Inactivation of enveloped virus by laser-driven protein aggregation

Shaw-Wei D. Tsen; Travis Chapa; Wandy Beatty; Kong-Thon Tsen; Dong Yu; Samuel Achilefu

doi:10.1117/1.JBO.17.12.128002

10 December 2012 Inactivation of enveloped virus by laser-driven protein aggregation

Shaw-Wei D. Tsen, Travis Chapa, Wandy Beatty, Kong-Thon Tsen, Dong Yu, Samuel Achilefu

Author Affiliations +

Journal of Biomedical Optics, Vol. 17, Issue 12, 128002 (December 2012). https://doi.org/10.1117/1.JBO.17.12.128002

Abstract

Ultrafast lasers in the visible and near-infrared range have emerged as a potential new method for pathogen reduction of blood products and pharmaceuticals. However, the mechanism of enveloped virus inactivation by this method is unknown. We report the inactivation as well as the molecular and structural effects caused by visible (425 nm) femtosecond laser irradiation on murine cytomegalovirus (MCMV), an enveloped, double-stranded DNA virus. Our results show that laser irradiation (1) caused a 5-log reduction in MCMV titer, (2) did not cause significant changes to the global structure of MCMV virions including membrane and capsid, as assessed by electron microscopy, (3) produced no evidence of double-strand breaks or crosslinking in MCMV genomic DNA, and (4) caused selective aggregation of viral capsid and tegument proteins. We propose a model in which ultrafast laser irradiation induces partial unfolding of viral proteins by disrupting hydrogen bonds and/or hydrophobic interactions, leading to aggregation of closely associated viral proteins and inactivation of the virus. These results provide new insight into the inactivation of enveloped viruses by visible femtosecond lasers at the molecular level, and help pave the way for the development of a new ultrafast laser technology for pathogen reduction.

1. Introduction

Pathogen reduction (PR), which aims to proactively eliminate infectious agents from blood products, is an attractive strategy to address the threat of known and emerging pathogens and ensure the continued safety of the blood supply. However, the various PR methods explored to date suffer from limitations that prevent their widespread use and acceptance by the transfusion medicine community. Clinically tested PR techniques for human plasma include solvent-detergent (SD) treatment,¹ visible light-activated sensitizers such as methylene blue,² and ultraviolet (UV) light-activated photochemicals such as riboflavin and amotosalen.³^–¹¹ All current techniques involve the introduction of chemicals with risks of unknown or unpredictable side effects. These side effects include immune reactions, carcinogenicity, or loss of coagulation factors in the product, all of which can lead to adverse consequences in patients.¹² SD treatment is also limited because it cannot inactivate nonenveloped viruses, and thus is ineffective against many transfusion-transmitted pathogens, such as parvovirus B19 and hepatitis A virus (HAV).¹² Furthermore, with all of the above mentioned methods, the introduction and subsequent removal of chemicals is an additional step that adds to the cost of implementing the PR technology.

Short wavelength UV (UVC) radiation has been tested as an alternative, chemical-free PR technology. UVC radiation inactivates pathogens by DNA damage through dimerization of adjacent pyrimidines¹³ as well as generation of reactive oxygen species.¹⁴ UVC treatment has shown effects against certain viruses and bacteria.¹⁵^–¹⁷ However, there is already evidence of resistance to UVC among blood borne pathogens such as HIV.¹⁷ Moreover, UVC is strongly absorbed by proteins and has been shown to damage plasma components¹⁸ and cause platelet aggregation.¹⁹ Thus, there is a need to develop a new chemical-free PR technique with broader pathogen coverage and minimal effects on the blood product.

In this regard, ultrafast lasers in the visible and near-infrared range are a potentially ideal approach for PR. Visible/near-infrared ultrafast laser irradiation does not cause ionization effects that can damage the blood product. It does not introduce potentially toxic or carcinogenic chemicals, and thereby has minimal concern of adverse effects. Our group has recently shown femtosecond laser irradiation to be effective in inactivating (achieving 3 to 5 log reduction of) a broad spectrum of viruses,²⁰ including human immunodeficiency virus (HIV),²¹^,²² human papillomavirus (HPV),²² encephalomyocarditis virus,²³ M13 bacteriophage,²³^–²⁷ and tobacco mosaic virus (TMV).²² More importantly, femtosecond laser irradiation at sufficient power to kill the above mentioned viruses does not kill human cells²⁷ and does not appear to damage either bovine serum albumin (BSA) protein or single stranded DNA.²³

Human cytomegalovirus (HCMV) is a widespread pathogen responsible for multiple significant diseases. It is the leading viral cause of congenital diseases in newborns, a common cause of opportunistic infections in acquired immunodeficiency syndrome (AIDS) and transplant patients, and a potential risk factor in certain cardiovascular diseases.²⁸^,²⁹ Significant limitations are seen with current antiviral therapeutics,³⁰^–³³ and there are considerable needs for new treatments of HCMV disease.³⁴ The severity of medical problems associated with HCMV in these vulnerable populations underlies the necessity for ensuring that blood products are safer for this group of patients. Murine cytomegalovirus (MCMV) is now widely used as a surrogate model for HCMV because of its robust replication, its tractable genetic systems, the availability of many reagents for both the virus and host, and access to an animal model for in vivo experimentation which is impossible for HCMV.

We note that the specific effects of femtosecond laser irradiation on viral membranes, capsids, and nucleic acids at the molecular level remain unclear. This information is essential for the optimization, application, and approval of femtosecond lasers for use in PR of therapeutics including pharmaceuticals and blood products. Toward these goals, we report the inactivation of MCMV, a model herpes virus, by using a 425 nm-femtosecond laser and determine the molecular effects of laser irradiation on MCMV virions, viral genomic DNA, and virion-associated proteins. In remarkable contrast to the atomic force microscope images of nonenveloped viruses such as M13 bacteriophage and TMV showing that the capsids were broken by the ultrashort pulsed (USP) laser irradiation presented in the previous work, our TEM images revealed that the USP laser did not break/dissociate the capsid of MCMV. We propose a novel mechanism for the enveloped virus inactivated by visible femtosecond lasers through induction of viral protein aggregation. By correlating viral inactivation with the observed structural and molecular effects, a better insight into the inactivation of enveloped viruses by femtosecond laser irradiation was obtained.

2. Materials and Methods

2.1.

Cells and Viruses

Murine embryonic fibroblast 10.1 (MEF 10.1) cells were cultured in Dulbecco’s Modified Eagle Medium (DMEM), supplemented with 10% fetal calf serum, 1 mM sodium pyruvate, and nonessential amino acids. GFP-expressing MCMV virus (hereafter referred to as MCMV) was generated as previously described.³⁵ To produce viral stocks, MEF 10.1 cells were infected with MCMV at a low multiplicity of infection. Cell supernatants were harvested 24 h postinfection after 100% cytopathic effect and cleared of cell debris by centrifugation. Extracellular virions were pelleted by ultracentrifugation with sorbitol cushion and resuspended in phosphate-buffered saline (PBS). Viral titers were determined in quadruplicate using a median tissue culture infectious dose ( ${TCID}_{50}$ ) assay.

2.2.

Femtosecond Laser Irradiation

The experimental setup for laser irradiation is shown in Fig. 1. The excitation source employed in this work was a diode-pumped cw mode-locked Ti-sapphire laser. The laser produced a continuous train of 60 fs pulses at a repetition rate of 80 MHz. The output of the second harmonic generation system of the Ti-sapphire laser was used to irradiate the sample. The excitation laser was chosen to operate at a wavelength of $λ = 425 nm$ and with an average power of approximately 150 mW. It has a pulse width of full width at half maximum $= 100 fs$ . An achromatic lens was used to focus the laser beam into a spot about 100 μm in diameter within the sample volume. Samples of virus suspended in phosphate buffered saline at a concentration of $\sim 2 \times 10^{7} pfu / ml$ were irradiated for 1.5 h. In order to facilitate the interaction of laser with the virus, a magnetic stirring system was used so that the virus would enter the laser-focused volume as described above and interact with the photons. Controls were similarly stirred. Irradiation was carried out at 22°C and with the single laser beam excitation. After laser irradiation, samples were immediately stored at $- 80 ° C$ .

Fig. 1

Experimental setup for femtosecond laser irradiation. An 850 nm (near-infrared) laser beam was frequency doubled to produce 425 nm (visible) irradiation. Samples were magnetically stirred to expose the virus to the laser-focused volume.

2.3.

${TCID}_{50}$ Assays

${TCID}_{50}$ assays were performed to determine reduction in viral titers following laser irradiation. MEF 10.1 cells were seeded into 96 well plates at a density of $1.25 \times 10^{5} cells / ml$ and incubated overnight. Cells were approximately 80% confluent at the time of infection. Laser-treated or control (untreated) virus were serially diluted and added to cells, and cells were incubated for four days. Viral titers were determined on day 4 postinfection by scoring each well for GFP-positive cells using a fluorescent microscope.

2.4.

Electron Microscopy

Laser-treated or control (untreated) MCMV virions were allowed to absorb onto formvar/carbon-coated copper grids for 10 min. Grids were washed in distilled water and stained with 1% phosphotungstic acid (Electron Microscopy Sciences, Hatfield, Pennsylvania) for 1 min. Excess liquid was gently wicked off and grids were allowed to air dry. Samples were viewed on a JEOL 1200EX transmission electron microscope (JEOL USA, Peabody, Massachusetts) at an accelerating voltage of 100 kV. Images were acquired with a XR80M-B 8 megapixel CCD camera system (Advanced Microscopy Techniques Corporation, Woburn, Massachusetts).

2.5.

Purification of MCMV DNA

Laser-treated or control (untreated) MCMV virions were treated with DNase I for 30 min at 37°C, and then transferred to 75°C to inactivate DNase I. Viral membranes were lysed using a lysis buffer {800 mM NaCl, 20 mM Tris [pH 8.0], 20 mM EDTA, 0.4% sodium dodecyl sulfate (SDS)}, and viral capsids were digested by incubation with proteinase K ( $0.2 mg / ml$ ) at 55°C overnight. DNA was extracted with phenol-chloroform, precipitated with isopropanol, and centrifuged at 13,000×g for 30 min at 4°C. The pellets were washed with 70% ethanol and resuspended in water. For subsequent agarose gel electroporesis, MCMV DNA samples were left intact or digested using EcoRI or HindIII restriction enzymes for 5 h at 37°C prior to gel loading.

2.6.

Agarose Gel Electrophoresis

Agarose gels, 0.6% and 5 mm in thickness, were cast in a full-length gel apparatus. The MCMV DNA samples were mixed with loading buffer and then loaded into wells. Electrophoresis was carried out at $30 V / cm$ overnight. The gel was then stained with ethidium bromide for 30 min, destained for 3 h and visualized under UV illumination.

2.7.

Protein Gel Electrophoresis

Protein concentration of viral solutions was determined by Bradford assay (colorimetric protein assay kit, Bio-Rad). Solutions of laser-treated or control (untreated) virus containing equivalent quantities of protein were boiled in reducing loading buffer and separated on a 10% SDS-PAGE gel. Protein bands were visualized with Coomassie blue staining (LabSafe Gel Blue, G-Biosciences).

2.8.

Mass Spectrometry Analysis

Gel slices were excised manually and submitted to Midwest Bio Services LLC (Overland Park, Kansas) for trypsin digest followed by nano LC-MS/MS analysis and protein identification. For details on the protocol, please refer to http://www.midwestbioservices.com/proteinid.html.

2.9.

Dynamic Light Scattering

mAb(04) samples in buffer solution (50 mM sodium acetate, PH 7.0) were from Enzo life Sciences (Farmingdale, New York). BSA samples in buffer solution (50 mM sodium acetate, pH 7.0) were from Thermal Scientific Inc. (Mansfield, Texas). The dynamic light scattering (DLS) experiments were carried out by using a 90Plus Particle Size Analyzer from Brookhaven Instruments Corp. (Holtsville, New York).

2.10.

Statistics

Differences between mean ${TCID}_{50}$ titers of control and laser-treated virus were analyzed by Student’s $t$ -test. $p < 0.05$ was used as a threshold for statistical significance.

3. Results

3.1.

MCMV is Efficiently Inactivated by Femtosecond Laser Irradiation

We have previously shown that a variety of enveloped/nonenveloped, single-stranded DNA/RNA viruses can be inactivated by femtosecond laser irradiation.²¹^–²⁷ Therefore, we sought to demonstrate that irradiation with a femtosecond laser at a similar laser power (150 mW) could also inactivate MCMV, an enveloped, double-stranded DNA virus. The laser setup is illustrated in Fig. 1. For all experiments in this report, we used a previously established GFP-expressing MCMV³⁵ for ease of detection of infectious virus by ${TCID}_{50}$ assay. As shown in Fig. 2, irradiation with a 425 nm-femtosecond laser at 150 mW caused a 5-log reduction in MCMV titer relative to the control (nonirradiated) MCMV ( $p = 0.0072$ ). The titers of all laser-treated samples were at or near the limit of detection of the assay. This is consistent with the inactivation efficiency (3 to 5 log) for other viruses using the same laser conditions. Therefore, we conclude that 425 nm-femtosecond laser irradiation is an effective method to inactivate MCMV.

Fig. 2

Inactivation of MCMV using a femtosecond laser. Femtosecond laser-induced reduction in viral titer was assessed by TCID³⁶ assay. Results are representative of quadruplicate experiments and error bars indicate SEM.

3.2.

MCMV Global Virion Structure is Preserved after Femtosecond Laser Irradiation

We used negative-stain transmission electron microscopy (TEM) to investigate whether the envelope or capsid structures of MCMV virions were affected by 425 nm-femtosecond laser irradiation at an average laser power of 150 mW. As shown in Fig. 3, no clear differences in the global appearance of the envelope or capsid structure of virions in control (nonirradiated) relative to laser-irradiated groups were observed. At this resolution, we could not find any evidence of MCMV capsid disintegration after laser irradiation. These experimental results suggest that the global envelope and capsid structures of MCMV remained intact after 425 nm-femtosecond laser irradiation.

Fig. 3

Preservation of MCMV global virion structure after femtosecond laser irradiation. Representative electron microscopy images are shown of control and laser-irradiated virions (150 to 200 nm in diameter) at both $50,000 \times$ and $150,000 \times$ magnification, showing no clear differences in the global appearance of viral envelope and capsid structures after irradiation.

3.3.

MCMV Genomic DNA Structure is Preserved after Femtosecond Laser Irradiation

We used gel electrophoresis to assess whether MCMV genomic double-stranded DNA was covalently damaged by 425 nm-femtosecond laser irradiation at an average power of 150 mW. DNA was electrophoresed intact or after digestion with restriction enzymes. If double strand breakage or extensive crosslinking occurred, we would expect to see a change in the banding pattern of laser-irradiated DNA. As shown in Fig. 4, viral genomic DNA from femtosecond laser-irradiated MCMV exhibited identical banding patterns to genomic DNA from control (nonirradiated) MCMV. These experimental findings are consistent with our previous reports that 425 nm-femtosecond laser irradiation does not cause strand breaks in the single-stranded DNA of M13 bacteriophage.²³ These data indicate that 425 nm-femtosecond laser irradiation did not cause double strand breaks or crosslinking of the MCMV genome.

Fig. 4

Preservation of MCMV genomic DNA integrity after femtosecond laser irradiation. Agarose gel analysis was performed on genomic DNA isolated from control or irradiated MCMV, showing essentially identical banding patterns, which suggests a lack of double-strand breaks or crosslinking of viral DNA after femtosecond laser irradiation. DNA was electrophoresed intact or after digestion using restriction enzymes. For clarity, image contrast and sharpness were enhanced uniformly across the entire image using Photoshop. Results are representative of at least two experiments.

3.4.

Femtosecond Laser Irradiation Causes Selective Aggregation of MCMV Capsid and Tegument Proteins

We employed SDS-PAGE to determine the effects of femtosecond laser irradiation on MCMV virion-associated proteins. Interestingly, several protein bands from laser-irradiated virions showed substantially reduced intensities relative to those of control (nonirradiated) virions (Fig. 5). Since our 425-nm laser treatment lacks the energy required to disrupt the covalent bonds commonly found in proteins, fragmentation of viral proteins or the production of covalent cross-linkages were unlikely scenarios. As shown by the arrow in Fig. 5, a high molecular weight protein aggregate was consistently detected in the laser-irradiated group. Based on this observation, we reasoned that laser irradiation may have caused aggregation of viral proteins. Therefore, the aggregate was excised from the gel and submitted for protein identification. The list of MCMV proteins identified is shown in Table 1. The aggregate contained predominantly MCMV virion-associated capsid and tegument proteins. The identified MCMV proteins have previously been detected in MCMV virions.³⁷ In contrast, the MCMV envelope glycoproteins such as glycoprotein B,³⁸ glycoprotein H,³⁹ and glycoprotein M⁴⁰ were not detected in the aggregate. These data indicate that femtosecond laser irradiation causes selective aggregation of MCMV capsid and tegument proteins, an effect that may hinder viral capsid function (i.e., uncoating) and contribute to inactivation of the virus.

Fig. 5

Aggregation of MCMV virion proteins after femtosecond laser irradiation. SDS-PAGE analysis was performed on control and laser-irradiated virions. The arrow denotes a high molecular weight aggregate formed by proteins in the laser-treated group. The aggregate was excised for mass spectrometry analysis. For clarity, image contrast and sharpness were enhanced uniformly across the entire image using Photoshop. Results are representative of at least two experiments.

Table 1

MCMV proteins from the aggregate identified by LC-MS/MS.

Protein	Accession	Comment	HCMV homologue	$p$ -value	No. of peptides
M25	gi:190886806	Tegument protein⁴¹	UL25	$4.42 \times 10^{- 6}$	29
M32	gi:190886815	(HCMV: pp150)⁴²	UL32	$6.17 \times 10^{- 8}$	18
M35	gi:190886819	UL25 family member, virulence factor⁴³	UL35	$3.54 \times 10^{- 6}$	4
M44	gi:90954727	DNA binding phosphoprotein⁴⁴	UL44	$1.57 \times 10^{- 5}$	4
M80	gi:157676178	Assembly protein-protease⁴⁵	UL80	$4.82 \times 10^{- 4}$	4
M82	gi:157676179	Upper matrix phosphoprotein, pp71⁴⁶	UL82	$3.63 \times 10^{- 4}$	2
M83	gi:1532178	Lower matrix phosphoprotein, pp65⁴⁶	UL83	$8.19 \times 10^{- 4}$	2
M86	gi:157676184	(HCMV: major capsid protein)⁴⁷	UL86	$9.09 \times 10^{- 7}$	43
M94	gi:157676191	(HCMV: virion-associated protein)³⁶	UL94	$1.02 \times 10^{- 5}$	6

4. Discussion

In this report we have examined the effects of femtosecond lasers on MCMV structures at the molecular level. The capability of 425 nm-femtosecond laser treatment to inactivate a spectrum of different viruses and bacteria has been well documented.²⁰^–²⁷ In these previous studies, it was demonstrated that the nonenveloped viruses such as M13 bacteriophages were inactivated by the USP laser irradiation through breaking/dissociation of their capsids. However, the inactivation mechanism for the enveloped viruses remains unexplored. In this work, we demonstrate that in great contrast to the nonenveloped virus such as M13, whose capsid was broken/dissociated by the USP laser irradiation, our TEM images suggest that the USP laser does not break/dissociate the capsid of the enveloped virus like MCMV. This indicates that the inactivation mechanism for nonenveloped virus is drastically different from that of an enveloped virus. We attribute the inactivation mechanism for MCMV by the USP laser to the aggregation of proteins within the virion.

Interestingly, our experimental results suggest that laser irradiation causes selective aggregation of viral capsid and tegument proteins. It has been suggested that partial unfolding of proteins is required for protein aggregation.⁴⁸ We posit that femtosecond laser irradiation disrupts hydrogen bonds and/or hydrophobic interactions in viral proteins through the impulsive stimulated Raman scattering process.²²^,²³ Although the reformation time for broken hydrogen bonds/hydrophobic contacts is believed to be short (of the order of 10 picoseconds),⁴⁹^,⁵⁰ there is a significant chance for the MCMV capsid and tegument proteins to become aggregated since they are confined within a small volume in the virion. This explains the observation of aggregated proteins under femtosecond laser irradiation. As a result, laser-induced aggregation of MCMV capsid and tegument proteins may hinder the function of the viral capsid (i.e., uncoating) and contribute to virus inactivation. The concentration dependence of protein aggregation may thus provide a window for selectively damaging virions while leaving mammalian proteins intact.²³

To get better insight into the proposed protein aggregation model for enveloped virus inactivation, we have also performed DLS experiments for a variety of proteins in their buffer solutions: (1) on the concentration dependence of aggregation for monoclonal antibody 04, (2) on the aggregation of BSA proteins, and (3) on the aggregation of the mixture of BSA and mAb04, under the same experimental conditions as MCMV. The integrated area under the primary peak—the monomer, which happens at about 12 nm, 6 nm in diameter for mAb04 and BSA, respectively, divided by the total integrated area is taken as the percentage of the nonaggregated protein. The integrated area under the higher size/mass region divided by the total area is considered as the aggregated percentage.

The results, summarized in Table 2, indicate that (1) the structure of nonaggregated protein is not compromised, (2) the protein aggregation effect by irradiation of the USP laser depends on the type of proteins; apparently, BSA is much more stable than mAb04 and exhibits very little aggregation upon USP laser irradiation, (3) the aggregation effect depends on protein concentration, with higher concentration tending to aggregate more, and (4) mixing the stable protein (BSA) with a less stable one (mAb04) does not help stabilize the less stable protein. This information further supports our proposed model that the USP laser first unfolds the proteins by disrupting their hydrogen bonds/hydrophobic contacts. The unfolded proteins then aggregate before the rapid reformation of these weak bonds. The higher protein concentration means they are closer to each other and as a result have a higher chance of aggregating. We note that under our experimental conditions, the proteins were completely dissolved in their buffer solutions, as evidenced by the almost 99% of monomer (nonaggregated proteins) in the solutions. In other words, our interpretations of protein aggregation by USP laser irradiation were not affected by the problem of solubility of the proteins in the buffer solution. In addition, the two proteins, BSA and mAb04, were chosen for the DLS experiments because neither of them absorb near 425 nm. As a matter of fact, we measured the temperature of the solutions during the laser irradiation experiments with a thermal couple immersed into the solution. The temperature of the solution rose no more than 2°C. Since the denature temperature of both proteins is around 60°C, our results cannot be due to the heating effects.

Table 2

Dynamic light scattering data for a variety of laser-treated proteins in buffered solution.

Sample, titer	% of aggregation	% of nonaggregation
mAb(04), $5 mg / ml$ (Control)	$2.7 \pm 0.3$	$97.3 \pm 0.3$
mAb (04), $5 mg / ml$ (laser treated)	$18.6 \pm 0.3$	$81.4 \pm 0.3$
mAb (04), $1 mg / ml$ (Control)	$2.7 \pm 03$	$97.3 \pm 0.3$
mAb (04), $1 mg / ml$ (laser treated)	$4.1 \pm 0.3$	$95.9 \pm 0.3$
BSA, $5 mg / ml$ (Control)	$1.5 \pm 0.3$	$98.5 \pm 0.3$
BSA, $5 mg / ml$ (laser treated)	$1.6 \pm 0.3$	$98.4 \pm 0.3$
mAb(04), $5 mg / ml + BSA$ , $5 mg / ml$ (Control)	$2.3 \pm 0.3$	$48.6 \pm 0.3$ (mAb04) $49.1 \pm 0.3$ (BSA)
mAb(04), $5 mg / ml + BSA$ , $5 mg / ml$ (laser treated)	$30.7 \pm 0.3$	$24.2 \pm 0.3$ (mAb04) $45.3 \pm 0.3$ (BSA)

We notice that in contrast to the atomic force microscope images of nonenveloped viruses such as M13 bacteriophage and TMV showing that the capsids were broken by the USP laser irradiation presented in the previous work, our TEM images indicate that the USP laser does not break/dissociate the capsid of the enveloped virus like MCMV. Based upon our results from DLS experiments, we propose, for enveloped viruses such as MCMV, that the USP laser partially unfolds both the protein unit of which the capsid is made up without dissociating the capsid and the tegument proteins by breaking some of their hydrogen bonds/hydrophobic contacts. These proteins then form aggregates before the reformation of the weak noncovalent bonds.

In this study, the treated volume is about 100 µL. To scale up our approach for the disinfection of blood products, we suggest the use of a syringe pump-capillary configuration in which the treated solution is forced through a capillary of the order of 1 mm in inner diameter. The laser beam will be adjusted to have the same diameter and passes through the capillary in a perpendicular geometry. A much more powerful commercially available USP laser system with an average power of the order of 10 W can be used for laser irradiation.

The USP laser technology presented here can be readily used for the disinfection of pharmaceuticals, which typically do not contain hemoglobin. The application of this technology to the disinfection of blood products can be done with USP lasers operating at a wavelength of about 700 nm where the absorption of hemoglobin is a minimum and the potential damaging effects can be minimized. In conclusion, we report the first experimental evidence of inactivation of an enveloped virus: MCMV by the USP laser. The molecular and structural effects caused by 425 nm-femtosecond laser irradiation on MCMV are presented and analyzed. In contrast to the atomic force microscope images of nonenveloped viruses such as M13 bacteriophage and TMV showing that the capsids were broken by the USP laser irradiation presented in the previous work, our TEM images revealed that the USP laser did not break/dissociate the capsid of MCMV. A novel mechanism for the inactivation of an enveloped virus by visible femtosecond lasers through induction of viral protein aggregation was proposed. By correlating viral inactivation with the observed structural and molecular effects, a better insight into the inactivation of enveloped viruses by femtosecond laser irradiation was obtained. Furthermore, continued exploration of this laser pathogen inactivation technology is expected to generate applications including sterilization of pharmaceuticals, blood products, and medical equipment.

Acknowledgments

We would like to thank Irina Sorokina (Midwest Bio Services LLC, Overland Park, Kansas) for mass spectrometry analysis. This work was supported in part by the Mallinckrodt Institute of Radiology Development Fund, NIH Grant R33 CA123537, NHLBI Ruth L. Kirschstein NRSA F30 Grant HL116183-01 (Shaw-Wei Tsen), and Public Health Service Grant R01CA120768 (Dong Yu).

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Shaw-Wei D. Tsen, Travis Chapa, Wandy Beatty, Kong-Thon Tsen, Dong Yu, and Samuel Achilefu "Inactivation of enveloped virus by laser-driven protein aggregation," Journal of Biomedical Optics 17(12), 128002 (10 December 2012). https://doi.org/10.1117/1.JBO.17.12.128002

Published: 10 December 2012

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KEYWORDS

Proteins

Femtosecond phenomena

Laser irradiation

Viruses

Control systems

Molecular lasers

Pathogens

1.

Introduction

2.

Materials and Methods