: TR/TE = 25/2.7 msec, 20° excitation angle, 200 × 100 mm field of view (FOV), partial echo, bandwidth = 217 Hz/pixel, RF spoiling, and a 400 × 200 matrix. A 5.0-cm thick 3D volume was scanned with 50 z-encoding steps (0.5 × 0.5 × 1 mm3 acquired resolution). Scanning time was 3 minutes. For T2*-weighted imaging TR/TE was modified to 100/12 msec and the excitation angle was changed to 6°. All other parameters were kept identical to those of the T1-weighted imaging. The mean size of the abdominal lymph nodes was measured on coronal T1-weighted images and was expressed as cranio-caudal and left-right diameters.
Inversion Recovery With ON-Resonant Water Suppression (IRON)
Theoretical Background of IRON
The local external field-shift of a nondiamagnetic spherical particle exposed to the static magnetic field (B0) can be described as:
(1) |
In this equation ΔK is the difference in susceptibility between the particle and its surroundings, r refers to the distance from the particle, a refers to its radius and Θ represents the angle between r and B0. External to the particle, the frequency shift is ΔωExternal = γΔBExternal. The concept of IRON imaging comprises the use of a spectrally selective saturation prepulse on-resonance (ω0) with the bandwidth of BWIRON, in order to suppress the signal originating from on-resonant protons (Fig. 1a). This saturation pulse does not affect off-resonant protons in areas of superparamagnetic nanoparticles (Fig. 1b). Therefore, signal enhancement adjacent to these particles can be generated while the on-resonant background appears signal-attenuated (Fig. 1c). Fat saturation can be obtained by adding a fat suppression prepulse, as shown in Fig. 1a,b.
IRON Imaging
IRON was combined with gradient-echo and black-blood fast-spin-echo imaging. For all sequences an IRON prepulse with BWIRONof 100 Hz, a duration of τ = 50 msec, and an excitation angle aIRON of 100° was used. The preceding frequency selective pre-pulse used for fat saturation had a frequency offset of −480 Hz, a duration of 10 msec, and an excitation angle of 105°. Typical imaging parameters for the 3D gradient-echo imaging were: TR/TE = 3.9/1.54 msec, 15° excitation angle, 140 × 112 mm FOV, partial echo, bandwidth = 642 Hz/pixel, RF spoiling, and a 288 × 220 matrix. A 5.0 cm thick 3D volume was scanned with 25 z-encoding steps (0.49 × 0.51 × 2 mm3 acquired resolution). Scanning time was 3 minutes. For 3D black-blood fast-spin-echo imaging, the vector electrocardiogram (VCG) was used for R-wave triggering and the black blood dual-inversion delay was set at 370 msec. Typical parameters were: TR/TE = 857/8.2 msec, 90° excitation angle, 100 × 80 mm FOV, bandwidth = 248 Hz/pixel and a 288 × 288 matrix. A 1.4–2.0-cm thick 3D volume was scanned with 7–10 z-encoding steps (0.35 × 0.27 × 2 mm3 acquired resolution). Scanning time was 8.5–12 minutes.
Image Analysis
Quantitative analysis was performed by one of the authors (G.K.) using the “soap bubble” tool (19). Soap bubble is a software tool that was previously developed in order to facilitate the visualization and quantitative comparison of 3D volumetric data sets. In its present implementation the soap bubble tool enables the analysis of frequently explored quantitative parameters such as signal-to-noise ratio (SNR) and contrast-to-noise ratio (CNR). CNR was quantified on IRON images, at baseline, on day 1, and on day 3, using original, non-reformatted datasets. Regions of interest (ROIs) were placed manually on paraaortic lymph nodes and in the abdominal aorta of the rabbits for the measurement of the mean signal (Slymph and Sblood, respectively). Similar ROIs were placed in adjacent abdominal muscle and in fat to measure Smuscle and Sfat, respectively, and also in the air outside of the rabbit to calculate standard deviation of this region as a measure of noise (σbackground). CNR was calculated as:
(2) |
(3) |
Care was taken to standardize ROI size and placement for better comparison of the imaging sets. The size of the ROIs was 0.32 ± 0.05 cm2 for ROIs placed in vessels, 0.34 ± 0.04 cm2 for ROIs placed in lymph nodes, 0.37 ± 0.05 cm2 for ROIs placed in fat, 0.33 ± 0.05 cm2 for ROIs placed in the abdominal adjacent muscle, and 8.3 ± 1.1 cm2 for ROIs placed in the background.
Isolation of Abdominal Lymph Nodes and Histopathologic Examination
After MR imaging the rabbits were sacrificed with an overdose of thiopental and the abdominal lymph nodes were isolated and fixed with 4% paraformaldehyde. The lymph nodes were then frozen and 10-µm thick sections were obtained using a cryostat for histological analysis. Tissue sections were stained with Prussian blue to detect iron oxide particles and counterstained with nuclear fast red. In addition, an acid phosphates-estain (Sigma-Aldrich, St. Louis, MO) to detect phagocytic cells was performed on adjacent sections which were then counterstained with Prussian blue as described previously (20).
Statistical Analysis
Data are presented as mean ± one standard deviation. Differences in CNR of the abdominal lymph nodes and in blood between baseline, day 1, and day 3 were compared using a repeated-measures analysis of variance (ANOVA) with Bonferroni post-hoc comparison. Differences were considered statistically significant at P < 0.05.
RESULTS
On conventional T1-weighted images, two major lymph nodes could routinely be identified along the abdominal aorta at the level of the renal arteries in each rabbit (12 abdominal lymph nodes in total, mean size 8.4 ± 1.0 × 9.1 ± 1.1 mm2) (Fig. 2a, solid arrows). After the administration of MION-47, lymph nodes showed signal void on T2*-weighted images (Fig. 2b, solid arrow). However, the clear visualization of the lymph nodes was often compromised due to a general lack of signal (Fig. 2b, dotted arrow). Using IRON, fat, muscle, and blood were homogeneously suppressed at baseline (Fig. 2c). One day after injection, paraaortic lymph nodes were clearly visible (Fig. 2d). However, at this timepoint high contrast enhancement was present both in the paraaortic lymph nodes and in the aorta. After 3 days the signal decreased in the vessels but persisted in the lymph nodes (Fig. 2e). The location and morphology of the lymph nodes on MRI corresponded with their in situ localization (Fig. 2f). Corresponding postcontrast fast spin echo IRON images also demonstrated contrast enhancement in paraaortic lymph nodes in coronal (Fig. 3a, solid arrows) and in axial slices (Fig. 3b, solid arrow). Furthermore, in the same animal the lymphatic ducts along the aorta could be clearly visualized with high spatial resolution on coronal (Fig. 3c, hatched arrows) and on axial slices (Fig. 3d, hatched arrows). Note that the abdominal aorta (Fig. 3a,b, arrowheads) and adjacent muscles are signal-attenuated (Fig. 3a,b, dotted arrows) in all IRON images.
Quantitative assessment of IRON images showed that the CNR markedly increased in paraaortic lymph nodes after 24 hours (24.0 ± 5.3 on day 1 vs. 1.4 ± 0.8 at baseline, *P < 0.01) and remained high up to 3 days after MION-47 injection (22.3 ± 6.2, *P < 0.01 vs. baseline) (Fig. 4). In the aorta, CNR was high 24 hours after MION-47 administration (42.7 ± 7.2 on day 1 vs. 1.8 ± 0.7 at baseline, #P < 0.01) but returned to baseline after 3 days (1.9 ± 1.4, P = NS vs. baseline).
Prussian blue positive staining, representing iron oxide particles, was detected in abdominal lymph nodes of the rabbits (Fig. 5a). Combined acid phosphatase and Prussian blue staining shows colocalization of nodal macrophages (stained red) and accumulated iron (Fig. 5b).
DISCUSSION
This is to our knowledge the first report on ‘positive contrast’ MR-lymphography using (MION)-47 as an imaging agent. Using IRON, positive signal was created in the areas of superparamagnetic nanoparticles, which accumulated in functional lymphatic tissue. One day after MION-47 injection, contrast enhancement was present both intravascular and in the lymph nodes of the rabbits. On day 3, contrast enhancement was present only in the lymph nodes, while blood and adjacent muscles displayed homogeneously signal suppressed. The potential of this method to differentiate between functional and metastatic lymphatic tissue remains to be elucidated in further studies.
Conventional ‘negative contrast’ techniques for MR-lymphography are based on local changes of T2 and T2*-relaxation rates caused by superparamagnetic nanoparticles (1–10). These changes create susceptibility artifacts, which can be visualized as negative signal in normal lymph nodes using T2*-weighted imaging, while metastatic lymph nodes remain unchanged. However, a fundamental drawback of ‘negative contrast’ techniques is that low signal in normal lymph nodes cannot be distinguished from other sources of signal voids due to absence of tissue, motion, or calcifications. Furthermore, ‘negative contrast’ techniques suffer from partial-volume effects, where the ability to detect a void depends on spatial resolution (13). Particularly when small receiver coils with a small volume of sensitivity are used, the intensity variation across the image may further hamper the accurate identification of negative signal due to susceptibility effects (13). In addition, it should be noted that TE is longer in T2*-weighted sequences compared to both T1-weighted and IRON sequences. For this reason, T2*-weighted images may not only be more sensitive to motion artifacts but a reduced SNR may be another impediment. In agreement with these theoretical concerns the negative signal in the abdominal lymph nodes could not be readily detected as such on the T2*-weighted images in our study. This was attributed to other sources of signal void caused by absence of tissue or by respiratory motion at the level of the abdomen. However, it should be noted that the comparison of pre- to post-contrast T2*-weighted images is very useful for the differentiation of functional versus metastatic lymph nodes and may help to overcome some of the susceptibility- related problems and SNR constrains of T2*-weighted MR-images.
The results of the present study demonstrate the utility of IRON to create positive signal in small normal lymph nodes after a single bolus administration of superparamagnetic nanoparticles. IRON allowed the clear visualization of small lymph nodes (mean size <10 mm), and quantification analysis revealed high CNR in the abdominal lymph nodes 1 and 3 days after contrast agent administration. In particular, 3 days after injection of the superparamagnetic nanoparticles, IRON facilitated the clear visualization of functional lymphatic tissue, because blood, adjacent muscles, and fat are signal-attenuated at this timepoint. IRON can be combined both with conventional gradient echo and fast spin echo sequences in order to create positive signal originating from off-resonance in the area of superparamagnetic nanoparticles, which accumulate in functional lymph nodes.
The present study provides a proof-of-principle for the utility of IRON as a ‘positive contrast’ technique for MR-lymphography. Due to the small number of animals (n = 6) and lymph nodes (n = 12) studied, we did not perform a head-to-head comparison of conventional (T2*-weighted) versus IRON imaging for the delineation of normal lymph nodes. However, this is the aim of future studies. Furthermore, the potential of IRON to differentiate between normal and metastatic lymph nodes was not evaluated in this study, and IRON was not compared to other techniques, which create positive signal in areas of superparamagnetic materials (11–15). Previous studies have shown that, using T2*-weighted imaging, susceptibility artifacts in areas of accumulated USPIO in functional lymph nodes may obscure small focal metastases within the same or in neighboring lymph nodes. However, it is anticipated that on IRON images small focal metastases may also be missed due to the suppression of on resonant protons in tissue that does not contain accumulated superparamagnetic nanoparticles (metastatic tissue). An inherent limitation of IRON is that it is based on frequency selection so that IRON images can be affected by susceptibility interfaces and B1-inhomogeneity. Thus, unwanted magnetization from regions that are shifted in frequency, such as tissue near the lungs or intestines, could also create positive signal on the images. In our study, high-order shimming was used in order to circumvent such effects. Furthermore, IRON allows the clear visualization of functional lymph nodes only after contrast agent administration. Therefore, for the differentiation between functional and metastatic lymph nodes, the additional acquisition of precontrast T1-weighted images will still be necessary. Thus, IRON images are not likely to be a replacement of conventional techniques, but may rather be a useful adjunct.
In conclusion, IRON in concertwith superparamagnetic nanoparticles creates positive signal in normal lymph nodes and can be used to perform ‘positive contrast’ MR-lymphography, in particular, at 3 days after injection of the contrast agent. The potential of this technique to differentiate between normal and metastatic lymph nodes remains to be investigated in future studies.
ACKNOWLEDGMENTS
Dr. Matthias Stuber is compensated as a consultant by Philips Medical Systems, Netherlands, the manufacturer of the equipment described in this presentation. The terms of this agreement have been approved by the Johns Hopkins University in accordance with its conflict of interest policies.
Contract grant sponsor: Donald W. Reynolds Foundation; Contract grant sponsor: National Institutes of Health (NIH); Contract grant numbers: 1 K08 EB004922-01 (to M.S.), R01 HL084186 (to M.S.), R24CA92782 (to R.W.), P50CA86355 (to R.W.).
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