2020
DOI: 10.1016/j.physleta.2020.126609
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Nanoscale imaging of ferroelectric domain and resistance switching in hybrid improper ferroelectric Ca3Ti2O7 thin films

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Cited by 7 publications
(3 citation statements)
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“…The HIF of Ca 3 Ti 2 O 7 films originates from the interplay of trilinear-related lattice modes in layered oxides, and these interactions are directly strained tuneable [75]. The ferroelectric domain switching and ferroelectric resistance reverse behaviours of Ca 3 Ti 2 O 7 films were evaluated in a recent study, and the maximum resistive ratios reached ∼1750 [76]. These results indicate that HIF in Ca 3 Ti 2 O 7 films is a promising oxide employed in non-volatile memory and logic devices.…”
Section: Compoundsmentioning
confidence: 99%
“…The HIF of Ca 3 Ti 2 O 7 films originates from the interplay of trilinear-related lattice modes in layered oxides, and these interactions are directly strained tuneable [75]. The ferroelectric domain switching and ferroelectric resistance reverse behaviours of Ca 3 Ti 2 O 7 films were evaluated in a recent study, and the maximum resistive ratios reached ∼1750 [76]. These results indicate that HIF in Ca 3 Ti 2 O 7 films is a promising oxide employed in non-volatile memory and logic devices.…”
Section: Compoundsmentioning
confidence: 99%
“…A recent experimental work on a polycrystalline Ca 3 Ti 2 O 7 sample reported a negative longitudinal piezoelectric strain coefficient d 33 = −45 pm/V . Negative longitudinal piezoelectricity, where polarization decreases under an applied stress is quite unusual and has only been reported in a few other materials. , However, another work on Ca 3 Ti 2 O 7 thin films measured a very small positive value d 33 = 5 pm/V . These piezoelectric coefficients are small compared to those of state-of-the-art piezoelectric perovskites such as PMN–PT, with d 33 values as high as 2500 pm/V reported .…”
Section: Introductionmentioning
confidence: 99%
“…20,21 However, another work on Ca 3 Ti 2 O 7 thin films measured a very small positive value d 33 = 5 pm/V. 22 These piezoelectric coefficients are small compared to those of state-of-the-art piezoelectric perovskites such as PMN−PT, with d 33 values as high as 2500 pm/V reported. 23 However, the presence of multiple lowenergy competing structural phases in n = 2 Ruddlesden− Popper layered perovskites together with the coupling between octahedral rotations and polarization, may enable interesting electromechanical effects in these materials.…”
Section: ■ Introductionmentioning
confidence: 99%