Supramolecular red-light-photosensitized nitric oxide release with fluorescence self-reporting within biocompatible nanocarriers

The strict dependence of the biological effects of nitric oxide (NO) on its concentration and generation site requires this inorganic free radical to be delivered with precise spatiotemporal control. Light-activation by suitable NO photoprecursors represents an ideal approach. Developing strategies to activate NO release using long-wavelength excitation light in the therapeutic window (650–1300 nm) is challenging. In this contribution, we demonstrate that NO release by a blue-light activatable NO photodonor (NOPD) with self-fluorescence reporting can be triggered catalytically by the much more biocompatible red light exploiting a supramolecular photosensitization process. Different red-light absorbing photosensitizers (PS) are co-entrapped with the NOPD within different biocompatible nanocarriers such as Pluronic  micelles, microemulsions and branched cyclodextrin polymers. The intra-carrier photosensitized NO release, involving the lowest, long-lived triplet state of the PS as the key intermediate and its quenching by the NOPD, is competitive with that by molecular oxygen. This allows NO to be released with good efficacy, even in aerobic conditions. Therefore, the adopted general strategy provides a valuable tool for generating NO from an already available NOPD, otherwise activatable with the poorly biocompatible blue light, without requiring any chemical modification and using sophisticated and expensive irradiation sources.


Introduction
Nitric oxide (NO) is a small inorganic free radical that plays a multifaceted role in many physiological and pathophysiological processes 1,2 and is coming into the limelight as unconventional therapeutic in treating severe diseases 3,4 , including cancer 5 and bacterial infections 6 .Over the last two decades, these intriguing prospects and the difficulties in handling gaseous NO have stimulated a growing interest in developing NO-releasing precursors integrated into molecular and macromolecular scaffolds and functional materials that can store and deliver NO [7][8][9][10][11][12] .Due to the strict dependence of the biological effects of NO on its doses and concentration site 13,14 , the spatiotemporal control of NO release is a highly demanding requisite.Given that light can be easily manipulated in terms of energy, intensity, location, and duration, it represents a non-invasive, powerful tool to control the NO release in space and time with great accuracy.A significant arsenal of photoactivatable precursors, namely NO photodonors (NOPDs), based on organic and inorganic chromophoric motifs and activatable with UV and Vis light, have been developed in recent years [15][16][17][18][19][20] .In this arena, the generation of NO by one-photon excitation in the so-called "therapeutic window" (650-1300 nm) 21 with conventional and lowcost red or near-infrared (NIR) light sources is highly suitable for biomedical applications.This spectral region is, in fact, highly tissuepenetrating due to the negligible absorption of water and haemoglobin. 21Therefore, achieving NOPDs activatable with onephoton red light is very challenging.Compared with NOPDs based on metal complexes, only a few examples of non-metal-based NOPDs controlled by one-photon red/NIR light have been reported.They involve different approaches based on red-light-harvesting antennae linked with N-nitrosoaniline appendages uncaging NO through photoinduced electron transfer, 22,23 red-light absorbing J-aggregates of nitrosated BODIPY chromophores 24 and thermolabile NO precursors which exploit the NIR-induced photothermia of plasmonic inorganic nanostructures 25 .In our recent work, we have reported a straightforward approach to trigger the NO release in a catalytic fashion from NBF-NO, 26 a bluelight activatable NOPD 27 (Scheme 1).It consists of a triplet-mediated photosensitization process upon one-photon red light excitation of Verterporfin (VTP), a clinically approved lipophilic photosensitizer (PS) for photodynamic therapy (PDT) 28,29 .A remarkable improvement of about 300 nm towards longer wavelengths and without requiring any chemical modification efforts was obtained.The process occurred effectively within biodegradable polymeric nanoparticles (NPs) of methoxy-polyethyleneglycol-bpolycaprolactone NPs (mPEG-PCL). 26The highly green fluorescent photoproduct NBF generated in parallel to the NO release acted as an optical NO self-reporter, permitting its easy and real-time quantification without the addition of external fluorescent probes also in the cell environment 26 .These results prompted us to extend the applicability of the adopted strategy to different types of red-light-absorbing PSs and other To this purpose, we selected, besides VTP, the lipophilic porphyrinoid PS THP (5,10,15,20-tetra(4-hydroxyphenyl)porphyrin) and the hydrophilic ZnPCS (Zn(II) phthalocyanine tetrasulfonate) to activate NO photorelease (Scheme 1).To promote the photosensitization reaction, we encapsulated the PS/NBF-NO pair in optically transparent, biocompatible nanocarriers.We tested Pluronic® micelles (PLM) and microemulsions (ME), both suitable to host lipophilic molecules, and a -cyclodextrin branched polymer (Poly-CD) able to entrap both lipophilic and hydrophilic guest compounds (Scheme 1).We investigate if the communication between the excited triplet state of the PSs and the NBF-NO within the same hosts leads to the generation of NO and its self-fluorescent reporter.The effect of the dissolved molecular oxygen on the photosensitization reaction is also explored.

Results and discussion
Besides to VTP, the present study was extended also to other two porphyrinoid PS such as THP and ZnPCS, which have hydrophobic and hydrophilic features, respectively (see Scheme 1).For the sake of clarity, the absorption spectra of all the chromophoric components investigated here are shown in Fig. 1.Analogously to VTP, both THP and ZnPCS show typical Q-bands in the red region well beyond the absorption region of NBF-NO and its stable photoproduct NBF formed after NO release.These experimental conditions permit the PSs to be selectively activated with red light at ac > 600 nm.
To promote the communication between PSs and NBF-NO, these molecules were loaded in three biocompatible host vehicles that share biocompatibility and excellent optical transparency.The latter property represents an ideal requisite for spectroscopic and photochemical investigations.PLM are supramolecular structures with a hydrophobic core of polypropylene oxide able to encapsulate hydrophobic molecules and a surrounding shell of polyoxyethylene.Micelles prepared by a mixture of Pluronic® F127 and P123 are less inclined to dissociation in monomers upon dilution in aqueous media due to a lower critical micelle concentration (CMC) than the single components 30 .
PLM were prepared at 1% (w/v) of P123:F127 at 1:1 ratio by wt.Under these conditions, the CMC is 0.0030%, ensuring the formation of micelles with a diameter of ca. 30 nm.
The water-insoluble NBF-NO was co-encapsulated with the waterinsoluble VTP in a molar ratio of ca.40:1, leading to a nanoassembly of ca.34 nm with a polydispersity index (PI) of 0.18.The UV-Vis absorption profile of this sample (spectrum a in Fig. 2A) matches well the arithmetic sum of the spectra of the individual components Scheme 1. Schematic of the red-light photosensitization mechanism for the NO release with fluorescent self-reporting, a sketch of the biocompatible nanocarriers structure and the molecular structures of the PSs, the NOPD and its green fluorescent reporter.Please do not adjust margins Please do not adjust margins encapsulated in the same host (data not shown), accounting for the absence of relevant intra/inter chromophoric aggregation.Fig. 2A reports the absorption spectral changes observed upon red light irradiation of the sample under anaerobic conditions.They show the bleaching of the absorption bands at 390 nm and 270 nm, and the formation of a new, intense absorption at ca. 470 nm accompanied by the presence of 4 isosbestic points, indicative of a well-defined photochemical process.Besides, only negligible spectral changes are observed in the Q bands absorption region of VTP beyond 550 nm.The corresponding evolution of the fluorescence emission spectra recorded at  exc = 420 nm (isosbestic point) shows a remarkable increase of the initially weak green emission at  max = 530 nm (Fig. 2B).The absorption and emission changes observed are in excellent agreement with those reported upon direct irradiation of NBF-NO with blue light 27 and are consistent with the formation of the highly green fluorescent NBF as stable photoproduct.These results parallel those recently observed for the same chromophoric components co-encapsulated within mPEG-PCL NPs 26 , demonstrating that the same photosensitization process also occurs in PLM.The red-light triggered photosensitization also occurs in the presence of oxygen but at a reduced transformation rate (see inset Fig. 2A).This confirms i) the involvement of the lowest triplet state of VTP as the key intermediate in the photosensitization process and ii) a quenching by NBF-NO highly competitive with that by molecular oxygen.Unambiguous evidence for the red-light-triggered NO release was provided by its direct detection through an amperometric technique using an ultrasensitive NO electrode.Fig. 3A shows that NO generation exclusively regulated by red light is observed only in the PLM co-loaded with VTP and NBF-NO.As already anticipated, the highly fluorescent photoproduct NBF can act as a NO optical reporter, permitting the NO release to be monitored in real-time and exploiting fluorescence techniques.This feature was demonstrated by the experimental set-up illustrated in Fig. 3B.The sample was continuously excited at  exc = 420 nm, and the fluorescence signal was constantly monitored at  em = 530 nm upon alternated OFF and ON activation cycles of irradiation with red light at ac = 630 nm.It can be seen that the green fluorescence of NBF regularly increases upon irradiation with red light, stops as this light source is turned OFF, and restarts when it is turned ON again.Note that, despite NBF-NO absorbs at  exc = 420 nm, the light intensity used in this experiment is not high enough to trigger the NO photorelease by direct photolysis.Although the concentration of VTP was 40-fold lower than that of NBF-NO, this latter is transformed almost quantitatively into NBF upon red light irradiation.This finding highlights another remarkable point of this strategy: the photocatalytic nature of the photosensitization process.The negligible spectral changes observed in the absorption region of VTP   Please do not adjust margins Please do not adjust margins beyond 600 nm (see Fig. 2A) suggest only a minor consumption of this PS, in excellent agreement with the photocatalytic mechanism.Analogously to VTP, the NO release was also photosensitized by the red-light irradiation of THP, another porphyrinic PS known to generate its low and long-lived triplet state upon light irradiation. 31HP is water insoluble but becomes well soluble under its photoresponsive monomeric form within PLM.Co-encapsulation of NBF-NO leads to supramolecular assemblies with a hydrodynamic diameter of ca.32 nm and a PI of 0.18.The spectroscopic and photochemical results obtained are illustrated in Fig. 4. Also in this case, the absorption profile of this ternary nanoassembly (spectrum a in Fig. 4A) matches well the arithmetic sum of the spectra of the individual encapsulated components, accounting for negligible intra/inter chromophoric aggregation.The absorption spectral changes observed upon red light irradiation of the sample under anaerobic conditions are characterized by well-defined isosbestic points, indicating a clean photochemical transformation as for NBF-NO/VTP case.The absorption profiles show the bleaching of the absorption bands in the 390 and 280 nm region and the simultaneous formation of the intense absorption band at ca. 470 nm, typical for the stable photoproduct NBF.The presence of oxygen did not affect the nature of the photolytic process but slightly affected the phototransformation rate due to the quenching of the THP triplet state (see inset Fig. 4A).Fig. 4B shows the direct evidence for the photosensitized NO release from the nanoassembly, which strictly depends on the presence of the red light irradiation.The emission of the optical reporter NBF is visible even to naked eye (Fig. 4C) and gives easily readable information about the NO generated.A representative result regarding the role of NBF as NO reporter is shown in Fig. 4D.The increase of the green fluorescence emission is related to the amount of photoreleased

C)
Please do not adjust margins Please do not adjust margins NBF-NO is well soluble in ME, and its co-encapsulation with either VTP or THP leads to nanoassemblies with similar diameters of ca.33 and 31 nm, respectively and PI of ca.0.11 (Fig. 5A).The results obtained with both red-absorbing PSs were very similar to those already found with PLM and some representative data are summarized in Fig. 5B-D.Fig. 5B shows the absorption spectral changes observed in the case of NBF-NO co-encapsulated with VTP.
The spectral evolution confirms the formation of the NBF as the sole stable photoproduct with its absorption maximum at ca. 470 nm.Besides, negligible spectral modifications were observed in the region of the Q band of VTP beyond 500 nm, according to the photocatalytic photosensitization process.A similar spectroscopic scenario was observed for THP (data not shown).As reported in the inset of Fig. 5B, the photochemical transformation sensitized by both VTP and THP was only in part quenched by molecular oxygen and the NO release under aerobic conditions and red-light irradiation was again confirmed by its direct monitoring (Fig. 5C).Finally, as reported in Fig. 5D, the green emission of the NBF was very intense and visible to naked eye also in this nanocarrier, and its fluorescence decay was a clean mono-exponential with a lifetime of ca. 10 ns (see Fig. 5D).These findings confirm the capability of NBF to act as a NO fluorescent reporter also in ME.
The validity of the photosensitization strategy to trigger NO release with hydrophilic PSs absorbing red light was finally tested with poly-CD, a class of branched polymeric nanocarriers made of CD units crosslinked through the epichlorohydrin crosslinker agent 33,34 .Due to nanodomains with different sizes and polarity, these polymers exhibit high water solubility and can solubilize and stabilize a wide range of guests much more effectively than monomeric CDs. 33,34][37][38] This allows to extend our strategy also to a PS with hydrophilic features such as ZnPCS (see Scheme 1).ZnPCS is a well-known watersoluble PS for PDT that exhibits an absorption band in the red region at 635 nm (spectrum e in Fig. 1).However, under these conditions, ZnPCS is self-aggregated and non-responsive to light [39][40][41] , resulting in the ineffective population of its lowest triplet state, which is the indispensable intermediate for the photosensitization mechanism.
As already demonstrated in our previous works, poly-CD significantly breaks the self-aggregation of ZnPCS [35][36][37] , encouraging the entangling within the polymeric network as a photoresponsive monomeric form in a satisfactory amount.
Co-encapsulation of NBF-NO and ZnPCS within a suspension of poly-CD leads to a nanoassembly ca. 25 nm in diameter.Its absorption spectrum (spectrum a in Fig. 6A) clearly shows a new absorption band with  max = 680 nm, typical of the monomeric species of ZnPCS. 39Based on the absorbance of this band and the molar absorptivity of the monomeric form, a monomerization degree of ca.
30 % can be estimated.According to the literature, entrapment of the monomeric ZnPCS can be favoured by the 3D structure of the  Please do not adjust margins Please do not adjust margins branched polymer in which the high local concentration of the CD nanocavities in the crosslinked network may act cooperatively in the disruption of the aggregate forms 42 .Irradiation of this ternary complex with red light led, also in this case, to the unambiguous formation of the NBF characterized by the formation of its characteristic absorption at 470 nm and the simultaneous release of NO (inset Fig. 6A).The green, fluorescent properties of NO were also preserved in this nanocarrier as demonstrated by the remarkable increase of the fluorescence emission upon red light irradiation (Fig. 6B).The absorption and spectral evolution did not change in the presence of oxygen but, analogously to the previous systems, the photoreaction rate was partially slowed down, according to the triplet-mediated photosensitization (inset Fig. 6B).An essential point of this work that deserves to be discussed further is the effect of oxygen on the efficiency of NO photorelease.As illustrated above, in all systems investigated, the phototransformation rate of NBF-NO generating NO is in part slowed down by molecular oxygen.This is reasonable since oxygen is a typical triplet quencher.Usually, this diffusional-controlled collisional process leads to the formation of singlet oxygen ( 1 O 2 ) the key species for PDT. 28The most suitable method to detect 1 O 2 is monitoring its typical and very diagnostic phosphorescence in the near-IR spectral window, which exhibits a maximum at 1270 nm 43 .As reported in Fig. 7, 1 O 2 is photogenerated by all PSs when individually encapsulated in the nanocarriers.In contrast, negligible amounts of 1 O 2 are observed when the PSs are co-encapsulated with NBF-NO.These findings demonstrate that, under the adopted experimental conditions, NBF-NO is a highly competitive quencher with molecular oxygen, permitting the photosensitized NO release to occur even under aerobic conditions, although at a slightly slower rate.This competitive quenching by NBF-NO can be the result of two opposite effects that are: i) an increase in the rate constant for the donor/acceptor pairs (PS/NOPD) confined in a restricted space like the host nanoenvironment, typically due to the high local concentration of the reactants 44 ; ii) a reduction of the quenching constant of the triplet state by the molecular oxygen typically attributable to a shielding effect by host nanocarriers from the external environment. 45,46

Conclusions
This work demonstrates the validity of a supramolecular strategy to trigger NO release from an otherwise blue-light activatable NOPD with the much more biocompatible and highly tissue-penetrating red light.This occurs through a supramolecular photosensitization process mediated by the lowest triplet state of different PSs coencapsulated with the NOPD in different biocompatible carrier systems and leads to an improvement of about 300 nm towards a longer excitation wavelength.The process occurs catalytically both under anaerobic and aerobic conditions.It is always accompanied by the formation of a highly green, fluorescent stable photoproduct, which acts as an optical reporter to detect NO release in real-time.A remarkable point of this work is that the proposed strategy does not require any chemical modification efforts on the NOPD used or any excitation with sophisticated two-photon irradiation sources.Studies Please do not adjust margins Please do not adjust margins addressed to bio-applications of the systems presented herein will be performed in our laboratories in the future.

Samples preparation
Polymeric micelles (PLM).Empty micelles were prepared using the thin-film hydration method [30].Briefly, 40 mg of Pluronic® (20 mg of P123 and 20 mg of F127) were dissolved in absolute ethanol (4 mL) in a round-bottom flask.Then, the solvent was evaporated by rotary evaporation (35 °C, 25 min) to obtain a film.The film was left under vacuum overnight to remove residual solvent.After that, the dried film was hydrated with 4 mL of water, and the material was sonicated (10 min) giving a micellar solution.The PSs were added by employing the thin-film method: briefly, an ethanolic stock solution was evaporated and stirred with the micelles overnight.Then, ca. 1 mg of NBF-NO was added to the previously prepared micelles.The sample was stirred for 4 h at room temperature and filtered (0.22 μm filters, RC Chemtek, Italy) to remove the unincorporated components or possible large cylindrical aggregates formed by P123.The actual concentration of the loaded molecules was optimized by dilution with the solution of empty micelles and determined by UV-vis spectrophotometry.

Microemulsions (ME).
An aliquot of NBF-NO and PSs stock solutions in THF were mixed in appropriate ratios, dried and then dissolved in 0.25 mL of Labrafac TM Lipophile WL 1349 under stirring.Thereafter, 0.5 mL of Kolliphor TM HS 15, previously warmed at 40°C, were added to the previous solution and stirred for 10 minutes.Thereafter, 4.25 mL water were added, and the sample was cooled down to room temperature and left to stir (600 rpm) for 30 minutes.The optically transparent resulting ME was stabilized overnight in the fridge.
Poly-CD.Poly-CD (2 mg mL -1 ) was added to an aqueous solution of the PS.The resulting solution was stirred for 24 h.Then, ca. 1 mg of NBF-NO was added and left to stir for 4 h in the dark.

Instrumentations
UV-Vis spectra absorption and fluorescence emission spectra were recorded with a Perkin Elmer spectrophotometer (mod.Lambda 365) and a Spex Fluorolog-2 (mod.F-111) spectrofluorimeter, respectively, using either quartz cells with a path length of 1 cm.Fluorescence lifetimes were recorded with the same fluorimeter equipped with a TCSPC Triple Illuminator.The samples were irradiated by a pulsed diode excitation source Nanoled at 455 nm.The kinetics were monitored at 540 and the solvent was used to register the prompt at 455 nm.The system allowed measurement of fluorescence lifetimes from 200 ps.The exponential fit of the fluorescence decay was obtained using equation (1): Steady-state irradiation experiments were performed in a thermostated quartz cell (1 cm pathlength, 3 mL capacity) under gentle stirring using a LED source at  = 630 nm.The photolysis experiments under anaerobic conditions were performed by deoxygenating the solution by bubbling with a vigorous and constant flux of pure nitrogen (previously saturated with solvent).Direct monitoring of NO release for samples in solution was performed by amperometric detection with a World Precision Instrument, ISO-NO meter, equipped with a data acquisition system, and based on direct amperometric detection of NO with short response time (< 5 s) and sensitivity range 1 nM -20 µM.The analog signal was digitalized with a four-channel recording system and transferred to a PC.The sensor was accurately calibrated by mixing standard solutions of NaNO 2 with 0.1 M H 2 SO 4 and 0.1 M KI according to the reaction (2): Irradiation was performed in a thermostated quartz cell (1 cm pathlength, 3 mL capacity) using a continuum red laser at  exc = 671 nm (100 mW) having a beam diameter of ca.1.5 mm.NO measurements were carried out under stirring with the electrode positioned outside the light path to avoid NO signal artifacts due to photoelectric interference on the ISO-NO electrode.
The NIR luminescence of 1 O 2 at 1.27 µm results from the forbidden transition 3  g - 1  g .This steady-state emission was registered with the same spectrofluorimeter as above equipped with a NIR-sensitive liquid nitrogen-cooled photomultiplier, exciting the air-equilibrated samples with the above continuum laser with  exc = 671 nm (200 mW). 1 O 2 emission was registered in the D2O solution.
Hydrodynamic diameter (DH), polydispersity index (PdI), and zeta potential (ζ) of the NPs were determined on a Zetasizer Nano ZS (Malvern Instruments Ltd, Malvern, UK).Measurements were performed at a temperature of 25°C.

Fig. 1
Fig. 1 Absorption spectra of NBF-NO (a), NBF (b), VTP (c), THP (d) and ZnPCS (e).Spectra a-d and spectrum e are recorded in MeOH and H 2 O, respectively.T = 25 °C.Spectra a, b and d are multiplied for a factor, for sake of clarity.

Fig. 3 (
Fig. 3 (A) NO release profiles observed for an air-equilibrated aqueous dispersions of PLM (1% w/v) co-encapsulating NBF-NO (60 µM) and VTP (1.5 µM) (a) and, as control, only VTP (b) upon alternate cycles of redlight irradiation at  ac = 671 nm.T = 25 °C.(B) Real-time fluorescence intensity monitored at  em = 530 nm and observed in an air-equilibrated dispersion of PLM (1% w/v) co-encapsulating NBF-NO (60 µM) and VTP (1.5 µM) keeping constant the excitation source at  exc = 420 nm and alternating ON/OFF cycles of the red light activation source at  ac = 630 nm.The schematic of the optical experimental set-up used is also shown.

Fig. 2
Fig. 2 (A) Absorption spectral changes observed upon exposure of an N 2saturated aqueous dispersion of PLM (1% w/v) co-encapsulating NBF-NO (60 µM) and VTP (1.5 µM) at  ac = 630 nm (ca.30 mW cm -2 ) for time intervals from 0 (spectrum a) to 28 min.The arrows indicate the course of the spectral profile with the illumination time.The inset shows the difference absorbance changes at  = 470 nm observed in N 2 -saturated () and air-equilibrated () conditions as a function of the irradiation time.(B) Evolution of the fluorescence emission spectra corresponding to the sample of Fig. 2A and recorded at  exc = 420 nm (isosbestic point).T = 25°C.
.u.) Wavelength (nm) This journal is © The Royal Society of Chemistry 20xx

Fig. 4 (
Fig. 4 (A) Absorption spectral changes observed upon exposure of an N 2 -saturated aqueous dispersion of PLM (1% w/v) co-encapsulating NBF-NO (30 µM) and THP (2 µM) at  ac = 630 nm (ca.30 mW cm -2 ) for time intervals from 0 (spectrum a) to min.The arrows indicate the course of the spectral profile with the illumination time.The inset shows the difference absorbance changes at  = 470 nm observed in N 2 -saturated () and air-equilibrated () conditions as a function of the irradiation time.(B) NO release profiles in air-equilibrated aqueous dispersions of PLM (1% w/v) co-encapsulating NBF-NO (30 µM) and THP (2 µM) (a) and, as control, only THP (b) upon alternate cycles of red-light irradiation at  ac = 671 nm.(C) Actual images of the sample as in (A) under illumination with a blue LED and different times of irradiation at  ac = 630 nm from 0 (left) to 60 min (right).(D) Correlation of the fluorescence increase at  em = 530 nm ( exc = 420 nm) observed upon red-light irradiation at  ac = 671 nm of sample as in (A) under aerobic conditions and the concentration of NO photoreleased measured by direct amperometric detection.I and I 0 represent the fluorescence intensities after and before irradiation, respectively.T = 25 °C.

Fig. 5 (
Fig. 5 (A) Hydrodynamic diameters of ME co-loaded with () NBF-NO (45 µM) and VTP (3 µM) or () NBF-NO (45 µM) and THP (4 µM).(B) Absorption spectral changes observed upon exposure of N 2 -saturated ME co-encapsulating NBF-NO (45 µM) and VTP (3 µM) at  ac 630 nm (ca.30 mW cm -2 ) for time intervals from 0 (spectrum a) to 9 min.The arrows indicate the course of the spectral profile with the illumination time.The inset shows the difference absorbance changes at  = 470 nm observed for N 2 -saturated (open symbols) and air-equilibrated (solid symbols) ME co-loaded with NBF-NO (45 µM) and VTP (3 µM) (circles) and ME co-loaded with NBF-NO (45 µM) and THP (4 µM) (square) as a function of the irradiation time.(C) NO release profiles observed for air-equilibrated ME co-loaded with (a) NBF-NO and VTP or (b) NBF-NO and THP and, for sake of control, only VTP (c) and THP (d), upon alternate cycles of red light irradiation at  ac = 671 nm.Same concentrations as in (B).(D) Representative actual images of the sample as in (B) acquired under illumination with a blue LED and different times of irradiation at  ac = 630 nm from 0 (left) to 10 min (right) and representative fluorescence decay and the related fitting recorded at the end of the irradiation and monitored at  exc = 455 nm and  exc = 530 nm.T = 25 °C.
This journal is © The Royal Society of Chemistry 20xx

Fig. 6 (Fig. 7 1
Fig. 6 (A) Absorption spectral changes observed upon exposure of an N 2saturated aqueous dispersion of poly-CD (2 mg mL -1 ) co-encapsulating NBF-NO (30 µM) and ZnPCS (5 µM of monomer) at  ac = 671 nm for time intervals from 0 (spectrum a) to 15 min.The arrows indicate the course of the spectral profile with the illumination time.The inset shows NO release profile observed for an air-equilibrated poly-CD aqueous dispersion as above upon alternate cycles of red light irradiation at  ac = 671 nm.(B) Evolution of the fluorescence emission spectra corresponding to the sample of Fig. 6A and recorded at  exc = 420 nm.The inset shows the difference intensity changes at  em = 530 nm observed in N 2 -saturated () and air-equilibrated () conditions as a function of the irradiation time.T = 25°C.
32, measured by its direct detection.Analogously to what was already found using VTP as PS, NBF-NO is transformed almost quantitatively into NBF upon red light irradiation of THP despite the concentration of this PS being ca.15 fold smaller, in excellent agreement with the photocatalytic nature of the photosensitization process.The feasibility of the photosensitized NO release from NBF-NO by the hydrophobic VTP and THP was then tested in ME as an example of a biocompatible nanocarrier with features different from PLM. ME are single-phase, optically isotropic nanocarriers made of oil, water, and surfactants with sizes below 100 nm and high thermodynamic stability.In recent years ME have gained increasing attention in the pharmaceutical field due to their capability to solubilize and deliver highly lipophilic compounds that remain mainly confined in the apolar phase.32MEtested here are made of LabrafacTM Lipophile WL 1349 and Kolliphor TM HS15, two lipophilic components able to solubilize poorly water-soluble molecules.The ME is spontaneously formed under low mixing rates from LabrafacTM Lipophile WL 1349/Kolliphor HS15 mixture and water at appropriate ratios (see experimental).