Satoru Tsukada*,
Masatsugu Doi,
Kan Nogami and
Katsuyoshi Hoshino
Department of Materials Science, Graduate School of Engineering, Chiba University, Inage-ku, Chiba 263-8522, Japan. E-mail: tsukada@chiba-u.jp
First published on 9th April 2025
Materials that exhibit metallic luster without containing metals are promising alternatives to existing metallic paints and coatings. In this study, we successfully synthesized four types of anion-doped poly(3-alkoxyselenophene) and used them to develop metal-free metal-like lustrous films. By employing polyselenophene, we achieved the expression of luxurious glossy colors such as black and purple, which were difficult to obtain with previously reported polythiophene-based materials. The developed films were thoroughly investigated through reflectance spectroscopy, colorimetry, gloss measurements, and XRD analysis. The glossy colors exhibited by the polyselenophene films are suggested to arise from a well-balanced presence of face-on and edge-on lamellar crystals within the coated films, in addition to the optical properties of the polymer itself. The developed metal-like lustrous films do not contain any metals, being highly promising for applications in essential everyday items such as writing instruments, cosmetics, anti-counterfeiting inks, and automotive paints.
The origin of luster in bulk metals is attributed to free electrons. At the same time, structural colors are produced by the reflection of light from periodic microstructures commonly observed in insects and birds.1,2 Metallic luster paints containing metallic flakes, such as aluminum and zinc, are commonly used in everyday life.3,4 The size of these flakes varies from a few to several tens of micrometers, with thicknesses ranging from less than 0.1 to 1 μm, facilitating the creation of attractive luster colors.3,4 However, the use of metal flakes exhibits certain drawbacks, including susceptibility to corrosion, color migration, increased weight of the paint, and electromagnetic shielding issues.3–5 Additionally, metal flakes can contribute to environmental pollution.4,6–8
The development of metal-free organic materials to create a metallic luster is highly promising in the field such as plating and polymers.9–29 Compounds such as pyrrole,11–16 polyaniline,17,21 porphyrin,23,30 azobenzene,18,20,21,24,29,31,32 stilbene,25 polyacetylene,10,26 diarylethene,27 and indole squaraine28 derivatives have been reported to exhibit such luster. Furthermore, some of these compounds can change their gloss color when exposed to external stimuli,27,29,31 while others are soluble in solvents, allowing the preparation of films. However, it is important to note that most of these compounds develop their gloss color in the bulk or crystalline state.
We previously demonstrated a coating film of an anion-doped poly(3-alkoxythiophene), synthesized via chemical oxidative polymerization, exhibiting a metal-like luster similar to gold and copper luster.33–42 Such polythiophenes can be easily prepared as a coating solution using solvents with high polarity and afford metal-like luster films. Furthermore, films prepared via electrochemical polymerization also exhibit a gold-like luster.43,44 Previous studies revealed that the existence of highly dense edge-on lamellar crystals causes a high refractive index and extinction coefficient, thus affording a metal-like luster. The development of materials with a higher reflectance that exhibit various luster colors is important for scientific research and practical applications.
So far, only thiophene derivatives have been employed to develop such films. Heterocyclic compounds containing other elements could be potentially used to fabricate metallic-tone glossy films with different properties from those of thiophene derivatives. Therefore, in this study, we focused on selenophene, a high-period analog of thiophene with a smaller HOMO–LUMO gap than thiophene. Polymers containing selenophene have been studied as electronic materials.45–47 Compared to polythiophene, polyselenophene has a rigid main chain backbone owing to its stronger quinoid properties and resistance to torsion.47 In addition, a selenium atom has the same degree of electronegativity as a carbon atom and higher atomic radius and polarizability than a sulfur atom, which lead to a larger atomic refractive index in the Lorentz–Lorenz equation; therefore, a higher refractive index is expected.48–51 These characteristics of (poly)selenophene are expected to afford films with a different color tone from that of polythiophene films. In this study, we developed metallic glossy materials based on anion-doped poly(3-alkoxyselenophene). The use of selenophene afforded a different luster color, significantly different from the typical color of thiophene-based materials, thereby opening new possibilities for material design and applications.
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Scheme 1 Synthesis of the anion-doped poly(3-alkoxyselenophene) via chemical oxidative polymerization. |
Polymer | Mp![]() |
DPp![]() |
Doping levelc (%) | Film thicknessd (mm) | Rqd (μm) | σe (S cm−1) | Pencil hardness |
---|---|---|---|---|---|---|---|
a Molecular weight corresponding to the main peak in the differential molecular weight distribution curve.b Polymerization degree calculated from Mp.c Determined via SEM-EDX analysis.d Determined via CLSM.e The electric conductivity of films was determined by measuring the sheet resistance via the double ring method using a resistivity meter. | |||||||
MeOSe_ClO4 | 1110 | 7 | 20 | 2.19 | 0.03 | 1.4 × 10−5 | 2B |
BuOSe_ClO4 | 1210 | 6 | 21 | 2.21 | 0.03 | 1.4 × 10−7 | 2B |
MeOSe_BF4 | 1080 | 7 | 18 | 2.57 | 0.02 | 2.7 × 10−4 | 2B |
BuOSe_BF4 | 1240 | 6 | 28 | 2.11 | 0.04 | 1.2 × 10−6 | B |
The doping level of each polymer was calculated via SEM-EDX analysis (Table 1). The doping level of polymers except for BuOSe_BF4 was approximately 20%, which is lower than that of the alkoxythiophene polymers (approximately 30%).42 This is because the molecular weight of these polyselenophenes is small, and the doping level is also relatively small.
To investigate the regioregularity of polyselenophenes, we attempted to perform 1H NMR measurements using the method from our previous study.37 Our previous polythiophenes could be dedoped in DMSO-d6 solution, and their NMR spectra could be measured after de-doping. However, the dedoped polyselenophenes were not soluble in DMSO-d6 or other deuterated solvents. Therefore, 1H NMR measurements could not be performed.
We have carried out TG-DTA measurements for all the polymers to investigate their thermal stability. TG-DTA curves are provided in the ESI as Fig. S5.‡ No significant weight loss was observed up to 200 °C. The values of 5% weight loss (Td5), one of the indicators of thermal stability, are summarized in Table S3.‡ We note that ClO4−-doped polymers were measured to 200 °C due to the possibility of rupture caused by ClO4− ions.
The preparation of the coating solution and films was attempted using MeOSe_ClO4. First, the coating solution of MeOSe_ClO4 was prepared as a 1 wt% coating solution using nitromethane as the solvent, following the same procedure as that of the previous polyalkoxythiophene coating solution that afforded a metal-like lustrous coating film. However, the MeOSe_ClO4 powder produced residues in acetonitrile, which did not completely dissolve, and the coating film did not exhibit a lustrous effect. The glass substrate was covered with the polymer powder (Fig. S5‡). Conversely, MeOSe_ClO4 was completely dissolved in propylene carbonate and the coating film prepared from the propylene carbonate coating solution exhibited a metal-like lustrous effect. Details on the glossy color of the film will be provided later.
Fig. 1 shows photographs of the polyselenophene coating films, which were prepared using propylene carbonate as the solvent. The images were captured using a digital camera. All films reflected the scale of a stainless-steel ruler positioned perpendicular to the film surface, exhibiting a high luster. The surface of each film was observed with laser scanning microscopy (Fig. S7‡). The film thickness ranged from 2 to 3 μm, with all films exhibiting a relatively flat surface morphology and low root-mean-square roughness (Rq) of approximately 0.03 μm (Table 1). The electrical conductivity of polyselenophenes was 10−4 to 10−7, which was almost the same as that of general π-conjugated organic polymers. Additionally, the electrical conductivity of BuOSe_ClO4 and BuOSe_BF4, which have long alkoxy chain, was low. This trend is in agreement to that of polyalkoxythiophenes observed in our previous study.42 This may be attributed to the alkoxy chain acting as an insulator that is separating the conductive main chains.52 Moreover, when the alkoxy chain length was the same, the electric conductivity was higher for the BF4− dopant than for the ClO4− dopant, even though it had the same doping level. This finding will be further discussed below, together with the XRD crystal structure analysis of the coating films.
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Fig. 1 Photographs of the (a) MeOSe_ClO4, (b) MeOSe_BF4, (c) BuSe_ClO4, and (d) BuOSe_BF4 coating films prepared from propylene carbonate coating solutions of the corresponding polymer. |
Furthermore, no significant difference in pencil hardness was observed between the polyalkoxyselenophene and poly(3-methoxythiophene) films (Table 1 and Table S3‡).
Our previous studies on polyalkoxythiophenes were conducted using nitromethane as the solvent. Conversely, a coating solution of polyselenophenes was prepared using propylene carbonate. For comparison, a coating solution was prepared using the same solvent in the MeOT_ClO4, and a film was prepared. The MeOT_ClO4 coating film exhibited a gold-like lustrous color (Fig. S8‡). More information regarding MeOT_ClO4 is provided in the ESI.‡
Spectral colorimetry was employed to evaluate the polymer film reflection color quantitatively. Fig. 2a shows the L*, a*, and b* coordinates in the L*a*b* color space for all the polymer films, with the vacuum-evaporated metallic gold and copper films as the reference for comparison. The a* and b* values of all the polyselenophene films were closer to the origin than those of the vacuum-evaporated metallic gold and MeOT_ClO4 film (Fig. S9a‡). The a* and b* values of all polyselenophenes were located at 0 to 11 and −3 to 7, respectively (Table S4‡). The films containing a methoxy group exhibited larger a* and b* values than those with a butoxy group. In the L*a*b* color space, a higher a* means more red components, whereas a higher b* means more yellow components. The BuOSe_ClO4 and BuOSe_BF4 films were located close to their origin of the L*a*b* color space. Whereas, the MeOSe_ClO4 and MeOSe_BF4 films exhibited more reddish and yellowish tones and a reddish-purple luster.
The color lightness (L*) of all polyselenophene films was 20–30, whereas that of MeOT_ClO4 was almost 40. In contrast, the L* values for the evaporated gold and copper films were 80–90.
The lustrous properties of the polymer films were evaluated via specular reflection spectrometry (Fig. 2b). The small reflection peak at approximately 690 nm was due to switching the light source and does not have a substantial reflection. The specular spectrum of all polyselenophenes exhibited a red-shift relative to that of MeOT_ClO4 (Fig. S9b‡). The polyselenophene films exhibited a strong reflection of red light (620–750 nm), a slightly strong reflection of orange (590–620 nm), and a lower reflection of purple (380–450 nm), blue (450–495 nm), green (495–570 nm), and yellow (570–590 nm) regions. Therefore, it was concluded that compared with MeOT_ClO4, the polyselenophene films had a lower reflectance, especially in the green region, with the color of the film being closer to reddish-purple or black. The reflectance of the MeOSe_BF4 and BuOSe_BF4 films reached 20%, which is 5% higher than those of the MeOSe_ClO4 and BuOSe_ClO4 films. This may be attributed to the high crystallinity of the MeOSe_BF4 and BuOSe_BF4 films (more details on the XRD analysis section).
The diffuse reflection spectra were flat and demonstrated almost no reflectance values for all films (Fig. 2c), which are characteristics of the metallic luster.
In our previous study, we reported that the polyalkoxythiophene films exhibit gloss owing to their higher optical constants (refractive index (n) and extinction coefficient (κ)) compared to general transparent polymers. For instance, the n values of commercially available transparent polymers range from 1.3 to 1.7, exhibiting no photoabsorption in the visible region (i.e., κ = 0)53 and no metallic reflection. Our anion-doped poly(3-alkoxythiophene) films exhibited strong lustrous, unlike transparent resins, owing to the large n and κ values of organic materials in the visible region.36,38,39,42 This is a characteristic of organic materials that develop metallic glosses. The optical constants of the polymer films were measured using ellipsometry to investigate the mechanism of luster appearance. Generally, the reflectance and chromaticity of a material are determined by the magnitude and wavelength dependence of the optical constants. In the case of normal incidence, the reflectance (R) between air and a given medium is related to n and κ, following eqn (1).21
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Fig. 2d–f show the n, κ, and R values obtained using eqn (1). The refractive index of the polyselenophene films is constant from 400 to 600 nm, being higher than that of the MeOT_ClO4 film. Then, after 600 nm, it increases. The reflectance rise wavelength of the polyselenophene films is red-shifted compared to that of the MeOT_ClO4 film. The refractive index in the long wavelength region was approximately 2, which is higher than that of general transparent resins and as high as that of metallic glossy materials comprising organic compounds.
π-Conjugated polymer incorporating a porphyrin unit (porphyrin film) that exhibits green metal-lustrous effects exhibit a κmax value of 2–3.23,30 The κmax of the polyaniline analogs containing an azobenzene unit that exhibits green metal-lustrous effects is approximately 2.3.21 The extinction coefficient gradually increases from 400 nm, followed by a drastic increase from 550 nm, and becomes almost constant from ∼700 nm. The calculated refraction spectra of the polyselenophene films were red-shifted compared to those of the polyalkoxythiophene films (Fig. 2f). Such findings are in agreement with the specular reflection spectra (Fig. 2b).
Our previous studies concluded that the glossy appearance of anion-doped polythiophene films was attributed to the compact lamellar crystallites formed by the polyalkoxythiophene chains in the film (more information is provided in the discussion on XRD Analysis).33–42 In the anion-doped polyalkoxyselenophene films of this study, these crystallites also exhibited very large optical constants, as shown in Fig. 2d and e. Although the specular refraction spectra of the polyselenophene films and the vacuum-deposited metal film appear similar, the n and κ characteristics and mechanisms that produce the reflections differ. Therefore, the luster color of the poly(3-alkoxyselenophene) films was not caused by Drude's metallic response, which involves the screening of electromagnetic waves by free electrons; it was induced by the same mechanism observed in the thiophene polymer films.
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Fig. 3 (a) Structure of edge-on lamellar crystallites. (b) X-ray diffraction patterns of the anion-doped poly(3-alkoxyselenopehen) films. (c) Structure of face-on lamellar crystallites. |
The high-angle peak observed at approximately 2θ = 25° was attributed to the face-on lamellar crystals (Fig. 3c), and was independent of the dopant type and side chain. Such a finding indicates that the stacking distance is the same for all the tested polymers (ca. 0.36 nm). In previously reported polythiophenes with a liner alkoxy group, the amount of the face-on lamellar crystals was significantly lower compared to that of the edge-on lamellar crystals.34–37,39,42 Conversely, the polyselenophenes developed in this study exhibit a distinct, broad peak in the high-angle region compared to the low-angle region. This suggests that the quantity of face-on lamellar crystals in polyselenophenes is greater than that observed in polythiophenes.
Our previously developed films with polythiophenes with a branched alkoxy group exhibited a dark color close to black.42 Additionally, electrochemical methods can produce films where face-on lamellae dominate, resulting in a low-gloss red-purple color.43 These results indicate that in polythiophenes with a branched alkoxy group, edge-on lamellar crystals are not completely formed, while edge-on and face-on lamellar crystals coexist in roughly equal amounts resulting in a low-gloss black-purple color. In contrast, polyselenophene films contain a higher proportion of edge-on lamellar crystals, which likely contribute to the observed higher brightness compared to the branched polythiophenes. This suggests that the edge-on lamellar crystals in polyselenophene are more effective at reflecting light, especially in the yellow and orange regions. Additionally, the face-on lamellar crystals contribute to a low-reflective black luster. The combination of these two factors is thought to produce the exquisite, luxurious black and purple metallic gloss observed in the selenophene-based films.
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Fig. 4 Ultraviolet–visible (UV-vis) spectra of a diluted coating solution of anion-doped poly(3-alkoxyselenophene)s in propylene carbonate. |
Polymers composed of selenophene and tellurophene are known to form aggregates due to the interactions between the selenium or tellurium elements that make them up.54–56 It is also known that such aggregates are less likely to form in thiophene-based systems. In the cases of MeOSe_ClO4 and BuOSe_BF4, multiple peaks are observed in the region between 600 and 700 nm, suggesting the formation of multiple aggregation states. Other spectra exhibit broadening as shoulder peaks in this region; however, multiple aggregation states are believed to be present. These are thought to be aggregates formed due to Se–Se interactions. On the other hand, UV-vis measurements of the undiluted coating solution were performed, and a broadening of the spectra was observed for all the polymers. No significant spectral changes were observed due to differences in the side chain groups; however, a trend of varying peak positions was observed depending on the dopant. In other words, the peak top for ClO4−-doped polymers appeared around 650 nm, whereas the peak top for BF4−-doped polymers shifted to a higher wavelength region. This suggests that, in concentrated solutions, the dopant has a more significant influence on the formation of aggregates than the side chain groups. Additionally, UV-vis measurements of the dedoped polymers were also attempted; however, the dedoped polymers did not dissolve in propylene carbonate. To obtain more detailed information on the chemical species in the aggregated state, further investigations using dilution tests and theoretical calculations are considered necessary.
To investigate the stability of the coating solution, we conducted viscosity measurements (Fig. S12‡). The coating solution prepared using propylene carbonate showed no changes in viscosity, indicating a high stability. In contrast, the viscosity of the MeOT_ClO4 coating solution prepared using nitromethane is known to increase significantly within approximately one week.34 Thus, the coating solution using propylene carbonate can be stored stably for an extended period. Notably, the coating solution prepared in propylene carbonate exhibited a higher initial viscosity compared to that prepared in nitromethane, which is attributed to the higher viscosity of pure propylene carbonate compared to nitromethane.
The metal-like lustrous films developed in this study do not contain any metals, similar to previously reported polythiophene-based materials. In the future, conducting light stability and durability tests will be important to support the claim that the oligomers in this study can serve as alternatives to conventional paints containing metals, being promising for applications in essential everyday items such as writing instruments, cosmetics, anti-counterfeiting inks, and automotive paints. Moreover, the presence of face-on and edge-on lamellar crystals renders them suitable for applications in optoelectronic conversion devices (OPVs) and organic field-effect transistors (OFETs), for which further development is required.
Footnotes |
† This paper is dedicated to Emeritus Professor Takayuki Kawashima on the occasion of his 77th birthday (“Kiju” in Japanese). |
‡ Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4lp00338a |
This journal is © The Royal Society of Chemistry 2025 |