Nicola Cusick and
Holger Schönherr
*
Physical Chemistry I & Research Center of Micro- and Nanochemistry and (Bio)Technology (Cμ), Department of Chemistry and Biology, School of Science and Technology, University of Siegen, 57076 Siegen, Germany. E-mail: schoenherr@chemie.uni-siegen.de
First published on 4th June 2025
Utilised for decades in cancer therapy, the application of photosensitisers in antimicrobial photodynamic therapy is now well explored. In a smart wound dressing, an externally triggered antimicrobial strategy would enable on-demand infection eradication. Hence, in this work, the light-initiated production of reactive oxygen species from photosensitiser-loaded nanocarriers was explored. Such systems enable highly localised delivery of photosensitiser, without associated “dark toxicity” effects. The amphiphilic block copolymer PEG-block-PLA was synthesised via ring-opening polymerisation in the melt. Via the solvent shift method, the polymer was self-assembled into nanosized vesicles encapsulating Phloxine B, a commercial water-soluble photosensitiser. In vitro bacteria experiments with Phloxine B-loaded vesicles relied on localised illumination with green light (530 nm, 4 mW cm−2, 15 minutes) to generate 1O2, killing the bacterial cells. A 6.8log10 reduction in CFU mL−1 for Staphylococcus aureus and a 4.7
log10 reduction in CFU mL−1 for Pseudomonas aeruginosa are reported. Incorporation of these vesicles into a support matrix in combination with a reporter dye could provide a pathway towards promising smart wound dressings.
Antimicrobial resistance to light-based approaches, such as visible light activation of photosensitisers (PSs), or the use of UVC light, are rarely reported.6,11,12 Antimicrobial photodynamic therapy (aPDT) using PSs therefore represents a viable alternative strategy to traditional antibiotics for the treatment of infected wounds. aPDT requires a PS, molecular oxygen, and light of an appropriate wavelength.11 The absorption of light by the PS followed by intersystem crossing results in the formation of the PS triplet excited state, which can interact with molecular oxygen to produce reactive oxygen species (ROS) via electron transfer (Type I) or energy transfer (Type II).13 These ROS cause oxidative stress to cells, hence PSs act as broad-spectrum antibacterial and antifungal killing agents.14 PDT is already clinically approved for multiple conditions, including a variety of cancers.15 The first clinically used PS, hematoporphyrin, was first used in the 1970s in the United States.3 Limitations of these first generation PSs, including short wavelength absorption and prolonged patient photosensitivity, lead to research into so-called second generation PSs with longer wavelength absorption.16 Such PSs are largely based on porphyrin, with absorption wavelengths >600 nm.17
The use of PDT to eradicate bacteria, aPDT, has received growing research interest in the previous two decades.18 It is particularly advantageous as it can provide localised treatment to fight infections caused by both Gram-positive and Gram-negative pathogens, as well as fungal and viral infections.8 A wide variety of PSs are available, with different chemical properties, degrees of hydrophilicity, and absorption maxima.19 A suitable PS can therefore be selected for a specific application. Halogenated xanthenes such as Rose Bengal possess large singlet oxygen quantum yields and are photoactivated in the visible light region.20 This is advantageous for superficial infection treatment, where light is not required to penetrate through tissue.21 However, as the diffusion of singlet oxygen is limited to a few hundred nanometres (estimations of ∼268 nm over 2 lifetimes in a cell have been reported),22 and it has a short half-life of ∼4 × 10−6 s in H2O, it is only cytotoxic to cells in the immediate vicinity.23,24 Therefore, the efficacy of aPDT depends on the localisation, and approaches in which photosensitisers are encapsulated or conjugated with targeting moieties are reported to enhance PS delivery by more accurate targeting to cells, but also by preventing PS aggregation in solution.7,25 These third generation photosensitisers are reported to overcome limitations of neat PS administration such as limited solubility, uncontrolled PS release, photo-bleaching and poor selectivity.9
Many PSs are inherently “theranostic” (therapeutic and diagnostic) as their fluorescence can be utilised in detection of pathogens.26 For the application of PSs in a wound dressing, it is likely that the PS would be located at the wound bed for a period of time and only irradiated upon the presence of infection. Hence, encapsulation is important to prevent contact of the PS with the initial small population of bacteria of a non-infected wound, which would provide time for bacteria to adapt and develop resistance.8 Moreover, diffusion of a PS-loaded carrier is much slower than the PS itself, providing a higher local concentration. It has been reported that aPDT nanosystems enable improved PS solubility, a reduction in the required PS concentration, controlled release, increased penetration and selectivity.9,27 For example, lipid nanoparticles encapsulating the PS toluidine blue O resulted in increased PS uptake by S. aureus (ATCC 6538), P. aeruginosa (ATCC 27853) and E. coli (ATCC 25922), more sustained 1O2 generation and improved bacterial inactivation due to improvements in solubility.25 However, CFU reductions were no greater than 4log10.22 To improve stability, versatility and robustness of such systems, polymer-based nanocarriers have also been explored for delivery of PSs.28,29 Amphiphilic block copolymers, in which a hydrophilic and hydrophobic chain are covalently bonded, provide a facile approach to self-assemble kinetically trapped nanostructures.30 These structures are reported to be more stable, mechanically stronger and less permeable to small water-soluble molecules than liposomes.31
Often, the biocompatible polymer poly(ethylene glycol) (PEG) is utilised as the hydrophilic block as it is hypothesised to provide a stealth function, prolonging circulation times by resisting protein adsorption.32,33 As previously reported, the use of polyesters such as poly(caprolactone) (PCL) or poly(lactic acid) (PLA) as the hydrophobic block can provide an enzyme-responsive function to the vesicles; the ester bonds are cleaved by proteases and lipases.34,35 A biodegradable polymersome composed of polyester-containing block copolymers can be degraded in the biological environment in the presence of esterases, releasing the cargo molecules via simple ester hydrolysis.32 For example, the lipophilic PS hypocrellin A (HA) was loaded into PEG-b-PCL micelles and the lipase-dependent release of HA in the presence of MRSA was observed.33 Irradiation (λ = 470 nm, 90 mW cm−2, 60 minutes, 324 J cm−2) afforded complete killing of the pathogen, but had a higher minimum inhibitory concentration compared to neat HA in vitro.34
Previous work in our group highlighted the encapsulation of the hydrophobic photosensitiser Ru(Phen)3 in PEG-b-PLA micelles and vesicles.36 A reduction of at least 4.7log10 in CFU mL−1 was reported against P. aeruginosa upon irradiation (λ = 455 nm, 3 mW cm−2, 30 minutes, 5.4 J cm−2) of vesicle suspensions with high Ru(Phen)3 concentrations (187 μM).36 As greater photodynamic inactivation was observed with vesicular rather than micellar suspensions, in this current work the length of the hydrophobic chain was increased to obtain vesicular structures, which can also be used as carriers for hydrophilic molecules owing to the aqueous lumen.37 To avoid the use of expensive and potentially toxic heavy metals, alternative organic photosensitisers were investigated.38 Phloxine B (PhB) is a hydrophilic xanthene dye approved for use as a colour additive in the US and Japan that is also known to act as a photosensitiser.39,40 As PhB does not absorb in the higher wavelength range of the visible region of the spectrum, it is a good candidate for superficial wound treatment.41 PhB has previously been incorporated into saponite-based films (PhB surface concentration ∼1.8 × 10−6 mmol cm−2) and was shown to provide an antibacterial effect against S. aureus with up to a 3
log10 reduction in CFU mL−1 after irradiation (green LEDs, 2.42 mW cm−2, 2.5 hours, 21.8 J cm−2).42 Polyurethane composites containing PhB afford a slow release of PhB. A 2
log10 reduction in CFU mL−1 was observed in the dark, attributed to the composite itself, with a further 2
log10 reduction after irradiation (green laser, λ = 532 nm, 100 mW, 120 s).43 However, encapsulation of PhB into polymersomes has not yet been reported. The aim of this study was to investigate the encapsulation of PhB into carriers composed of the biodegradable block copolymer PEG-b-PLA, and to investigate their potential to generate 1O2 and kill bacteria. This would enable highly concentrated PhB delivery at the target site.
In this work, a library of PEG-b-PLA block copolymers was synthesised and characterised with 1H-NMR spectroscopy and thermogravimetric analysis (TGA). The amphiphilic block copolymer was self-assembled into vesicles loaded with PhB, and characterised via Dynamic Light Scattering (DLS), Scanning Electron Microscopy (SEM) and Transmission Electron Microscopy (TEM). The PhB-loaded vesicles were then assessed for their ability to generate singlet oxygen using the sensor Singlet Oxygen Sensor Green (SOSG). Finally, incubation of the PhB-loaded vesicles with planktonic S. aureus and P. aeruginosa cultures, followed by irradiation for a short time with low-power green LEDs (4 mW cm−2, 15 minutes, 3.6 J cm−2) enabled determination of their antimicrobial efficiency. This system provides a rapid eradication of both clinically relevant wound infection pathogens with FDA-approved materials, highlighting a promising approach for combatting wound infections.
All solvents were used as purchased: dichloromethane (DCM, 99.9%) (Fisher Scientific, Germany), tetrahydrofuran (THF, 100%) (VWR, Germany), diethyl ether (99.5%) (Thermos Scientific, Germany), methanol (99.9%) (Sigma-Aldrich, Merck, Germany) and chloroform-d (CDCl3, 99.8 atom%) (Deutero, Germany).
Acrylic cuvettes and transparent flat-bottom polystyrene 96-well plates were purchased from Sarstedt (Germany), and cell culture 96 black half-area μ-clear well plates and 384-well plates from Greiner Bio-One (Germany). Glass NMR tubes (Boro 400-5-7) were purchased from Deutero GmbH (Germany).
Lysogeny broth (LB medium, 10 g per L tryptone, 5 g per L yeast extract, 10 g per L NaCl, pH 7.0 ± 0.2) and LB agar (10 g per L tryptone, 5 g per L yeast extract, 10 g per L NaCl, 15 g per L agar–agar, pH 7.0 ± 0.2) were purchased from Carl Roth GmbH (Germany). Phosphate buffer solution (PBS, pH 7.4) was prepared by dissolving a PBS tablet (Sigma-Aldrich, Merck, Germany) in 200 mL Milli-Q water. Simulated thin wound exudate (STWE) was prepared by dissolving sodium chloride (NaCl, 0.8298%, Sigma-Aldrich, Merck, Germany) and calcium chloride (CaCl2, 0.0368%, AppliChem, Germany) in Milli-Q water. Singlet Oxygen Sensor Green (SOSG) was purchased from Thermo Fischer Scientific (Germany), and Tris buffer (100 mM, pH 7.4) from Millipore (MA, USA).
Pseudomonas aeruginosa lab strain ATCC 19660 (isolated from sepsis in Lima, Peru, and purchased from LGC Standard GmbH (Germany)) and Staphylococcus aureus lab strain RN4220 (ATCC 35556; originally derived from NCTC 8325-4 via UV and chemical mutagenesis, purchased from Leibniz-Institut DSMZ GmbH (Germany)) were used in this study. All bacteria were grown in LB medium at 37 °C.
The synthesis of PEG-b-PLA was adapted from Tücking et al.44 Molar ratios were adjusted according to desired PLA chain length. Briefly, with amounts corresponding to a nominal PLA chain length of 500, mPEG (100 μmol) was added to stannous octoate (0.1 mL) at 80 °C and stirred. After heating to 130 °C, L-lactide (25 mmol) was added and the mixture was stirred for 30 min. After cooling to room temperature, the white solid obtained was dissolved in dichloromethane (∼10 mL) and recrystallised in ice-cold diethylether (>10× volume of solvent). The precipitate was centrifuged (6000×g, 10 min), the supernatant discarded, and the precipitate redissolved in dichloromethane. This process was repeated a further 4 times, and the final white solid product was dried overnight (40 °C, 5 mbar).
The number of repeat units in the hydrophobic block was determined by calculating the ratio of the integral of the proton signals of the mPEG to the PLA block. The integral of the mPEG protons at 3.64 ppm was normalised to 456 protons, assuming a Mn of 5000 g mol−1. The integrals of the proton signals for the PLA protons were divided by the number of protons in 1 PEG repeat unit to calculate the number of PLA repeat units.
Thermogravimetric analysis (TGA) was performed on a TGA Q50 V6.7 Build 203 (Universal V4.4A, TA Instruments). The sample was dried overnight at 5 mbar, filled into a platinum crucible, placed in the autosampler of the device, and equilibrated at 50 °C under nitrogen atmosphere. After equilibration, the temperature was increased (50 °C min−1) to 500 °C. The gas was then changed to oxygen to oxidise remaining organic residues and the temperature was increased (50 °C min−1) from 500 to 850 °C.
PhB concentration and encapsulation efficiency were determined via fluorescence spectroscopy. Emission spectra were recorded using a Varian Cary Eclipse spectrometer (Mulgrave, Victoria, Australia) at 25 °C. A calibration curve of PhB in water was created (λex/λem = 504/555 nm, 0–3.125 μM, R2 = 0.99) (Fig. S3†). The emission intensity of blank (water-filled) vesicles was subtracted from PhB-loaded vesicles, then PhB concentration inside the vesicle suspension (diluted to 5% v/v in Milli Q water) was determined by comparison with the calibration curve. This was also verified by comparison to the absorption calibration curve (0–50 μM, R2 = 0.99) (Fig. S4†). Encapsulation efficiencies were calculated as the ratio of the concentration of PhB in the final suspension relative to the initial PhB concentration.
The samples were observed via Field Emission Scanning Electron Microscopy (FESEM, Zeiss Ultra 55cv, Zeiss, Oberkochen, Germany) by drop casting a diluted vesicle suspension (1% v/v in Milli Q water) onto silicon wafers pre-cleaned with chloroform, ethanol, water and UV-ozone. To generate a conductive surface, samples were sputtered with gold for 30 s, corresponding to a ∼5.0 ± 0.5 nm thin gold layer. FESEM measurements were collected using the Inlens secondary electron detector, with an operation voltage of 5 kV. The images were analysed using ImageJ (software version 1.53r).
Transmission Electron Microscopy (TEM, FEI Talos F200X) images of samples drop casted onto copper grids (mesh 400) with ultra-thin carbon film (<3 nm) supported by lacy-carbon-film (Plano GmbH, Germany) were recorded using an acceleration voltage of 80–200 kV. The images were analysed using ImageJ.
The structures were also observed via epifluorescence microscopy, using an Axiovert 135 microscope equipped with an AxioCamMRm and Zen 2.3 lite software and a filter set with λex = 540–552 nm and λem > 590 nm (Carl Zeiss MicroImaging GmbH, Germany). The camera exposition time was 80 ms in brightfield, and 2000 ms with the filter set.
Radiant exposure (J cm−2) = irradiance (W cm−2) × exposure time (s) |
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Scheme 1 Ring-opening polymerisation of L-lactide with the macroinitiator mPEG114 and Sn(II) octoate as catalyst. |
The final products were characterised by 1H-NMR spectroscopy to determine the PLA block length. The 1H-NMR spectra (Fig. S1 and S2†) confirm the successful synthesis of the polymers, with characteristic proton signals for PEG and PLA blocks observed at 3.64 ppm (PEG), 1.56 ppm and 5.16 ppm (PLA). The ratios of the integrals of the PLA to PEG block proton signals were used to calculate the number average degree of polymerisation (Mn), and the hydrophobic block length (Table 1). The calculated chain length was close to the expected chain length (86–98% expected value).
Nominal PLA chain length, x | Mn/kg mol−1 | Hydrophobic block length/number of repeat units | ||
---|---|---|---|---|
Expected | Observed | Expected | Observed | |
100 | 12.2 | 11.6 | 100 | 92 |
150 | 15.8 | 15.3 | 150 | 143 |
300 | 26.6 | 26.2 | 300 | 294 |
400 | 33.8 | 32.9 | 400 | 389 |
500 | 41.0 | 40.1 | 500 | 488 |
Amphiphilic block copolymers can self-assemble into various morphologies depending on the composition of the initial polymer. The resulting morphology is dependent on the packing parameter, p, which is calculated by division of the volume of the hydrophobic chains by the hydrophilic headgroup area and hydrophobic tail length.16 Micelles are formed when p ≤ ⅓, and possess a hydrophobic core composed of hydrophobic tails, while the hydrophilic head group is in contact with the surrounding water. Vesicles are formed when 1/2 ≤ p ≤ 1, and are composed of a polymeric bilayer with hydrophilic head groups in contact with both the exterior and interior solvent, creating an aqueous lumen in which hydrophilic molecules can be encapsulated. In this work, the aim was to create a high local concentration of PhB by loading it into a carrier. Hence, the encapsulation of the hydrophilic PhB molecule was achieved via formation of vesicular structures, which provide a large lumen for higher loading capacity. To ensure vesicles were obtained in the self-assembly of PEG-b-PLA, the polymer with the longest hydrophobic PLA chain (and hence the largest p) was chosen for further studies.
As previously reported, gel permeation chromatography (GPC) was unsuccessful with this system due to the inherent differences in solubility of the two blocks.36 Hence, TGA was used to provide a weight average degree of polymerisation for the polymer with expected PLA chain length of 500. The TGA trace (Fig. S7†) shows distinctive mass losses at the decomposition temperatures of PEG (330–400 °C) and PLA (150–250 °C).46 The ratio of the residual weight lost at the characteristic decomposition temperatures was used to calculate the PLA block length and was in good agreement with the 1H-NMR data (Mw: 40.3 kg mol−1, PLA block length: 490 compared to Mn: 40.1 kg mol−1, PLA block length: 488 from 1H-NMR). Therefore, from hereon in, this polymer will be referred to as PEG114-b-PLA488.
The self-assembly of PEG114-b-PLA488 was achieved via nanoprecipitation. Here, the amphiphilic block copolymers are dissolved in a common solvent for both blocks, in this case THF. The addition of water, a non-solvent for the hydrophobic PLA chains, results in the formation of nanoassemblies via microphase separation.14,47 To encapsulate PhB, a 1 mM solution in Milli-Q water was used as the non-solvent.
The resulting suspensions were characterised by DLS, FESEM and TEM (Fig. 1). The distributions by number of the suspensions indicated an average hydrodynamic diameter of 230 ± 7 nm for PhB-loaded PEG114-b-PLA488 assemblies (Fig. 1a). The FESEM and TEM images (Fig. 1b and c) exhibit spherical features that are likely vesicles, according to the report of Reverchon et al., who studied very similar PEG-b-PLA polymers.48 These round features possess diameters (101 ± 16 nm) that are consistent with the DLS data. These images also confirm that the spherical shapes are largely retained upon drying, indicating structural stability of the assemblies upon drying.
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Fig. 1 (a) DLS particle size distribution by number, (b) FESEM and (c) TEM images of PhB-loaded PEG114-b-PLA488 vesicles (1% dilution in Milli-Q water). |
To confirm that PhB is encapsulated, fluorescence microscopy images were acquired. By overlaying the bright field and emission images, it is possible to visualise clusters of vesicles which contain the fluorescent PhB (Fig. 2). These fluorescent spots are not visible in water-loaded vesicles, confirming they are due to the presence of PhB (Fig. S8†).
To estimate the concentration of PhB in the final vesicle suspension, the fluorescence emission of the vesicle suspension (diluted to 5% v/v in Milli Q water) was measured and compared to the calibration curve of neat PhB in water (Fig. S9†). The concentration of PhB in the vesicle suspension was estimated to be 34 ± 1.6 μM, corresponding to an encapsulation efficiency of 3.4 ± 0.2% (Fig. S9b†). Attempts to quantify loading with UV-vis spectroscopy proved difficult as the scattering from the polymer shell in the vesicle suspension prevented any estimation of PhB concentration (Fig. S10†). Hence the absorption spectra were used only to confirm the presence of the dye in the suspension.
PhB is known to generate reactive oxygen species primarily via a Type II energy transfer from the triplet excited state to molecular oxygen, affording singlet oxygen, 1O2.18,42 Singlet Oxygen Sensor Green (SOSG) was therefore used as a probe molecule to confirm the production of 1O2. This non-fluorescent fluorescein-based probe reacts with 1O2 to produce an SOSG-endoperoxide which exhibits green fluorescence (Fig. S11†).49 The conversion of SOSG to SOSG-endoperoxide in the presence of PhB and PhB-loaded vesicles upon irradiation was monitored by measuring the fluorescence emission intensity at 528 nm. The impact of increasing irradiation time of PhB and PhB-loaded vesicles on 1O2 production was investigated (Fig. 3).
As controls, water and water-loaded vesicles were also irradiated in the presence of SOSG. Irradiation of SOSG (10 μM in Milli Q water) in the absence of a photosensitiser resulted in an increase in the fluorescence emission intensity over time, suggesting the fluorescein moiety itself is excited by the green light, forming 1O2 and self-converting to SOSG-endoperoxide.50 It has been reported that both the SOSG and the SOSG endoperoxide derivative can sensitise 3O2, generating more 1O2 and therefore further increasing SOSG fluorescence.25,51 For these reasons, SOSG was not used to quantify 1O2 production, only to qualitatively detect it. Irradiation of water-loaded vesicles showed a similar trend to SOSG alone, confirming the lack of 1O2 production from the polymer itself. However, the fluorescence intensity of PhB and PhB-loaded vesicles was up to 4-fold higher than the signal from the SOSG itself. This indicates that the irradiation of both neat dye and dye loaded vesicles generates 1O2, converting SOSG to SOSG-endoperoxide. Nevertheless, it can be observed in Fig. 3 that upon increasing irradiation times beyond 15 minutes, there is no further apparent 1O2 production, as has been observed with other systems.52 This saturation could be consistent with the consumption of all methylanthracene moieties or depletion of oxygen in the local environment.24 It could also be due to the visible light-induced degradation of PhB (Fig. S12†), resulting in fewer molecules available to sensitise molecular oxygen.53
To confirm the production of 1O2 in the presence of bacteria, the vesicle suspensions were pre-incubated for 15 minutes with S. aureus and P. aeruginosa in STWE. This industry standard medium, also referred to as solution A, is a good approximation to mimic a wound exudate.54,55 An increase in fluorescence emission at 528 nm, indicating an increase in 1O2 production, was detected upon irradiation of PEG114-b-PLA488 vesicle suspensions in the presence of both S. aureus and P. aeruginosa and SOSG (Fig. 4 and S13†). In comparison to the signal in the absence of bacteria, the emission after 15 minutes of irradiation in the presence of both S. aureus and P. aeruginosa is >2× higher. Such an increase has been observed before.36 This could be an indication that the PS is interacting with the bacteria, increasing the local concentration of 1O2 and therefore enhancing the SOSG signal. In addition, upon irradiation of PhB, the bacteria are under oxidative stress, triggering antioxidant reactions which generate reactive intermediates which may non-specifically activate SOSG.56 Moreover, the permeabilisation of bacterial membranes upon 1O2 treatment may facilitate SOSG staining, as has been observed in E. coli, creating environments with concentrated SOSG.57
The PhB-loaded vesicle suspensions were used as produced in antibacterial tests against S. aureus lab strain RN4220 and P. aeruginosa lab strain ATCC 19660. These strains were chosen as they are often reported to be resistant to antibiotic treatment; RN4220 is a methicillin-resistant S. aureus (MRSA) lab strain, a key target of aPDT treatment. Both bacteria were used at a starting concentration of ∼106 CFU mL−1, a concentration which is associated with increased infection risk in wound exudates, and the experiment was performed in the clinically relevant STWE.58 Both neat PhB and PhB-loaded vesicles were incubated in equal volumes with the bacteria and the CFU mL−1 after 15 minutes of irradiation (radiant exposure 3.6 J cm−2) or dark incubation were determined. Exposure to light irradiation in the absence of vesicles, or in the presence of water-loaded vesicles, had no effect on cultures of S. aureus or P. aeruginosa (Fig. 5 and S14†). Likewise, both neat PhB and PhB-loaded PEG-b-PLA vesicle suspensions caused no reduction in CFU mL−1 of S. aureus or P. aeruginosa in the dark. However, upon irradiation of neat PhB and PhB-loaded vesicles, there were no countable S. aureus or P. aeruginosa colonies observed (Fig. 5a). This represents a log reduction factor (LRF) of >4.8 for S. aureus, and >4.7 for P. aeruginosa.
The eradication of P. aeruginosa in these experiments was unexpected, as neat Phloxine B is commonly reported to be active only against Gram-positive bacteria.59 Gram-negative bacteria, including P. aeruginosa, are generally more difficult to kill due to their cell wall structure. Combination treatment of aPDT with chelating agents, antibiotics or antimicrobial peptides to permeabilise the cell wall and facilitate PS uptake has been proposed.60–62 The use of neat PhB to photodynamically inactivate P. aeruginosa has not yet been reported. In general, Gram-negative bacteria are often resistant to neutral and anionic PSs.62 Antimicrobial activity of Phloxine B has been achieved against Gram-negative bacteria in the presence of EDTA, a chelating agent which binds to cations holding the lipopolysaccharides (LPS) of the cell wall in place, which increases cell permeability and enables dye penetration.59 Possibly the Ca2+ ions in STWE in this experiment are permeabilising the LPS, a process known and used for decades in DNA transformation of cells.63 Moreover, the presence of Cl− counterions in the STWE may be providing a synergistic effect, as they can combine with the singlet oxygen to produce the longer-lived hypochlorite, ClO−, which can also have an antimicrobial effect.64,65
To investigate the extent of the antibacterial activity of the developed PhB-loaded vesicle systems, the experiment was repeated with increasing bacteria concentrations, 107 CFU mL−1 and 108 CFU mL−1. Increasing the S. aureus concentration did not limit the antibacterial activity of neat or encapsulated PhB upon irradiation (Fig. 6a and b), with still no colonies visible after irradiation (Fig. S15 and S16†). These data now provide a LRF of >6.8 (accounting for a LOD of 1.5log10 CFU mL−1), indicating that >99.9999% bacteria are eradicated after just 15 minutes. From Fig. 6c and d, it is evident that with higher P. aeruginosa concentrations, the ability of this concentration of PhB to eradicate the bacteria is limited, with a maximum LRF of 2, compared to the LRF of >4.7 when the inoculum is ∼106 CFU mL−1. This highlights the importance of early detection of P. aeruginosa infections for utilisation of PhB treatment. However, it is likely that longer irradiation times or more concentrated vesicle suspensions would enable killing of higher inoculum concentrations.
It is advantageous to eradicate both S. aureus and P. aeruginosa as polymicrobial wound infection is common; 27% of wounds in one study were diagnosed with a polymicrobial infection, most commonly S. aureus and P. aeruginosa.66 The susceptibility and antibiotic resistance patterns of different bacterial species and strains differs. Hence, multiple antibiotics would be required to treat one wound. With this approach, both Gram-positive and Gram-negative species could be eradicated with one treatment, using biocompatible polymer carriers which localise the PS. The lack of reported microbial resistance to aPDT is likely due to the short interval between PS administration and light irradiation, in which time there is no time to select for resistant strains.67 In addition, the success with a low-cost, low-power, non-coherent LED array enables treatment over a large area due to the wide illumination area relative to a laser light source, without causing damage to healthy tissue.19 Further work to optimise the concentration of Phloxine B inside the carriers with regards to the irradiation time will provide an “optimal” system with a low active concentration with the minimum treatment time.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5ra02238j |
This journal is © The Royal Society of Chemistry 2025 |