The treatment of skin with a low-power continuous-wave (CW) near-infrared (NIR) laser prior to vaccination is an emerging strategy to augment the immune response to intradermal vaccine, potentially substituting for chemical adjuvant, which has been linked to adverse effects of vaccines. This approach proved to be low cost, simple, small, and readily translatable compared with the previously explored pulsed-wave medical lasers. However, little is known on the mode of laser–tissue interaction eliciting the adjuvant effect. In this study, we sought to identify the pathways leading to the immunological events by examining the alteration of responses resulting from genetic ablation of innate subsets including mast cells and specific dendritic cell populations in an established model of intradermal vaccination and analyzing functional changes of skin microcirculation upon the CW NIR laser treatment in mice. We found that a CW NIR laser transiently stimulates mast cells via generation of reactive oxygen species, establishes an immunostimulatory milieu in the exposed tissue, and provides migration cues for dermal CD103+ dendritic cells without inducing prolonged inflammation, ultimately augmenting the adaptive immune response. These results indicate that use of an NIR laser with distinct wavelength and power is a safe and effective tool to reproducibly modulate innate programs in skin. These mechanistic findings would accelerate the clinical translation of this technology and warrant further explorations into the broader application of NIR lasers to the treatment of immune-related skin diseases.

Skin-based vaccination has been demonstrated to permit dose sparing of the vaccine Ag and improve long-term protection conferred by vaccination, thus showing clear advantages over the standard i.m. injection (13). However, modern inactivated vaccines used for intradermal (ID) influenza vaccination, for instance, are still poorly immunogenic and induce little protective T cell response, conferring insufficient protection to vulnerable populations, including children and the elderly (46). The shortcomings of the current inactivated vaccine strategies would be improved by use of immunologic adjuvants, as incorporation of an adjuvant into vaccine formulations is an established strategy to enhance immunogenicity of a vaccine Ag and induce long-term immunity and protective T cell responses (7). Unfortunately, most conventional chemical or biological adjuvants are inappropriate for use in the skin because of issues related to the potential to induce persistent local toxicity caused by overstimulated innate immunity in the confined space (8, 9). As a result, no adjuvant has been incorporated into clinically approved ID vaccines.

Recently, stimulating the skin with a physical parameter, namely laser light, prior to the administration of an ID vaccine has been shown to augment the immunogenicity without applicable adverse effects, representing an emerging alternative approach to the conventional chemical or biological adjuvants (10). To date, four classes of lasers have been used to enhance the efficacy of vaccines in preclinical mouse models (11). The application of a nonablative fractional laser has been demonstrated to augment the immune response to a model ID influenza vaccine via release of damage-associated molecular patterns from columns of coagulated (dead) tissue created after the treatment of skin with a fractional laser and subsequent recruitment of plasmacytoid dendritic cells (DCs) around the columns (12, 13). An ablative fractional laser has been similarly shown to activate skin-resident Xcr1+ DCs and enhance the efficacy of prophylactic and therapeutic tumor vaccines through the local inflammatory response induced by dead keratinocytes around skin micropores (14). In contrast, brief exposures of skin with a low-power, visible pulsed-wave (PW) laser were also found to augment the immune response to a model ID vaccine via release of hsp70 from skin cells and subsequent activation of skin-resident Langerhans cells (15) or disruption of cell–matrix interactions induced by disarray of dermal collagen fibers and resultant increase in the motility of APCs in the skin tissue (9, 16, 17). In contrast to the fractional lasers, this class of visible PW laser induces no histological skin tissue damage (9), but its condensed energy in laser pulses induces the heat shock response (15) or ultrastructural change in the extracellular matrix (17). We have shown that another distinct class of laser, a low-power continuous-wave (CW) near-infrared (NIR) invisible laser between 1061 and 1301 nm, significantly enhances the immune response to a model ID vaccine and improves survival in a lethal challenge murine influenza model (1820). In these studies, exposure of the skin to the CW NIR laser was found to induce no detectable tissue damage or inflammation (1820). The energy of a CW NIR laser, which is delivered homogenously over the time period, is not high enough to induce any heat shock response or ultrastructural change in the exposed tissue (21). These observations indicate that the CW NIR laser has the distinct mechanisms of action compared with the other three PW lasers. We have demonstrated that a CW NIR laser induces transient upregulation of a selective set of chemokines in skin and migration of specific subsets of skin-resident DCs (19, 20). However, the precise details of CW NIR laser–skin tissue and cell–cell interactions leading to the augmentation of the immune response are largely unknown.

In this study, we demonstrate that a CW NIR laser induces a unique immunologic cascade in skin-stimulating mast cells (MCs) via reactive oxygen species (ROS) generation and creates immunostimulatory milieu for DCs, thus augmenting the adaptive immune response. These findings not only contribute to the optimization of a CW NIR laser for immunologic adjuvant but open a pathway to broader applications of this technology to treat immune-related conditions.

We purchased 8-wk-old female C57BL/6J mice (stock number: 000664) from The Jackson Laboratory (Bar Harbor, ME). We acclimated all animals for at least 2 wk prior to the experiments. We purchased breeding pairs of Ccr7-deficient (Ccr7−/−; 006621), Batf3-deficient (Batf3−/−; 013755), KitW-sh/KitW-sh (012861), and CD11c-EYFP (008829) mice from The Jackson Laboratory and bred them at Massachusetts General Hospital (MGH). All animal procedures were performed following the Public Health Service Policy on Humane Care of Laboratory Animals and approved by the Institutional Animal Care and Use Committee of MGH.

We applied a Nd:YVO4 1064-nm laser emitting either CW or nanosecond PW at a repetition rate of 10 kHz (RMI Laser, Lafayette, CO) on the surface of depilated skin as previously described (19, 20). We used a non–tissue damaging power density of 5 W/cm2 on a circular spot on the skin surface of ∼5 mm in diameter (0.2 cm2) for 1 min with a total dose of 300 J/cm2 as previously determined (19, 20). We monitored the skin temperature throughout the laser application using an infrared (IR) thermal imager (FLIR Systems).

We depilated the mouse back skin with commercial depilatory cream (Nair; Church & Dwight) 2 d before the NIR laser treatment and vaccination. We injected an inactivated influenza virus vaccine (A/PR/8/34, 1 μg in 10 μl of saline; Charles River) ID in the center of the spot on the mouse back skin within 5 min of the laser treatment. The vaccine mixed with Alum (diluted 1:1 v/v, Imject; Thermo Fisher Scientific) or c48/80 (3.2 ng/spot; Millipore Sigma) was used for comparison as appropriate. We homologously challenged mice intranasally with live influenza A/PR/8/34 virus at a dose of 2 × 105 50% egg infectious doses at day 28. We euthanized mice and obtained blood and spleen samples for further analysis 4 d after challenge as established previously (1820).

We examined the involvement of ROS in the effect of an NIR laser using a ROS scavenger. We pretreated mice with s.c. injections of 100 mg/kg N-acetyl-l-cysteine (NAC; Millipore Sigma) at day −3, −2, −1, and 0 as appropriate (22) before the experiment. Control mice received vehicle only (PBS) s.c.

We measured anti-influenza–specific IgG, IgG1, and IgG2c humoral responses by ELISA as previously described (19). We coated Immulon plates (Thermo Fisher Scientific) with 100 ng of the inactivated influenza virus and then added serially diluted mouse serum samples to the wells. We detected bound Igs with the secondary Ab (goat anti-mouse IgG [1:10,000; Millipore Sigma], rat anti-mouse IgG1 [1:2000; SouthernBiotech], or goat anti-mouse IgG2c [1:4000; SouthernBiotech]). We designated a titer as the serum dilution corresponding to the inflection point of the plot of the OD versus dilution of serum. SRI International (Harrisonburg, VA) determined hemagglutination inhibition (HAI) titers in sera samples. Operators performed all immunoassays in a blinded manner to control or experimental groups.

We harvested and immediately processed splenocytes 4 d after challenge as previously described (1820). Briefly, we incubated splenocyte preparations containing 1 × 106 cells with or without the inactive influenza at a concentration of 1 μg/ml for 60 h for determination of cytokine release in a round-bottom 96-well plate. We collected splenocyte culture supernatants and determined the amounts of IFN-γ or IL-4 using the DuoSet ELISA Kit (R&D Systems) following manufacturer’s instructions. Operators performed all immunoassays in a blinded manner to control or experimental groups.

We challenged immunized mice intranasally with live influenza A/PR/8/34 virus at a dose of 1.5 × 106 50% egg infectious doses, which is equivalent to 150 × 50% mouse lethal dose, in 30 μl of saline 28 d after vaccination as previously described (1820). We monitored survival and body weight for 15 d postchallenge. We considered mice showing a hunched posture, ruffled fur, or >20% body weight loss or mice that were not eating or drinking to have reached the experimental endpoint. Operators performed monitoring in a blinded manner to control or experimental groups.

We shaved and depilated mice 2 d before the assay. We painted mice on four spots of the flank back skin (∼5 mm in diameter per spot) with 10 μl of a 0.5% FITC solution (Isomer I; Millipore Sigma) 4 h prior to the assay as previously described (20, 23). The FITC solution was prepared in acetone:dibutyl phthalate (1:1, vol/vol; Millipore Sigma). We performed the NIR laser treatment followed by vaccination with OVA (EndoFit OVA; InvivoGen) at each treatment site (10 μg in 10 μl of saline per spot, four spots in total) on the FITC-painted sites. We then harvested skin-draining lymph nodes (dLN) 24 and 48 h after the vaccination and laser treatment and then isolated DCs from lymph nodes (LN). We mechanically dissociated LN and incubated them with collagenase D (2.5 mg/ml; Roche) and 10 mM EDTA as previously described (24). We labeled cells isolated from LN for CD11c (N418; eBioscience), I-A/I-E (M5/114.15.2; eBioscience), CD11b (M1/70; BioLegend), CD103 (2E7; BioLegend), langerin/CD207 (4C7; BioLegend), CD8α (53-6.7; eBioscience), and CD86 (GL1; BioLegend). We also stained isolated cells with LIVE/DEAD Fixable Aqua (Life Technologies) to distinguish live cells. We performed data acquisition on a Fortessa cytometer (BD Bioscience) followed by analysis on FlowJo software (FlowJo, LLC). We selected classical LN-resident cells (classical DCs [cDCs]) based on CD11chi status and I-A/I-E intermediate levels. We selected migratory DCs (migDCs) based on CD11c intermediate levels and I-A/I-Ehi status as distinct from cDCs, which were further gated for langerin+ (Lang+) versus CD11b+. We further gated CD11b+ versus CD103+ subpopulations from cells within the Lang+ migDC gate, as previously described (20, 24, 25).

We reconstituted MC-deficient sash mice with bone marrow–derived MCs (BMMCs) as previously described (26). Briefly, we collected bone marrow (BM) from wild-type (WT) host mice. We cultured BM-derived cell suspensions for 6 wk in the presence of 10 ng/ml IL-3 and 10 ng/ml SCF (R&D Systems) until we obtained a pure population of MCs. We confirmed the differentiation of MCs by flow cytometry with positive staining for c-kit and FcεɛRI. We injected 4 × 106 BMMCs into the flank skin of 4-wk-old sash mice. We allowed mice to recover for 8 wk prior to the experiments.

Mouse ears were shaved and depilated 2 d before the tissue preparation. Depilated ears were treated with the NIR laser as described above. Six hours after the treatment, mice were heart perfused with 4% paraformaldehyde following i.v. injection with DyLight 649-labeled Tomato Lectin (Vector Laboratories). Lymphatic vessels were identified using Ab to Lyve-1 (1:200, clone: ALY7; eBioscience; or 1:200, rabbit polyclonal; Relia Tech), and CD11b+ or Lang+ DCs were identified using Ab to CD11b (1:200, rabbit polyclonal; Novus Biologicals) or langerin/CD207 (1:200, clone:929F3.01; IMGENEX). We randomly sampled three to four photographic imaging stacks (450 × 450 μm2, 40–60 μm thick each) for each ear using confocal laser-scanning microscopy and determined density and width of perfused blood and lymphatic vessels and spatial relationships between CD11b+ or Lang+ DCs and blood or lymphatic vessels using a three-dimensional analysis system on Imaris software (Bitplane). We counterstained cell nuclei by DAPI.

CCL21+ cells were identified using Ab to CCL21 (1:200, goat polyclonal; R&D Systems). We determined the total surface area of lymphatic vessels, then quantified the number of CCL21+ cells on the lymphatic vessels on Imaris software. These parameters were determined in three to four photographic areas from each ear.

Mice were heart perfused with 4% paraformaldehyde at 6 h after the treatment with the CW NIR laser at a power of 5.0 W/cm2 for 1 min. TUNEL staining was performed on 5-μm-thick paraffin sections using the In Situ Cell Death Detection Kit, TMR red (Roche Applied Science). Nuclei were identified by counterstaining using DAPI. Slides were imaged using an inverted fluorescence microscope (Carl Zeiss Axio A1; Carl Zeiss North America). Apoptotic cells were identified in red and counted in four photographic areas from each skin sample.

Mice were heart perfused with 4% paraformaldehyde. Skin biopsies were embedded in paraffin blocks. Five-micrometer-thick paraffin sections were stained with 0.1% toluidine blue (Millipore Sigma) (27). Slides were imaged using an inverted microscope (Axio A1; Carl Zeiss). Dermal MCs were identified by their characteristic morphology and staining reactions (28) and counted in four to five photographic areas.

Differentiated BMMCs were cultured in 24-well plates at a density of 5 × 105 cells per well. We used a CW 1064-nm Nd:YVO4 laser for laser treatment as described above. The spot diameter on the well was adjusted to be ∼16 mm. The BMMC culture was treated with the CW NIR laser at a power of 0.5 W/cm2 for 1–3 min. To detect ROS generation, BMMCs were incubated in 0.5% FBS/HBSS during the laser treatment, then washed and incubated with 0.1 μM H2DCFDA (Thermo Fisher Scientific) for 15 min immediately after the conclusion of the NIR laser treatment. Negative or positive control cells were treated with NAC or H2O2, respectively. ROS-reacted DCF-dependent fluorescence was measured by flow cytometry. We performed data acquisition on a Fortessa cytometer (BD Bioscience) followed by analysis on FlowJo v10 software (FlowJo, LLC). Primary cultured human epidermal keratinocytes were purchased from Life Technologies. The keratinocytes were cultured in EpiLife media (Life Technologies) with Human Keratinocyte Growth Supplement (Life Technologies) until they reached 80–90% confluency in 24-well plates. We used a CW 1064-nm Nd:YAG laser (Ventus; Laser Quantum, Cheshire, England) for laser treatment. The laser treatment and ROS detection on the keratinocyte culture were performed as described above. We performed data acquisition on a BD Accuri C6 Cytometer (BD Bioscience) followed by analysis on the FlowJo software. Fold increase in DCF-positive population compared with no laser-treated control was calculated for each experiment.

Skin sections measuring 0.2 mm2, including both the epidermis and dermis, were excised 6 h after laser illumination. The skin tissue was homogenized using a bead mill homogenizer, and total RNA was extracted using the RNeasy Kit (Qiagen) and reverse transcribed using the RT2 First Strand Kit (Qiagen). Differentiated BMMCs were cultured in 24-well plates and treated with the CW NIR laser at a power of 0.5 W/cm2 for 1 min as described above. Four hours after the laser treatment, total RNA was extracted and reverse transcribed as described above. The samples were tested for previously identified selected genes of importance (Ccl2, Ccl6, Ccl11, Ccl17, Ccl20, Il1a) in addition to inflammatory cytokines (Ifng, Tnf, Il1b) (19) using an RT2 qPCR Primer Assay (Qiagen) and RT2 SYBR Green ROX qPCR Mastermix (Qiagen) on the StepOnePlus PCR System (Applied Biosystems). Fold changes in the expression over sham-treated controls were normalized against housekeeping genes and calculated following the 2−ΔΔCT method. Cycle threshold values that were higher than the cutoff of 40 were not considered as reliable and were removed from further analysis.

Human primary keratinocytes were cultured and treated with the CW NIR laser at a power of 0.5 W/cm2 for 1 min as described above. Four hours after the laser treatment, total RNA was extracted and reverse transcribed as described above. The samples were tested on the Human Inflammatory Cytokines and Receptors RT2 Profiler PCR Array (number 330231; Qiagen) on the GVP-9600 System (Shimadzu, Kyoto, Japan). Fold changes in the expression over no treatment controls were analyzed as described above.

Microvascular permeability in the skin tissue was measured as previously described (29). Briefly, Evans blue was injected from retroorbital plexus 0, 1, 2, and 6 h after a 1-min CW 1064-nm laser treatment at 5.0 W/cm2. Thirty minutes after the injection of Evans blue dye, the laser-treated skin tissue portion was excised and dissolved in formamide to elute Evans blue at 55°C overnight. Evans blue leak in the tissue was quantitated by spectrophotometry at 650 nm.

We ran a one-way ANOVA across treatments (vaccine ID only, CW 1064-nm laser, PW 1064-nm laser, Alum, c48/80, i.m., NAC) restricted to the WT genotype with Tukey adjusted post hoc pairwise mean comparison tests. We also ran two-way genotype (WT, Ccr7−/−, Batf3−/−, sash, sash reconstituted) by treatment factorial ANOVAs with different selected genotypes and treatments depending on the question addressed. A log transformation of Ab titers was applied for Ab titer analysis. Separate analyses were run for the dependent variables IgG, IgG1, and IgG2c. If the interaction was not significant, we removed it and tested only the main effects of genotype and treatment. Significant main and interaction effects were followed up with Tukey post hoc tests. Because the Ab responses of WT mice injected with or without vehicle for NAC treatment were not statistically significant for all the treatments, we pooled the results within the same treatment groups.

For quantitative PCR results, in addition to Student unpaired two-tailed t test with stepdown bootstrap and false discovery rate corrections (30), we ran a discriminant analysis to see if previously identified selected genes of importance (Ccl2, Ccl6, Ccl11, Ccl17, Ccl20, Ifng, Tnf, Il1a, Il1b) (19) could predict the effect of the NIR laser treatment.

The data analysis for this paper was conducted using SAS/STAT software for Windows (Version 9.4; SAS Institute, Cary, NC) and Prism 7 (GraphPad software 2016). We used the SAS Candisc Procedure followed by SAS Stepdisc Procedure for the discriminant analysis. Data were pooled from at least two independent experiments.

MCs are enriched for the expression of genes encoding a diverse array of factors involved in the innate and adaptive immune response (31) and play a critical role in host defense against parasitic, bacterial, and viral infections (3236). We therefore hypothesized that the CW NIR laser stimulates connective tissue MCs in skin and initiates an immunostimulatory milieu for skin-resident DCs. To test this hypothesis, we compared the immune response to an experimental ID influenza vaccination (whole inactivated influenza A/PR/8/34 virus) with or without CW or nanosecond PW NIR laser treatment at 5.0 W/cm2 for 1 min (1820) or a MC activator c48/80 (37) in mice.

Consistent with the previous reports (1820), the CW, but not PW, NIR laser significantly augmented anti-influenza IgG response (Fig. 1A, the CW laser versus ID only group for IgG: p = 0.0033), provoked a statistically marginal increase in IgG2c (Fig. 1C, the CW laser versus ID only group for IgG2c: p = 0.0664), induced similar anti-influenza IgG2c:IgG1 ratios (Fig. 1D) without increasing IgE responses (Fig. 1E) and IFN-γ and IL-4 secretion levels from ex vivo stimulated splenocytes (Fig. 1F, 1G), and increased the HAI geometric mean titers (the CW laser versus ID only, 18.81, 95% CI: 9.024–39.19 versus 6.936, 95% CI: 3.520–13.67) (Fig. 1H) compared with the nonadjuvanted ID only group. Interestingly, the application of c48/80 significantly augmented anti-influenza IgG response (Fig. 1A, the c48/80 versus ID only group for IgG: p = 0.0201) (which is consistent with the published literature reporting the adjuvant effect of activated MCs) (38, 39) to a similar magnitude as did the CW NIR laser, compared with the ID only group. The geometric mean titers for the c48/80 group were consistently higher (13.13, 95% CI: 3.824– 45.07) than that of the ID only group, although this difference was not statistically significant (Fig. 1H). The c48/80 induced similar anti-influenza IgG2c:IgG1 ratios (Fig. 1D) without increasing IgE responses (Fig. 1E) and IFN-γ and IL-4 secretion levels (Fig. 1F, 1G) compared with the ID only and laser-treated groups, in contrast to alum adjuvant inducing a profoundly skewed TH2 response with high IgE responses (Fig. 1E) and low IFN-γ levels (Fig. 1F) and IgG2c:IgG1 ratios (Fig. 1D) (40). These results show that activation of MCs in skin augments the immune response and produces a mixed TH1 and TH2 response.

FIGURE 1.

A critical role of MCs in the effect of the NIR laser on anti-influenza immune responses. The effect of an NIR laser on anti-influenza immune responses was evaluated in WT and MC-deficient sash mice. Reconstitution of sash mice was performed by ID injection of BMMCs 8 wk before vaccination. WT, sash, and reconstituted mice were vaccinated with 1 μg of inactivated influenza virus (A/PR/8/34) with or without the NIR laser exposure or c48/80 and challenged intranasally with live homologous virus 28 d after vaccination. Immune correlates were analyzed at day 32. Plates for ELISA were coated with the inactivated influenza virus. Serum anti-influenza specific (A) IgG, (B) IgG1, (C) IgG2c, (D) IgG2c/IgG1 ratio, and (E) IgE. (F and G) The effect of the NIR laser on systemic anti-influenza specific T cell responses. The cytokine responses were measured 4 d after challenge by restimulating cultured splenocytes with the inactivated influenza vaccine Ag. Levels of (F) IFN-γ and (G) IL-4 in supernatants are shown. (H) HAI titers 4 d after challenge are shown. (A–D) n  =  44, 48, 38, 33, 22, 12, 23, 26, 10, 8, and 10; (E) n  =  40, 29, 25, 13, 7, 7, 15, 17, 2, 8, and 10; and (F and G) n  =  35, 39, 30, 24, 9, 4, 10, 10, 7, 8, and 10 for no vaccine, vaccine ID only, vaccine ID + CW 1064-nm laser, vaccine ID + PW 1064-nm laser, vaccine + Alum ID, vaccine + c48/80 ID, vaccine ID only in sash, vaccine ID + CW 1064-nm laser in sash, vaccine ID + PW 1064-nm laser in sash, vaccine ID only in sash reconstituted (sash-R), and vaccine ID + CW 1064-nm laser in sash-R groups, respectively. (H) n  =  17, 35, 29, 22, 12, and 12 for no vaccine, vaccine ID only, vaccine ID + CW 1064-nm laser, vaccine ID + PW 1064-nm laser, vaccine + Alum ID, and vaccine + c48/80 ID group, respectively. Results were pooled from (A–E) 10, (F and G) 8, and (H) 5 independent experiments. The p values for the tests of treatments within the WT genotype were based on a one-way ANOVA between subjects of the WT data with Tukey post hoc tests, whereas those for other comparisons are based on a two-way treatment by genotype ANOVA with Tukey tests. (I) Kaplan–Meier survival plots for 15 d following lethal influenza challenge; Gehan–Breslow–Wilcoxon test. (J) The effect of the NIR laser on body weight of vaccinated mice following viral challenge. Body weights were monitored daily for 15 d. Mean body weight ± SEM of each experimental group was determined at each time point. n  = 10, 12, 13, 5, 10, 10, 4, 6, and 6 for no vaccine, vaccine ID only, vaccine ID + CW 1064-nm laser, no vaccine in sash, vaccine ID only in sash, vaccine ID + CW 1064-nm laser in sash, no vaccine in sash-R, vaccine ID only in sash-R, and vaccine ID + CW 1064-nm laser in sash-R groups, respectively. (I and J) Results were pooled from four independent experiments.

FIGURE 1.

A critical role of MCs in the effect of the NIR laser on anti-influenza immune responses. The effect of an NIR laser on anti-influenza immune responses was evaluated in WT and MC-deficient sash mice. Reconstitution of sash mice was performed by ID injection of BMMCs 8 wk before vaccination. WT, sash, and reconstituted mice were vaccinated with 1 μg of inactivated influenza virus (A/PR/8/34) with or without the NIR laser exposure or c48/80 and challenged intranasally with live homologous virus 28 d after vaccination. Immune correlates were analyzed at day 32. Plates for ELISA were coated with the inactivated influenza virus. Serum anti-influenza specific (A) IgG, (B) IgG1, (C) IgG2c, (D) IgG2c/IgG1 ratio, and (E) IgE. (F and G) The effect of the NIR laser on systemic anti-influenza specific T cell responses. The cytokine responses were measured 4 d after challenge by restimulating cultured splenocytes with the inactivated influenza vaccine Ag. Levels of (F) IFN-γ and (G) IL-4 in supernatants are shown. (H) HAI titers 4 d after challenge are shown. (A–D) n  =  44, 48, 38, 33, 22, 12, 23, 26, 10, 8, and 10; (E) n  =  40, 29, 25, 13, 7, 7, 15, 17, 2, 8, and 10; and (F and G) n  =  35, 39, 30, 24, 9, 4, 10, 10, 7, 8, and 10 for no vaccine, vaccine ID only, vaccine ID + CW 1064-nm laser, vaccine ID + PW 1064-nm laser, vaccine + Alum ID, vaccine + c48/80 ID, vaccine ID only in sash, vaccine ID + CW 1064-nm laser in sash, vaccine ID + PW 1064-nm laser in sash, vaccine ID only in sash reconstituted (sash-R), and vaccine ID + CW 1064-nm laser in sash-R groups, respectively. (H) n  =  17, 35, 29, 22, 12, and 12 for no vaccine, vaccine ID only, vaccine ID + CW 1064-nm laser, vaccine ID + PW 1064-nm laser, vaccine + Alum ID, and vaccine + c48/80 ID group, respectively. Results were pooled from (A–E) 10, (F and G) 8, and (H) 5 independent experiments. The p values for the tests of treatments within the WT genotype were based on a one-way ANOVA between subjects of the WT data with Tukey post hoc tests, whereas those for other comparisons are based on a two-way treatment by genotype ANOVA with Tukey tests. (I) Kaplan–Meier survival plots for 15 d following lethal influenza challenge; Gehan–Breslow–Wilcoxon test. (J) The effect of the NIR laser on body weight of vaccinated mice following viral challenge. Body weights were monitored daily for 15 d. Mean body weight ± SEM of each experimental group was determined at each time point. n  = 10, 12, 13, 5, 10, 10, 4, 6, and 6 for no vaccine, vaccine ID only, vaccine ID + CW 1064-nm laser, no vaccine in sash, vaccine ID only in sash, vaccine ID + CW 1064-nm laser in sash, no vaccine in sash-R, vaccine ID only in sash-R, and vaccine ID + CW 1064-nm laser in sash-R groups, respectively. (I and J) Results were pooled from four independent experiments.

Close modal

To further assess the contribution of MCs to the effect of the NIR laser, the response in MC-deficient KitW-sh/W-sh (sash) mice and sash mice selectively reconstituted for MCs in skin (sash-R mice) by ID injection with genetically compatible BMMCs from WT mice (26) was also evaluated. In this model, MCs were reconstituted locally in the injection sites (Supplemental Fig. 1A–D). The effect of the CW NIR laser on anti-influenza Ab responses was attenuated in sash mice, although a comparable level of Ab responses as well as a similar value of IgG2c:IgG1 ratios to those in the ID only group in WT mice was observed (Fig. 1A–D). Interestingly, a level of Ab responses in the CW NIR laser group was higher than that in the ID only group in sash-R mice (Fig. 1A–C). Anti-influenza IgG1 response in the CW NIR group in sash-R mice was significantly higher than that in sash mice (Fig. 1B, p = 0.0259). In addition, anti-influenza IgG2c response in the CW NIR group in sash-R mice was significantly higher than in the ID only group in WT mice (Fig. 1C, p = 0.0347). These results indicate that the attenuated Ab response to the CW NIR laser in sash mice was restored by the MC reconstitution in the skin tissue and that MCs are critical in augmentation of Ab response with the CW NIR laser.

We next assessed the contribution of MCs to protection augmented by the CW NIR laser. The vaccinated mice were challenged intranasally with homologous live influenza virus and monitored for survival time. Consistent with the previous reports (1820), the CW NIR laser treatment conferred better protection compared with the ID only group (Fig. 1I, 1J). The survival rate in the ID only group in sash mice was lower than that in WT mice (p = 0.0022), showing a critical role of MCs in host defense (3236). The survival rate in the CW NIR laser in sash mice was significantly lower than that in WT mice (Fig. 1I, 1J, WT versus sash in the CW NIR laser group: p  =  0.0030), suggesting that the effect of the CW NIR laser treatment on protection was attenuated in sash mice. In contrast, the CW NIR laser was able to confer significantly better protection compared with the ID only group in sash-R mice (Fig. 1I, 1J, the CW laser versus ID only group in sash-R mice: p = 0.0406), indicating that the effect of the CW NIR laser on protection was restored by the MC reconstitution. These results suggest that MCs play a critical role in augmentation of protective immunity with the CW NIR laser.

MCs are known to respond to physical stimuli, including heat (41, 42). However, consistent with the previous report (20), the PW NIR laser showed marginal immunological effects (Fig. 1A–H), although it generated the same degree of heat within the skin as did the CW NIR laser (19). These observations collectively suggest that heat plays a minimal role in the effect of the CW NIR laser.

Together, our results support the view that the adjuvant effect of the CW NIR laser in the context of ID vaccination functionally depends on MCs in skin.

MCs are known to significantly impact the adaptive immune response by regulating trafficking of DCs to dLN (33, 43). We have previously shown that exposures of skin to the CW NIR laser enhance migration of skin-resident migDCs, namely the Lang+ and LangCD11b migDC subsets, although they have no appreciable effect on cDCs within LN or plasmacytoid DCs, resulting in augmentation of the adaptive immunity (20). To investigate the role of MCs in the augmentation of migDC migration, we evaluated the migration response in sash and MC-reconstituted sash-R mice using the FITC paint technique (23). We applied FITC solution to the back skin of mice prior to the application of the 1-min CW NIR laser, followed by ID injection of a model vaccine, OVA. We then measured the migration of migDC subsets into the skin-dLN by flow cytometry as previously described (20).

Consistent with the previous report (20), the CW NIR laser increased the number of FITC+ migDC populations (Fig. 2B, 2C, p < 0.0001, 24 and 48 h) and Lang+ (48 h, p = 0.0341) and LangCD11b (p < 0.0001, 24 and 48 h) migDC subsets (Fig. 2D, 2E), as compared with the ID only group. In contrast, the CW NIR laser did not induce any increase in the migDC migration in sash mice, although a comparable level of the migration response to that in the ID vaccine only group of WT mice was observed (Fig. 2B–E). The number of FITC+ migDC and LangCD11b migDC populations of the CW NIR laser group in sash mice was significantly smaller than that in WT mice (Fig. 2A–E, migDC: 24 h, p  = 0.0031; 48 h, p  < 0.0001; LangCD11b migDC: 24 h, p  = 0.0492; 48 h, p  < 0.0001). Interestingly, the CW NIR laser increased the number of FITC+ migDC populations in sash-R mice compared with that in the ID vaccine only group of WT mice (Fig. 2A–C, p < 0.0001, 24 h) or the CW NIR laser group of sash mice (Fig. 2A–C, p = 0.0002, 24 h), indicating restoration of the migration response of migDCs to the CW NIR laser by the MC reconstitution. Consistently, sash-R mice showed the significantly higher number of FITC+ LangCD11b migDC population in the CW NIR group compared with those in the ID vaccine only group of WT mice (Fig. 2D, 2E, p < 0.0001, 24 h) or the CW NIR laser group of sash mice (Fig. 2D, 2E, p = 0.0002, 24 h).

FIGURE 2.

Effect of the NIR laser on DC migration in skin and the effect of the NIR laser on migration responses of migDC subsets in skin. Mice were painted with 0.5% FITC solution on the flank skin 4 h before vaccination with 40 μg of OVA, with or without the NIR laser treatment. Skin-dLN were analyzed by flow cytometry. (A) Gating schematic to identify DC subsets within skin-dLN. Cell counts of (B and C) DC subsets (D and E) and migDC subsets in the skin-dLN 24 and 48 h after OVA vaccination are shown. (A–D) n  =  13, 10, 4, 6, 6, 5, 4, and 4 at 24 h and n  =  20, 11, 4, 6, 6, 4, 3, and 5 at 48 h for OVA only in WT, CW 1064-nm laser in WT, PW 1064-nm laser in WT, OVA only in sash, CW 1064-nm laser in sash, PW 1064-nm laser in sash, OVA only in sash-R, and CW 1064-nm laser in sash-R groups, respectively. Results were pooled from six independent experiments and analyzed using two-way ANOVA followed by Tukey honestly significant difference tests.

FIGURE 2.

Effect of the NIR laser on DC migration in skin and the effect of the NIR laser on migration responses of migDC subsets in skin. Mice were painted with 0.5% FITC solution on the flank skin 4 h before vaccination with 40 μg of OVA, with or without the NIR laser treatment. Skin-dLN were analyzed by flow cytometry. (A) Gating schematic to identify DC subsets within skin-dLN. Cell counts of (B and C) DC subsets (D and E) and migDC subsets in the skin-dLN 24 and 48 h after OVA vaccination are shown. (A–D) n  =  13, 10, 4, 6, 6, 5, 4, and 4 at 24 h and n  =  20, 11, 4, 6, 6, 4, 3, and 5 at 48 h for OVA only in WT, CW 1064-nm laser in WT, PW 1064-nm laser in WT, OVA only in sash, CW 1064-nm laser in sash, PW 1064-nm laser in sash, OVA only in sash-R, and CW 1064-nm laser in sash-R groups, respectively. Results were pooled from six independent experiments and analyzed using two-way ANOVA followed by Tukey honestly significant difference tests.

Close modal

These results indicate that MCs mediate the enhanced migration of the migDC subsets induced by the CW NIR laser.

Exposure of skin to NIR light has been reported to induce generation of ROS in the skin tissue (4447). In turn, ROS have been shown to modulate the function of MCs (48). We therefore investigated if the CW NIR laser induces ROS generation in MCs, using an established culture model of BMMCs (49) and a ROS-sensitive fluorescence probe H2DCFDA (50). In addition, in light of the fact that ROS can travel across cell types in the tissue (51), we evaluated ROS generation in primary cultured keratinocytes.

After confirming the maturity and purity of BM-derived cells by flow cytometry (Supplemental Fig. 1A, 1B), cultured BMMCs were treated with the CW NIR laser for 1–3 min in vitro. ROS-reacted DCF-dependent fluorescence was measured by flow cytometry. Hydrogen peroxide–treated cells served as a positive control. DCF fluorescence–positive population was identified in the non–laser-treated control cells (Fig. 3A, 3B), indicating that this system could detect constantly generated ROS through aerobic metabolism (52). An addition of an ROS scavenger, NAC, significantly reduced DCF+ cells, confirming the constant generation from the control cells (Fig. 3A, 3B). The CW NIR laser treatment significantly increased the ROS-related DCF+ population in BMMCs (Fig. 3A, 3B, 2.0 folds for 1 min: p = 0.0278; 2.1 folds for 3 min: p = 0.0157) compared with the non–laser-treated control group. These data demonstrate that the CW NIR laser induces ROS generation in MCs. The CW NIR laser treatment also increased the ROS-related DCF+ population in keratinocytes compared with the non–laser-treated control group (Fig. 3C, 3D, p = 0.0420). This result indicates that keratinocytes could serve as a source of ROS for MCs in response to the CW NIR laser in skin.

FIGURE 3.

Effect of the NIR laser on cultured MCs and keratinocytes. (A and B) The effect of the NIR laser on MCs. (A) Release of ROS by the NIR laser treatment was assessed using a ROS-sensitive fluorescence probe H2DCFDA in BMMCs in vitro. The differentiated BMMC culture was treated with the NIR laser at a power of 0.5 W/cm2 for 1–3 min. ROS-activated DCF fluorescence was measured by flow cytometry. (B) Fold increase in DCF+ population compared with non–laser-treated control was calculated for each experiment. One-way ANOVA followed by the Tukey honestly significant difference (HSD) tests. n  =  6, 8, 12, 7, 6, 6, and 6 for no H2DCFDA control, no laser control, CW 1064-nm laser for 1 min, CW 1064-nm laser for 3 min, no laser control with NAC, CW 1064-nm laser for 1 min with NAC, and H2O2-treated positive control groups, respectively. Results were pooled from three independent experiments. (C and D) The effect of the NIR laser on primary cultured keratinocytes. (C) Release of ROS in primary cultured human dermal keratinocytes in response to the CW NIR laser at a power of 0.5 W/cm2 for 1 min was assessed in vitro as described above. (D) Fold increase in DCF+ population compared with non–laser-treated control was calculated. One-way ANOVA followed by Tukey HSD tests. n  =  3 for each of the following groups: no H2DCFDA control, no laser control, CW 1064-nm laser for 1 min, no laser control with NAC, CW 1064-nm laser for 1 min with NAC, and H2O2-treated positive control groups. Representative data from two independent experiments are presented.

FIGURE 3.

Effect of the NIR laser on cultured MCs and keratinocytes. (A and B) The effect of the NIR laser on MCs. (A) Release of ROS by the NIR laser treatment was assessed using a ROS-sensitive fluorescence probe H2DCFDA in BMMCs in vitro. The differentiated BMMC culture was treated with the NIR laser at a power of 0.5 W/cm2 for 1–3 min. ROS-activated DCF fluorescence was measured by flow cytometry. (B) Fold increase in DCF+ population compared with non–laser-treated control was calculated for each experiment. One-way ANOVA followed by the Tukey honestly significant difference (HSD) tests. n  =  6, 8, 12, 7, 6, 6, and 6 for no H2DCFDA control, no laser control, CW 1064-nm laser for 1 min, CW 1064-nm laser for 3 min, no laser control with NAC, CW 1064-nm laser for 1 min with NAC, and H2O2-treated positive control groups, respectively. Results were pooled from three independent experiments. (C and D) The effect of the NIR laser on primary cultured keratinocytes. (C) Release of ROS in primary cultured human dermal keratinocytes in response to the CW NIR laser at a power of 0.5 W/cm2 for 1 min was assessed in vitro as described above. (D) Fold increase in DCF+ population compared with non–laser-treated control was calculated. One-way ANOVA followed by Tukey HSD tests. n  =  3 for each of the following groups: no H2DCFDA control, no laser control, CW 1064-nm laser for 1 min, no laser control with NAC, CW 1064-nm laser for 1 min with NAC, and H2O2-treated positive control groups. Representative data from two independent experiments are presented.

Close modal

To assess the functional link between the ROS generation and augmentation of the migDC migration induced by the CW NIR laser, we pretreated mice by s.c. injections of NAC to suppress ROS generation in response to the CW NIR laser in skin (22) prior to measurements of DC migration, using the FITC paint technique.

The NAC treatment significantly attenuated the effect of the CW NIR laser on the migration response of the migDC population (Fig. 4A) and migDC subsets (Fig. 4B), although a comparable level of the migration responses in the ID only groups of NAC-treated mice to that of non–NAC-treated control mice was observed. The migration response of the CW NIR laser-treated group in NAC-treated mice was significantly smaller than that in non–NAC-treated mice (Fig. 4A, migDC: p = 0.0007; LangCD11b: p < 0.0001).

FIGURE 4.

The impact of ROS deletion on DC migration enhanced by the NIR laser. The effect of ROS deletion on the migration response of DCs to the NIR laser in skin. Mice were treated with s.c. injection of 100 mg/kg NAC daily for four consecutive days before vaccination and the NIR laser treatment, as appropriate. Mice were painted with 0.5% FITC solution on the flank skin 4 h before vaccination with 40 μg of OVA with or without the NIR laser treatment. Cell counts of (A) DC subsets and (B) migDC subsets in the skin-dLN 48 h after OVA vaccination are shown. Results were pooled from four independent experiments. One-way ANOVA followed by Tukey honestly significant difference tests. n  =  20, 11, 6, and 7 for OVA only in WT, CW 1064-nm laser in WT, OVA only in NAC-treated groups, and CW 1064-nm laser in NAC-treated groups, respectively. Data of the control group from Fig. 2 are shown for comparison.

FIGURE 4.

The impact of ROS deletion on DC migration enhanced by the NIR laser. The effect of ROS deletion on the migration response of DCs to the NIR laser in skin. Mice were treated with s.c. injection of 100 mg/kg NAC daily for four consecutive days before vaccination and the NIR laser treatment, as appropriate. Mice were painted with 0.5% FITC solution on the flank skin 4 h before vaccination with 40 μg of OVA with or without the NIR laser treatment. Cell counts of (A) DC subsets and (B) migDC subsets in the skin-dLN 48 h after OVA vaccination are shown. Results were pooled from four independent experiments. One-way ANOVA followed by Tukey honestly significant difference tests. n  =  20, 11, 6, and 7 for OVA only in WT, CW 1064-nm laser in WT, OVA only in NAC-treated groups, and CW 1064-nm laser in NAC-treated groups, respectively. Data of the control group from Fig. 2 are shown for comparison.

Close modal

These results suggest that ROS generation in response to the CW NIR laser enhances migration of migDCs in skin.

Our data suggest that ROS generation followed by migration of the migDCs plays a pivotal role in the effect of the CW NIR laser. To probe the contribution of ROS generation upon the CW NIR laser treatment to the formation of the adaptive immune response, we next treated mice with NAC prior to vaccination and examined the alteration of the immune response to the ID influenza vaccination.

The NAC treatment slightly increased a level of IgG responses as well as IgG2c:IgG1 ratios across the experimental groups, but none of these increases were significant compared with that in non–NAC-treated control mice (Fig. 5A–D). A level of Ab titers in the CW NIR laser group was not higher than that in the ID only group in NAC-treated mice, whereas an increased level of the Ab response was observed in the CW NIR laser group compared with that in the ID only group in non–NAC-treated control mice (Fig. 5A–C), indicating that ROS generation is involved in the adjuvant effect of the CW NIR laser.

FIGURE 5.

The impact of ROS deletion or selective ablation of DC subpopulations on the immune responses augmented by the NIR laser. The effect of the NIR laser on the immune response to the ID influenza vaccination was evaluated in NAC-treated mice or Ccr7−/− and Batf3−/− mice. For antioxidant treatment, mice were treated with NAC for four consecutive days before vaccination and the NIR laser treatment as described above. Serum anti-influenza specific (A) IgG, (B) IgG1, (C) IgG2c, and (D) IgG2c/IgG1 ratio 4 d after challenge are shown. The p values for the tests of treatments within the WT genotype were based on a one-way ANOVA between subjects of the WT data with Tukey post hoc tests, whereas those for other comparisons are based on a two-way treatment by genotype ANOVA with Tukey tests. (E and F) Systemic anti-influenza specific T cell responses measured in restimulated splenocytes upon influenza vaccination. Levels of (E) IFN-γ and (F) IL-4 in supernatants are shown. (A–D) n  =  44, 48, 38, 33, 25, 11, 12, 11, 14, 14, 3, 8, 9, 9, 3, and 6 and (E and F) n  =  35, 39, 30, 24, 16, 11, 12, 11, 14, 14, 3, 8, 9, 9, 3, and 6 for no vaccine, vaccine ID only, vaccine ID + CW 1064-nm laser, vaccine ID + PW 1064-nm laser, vaccine i.m., vaccine ID only in NAC-treated groups, vaccine ID + CW 1064-nm laser in NAC-treated groups, vaccine ID + PW 1064-nm laser in NAC-treated groups, vaccine ID only in Ccr7−/− groups, vaccine ID + CW 1064-nm laser in Ccr7−/− groups, vaccine ID + PW 1064-nm laser in Ccr7−/− groups, vaccine i.m. in Ccr7−/− groups, vaccine ID only in Batf3−/− groups, vaccine ID + CW 1064-nm laser in Batf3−/− groups, vaccine ID + PW 1064-nm laser in Batf3−/− groups, and vaccine i.m. in batf3−/ groups, respectively. (A–F) WT data from Fig. 1 are shown for comparison. Results were pooled from six independent experiments. (G and H) The effect of the NIR laser on protection. (G) Kaplan–Meier survival plots. (H) The effect of the NIR laser on body weight following viral challenge. Body weights were monitored daily for 15 d. Mean body weight ± SEM of each experimental group was determined at each time point. (G and H) n  =  10, 12, 13, 4, 5, and 8 for no vaccine in WT, vaccine ID only in WT, vaccine ID + CW 1064-nm laser in WT, no vaccine in Batf3−/−, vaccine ID only in Batf3−/−, and vaccine ID + CW 1064-nm laser in Batf3−/− groups, respectively. Gehan–Breslow–Wilcoxon test. Results were pooled from three independent experiments. WT data from Fig. 1 are shown for comparison.

FIGURE 5.

The impact of ROS deletion or selective ablation of DC subpopulations on the immune responses augmented by the NIR laser. The effect of the NIR laser on the immune response to the ID influenza vaccination was evaluated in NAC-treated mice or Ccr7−/− and Batf3−/− mice. For antioxidant treatment, mice were treated with NAC for four consecutive days before vaccination and the NIR laser treatment as described above. Serum anti-influenza specific (A) IgG, (B) IgG1, (C) IgG2c, and (D) IgG2c/IgG1 ratio 4 d after challenge are shown. The p values for the tests of treatments within the WT genotype were based on a one-way ANOVA between subjects of the WT data with Tukey post hoc tests, whereas those for other comparisons are based on a two-way treatment by genotype ANOVA with Tukey tests. (E and F) Systemic anti-influenza specific T cell responses measured in restimulated splenocytes upon influenza vaccination. Levels of (E) IFN-γ and (F) IL-4 in supernatants are shown. (A–D) n  =  44, 48, 38, 33, 25, 11, 12, 11, 14, 14, 3, 8, 9, 9, 3, and 6 and (E and F) n  =  35, 39, 30, 24, 16, 11, 12, 11, 14, 14, 3, 8, 9, 9, 3, and 6 for no vaccine, vaccine ID only, vaccine ID + CW 1064-nm laser, vaccine ID + PW 1064-nm laser, vaccine i.m., vaccine ID only in NAC-treated groups, vaccine ID + CW 1064-nm laser in NAC-treated groups, vaccine ID + PW 1064-nm laser in NAC-treated groups, vaccine ID only in Ccr7−/− groups, vaccine ID + CW 1064-nm laser in Ccr7−/− groups, vaccine ID + PW 1064-nm laser in Ccr7−/− groups, vaccine i.m. in Ccr7−/− groups, vaccine ID only in Batf3−/− groups, vaccine ID + CW 1064-nm laser in Batf3−/− groups, vaccine ID + PW 1064-nm laser in Batf3−/− groups, and vaccine i.m. in batf3−/ groups, respectively. (A–F) WT data from Fig. 1 are shown for comparison. Results were pooled from six independent experiments. (G and H) The effect of the NIR laser on protection. (G) Kaplan–Meier survival plots. (H) The effect of the NIR laser on body weight following viral challenge. Body weights were monitored daily for 15 d. Mean body weight ± SEM of each experimental group was determined at each time point. (G and H) n  =  10, 12, 13, 4, 5, and 8 for no vaccine in WT, vaccine ID only in WT, vaccine ID + CW 1064-nm laser in WT, no vaccine in Batf3−/−, vaccine ID only in Batf3−/−, and vaccine ID + CW 1064-nm laser in Batf3−/− groups, respectively. Gehan–Breslow–Wilcoxon test. Results were pooled from three independent experiments. WT data from Fig. 1 are shown for comparison.

Close modal

Our data earlier confirmed the causal link between ROS generation and enhanced migration of the migDC subsets in skin in response to the CW NIR laser. In addition, we have previously demonstrated that the Lang+ DC subset mediates migration of the LangCD11b DC subset in response to the CW NIR laser, using the Lang–diphtheria toxin receptor mouse model (20). However, this model cannot specify the distinct roles of epidermal Langerhans cells and Lang+ dermal DCs in the effect of the CW NIR laser. To further evaluate the contribution of the migration of the migDC subsets via ROS generation to the adjuvant effect, we determined the alterations of the immune response to ID vaccination in Batf3−/− mice. Batf3−/− mice lack the cross-presenting CD103+ DC subset in skin, which is included in Lang+ dermal DCs (53, 54), in mice with the C57BL/6 background (55). Batf3−/− mice have been, therefore, used to test the contribution of the CD103+ migDC subset in several models of skin infection (56, 57). Ccr7 loss in Ccr7−/− mice inhibits trafficking of migDC populations from the peripheral tissue (58, 59). The immune response in Ccr7−/− mice was also examined as a control in these experiments to confirm the importance of migDCs in the formation of the adaptive immunity to ID vaccination. In addition, we compared the immune responses between ID and i.m. vaccination in these genetic mouse models to assess the contribution of the migDC subsets to the immune response augmented with the treatment of skin with the CW NIR laser.

Consistent with the previous report (20), Ccr7−/− mice receiving an ID vaccine showed a significant reduction in anti-influenza IgG and IgG2c (Fig. 5A, 5C, WT versus Ccr7−/− in the ID only group: p  < 0.0001), with similar IgG2c:IgG1 ratios compared with WT mice (Fig. 5D). In addition, IFN-γ influenza-specific splenocyte responses in Ccr7−/− mice were significantly reduced, as compared with those in WT mice (Fig. 5E, WT versus Ccr7−/− in the vaccine ID only group: p  < 0.0001, WT versus Ccr7−/− in the CW NIR laser group: p  <  0.0001). A level of Ab responses in the CW NIR laser group in Ccr7−/− mice showed a significant reduction for IgG (Fig. 5A, p  < 0.0001) and statistically marginal reduction for IgG2c (Fig. 5C, p  = 0.0693) compared with that in WT mice. These results support dependence of the response to the ID vaccination with or without the CW NIR laser treatment on migDC, as Ccr7−/− mice lack CCR7-dependent migration of migDCs (59).

Interestingly, a level of Ab titers in the CW NIR laser group was not higher than that in the ID only group in Batf3−/− mice, whereas a comparable level of the Ab response of the ID only and CW NIR laser groups in Batf3−/− mice to that of the ID only group in WT mice was observed (Fig. 5A–C). A slight increase in a level of IgG1 responses (Fig. 5B) with a decrease in IgG2c:IgG1 ratios (Fig. 5D) across the experimental groups in Batf3−/− mice was observed, which is consistent with the previous reports showing that the CD103+ DC subset is critical for TH1 immunity (54). None of these changes were significant compared with that in WT mice. These results indicate that Batf3−/− mice were able to mount the comparable response to WT mice to ID vaccination, but they were not able to respond to the CW NIR laser.

IFN-γ influenza-specific splenocyte responses were reduced in Batf3−/− mice as compared with those in WT mice (Fig. 5E, WT versus Batf3−/− in the vaccine ID only group: p  < 0.0001; in the CW laser group: p  < 0.0071), whereas IL-4 responses were not significantly changed (Fig. 5F). In contrast, i.m. administration of the same dose of the vaccine mounted a comparable level of anti-influenza Ab responses across the IgG subclasses among WT, Ccr7−/−, and Batf3−/− mice (Fig. 5A–C), highlighting a critical role of the dermal CD103+ DC subset in the effect of the CW NIR laser on the Ab response in the context of the ID vaccination. These results collectively demonstrate that the dermal CD103+ DC subset is critical to the adjuvant effect of the CW NIR laser, as opposed to epidermal Langerhans cells playing a predominant role in the adjuvant effect of the visible PW laser adjuvant (15).

We next assessed the contribution of the dermal CD103+ DC subset to protection augmented by the CW NIR laser. Mice were challenged intranasally with homologous live influenza virus and monitored for survival time as described above. The survival rate of unvaccinated Batf3−/− mice was lower than that of WT mice (Fig. 5G, p  =  0.0134), showing a critical role of the dermal CD103+ DC subset in host defense (55). Consistent with the Ab response study (Fig. 5A–C), the survival rate in the CW NIR laser in Batf3−/− mice was significantly lower than that in WT mice (Fig. 5G, WT versus Batf3−/− in the CW NIR laser group: p  =  0.0003), with greater weight loss upon viral challenge (Fig. 5H), suggesting that the beneficial effect of the CW NIR laser on protection against lethal influenza virus challenge observed in WT mice was attenuated in Batf3−/− mice. These results confirm an important role of the CD103+ migDC subset in the beneficial effect of the CW NIR laser on protection.

In conclusion, these results support the view that ROS generation in response to the CW NIR laser modulates the MC function and enhances the migration of the CD103+ migDC subset in skin, ultimately augmenting the immune response to ID vaccination.

MCs have been shown to induce functional changes in microcirculation via their secretory responses, regulating vascular flow and permeability and recruitment of inflammatory cells (31). We therefore hypothesized that the CW NIR laser establishes an immunostimulatory milieu to augment protective immune responses in microcirculation in skin via MC activation. To test this hypothesis, we first measured microvascular permeability in the skin tissue treated with the CW NIR laser in WT and MC-deficient sash mice.

The CW, but not PW, NIR laser treatment increased microvascular permeability immediately after the treatment (Fig. 6A, 6B, the non–laser-treated versus laser-treated group at 0 h: p = 0.0305). The increase in microvascular permeability was no longer observed 1 h after the treatment, suggesting that the effect of the NIR laser on microvascular permeability resolved within 1 h. The PW NIR laser did not induce applicable increase, which confirms that heat generation in skin plays a minimum role in the functional changes induced by the CW NIR laser. To investigate the role of MCs in the transient increase in microvascular permeability, we further assessed the effect of the CW NIR laser in sash mice. No increase in microvascular permeability was observed in sash mice (Fig. 6C), demonstrating that the increase in microvascular permeability induced by the CW NIR laser was mediated by MCs.

FIGURE 6.

The effect of the NIR laser on microvascular permeability in skin. (A) Representative images of the mouse back skin 30 min after i.v. injection of Evans blue. (B) Quantification of tissue concentration of Evans blue 0, 1, 2 and 6 h after the 1-min CW or PW NIR 1064-nm laser treatment is shown. n  =  8, 12, and 6 for no laser, CW 1064-nm laser, and PW 1064-nm laser groups, respectively, at 0 h, and n  =  3, 3–4, and 3–4 for no laser, CW 1064-nm laser, and PW 1064-nm laser groups, respectively, at 1, 2, and 6 h. One-way ANOVA followed by Tukey honestly significant difference (HSD) tests. (C), The effect of the NIR laser on microvascular permeability in skin in WT and sash mice. Quantification of tissue concentration of Evans blue 0 h after the 1-min CW NIR 1064-nm laser treatment in WT and sash mice. n  =  8, 12, 3, 5, and 5 for no laser in WT, CW 1064-nm laser in WT, no laser in sash, CW 1064-nm laser in sash, and c48/80 in WT mice groups, respectively. Two-way ANOVA followed by Tukey HSD tests. WT data of the no laser group at 0 h from (B) are shown for comparison. (A–C) Results were pooled from three independent experiments.

FIGURE 6.

The effect of the NIR laser on microvascular permeability in skin. (A) Representative images of the mouse back skin 30 min after i.v. injection of Evans blue. (B) Quantification of tissue concentration of Evans blue 0, 1, 2 and 6 h after the 1-min CW or PW NIR 1064-nm laser treatment is shown. n  =  8, 12, and 6 for no laser, CW 1064-nm laser, and PW 1064-nm laser groups, respectively, at 0 h, and n  =  3, 3–4, and 3–4 for no laser, CW 1064-nm laser, and PW 1064-nm laser groups, respectively, at 1, 2, and 6 h. One-way ANOVA followed by Tukey honestly significant difference (HSD) tests. (C), The effect of the NIR laser on microvascular permeability in skin in WT and sash mice. Quantification of tissue concentration of Evans blue 0 h after the 1-min CW NIR 1064-nm laser treatment in WT and sash mice. n  =  8, 12, 3, 5, and 5 for no laser in WT, CW 1064-nm laser in WT, no laser in sash, CW 1064-nm laser in sash, and c48/80 in WT mice groups, respectively. Two-way ANOVA followed by Tukey HSD tests. WT data of the no laser group at 0 h from (B) are shown for comparison. (A–C) Results were pooled from three independent experiments.

Close modal

The endothelial dysfunction caused by damage may induce an increase of microvascular permeability (60). The laser parameter for the CW NIR laser treatment used in this study has been demonstrated to be non–tissue damaging in our previous studies (1820). Consistently, the laser treatment did not significantly increase the number of TUNEL+ cells in skin (Supplemental Fig. 2).

These results confirm that the CW NIR laser activates MCs and induces functional changes in microcirculation in skin.

Microcirculation including blood vessels and the lymphatic network plays an indispensable role in recruitment of immune cells to inflammatory sites, transportation of pathogenic Ags into dLN, and migration of Ag-presenting and effector cells to secondary lymphoid organs (61). We next determined the response of the vascular and lymphatic networks in skin to the CW NIR laser without vaccination. Mice received exposures of the CW NIR laser on the ear skin tissue at 5.0 W/cm2 for 1 min. Six hours later, we performed immunofluorescence of the whole-mount ear tissue and stained the lymphatic network and skin-resident DCs for analysis by confocal imaging.

The CW NIR laser treatment increased the density of the lymphatic network (Fig. 7A–C, the non–laser-treated versus laser-treated group for lymphatic density: p  = 0.0008), suggesting increased lymphatic flow in the laser-treated tissue, which is typically induced by an increase in microvascular permeability (62). Interestingly, this functional change was accompanied by a concomitant decrease in the distance between lymphatic vessels and Lang+, but not CD11b+, DCs (Fig. 7D, the non–laser-treated versus laser-treated group for Lang+ DC: p  = 0.0302), indicating that the functional changes in the lymphatics provided migration cues for skin-resident DCs. The CW NIR laser treatment without vaccination induced no change in the number of migDCs in the treated skin (Fig. 7E) nor in skin-dLN, which was examined using FITC painting technique (Fig. 7F, 7G), suggesting that Ag challenge is necessary to induce the migDC migration into LN (63).

FIGURE 7.

The effect of the NIR laser on microcirculation and DC migration without Ag challenge in skin. (AE) Morphometry of the vascular and lymphatic networks in skin with or without the NIR laser treatment. Morphological changes of the vascular and lymphatic networks in skin were measured in stacks of the three-dimensional confocal images using Imaris software. The depilated mouse ears were treated with the NIR laser, and the whole-mount ear tissue was immunostained and imaged for blood vessels, lymphatics, and DC subsets 6 h after the treatment. (A) Representative confocal images of mouse ear stained for blood vessels, lymphatics, and DCs 6 h following the CW NIR laser treatment. Scale bar, 40 μm. (B and C) Morphometry of blood and lymphatic vessels and DCs in skin using Imaris software. Two-way ANOVA followed by Tukey honestly significant difference (HSD) tests. (A–C) n  =  17 and 17 for no laser control and CW NIR laser-treated groups, respectively. (D) Distances between vasculature and DCs and (E) density of Lang+ and CD11b+ DCs in skin. n  =  5–8 and 5–8 for no laser control and CW NIR laser-treated groups, respectively. Two-way ANOVA followed by Tukey HSD tests. (A–E) Results were pooled from five independent experiments. (F and G) The effect of the NIR laser on the migration response of migDC subsets without Ag challenge in skin. Mice were painted with a 0.5% FITC solution on the flank skin 4 h before the NIR laser treatment without any Ag challenge. Cell counts of (F) DC subsets and (G) migDC subsets in the skin-dLN 24 and 48 h after FITC painting are shown. (F and G) n  =  13–14, 7, and 7 for no laser, CW 1064-nm laser, and PW 1064-nm laser groups, respectively. Two-way ANOVA followed by Tukey HSD tests. Results were pooled from four independent experiments.

FIGURE 7.

The effect of the NIR laser on microcirculation and DC migration without Ag challenge in skin. (AE) Morphometry of the vascular and lymphatic networks in skin with or without the NIR laser treatment. Morphological changes of the vascular and lymphatic networks in skin were measured in stacks of the three-dimensional confocal images using Imaris software. The depilated mouse ears were treated with the NIR laser, and the whole-mount ear tissue was immunostained and imaged for blood vessels, lymphatics, and DC subsets 6 h after the treatment. (A) Representative confocal images of mouse ear stained for blood vessels, lymphatics, and DCs 6 h following the CW NIR laser treatment. Scale bar, 40 μm. (B and C) Morphometry of blood and lymphatic vessels and DCs in skin using Imaris software. Two-way ANOVA followed by Tukey honestly significant difference (HSD) tests. (A–C) n  =  17 and 17 for no laser control and CW NIR laser-treated groups, respectively. (D) Distances between vasculature and DCs and (E) density of Lang+ and CD11b+ DCs in skin. n  =  5–8 and 5–8 for no laser control and CW NIR laser-treated groups, respectively. Two-way ANOVA followed by Tukey HSD tests. (A–E) Results were pooled from five independent experiments. (F and G) The effect of the NIR laser on the migration response of migDC subsets without Ag challenge in skin. Mice were painted with a 0.5% FITC solution on the flank skin 4 h before the NIR laser treatment without any Ag challenge. Cell counts of (F) DC subsets and (G) migDC subsets in the skin-dLN 24 and 48 h after FITC painting are shown. (F and G) n  =  13–14, 7, and 7 for no laser, CW 1064-nm laser, and PW 1064-nm laser groups, respectively. Two-way ANOVA followed by Tukey HSD tests. Results were pooled from four independent experiments.

Close modal

Together, these results demonstrate that the CW NIR laser induces functional changes in the lymphatic network and provides migration cues for skin-resident DCs toward the lymphatics in skin.

The CW NIR laser appears to induce a transient increase in microvascular permeability and lymphatic flow, which is consistent with the tissue changes upon MC activation (64). Chemical agents, which are designed to stimulate MC function, generally induce prolonged and exacerbated inflammatory responses (65). In contrast, exposures of skin to a low-power CW NIR laser have been shown to be free from tissue damage or inflammation, evidenced by no polymorphonuclear infiltration (1820) with upregulation of a selective set of chemokines (19). We therefore hypothesized that the CW NIR laser induces “differential” or “selective” secretion of mediators without degranulation of MCs (66, 67). To test this hypothesis, we assessed expression of a selective set of chemokines, which was established previously (19), as well as inflammatory cytokines in WT and MC-deficient sash mice.

The CW, but not PW, NIR laser treatment induced temporary expression of the selective chemokines at 6 h. Student t test with stepdown bootstrap and false discovery rate corrections showed that none of the nine selected chemokines and cytokines of importance predicted the effect of the NIR laser treatment significantly. However, a multivariate discriminant analysis that tests the linear combination of the nine genes, which optimally discriminates the treatments, found a significant treatment effect in WT mice (Fig. 8A, the non–laser-treated versus laser-treated group in WT: p  = 0.0437; Supplemental Fig. 3). Consistent with the previous report (19), no upregulation of inflammatory cytokines including Tnf and Il1b was observed. This change appeared to be transient in nature, as the upregulation of the genes of interest was not observed at 2 or 24 h (Fig. 8B). Importantly, no significant increase in the selective chemokine expression was observed in sash mice with the CW NIR laser treatment (Fig. 8A), suggesting that these changes in chemokine expression were dependent on MCs.

FIGURE 8.

A critical role of MCs and ROS in the chemokine expression in skin in response to the NIR laser. The effect of the NIR laser on the chemokine expression in skin was evaluated in WT and sash mice. The role of ROS in the chemokine expression in skin in response to the CW NIR laser was also evaluated in NAC-treated WT mice. For antioxidant treatment, mice were treated with NAC for four consecutive days before the NIR laser treatment as described above. (A) The expression of chemokines in the mouse back skin was measured 6 h following the CW NIR laser treatment in (left) WT, (middle) sash, and (right) NAC-treated WT mice, using qPCR. n = 7, 7, 4, 3, 3, 3, and 3 for no laser control in WT, CW, and PW 1064-nm laser treatment in WT groups; no laser control in sash, CW 1064-nm laser treatment in sash, NAC-treated only, and CW 1064-nm laser NAC-treated groups, respectively. (B) The expression of chemokines in the mouse back skin in (left) 2 and (right) 24 h after the NIR laser treatment in WT mice. n = 4 and 4 at 2 h, and n = 3 and 3 at 24 h for no NIR and CW 1064-nm laser groups, respectively. (A and B) Student t test with stepdown bootstrap and false discovery rate corrections followed by a multivariate discriminant analysis of the nine genes was used as appropriate. Error bars show means ± SEM.

FIGURE 8.

A critical role of MCs and ROS in the chemokine expression in skin in response to the NIR laser. The effect of the NIR laser on the chemokine expression in skin was evaluated in WT and sash mice. The role of ROS in the chemokine expression in skin in response to the CW NIR laser was also evaluated in NAC-treated WT mice. For antioxidant treatment, mice were treated with NAC for four consecutive days before the NIR laser treatment as described above. (A) The expression of chemokines in the mouse back skin was measured 6 h following the CW NIR laser treatment in (left) WT, (middle) sash, and (right) NAC-treated WT mice, using qPCR. n = 7, 7, 4, 3, 3, 3, and 3 for no laser control in WT, CW, and PW 1064-nm laser treatment in WT groups; no laser control in sash, CW 1064-nm laser treatment in sash, NAC-treated only, and CW 1064-nm laser NAC-treated groups, respectively. (B) The expression of chemokines in the mouse back skin in (left) 2 and (right) 24 h after the NIR laser treatment in WT mice. n = 4 and 4 at 2 h, and n = 3 and 3 at 24 h for no NIR and CW 1064-nm laser groups, respectively. (A and B) Student t test with stepdown bootstrap and false discovery rate corrections followed by a multivariate discriminant analysis of the nine genes was used as appropriate. Error bars show means ± SEM.

Close modal

Our data suggest that ROS generation plays a critical role in the adjuvant effect of the CW NIR laser. To explore the possible causal link between ROS generation upon the CW NIR laser treatment and chemokine expression, we next treated mice with NAC and examined the alteration of the chemokine response. The NAC treatment attenuated the effect of the CW NIR laser on expression of the selective set of chemokines (Fig. 8A), indicating that ROS generation mediates the chemokine expression in skin.

To further uncover pathways involved in the ROS generation and chemokine responses, we treated cultured BMMCs or keratinocytes with the CW NIR laser and measured expression of the selective set of chemokines in BMMCs or evaluated an expression array of inflammatory cytokines and receptors in keratinocytes in vitro. Except for a slight increase noted in Ccl11, Ccl17, and Ccl20 in BMMCs, no significant change was observed in the other chemokines in BMMCs or 84 genes examined on the array in keratinocytes (Supplemental Fig. 4). These results suggest that the skin microenvironment or collaboration among skin cells is essential to orchestrate the response to the CW NIR laser.

Together, these results further support the view that the CW NIR laser induces transient and selective activation of MCs, possibly in concert with other types of skin cells, via ROS generation.

Migration of DCs is a critical step for the initiation of protective immune responses (61). In response to inflammatory stimuli, the lymphatic network is known to increase expression of CCL21 on lymphatic vessels, triggering migration of skin-resident DCs (68, 69). Because our earlier observations showed that the CW NIR laser induced migrational changes of migDCs, we further hypothesized that the immunostimulatory milieu established by the selective activation of MCs with the CW NIR laser induces CCL21 response in the lymphatics. To test this hypothesis, we performed immunofluorescence of CCL21 and the lymphatic network in the mouse ear tissue exposed to the CW NIR laser for analysis by confocal imaging. To evaluate the contribution of MCs, we also assessed CCL21 response in MC-deficient sash mice.

CCL21 expression on Lyve-1+ lymphatics was distributed among small patch structures in the control and exposed skin tissue (Fig. 9A), as previously reported (70). Image analysis revealed an increase in the density of CCL21+ cells in the exposed skin tissue compared with the nonexposed control tissue (Fig. 9B, p  = 0.0314), which appeared to mediate the chemotaxis of migDCs to lymphatic vessels. Importantly, the effect of the CW NIR laser on the CCL21 response was not observed in sash mice (Fig. 9A, 9B). In the current study, we have shown that ROS are generated in MCs and keratinocytes in response to the CW NIR laser (Fig. 3A–D). Thus, it is possible that ROS from various sources in skin directly stimulate lymphatic endothelial cells and induce CCL21 expression. However, these data indicate that MCs are required for the upregulation of CCL21 in response to the CW NIR laser and that mediators derived from activated MCs via ROS generation are critically involved in the CCL21 upregulation.

FIGURE 9.

The effect of the NIR laser on CCL21 expression on the lymphatics in skin. Quantification of CCL21 expression on the lymphatics in stacks of the three-dimensional confocal images using Imaris software. The depilated mouse ears were treated with the NIR laser, and the whole-mount ear tissue was stained and imaged for the lymphatics and CCL21 6 h after the treatment. (A) Representative confocal images of CCL21 immunofluorescence are shown. Scale bar, 40 μm. (B) Quantification of CCL21+ cells on Lyve-1+ lymphatic vessels is shown. n  =  6, 6, 3, and 3 for no laser control in WT (CD11c-EYFP), CW 1064-nm laser treatment in WT (CD11c-EYFP), no laser control in sash, and CW 1064-nm laser in sash groups, respectively. Two-way ANOVA followed by Tukey honestly significant difference tests. Results were pooled from three independent experiments. (C) Schematic diagram of the mechanism of action of the CW NIR laser adjuvant.

FIGURE 9.

The effect of the NIR laser on CCL21 expression on the lymphatics in skin. Quantification of CCL21 expression on the lymphatics in stacks of the three-dimensional confocal images using Imaris software. The depilated mouse ears were treated with the NIR laser, and the whole-mount ear tissue was stained and imaged for the lymphatics and CCL21 6 h after the treatment. (A) Representative confocal images of CCL21 immunofluorescence are shown. Scale bar, 40 μm. (B) Quantification of CCL21+ cells on Lyve-1+ lymphatic vessels is shown. n  =  6, 6, 3, and 3 for no laser control in WT (CD11c-EYFP), CW 1064-nm laser treatment in WT (CD11c-EYFP), no laser control in sash, and CW 1064-nm laser in sash groups, respectively. Two-way ANOVA followed by Tukey honestly significant difference tests. Results were pooled from three independent experiments. (C) Schematic diagram of the mechanism of action of the CW NIR laser adjuvant.

Close modal

In summary, these results show that the CW NIR laser induces CCL21 expression in the lymphatics in skin via MC activation and confirm our earlier observations that the CW NIR laser provides migratory cues for migDCs.

In this study, we have shown for the first time, to our knowledge, that a CW NIR laser with a distinct power and dose has a unique capability to reproducibly activate selective innate programs, including MC function and migDC migration, via ROS generation without inducing prolonged and potentially harmful inflammatory responses in skin, thus augmenting the adaptive immune response (Fig. 9C). These mechanistic findings would significantly contribute to optimization of wavelength, power, duration of the treatment, the timing and location of delivery, and the size of the treatment spot on the skin of a CW NIR laser adjuvant in the context of ID vaccination for better safety and efficacy of this technology.

Although other medical PW lasers have been similarly reported to show the adjuvant effect to ID vaccines (10, 11), use of a CW NIR laser has clear advantages over the other classes of lasers. Current clinical-grade PW laser systems in these reports are typically large in size, complicated in machinery to generate PW, and expensive, posing financial and engineering challenges including high cost per unit and needs of maintenance by laser specialists. In contrast, the low-wattage CW NIR lasers are a mature and simple technology, and a small device emitting a CW NIR laser at the required powers used in this application (5 W/cm2 and below) proved to be economically produced (18), making this technology feasible and suitable for mass-vaccination programs and other clinically applicable approaches.

In this study, we have shown that ROS generation in MCs is critical for the effect of the CW NIR laser. There is ample evidence showing that NIR light induces generation of ROS in exposed tissue or cells. Low-power (1 mW–5 W/cm2) NIR light between 600 and 1000 nm has been established to show diverse beneficial effects in exposed tissue, including pain relief, facilitation of tissue regeneration, and reduction of inflammation. These biological effects of NIR light are broadly defined as photobiomodulation (44, 7176). Although the precise mechanisms of action for photobiomodulation are still under debate (44, 7577), it is clear that the effect of NIR light is partially, if not entirely, mediated by ROS (44, 7376). In turn, there is ample evidence showing that NIR light induces generation of ROS in exposed tissue or cells. Exposures to NIR light between 760 and 1400 nm have been shown to increase ROS generation in tumor cells (7880), keratinocytes (79), fibroblasts (81), and the skin tissue (46, 47, 82). In contrast to photobiomodulation, ROS generation upon exposure to NIR light has been linked to deleterious effects, including premature skin aging (83, 84) and the cytotoxic effect (85, 86). Beneficial or deleterious, ROS have been postulated to be generated by mitochondrial cytochrome c oxidase in the respiratory electron transport chain in response to NIR light exposure (87, 88), ultimately activating the NF-κB signaling pathway and innate signaling (44, 7375). In contrast, the numerous reliable data have reported that ROS play a significant role in MC-dependent inflammatory processes and activation of intracellular signaling for production of proinflammatory cytokines that regulate the innate immune response (48, 89). In accordance, we found that the CW NIR laser induced ROS generation in MCs (Fig. 3) and that the effects of the CW NIR laser on the migration of migDCs and the adaptive immune response are functionally dependent on ROS generation (Figs. 4, 5). In addition, in the absence of MCs, we observed no upregulation of the selective set of chemokines (Fig. 8) nor subsequent augmentation of the immune response by the CW NIR laser (Fig. 1). These results clearly indicate that MCs locate at an intersection between the adaptive immune response and ROS generation in response to the CW NIR laser. However, the precise mode of action for the MC activation via ROS generation upon the CW NIR laser treatment has yet to be defined. For example, it is possible that ROS generated in adjacent cells reach MCs in skin, modulating MC function indirectly, as ROS are small enough to travel across cell types in tissues (51). Further studies are warranted to determine the precise molecular identify of ROS, subcellular localization of ROS generation, spatial and temporal dynamics of ROS distribution in tissues, and the mode of activation of innate signaling pathways by ROS in response to the CW NIR laser treatment to selectively activate MCs and induce the specific immunomodulatory effect without deleterious inflammation.

Our data collectively demonstrate that there are distinct differences in the immunological effect between CW and PW NIR lasers. Although both CW and PW NIR lasers have been reported to induce ROS generation in the biological system (46, 47, 7882, 90, 91), the exact molecular identify, temporal distribution, or local concentration of ROS leading to the immunological events in response to the NIR lasers has not been characterized. A PW NIR laser has been shown to be more effective in ROS generation (90, 91) and photobiomodulation (92, 93) than CW in some biological systems. Because the pulse frequency, power level, and exposure time of an NIR laser can dictate a level of ROS generation in tissues (90, 91), we might be able to identify a parameter of PW NIR laser for the desired immunological effect. Nonetheless, in the current study, a nanosecond-pulsed 1064-nm laser at a frequency of 10 kHz did not show any significant immunological effect, suggesting that this particular parameter is suboptimal in inducing proper ROS generation for the subsequent immunological events. An optimal parameter of PW NIR laser might be sought for in the context of the molecular identify, local sources, and subcellular localization of ROS in response to the NIR laser ultimately leading to efficient activation of innate signaling in the future study.

IR irradiation and heat generation in exposed tissues have been linked to biological effects, including premature skin aging via expression of MMP-1 or generation of ROS (94). Accordingly, heat generated by NIR exposures could have a predominant role in MC activation and augmentation of the immune response. In fact, MCs are capable of responding to physical stimuli through transient receptor potential channels, which are functionally coupled to calcium signaling and regulate mediator release in MCs (42). Moreover, transient receptor potential channels of the vanilloid subtype have been shown to respond to IR radiation (41). However, our study shows that a thermal mechanism is not a major driver of the impact of the NIR laser on the immune system. As the CW and PW 1064-nm lasers in this study were emitted from the same platform with the same wavelength and average power, they proved to have the same heat generation profile in skin (19). Despite the same thermal profile, the PW NIR laser has shown little impact on MC function in skin (Fig. 6), if any, resulting in the marginal effect on the immune response (Fig. 1) (20). It is still possible that heat is required for the CW NIR laser to have these effects, as one study shows that water-filtered NIR light between 760 and 1400 nm induces ROS generation in a temperature-dependent manner (82). Nonetheless, our data support the view that heat alone is not sufficient to induce the subsequent immunological events and that specific photochemical events related to the CW NIR laser exposure are required for these effects.

Cytokines and chemokines are released by MCs, keratinocytes, DCs, melanocytes, tissue-resident macrophages, and inflammatory infiltrates in skin (95). The cutaneous cytokine and chemokine network is critically involved in regulation of skin functions as well as inflammatory conditions such as psoriasis or atopic dermatitis (9598). Because of their anatomical proximity, collaborative activities between MCs and keratinocytes via cytokine and chemokine signaling have been reported in coordinating cell proliferation and differentiation (96, 99102) and the immune response and inflammation (95, 103). The chemokines and their receptors upregulated in response to the CW NIR laser have been reported to be expressed in both MCs (103) and keratinocytes (95, 104) under certain conditions. In the current study, we have shown that the chemokine response to the CW NIR laser in the mouse skin is dependent on ROS generation and MCs (Fig. 8). Although ROS generation was observed in cultured BMMCs and keratinocytes in vitro (Fig. 3), small changes were detected in the subsequent chemokine expression in the individual culture systems (Supplemental Fig. 4). These results suggest that the chemokine response to the CW NIR laser is dependent on the local skin microenvironment and interactions among MCs, keratinocytes, and possibly other types of cells, including fibroblasts in close association with MCs and keratinocytes in skin. Further investigation is warranted to uncover the cross-talk among these cells in the context of regulation of this complex skin chemokine network in response to the CW NIR laser.

Our data show that the CW NIR laser induces a transient increase in microvascular permeability and lymphatic flow, which is consistent with the tissue changes upon MC activation (64). Contrary to chemical agents that are designed to stimulate MC function and may cause prolonged inflammatory responses with off-target effects (65), the low-power NIR exposures of skin are free from tissue damage or inflammation (1820). This feature may be compatible with differential or selective secretion of mediators without degranulation of MCs (66, 67). Unlike allergic reactions, MCs have been rarely reported to degranulate during inflammatory processes (66, 67). This activation in the nonallergic processes could be explained by selective secretion of mediators without degranulation through a process associated with their ultrastructural alterations (105108). This hypothesis is further supported by the observations that the CW NIR laser induces a selective set of chemokines without upregulating inflammatory cytokines, including TNF-α and IL-1β, and that the upregulation in the exposed skin tissue is dependent on MCs (Fig. 8). Reproducible control of microvascular permeability or lymphatic flow without widespread inflammation by CW NIR laser may offer a desirable approach for other medical purposes, including facilitation of drug delivery or the treatment of lymphedema. An optimal parameter of a CW NIR laser for such an application is yet to be found and awaits validation in relevant models in the future.

In summary, our results show that a CW NIR laser possesses a unique ability to selectively modulate innate responses in skin. These findings built upon mechanistic knowledge of the biological effect of the CW NIR laser would not only significantly contribute to optimization of the NIR laser vaccine adjuvant but also allow exploration of a novel use of this technology for the treatment of immune-related diseases.

We thank the Live Cell Imaging Facility, Karolinska Institutet, Sweden, the Swedish Research Council, the Centre for Innovative Medicine and the Jonasson Center at the Royal Institute of Technology, Sweden, and the Collaborative Research Resources, Keio University School of Medicine, Tokyo, Japan for the use of Imaris software, which provided the three-dimensional confocal image analysis service. We also thank Dr. Thomas J. Diefenbach (Ragon Institute of MGH, MIT, and Harvard) for expert technical assistance with confocal imaging, the Ragon Institute Imaging Core Facility for three-dimensional confocal imaging, the MGH Department of Pathology Flow and Image Cytometry Research Core for flow cytometry, and Madeline Penson and Don Sobell (all in the Vaccine and Immunotherapy Center at MGH) for excellent technical assistance and fruitful discussions.

This work was supported by funds from the National Institute of Allergy and Infectious Diseases/National Institutes of Health (NIH) under Award R01AI105131 (to S.K.), the Kanae Foundation for the Promotion of Medical Science (to Y.K.), the Mochida Memorial Foundation for Medical and Pharmaceutical Research (to Y.K.), the Uehara Memorial Foundation (to Y.K.), the Japan Foundation for Pediatric Research (to Y.K.), the Vaccine and Immunotherapy Center Innovation Fund (to S.K.), a Keio University Special Grant-in-Aid for Innovative Collaborative Research Projects (to K.T.), Keio University Research Grants for Global Initiative Research Projects (to K.T.), and the Japan Agency for Medical Research and Development Translational Research Network Program (to K.T.). The Live Cell Imaging Facility, Karolinska Institutet, Sweden, is supported by grants from the Knut and Alice Wallenberg Foundation. The Ragon Institute Imaging Core Facility is supported in part by the Harvard University Center for AIDS Research, an NIH-funded program (5 P30 AI060354-10). The Massachusetts General Hospital Department of Pathology Flow and Image Cytometry Research Core obtained support from the NIH Shared Instrumentation Program through Grants 1S10OD012027-01A1, 1S10OD016372-01, 1S10RR020936-01, and 1S10RR023440-01A1.

The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.

The online version of this article contains supplemental material.

Abbreviations used in this article:

Batf3−/−

Batf3-deficient

BM

bone marrow

BMMC

bone marrow–derived MC

Ccr7−/−

Ccr7-deficient

cDC

classical DC

CW

continuous-wave

DC

dendritic cell

dLN

draining lymph node

HAI

hemagglutination inhibition

ID

intradermal(ly)

IR

infrared

Lang+

langerin+

LN

lymph node

MC

mast cell

MGH

Massachusetts General Hospital

migDC

migratory DC

NAC

N-acetyl-l-cysteine

NIR

near-infrared

PW

pulsed-wave

ROS

reactive oxygen species

WT

wild-type.

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The authors have no financial conflicts of interest.

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