Porous single crystalline-like titanium dioxide monolith with enhanced photoelectrochemical performance
Macro-sized porous single crystalline-like (PSC-like) TiO 2 is endowed with unique structural advantages due to its structural consistency and porosity in a large area, which would significantly enhance its photoelectrochemical function. However, there are significant technical challenges in the gro...
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Veröffentlicht in: | Frontiers in materials 2023-04, Vol.10 |
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Hauptverfasser: | , , , , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Macro-sized porous single crystalline-like (PSC-like) TiO
2
is endowed with unique structural advantages due to its structural consistency and porosity in a large area, which would significantly enhance its photoelectrochemical function. However, there are significant technical challenges in the growth of porous single crystalline-like monoliths. The consistency of structure dominates the structure so that the grain boundary is reduced to the minimum, which is in contradiction with the three-dimensional percolation structure. Here we report a lattice reconstruction strategy based on solid-solid transformation to grow porous single crystal-like anatase TiO
2
dominated by (200) and (101) facets at 2 cm scale. In comparison with the traditional definition of porous single crystal, it has two different lattice orientations, but still has good photoelectrochemical properties. The band gap engineering introduces Ti
3+
gap into the lattice to generate Ti
n
O
2n−1
with Magneli phase, limiting the created active structure to the lattice with two-dimensional surface, which would open a new avenue to create highly active surfaces to capture photons and transport electrons stably. The PSC-like Ti
n
O
2n−1
provides enhanced exciton lifetime (3–5 ns) as a photocatalytic catalyst and shows significant visible light absorption. The independent PSC-like Ti
n
O
2n−1
delivers high photocurrent of 1.8–5.5 mA · cm
−2
at room temperature and does not decay for 10 h. |
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ISSN: | 2296-8016 2296-8016 |
DOI: | 10.3389/fmats.2023.1177093 |