Fabrication of Coatings with Structural Color on a Wood Surface

: A facile method for the fabrication of colloidal photonic crystal coatings with tunable structural color on a wood surface was presented. The photonic crystal coatings were formed from monodisperse latex spheres composed of poly(styrene-methyl methacrylate-acrylic acid) (P(St-MMA-AA)). The latex spheres with a hard PSt core and elastomeric P(MMA-AA) shell were prepared using the emulsion polymerization method. The sessile drop method, a rapid single-step self-assembly method through simple evaporation of emulsion, was used to form three-dimensional colloidal crystals. Coatings with brilliant colors and uniform Bragg’s di ﬀ raction covering the entire visible region were fabricated by controlling the sphere size. This simple method provided new insight into the development of wood color embellishment. UV-Vis spectra of each type of were tested twice. The photographs of the woodblocks were recorded using a digital camera. The photos were acquired under natural light.


Introduction
Research shows that colors can easily be divided into two types: pigmentary colors and structural colors, depending on the origin of the colors. In the field of wood processing, the main strategy for coloring wood is by attaching dyes or pigments onto wood cells, which can be referred to as the pigmentation process. In outdoor applications, wood is usually colored by applying pigmented coatings and then painted for protection. The dyes for interior wood can be classified in the following common categories: direct dyes, basic dyes, acid dyes, and reactive dyes. The change of wood color is the result of dyes and pigments reforming the absorb and reflect wavelengths of visible light [1,2]. In the traditional coloring wood process, liquid waste containing pigments and dyes will cause water and soil pollution, and the colors easily fade away with time.
Structural colors present on the surface of periodic photonic crystals by the coherent diffraction of reflected light [3]. It is one of the distinguishing features of opals and inverse opal photonic crystals, which show high brightness, high saturation, and iridescence [4]. These materials have three-dimensional periodic structures and form the photonic band gaps (PBGs), where propagation of a certain range of electromagnetic wavelengths is forbidden [5]. The PBGs result from multiple scattering and Bragg's diffractions of light by the periodic photonic crystals [6]. Lots of colors can be observed by adjusting the structure of the photonic crystals and the viewing angle [7]. As structural color originates from interference, diffraction, or scattering of visible light in the periodic structures [8], it can be used to change the dyeing and mimic the beauty often observed in nature, such as on the surface of the scarab and the wings of morphos. Moreover, the coloration mechanism is relatively different from dyes and pigments.
Among the artificial constructive approaches, many researchers have focused on long-term, intensive strategies to synthesize monodisperse colloidal latex spheres for building photonic crystal (1 g), AA (1 g), distilled water (100 g), SDBS (0-0.02 g), and ammonium bicarbonate (0.5 g) were added sequentially to a three-necked, round-bottomed flask equipped with a reflux condenser, thermometer, and a mechanical stirrer at a stirring speed of 200 rpm. The reaction was carried out initially at 70 • C for 30 min. The mixture turned to milky white by intensive mixing. Then the initiator APS was added to the reaction system. After the addition of an aqueous solution of APS (0.48 g dissolved in 15 g water), copolymerization was carried out for a further 6-10 h while stirring at 400 rpm. The copolymerization time was different for different SDBS contents. The resulting latex spheres were washed 3 times with water, centrifuged at 13,400 rpm, and ultrasonically dispersed, maintaining a concentration of 10 wt.%.

Fabrication of the Colloidal Crystal Coatings
The sessile drop method was used to fabricate the photonic crystal coatings. The poplar wood samples used for the coatings were sanded with abrasive paper (320#). Before being used for coating, the wood samples were rinsed with distilled water and then dried at 101 • C in an oven to remove the water absorbed from the surface. The moisture content of the wood samples used for coating was about 10%. The emulsions of monodisperse P(St-MMA-AA) latex spheres, synthesized using different amounts of SDBS, were dripped onto the surface of the wood. The concentration of the emulsions was 10 wt.%. The emulsions were dispersed using the ultrasonic technique for 30 min before dripping. The coated woodblocks were dried at 50 • C in an air-dry oven until the coatings dried completely. To compare the visible light reflections of the coatings formed by different emulsion amounts per unit area, the dropping quantities of emulsion were set as 110, 88, 66, 44, and 22 µL/cm 2 .

Characterization
The intensity-average hydrodynamic sizes of the latex spheres in the emulsion were measured using dynamic light scattering (DLS) measurements with a particle size analyzer (Zetasizer Nano ZS, Malvern, UK). This technique measures the diffusion of spheres moving under Brownian motion and converts this to size and a size distribution using the Stokes-Einstein relationship. The instrument provided a constant temperature at 25 • C during the test. The dispersant of spheres for the test was water, and the concentration of the emulsion was a 1 wt.%. The morphologies of the latex spheres were characterized by transmission electron microscopy (TEM, JEM1400 and JEM2100 UHR, JEOL, Tokyo, Japan). To determine the diameters of the monodisperse latex spheres in the TEM image, we measured the sizes of over 200 spheres using Image J software (versions 1.52a). In the sample preparation stage, the diluted emulsion was dripped onto the copper mesh and dried under the light. The copper mesh loaded with the spheres was fed into the test system by a sample rod. The TEM images were taken from multiple holes in a copper mesh. Scanning electron microscopic (SEM) images were obtained with a tabletop microscope (TM4000Plus, HITACHI, Tokyo, Japan). The wood samples with coatings adhered to the sample stage. After sputter coating with a thin layer of gold, the samples were placed in the sample storehouse. During the testing process, the sample chamber was guaranteed to have a certain degree of vacuum. Fourier transform infrared spectroscopic (FTIR) analysis was carried out using a Vertex 80V (Bruker, Bremen, Germany) to identify the functional groups present in the colloidal crystal coatings using ATR-FTIR. The wood samples were pressed closely with the ATR crystal. The infrared beam attenuated and reflected in the ATR crystal and reached the detector. The UV-Vis spectra were obtained using a UV-Vis spectrometer (Lambda 950, Perkin-Elmer, Waltham, MA, USA) with a 150 mm integrating sphere accessory. The background material used in the scan was barium sulfate. The wavelength range was set as 350 to 750 nm. The infrared spectra and UV-Vis spectra of each type of coating were tested twice. The photographs of the woodblocks were recorded using a digital camera. The photos were acquired under natural light.

Monodisperse Core-Shell Latex Spheres
Monodisperse latex spheres of P(St-MMA-AA) were prepared by single-step emulsion polymerization. The mechanism of nucleation of the latex spheres could be considered to be homogeneous nucleation [31][32][33]. A latex sphere with a hydrophobic polystyrene core and hydrophilic P(MMA-AA) shell was synthesized [34], as shown in Figure 1. The concentration of the emulsion for this image was 0.6%. The polystyrene (dark part) was surrounded by P(MMA-AA) (light part). The spherical form showed the dependence of particle morphology on the MMA-AA/St ratio. The intensity-average hydrodynamic diameters of the spheres were 295.03, 289.66, 278. 33, 278.15, and 258.96 nm when the SDBS in the emulsion polymerization system was 0, 0.005, 0.01, 0.015 g, and 0.02 g. The measured diameters from the TEM results were 285, 254, 230, 223, and 193 nm. These results illustrated that the diameters of spheres could be controlled by changing the amount of emulsifier in the polymerization system. The diameters measured with TEM were slightly smaller than the hydrodynamic diameters measured by DLS, similar to Tang et al. [11] and Ríos-Osuna et al. [27]. This phenomenon could be explained by the weak aggregation of the spheres and water loss shrinkage of the shell of spheres. In Figure 1, the diameter of the latex sphere was about 285 nm and the thickness of the shell part, formed from P(MMA-AA) with abundant COOH groups, was about 45-50 nm. The hydrophilicity of the co-monomer was the main parameter that influenced the morphology of the latex sphere. The outermost shell of the sphere was different from its core, wherein it was enriched with polar groups due to some degree of phase separation [35]. According to the literature, a significant decrease in the size of latex spheres after sample drying was observed when compared to the swollen and hydrated form in an aqueous medium. It was proposed that the change in size was primarily due to the evaporation of water from the PMMA and PAA rich peripheries of the spheres. Meanwhile, the spherical shape was effectively perceived to be the result of a dense PSt rich core.
Coatings 2019, 9, x FOR PEER REVIEW 4 of 12 homogeneous nucleation [31][32][33]. A latex sphere with a hydrophobic polystyrene core and hydrophilic P(MMA-AA) shell was synthesized [34], as shown in Figure 1. The concentration of the emulsion for this image was 0.6%. The polystyrene (dark part) was surrounded by P(MMA-AA) (light part). The spherical form showed the dependence of particle morphology on the MMA-AA/St ratio.  [11] and Ríos-Osuna et al. [27]. This phenomenon could be explained by the weak aggregation of the spheres and water loss shrinkage of the shell of spheres. In Figure 1, the diameter of the latex sphere was about 285 nm and the thickness of the shell part, formed from P(MMA-AA) with abundant COOH groups, was about 45-50 nm. The hydrophilicity of the co-monomer was the main parameter that influenced the morphology of the latex sphere. The outermost shell of the sphere was different from its core, wherein it was enriched with polar groups due to some degree of phase separation [35]. According to the literature, a significant decrease in the size of latex spheres after sample drying was observed when compared to the swollen and hydrated form in an aqueous medium. It was proposed that the change in size was primarily due to the evaporation of water from the PMMA and PAA rich peripheries of the spheres. Meanwhile, the spherical shape was effectively perceived to be the result of a dense PSt rich core. The TEM image ( Figure 2) of the two-dimensional array formed from a 5% emulsion of the sample suggested that there was an adhesive interaction at the inter-particle contact points. These latex spheres were aligned in two-dimensional long arrays on the copper mesh. The introduction of the soft monomer P(MMA-AA) increased the flexibility and facilitated the relaxation of the resulting polymer segments, owing to its high mobility. A more concentrated array of latex spheres demonstrated a marked difference in the spherical shape. These spheres dried and came into closer contact with each other. They spontaneously adopted this arrangement mode due to the uniform spherical shape and the flexibility and adhesiveness of soft interfaces of the shell. This adhesive between microspheres could be due to the network of the polymer during the evaporation of water. Figure 3 shows variations in the core and shell morphologies of spheres when more spheres were present, similar to McGrath et al. [35]. The shape became less spherical where the edges became conjoined as the spheres were forced together into a dense array, as shown by the red line. This result demonstrated the inter-particle adhesion between conjoint parts due to the hydrophilic PAA peripheries. Some spheres assembled in such a way that not only the shells but also the cores of the spheres were connected, as shown by the green line. Figure 3b,c shows the high resolution TEM image of the inter-particle contact points. This result also indicated a strong adhesive force between the latex spheres and contributed to the well-ordered arrangement of the latex spheres. The TEM image (Figure 2) of the two-dimensional array formed from a 5% emulsion of the sample suggested that there was an adhesive interaction at the inter-particle contact points. These latex spheres were aligned in two-dimensional long arrays on the copper mesh. The introduction of the soft monomer P(MMA-AA) increased the flexibility and facilitated the relaxation of the resulting polymer segments, owing to its high mobility. A more concentrated array of latex spheres demonstrated a marked difference in the spherical shape. These spheres dried and came into closer contact with each other. They spontaneously adopted this arrangement mode due to the uniform spherical shape and the flexibility and adhesiveness of soft interfaces of the shell. This adhesive between microspheres could be due to the network of the polymer during the evaporation of water. Figure 3 shows variations in the core and shell morphologies of spheres when more spheres were present, similar to McGrath et al. [35]. The shape became less spherical where the edges became conjoined as the spheres were forced together into a dense array, as shown by the red line. This result demonstrated the inter-particle adhesion between conjoint parts due to the hydrophilic PAA peripheries. Some spheres assembled in such a way that not only the shells but also the cores of the spheres were connected, as shown by the green line. Figure 3b,c shows the high resolution TEM image of the inter-particle contact points. This result also indicated a strong adhesive force between the latex spheres and contributed to the well-ordered arrangement of the latex spheres.

Fabrication of Colloidal Crystal Structure
To obtain photonic crystals, we arranged the monodisperse core-shell latex spheres into a crystalline lattice. The sessile drop method was used for the coating of 3-D colloidal crystals onto the wood surface. The emulsion was coated on the surface of the wood substrate using a dropper. Since the raw wood was made of cells that possessed hierarchical microstructures [36], the main components of wood were cellulose, hemicellulose and lignin, which has many hydrophilic groups. The latex spheres self-assembled on the wood mainly through capillary force [16] and inter-particle forces when the water evaporated. The spheres filled the cell structure, then fabricated a well-ordered crystal structure. In this process, the soft shell-hard core morphology of latex spheres promoted the formation of a colloidal crystal, and the soft shell facilitated assembly of the latex spheres and the hard core enhanced crystalline stability [37]. Figure 4 presents a top-view SEM image of 3-D colloidal crystals on the wood surface, assembled by monodisperse latex spheres with diameters of about 230 nm. It was evident that the majority of the microspheres formed a hexagonal structure and demonstrated long-range organized structures. The structure with cubic close-packed {111} planes was oriented parallel to the substrate [38], with each sphere touching six others in one layer. As seen in Figure 5, the drying process in an air-dry oven resulted in the formation of cracks. The cracks are frequently observed in colloidal crystals fabricated with the rapid evaporation of the dispersant. The latex spheres shrunk during the assembly process. There was a difference in shrinkage between the wood and microspheres. Drying resulted in contraction that did not occur in the woodblocks. This could only be accompanied by the formation of cracks, which did not greatly impact the optical properties of the colloidal crystal structure. Figure  6 shows the cross-sectional SEM image of a 3-D colloidal crystal. The P(St-MMA-AA) spheres were arranged as typical {100} facets of the fcc lattice. There was continuous air space between the arranged latex spheres, which demonstrated a typical feature of polymer-air bicontinuous fcc structures [39]. The 3-D uniformity of the colloidal crystals coating indicated the adhesion between latex spheres.

Fabrication of Colloidal Crystal Structure
To obtain photonic crystals, we arranged the monodisperse core-shell latex spheres into a crystalline lattice. The sessile drop method was used for the coating of 3-D colloidal crystals onto the wood surface. The emulsion was coated on the surface of the wood substrate using a dropper. Since the raw wood was made of cells that possessed hierarchical microstructures [36], the main components of wood were cellulose, hemicellulose and lignin, which has many hydrophilic groups. The latex spheres self-assembled on the wood mainly through capillary force [16] and inter-particle forces when the water evaporated. The spheres filled the cell structure, then fabricated a well-ordered crystal structure. In this process, the soft shell-hard core morphology of latex spheres promoted the formation of a colloidal crystal, and the soft shell facilitated assembly of the latex spheres and the hard core enhanced crystalline stability [37]. Figure 4 presents a top-view SEM image of 3-D colloidal crystals on the wood surface, assembled by monodisperse latex spheres with diameters of about 230 nm. It was evident that the majority of the microspheres formed a hexagonal structure and demonstrated long-range organized structures. The structure with cubic close-packed {111} planes was oriented parallel to the substrate [38], with each sphere touching six others in one layer. As seen in Figure 5, the drying process in an air-dry oven resulted in the formation of cracks. The cracks are frequently observed in colloidal crystals fabricated with the rapid evaporation of the dispersant. The latex spheres shrunk during the assembly process. There was a difference in shrinkage between the wood and microspheres. Drying resulted in contraction that did not occur in the woodblocks. This could only be accompanied by the formation of cracks, which did not greatly impact the optical properties of the colloidal crystal structure. Figure  6 shows the cross-sectional SEM image of a 3-D colloidal crystal. The P(St-MMA-AA) spheres were arranged as typical {100} facets of the fcc lattice. There was continuous air space between the arranged latex spheres, which demonstrated a typical feature of polymer-air bicontinuous fcc structures [39]. The 3-D uniformity of the colloidal crystals coating indicated the adhesion between latex spheres.

Fabrication of Colloidal Crystal Structure
To obtain photonic crystals, we arranged the monodisperse core-shell latex spheres into a crystalline lattice. The sessile drop method was used for the coating of 3-D colloidal crystals onto the wood surface. The emulsion was coated on the surface of the wood substrate using a dropper. Since the raw wood was made of cells that possessed hierarchical microstructures [36], the main components of wood were cellulose, hemicellulose and lignin, which has many hydrophilic groups. The latex spheres self-assembled on the wood mainly through capillary force [16] and inter-particle forces when the water evaporated. The spheres filled the cell structure, then fabricated a well-ordered crystal structure. In this process, the soft shell-hard core morphology of latex spheres promoted the formation of a colloidal crystal, and the soft shell facilitated assembly of the latex spheres and the hard core enhanced crystalline stability [37]. Figure 4 presents a top-view SEM image of 3-D colloidal crystals on the wood surface, assembled by monodisperse latex spheres with diameters of about 230 nm. It was evident that the majority of the microspheres formed a hexagonal structure and demonstrated long-range organized structures. The structure with cubic close-packed {111} planes was oriented parallel to the substrate [38], with each sphere touching six others in one layer. As seen in Figure 5, the drying process in an air-dry oven resulted in the formation of cracks. The cracks are frequently observed in colloidal crystals fabricated with the rapid evaporation of the dispersant. The latex spheres shrunk during the assembly process. There was a difference in shrinkage between the wood and microspheres. Drying resulted in contraction that did not occur in the woodblocks. This could only be accompanied by the formation of cracks, which did not greatly impact the optical properties of the colloidal crystal structure. Figure 6 shows the cross-sectional SEM image of a 3-D colloidal crystal. The P(St-MMA-AA) spheres were arranged as typical {100} facets of the fcc lattice. There was continuous air space between the arranged latex spheres, which demonstrated a typical feature of polymer-air bicontinuous fcc structures [39]. The 3-D uniformity of the colloidal crystals coating indicated the adhesion between latex spheres.    The order of colloidal crystal coatings may be due to the arrangement of the latex spheres by the interface and gravity joint self-assembly during dispersant evaporation. When the latex spheres assembled into a well-ordered crystal structure in the oven, there were three kinds of forces acting on the latex spheres. P(St-MMA-AA) latex spheres suspended in water before self-assembly, then a part of the spheres moved up to the air-liquid interface. The components of the spheres shell are PAA equipped with an abundant number of COOH groups and exhibited hydrophilicity which promoted the generation of hydrogen bonds. The hydrogen bonding interaction increased the bonding between the latex spheres and accelerated the process of self-assembly. Driven by capillary force and convection force, on the air-liquid interface, the initial colloidal crystals grow on the first layer.
Meanwhile, the hydrophilic P(MMA-AA) shell merged into a continuous matrix in an aqueous system. The shell part of the latex spheres assisted self-assembly of the particles in forming a closepacked ordered structure [35]. Then the latex spheres in the emulsion are assembled layer-by-layer to the first layer, which acts as a seed. At the same time, part of the sphere's sediment in the cell cavity of the wood surface under the action of gravity. The monodispersity of the spheres maintained the well-ordered arrangement during the fabrication of the photonic crystals [40]. Meanwhile, the hard and hydrophobic cores maintained the crystalline order structure [40,41]. These factors accelerated the arrangement of well-ordered latex spheres and contributed to the homogeneous colloidal photonic crystals on the wood surface.
The orderly structure of colloidal crystal coatings could be attributed to the elastomeric deformation of the P(MMA-AA) shell and the hydrogen bonding interactions between the carboxyl groups at the surface of the latex spheres. FTIR spectroscopic analysis helped to determine the functional groups and clarified the role of hydrogen bonds between the carboxyl groups on the shell    The order of colloidal crystal coatings may be due to the arrangement of the latex spheres by the interface and gravity joint self-assembly during dispersant evaporation. When the latex spheres assembled into a well-ordered crystal structure in the oven, there were three kinds of forces acting on the latex spheres. P(St-MMA-AA) latex spheres suspended in water before self-assembly, then a part of the spheres moved up to the air-liquid interface. The components of the spheres shell are PAA equipped with an abundant number of COOH groups and exhibited hydrophilicity which promoted the generation of hydrogen bonds. The hydrogen bonding interaction increased the bonding between the latex spheres and accelerated the process of self-assembly. Driven by capillary force and convection force, on the air-liquid interface, the initial colloidal crystals grow on the first layer.
Meanwhile, the hydrophilic P(MMA-AA) shell merged into a continuous matrix in an aqueous system. The shell part of the latex spheres assisted self-assembly of the particles in forming a closepacked ordered structure [35]. Then the latex spheres in the emulsion are assembled layer-by-layer to the first layer, which acts as a seed. At the same time, part of the sphere's sediment in the cell cavity of the wood surface under the action of gravity. The monodispersity of the spheres maintained the well-ordered arrangement during the fabrication of the photonic crystals [40]. Meanwhile, the hard and hydrophobic cores maintained the crystalline order structure [40,41]. These factors accelerated the arrangement of well-ordered latex spheres and contributed to the homogeneous colloidal photonic crystals on the wood surface.
The orderly structure of colloidal crystal coatings could be attributed to the elastomeric deformation of the P(MMA-AA) shell and the hydrogen bonding interactions between the carboxyl groups at the surface of the latex spheres. FTIR spectroscopic analysis helped to determine the functional groups and clarified the role of hydrogen bonds between the carboxyl groups on the shell     The order of colloidal crystal coatings may be due to the arrangement of the latex spheres by the interface and gravity joint self-assembly during dispersant evaporation. When the latex spheres assembled into a well-ordered crystal structure in the oven, there were three kinds of forces acting on the latex spheres. P(St-MMA-AA) latex spheres suspended in water before self-assembly, then a part of the spheres moved up to the air-liquid interface. The components of the spheres shell are PAA equipped with an abundant number of COOH groups and exhibited hydrophilicity which promoted the generation of hydrogen bonds. The hydrogen bonding interaction increased the bonding between the latex spheres and accelerated the process of self-assembly. Driven by capillary force and convection force, on the air-liquid interface, the initial colloidal crystals grow on the first layer.
Meanwhile, the hydrophilic P(MMA-AA) shell merged into a continuous matrix in an aqueous system. The shell part of the latex spheres assisted self-assembly of the particles in forming a closepacked ordered structure [35]. Then the latex spheres in the emulsion are assembled layer-by-layer to the first layer, which acts as a seed. At the same time, part of the sphere's sediment in the cell cavity of the wood surface under the action of gravity. The monodispersity of the spheres maintained the well-ordered arrangement during the fabrication of the photonic crystals [40]. Meanwhile, the hard and hydrophobic cores maintained the crystalline order structure [40,41]. These factors accelerated the arrangement of well-ordered latex spheres and contributed to the homogeneous colloidal photonic crystals on the wood surface.
The orderly structure of colloidal crystal coatings could be attributed to the elastomeric deformation of the P(MMA-AA) shell and the hydrogen bonding interactions between the carboxyl groups at the surface of the latex spheres. FTIR spectroscopic analysis helped to determine the functional groups and clarified the role of hydrogen bonds between the carboxyl groups on the shell The order of colloidal crystal coatings may be due to the arrangement of the latex spheres by the interface and gravity joint self-assembly during dispersant evaporation. When the latex spheres assembled into a well-ordered crystal structure in the oven, there were three kinds of forces acting on the latex spheres. P(St-MMA-AA) latex spheres suspended in water before self-assembly, then a part of the spheres moved up to the air-liquid interface. The components of the spheres shell are PAA equipped with an abundant number of COOH groups and exhibited hydrophilicity which promoted the generation of hydrogen bonds. The hydrogen bonding interaction increased the bonding between the latex spheres and accelerated the process of self-assembly. Driven by capillary force and convection force, on the air-liquid interface, the initial colloidal crystals grow on the first layer.
Meanwhile, the hydrophilic P(MMA-AA) shell merged into a continuous matrix in an aqueous system. The shell part of the latex spheres assisted self-assembly of the particles in forming a close-packed ordered structure [35]. Then the latex spheres in the emulsion are assembled layer-by-layer to the first layer, which acts as a seed. At the same time, part of the sphere's sediment in the cell cavity of the wood surface under the action of gravity. The monodispersity of the spheres maintained the well-ordered arrangement during the fabrication of the photonic crystals [40]. Meanwhile, the hard and hydrophobic cores maintained the crystalline order structure [40,41]. These factors accelerated the arrangement of well-ordered latex spheres and contributed to the homogeneous colloidal photonic crystals on the wood surface.
The orderly structure of colloidal crystal coatings could be attributed to the elastomeric deformation of the P(MMA-AA) shell and the hydrogen bonding interactions between the carboxyl groups at the surface of the latex spheres. FTIR spectroscopic analysis helped to determine the functional groups and clarified the role of hydrogen bonds between the carboxyl groups on the shell of the latex spheres. The results are presented in Figure 7. The absorbance peak at 1729 cm −1 was ascribed to the hydrophilic C=O groups of PAA, whereas the absorbance peaks at 1600, 756, and 701 cm −1 were ascribed to the hydrophobic benzene groups of PSt [8]. Absorption peaks in the spectra of all coatings at 3647, 3442, and 620 cm −1 could be ascribed to the vibrations of the O-H groups. The peaks at around 3025 cm −1 were characteristic of C-H in benzene. Peaks at around 2922 cm −1 corresponded to the C-H stretching vibration absorption of -CH 3 and -CH 2 -, and 1492 and 1450 cm −1 corresponded to the C-H bending vibration peak in -CH 2 -. Thus, the formation of the core-shell morphology of the materials in the microspheres was confirmed by FTIR spectroscopy.
Coatings 2019, 9, x FOR PEER REVIEW 7 of 12 of the latex spheres. The results are presented in Figure 7. The absorbance peak at 1729 cm -1 was ascribed to the hydrophilic C=O groups of PAA, whereas the absorbance peaks at 1600, 756, and 701 cm -1 were ascribed to the hydrophobic benzene groups of PSt [8]. Absorption peaks in the spectra of all coatings at 3647, 3442, and 620 cm -1 could be ascribed to the vibrations of the O-H groups. The peaks at around 3025 cm -1 were characteristic of C-H in benzene. Peaks at around 2922 cm -1 corresponded to the C-H stretching vibration absorption of -CH₃ and -CH2-, and 1492 and 1450 cm -1 corresponded to the C-H bending vibration peak in -CH2-. Thus, the formation of the core-shell morphology of the materials in the microspheres was confirmed by FTIR spectroscopy.

Full Color Colloidal Crystal Coatings
When photonic crystals are used as surface finishing materials, the coatings exhibit brilliant colors [41,42] due to the stop bands laying in the visible region. In this work, red, yellow, green, cyan, and violet photonic crystal coatings were prepared on the wood surface using P(St-MMA-AA) latex spheres with diameters of 285, 254, 230, 223, and 193 nm measured using the TEM image, respectively. The color was consistent throughout the woodblock surface due to the well-ordered arrangement of spheres. The diameter modulation of the monodisperse latex spheres was variated by altering the ratio of emulsifier (SDBS) in the emulsion polymerization process. The emulsifier SDBS was distributed around the surface of the latex spheres, which ensured the formation of a stable emulsion system. Figure 8 shows a photograph of the coatings deposited on the wood surface. The amount of drop per square centimeter was 110 μL. The area of the coating was ca. 2 × 2 cm 2 and could be modulated with the size of the substrate. The brilliant structural colors of the coatings showed dependence on the viewing angle. The specific dimensions of latex spheres ensured that the stop band of the as-prepared photonic crystal coating covered the entire visible range. The colors resulted from the diffraction/reflectance of light from the colloidal photonic crystal as visualized by SEM (Figure 4). Relative reflectance spectroscopy was used to determine the wavelength of the Bragg's diffraction for the colloidal photonic crystal. The solid UV-Vis spectra could measure the surface of well-ordered photonic crystal

Full Color Colloidal Crystal Coatings
When photonic crystals are used as surface finishing materials, the coatings exhibit brilliant colors [41,42] due to the stop bands laying in the visible region. In this work, red, yellow, green, cyan, and violet photonic crystal coatings were prepared on the wood surface using P(St-MMA-AA) latex spheres with diameters of 285, 254, 230, 223, and 193 nm measured using the TEM image, respectively. The color was consistent throughout the woodblock surface due to the well-ordered arrangement of spheres. The diameter modulation of the monodisperse latex spheres was variated by altering the ratio of emulsifier (SDBS) in the emulsion polymerization process. The emulsifier SDBS was distributed around the surface of the latex spheres, which ensured the formation of a stable emulsion system. Figure 8 shows a photograph of the coatings deposited on the wood surface. The amount of drop per square centimeter was 110 µL. The area of the coating was ca. 2 × 2 cm 2 and could be modulated with the size of the substrate. The brilliant structural colors of the coatings showed dependence on the viewing angle. of the latex spheres. The results are presented in Figure 7. The absorbance peak at 1729 cm -1 was ascribed to the hydrophilic C=O groups of PAA, whereas the absorbance peaks at 1600, 756, and 701 cm -1 were ascribed to the hydrophobic benzene groups of PSt [8]. Absorption peaks in the spectra of all coatings at 3647, 3442, and 620 cm -1 could be ascribed to the vibrations of the O-H groups. The peaks at around 3025 cm -1 were characteristic of C-H in benzene. Peaks at around 2922 cm -1 corresponded to the C-H stretching vibration absorption of -CH₃ and -CH2-, and 1492 and 1450 cm -1 corresponded to the C-H bending vibration peak in -CH2-. Thus, the formation of the core-shell morphology of the materials in the microspheres was confirmed by FTIR spectroscopy.

Full Color Colloidal Crystal Coatings
When photonic crystals are used as surface finishing materials, the coatings exhibit brilliant colors [41,42] due to the stop bands laying in the visible region. In this work, red, yellow, green, cyan, and violet photonic crystal coatings were prepared on the wood surface using P(St-MMA-AA) latex spheres with diameters of 285, 254, 230, 223, and 193 nm measured using the TEM image, respectively. The color was consistent throughout the woodblock surface due to the well-ordered arrangement of spheres. The diameter modulation of the monodisperse latex spheres was variated by altering the ratio of emulsifier (SDBS) in the emulsion polymerization process. The emulsifier SDBS was distributed around the surface of the latex spheres, which ensured the formation of a stable emulsion system. Figure 8 shows a photograph of the coatings deposited on the wood surface. The amount of drop per square centimeter was 110 μL. The area of the coating was ca. 2 × 2 cm 2 and could be modulated with the size of the substrate. The brilliant structural colors of the coatings showed dependence on the viewing angle. The specific dimensions of latex spheres ensured that the stop band of the as-prepared photonic crystal coating covered the entire visible range. The colors resulted from the diffraction/reflectance of light from the colloidal photonic crystal as visualized by SEM (Figure 4). Relative reflectance spectroscopy was used to determine the wavelength of the Bragg's diffraction for the colloidal photonic crystal. The solid UV-Vis spectra could measure the surface of well-ordered photonic crystal The specific dimensions of latex spheres ensured that the stop band of the as-prepared photonic crystal coating covered the entire visible range. The colors resulted from the diffraction/reflectance of light from the colloidal photonic crystal as visualized by SEM (Figure 4). Relative reflectance spectroscopy was used to determine the wavelength of the Bragg's diffraction for the colloidal photonic crystal. The solid UV-Vis spectra could measure the surface of well-ordered photonic crystal and monochromatic structural colors in reflectance mode (along the crystallographic {111} direction). As seen in Figure 9, a strong reflectance of coatings was observed. Peaks appeared at 621, 569, 514, 490, and 433 nm. These wavelengths were consistent with the colors shown in Figure 8. and monochromatic structural colors in reflectance mode (along the crystallographic {111} direction). As seen in Figure 9, a strong reflectance of coatings was observed. Peaks appeared at 621, 569, 514, 490, and 433 nm. These wavelengths were consistent with the colors shown in Figure 8. The spectra showed variations in the reflectance peaks with changes in the latex sphere sizes. Stop band positions were blue-shifted for spheres with smaller diameters packed with smaller lattice constants [43][44][45]. Thus, the sessile drop method was effective for the fabrication of the tunable photonic band gap and colloidal crystal structure on the wood surface. In the UV-Vis spectra of coatings composed of spheres of different diameters, the photonic crystals showed broad peaks and large backgrounds. This could be because the self-assembly of photonic crystals was influenced by the micron-scale tubular structures of the wood surface. The well-ordered structure was only present on the surface layer of the coatings. Colvin et al. reported that most of the radiations interacted only with a few lattice planes near the surface and there was no subsequent propagation through the photonic crystals [46]. Hence, the as-prepared photonic crystals demonstrated iridescent structural color (Figure 8).
In Figure 9, the curves of the red and yellow coatings showed a declining trend, whereas the curves of the green, cyan, and purple coatings showed an increasing trend in the wavelength range of 650 nm to 750 nm. These trends were due to the influence of the wood base which showed an upward trend in the visible light range. The coatings, except the purple one, were assembled by spheres with diameters of 193 nm which were measured by the TEM image. They showed reflection peaks at wavelengths of 396 (red), 403 (yellow), 397 (green), and 391 nm (cyan). Figure 10 shows the diffuse reflectance spectra of the dried latex spheres, which showed peaks at 396 (red), 403 (yellow), 393 (green), and 391 nm (cyan). Thus, peaks at about 395 nm in the UV-Vis spectra of coatings on the wood surface were the result of diffuse reflectance of P(St-MMA-AA) microspheres.  The spectra showed variations in the reflectance peaks with changes in the latex sphere sizes. Stop band positions were blue-shifted for spheres with smaller diameters packed with smaller lattice constants [43][44][45]. Thus, the sessile drop method was effective for the fabrication of the tunable photonic band gap and colloidal crystal structure on the wood surface. In the UV-Vis spectra of coatings composed of spheres of different diameters, the photonic crystals showed broad peaks and large backgrounds. This could be because the self-assembly of photonic crystals was influenced by the micron-scale tubular structures of the wood surface. The well-ordered structure was only present on the surface layer of the coatings. Colvin et al. reported that most of the radiations interacted only with a few lattice planes near the surface and there was no subsequent propagation through the photonic crystals [46]. Hence, the as-prepared photonic crystals demonstrated iridescent structural color ( Figure 8).
In Figure 9, the curves of the red and yellow coatings showed a declining trend, whereas the curves of the green, cyan, and purple coatings showed an increasing trend in the wavelength range of 650 nm to 750 nm. These trends were due to the influence of the wood base which showed an upward trend in the visible light range. The coatings, except the purple one, were assembled by spheres with diameters of 193 nm which were measured by the TEM image. They showed reflection peaks at wavelengths of 396 (red), 403 (yellow), 397 (green), and 391 nm (cyan). Figure 10 shows the diffuse reflectance spectra of the dried latex spheres, which showed peaks at 396 (red), 403 (yellow), 393 (green), and 391 nm (cyan). Thus, peaks at about 395 nm in the UV-Vis spectra of coatings on the wood surface were the result of diffuse reflectance of P(St-MMA-AA) microspheres. and monochromatic structural colors in reflectance mode (along the crystallographic {111} direction). As seen in Figure 9, a strong reflectance of coatings was observed. Peaks appeared at 621, 569, 514, 490, and 433 nm. These wavelengths were consistent with the colors shown in Figure 8. The spectra showed variations in the reflectance peaks with changes in the latex sphere sizes. Stop band positions were blue-shifted for spheres with smaller diameters packed with smaller lattice constants [43][44][45]. Thus, the sessile drop method was effective for the fabrication of the tunable photonic band gap and colloidal crystal structure on the wood surface. In the UV-Vis spectra of coatings composed of spheres of different diameters, the photonic crystals showed broad peaks and large backgrounds. This could be because the self-assembly of photonic crystals was influenced by the micron-scale tubular structures of the wood surface. The well-ordered structure was only present on the surface layer of the coatings. Colvin et al. reported that most of the radiations interacted only with a few lattice planes near the surface and there was no subsequent propagation through the photonic crystals [46]. Hence, the as-prepared photonic crystals demonstrated iridescent structural color ( Figure 8).
In Figure 9, the curves of the red and yellow coatings showed a declining trend, whereas the curves of the green, cyan, and purple coatings showed an increasing trend in the wavelength range of 650 nm to 750 nm. These trends were due to the influence of the wood base which showed an upward trend in the visible light range. The coatings, except the purple one, were assembled by spheres with diameters of 193 nm which were measured by the TEM image. They showed reflection peaks at wavelengths of 396 (red), 403 (yellow), 397 (green), and 391 nm (cyan). Figure 10 shows the diffuse reflectance spectra of the dried latex spheres, which showed peaks at 396 (red), 403 (yellow), 393 (green), and 391 nm (cyan). Thus, peaks at about 395 nm in the UV-Vis spectra of coatings on the wood surface were the result of diffuse reflectance of P(St-MMA-AA) microspheres.   We explained the influence of coating thickness on the structural color as the droplet quantity varied. Figure 11 shows the reflectance spectra of the coatings formed from the emulsions of different concentrations. The as-prepared photonic crystal coatings were formed from P(St-MMA-AA) latex spheres with diameters of 230 nm. The number of spheres for self-assembly on the wood surface varied with the volume of an emulsion having the same concentration. Coatings with different thicknesses could be constructed on the same area of the wood substrate with different quantities of drops. In the image, the intensity of the reflection peaks decreased as the drop amount decreased. This phenomenon indicated that as the number of latex spheres increased, coating thickness and more effective crystal structures with a long-range ordering of latex spheres appeared. Figure 12 shows the images of coatings with different thicknesses. The coatings showed uniform structural color and excellent reflectivity. Coatings formed from more latex spheres completely shaded the wood surface and exhibited a more complete and bright color. It was worth noting that the reflection peaks red-shifted when the droplet amount increased from 66 to 88 µL/cm 2 . The reflection peaks appeared at wavelengths of 508 nm (22,44 and 66 µL/cm 2 ) and 514 nm (88 and 110 µL/cm 2 ). This phenomenon could be attributed to the cellular structure of the wood surface. In Figure 12, the coatings formed from 22, 44 and 66 µL/cm 2 droplet amounts could still retain the texture of the wood cellular structure. When more drops were used to make coatings, the surface of coatings showed more distinct photonic crystal structures and cracks could be seen in the image. We explained the influence of coating thickness on the structural color as the droplet quantity varied. Figure 11 shows the reflectance spectra of the coatings formed from the emulsions of different concentrations. The as-prepared photonic crystal coatings were formed from P(St-MMA-AA) latex spheres with diameters of 230 nm. The number of spheres for self-assembly on the wood surface varied with the volume of an emulsion having the same concentration. Coatings with different thicknesses could be constructed on the same area of the wood substrate with different quantities of drops. In the image, the intensity of the reflection peaks decreased as the drop amount decreased. This phenomenon indicated that as the number of latex spheres increased, coating thickness and more effective crystal structures with a long-range ordering of latex spheres appeared. Figure 12 shows the images of coatings with different thicknesses. The coatings showed uniform structural color and excellent reflectivity. Coatings formed from more latex spheres completely shaded the wood surface and exhibited a more complete and bright color. It was worth noting that the reflection peaks red-shifted when the droplet amount increased from 66 to 88 μL/cm 2 . The reflection peaks appeared at wavelengths of 508 nm (22,44 and 66 μL/cm 2 ) and 514 nm (88 and 110 μL/cm 2 ). This phenomenon could be attributed to the cellular structure of the wood surface. In Figure 12, the coatings formed from 22, 44 and 66 μL/cm 2 droplet amounts could still retain the texture of the wood cellular structure. When more drops were used to make coatings, the surface of coatings showed more distinct photonic crystal structures and cracks could be seen in the image.

Conclusions
In conclusion, dried P(St-MMA-AA) colloidal crystal coatings were successfully fabricated on a wood surface using the sessile drop method. The colloidal crystal coatings were self-assembled from latex spheres with a core-shell structure using the emulsion evaporation method. Soft shells with an abundant number of COOH groups allowed for the ordering of spheres by introducing flexibility, whereas the hard core provided the final crystalline stability when fully dried. The dried coatings exhibited Bragg's diffraction and tunable brilliant and monochromatic structural colors covering the entire visible range. SEM and reflectance spectroscopy characterized the coatings and demonstrated the extent of the crystalline order. Variations in the number of latex spheres altered the integrity of We explained the influence of coating thickness on the structural color as the droplet quantity varied. Figure 11 shows the reflectance spectra of the coatings formed from the emulsions of different concentrations. The as-prepared photonic crystal coatings were formed from P(St-MMA-AA) latex spheres with diameters of 230 nm. The number of spheres for self-assembly on the wood surface varied with the volume of an emulsion having the same concentration. Coatings with different thicknesses could be constructed on the same area of the wood substrate with different quantities of drops. In the image, the intensity of the reflection peaks decreased as the drop amount decreased. This phenomenon indicated that as the number of latex spheres increased, coating thickness and more effective crystal structures with a long-range ordering of latex spheres appeared. Figure 12 shows the images of coatings with different thicknesses. The coatings showed uniform structural color and excellent reflectivity. Coatings formed from more latex spheres completely shaded the wood surface and exhibited a more complete and bright color. It was worth noting that the reflection peaks red-shifted when the droplet amount increased from 66 to 88 μL/cm 2 . The reflection peaks appeared at wavelengths of 508 nm (22,44 and 66 μL/cm 2 ) and 514 nm (88 and 110 μL/cm 2 ). This phenomenon could be attributed to the cellular structure of the wood surface. In Figure 12, the coatings formed from 22, 44 and 66 μL/cm 2 droplet amounts could still retain the texture of the wood cellular structure. When more drops were used to make coatings, the surface of coatings showed more distinct photonic crystal structures and cracks could be seen in the image.

Conclusions
In conclusion, dried P(St-MMA-AA) colloidal crystal coatings were successfully fabricated on a wood surface using the sessile drop method. The colloidal crystal coatings were self-assembled from latex spheres with a core-shell structure using the emulsion evaporation method. Soft shells with an abundant number of COOH groups allowed for the ordering of spheres by introducing flexibility, whereas the hard core provided the final crystalline stability when fully dried. The dried coatings exhibited Bragg's diffraction and tunable brilliant and monochromatic structural colors covering the entire visible range. SEM and reflectance spectroscopy characterized the coatings and demonstrated the extent of the crystalline order. Variations in the number of latex spheres altered the integrity of

Conclusions
In conclusion, dried P(St-MMA-AA) colloidal crystal coatings were successfully fabricated on a wood surface using the sessile drop method. The colloidal crystal coatings were self-assembled from latex spheres with a core-shell structure using the emulsion evaporation method. Soft shells with an abundant number of COOH groups allowed for the ordering of spheres by introducing flexibility, whereas the hard core provided the final crystalline stability when fully dried. The dried coatings exhibited Bragg's diffraction and tunable brilliant and monochromatic structural colors covering the entire visible range. SEM and reflectance spectroscopy characterized the coatings and demonstrated the extent of the crystalline order. Variations in the number of latex spheres altered the integrity of the coating and optical properties. The results provided new insights into the coloring of a wood surface. Such a rapid fabrication of self-assembly of structural color coatings with tunable photonic band gaps on wood is of great significance for wood surface coating and improved performance.
Author Contributions: Y.L. and J.H. contributed to the synthesis, testing, data analysis, and wrote the manuscript. Z.W. provided constructive suggestions about this work. All authors have read and agreed to the published version of the manuscript.
Funding: This research was funded by the Scientific Research Foundation of Nanjing Forestry University (GXL 2018022).