Open Access Article
Claire
Leterrier
a,
Guillaume
Pinna
bc,
Marie
Vandamme
bc,
Mélissa
Glatigny
d,
Erwan
Selingue
d,
Françoise
Geffroy
d,
Sébastien
Mériaux
*d,
Edmond
Gravel
*a and
Eric
Doris
*a
aCEA, INRAE, Département Médicaments et Technologies pour la Santé (DMTS), SCBM, Université Paris-Saclay, 91191 Gif-sur-Yvette, France. E-mail: edmond.gravel@cea.fr; eric.doris@cea.fr
bCEA, Stabilité Génétique Cellules Souches et Radiations, Université Paris Cité, Plateforme PARi, 92260 Fontenay-aux-Roses, France
cCEA, Stabilité Génétique Cellules Souches et Radiations, Université Paris-Saclay, Plateforme PARi, 92260 Fontenay-aux-Roses, France
dCEA, CNRS, BAOBAB, NeuroSpin, Université Paris-Saclay, 91191 Gif-sur-Yvette, France. E-mail: sebastien.meriaux@cea.fr
First published on 19th September 2025
We report the development of a fluorinated micellar nanosystem whose 19F-MRI signal can be selectively dimmed by application of an external stimulus. A photo-activatable quencher unit (ferrocene) was co-encapsulated with the superfluorinated PERFECTA probe in colloidal micelles. While pristine micelles were MRI responsive (“On” state), their irradiation by light triggered the “Off” MRI-state of PERFECTA.
New conceptsA light-activated switch was designed to enable controlled extinction of the 19F-MRI signal from a micellar nanocarrier containing a MRI-responsive superfluorinated probe (PERFECTA) and a photo-activatable ferrocene quencher. Upon illumination, the ferrocene is converted into paramagnetic ferrocenium, which shortens the T2 relaxation time of nearby 19F nuclei, effectively silencing the MRI signal. Unlike most activatable 19F-MRI probes, which operate from an “off” to “on” transition, our method switches-off MRI signals on demand, and this phenomenon is triggered for the first time by light. The co-encapsulation of a photo-activatable quencher unit and a superfluorinated probe within micellar nanocarriers provided the requisite proximity and confinement for effective paramagnetic resonance enhancement effect-mediated signal attenuation of PERFECTA. This light-responsive signal modulation introduces a novel approach to MRI contrast enhancement that could enable selective signal dimming in extraneous tissues, thus improving delineation of pathological sites in clinical practice. Proof of concept was established using a rodent model. |
On the other hand, contrast agents incorporating responsive atoms such as 13C, 31P, 17O or 19F, can be directly observed by magnetic resonance techniques, guaranteeing signal specificity and ease of quantification.4 In this case, the agents themselves are imaged, enabling absolute quantification of the MRI signal, which is proportional to the probe concentration. In the context of in vivo quantitative imaging, fluorine-19 is a promising nucleus,5 which benefits from 100% natural abundance, spin ½, high nuclear receptivity,6 and low background noise as virtually no endogenous fluorine is found in living bodies.
When designing 19F-MRI probes, the number and nature of fluorine atoms must be taken into account. PERFECTA is one of the few 19F probes currently available in the literature.7 It is a symmetrical molecule with 36 chemically equivalent fluorine atoms, all resonating at the same frequency and providing a unique and strong magnetic resonance signal.8 However, PERFECTA is not water-soluble, and if it is to be used in biomedical applications, it must be formulated so that it can be dispersed in aqueous medium prior to administration.9–12
Our group has long been involved in the development of nanometric carrier systems for drug delivery and imaging applications.13–24 We recently reported the design of fluorinated micelles for the encapsulation and biocompatibilization of PERFECTA, applied to in vivo19F-MRI detection of tumors.25 These micelles consist of supramolecular aggregates of PFTD-PEG amphiphilic units comprising: (i) a perfluorinated chain forming the central hydrophobic core of the micelle and designed to accommodate fluorinated probes; and (ii) a hydrophilic poly(ethylene glycol) (PEG, MW = 2000) head group forming the outer hydrophilic layer and designed to delay adsorption of plasma proteins and prevent rapid opsonisation/elimination in vivo.26 In the context of cancer diagnosis, we evaluated PERFECTA-loaded micelles (PERFECTA@PFTD-PEG micelles) in a mouse model for their ability to passively target tumors through the enhanced permeability and retention (EPR) effect. Micelles were intravenously injected to MC38 tumor-bearing mice and were found to selectively accumulate (>3.5% of the injected dose) in the tumor area, as evidenced and quantified by 19F-MR imaging. Yet, preclinical imaging performance was somewhat impaired by the non-specific accumulation of micelles in the liver, resulting in a strong MRI signal in the abdomen and reducing the contrast in the area of interest (i.e. the tumor, Fig. 1).
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| Fig. 1 Illustration of PERFECTA-loaded micelles and previous in vivo19F-MR imaging of PERFECTA@PFTD-PEG 96 h after intravenous injection of the micelles to a tumor-bearing mouse. | ||
To selectively improve the contrast-to-noise ratio of the pathological site, we conceived that selective attenuation of the MRI signal in non-pathological liver tissue should facilitate the visualization of the tumor zone. With this feature in mind, we have developed a micellar 19F-MRI probe whose signal can be selectively dimmed in chosen areas (those not to be imaged) by application of an external stimulus. We selected the ferrocenyl group as the quencher unit to be associated to PERFECTA-loaded micelles. In fact, some ferrocene derivatives can be activated by light27 and converted to higher oxidation state ferroceniums.28 Since the latter possesses paramagnetic properties, capable of interfering with the magnetic resonance response of the observed nuclei, we sought to exploit the light-triggered transition from ferrocene to ferrocenium to selectively attenuate the 19F-MRI signals of PERFECTA micelles, in a controlled manner.
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| Fig. 2 Multi-slice multi-echo (MSME) sequence for 19F-MR imaging of PFTD-PEG micelles containing various concentrations of PERFECTA. | ||
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| Scheme 1 Synthesis of fluorinated ferrocene (FFc): (a) N-methyl morpholine, isobutyl chloroformate, N-Boc ethylenediamine, THF; (b) HCl in dioxane, THF; (c) EDC·HCl, NHS, DMF; (d) NEt3, CHCl3. | ||
Mixed FFc/PERFECTA@PFTD-PEG micelles were produced by co-encapsulation of PERFECTA and FFc in the presence of PFTD-PEG amphiphiles, under ultrasonic activation (Fig. 3). It is worth noting that PERFECTA loading remained constant at 13.5 mg mL−1, while the FFc load reached a maximum of 5 mg mL−1, as measured by NMR experiments (encapsulation efficiency = 100%). Stability tests indicated that micelles were stable over several weeks at room temperature, as neither precipitation nor leaching of the payload was observed.
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| Fig. 3 (a) Structure of PFTD-PEG; (b) assembly of PFTD-PEG micelles and co-encapsulation of PERFECTA and FFc; (c) structure of FFc; (d) structure of PERFECTA. | ||
In the absence of light, pristine FFc had moderate impact on the transverse relaxation times of the fluorine atoms of micelle-encapsulated PERFECTA. Estimated T2 values ranged from 150 ms in the absence of FFc to 118 ms for the highest FFc concentration studied (4.35 mM). This minor variation of T2 values did not significantly affect the recorded 19F-MR images of the different tubes whose signal intensity remained nearly constant (Fig. 5a). We can thus conclude that FFc in its initial state does not interfere much with 19F-MRI signals of PERFECTA, which can be readily acquired with high sensitivity using the MSME sequence.
The different tubes were then illuminated with a blue LED lamp for 10 min, and T2 relaxation times were measured again. While the signal of sample F containing no FFc was not affected by the illumination process, a major change in T2 values was detected for samples containing FFc and this effect was accentuated by increasing FFc concentrations (samples G and H, Fig. 5b). For example, a nearly two-fold decrease in T2 (from 129 to 72 ms) was measured for sample G containing 0.92 mM of FFc. At the highest concentration studied ([FFc] = 4.35 mM), the FFc-derived ferrocenium induced a massive drop in T2 from 118 to 10 ms. As a result, the 19F-signal was strongly attenuated for FFc/PEFECTA@PFTD-PEG micelles exposed to light, resulting in a significant decrease in contrast. As with any MRI paramagnetic contrast agent, the impact of oxidized FFc on the transverse fluorine relaxation rate was characterized by the transverse relaxivity factor (r2) (Fig. 5d), calculated according to the formula:
ref the transverse relaxation time of 19F nuclei in the absence of FFc. In our experiment, the transverse relaxivity factor of oxidized FFc was found to be r2 = 22.5 mM−1 s−1. This value is higher than that of other paramagnetic systems, such as gadolinium, a conventional MRI contrast agent (for comparison with other paramagnetic systems, see Table S1).
We nevertheless further proceeded with preliminary in vivo experiments. C57Bl/6 immunocompetent male mice (N = 5) were injected with FFc/PERFECTA@PFTD-PEG micelles suspended in 0.9% aqueous NaCl. A stock solution containing 13.5 mg of PERFECTA and 5 mg of FFc in 20 mg of PFTD-PEG micelles suspended in 1 mL 0.9% NaCl/H2O was prepared and 150 μL were injected intravenously to each mouse, once a day for 3 days to ensure optimal biodistribution and 19F-MRI detection. Twenty-four hours after the last injection, animals were scanned by 1H/19F MRI (1H images were recorded for anatomical superposition). As anticipated, a clear and intense 19F-signal was observed in the liver (Fig. S6), indicating nanoparticles accumulation, with [19FPERFECTA] locally reaching 43 ± 5 mM. In an attempt to quench the 19F-MRI signal in the organ of interest, mice were sacrificed and their liver harvested. Given the limited tissue penetration of blue light used to convert FFc into ferrocenium, we conceived that ex vivo activation could offer a suitable proof of concept for attenuating PERFECTA signals in interaction with biological systems. The organ of interest was collected and a liver lobe was ground into a fine suspension to allow deeper light penetration. 19F-MRI of the suspension was recorded before and after 10 min exposure to blue light. Gratifyingly, we detected a ca. 15% decrease in the 19F-signal intensity of PERFECTA after light irradiation of the sample. The partial signal attenuation was attributed to the turbidity of the ground liver sample, which likely impeded optimal photoconversion of the ferrocene moiety. Yet, this observation reflects activation of FFc into paramagnetic ferrocenium, and the subsequent acceleration of transverse relaxation rates of nearby fluorine atoms in the micelle-encapsulated PERFECTA that has accumulated in the liver.
Another possible strategy to maintain the initial “Off” state relies on the proximity of a “silencing” paramagnetic metal center, whose separation from the 19F probe can reveal MRI signals, thus switching the system to its “On” state. For example, the group of Kikuchi engineered a gadolinium (Gd) chelate linked to a fluorinated probe via a short peptide sequence cleavable by caspase enzymes.37 The paramagnetic properties of Gd3+ ion initially attenuated the 19F-MRI signal, but in the presence of active caspases, the peptide bond was cleaved, moving Gd3+ away from the probe and restoring the signal.
A third option to modulate MRI signals is the change in the redox state of the probe to take advantage of the paramagnetic relaxation enhancement (PRE) effect induced by metals nearby the 19F nuclei. As an example, Xie et al. designed a copper chelate with a fluorinated side chain.38 The fluorine atoms were initially silent in 19F-NMR due to the proximity of Cu(II). However, upon reduction of paramagnetic Cu2+ to diamagnetic Cu+, the signal was activated due to the suppression of PRE effect, thus allowing the monitoring of cellular hypoxic/normoxic conditions by 19F-NMR.
In our case, and as opposed to most approaches that were previously developed in the literature, we chose to modulate the signal of PERFECTA by inducing an “On → Off” transition. Indeed, if PERFECTA-loaded micelles are to be used in cancer diagnosis with no a priori knowledge of the tumor location, it is difficult to envisage increasing the local MRI contrast in the pathological zone by externally turning-on the probe. Yet, contrast can be enhanced by selectively turning-off the interfering signals present in a well-defined organ such as the liver.
To turn-off the signal of PERFECTA-loaded micelles, we co-encapsulated a redox active modulator of the MRI signal in the form of a fluorophilic ferrocene derivative (FFc). FFc is photo-responsive and can undergo oxidation to ferrocenium upon illumination at a suitable wavelength (i.e. 460 nm). In the absence of light, the ferrocene derivative is in its diamagnetic state and does not disturb the signal of PERFECTA. This corresponds to the initial “On” state of the probe that can be readily visualized by 19F-MRI. However, when light is applied, FFc is photo-oxidized into paramagnetic ferrocenium, which results in reduction of the spin–spin relaxation times (T2 → 0) and broadening/attenuation of the 19F signals of PERFECTA. In our experiments, a strong decrease of the T2 of PERFECTA, from 118 to 10 ms, was observed at the highest FFc concentration studied (4.35 mM), together with a significant attenuation of the MRI signal. This corresponds to the “Off” state of the probe due to the generation of paramagnetic iron that triggers a PRE effect. This phenomenon is due to dipolar interactions between unpaired electrons of ferrocenium ions and nuclear spins of 19F atoms, leading to accelerated transverse relaxation rates of the latter (shorter T2 relaxation times) and hence lowering 19F-MRI signal in T2 weighted images.38,39
To the best of our knowledge, there are only two other examples in the literature of ferrocene-based systems for modulating the 19F-magnetic resonance signals. Ferrocene-functionalized fluorinated dendrimers were synthesized by the group of Chujo as redox-responsive 19F-NMR probes.40 Chemical oxidation of the ferrocenyl unit by ammonium persulfate led to the formation of the ferrocenium cation. The latter induced a PRE effect to the adjacent fluorine nuclei, leading to a significant decrease in 19F-NMR signal intensity. Chemical reduction of the ferrocenium cation back to ferrocene resulted in the recovery of the 19F-NMR signal. Yet, this system was not applied to magnetic resonance imaging. The second example is from the team of Hruby,41 who investigated polymers incorporating fluorinated ferrocene derivatives that were treated under ammonium peroxydisulfate/CuCl2 as the oxidant system. This permitted the conversion of the diamagnetic ferrocene moiety into paramagnetic ferrocenium, which markedly changed the chemical shift and relaxation time of the 19F nuclei, as visualized by 19F-MRI.
Here, we used light-activation of the ferrocenyl unit, which is unprecedented in MRI. In addition, our system enables signals from the fluorinated probe to be disabled, which has only been scarcely explored in the literature as most of the current approaches deal with turn-on probes. The latter strategy, when externally activated, cannot be used in the context of cancer diagnosis without prior knowledge of the tumor location. In that sense, our nanoscale platform, combining MRI-responsive PERFECTA and photo-activatable FFc in a biocompatible micelle, could provide images with enhanced contrast in targeted tumors, by selectively quenching the MRI signal in anatomically defined satellite organs, such as the liver. Yet, a preliminary proof of concept could be achieved ex vivo, but we still have to solve the problem of the activation wavelength of FFc, which needs to be shifted towards the near-infrared region for better light penetration into deep tissues. A potential strategy could be the co-encapsulation of upconverting nanoparticles, which convert low-energy near-infrared photons into higher-energy photons capable of inducing ferrocene photo-oxidation – a direction currently under investigation.
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