Ultrathin-layer α-Fe2O3 deposited under hematite for solar water splitting
This work proposes a new strategy to prepare a hematite (α-Fe 2 O 3 ) bilayer photoanode by hydrothermally depositing α-Fe 2 O 3 (B) on the α-Fe 2 O 3 (A) films prepared by electrochemical deposition. Compact smooth surfaced α-Fe 2 O 3 (A) films were electrochemically deposited on FTO (SnO 2 :F) sub...
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Veröffentlicht in: | Journal of solid state electrochemistry 2018-08, Vol.22 (8), p.2347-2356 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | This work proposes a new strategy to prepare a hematite (α-Fe
2
O
3
) bilayer photoanode by hydrothermally depositing α-Fe
2
O
3
(B) on the α-Fe
2
O
3
(A) films prepared by electrochemical deposition. Compact smooth surfaced α-Fe
2
O
3
(A) films were electrochemically deposited on FTO (SnO
2
:F) substrates from an aqueous bath. The α-Fe
2
O
3
(A), α-Fe
2
O
3
(B), and α-Fe
2
O
3
/α-Fe
2
O
3
bilayer films’ characteristics were defined by X-ray diffraction (XRD) measurements, field emission scanning electron microscopy (FESEM), and energy-dispersive X-ray (EDX) spectroscopy. Pure crystalline α-Fe
2
O
3
(B) films with a typical anisotropic-like nanoparticle formation, which exhibited nanostructured rods covering the substrate and formed the characteristic mesoporous film morphology, were hydrothermally deposited on α-Fe
2
O
3
(A) films prepared by electrochemical depositing in a solution bath at 25 °C and a potential of − 0.15 V. The photocurrent measurements exhibited increased intrinsic surface states (or defects) at the α-Fe
2
O
3
(A)/α-Fe
2
O
3
(B) interface. The photoelectrochemical performance of the α-Fe
2
O
3
(A)/α-Fe
2
O
3
(B) structure was examined by chronoamperometry, which found that the α-Fe
2
O
3
(A)/α-Fe
2
O
3
(B) structure exhibited greater photoelectrochemical activity than the α-Fe
2
O
3
(A) and α-Fe
2
O
3
(B) thin films. The highest photocurrent density was obtained for the bilayer α-Fe
2
O
3
(A)/α-Fe
2
O
3
(B) films in 1 M NaOH electrolyte. This great photoactivity was ascribed to the highly active surface area, and to the externally applied bias that favored the transfer and separation of photogenerated charge carriers in α-Fe
2
O
3
(A)/α-Fe
2
O
3
(B). The improved photocurrent density was attributed to an appropriate band edge alignment of semiconductors and to enhanced light absorption by both semiconductors. The best performing samples were α-Fe
2
O
3
(A)/α-Fe
2
O
3
(B), which reached the maximum incident photon conversion efficiencies (IPCE) of 400 nm at the potential of 0.1 V. In this case, the IPCE values were 3-fold higher than those of the α-Fe
2
O
3
(A) and α-Fe
2
O
3
(B) films. |
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ISSN: | 1432-8488 1433-0768 |
DOI: | 10.1007/s10008-018-3946-7 |