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Photonic crystals for applications in photoelectrochemical processes: Photoelectrochemical solar cells with inverse opal topology - Notes

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Published abstract

Photonic crystal structures, that present strong light localization effects near photonic band gap frequency regions, can be very useful to maximize chemical processes of phototoactive materials. One example is the use of photonic crystals to improve solar energy harvesting in photoelectrochemical solar cells. Here, we describe the optical monitoring synthesis of macroporous materials, with inverse opal topology, made of transition metal and rare-earth oxide nanoparticles. Through the optical properties we can obtain information concerning both infiltration and over layer growth. Finally, we report on the efficiency improvement of photoelectrochemical cells when titania inverse opal topology is used.

Figures

Complete original Figure 1 composition extracted directly from the embedded PDF image
Figure 1. Summary. SEM images of the cleft edge of a thin film (30 monolayers) opal made of 615 nm latex particles: (a) before; (b)-(d) after infiltration with ceria nanoparticles. Scale bars: (a) 10 μm; (c) 2 μm; (b) and (d) 5 μm.

Source: I. Rodriguez et al., Photonics Nanostruct. Fundam. Appl. 3, 148-154 (2005). © Elsevier B.V.

Complete original Figure 2 composition extracted directly from the embedded PDF image
Figure 2. Summary. Optical reflectance of samples, along the (111) direction, during the spin-coating-mediated CeO2 infiltration process. The number of infiltration cycles increases from spectrum ‘a’ to ‘e’.

Source: I. Rodriguez et al., Photonics Nanostruct. Fundam. Appl. 3, 148-154 (2005). © Elsevier B.V.

Complete original Figure 3 composition extracted directly from the embedded PDF image
Figure 3. Summary. (a and b) SEM images of inverse ceria structure after the colloidal crystal template removal. (c) Inverse structure with an overlayer of CeO2 on the top surface.

Source: I. Rodriguez et al., Photonics Nanostruct. Fundam. Appl. 3, 148-154 (2005). © Elsevier B.V.

Complete original Figure 4 composition extracted directly from the embedded PDF image
Figure 4. Summary. The reflectance spectra track zirconia and yttria opal templates through nanoparticle infiltration and subsequent removal of the polymer spheres. Infiltration shifts the Bragg peak to longer wavelength as the mean refractive index rises, whereas formation of the inverse structure shifts it strongly towards shorter wavelength. The accompanying electron micrographs confirm ordered, interconnected macroporous replicas without a surface overlayer, so the spectral changes provide a non-destructive measure of loading and template removal.

Source: I. Rodriguez et al., Photonics Nanostruct. Fundam. Appl. 3, 148-154 (2005). © Elsevier B.V.

SEM image of a titania inverse opal electrode with a 2 micrometre scale bar
Figure 5. Summary. SEM image of a titania inverse opal 8 μm thick electrode used for a photoelectrochemical solar cell. The void size is 170 nm and the bar corresponds to 2 μm.

Source: I. Rodriguez et al., Photonics Nanostruct. Fundam. Appl. 3, 148-154 (2005). © Elsevier B.V.

Complete Figure 6 composition with current-voltage curve and spectral response panels
Figure 6. Summary. Panel a compares current-voltage curves for titania inverse-opal and conventional photoelectrochemical cells of equal thickness under AM1.5 one-sun illumination. The inverse-opal cell has higher open-circuit voltage and short-circuit current, yielding about 35% more total power despite containing roughly one quarter of the active material and therefore about five times greater conversion per active-material volume. Panel b places the strongest spectral response near the titania absorption edge, consistent with the deliberately aligned low-frequency edge of the photonic pseudogap, although the paper treats this photonic interpretation as a preliminary result requiring further verification.

Source: I. Rodriguez et al., Photonics Nanostruct. Fundam. Appl. 3, 148-154 (2005). © Elsevier B.V.

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Research fields

Bottom-up

Latex opals are infiltrated with TiO₂, CeO₂, ZrO₂ or Y₂O₃ nanoparticles and then removed to leave interconnected inverse-opal frameworks. Repeated infiltration controls wall loading while preserving the three-dimensional macropore topology.

Characterization

Infrared reflectance follows stop-band shifts during infiltration and template removal, providing a non-destructive measure of how the pores fill. SEM and photoelectrochemical current-voltage tests then connect the completed inverse-opal morphology with improved light harvesting in solar-cell electrodes.