DYE SENSITIZED PHOTOACTIVE SURFACES

CLAIM OF PRIORITY

This application claims the benefit of prior U.S. Provisional Application No. 62/181,833 filed on June 19, 2015, which is incorporated by reference in its entirety.

TECHNICAL FIELD

This invention relates to photoactive surfaces.

BACKGROUND

Controlling and/or modifying the wettability of solid surfaces has attracted significant attraction due to a wide range of potential applications, including separation, microfluidic and lab-on-a-chip devices, controllable drug delivery, self-cleaning, antibacterial and antibiofouling. For these applications, it is particularly desirable to dynamically manipulate the behaviors of the contacting liquid on the surfaces, including the contact angles, droplet motion and effective area of the solid-liquid interface.

Photoactive materials such as titanium dioxide (Ti0 ₂ ) have attracted significant attention due to their ability to switch wettability upon irradiation of UV light. However, the large band gap limits their ability to absorb visible light or sunlight effectively. Although doping has been demonstrated as an effective solution to enhance the visible light-induced wettability switching of photoactive materials, typically it demands harsh conditions including high temperature, high pressure or toxic chemical environments, which limits versatility in fabrication process.

Stimuli-responsive surfaces that can switch wettability towards liquids upon the application of an external stimuli have been extensively fabricated. Typically such surfaces are reversibly switched from hydrophobicity (contact angle for water, # _water > 90°) or

superhydrophobocity (# _water > 150°) to hydrophilicity (0° < # _water <90°) or superhydrophlicity (# _water = 0°). In order to induce wettability switching, various external stimuli have been employed including pH, electric potential, chemical composition, solvent environment.

Among numerous stimuli-responsive materials, photoactive materials, mainly of Ti0 ₂ and ZnO, are widely studied due to their ability to switch wettability from hydrophobicity to hydrophilicity upon alternation of ultraviolet (UV) irradiation and storage in dark. Recently it was revealed that hierarchical roughness on the photoactive surfaces consisting of micro- and nanostructures cause amplification of contact angle changes. Such a unique photo-induced switchable wettability of photoactive materials has attracted wide scientific attention for both fundamental research and practical applications in antibacteria, antifogging, self-cleaning, biomedical, device, fluid transportation, liquid separation, anticorrosion, offset printing, site-selective functional printing, water condensation, as well as agricultural and environmental fields.

SUMMARY

A surface of a solid-liquid interface, the surface modified with a composition can include a matrix including a plurality of particles, where a surface of the particles is modified with a photosensitizer, where the wettability of the surface changes upon irradiation with light.

In certain embodiments, the plurality of particles can include a metal oxide.

In certain embodiments, the metal oxide can include Ti0 ₂ , ZnO, W0 ₃ , SrTi0 ₃ , Sn0 ₂ , V ₂ 0 ₅ , Ce0 ₂ , CuO, M0O3, Fe ₂ 0 ₃ , Cr ₂ 0 ₃ or ln ₂ 0 ₃ .

In certain embodiments, the particle can be a nanoparticle.

In certain embodiments, the matrix can include a multilayer including a first layer including a polyelectrolyte polymer and a second layer including the plurality of particles in contact with the first layer.

In certain embodiments, the polyelectrolyte polymer can include poly(allylamine hydrochloride).

In certain embodiments, the photosensitizer can include Chlorin.

In certain embodiments, the photosensitizer can include a Ruthenium (II) polypyridyl complex.

In certain embodiments, the photosensitizer can be N3, D149, Chlorin, Coumarin 343, Eosin Y, N719, N621, N179, N749, N945, Z907, Z907-Na, Z910, Z675, Z646, Z991, K8, K19, K20, K51, K60, K68, K73, K77, D5, D6, D102, D205, D29, D35, D37, DPP07, DPP13, DPP 14, DPP 15, DPP 17, Al, A2, A3, A597, ClOl, C102, C217, CYC-B 1, CYC-B3, CYC-B11, YS-1, YS-2, YS-3, YS-4, YS-5, YE05, Y123, YD2, YD2-0-C8, T18, T66, TFRS-1, TFRS-2, TFRS-3, HRS-1, SJW-E1, S8, JK-91, JK-92, LI17, HY2, DX1, SM371, SM315, RK1, KX-2569, MB18-N, LEG4, DEKl, B18, D45, D51, D77, C106, N820, N823, N886, K9, N712, NKK-2553, NKK-2554, TG6, JF419, MKA253, LI, MK245, HSQ4, or PI . In certain embodiments, the particles can be covalently bonded to the photosensitizer. In certain embodiments, the solid can include glass, fiber, stainless steel, inorganic materials or sand.

In certain embodiments, the solid can be coated with indium tin oxide.

An oil-water separation device can include a membrane includin the surface described above.

A method of separating oil from water in an oil-water mixture can include contacting a surface of an oil-water separation device with the oil-water mixture, the surface, the surface modified with a composition comprising a matrix including a plurality of particles, where a surface of the particles are modified with a photosensitizer, where the wettability of the surface changes upon irradiation with light and irradiating the surface with light.

In certain embodiments, the plurality of particles can include a metal oxide.

In certain embodiments, the metal oxide can include Ti0 ₂ , ZnO, W0 ₃ , SrTi0 ₃ , Sn0 ₂ , V ₂ 0 ₅ , Ce0 ₂ , CuO, M0O ₃ , Fe ₂ 0 ₃ , Cr ₂ 0 ₃ or ln ₂ 0 ₃ .

In certain embodiments, the photosensitizer can include Chlorin.

In certain embodiments, the photosensitizer can include a Ruthenium (II) polypyridyl complex.

A method of coating a surface of an oil-water separating device can include depositing a matrix including a plurality of particles on the surface, where a surface of the particles are modified with a photosensitizer, where the wettability of the surface changes upon irradiation with light.

In certain embodiments, the plurality of particles can include a metal oxide.

Other aspects, embodiments, and features will be apparent from the following description, the drawings, and the claims.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a schematic illustration of the deposition of a single bilayer of

(PAH/Ti0 ₂ ) during the Layer-by-layer deposition process.

FIG. 2 shows an scanning electron microscopy image of LBL Ti0 ₂ films.

FIG. 3 shows UV- Visible absorbance data of as-prepared dye-sensitized Ti0 ₂ surface and a neat Ti0 ₂ surface. FIG. 4 shows the XPS spectrum of dye-sensitized Ti0 ₂ surface.

FIG. 5 shows rates of decrease in contact angles for potassium iodide (KI) solutions at different concentrations as a function of visible light irradiation time.

FIGS. 6A-6C show wetting behaviors of liquids on an N3 dye-sensitized Ti0 ₂ surface. FIG. 6A shows visible light absorption data of an N3-sensitized Ti0 ₂ surface. Corresponding absorption data for an unsensitized neat Ti0 ₂ surface is also shown for comparison. Insets: (i) A scanning electron microscopic (SEM) image of a nanostructured Ti0 ₂ surface, (ii) A photograph of an N3 dye-sensitized Ti0 ₂ surface. FIG. 6B shows evolution in the measured equilibrium contact angles for potassium iodide (KI, 10 wt% in water), deionized (DI) water and potassium chloride (KCl, 10 wt% in water) on an N3 dye-sensitized Ti0 ₂ surface as a function of illumination time (Intensity = 145 mW/cm ² ). Inset: A schematic of in situ contact angle measurement of an aqueous droplet on a dye-sensitized Ti0 ₂ surface submerged in dodecane under visible-light illumination. FIG. 6C shows a plot of evolution in contact angles for multiple wetting cycles of KI and KCl droplets on an N3 dye-sensitized Ti0 ₂ surface under visible-light illumination.

FIGS. 7A-7C show the origin of the photo-induced wettability change of an N3 dye- sensitized Ti0 ₂ surface. FIG. 7A shows schematic illustration and relative energy state diagram of an N3 dye-sensitized Ti0 ₂ surface contacting either KI or KCl droplet. FIG. 7B shows a plot of measured voltages (symbols) and fit (lines; equation (1)) across the contacting liquids (KI or KCl) and the N3 dye-sensitized Ti0 ₂ surface under visible light illumination (Intensity = 145 mW/cm ² ). Inset: A zoomed-in image showing voltages immediately after the onset of visible- light illumination. FIG. 7C shows evolution in the measured contact angles for KI and KCl droplets on the electrically-grounded N3 dye-sensitized Ti0 ₂ surface. Inset: A schematic illustration of in situ contact angle measurement of a droplet on the electrically-grounded dye- sensitized Ti0 ₂ surface.

FIGS. 8A-8C show photo-induced wetting of contacting liquids on various dye-sensitized Ti0 ₂ surfaces. FIG. 8A shows an energy diagram of various dyes (N3, D149 and Chlorin) and 10 wt% ionic aqueous solutions (potassium thiosulfate (K ₂ S ₂ O ₃ ), KI, potassium bromide (KBr) and KCl). FIGS. 8B and 8C show evolution in the measured contact angles for 10 wt% ionic aqueous K ₂ S ₂ O ₃ , KI, KBr and KCl droplets on a D149 dye-sensitized Ti0 ₂ surface and on a Chlorin dye- sensitized Ti0 ₂ surface submerged in dodecane, respectively, as a function of illumination time. FIGS. 9A-9E show manipulating droplet motion on a Chlorin dye-sensitized Ti0 ₂ surface. FIG. 9A (i)-(iii) show a sequence of images showing visible-light-guided movement of a droplet of sodium chloride (NaCl, 10 wt% in water) on a patterned Chlorin dye-sensitized Ti0 ₂ surface. FIG. 9A (iv)-(vi) show sequential images captured from contact angle goniometry of anisotropic wetting of an NaCl droplet (9 μΐ) upon focused visible-light illumination. FIG. 9B shows sequential images of photo-induced coalescence of multiple NaCl droplets placed on a Chlorin dye-sensitized Ti0 ₂ surface submerged in dodecane. FIG. 9C shows a demulsifi cation apparatus with a 30:70 v:v Span80 (0.1 wt%)-stabilized brine (10 wt% NaCl in water)-in- dodecane emulsion above the membrane coated with Chlorin dye-sensitized Ti0 ₂ film. FIG. 9D shows brine droplets contacting the membrane surface coalesce upon visible light illumination resulting in spontaneous demulsification and gravity separation. FIG. 9E shows measured number size distribution of brine droplets for the feed emulsion.

FIG. 10 shows evolution in the measured contact angles for potassium iodide (KI) droplets with various ionic concentrations on an N3 dye-sensitized Ti0 ₂ surface as a function of illumination time.

FIG. 11 shows survey XPS spectra of an N3 dye-sensitized Ti0 ₂ surface before and after multiple wetting cycles under visible light illumination.

FIG. 12 shows evolution in the measured contact angles for a KI droplet (10 wt% in water) on an N3 dye-sensitized Ti0 ₂ surface upon intermittent visible light illumination.

FIG. 13 shows visible light absorption data of a D149 dye-sensitized Ti0 ₂ surface and a

Chlorin dye-sensitized Ti0 ₂ surface. Corresponding absorption data of an unsensitized neat Ti0 ₂ surface is also shown for comparison. Insets: (i) A photograph of a D149 dye-sensitized Ti0 ₂ surface and (ii) a photograph of a Chlorin dye-sensitized Ti0 ₂ surface.

FIG. 14A shows a plot of measured voltages across the contacting liquids (K ₂ S ₂ O ₃ and KBr) on the N3 dye-sensitized Ti0 ₂ surface under visible light illumination. FIGS. 14B and 14C plots of measured voltages across the contacting liquids (K ₂ S ₂ 0 ₃ , KI, KBr and KCl) on the D149 dye-sensitized Ti0 ₂ surface and Chlorin dye-sensitized Ti0 ₂ surface, respectively, under visible light illumination.

FIG. 15 shows evolution in the measured contact angles for potassium thiosulfate (K ₂ S ₂ O ₃ ) and potassium bromide (KBr) droplets on an N3 dye-sensitized Ti0 ₂ surface upon visible light illumination. DETAILED DESCRIPTION

Disclosed herein a method and a system to switch the wettability of photoactive materials to be responsive in the visible spectral regime using dye sensitization. A surface of a solid-liquid interface modified with a composition can include a matrix including a plurality of particles, where a surface of the particles is modified with a photosensitizer, where the wettability of the surface changes upon irradiation with light. The matrix can include a polymer or inorganic matrix. For example, the matrix can be a polymer film. In certain embodiments, the polymer film can be a multilayer film. The matrix can be deposited on a surface by a variety of different methods, for example, spray coating, dip coating, stamping, spin coating, ink jet printing, or layer-by-layer deposition. A photosensitizer can be selected to target a particular spectral range of light (e.g. UV or visible light). The particles can be micron-sized particles or nanoparticles. In certain embodiments, upon visible light irradiation, dye sensitized photoactive surfaces underwent hydrophobic to hydrophilic conversion in both in air and oil environments. In certain embodiments, a dye-sensitized Ti0 ₂ surface can also be engineered utilizing a facile dip-coating- based method to selectively switch its wettability state towards contacting liquids upon visible light illumination. This wettability change arises due to the electric potential difference established between the surface and the liquid upon incident illumination. A systematic study of the relationship between the energy levels of the dye and the contacting liquid reveals that the HOMO (highest occupied molecular orbital) energy level of the dye and the reduction potential of the liquid govern the ensuing wetting behaviors. Utilizing this photo-electro-wettability change of the dye-sensitized Ti0 ₂ surface, light-guided manipulation of liquid droplet motion was demonstrated along the surface. Further demulsification of surfactant-stabilized brine-in-oil emulsion is shown via interfacial coalescence of brine droplets under visible light illumination. Such surfaces thus offer a wide range of potential applications including optically driven, microfluidic devices with customizable wettability and continuous solar-driven self-cleaning and oil-water separation technologies.

Photo-responsive titania (Ti0 ₂ ) surfaces are of great interest due to their unique responsive wettability change upon ultraviolet (UV) light. See, Wang, R. et al. Light-induced amphiphilic surfaces. Nature 388, 431-432, doi:Doi 10.1038/41233 (1997), Wang, R. et al. Photogeneration of highly amphiphilic Ti02 surfaces. Adv Mater 10, 135-138, doi:Doi 10.1002/(Sici)1521-4095(199801)10:2<135: :Aid-Admal35>3.0.Co;2-M (1998), Watanabe, T. et al. Photocatalytic activity and photoinduced hydrophilicity of titanium dioxide coated glass. Thin Solid Films 351, 260-263, doi:Doi 10.1016/S0040-6090(99)00205-9 (1999), and Liu, K. S., Cao, M. Y., Fujishima, A. & Jiang, L. Bio-Inspired Titanium Dioxide Materials with Special

Wettability and Their Applications. Chem Rev 114, 10044-10094, doi: 10.1021/cr4006796

(2014), each of which is incorporated by reference in its entirety. However, their applications are often limited either by the inability to respond to the visible-light spectrum of natural sunlight or by the slow kinetics and special environment (i.e., storage in dark or heat) required to recover the original wettability state. See, Hashimoto, K., Irie, H. & Fujishima, A. Ti02 photocatalysis: A historical overview and future prospects. Jpn JAppl Phys 1 44, 8269-8285,

doi: 10.1143/JJAP.44.8269 (2005), Irie, H., Washizuka, S., Yoshino, N. & Hashimoto, K.

Visible-light induced hydrophilicity on nitrogen-substituted titanium dioxide films. Chem Commun, 1298-1299, doi: 10.1039/b302975a (2003), Wang, R., Sakai, N., Fujishima, A., Watanabe, T. & Hashimoto, K. Studies of surface wettability conversion on Ti02 single-crystal surfaces. J Phys Chem B 103, 2188-2194, doi:Doi 10.1021/Jp983386x (1999), and Sakai, N., Fujishima, A., Watanabe, T. & Hashimoto, K. Quantitative evaluation of the photoinduced hydrophilic conversion properties of Ti02 thin film surfaces by the reciprocal of contact angle. J Phys Chem B 107, 1028-1035, doi: 10.1021/jp022105p (2003), each of which is incorporated by reference in its entirety. The strategy of sensitizing Ti0 ₂ surfaces with dopants and visible light absorbing materials (e.g., organic dyes) has been utilized in photovoltaics to efficiently absorb solar radiation and convert it to electrical energy. See, Oregan, B. & Gratzel, M. A Low-Cost, High-Efficiency Solar-Cell Based on Dye- Sensitized Colloidal Tio2 Films. Nature 353, 737-740, doi:Doi 10.1038/353737a0 (1991), Bach, U. et al. Solid-state dye-sensitized mesoporous Ti02 solar cells with high photon-to-electron conversion efficiencies. Nature 395, 583-585 (1998), and Mathew, S. et al. Dye-sensitized solar cells with 13% efficiency achieved through the molecular engineering of porphyrin sensitizers. Nat Chem 6, 242-247, doi: 10.1038/NCHEM.1861 (2014), each of which is incorporated by reference in its entirety.

Photo-driven manipulation of liquid motion on a Ti0 ₂ surface is highly attractive because it would eliminate any need for either direct electrical contact with liquids or complex electronic circuitry. See, Monteleone, F. V. et al. Light-Controlled Directional Liquid Drop Movement on Ti02 Nanorods-Based Nanocomposite Photopatterns. Langmuir 26, 18557-18563, doi: 10.1021/lal026398 (2010), Kataoka, S. & Anderson, M. A. Capillary rise between two Ti02 thin-films: evaluating photo-activated wetting. Thin Solid Films 446, 232-237,

doi: 10.1016/j .tsf.2003.10.001 (2004), and Baigl, D. Photo-actuation of liquids for light-driven microfluidics: state of the art and perspectives. Lab Chip 12, 3637-3653,

doi: 10.1039/c21c40596b (2012), each of which is incorporated by reference in its entirety. A great deal of work has been devoted to elucidating the origin of the well-documented unique UV light-induced wettability change on Ti0 ₂ surfaces. See, Sun, R. D., Nakajima, A., Fujishima, A., Watanabe, T. & Hashimoto, K. Photoinduced surface wettability conversion of ZnO and Ti02 thin films. J Phys Chem B 105, 1984-1990, doi: 10.1021/jp002525j (2001), Sakai, N., Fujishima, A., Watanabe, T. & Hashimoto, K. Enhancement of the photoinduced hydrophilic conversion rate of Ti02 film electrode surfaces by anodic polarization. J Phys Chem B 105, 3023-3026, doi:Doi 10.1021/Jp003212r (2001), Ohtsu, N., Masahashi, N., Mizukoshi, Y. & Wagatsuma, K. Hydrocarbon Decomposition on a Hydrophilic Ti02 Surface by UV Irradiation: Spectral and Quantitative Analysis Using in-Situ XPS Technique. Langmuir 25, 11586-11591,

doi : 10.102 l/la901505m (2009), and Lee, K. et al. Superwetting of Ti02 by light-induced water- layer growth via delocalized surface electrons. P Natl Acad Sci USA 111, 5784-5789, doi: 10.1073/pnas. l319001111 (2014), each of which is incorporated by reference in its entirety. Although this continues to remain an active area of research, it is widely accepted that photo- generated electrons and holes change the surface chemistry so that it is favorable for contacting liquids to spread either by photocatalytic oxidation of surface adsorbed organic species or by the increase of hydroxyl species due to dissociative water adsorption. See, Zubkov, T. et al.

Ultraviolet light-induced hydrophilicity effect on Ti02(l 10)(lxl). Dominant role of the photooxidation of adsorbed hydrocarbons causing wetting by water droplets. J Phys Chem B 109, 15454-15462, doi: 10.1021/jp058101c (2005), White, J. M., Szanyi, J. & Henderson, M. A. The photon-driven hydrophilicity of titania: A model study using Ti02(l 10) and adsorbed trimethyl acetate. J Phys Chem B 107, 9029-9033, doi: 10.1021/jp0345046 (2003), Takeuchi, M., Sakamoto, K., Martra, G., Coluccia, S. & Anpo, M. Mechanism of photoinduced

superhydrophilicity on the Ti02 photocatalyst surface. J Phys Chem B 109, 15422-15428, doi: 10.1021/jp058075i (2005), and Wang, C. Y., Groenzin, H. & Shultz, M. J. Molecular species on nanoparticulate anatase Ti0 ₂ film detected by sum frequency generation: Trace hydrocarbons and hydroxyl groups. Langmuir 19, 7330-7334, doi: 10.1021/la0345542 (2003), each of which is incorporated by reference in its entirety.

Among various photoactive materials, titanium dioxide (Ti0 ₂ ) is one of the most widely studied one ever since Fujishima et al. first reported the ultraviolet (UV) light-induced superhydrophilicity of Ti0 ₂ surfaces. See, Wang, R. et al. Light-induced amphiphilic surfaces. Nature 388, 431-432, (1997), which is incorporated by reference in its entirety. In the report, Ti0 ₂ surface exhibited a water contact angle around 72° before UV irradiation. After UV irradiation, a water droplet spreads completely on the surface, resulting in 6 _w&te r = 0°. They also reported that wettability change of the surfaces was reversible by alternation of UV irradiation and long-term storage in dark. After this discovery, a great deal of works has been focused on developing light-induced wettability switches on photoactive materials.

A polyelectrolyte has a backbone with a plurality of charged functional groups attached to the backbone. A polyelectrolyte can be polycationic or polyanionic. A polycation has a backbone with a plurality of positively charged functional groups attached to the backbone, for example poly(allylamine hydrochloride) (PAH). A polyanion has a backbone with a plurality of negatively charged functional groups attached to the backbone, such as sulfonated polystyrene (SPS) or poly(acrylic acid) (PAA), or a salt thereof. Some polyelectrolytes can lose their charge (i.e., become electrically neutral) depending on conditions such as pH. Some polyelectrolytes, such as copolymers, can include both polycationic segments and polyanionic segments.

The polyelectrolyte solutions can be applied in a single step, in which a mixed polymer and particle solution is applied to a substrate in a controlled manner to achieve required nano- porosity inside the coating. This approach can provide low fabrication cost and high yield. Alternatively, the polyelectrolyte solutions can be applied in a multi-step method, in which polymer layers and nano-particle layers are deposited in an alternating fashion. The multi-step approach can be more efficient for manufacturing with a spray method than an immersion-based method, because spray deposition does not require a rinse between immersions. With either method, the coating parameters such as material composition, solution concentration, solvent type, and so on, can be optimized to efficiently produce a coating with desired properties.

Layer-by-Layer (LbL) assembly technique can be used to form a multilayer to enable the uniform coating thickness with conformal thin film coatings with molecular level control over film thickness and chemistry. See, Wu, Z.; Lee, D.; Rubner, M. F.; Cohen, R. E., Small 2007, 3, 1445, Decher, G., Science 1997, 277, 1232, and Nuraje, N.; Asmatulu, R.; Cohen, R. E.; Rubner, M. F., Langmuir 2011, 27, 782, each of which is incorporated by reference in its entirety. Using oppositely charged polymeric solution and nanoparticle solutions, a conformal coating that is essential to reduce scattering or haze can be obtained. See, Lee, D.; Gemici, Z.; Rubner, M. F.; Cohen, R. E., Langmuir 2007, 23, 8833, and Shimomura, H.; Gemici, Z.; Cohen, R. E.; Rubner, M. F., Applied Materials and Interfaces 2010, 2, 813, each of which is incorporated by reference in its entirety. This coating method has benefits of extremely precise control of film thicknesses and uniformity even on curved surfaces, compared to other typical coating methods such as dip- coating, spray-coating, and solvent-casting.

One method of depositing the poly electrolytes is to contact the substrate with an aqueous solution of polyelectrolyte at an appropriate pH. The pH can be chosen such that the

polyelectrolyte is partially or weakly charged, or such that the polyelectrolyte is substantially completely or strongly charged. See, for example, G. Decher, Science 1997, 277, 1232;

Mendelsohn et al., Langmuir 2000, 16, 5017; Fery et al., Langmuir 2001, 17, 3779; Shiratori et al., Macromolecules 2000, 33, 4213; and U.S. Patent Application No. 10/393,360, each of which is incorporated by reference in its entirety. The multilayer can be described by the number of bilayers it includes, a bilayer resulting from the sequential application of oppositely charged polyelectrolytes.

A coating of this type can be applied to any surface amenable to the water based layer-by- layer (LbL) adsorption process used to construct these polyelectrolyte multilayers. Because the water based process can deposit polyelectrolytes wherever the aqueous solution contacts a surface, even the inside surfaces of objects having a complex topology can be coated. In general, a polyelectrolyte can be applied to a surface by any method amenable to applying an aqueous solution to a surface, such as dipping or spraying.

Other modifications of a deposited polyelectrolyte multilayer are possible. For example, a nonporous polyelectrolyte multilayer can form porous thin film structures induced by a simple acidic, aqueous process. Tuning of this pore forming process, for example, by the manipulation of such parameters as salt content (ionic strength), temperature, or surfactant chemistry, can lead to the creation of micropores, nanopores, or a combination thereof. A nanopore has a diameter of less than 150 nm, for example, between 1 and 120 nm or between 10 and 100 nm. A nanopore can have diameter of less than 100 nm. A micropore has a diameter of greater than 150 nm, typically greater than 200 nm. Selection of pore forming conditions can provide control over the porosity of the coating. For example, the coating can be a nanoporous coating, substantially free of micropores. Alternatively, the coating can be a microporous coating having an average pore diameters of greater than 200 nm, such as 250 nm, 500 nm, 1 micron, 2 microns, 5 microns, 10 microns, or larger.

Desired chemistries can be included in the polyelectrolyte multilayers. The chemistry can be added during manufacture of the multilayer, or after manufacture. For example, antibacterial chemistries (such as silver nanoparticles or quaternary ammonium salts) can be included in the multilayer during manufacture. The resulting multilayer can then have desired properties (such as antibacterial properties) arising from the incorporated chemistry. In some circumstances, the chemistry can be controllably released from the multilayer.

Surfaces having a nanotexture can exhibit extreme wetting properties. A nanotexture refers to surface features, such as ridges, valleys, or pores, having nanometer (i.e., typically less than 1 micrometer) dimensions. In some cases, the features will have an average or rms dimension on the nanometer scale, even though some individual features may exceed 1 micrometer in size. The nanotexture can be a 3D network of interconnected pores. Depending on the structure and chemical composition of a surface, the surface can be hydrophilic, hydrophobic, or at the extremes, superhydrophilic or superhydrophobic. One method to create the desired texture is with a polyelectrolyte multilayer. Polyelectrolyte multilayers can also confer desirable optical properties to surfaces, such as anti -reflectivity, or reflectivity in a desired range of wavelengths. See, for example, U.S. Patent Application Publication No. 2003/0215626, and U.S. Patent Application No. 10/912,540, each of which is incorporated by reference in its entirety.

Hydrophilic surfaces attract water; hydrophobic surfaces repel water. In general, a non- hydrophobic surface can be made hydrophobic by coating the surface with a hydrophobic material. The hydrophobicity of a surface can be measured, for example, by determining the contact angle of a drop of water on the surface. The contact angle can be a static contact angle or dynamic contact angle. A dynamic contact angle measurement can include determining an advancing contact angle or a receding contact angle, or both. A hydrophobic surface having a small difference between advancing and receding contact angles (i.e., low contact angle hysteresis) can be desirable. Water droplets travel across a surface having low contact angle hysteresis more readily than across a surface having a high contact angle hysteresis. A surface can be superhydrophilic. A superhydrophilic surface is completely and instantaneously wet by water, i.e., exhibiting water droplet advancing contact angles of less than 5 degrees within 0.5 seconds or less upon contact with water. See, for example, Bico, J. et al., Europhys. Lett. 2001, 55, 214-220, which is incorporated by reference in its entirety. At the other extreme, a surface can be superhydrophobic, i.e. exhibiting a water droplet advancing contact angles of 150° or higher. The lotus leaf is an example of a superhydrophobic surface (See Neinhuis, C; Barthlott, W. Ann. Bot. 1997, 79, 677; and Barthlott, W.; Neinhuis, C. Planta 1997, 202, 1, each of which is incorporated by reference in its entirety). The lotus leaf also exhibits very low contact angle hysteresis: the receding contact angle is within 5° of the advancing contact angle (See, for example, Chen, W.; et al. Langmuir 1999, 75, 3395; and Oner, D.;

McCarthy, T. J. Langmuir 2000, 16, 7777, each of which is incorporated by reference in its entirety).

Textured surfaces can promote superhydrophilic behavior. Early theoretical work by

Wenzel and Cassie-Baxter and more recent studies by Quere and coworkers suggest that it is possible to significantly enhance the wetting of a surface with water by introducing roughness at the right length scale. See, for example, Wenzel, R. N. J. Phys. Colloid Chem. 1949, 53, 1466;

Wenzel, R. N. Ind. Eng. Chem. 1936, 28, 988; Cassie, A. B. D.; Baxter, S. Trans. Faraday Soc.

1944, 40, 546; Bico, J.; et al., D. Europhysics Letters 2001, 55, (2), 214-220; and Bico, J.; et al.

Europhysics Letters 1999, 47, (6), 743-744, each of which is incorporated by reference in its entirety. Building on this work, both lithographically textured surfaces and microporous surfaces can be rendered superhydrophilic. See, e.g., McHale, G.; Shirtcliffe, N. J.; Aqil, S.; Perry, C. C;

Newton, M. I. Physical Review Letters 2004, 93, (3), which is incorporated by reference in its entirety. The intriguing possibility of switching between a superhydrophobic and

superhydrophilic state has also been demonstrated with some of these surface structures. See, for example, Sun, T. L.; et al. Angewandte Chemie-International Edition 2004, 43, (3), 357-360; and

Gao, Y. F.; et al. Langmuir 2004, 20, (8), 3188-3194, each of which is incorporated by reference in its entirety.

UV light-induced switching wettability of photoactive materials

Although the mechanism for light-induced switching wettability of photoactive materials is not fully understood, the prerequisite is the excitation of photoactive materials by light with energy equal to or larger than the band gap. This results in the generation of charge carriers (i.e., electrons and holes) that change the reactivity of the material. Typically the band gap of photoactive materials is large (Ti0 ₂ ~ 3.2 eV and ZnO - 3.3 eV). Thus in order to excite photoactive materials, irradiation of light with high energy (UV light, λ < 390 nm) is required.

1. Ti0 ₂

A number of methods have been used to create Ti0 ₂ surfaces including the sol-gel method, aerosol-deposition, hydrothermal method, spray pyrolysis, anodic oxidation and templating. See, Kontos, A. I, Kontos, A. G., Tsoukleris, D. S., Vlachos, G. D. & Falaras, P. Superhydrophilicity and photocatalytic property of nanocrystalline titania sol-gel films. Thin Solid Films 515, 7370-7375, doi:Doi 10.1016/J.Tsf2007.02.082 (2007), Park, J. J. et al.

Superhydrophilic Transparent Titania Films by Supersonic Aerosol Deposition. J Am Ceram Soc 96, 1596-1601, doi:Doi 10.1111/Jace.12164 (2013), Miyauchi, M. & Tokudome, H. Superhydrophilic and transparent thin films of Ti02 nanotube arrays by a hydrothermal reaction. J Mater Chem 17, 2095-2100, doi:Doi 10.1039/B700387k (2007), Sun, R. D., Nakajima, A., Fujishima, A., Watanabe, T. & Hashimoto, K. Photoinduced surface wettability conversion of ZnO and Ti02 thin films. J Phys Chem B 105, 1984-1990, doi:Doi 10.1021/Jp002525j (2001), Li, Y. et al. Superhydrophobicity of 2D ZnO ordered pore arrays formed by solution-dipping template method. J Colloid Inter/ Sci 287, 634-639, doi:Doi 10.1016/J.Jcis.2005.02.010 (2005), and Kamegawa, T., Suzuki, N. & Yamashita, H. Design of macroporous Ti02 thin film photocataly sts with enhanced photofunctional properties. Energ Environ Sci 4, 1411-1416, doi:Doi 10.1039/C0ee00389a (2011), each of which is incorporated by reference in its entirety. Ti0 ₂ surfaces prepared by such methods alter the wettability to superhydrophilicity upon irradiation of UV light. Due to intrinsic hydrophilicity of Ti0 ₂ , water contact angle change under UV light may not be significant. In order to amplify wettability switching, textured Ti0 ₂ surfaces have been developed. Rough Ti0 ₂ surfaces contain nanotube arrays, inverse opal three- dimensional structures, nanorod arrays and nanopores. See, Kamegawa, T., Suzuki, N. &

Yamashita, H. Design of macroporous Ti02 thin film photocataly sts with enhanced

photofunctional properties. Energ Environ Sci 4, 1411-1416, doi:Doi 10.1039/C0ee00389a (2011), Gu, Z. Z., Fujishima, A. & Sato, O. Biomimetic titanium dioxide film with structural color and extremely stable hydrophilicity. Appl Phys Lett 85, 5067-5069, doi:Doi

10.1063/1.1825052 (2004), and Feng, X. J., Zhai, J. & Jiang, L. The fabrication and switchable superhydrophobicity of Ti02 nanorod films. Angew Chem Int Edit 44, 5115-5118, doi :Doi 10.1002/ Anie.200501337 (2005), each of which is incorporated by reference in its entirety. Such surfaces exhibited hydrophobicity or even superhydrophobicity before UV irradiation and became superhydrophilic after UV irradiation.

2. T1O ₂ modified with hydrophobic coatings

Ti0 ₂ surfaces have been modified with low surface energy materials (i.e., hydrophobic coatings) including fluoroalkylsilane, octadecylsilane, poly(methyl methacrylate) (PMMA) and styrene-co-acrylate oligomers. See, Nakajima, A. et al. Transparent superhydrophobic thin films with self-cleaning properties. Langmuir 16, 7044-7047, doi:Doi 10.1021/La000155k (2000), Li, J. S. S., Ueda, E., Nallapaneni, A., Li, L. X. X. & Levkin, P. A. Printable Superhydrophilic- Superhydrophobic Micropatterns Based on Supported Lipid Layers. Langmuir 28, 8286-8291, doi:Doi 10.1021/La3010932 (2012), Zhang, X. T. et al. Self-cleaning particle coating with antireflection properties. ChemMater 17, 696-700, doi:Doi 10.1021/Cm0484201 (2005), Yang, M. J., Di, Z. F. & Lee, J. K. Facile control of surface wettability in Ti02/poly(methyl

methacrylate) composite films. J Colloid Inter j Sci 368, 603-607, doi:Doi

10.1016/J.Jcis.2011.11.037 (2012), and Ding, X. F., Zhou, S. X., Wu, L. M., Gu, G. X. & Yang, J. T. Formation of supra-amphiphilic self-cleaning surface through sun-illumination of titania- based nanocomposite coatings. Surf Coat Tech 205, 2554-2561, doi:Doi

10.1016/J.Surfcoat.2010.10.002 (2010), each of which is incorporated by reference in its entirety. Surface modifications lead to hydrophobicity by lowering solid surface energy before UV irradiation. After UV irradiation, the surfaces became superhydrophilic with $y _at er = 0°. This is due to the formation of microcracks and decomposition of hydrophobic coatings.

3. T1O ₂ coupling/doping with other materials

Coupling and/or doping with other semiconductors and/or metals are another strategy to enhance wettability switching of Ti0 ₂ . Various materials used for this purpose including Si0 ₂ , W0 ₃ , Sn0 ₂ , A1 ₂ 0 ₃ and SrTi0 ₃ . See, Zhang, X. T., Fujishima, A., Jin, M., Emeline, A. V. & Murakami, T. Double-layered Ti02-Si02 nanostructured films with self-cleaning and

antireflective properties. J Phys Chem B 110, 25142-25148, doi:Doi 10.1021/Jp064442u (2006), Emeline, A. V., Rudakova, A. V., Sakai, M., Murakami, T. & Fujishima, A. Factors Affecting UV-Induced Superhydrophilic Conversion of a Ti02 Surface. J Phys Chem C 111, 12086-12092, doi:Doi 10.1021/Jp400421v (2013), Miyauchi, M., Nakajima, A., Hashimoto, K. & Watanabe, T. A highly hydrophilic thin film under 1 mu W/cm(2) UV illumination. Adv Mater 12, 1923-1927, doi:Doi 10.1002/1521-4095(200012)12:24<1923 : :Aid-Admal923>3.0.Co;2-# (2000), Wu, Z., Lee, D., Rubner, M. F. & Cohen, R. E. Structural color in porous, superhydrophilic, and self- cleaning Si02/Ti02 Bragg stacks. Small 3, 1445-1451, doi:Doi 10.1002/Smll.200700084 (2007), Hattori, A., Tokihisa, Y., Tada, H. & Ito, S. Acceleration of oxidations and retardation of reductions in photocatalysis of a Ti02/Sn02 bilayer-type catalyst. J Electrochem Soc 147, 2279- 2283, doi:Doi 10.1149/1.1393521 (2000), Tadanaga, K., Morinaga, J., Matsuda, A. & Minami, T. Superhydrophobic-superhydrophilic micropatterning on flowerlike alumina coating film by the sol-gel method. Chem Mater 12, 590-+, doi:Doi 10.1021/Cm990643h (2000), and Miyauchi, M., Nakajima, A., Fujishima, A., Hashimoto, K. & Watanabe, T. Photoinduced surface reactions on Ti02 and SrTi03 films: Photocatalytic oxidation and photoinduced hydrophilicity. Chem Mater 12, 3-5, doi:Doi 10.1021/Cm990556p (2000), each of which is incorporated by reference in its entirety. Coupled or doped Ti0 ₂ surfaces exhibited wettability switching under very weak UV illumination (< 1 μW/cm ² ), enhanced photocatlaysis and self-cleaning ability.

4. Various photoactive materials

In addition to Ti0 ₂ , a wide range of photoactive materials has been utilized. ZnO is extensively studied due to its superior photocatalytic ability and switchable wettability under UV irradiation. See, Liu, H., Feng, L., Zhai, J., Jiang, L. & Zhu, D. B. Reversible wettability of a chemical vapor deposition prepared ZnO film between superhydrophobicity and

superhydrophilicity. Langmuir 20, 5659-5661, doi:Doi 10.1021/La036280o (2004), Feng, X. J. et al. Reversible super-hydrophobicity to super-hydrophilicity transition of aligned ZnO nanorod films. J Am Chem Soc 126, 62-63, doi:Doi 10.1021/Ja038636o (2004), Huang, L. et al. Stable superhydrophobic surface via carbon nanotubes coated with a ZnO thin film. JPhys Chem B 109, 7746-7748, doi:Doi 10.1021/Jp046549s (2005), and Zhang, X. T., Sato, O. & Fujishima, A. Water ultrarepellency induced by nanocolumnar ZnO surface. Langmuir 20, 6065-6067, doi:Doi 10.1021/La049471f (2004), each of which is incorporated by reference in its entirety. Miyauchi et al. thoroughly studied wettability switching and photocatalysis of arrays of photoactive materials. See, Miyauchi, M., Nakajima, A., Watanabe, T. & Hashimoto, K. Photocatalysis and photoinduced hydrophilicity of various metal oxide thin films. Chem Mater 14, 2812-2816, doi:Doi 10.1021/Cm020076p (2002), which is incorporated by reference in its entirety. They reported that Ti0 ₂ , ZnO, Sn0 ₂ , W0 ₃ , V ₂ 0 ₅ exhibited superhydrophilicity whereas CeO, CuO, M0O ₃ , Fe ₂ C"3, Cr ₂ 0 ₃ and ln ₂ 0 ₃ did not alter wettability upon UV light irradiation.

Visible light-induced switching wettability of photoactive materials

The large band gap photoactive materials require an excitation light wavelength range shorter than 400 nm (such as UV light), which limits its ability to absorb visible light or sunlight effectively. Tuning the bang gap response to the visible region is indispensable to enhance efficiency of wettability change as well as photocatalysis by utilizing a large fraction of solar spectrum.

Doping has been demonstrated as an effective solution to enhance the visible light- induced wettability switching of photoactive materials. Therefore, various materials have been employed in doping to lower the band gap. Among various dopants, nitrogen (N) is the most widely used material in doping techniques because nitrogen can be readily introduced in the structures due to its compatible atomic size with oxygen and high stability. See, Irie, H.,

Washizuka, S., Yoshino, N. & Hashimoto, K. Visible-light induced hydrophilicity on nitrogen- substituted titanium dioxide films. Chem Commun, 1298-1299, doi:Doi 10.1039/B302975a (2003), and Asahi, R., Morikawa, T., Ohwaki, T., Aoki, K. & Taga, Y. Visible-light

photocatalysis in nitrogen-doped titanium oxides. Science 293, 269-271, doi:Doi

10.1126/Science.1061051 (2001), each of which is incorporated by reference in its entirety. Nitrogen doping has been achieved utilizing various techniques including sol-gel method, metalorganic chemical vapor deposition, anodizing, hydrothermal method and ultrasonic spray pyrolysis. See, Dunnill, C. W. et al. Visible light photocatalysts-N-doped Ti02 by sol-gel, enhanced with surface bound silver nanoparticle islands. J Mater Chem 21, 11854-11861, doi:Doi 10.1039/Cljml l557j (2011), Borras, A. et al. Effect of visible and UV illumination on the water contact angle of Ti02 thin films with incorporated nitrogen. JPhys Chem C 111, 1801- 1808, doi:Doi 10.1021/Jp065392w (2007), Antony, R. P., Mathews, T., Dash, S. & Tyagi, A. K. Kinetics and Physicochemical Process of Photoinduced Hydrophobic <-> Superhydrophilic Switching of Pristine and N-doped Ti02 Nanotube Arrays. JPhys Chem C 117, 6851-6860, doi:Doi 10.1021/Jp400718t (2013), Wang, J. W., Mao, B. D., Gole, J. L. & Burda, C. Visible- light-driven reversible and switchable hydrophobic to hydrophilic nitrogen-doped titania surfaces: correlation with photocatalysis. Nanoscale 2, 2257-2261, doi:Doi 10.1039/C0nr00313a (2010), and Sahoo, M. et al. Physico-chemical Processes and Kinetics of Sunlight-Induced Hydrophobic <-> Superhydrophilic Switching of Transparent N-Doped Ti02 Thin Films. Acs Appl Mater Inter 5, 3967-3974, doi:Doi 10.1021/Am400785x (2013), each of which is incorporated by reference in its entirety. Similar to nitrogen, doping of carbon (C) and sulfur (S) has also been found to be effective in altering wettability of photoactive materials under visible light irradiation. See, Zhang, L. W., Dillert, R., Bahnemann, D. & Vormoor, M. Photo-induced hydrophilicity and self-cleaning: models and reality. Energ Environ Sci 5, 7491-7507, doi:Doi 10.1039/C2ee03390a (2012), Sakai, Y. W., Obata, K., Hashimoto, K. & Irie, H. Enhancement of visible light-induced hydrophilicity on nitrogen and sulfur-codoped Ti02 thin films. Vacuum 83, 683-687, doi:Doi 10.1016/J.Vacuum.2008.04.022 (2008), and Dunnill, C. W. et al. White light induced photocatalytic activity of sulfur-doped Ti02 thin films and their potential for antibacterial application. J Mater Chem 19, 8747-8754, doi:Doi 10.1039/B913793a (2009), each of which is incorporated by reference in its entirety. Codoping of two materials such as nitrogen and fluorine is another approach to achieve fast switching wettability and controlling absorption of visible light. See, Li, Q. & Shang, J. K. Composite Photocatalyst of Nitrogen and Fluorine Codoped Titanium Oxide Nanotube Arrays with Dispersed Palladium Oxide Nanoparticles for Enhanced Visible Light Photocatalytic Performance. Environ Sci Technol 44, 3493-3499, doi:Doi 10.1021/Es903928n (2010), and Kontos, A. G. et al. Visible light induced wetting of nanostructured N-F co-doped titania films. Photoch Photobio Sci 10, 350-354, doi:Doi

10.1039/C0pp00159g (2011), each of which is incorporated by reference in its entirety. In order to shift the absorption of photoactive materials into the visible spectral region, doping of transition metal such as vanadium (V) and Y ₂ 0 ₃ has also been employed. See, Mokhtarimehr, M., Pakshir, M., Eshaghi, A. & Shariat, M. H. Super-hydrophilic property of vanadium doped Ti02-Si02 sol-gel derived thin film. Thin Solid Films 532, 123-126, doi:Doi

10.1016/J.Tsf.2012.12.104 (2013), and Zhang, X. C, Yang, H. M. & Tang, A. D. Optical,

Electrochemical and Hydrophilic Properties of Y203 Doped Ti02 Nanocomposite Films. JPhys Chem B ill, 16271-16279, doi:Doi 10.1021/Jp806820p (2008), each of which is incorporated by reference in its entirety. Using dyes (photosensitizers) to sensitize surfaces Doping with various materials mentioned above has been successfully employed in altering wettability of photoactive materials under visible light. However, such doping techniques typically demand harsh conditions including high temperature, high pressure or toxic chemical environments, which limits versatility in the fabrication process. Further since visible light directly excites the doped photoactive materials, this may result in phtocatalytic

decomposition of any organic deposits. Such visible light-induced photocatalysis of photoactive materials may hinder further surface modification processes that are needed for practical applications.

Dye sensitization has been used to improve spectral characteristics particularly for photovoltaics, so called dye-sensitized solar cells (DSSCs). DSSCs are based on the sensitization of mesoporous, nanocrystalline metal oxide films such as Ti0 ₂ to visible light by the adsorption of organic molecular dyes. In contrast to doping, the dye gets excited rather than the Ti0 ₂ under visible light irradiation into appropriate singlet or triplet states. The dyes are subsequently converted to cationic radicals after the dye injects electrons to the conduction band of the Ti0 ₂ . Thus it is usually referred to as an indirect excitation process that results in slow or negligible degradation of adsorbed dyes. Although dye sensitization has been widely used in solar applications to improve spectral characteristics, there is no prior art on using dye sensitized photoactive materials to control wettability of liquids. Design considerations for photoactive materials sensitized with photosensitizers (dyes)

1. Photoactive materials

In the present disclosure, Ti0 ₂ was chosen as a photoactive material due to its

nontoxicity, water insolubility, cheap availability and stability against chemical environments. Further, Ti0 ₂ surfaces can be supported on various substrates such as glass, fibers, stainless steel, inorganic materials and sand. However, any of a wide range of materials can be used in fabrication of photoactive surfaces provided it has a suitable flat band potential that can induce photochemical reactions without biased potential. Non-limiting examples include Ti0 ₂ , ZnO, W0 ₃ , SrTi0 ₃ , Sn0 ₂ , V ₂ 0 ₅ , Ce0 ₂ , CuO, M0O3, Fe ₂ 0 ₃ , Cr ₂ 0 ₃ , ln ₂ 0 ₃ .

2. Methods for fabrication of photoactive surfaces

Various fabrication methods can be utilized to develop photoactive surfaces. Non- limiting examples include sol-gel method, sol method, hydrothermal method, chemical vapor deposition, atomic layer deposition, electro-deposition, direct oxidation, magnetron sputtering, spincoating, dipcoating.

3. Selection of photosensitizers (dyes)

A large number of photosensitizers have been synthesized from various research groups and some of them are commercially available. For an effective sensitization process, it is important to select proper photosensitizers by considering following factors.

a) Adsorption: Liquids contacting the photoactive surfaces must not desorb the photosensitizers from the surface. In the sensitization process, photosensitizer molecules anchor on the surface via the -COOH groups, most likely in the form of carboxylate. However such anchoring was found to be insufficient to resist high shear forces as well as agitation or sonication. Thus it is desirable for photosensitizers to be strongly bonded to the surfaces.

b) Stability: Photoactive material can act as a photocatalyst for the light-induced photochemical reactions. Since photocatalytic reactions proceed in air-saturated and water-rich environment, the stability of the chosen photosensitizers is vital under these conditions.

In the present disclosure, N3 (cis-Bis(isothiocyanato) bis(2,2'-bipyridyl-4,4'-dicarboxylato) ruthenium(II)) as a photosensitizer was initially chosen due to its favorable photoelectrochemical properties and high stability in the oxidized state, thus making practical applications feasible. A wide range of photosensitizers can be used in the fabrication of photosensitized surfaces. Non- limiting examples are (by code name) N3, D149, Chlorin, Coumarin 343, Eosin Y, N719, N621, N179, N749, N945, Z907, Z907-Na, Z910, Z675, Z646, Z991, K8, K19, K20, K51, K60, K68, K73, K77, D5, D6, D102, D205, D29, D35, D37, DPP07, DPP13, DPP 14, DPP 15, DPP 17, Al, A2, A3, A597, ClOl, C102, C217, CYC-Bl, CYC-B3, CYC-B l l, YS-1, YS-2, YS-3, YS-4, YS- 5, YE05, Y123, YD2, YD2-0-C8, T18, T66, TFRS-1, TFRS-2, TFRS-3, HRS-1, SJW-E1, S8, JK-91, JK-92, LI17, HY2, DX1, SM371, SM315, RK1, NKX-2569, MB18-N, LEG4, DEK1, B18, D45, D51, D77, C106, N820, N823, N886, K9, N712, NKK-2553, NKK-2554, TG6,

JF419, MKA253, LI, MK245, HSQ4, and PI . See table below for a full chemical name for each code name when it is known. Dyes with only codes names are known are also listed in the table. See also, Yuancheng Qin and Qiang Peng, "Ruthenium Sensitizers and Their Applications in Dye-Sensitized Solar Cells/'International Journal of Photoenergy, vol. 2012, Article ID 291579, 21 pages, 2012, Jun-Ho Yum et al., "Blue-Coloured Highly Efficient Dye-Sensitized Solar Cells by Implementing the Diketopyrrolopyrrole Chromophore," Scientific Reports, 3, Article number 2446, 2013, S. Shalini et al., "Status and outlook of sensitizers/dyes used in dye sensitized solar cells (DSSC): a review," International Journal of Energy Research, 2016, and Giuseppe Calogero et al., "Vegetable-based dye-sensitized solar cells," Chem. Soc. Rev. 2015, 44, 3244, each of which is incorporated by reference in its entirety.

D102 (5-{ 1,2,3, 3a,4,8b-hexahydro-4-[4-(2,2-diphenylvinyl)phenyl]-cyclopeant a[b]indole-7- ylmethylene } -4-oxo-2-thioxo-thiazolidin-3 -yl)acitic acid

D35 (E)-3 5 4 bis(2^4'-dibutoxy-[l,r-biphenyl]-4-yl)amino)phenyl)thiophen- 2-yl)-2- cyanoacrylic acid

DPP 13 (E)-3-(5-(4-(4-(5-(4-(bis(4-(hexyloxy)phenyl)amino)phenyl)th iophen-2-yl)-2,5-bis(2- emylhexyl)-3,6-dioxo-2,3,5,6-tetrahydropyrrolo[3,4-c]pyrrol- l-yl)phenyl)furan-2-yl)- 2-cyanoacrylic acid

Al [Ru(tctpy)(tfpd)(NCS)]; tctpy = 4,4^4''-tricarboxy-2,2':;6',2''-terpyridine; tfpd =1, 1,1- trifluoropentane-2,4-dione

A2 [Ru(tctpy)(tfdd)(NCS)] ; tctpy = 4,4',4"-tricarboxy-2,2':;6',2"^yridine; tfdd =

1, 1, l-trifluorodecane-2,4-dione

A3 [Ru(tctpy)(tfid)(NCS)] ;tctpy = 4,4^4''-tricarboxy-2,2':;6',2''-terpyridine; tfid =1, 1, 1- trifluoroicosane-2,4-dione

ClOl Ruthenate(2-), [[2,2'-bipyridine]-4,4'-dicarboxylato(2-)-KN ¹ ,KN ¹ '][4,4'-bis(5-hexyl-2- thienyl)-2,2'-bipyridine-KN ¹ ,KN ¹ ']bis(thiocyanato-KN)-, hydrogen (1 :2), (OC-6-32)-

CYC-B3 (cis-di(thiocyanato)-4,4'- di(octylthienyl)-2,2'-bipyridine-4,4'-dicarboxylate-2,2'- bipyridine ruthenium(II))

CYC-B 11 Ruthenate(2-), [[2,2'-bipyridine]-4,4'-dicarboxylato(2-)-KN ^; ,KN ^; ] [4,4'-bis[5 '- (hexylthio) [2,2 ^' -bithiophen] -5 -yl] -2,2 ^' -bipyridine-KN ^; ,KN ^; ]bis(thiocyanato-KN)-, hydrogen (1 :2), (OC-6-32)-

YS-1 [Ru{(dcbpy)(dfbpy)(NCS) ₂ }]; dcbpy = 4,49-dicarboxy-2,29-bipyridyl; dfbpy=4,4'- Bis(9,9-diethyl-9H fluoren-2-yl)-2,2'-bipyridine

YS-2 Ru[(dcbpy)(sdfbpy)(NCS)2]; dcbpy = 4,49-dicarboxy-2,29-bipyridyl; stdfbpy = 4,4'- Bis(9,9-dihexyl-7-(5-hexylthiophen-2-yl)-9H-fluoren-2-yl)-2, 2'-bipyridine

YS-3 Ru[(dcbpy)(stdfbpy)(NCS)2]; dcbpy = 4,49-dicarboxy-2,29-bipyridyl; stdfbpy=4,4'- Bis(9,9-dihexyl-7-(5-hexylthiophen-2-yl)-9H-fluoren-2-yl)-2, 2'-bipyridine.

YS-4 Ru[(dcbpy)(dcabpy)(NCS)2]; dcbpy = 4,49-dicarboxy-2,29-bipyridyl; dcabpy=4,4'- Bis(9-hexyl-9H-carbazol-2-yl)-2,2'-bipyridine

YS-5 Ru[(dcbpy)(dtpbpy)(NCS)21; dcbpy = 4,49-dicarboxy-2,29-bipyridyl;

Y123 3 - { 6- {4- [bis(2 ' ,4 ' -dihexyloxybiphenyl-4-yl)amino-]phenyl} -4,4-dihexyl-cyclopenta- [2, l-b:3,4-b']dithiphene-2-yl}-2-cyanoacrylic acid

YD2 Zinc(II) 5,15-Bis(3,5-di-tert-butylphenyl)-10-(bis(4-hexylphenyl)amin o)-20- (4-carboxyphenylethynyl)po hyrin

YD2-0-C8 5, 15-bis(2,6-dioctoxyphenyl)-10-(bis(4-hexylphenyl)amino-20-4- carboxyphenyl

ethynyl)po hyrinato] zinc(II)

T18 (cis-bis(thiocyanato)(2,20 -bipyridyl-4,40 -dicarboxylato){4,40 -bis(l,3-dithian-2- ylidenemethyl)-2,20 -bipyridine} ruthenium (II) mono-tetrabutylammonium salt

T66 [Ru(6'-phenyl-4'-tliiopheri-2~yl-[2,2']bipyndiiiyl~4-carboxy lic acid)(4,4',4"~tricarboxy- 2,2':6',2 ^f '-terpyridine) |Cl

HPvS-1 2-thiophen-2-yl-vinyl-conjugated ruthenium complex, cis-Ru(dhtbpy)(dcbpy)(NCS)2

[dhtbpy = 4,49-di(hexylthienylvinyl)-2,29-bipyridyl; dcbpy = 4,49-dicarboxy-2,29- bipyridyl],

SJW-E1 (cis-di(thiocyanato)-4,4'-di(octylethylenedioxythienyl)-2,2' -bipyridine- 4,4'- dicarboxylate-2,2'-bipyridine ruthenium(II))

JK-91 c/5-[Ru(R3)(H ₂ dcbpy)(NCS)2l ; dcbpy = 4,4'-dicarboxylic acid-2,2'-bipyridine;

JK-92 c/5-[Ru(R4)(H ₂ dcbpy)(NCS)2] ; dcbpy = 4,4'-dicarboxylic acid-2,2'-bipyridine;

SM371 4-{2-[(2Z,7Z, l l£,16Z)-7,17-Bis[2,6-bis(octyloxy)phenyl]-12-[bis({4-[2,4-b is(hexylox y)phenyl]phenyl})amino]-21,23,24,25-tetraaza-22-zincahexacyc lo[9.9.3.1 ³ , ⁶ . l ¹³ , ¹⁶ .0 ⁸ , ²³ .0 ¹⁸ , ²¹ ]pentacosa-l(20),2,4,6(25),7,9, l l, 13(24),14, 16,18-undecaen-2-yl]ethynyl}benzoi c acid D37

C102

C217

TFRS-1

TFRS-2

TFRS-3

S8

un

HY2

DX1

DPP07

DPP 14

DPP 15

DPP 17

A597

YE05

RK1

MB18-N

DEK1

B18

4. Liquids

Photosensitized surfaces alter their wettability upon irradiation of light. Changes in wettability allows for controlling the behavior of contacting liquids on the surfaces including contact angles, droplet motion and effective area of the solid-liquid interface. Utilizing photosensitized surfaces, it is feasible to control the behaviors of various liquids including but not limited to water, hydrocarbons, fluorocarbons, electrolyte, ionic liquids, dielectric liquids, emulsions, mixtures of any of liquids.

5. Light

Photosensitizers absorb light with particular wavelength depending on their molecular structures. For an effective photo-induced wettability switching of surfaces, it is important to irradiate light with a particular wavelength which photosensitizers can absorb.

For example, N3 absorbs a broad range of visible light with _max = 532 nm. However, UV-Vis absorbance spectrum of N3 shows that it barely absorbs visible light with λ > 700 nm whereas it has a strong absorption of light with λ < 550 nm. In this case, in order for photo-induced wettability switching, irradiation of light with λ < 550 nm is necessary.

6. Combinations of multiple photoactive materials/photosensitizers/liquids/light Due to various absorption spectra of a range of photosensitizers, sensitization of two or more photosensitizers with different absorption spectra may be advantageous in certain aspects. For example, if one sensitizer absorbs light with λ < 550 nm and the other absorbs light with 550 nm < λ < 750 nm, the surface sensitized by both sensitizers can absorb light with λ < 750 nm. Thus the surface can be sensitive to light with a broad band spectrum.

Further, selective wettability switching can be achieved. For example, let us assume that one sensitizer adsorbed on the surface induces change in contact angle for oil upon a light with 550 nm < λ < 750 nm. The other sensitizer on the same surface induces change in contact angle for water under a light with 550 nm < λ. In this case, controlling oil and/or water contact angles and droplet motions is feasible by irradiating a light with different wavelength.

By considering the above parameters, photoactive materials with photosensitizers can be useful a wide range of applications including separation, self-cleaning, lab-on-a-chip applications for controlling motion of liquid drops under light irradiation, antibacterial, antibiofouling coatings and photo-active switches.

Dye sensitized TiO? surfaces with switchable wettability

Imbibition of a liquid dye or adsorption of dye to a Ti0 ₂ surface is an alternative approach for generating charge carriers upon light illumination. See, Oregan, B. & Gratzel, M. A Low-Cost, High-Efficiency Solar-Cell Based on Dye- Sensitized Colloidal Tio2 Films. Nature 353, 737-740, doi:Doi 10.1038/353737a0 (1991), Bach, U. et al. Solid-state dye-sensitized mesoporous Ti02 solar cells with high photon-to-electron conversion efficiencies. Nature 395, 583-585 (1998), Mathew, S. et al. Dye-sensitized solar cells with 13% efficiency achieved through the molecular engineering of porphyrin sensitizers. Nat Chem 6, 242-247,

doi: 10.1038/NCHEM.1861 (2014), and Gratzel, M. Photoelectrochemical cells. Nature 414, 338- 344, doi:Doi 10.1038/35104607 (2001), each of which is incorporated by reference in its entirety. On a dye-sensitized Ti0 ₂ surface, the optical absorption and charge-generating functions are achieved by excitation of dye and subsequent injection of charge carriers (e.g., electrons) into the conduction band of Ti0 ₂ . See, Gratzel, M. Photoelectrochemical cells. Nature 414, 338-344, doi:Doi 10.1038/35104607 (2001), Hardin, B. E., Snaith, H. J. & McGehee, M. D. The renaissance of dye-sensitized solar cells. Nat Photonics 6, 162-169,

doi: 10.1038/NPHOTON.2012.22 (2012), and Gratzel, M. Dye-sensitized solar cells. J Photoch Photobio C 4, 145-153, doi: 10.1016/S1389-5567(03)00026-l (2003), each of which is incorporated by reference in its entirety. The light absorption behavior of a dye-sensitized Ti0 ₂ surface can be readily tuned by careful consideration of the energy levels of the selected dye. Ruthenium (II) polypyridyl complexes have received particular interest due to their wide absorption range from the visible to the near-infrared regime and high stability in the oxidized state. See, Qin, Y. C. & Peng, Q. Ruthenium Sensitizers and Their Applications in Dye- Sensitized Solar Cells. Int J Photoenergy (2012) and Nazeeruddin, M. K., Klein, C, Liska, P. & Gratzel, M. Synthesis of novel ruthenium sensitizers and their application in dye-sensitized solar cells. Coordin Chem Rev 249, 1460-1467, doi: 10.1016/j .ccr.2005.03.025 (2005), each of which is incorporated by reference in its entirety. Further, introduction of a textured roughness or porosity to the Ti0 ₂ surface can dramatically increase the light absorption efficiency due to an increased specific surface area providing capillary stabilization of a surface adsorbed liquid film in which a large number of dye molecules can be directly adsorbed. Consequently, dye- sensitization may provide a versatile tool to tune the wettability of Ti0 ₂ surfaces under visible- light illumination.

Disclosed herein are a method and a system to switch the wettability of photoactive materials to be responsive in the visible spectral regime using dye sensitization. As an example, an N3 dye-sensitized Ti0 ₂ surface can be fabricated. A thin, nanostructured and highly porous Ti0 ₂ surface is prepared by layer-by-layer (LBL) deposition of negatively charged Ti0 ₂ nanoparticles (average diameter « 20 nm) and positively charged poly(allylamine hydrochloride) on an indium tin oxide (ITO)-coated glass slide followed by calcination (see Examples). A scanning electron microscopy (SEM) image (see inset (i) in FIG. 6A) shows that the surface is highly porous with a large specific surface area. The ratio of the total surface area per unit projected area is estimated to be 56 (see Examples). The resulting porous Ti0 ₂ surface is subsequently dip-coated in N3 dye solution (see Examples). N3 dye molecules chemisorb to the surface via carboxylate groups. See, Wayment-Steele, H. K. et al. Monitoring N3 Dye

Adsorption and Desorption on Ti02 Surfaces: A Combined QCM-D and XPS Study. Acs Appl Mater Inter 6, 9093-9099, doi: 10.1021/am500920w (2014), which is incorporated by reference in its entirety. Adsorption of N3 dye molecules leads to a deep brown coloration of the surface (see inset (ii) in FIG. 6A). The visible light absorption spectra of an N3 dye-sensitized Ti0 ₂ surface was measured, and, as shown in FIG. 6 A, the surface absorbs a broad range of the incident visible spectrum (390 nm < λ < 700 nm). In contrast, an unsensitized LBL-deposited Ti0 ₂ nanostructured surface displays negligible absorption in the visible regime due to the wide band gap energy of the Ti0 ₂ particles (« 3.2 eV). See, Fujishima, A., Zhang, X. T. & Tryk, D. A. Ti02 photocatalysis and related surface phenomena. Surf Sci Rep 63, 515-582,

doi: 10.1016/j .surfrep.2008.10.001 (2008), which is incorporated by reference in its entirety.

To study the photo-induced wettability change of the N3 dye-sensitized Ti0 ₂ surface, the evolution in the contact angles were measured in situ for three liquid droplets: deionized (DI) water, potassium iodide (KI, 10 wt% in water) and potassium chloride (KCl, 10 wt% in water). In situ contact angle measurements were conducted under oil (e.g., dodecane) environment to minimize evaporation of a droplet due to the heat generated from the light source (see inset in FIG. 6B and Examples) and to simulate the condition expected in oil-water separation operation. See, Kwon, G. et al. On-Demand Separation of Oil-Water Mixtures. Adv Mater 24, 3666-3671, doi: 10.1002/adma.201201364 (2012), Jen-Shih Chang, A. J. K., Joseph M. Crowley. Handbook of Electrostatic Processes. (CRC Press, 1995), and Anil K. Pabby, S. S. H. R., Ana Maria Sastre Requena. Handbook of Membrane Separations: Chemical, Pharmaceutical, Food, and

Biotechnological Applications. (CRC Press, 2008), each of which is incorporated by reference in its entirety. The visible light source with intensity (/ = 145 mW/cm ² ) is projected from above the surface in order to minimize intensity loss along the light transmission path. FIG. 6B shows the evolution in the macroscopic contact angles ( 6> ^* ) for DI water, KI and KCl droplets as a function of illumination time. The equilibrium contact angles for DI water and KCl remain almost constant during illumination ( A6 _D ^* _Iwater ~ 3° and Αθ _κ ^* _α ~ 2° where ΑΘ ^* = θ ^* ₌₀ - θ ^* _{=Ι β]ήη} ), while those for KI decrease progressively from θ _{η t=0} = 119° with increasing illumination time before finally approaching έ¾ _{ι=120πιίη} ⁼ 77° (see FIG. 6B). The negligible wettability change for KCl was also independent of concentration while KI droplets with higher ionic concentration exhibited rapid decrease in contact angles (see Examples). Such a selective photo-induced wetting response of KI over KCl (or DI water) is further exemplified by considering multiple wetting cycles as shown in FIG. 6C. The contact angles for fresh droplets of KI placed at a fixed location on the surface cycles between θ _η ^* _t=0 « 119° and Θ _Ώ ^* _(=120mi]1 * 77° under repeated illumination while that for KCl remains almost constant. Unlike an unsensitized, as-fabricated Ti0 ₂ surface, X-ray photoelectron spectroscopy (XPS) analysis of the N3 dye-sensitized Ti0 ₂ surface clearly indicates that the surface chemistry remains unaffected after multiple cycles of wetting under visible light illumination (Examples).

On dye-sensitized Ti0 ₂ surfaces, photo-generated electrons from incident visible light illumination are injected and travel through the nanoporous Ti0 ₂ network. See, Hardin, B. E., Snaith, H. J. & McGehee, M. D. The renaissance of dye-sensitized solar cells. Nat Photonics 6, 162-169, doi: 10.1038/NPHOTON.2012.22 (2012), and Gratzel, M. Dye-sensitized solar cells. J Photoch Photobio C 4, 145-153, doi: 10.1016/S1389-5567(03)00026-l (2003), each of which is incorporated by reference in its entirety. It is anticipated that this electron transfer results in the generation of an electric potential difference between the surface and the contacting liquid which can then induce electrowetting effects in liquid droplets on the surface. To understand this further, the physico-chemical origin of a photo-induced electric potential difference was considered under light illumination.

FIG. 7A shows a schematic and energy diagram of an N3 dye-sensitized Ti0 ₂ surface contacting a KI droplet. After electron transfer upon illumination, a region over which the charge distribution differs from the bulk is produced. This corresponds to the electrolytic double layer and the accumulation layer at the contacting KI and Ti0 ₂ , respectively. See, Gratzel, M.

Photoelectrochemical cells. Nature 414, 338-344, doi:Doi 10.1038/35104607 (2001), which is incorporated by reference in its entirety. Consequently, an electric potential difference (i.e., a measurable voltage) is generated between the contacting KI droplet and the underlying substrate. The oxidized dye (D ⁺ ) can be subsequently reduced by accepting an electron from the reducing agent (i.e., the iodide, Γ) in the KI through the chemical reaction 2D ⁺ + 3 → 2D + I ^~ (a process known as regeneration). See, Pelet, S., Moser, J. E. & Gratzel, M. Cooperative effect of adsorbed cations and iodide on the interception of back electron transfer in the dye sensitization of nanocrystalline Ti02. JPhys Chem B 104, 1791-1795, doi:Doi 10.1021/Jp9934477 (2000), Clifford, J. N., Palomares, E., Nazeeruddin, M. K., Gratzel, M. & Durrant, J. R. Dye dependent regeneration dynamics in dye sensitized nanocrystalline solar cells: Evidence for the formation of a ruthenium bipyridyl cation/iodide intermediate. JPhys Chem C 111, 6561-6567,

doi: 10.1021/jp067458t (2007), and Alebbi, M., Bignozzi, C. A., Heimer, T. A., Hasselmann, G. M. & Meyer, G. J. The limiting role of iodide oxidation in cis-Os(dcb)(2)(CN)(2)/Ti02 photoelectrochemical cells. JPhys Chem B 102, 7577-7581, doi:Doi 10.1021/Jp981643s (1998), each of which is incorporated by reference in its entirety. An alternative pathway for reducing the oxidized dye is by recombining with an electron in the Ti0 ₂ (i.e., the process of

recombination). See, Boschloo, G. & Hagfeldt, A. Characteristics of the Iodide/Triiodide Redox Mediator in Dye-Sensitized Solar Cells. Accounts Chem Res 42, 1819-1826,

doi: 10.1021/ar900138m (2009), and Antila, L. J., Myllyperkio, P., Mustalahti, S., Lehtivuori, H. & Korppi-Tommola, J. Injection and Ultrafast Regeneration in Dye-Sensitized Solar Cells. J Phys Chem C 118, 7772-7780, doi: 10.1021/jp4124277 (2014), each of which is incorporated by reference in its entirety. While the regeneration is more favorable and orders of magnitude faster, the recombination also plays an important role in dye reduction process, especially under open- circuit conditions. See, Montanari, L, Nelson, J. & Durrant, J. R. Iodide electron transfer kinetics in dye-sensitized nanocrystalline Ti02 films. J Phys Chem B 106, 12203-12210,

doi: 10.1021/jp025824c (2002), Bauer, C, Boschloo, G., Mukhtar, E. & Hagfeldt, A. Interfacial electron-transfer dynamics in Ru(tcterpy)(NCS)(3)-sensitized Ti02 nanocrystalline solar cells. J Phys Chem B 106, 12693-12704, doi: 10.1021/jp0200268 (2002), Nelson, J. Continuous-time random-walk model of electron transport in nanocrystalline Ti02 electrodes. Phys Rev B 59, 15374-15380, doi:Doi 10.1 103/Physrevb.59.15374 (1999), Haque, S. A., Tachibana, Y., Klug, D. R. & Durrant, J. R. Charge recombination kinetics in dye-sensitized nanocrystalline titanium dioxide films under externally applied bias. J Phys Chem B 102, 1745-1749, doi:Doi

10.1021/Jp973335k (1998), and Cahen, D., Hodes, G, Gratzel, M., Guillemoles, J. F. & Riess, I. Nature of photovoltaic action in dye-sensitized solar cells. J Phys Chem B 104, 2053-2059, doi:Doi 10.1021/Jp993187t (2000), each of which is incorporated by reference in its entirety.

To validate hypothesis, the in situ voltage was measured across the contacting liquids and the N3 dye-sensitized Ti0 ₂ surface while illuminating with visible light (see FIG. 7B).

Immediately after the onset of illumination, a potential difference J¾ t=o ~ 0.42 V is observed between the KI droplet and the lower ITO electrode. The voltage decreases gradually with increasing illumination time and eventually reaches zero after t « 45 min. Similar to conventional electrowetting, this photo-induced voltage causes spreading of the KI droplet on the N3 dye- sensitized Ti0 ₂ surface. The gradual decrease in the measured voltage can be explained by considering the electrolytic double layer as a capacitor (C) and the underlying Ti0 ₂ film as a resistor (R). Thus the KI droplet and the Ti0 ₂ film can be considered as an imperfect RC circuit connected in series. When the capacitor in an imperfect RC circuit is discharged, the voltage V(f) is given by

V(t) = V ₀ exp[-(t / T _d ) ^a ] _{( 1 )}

where V ₀ , ¾ a denote the voltage at t = 0, the relaxation time constant and the fractional derivative order, respectively. Note that equation (1) characterizes a fractional RC circuit where the capacitor (or a resistor) is imperfect. See, Westerlund, S. & Ekstam, L. Capacitor Theory. Ieee T Dielect El In 1, 826-839, doi:Doi 10.1 109/94.326654 (1994), and Radwan, A. G. & Salama, K. N. Fractional-Order RC and RL Circuits. Circ Syst Signal Pr 31, 1901-1915, doi: 10.1007/s00034-012-9432-z (2012), each of which is incorporated by reference in its entirety. The measured voltages across the KI and ITO (see FIG. 7B) are well described by equation (1) with r _d = 130 sec and a = 0.42. Furthermore, changes in the contact angle halt instantaneously and the droplet shape remains unchanged when the illumination is turned off.

Unlike the gradual decrease in voltage between the KI droplet and the surface during optical illumination, a rapid decrease in the voltage was observed between a KCl droplet and the surface after the onset of illumination (see FIG. 7B). Rapid decrease in the voltage highlights the importance of the dye reduction process in photo-induced voltage generation. As the reduction potential of iodide (Γ, E _re d, i- = 0.53 V vs. NHE (Normal hydrogen electrode)) is above (i.e., less positive than) the HOMO energy level of N3 dye (E _H OMO, N3 = 1.0 V vs. NHE), it presents a driving force to reduce the oxidized dye. As a consequence, an N3 dye-sensitized Ti0 ₂ surface contacting a KI droplet can maintain a prolonged voltage difference by suppressing the recombination process. In contrast, chloride (CT, E _rec i, ci- = 1.36 V vs. NHE) cannot effectively reduce the oxidized N3 dye due to its higher reduction potential resulting in a dominant recombination process. See, Haynes, W. M. CRC Handbook of Chemistry and Physics, 96th edition. (CRC Press, 2015), and Jeon, J., Goddard, W. A. & Kim, H. Inner-Sphere Electron- Transfer Single Iodide Mechanism for Dye Regeneration in Dye-Sensitized Solar Cells. J Am Chem Soc 135, 2431-2434, doi: 10.1021/ja31 1714a (2013), each of which is incorporated by reference in its entirety.

To probe the hypothesis that suppressing the recombination process leads to prolonged photo-induced voltage generation, and subsequently extension of the wetting (i.e., a larger change in contact angles), an electrically-grounded N3 dye-sensitized Ti0 ₂ surface was fabricated (see inset in FIG. 7C). In contrast to the previous surface where photo-generated electrons continue to accumulate and participate in the recombination process, the electrically- grounded surface minimizes electron accumulation. FIG. 7C shows an enhanced decrease in macroscopic contact angles for KI ( Θ _Κ ^* _Ι ∞ 72°) and KC1 ( θ _κ ^* _α ∞ 7°) droplets on the electrically- grounded N3 dye-sensitized Ti0 ₂ surface after 120 min of illumination. This may be a direct consequence of the suppression of the recombination process.

These findings provide us with design parameters to systematically manipulate the wettability of dye-sensitized Ti0 ₂ surfaces towards different contacting liquids in response to visible light illumination. For effective wetting of specific liquids, it is preferential to regenerate the oxidized dye by a reducing agent within the contacting liquid (see FIG. 7A). This often requires careful consideration of the energy levels of the dye and different contacting liquids. As is well documented in the dye-sensitized solar cell literature (see Hardin, B. E., Snaith, H. J. & McGehee, M. D. The renaissance of dye-sensitized solar cells. Nat Photonics 6, 162-169, doi: 10.1038/NPHOTON.2012.22 (2012), and Gratzel, M. Dye-sensitized solar cells. JPhotoch Photobio C 4, 145-153, doi: 10.1016/S1389-5567(03)00026-l (2003), each of which is incorporated by reference in its entirety), effective dye-regeneration is typically achieved by using electrolytes that possess a reduction potential which is less positive than the HOMO energy level of dye. This enables us to create a design chart for photo-induced wetting of contacting liquids on a dye-sensitized Ti0 ₂ surface. FIG. 8A shows an energy diagram of various dyes and electrolytes. The HOMO energy levels of the dyes are located in between the reduction potential of liquids considered in this work. Here D149 dye and Chlorin dye were chosen as sensitizers (see Examples). See, Liu, Z. Y. et al. Solution-Processed Organic Photovoltaics Based on Indoline Dye Molecules Developed in Dye-Sensitized Solar Cells. Molecules 18, 3107-3117, doi: 10.3390/moleculesl8033107 (2013), and Wang, X. F. & Kitao, O. Natural Chlorophyll- Related Porphyrins and Chlorins for Dye- Sensitized Solar Cells. Molecules 17, 4484-4497, doi: 10.3390/moleculesl7044484 (2012), each of which is incorporated by reference in its entirety. Similar to the N3 dye-sensitized Ti0 ₂ surface, a D149 dye-sensitized Ti0 ₂ and a Chlorin dye-sensitized Ti0 ₂ absorb across a broad range of the visible light spectrum. As their lowest unoccupied molecular orbital (LUMO) energy levels are above (i.e., less positive than) the conduction band of Ti0 ₂ , efficient electron transfer can be achieved ^47"49 . See, Liu, Z. Y. et al. Solution-Processed Organic Photovoltaics Based on Indoline Dye Molecules Developed in Dye- Sensitized Solar Cells. Molecules 18, 3107-3117, doi: 10.3390/moleculesl8033107 (2013), Wang, X. F. & Kitao, O. Natural Chlorophyll-Related Porphyrins and Chlorins for Dye- Sensitized Solar Cells. Molecules 17, 4484-4497, doi: 10.3390/moleculesl7044484 (2012), and Lightbourne, S. K. S., Gobeze, H. B., Subbaiyan, N. K. & D'Souza, F. Chlorin e6 sensitized photovoltaic cells: effect of co-adsorbents on cell performance, charge transfer resistance, and charge recombination dynamics. J Photon Energy 5, doi: Artn 053089

10.1117/1. Jpe.5.053089 (2015), each of which is incorporated by reference in its entirety.

However, subsequent regeneration of the oxidized dyes by various electrolytes will be selective due to their different HOMO energy levels (E _H O _M O _{, DI} 4 = 1.14 V vs. NHE and E _H O _M O, chiorin = 1.72 V vs. NHE) with respect to the reduction potentials of various electrolytes. Along with KI and KC1, potassium thiosulfate (K ₂ S ₂ O ₃ , 10 wt% in water, E _re d, ₂ s ₂ o ₃ = 0.08 V vs. NHE) and potassium bromide (KBr, 10 wt% in water, E _rec i, KBr = 1 09 V vs. NHE) were used as contacting liquids. In situ photo-induced voltage measurements of a D149 dye-sensitized Ti0 ₂ and a Chlorin dye-sensitized Ti0 ₂ in contact with droplets of various electrolytes clearly indicate that a prolonged voltage difference across the surface and the contacting liquid droplet is achieved when E _H O _M O, dye > E _re d, liquid · FIG. 8B shows the evolution in the macroscopic contact angles for K ₂ S ₂ 0 ₃ , KI, KBr and KC1 droplets on a D149 dye-sensitized Ti0 ₂ surface under illumination. Contacting liquids with a lower reduction potential (i.e., less positive) than E _H O _M O _{, DI} 49 (e.g., K ₂ S ₂ O ₃ , KI and KBr, see also FIG. 8 A) spread on the surface while a droplet of KC1 exhibits a negligible contact angle decrease. In contrast, a decrease in the macroscopic contact angles were observed for all contacting liquids on a Chlorin dye-sensitized Ti0 ₂ surface under visible light illumination (see FIG. 8C). This is a direct consequence of the effective dye-regeneration process with all contacting liquids as a result of the very high E _H O _M O of Chlorin dye. See, Wang, X. F. & Kitao, O. Natural Chlorophyll-Related Porphyrins and Chlorins for Dye- Sensitized Solar Cells. Molecules 17, 4484-4497, doi: 10.3390/moleculesl7044484 (2012), and Lightbourne, S. K. S., Gobeze, H. B., Subbaiyan, N. K. & D'Souza, F. Chlorin e6 sensitized photovoltaic cells: effect of co-adsorbents on cell performance, charge transfer resistance, and charge recombination dynamics. J Photon Energy 5 (2015), each of which is incorporated by reference in its entirety. Selective wetting behaviors of K ₂ S ₂ O ₃ (or KI) over KBr (or KC1) on an N3 dye-sensitized Ti0 ₂ surface is also observed (FIG. 8B). This is the first-ever systematic demonstration of visible light induced wetting of contacting liquid droplet on dye-sensitized Ti0 ₂ surfaces. The ability to photo-induce the selective wetting of contacting liquids on a dye-sensitized Ti0 ₂ surface provides a versatile tool to manipulate liquid motion. FIG. 9A shows visible-light- guided movement of an NaCl (10 wt% in water) droplet on a patterned dye-sensitized Ti0 ₂ surface submerged in dodecane. The patterned surface consists of a thin channel of Chlorin dye- sensitized LBL-assembled nanoporous Ti0 ₂ surrounded by a hydrophobic background (see

Methods). A droplet of NaCl is placed on the channel, and white light is focused on one edge of the droplet (see FIG. 9A (i)). The contact angle at the interface between the liquid and the illuminated surface decreases while the other side remains pinned. Consequently, the droplet moves towards the illuminated edge (see FIG. 9A (ii)). Further illumination leads to an elongation of the droplet shape (see FIG. 9A (iii)). The photo-induced anisotropic wetting (i.e., progressive spreading in one direction while the other side remians pinned) of a NaCl droplet was observed on a Chlorin dye-sensitized Ti0 ₂ surface (sequential snapshot images are shown in FIGS. 9A (iv)-(vi)). This anisotropic wetting behavior under focused optical illumination allows for coalescence of multiple aqueous droplets that are initially pinned on the surface. FIG. 9B shows sequential photographs of the coalescence of multiple NaCl droplets on a Chlorin dye- sensitized Ti0 ₂ surface submerged in dodecane. By shining visible light at various locations between the droplets, photo-induce coalescence of all droplets result in a single continuous NaCl aqueous layer on the surface.

This photo-induced coalescence process is an ideal candidate to substitute for

conventional electrostatic coalescence technique employed in demulsification (i.e., the conversion of an oil-water emulsion into two separate oil-free and water-free phases), especially for mixtures with high salt concentration (e.g., brine-oil emulsions) that are typically generated in enhanced oil-recovery operations. See, Kwon, G. et al. On-Demand Separation of Oil-Water Mixtures. Adv Mater 24, 3666-3671, doi: 10.1002/adma.201201364 (2012), Jen-Shih Chang, A. J. K., Joseph M. Crowley. Handbook of Electrostatic Processes. (CRC Press, 1995), and Anil K. Pabby, S. S. H. R., Ana Maria Sastre Requena. Handbook of Membrane Separations: Chemical, Pharmaceutical, Food, and Biotechnological Applications. (CRC Press, 2008), each of which is incorporated by reference in its entirety. The demulsificiation of brine-oil emulsions using the photo-induced coalescence is highly desirable because conductive emulsions resulting from ionized salts create a current path upon application of an external electric field which hinders generation of induced dipole moments. See, Eow, J. S. & Ghadiri, M. Electrostatic enhancement of coalescence of water droplets in oil: a review of the technology. Chem Eng J 85, 357-368, doi:Doi 10.1016/S1385-8947(01)00250-9 (2002), which is incorporated by reference in its entirety. Here demulsification of a brine-oil emulsion was demonstrated utilizing photo-induced coalescence of water droplets containing salts on a dye-sensitized Ti0 ₂ surface. FIGS. 9C and 9D show demulsificatoin of a brine (10 wt% NaCl in water)-in-dodecane emulsion stabilized by 0.1 wt% of Span80 surfactant (see Examples). The demulsification apparatus consists of a stainless steel membrane (pore size « 2 μπι) coated with Chlorin dye-sensitized Ti0 ₂

nanostructured film sandwiched between the two vertical glass tubes. The emulsion is added to the upper tube and immediately visible light is illuminated on the membrane surface (see FIG. 9C). Brine droplets that contact the Chlorin dye-sensitized Ti0 ₂ mesh surface spread and coalesce with other droplets under white light illumination. Within minutes of illumination, the brine-in-dodecane emulsion demulsifies into brine-rich and dodecane-rich phases (see FIG. 9D). FIG. 9E shows the number size distribution of the dodecane-rich retentate after 4 min of demulsification. The shaded region represents the brine droplets removed (corresponding to > 99.9 vol%) during demulsification. By comparing with the feed emulsion, it is evident that nearly all brine droplets above 25 μπι (i.e., > 99.9 vol% of brine) are removed by photo-induced coalescence. The demulsification of a brine-in-oil emulsion using photo-induced coalescence of brine droplets was demonstrated on Chlorin dye-sensitized Ti0 ₂ mesh surface.

In summary, dye-sensitized nanoporous Ti0 ₂ surfaces can selectively change the wettability towards contacting liquids upon visible light illumination, due to a photo-induced voltage difference across the liquid and the surface. The HOMO energy level of the selected dye and the reduction potential of the contacting liquid droplet phase govern the effective dynamics of the photo-induced voltage difference. The photo-induced wettability change of a dye- sensitized Ti0 ₂ surface enables external manipulation of liquid droplet motion across a surface upon visible light illumination. Spontaneous demulsification and separation of surfactant- stabilized brine-in-oil emulsion was demonstrated using photo-induced coalescence of brine droplets on a dye-sensitized Ti0 ₂ surface. Such abilities to remotely activate and control the wettability states of surfaces through optical illumination will enable new microfluidic separation technologies as well as result in new sunlight-driven oil-water clean-up and deemulsification approaches. EXAMPLES

Fabrication of TiO surfaces

A number methods can be used to create Ti0 ₂ surfaces including sol-gel method, sol method, hydrothermal method, chemical vapor deposition, atomic layer deposition, electro- deposition, direct oxidation, magnetron sputtering, layer-by-layer (LBL) deposition.

Example 1.

LBL deposition technique was utilized to fabricate Ti0 ₂ surfaces (FIG. 1). Here glass slides obtained from VWR were used as substrates where Ti0 ₂ films were deposited. The glass slide is first washed with DI water. Then it is treated with oxygen plasma for 10 min to remove any contaminants present on the glass slide surface and to endow negative surface charge on the surface. Here Ti0 ₂ nanoparticles serve as the negative species while a positive polyelectrolyte, poly(allylamine hydrochloride) (PAH, Mw = 58,000 Da) obtained from Sigma-Aldrich is used as the positive species. The coating solutions containing Ti0 ₂ nanoparticles (average diameter = 20 ± 5nm) and PAH are prepared in a solvent of deionized water. Concentrations for both solutions were maintained at 0.03 wt% and 1 mg/mL, respectively. The pH for both solutions were adjusted to 9.0 ± 0.1 and 7.5 ± 0.1, respectively. The substrate was dipcoated in the prepared LBL solutions by using an automated machine (Nanostrata Inc.). Since LBL process used a polyelectrolyte as intermediate layers between the Ti0 ₂ layers, it was necessary to remove this organic content. In order to remove PAH layers, the substrate was calcined at 400 °C for 2 hours. The prepared Ti0 ₂ surfaces are nanoporous with - 150 nm thickness (FIG. 2).

Example 2.

A thin, nanostructured Ti0 ₂ surface was fabricated using layer-by-layer (LBL) deposition either on an indium tin oxide (ITO) coated glass slide (Sigma Aldrich, surface resistivity = 8 - 12 Ω/sq) or stainless steel mesh (TWP Inc., pore size « 2 μπι) substrates. First, the substrates were thoroughly rinsed with isopropyl alcohol and DI water followed by drying with nitrogen gas. The cleaned substrates were sequentially dip-coated in poly(allylamine hydrochloride) (PAH) (Sigma Aldrich, average molecular weight = 15,000 g/mol) aqueous solution (1 mg/mL, pH = 7.5) and Ti0 ₂ nanoparticle (Svaya Nanotechnology, average diameter « 20 nm) aqueous dispersion (0.03 wt%, pH = 9.0). After depositing 30 bilayers of PAH and Ti0 ₂ , the substrates were calcined at 400 °C for 2 hours to remove PAH from the surface. A scanning electron microscopy (SEM) image shows that the surface is highly porous (see inset (i) in FIG. 6A). Dye sensitization

Example 1.

N3 (cis-Bis(isothiocyanato) bis(2,2'-bipyridyl-4,4'-dicarboxylato) ruthenium(II)) was used for sensitization. First the dye was dissolved in ethanol at a concentration of 0.3 mM. The substrate was immersed into the dye solution for 12 hours at room temperature followed by washing with copious amounts of ethanol in order to remove excess dye. Dye molecules anchor on the Ti0 ₂ surface via the -COOH groups, most likely in the form of carboxylate.

The UV- Visible absorption spectrum of prepared dye sensitized Ti0 ₂ surface was measured between 350 and 800 nm (FIGS. 8A-8C). It absorbs visible light spectral region with wavelengths between 390 nm - 650 nm. By contrast, a neat Ti0 ₂ surface (i.e., without dye sensitization) exhibited negligible absorbance on the same spectral region. This clearly indicates that absorption of dye sensitized Ti0 ₂ surfaces due to excitation of dye molecules.

The composition of the surfaces was analyzed using XPS. FIGS. 9A-9E shows the N Is and S 2p regions that reveal the presence of components from the dye. Further the atomic concentration ratio of N and S was found to be 3 : 1. This value is same as that of stoichiometric ratios for nitrogen and sulfur in the dye molecule.

Example 2.

Solutions (0.3 mM) of N3 dye (Sigma Aldrich), D149 dye (Sigma Aldrich) and Chlorin dye (Frontier Scientific) were prepared in anhydrous ethanol (Fischer Scientific). Note that N3 dye, D149 dye and Chlorin dye denote cis-bis(isothiocyanato) bis(2,2'-bipyridyl-4,4'- dicarboxylato ruthenium (II), 5-[[4-[4-(2,2-diphenylethenyl)phenyl]-l,2,3,3a,4,8b- hexahydrocyclopent[b]indol-7 yl]methylene]-2-(3-ethyl-4-oxo-2-thioxo-5-thiazolidinylidene )-4- oxo-3-thiazolidineacetic acid and 13-carboxy-17-(2-carboxyethyl)-15-carboxymethyl-17,18- trans-dihydro-3-vinyl-8-ethyl-2,7, 12,18 tetramethylporphyrin, respectively. Small pieces of substrates with Ti0 ₂ surface were dip-coated in the desired solution for 12 hours followed by thorough rinsing with ethanol to remove any residual dye molecules from the surface. The substrates were then dried with nitrogen gas. In situ contact angle measurements under visible light illumination

A small volume (= 4 μΐ) of ionic aqueous droplet was placed onto a dye-sensitized Ti0 ₂ surface submerged in dodecane. Visible light (MI 150, Edmund Optics) was irradiated from the top of the droplet. Note that the intensity of the light was constant (1 = 145 mW/cm ² ) in all measurements. The contact angle measurements were conducted using a Rame-Hart 590-Fl goniometer.

Fabrication of a patterned dye-sensitized TiO? surface

A glass slide was masked in a channel (5 mm wide xl5 mm long) by Kapton polyimide adhesive tape (ULINE) by manual application. A Ti0 ₂ film was prepared on the unmasked region using LBL deposition followed by calcination as described above. Subsequently the substrate was dip-coated in a Chlorin dye solution for 12 hours to obtain a Chlorin dye-sensitized Ti0 ₂ channel. The channel was then masked by attaching a cross-linked poly dimethyl siloxane (x-PDMS) film. The substrate was treated with heptadecafluoro-l, l,2,2-tetrahydrodecyl trichlorosilane (Gelest) by vapor phase deposition at 90 °C for 1 hour to obtain hydrophobic background.

Demulsifwation of a brine -in-dode cane emulsion

A brine-in-dodecane emulsion (30:70 v:v) was prepared by mixing water with 10 wt% sodium chloride (NaCl) and dodecane using a stir bar at 1000 rpm. The concentration of Span80 surfactant was 0.1 wt% to dodecane phase. The emulsion is added onto a stainless steel mesh coated with a Chlorin dye-sensitized Ti0 ₂ film which is sandwiched between the two vertical glass tubes. After addition of emulsion, visible light is illuminated onto the mesh surface to induce coalescence of brine droplets.

Switching wettability upon irradiation of visible light

In order to study the wettability switch of the facbricated surfaces, the substrate was immersed in oil and irradiated with visible light to observe the water contact angle change.

Wettability changes under irradiation of UV or visible light were studied typically by measuring water contact angles in air. In the present example, however, water contact angles were measured in oil environments for two reasons. First, measurements of water contact angles in air are subject to the uncertainties which arise from intrinsic hydrophilicity of dye sensitized surfaces. Second, water drop evaporates during measurements due to a heat generation from visible light source. In order to avoid those limitations, water contact angles were measured in oil environments. Here octane was chosen as a representative oil because it has a low surface tension which leads to higher contact angles for water. Also it is immiscible with water.

A drop of DI water of size 3 μΐ _^ was inserted carefully on the surface immersed in oil. The initial contact angle for water is 121° ± 1°. Visible light was irradiated on the surface at a distance on 5 mm above a drop of water. After 60 min of irradiation, the contact angle decreased gradually and reached 115°. This result suggests that the surface alters wettability upon irradiation of visible light, investigated visible light-induced wettability switch was investigated using different liquids. Potassium iodide (KI) aqueous solution (10 wt%) was chosen as a representative electrolyte. Upon irradiation of visible light, rapid decrease in contact angles was observed in a short period of time (~ 5 min). After 60 min, the contact reached a value of 62°. Contact angles for KI solutions were also measured with different concentrations (0.5 wt%, 5.0 wt% and 20 wt%) under visible light irradiation. Rates of decrease in contact angles increases with increasing concentration of KI (FIG. 5).

Estimation of the ratio of total surface area per unit projected area

Tthe ratio of the total inner surface area per unit surface area was estimated. The absorbance of N3 dye-sensitized Ti0 ₂ surface at 478 nm is 0.1736 (see FIG. 6A). The extinction coefficient of N3 dye at 478 nm is e ₄₇₈ „ _m = 1.88 10 ⁷ cm ² mor ^l \ The dye concentration on the surface can be calculated by dividing the absorbance with the extinction coefficient. This yields 9.23 \0 ^~9 mol cm ^~2 . Considering that each dye molecule occupies an area of 1 nm ² , the inner surface area is 56 cm ² for each 1 cm ² projected area. See, Nazeeruddin, M. K., Liska, P., Moser, J., Vlachopoulos, N. & Gratzel, M., Helv. chim. Acta 73, 1788-1803 (1990), which is incorporated by reference in its entirety.

Measured contact angles for KI and KCl droplets with various concentrations on an N3 dye- sensitized TiO surface under visible light illumination

Contact angles were measured for aqueous KI and KCl droplets with a range of different concentrations on an N3 dye-sensitized Ti0 ₂ surface upon visible light illumination. FIG. 10 shows the contact angles for KI droplets with 0.5 wt%, 5 wt%, 10 wt% and 20 wt% as a function of illumination time (intensity = 145 mW/cm ² ). It shows that KI droplets with higher ionic concentration exhibited rapid decrease in the contact angles under optical illumination. On the other hand, the contact angles for KCl droplets remained almost unchanged during illumination and this negligible change in the contact angles was found to be independent of ionic

concentration (see Table 1).

Table 1. Measured contact angles for potassium chloride (KCl) droplets with various concentrations on an N3 dye-sensitized Ti0 ₂ surface before and after illumination for 120min.

X-ray photoelectron spectroscopy (XPS) analysis of the N3 dye-sensitized TiOj surface after visible light illumination

To verify that the surface chemistry of the N3 dye-sensitized Ti0 ₂ surface remains unaffected after visible light illumination, XPS measurements were conducted using a PHI 5600 ESC A multi-detection system with a base pressure of 1 x 10 ^"10 Torr. The X-ray radiation was the monochromatic Al Ka line (1486.7 eV); the X-ray spot size and the take-off angle were 0.8 mm and 45°, respectively.

The survey spectra of the N3 dye-sensitized Ti0 ₂ before and after multiple cycles of wetting under visible light illumination are shown in FIG. 11. The photoelectron peaks in the spectra can be attributed to titanium (Ti), oxygen (O), sulfur (S) and ruthenium (Ru). The origin of ruthenium and sulfur is due to N3 dye molecules adsorbed on the Ti0 ₂ surface. The surface compositions were obtained by normalizing the area under the curve. The atomic concentration ratio of titanium (Ti2p) and ruthenium (Ru3d) of the N3 dye-sensitized Ti0 ₂ surface remained unchanged (72.1 :27.9, atomic%:atomic%) even after multiple cycles of wetting under visible light illumination. This indicates that the N3 dye-sensitized Ti0 ₂ surface is robust against optical illumination. Prediction of voltages between the contacting liquid droplets and the N3 dye-sensitized TiO surfaces

As discussed above, the electrolytic double layer formed at the liquid-solid interface under incident illumination can be considered as a capacitor. The time-dependent voltages was predicted by assuming that the capacitor is discharged over time. When a capacitor is discharged in an RC circuit, the voltage decays exponentially over time which is characterized by

V(t) o exp[-(t / T _d )], where ¾ is the relaxation time constant. This can describe the voltages well when a capacitor (or a resistor) is perfect. Here this electrolytic double layer may not be a perfect capacitor. This is a reasonable assumption because the dye-sensitized Ti0 ₂ surface possesses nanometric pores contacting oil (dodecane) phase which leads to the increase its resistive characteristic. When such an 'imperfect' capacitor is discharged, the voltage can be characterized by a stretched exponential function, V{t)∞ exp[-(t / T _d ) ^a ] , where a (0 < a < 1) is the fractional derivative order (see also equation (1)). When a =1, the stretched exponential is reduced to the simple exponential. Equation (1) was used to predict the voltages between the KI (or KC1) droplet and the surface. The measured voltages match well with equation (1) with r _d = 130 sec and a = 0.42 for KI droplet and ¾ = 11.5 sec and a = 0.988 for KC1 droplet, respectively.

Measured contact angles for a KI droplet on an N3 dye-sensitized TiO surface upon intermittent visible light illumination

The contact angles for a KI droplet (10 wt% in water) were measured on an N3 dye- sensitized Ti0 ₂ surface upon intermittent visible light illumination. FIG. 12 shows the contact angles for a KI droplet as a function of illumination time (intensity = 145 mW/cm ² ). The contact angle decreases progressively from θ _{η t=0} = 119° after the onset of illumination and reaches θ _νι , ■ ⁼ 92° at t = 10 min. When the illumination is turned off at t = 10 min, the contact angle changes halt instantaneously and the contact angle remains unchanged. When the illumination is turned on at t = 30 min, the contact angle starts to decrease. The illumination is again turned off at t = 60 min and the contact angle was found to be almost constant ( # ^* .„ . « # ^* .„„ . « 81°) in the absence of optical illumination. The contact angle starts to decrease after the onset of illumination at t = 90 min and finally approaches θ _{η t=mmin} = 76°. Visible light absorbance data of a PI 49 dye-sensitized TiO? surface and a Chlorin dye-sensitized TiO surface

Two different dye-sensitized Ti0 ₂ surfaces were fabricated utilizing D149 dye and Chlorin dye. Adsorption of D149 dye molecules leads to a light-red coloration of the surface (see inset (i) in FIG. 13). A Chlroin dye sensitized Ti0 ₂ surface exhibits light-green color (see inset (ii) in FIG. 13). FIG. 13 shows the absorption spectra of a D149 dye-sensitized Ti0 ₂ surface and a Chlorin dye-sensitized Ti0 ₂ surface. It is evident that both surfaces absorb a broad range of visible spectrum (390 nm < λ < 700 nm).

Measured voltages between the contacting liquid droplets and dye-sensitized TiO surfaces

The in-situ voltages established were measured across the contacting liquids and the dye- sensitized Ti0 ₂ surfaces. Here four different ionic aqueous droplets (K ₂ S ₂ O ₃ , KI, KBr and KCl, all concentrations are 10 wt% in water) were used as probe contacting liquids.

(i) N3 dye-sensitized T1O2 surface: FIG. 14A shows the measured voltages across the contacting liquids (K ₂ S ₂ O ₃ and KBr) and the N3 dye-sensitized Ti0 ₂ surface while illuminating with visible light. The intensity of visible light is 145 mW/cm ² for all measurements.

Immediately after the onset of illumination, a potential difference (J¾¾o _{3; t} =o= 0.43 V and VKB _{Y, t} =o = 0.41 V) is observed. While the voltage gradually decreases between the K ₂ S ₂ O ₃ droplet and the surface over time, a rapid decrease in the voltage was observed between the KBr droplet and the surface. This is because bromide (Br ^" ) cannot effectively reduce the oxidized N3 dye as its reduction potential is higher (more positive) than the HOMO energy level of the N3 dye. The measured voltages between the K ₂ S ₂ O ₃ droplet and ITO match well with equation (1) with ¾ = 271 sec and a = 0.45 (see FIG. 14A and Table 2). The measured voltages between the KBr droplet and the surface can be well described with r _d = 20.6 sec and a = 0.76 (see FIG. 14A).

(ii) D149 dye-sensitized T1O2 surface: FIG. 14B shows the measured in-situ voltages between the contacting liquids and the D 149 dye-sensitized Ti0 ₂ surface. After a potential difference {V _t =o~ 0.355 V) is established for all contacting liquids upon the onset of optical illumination, a gradual decrease in the voltage is observed for K ₂ S ₂ O ₃ , KI and KBr. It is noteworthy that the KBr droplet exhibited a prolonged voltage difference on a D 149 dye- sensitized Ti0 ₂ surface in contrast to a rapid decrease on an N3 dye-sensitized Ti0 ₂ surface (see FIG. 14A). This is because the HOMO energy level of a D149 dye is lower (less positive) than the reduction potential of bromide which allows for regeneration process of oxidized D149 dye ² . In contrast, the measured voltage between the KCl droplet and the surface decreases rapidly and reaches zero within a minute of illumination. As expected, this is because the reduction potential of chloride is higher (more positive) than the HOMO energy level of D 149 dye which hinders effective regeneration of oxidized dye). Equation (1) describes the measured voltages well with various values of ¾ and a (see Table 2).

(Hi) Chlorin dye-sensitized Ti0 ₂ surface: FIG. 14C shows the measured in-situ voltages across the contacting liquids and the Chlorin dye-sensitized Ti0 ₂ surface. As the HOMO energy level of a Chlorin dye is higher (more positive) than the reduction potential of all contacting liquids (K2S2O3, KI, KBr and KCl), voltages for all contacting liquid droplets decrease gradually with increasing illumination time. This leads to spreading of all contacting liquids including KCl droplets (FIG. 8C).

Table 2 lists the values of ¾ and a found in the voltage predictions using the fractional RC circuit model.

Table 2. The values of ¾ and a found in the voltage predictions using the fractional RC circuit

KC1 50.7±11.6 0.41±0.049

Measured contact angles for K?S?Oi and KBr droplets on an N3 dye-sensitized TiO? surface under visible light illumination

The in-situ contact angles were measured for two liquid droplets: K ₂ S ₂ O ₃ and KBr (10 wt% in water) on an N3 dye-sensitized T1O ₂ surface. FIG. 15 shows the evolution in the macroscopic contact angles for K ₂ S ₂ 0 ₃ and KBr droplets as a function of illumination time (intensity = 145 mW/cm ² ). The contact angles for K ₂ S ₂ O ₃ decrease from θ ^* ₌₀ = 119° with increasing illumination time before it approaches # ^* _=120min = 77° while those for KBr remain almost constant during illumination ( ΑΘ ^* « 2° where ΑΘ ^* = θ ^* ₌₀ - θ ^* _=ηθΏάη ).

Other embodiments are within the scope of the following claims.