2018
DOI: 10.1021/acsami.7b16700
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Enhanced Switchable Ferroelectric Photovoltaic Effects in Hexagonal Ferrite Thin Films via Strain Engineering

Abstract: Ferroelectric photovoltaics (FPVs) are being extensively investigated by virtue of switchable photovoltaic responses and anomalously high photovoltages of ∼10 V. However, FPVs suffer from extremely low photocurrents due to their wide band gaps (E). Here, we present a promising FPV based on hexagonal YbFeO (h-YbFO) thin-film heterostructure by exploiting its narrow E. More importantly, we demonstrate enhanced FPV effects by suitably exploiting the substrate-induced film strain in these h-YbFO-based photovoltaic… Show more

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Cited by 50 publications
(39 citation statements)
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“…Unlike bulk systems, thin-film heterostructures can induce a lattice strain because of the lattice mismatch between a substrate and a film, which affects many physical properties such as ferroelectricity, electron mobility, ionic conductivity, and electrocatalysis 1720 . In particular, thin-film oxide fuel cells are attracting renewed attention owing to advantages of low temperature operation and portable device applications 2124 . Here, we demonstrate an unprecedently high degree of exsolution of nanoparticles in lattice misfit strained epitaxial thin films and achieve a particle density as high as ~1100 particles μm −2 , with a size of only ~5 nm, at a temperature as low as 550 °C.…”
Section: Introductionmentioning
confidence: 99%
“…Unlike bulk systems, thin-film heterostructures can induce a lattice strain because of the lattice mismatch between a substrate and a film, which affects many physical properties such as ferroelectricity, electron mobility, ionic conductivity, and electrocatalysis 1720 . In particular, thin-film oxide fuel cells are attracting renewed attention owing to advantages of low temperature operation and portable device applications 2124 . Here, we demonstrate an unprecedently high degree of exsolution of nanoparticles in lattice misfit strained epitaxial thin films and achieve a particle density as high as ~1100 particles μm −2 , with a size of only ~5 nm, at a temperature as low as 550 °C.…”
Section: Introductionmentioning
confidence: 99%
“…It has been shown, for instance, that J sc can be switched by reversing the ferroelectric polarization (P) of the film, which indicates that the Schottky barriers at interfaces with electrodes play a major role [20]. However, to the best of our knowledge, no evidence of BPE has ever been reported neither in h-RMnO 3 , nor in the isostructural h-RFeO 3 [21,22]. Here we report on the photoresponse of h-LuMnO 3 (h-LMO) single crystals, aiming at determining its BPE response which may open new avenues beyond promising opportunities in conventional photovoltaics [23].…”
Section: Introductionmentioning
confidence: 93%
“…For example, h-RFeO 3 structure can be easily obtained in thin films via the substrate matching route. Indeed, elevated temperature ferroelectricity in (Lu, Yb, Tm)FeO 3 epitaxial films has been demonstrated and the measured remnant polarization P r ∼ 5 μC/cm 2 [ 33 , 34 ], as shown in Fig. 3 .…”
Section: Type-i Multiferroicsmentioning
confidence: 99%
“… Room-temperature ferroelectric hysteresis loops of (a) hexagonal YbFeO 3 films grown on different substrates, and (b) hexagonal LuFeO 3 and TmFeO 3 films grown on Al 2 O 3 (0001) substrates [ 33 , 34 ]. Antiferromagnetic transition temperature T N as a function of (c) lattice parameter c / a , and (d) tolerance factor for hexagonal manganites and ferrites [ 37 , 38 ].…”
Section: Type-i Multiferroicsmentioning
confidence: 99%