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Applied and Environmental Microbiology, April 2009, p. 1932-1937, Vol. 75, No. 7
0099-2240/09/$08.00+0 doi:10.1128/AEM.01892-08
Copyright © 2009, American Society for Microbiology. All Rights Reserved.

The Robertson Trust Laboratory for Electronic Sterilisation Technologies, University of Strathclyde, 204 George Street, Glasgow, Scotland
Received 14 August 2008/ Accepted 28 January 2009
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The focus of the present study, however, concerns the photoinactivation of bacterial cells without the involvement of an applied photosensitizer. Previous studies have shown that exposure to visible light, more specifically, blue-light wavelengths, causes inactivation of certain bacterial species, including Propionobacterium acnes, Helicobacter pylori, and some oral pigmented bacteria (1, 8, 22). This inactivation mechanism, known to be oxygen dependent (6), is thought to be a result of the photoexcitation of naturally occurring endogenous porphyrins, which act as endogenous photosensitizers within the bacterial cells. This porphyrin excitation leads to energy transfer and, ultimately, the production of highly cytotoxic, oxygen-derived species, most notably, singlet oxygen (11, 26).
Previous work has demonstrated that Staphylococcus aureus can be photodynamically inactivated using 400- to 420-nm visible-light, with maximum visible-light inactivation at 405 nm (13, 9, 10, 14), through an oxygen-dependent process (15). This inactivation of S. aureus is thought to be the result of a porphyrin-mediated process similar to that demonstrated with P. acnes. A previous study by Maclean et al. (14) utilized a broad-spectrum xenon white-light source combined with a range of optical filters to identify the sensitivity of S. aureus to wavelengths of light within the visible region. The present study investigates specifically the use of 405-nm light as the inactivating wavelength and also extends the scope of previous studies by producing new information on the sensitivities of a range of bacterial pathogens to the bactericidal effects of 405-nm light.
The inactivating light used in the present study was generated from 405-nm light-emitting diodes (LEDs). Investigations were carried out on the use of the 405-nm light from the LED array source for the inactivation of methicillin-resistant S. aureus (MRSA) and a range of other important nosocomial bacterial pathogens—both gram-positive and gram-negative types—in the absence of any chemical pretreatment. The results are discussed with regard to the possible cellular mechanisms involved in this light-based inactivation and to the potential use of this method for environmental decontamination applications in both clinical and nonclinical environments.
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View this table: [in a new window] |
TABLE 1. Microorganisms and associated growth mediaa
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LED light source.
High-intensity 405-nm light was achieved with the LEDs in the form of a close-packed rectangular array of 99 individual LEDs in an 11 by 9 matrix. The light of these 405-nm LEDs is generated in the active region of an InGaN/GaN semiconductor junction. These arrays (OD-405-99-070) are produced by OptoDiode Corp (CA). The emission spectrum of the 405-nm LED array is shown in Fig. 1. It can be seen that the center wavelength for maximum emission is close to 405 nm, and the bandwidth is
10 nm at full-width half-maximum. The LED array was bonded to a heat sink and fan to minimize the temperature of the semiconductor junction. The junction temperature was maintained at around 30°C, well below the specified maximum operating temperature of 100°C. This arrangement also ensured that the heat produced by the complete light system was low and had no effect on the test samples exposed to the 405-nm light. The arrangement was mounted in a polyvinyl chloride housing designed to fit on top of a 12-well microplate (without lid), with the LED array positioned directly above a single sample well. The LED array was powered by a direct current supply with the output controllable in the range 0 to 3 A and 0 to 15 V. For all experiments the current was set to 0.5 ± 0.05 A at a voltage of 11.2 ± 0.1 V.
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FIG. 1. Emission spectrum of 99-LED array.
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The distance between the sample and the LED array was approximately 2 cm, and at this distance an irradiance of around 10 mW/cm2 at the surface of the liquid was recorded using a radiant power meter. This procedure was followed for (i) exposure of all bacterial strains used in the study (as in Table 1) and (ii) exposure of S. aureus suspensions at different population densities.
The experimental arrangement was such that no build-up of heat occurred around the light source or was transmitted to the liquid sample. The heat sink and fan bonded to the LED array allowed heat to be easily dissipated, and the LED housing was designed such that it included air vents enabling sufficient ventilation around the light source and sample container, thereby preventing any heat build-up. Temperature measurements of the 2-ml sample volume taken every 30 min throughout the duration of long exposure times (up to a 360-min duration) showed minimal temperature variation, with a mean temperature of 27 ± 1°C.
In order to examine quantitatively the inactivation process, it was necessary to account for any attenuation of the irradiance of the 405-nm light as it passed through a bacterial sample; attenuation is a result of light absorption and scattering. By allowing for attenuation, a mean value for the irradiance through the sample could be determined. Little attenuation in the PBS itself is likely to occur since its optical properties are similar to water or seawater, and the attenuation in these for a wavelength of 405 nm and a depth of 7 mm is less than 0.2% (21). Bacteria suspended in the PBS, on the other hand, will cause some degree of absorption and scattering of the 405-nm light.
Attenuation by the samples used in the study was examined by measuring the irradiance as the light entered the surface of the sample and comparing that value with the irradiance immediately below the sample depth of 7 mm, after allowing for the transmission loss through the base of the sample dish. These measurements showed that for samples containing bacterial populations of 107 CFU/ml and less, no measurable attenuation occurred. For the 109 CFU/ml sample, however, the 10-mW/cm2 irradiance at the sample surface was reduced to 5.6 mW/cm2 after passing through the 7-mm sample depth. Light attenuation through a transparent medium follows an exponential relation referred to as Lambert's law (4), and is written as follows: I(x) = I(0)e–kx, where I(x) and I(0) are the irradiances at the sample surface and at the sample depth x, respectively, and k is the attenuation coefficient. Using the above measurements of irradiance allows k for the 109-CFU/ml sample to be calculated as 0.083 mm–1. The mean value of the irradiance
through the sample can now be calculated by applying the integral mean value theorem, as follows (20):
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of 7.6 mW/cm2, and this is the value of irradiance used in the analysis of the results for inactivation of the 109-CFU/ml sample.
Statistical analysis.
Each data point on the graphs represents the results from at least two independent experiments, with a minimum of triplicate samples examined for each experiment. These results are documented as mean values with standard deviations included. Significant differences in the results were calculated at the 95% confidence interval using analysis of variance (one way) with Minitab, version 15, statistical software.
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FIG. 2. Results of 405-nm light inactivation of MRSA and other medically important gram-positive bacteria at an irradiance of 10 mW cm–2.
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FIG. 3. Results of 405-nm light inactivation of a range of medically important gram-negative bacteria at an irradiance of 10 mW cm–2. Also included is the inactivation curve for the gram-positive bacterium E. faecalis, which shows a significant inactivation effect after a 240-min exposure.
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The absolute dose in J/cm2, given by the irradiance (W/cm2) times the exposure time (in seconds), and the mean germicidal efficiency, defined as the log10 reduction of a bacterial population [log10(N/N0)] by inactivation per unit dose in J/cm2, for bacterial inactivation was calculated. Details of the inactivation parameters, including germicidal efficiencies, for all bacteria investigated following exposure to the 405-nm light are given in Table 2. S. aureus NCTC 4135 displayed the highest level of inactivation, and the lowest germicidal efficiency was shown by E. faecalis.
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TABLE 2. Energy densities and germicidal efficiencies for the inactivation of a range of bacterial species using narrow-spectrum 405-nm light
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FIG. 4. Results of 405-nm light inactivation of S. aureus suspensions with different starting populations.
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The inactivation curves shown in Fig. 2, 3, and 4 have a shape consistent with those obtained in an earlier study (14), where S. aureus was inactivated using visible light of a wavelength greater than 400 nm. Visible-light inactivation—as established for other bacteria such as P. acnes, H. pylori, and some black-pigmented bacteria (1, 8, 22)—has been credited to the photostimulation of endogenous intracellular porphyrins by visible light in the wavelength region of 400 nm to 500 nm and, more specifically, 400 nm to 420 nm in the cases of P. acnes and H. pylori (1, 8). Stimulation of these porphyrins leads to the production of reactive species, predominantly singlet delta oxygen (1O2), which is a well-recognized trigger of cell death (11).
A study by Nitzan et al. (17), which exposed bacteria pretreated with
-aminolevulinic acid (
-ALA) to 407- to 420-nm blue light, proposed that the different photoinactivation rates for the various bacteria examined (Staphylococcus, Streptococcus, Bacillus, Escherichia, Acinetobacter, and Aeromonas) were the result of the types of porphyrins produced in the different bacterial cells. They determined the porphyrins produced in a range of gram-positive and gram-negative bacteria upon induction with
-ALA and found that the predominant porphyrin produced in both S. aureus and Staphylococcus epidermidis was coproporphyrin, whereas there was no predominant porphyrin produced in the gram-negative E. coli, Acinetobacter, and Aeromonas strains. The amount of coproporphyrin produced by the staphylococcal strains was two to three times higher than in the gram-negative strains. Nitzan et al. reported that Streptococcus faecalis, reclassified as E. faecalis (19), did not demonstrate any inactivation for a dose of 100 J/cm2. This is in agreement with the present results (Fig. 2 and 3), where inactivation of E. faecalis was observed only for doses above this value.
In the present study, where no photosensitizing agent was used, the high level of photoinactivation of staphylococcal strains is also likely due to the presence of high levels of coproporphyrin, photosensitized through blue-light illumination. Two other results lend support to this conclusion. One is that P. acnes, which is readily inactivated by visible light through photostimulation of endogenous porphyrins, also contains high levels of coproporphyrin (16), and the other is that S. aureus inactivation through exposure to visible light has been found to be an oxygen-dependent process (15). Some of the variation in germicidal efficiency between bacteria (Fig. 3) may follow from the use of a source of narrow spectral distribution. Because different bacteria produce different porphyrins and because the peak absorption wavelengths of these porphyrins may differ, different wavelengths may be required for their optimum photostimulation. It must also be noted that the bacteria used in the present study were produced under laboratory cultivation conditions and that the levels of cellular constituents such as porphyrins as well as the physiological status of the cells may differ considerably from bacteria that are found in the natural environment, such as those that have been shed from a mammalian host.
The general result from the present study, that visible-light inactivation of gram-negative bacteria is much less efficient than the inactivation of gram-positive bacteria, agrees with results obtained by several other workers in studies involving bacteria pretreated with
-ALA (17, 18, 25, 23). These studies with
-ALA used a range of light sources including blue light, 630-nm laser light, and white light.
The results of the present study, compared to the similar results of previous studies, add strength to the probability that the inactivation of the bacteria used in this study through exposure to 405-nm light is the result of the photostimulation of endogenous porphyrin molecules. However, a limitation of the current study is that this aspect was not specifically investigated, and further work is required to fully elucidate the exact role of porphyrins in the inactivation process resulting from exposure to 405-nm irradiation. In addition to this, we are currently developing a mathematical model for inactivation through exposure to 405-nm light, based on the inactivation kinetics of the microorganisms used in the present study.
Visible-light inactivation of bacteria is a much less efficient process than is ultraviolet light inactivation. For example, Wang et al. (27) examined the UV inactivation of E. coli as a function of wavelength and calculated a maximum germicidal efficiency of 430 log10 per J/cm2 at a wavelength of 270 nm. This compares with the highest value of germicidal efficiency found in the present work with 405-nm blue light (for a 105-CFU/ml population density of S. aureus) of 0.14 log10 per J/cm2. In spite of the three orders of magnitude difference in germicidal efficiency, visible-light inactivation has clear advantages in terms of its ease of use and substantially greater safety. In addition to safety benefits, prolonged exposure of materials to 405-nm visible light would not induce the problematic levels of photodegradation that are associated with similar periods of exposure to UV light, particularly in the UV-C region of around 254 to 260 nm typically used with germicidal UV lamps.
A method that can inactivate a wide range of medically important microorganisms, including MRSA, using exposure to visible light and no requirement for pretreatment has potential for widespread application. Further development of this 405-nm narrow-spectrum illumination method could lead to potential applications as decontamination systems for air, contact surfaces, and medical instruments within the clinical environment. Due to visible light's much greater operational safety than UV light, an attractive potential method of environmental decontamination could involve the continuous irradiation of clinical areas, in the presence of patients and staff, with light of the appropriate photodynamic wavelengths in order to contribute to the control of infections in hospitals and other clinical environments. The broad spectrum of the bactericidal effect of the 405-nm-centered wavelengths against a wide range of bacteria also suggests other possible applications such as providing additional measures for controlling food-borne pathogens and food spoilage bacteria as well as for possible applications in water treatment and disinfection industries.
Although the present study has substantially extended the range of bacteria that have been shown to be susceptible to 405-nm visible light, much more work is required to establish if this type of light sensitivity is a widespread phenomenon among diverse types of bacteria. The sensitivity of Mycobacterium spp. would, for example, be of considerable interest due to the medical importance and environmental survival and persistence characteristics of these organisms. It would also be of interest to determine whether types of bacteria that are found in environments that are normally exposed to natural illumination also show similar levels of sensitivity to irradiation around 405 nm or if these types have developed protective features or mechanisms to counteract the inactivating effects of these visible-light wavelengths.
Published ahead of print on 6 February 2009. ![]()
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-aminolaevulinic acid and subsequent bacterial photoeradication. Laser Med. Sci. 14:269-277.[CrossRef]
-Aminolaevulinic acid-induced porphyrin synthesis and photodynamic inactivation of Escherichia coli B. J. Photochem. Photobiol. B 50:8-17.[CrossRef][Medline]
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