Abstract:A wealth of fascinating phenomena have been discovered at the BiFeO domain walls, examples such as domain wall conductivity, photovoltaic effects, and magnetoelectric coupling. Thus, the ability to precisely control the domain structures and accurately study their switching behaviors is critical to realize the next generation of novel devices based on domain wall functionalities. In this work, the introduction of a dielectric layer leads to the tunability of the depolarization field both in the multilayers and… Show more
“…[32,33] Figure 2a-d presents PFM amplitude and phase images along both the in-plane (IP) and out-of-plane (OP) directions. [32,33] Figure 2a-d presents PFM amplitude and phase images along both the in-plane (IP) and out-of-plane (OP) directions.…”
Section: Resultsmentioning
confidence: 99%
“…PFM technique is a powerful tool to reveal the ferroelectric polarization orientation and domain structure . Figure a–d presents PFM amplitude and phase images along both the in‐plane (IP) and out‐of‐plane (OP) directions.…”
Monoclinic phases, as intermediate phases at the morphotropic phase boundary, have been considered as the origin of high piezoelectricity in various piezoelectric systems. However, those monoclinic phases have seldom been experimentally observed at the phase boundary in lead‐free (K,Na)NbO3 (KNN)‐based materials. This work shows that KNN epitaxial thin films demonstrate a monoclinic MC phase stabilized by elastic strain at room temperature, which is identified by both synchrotron X‐ray reciprocal space mapping and piezoresponse force microscopy. It is revealed that the piezoelectricity is greatly enhanced at 170 °C due to the monoclinic MC–MA phase boundary. The discovery of monoclinic phases in this work may open an avenue for developing a new thermotropic phase boundary in KNN‐based materials. The results also provide a guide for the exploration of high piezoelectricity driven by monoclinic phases in lead‐free piezoelectric materials.
“…[32,33] Figure 2a-d presents PFM amplitude and phase images along both the in-plane (IP) and out-of-plane (OP) directions. [32,33] Figure 2a-d presents PFM amplitude and phase images along both the in-plane (IP) and out-of-plane (OP) directions.…”
Section: Resultsmentioning
confidence: 99%
“…PFM technique is a powerful tool to reveal the ferroelectric polarization orientation and domain structure . Figure a–d presents PFM amplitude and phase images along both the in‐plane (IP) and out‐of‐plane (OP) directions.…”
Monoclinic phases, as intermediate phases at the morphotropic phase boundary, have been considered as the origin of high piezoelectricity in various piezoelectric systems. However, those monoclinic phases have seldom been experimentally observed at the phase boundary in lead‐free (K,Na)NbO3 (KNN)‐based materials. This work shows that KNN epitaxial thin films demonstrate a monoclinic MC phase stabilized by elastic strain at room temperature, which is identified by both synchrotron X‐ray reciprocal space mapping and piezoresponse force microscopy. It is revealed that the piezoelectricity is greatly enhanced at 170 °C due to the monoclinic MC–MA phase boundary. The discovery of monoclinic phases in this work may open an avenue for developing a new thermotropic phase boundary in KNN‐based materials. The results also provide a guide for the exploration of high piezoelectricity driven by monoclinic phases in lead‐free piezoelectric materials.
“…Screening conditions affect the stability of domain walls and are a key parameter in the control of complex domain structures. By inserting a dielectric layer between the ferroelectric thin film and the metallic buffer, the 109 • stripe domain state could be favored in BFO [62] and 180 • domains were stabilized in PbTiO 3 (PTO) [63,64]; see Figure 2d,e, respectively.…”
Section: Ferroic Domain Engineering In Single Layers and Superlatticesmentioning
Forthcoming low-energy consumption oxide electronics rely on the deterministic control of ferroelectric and multiferroic domain states at the nanoscale. In this review, we address the recent progress in the field of investigation of ferroic order in thin films and heterostructures, with a focus on non-invasive optical second harmonic generation (SHG). For more than 50 years, SHG has served as an established technique for probing ferroic order in bulk materials. Here, we will survey the specific new aspects introduced to SHG investigation of ferroelectrics and multiferroics by working with thin film structures. We show how SHG can probe complex ferroic domain patterns non-invasively and even if the lateral domain size is below the optical resolution limit or buried beneath an otherwise impenetrable cap layer. We emphasize the potential of SHG to distinguish contributions from individual (multi-) ferroic films or interfaces buried in a device or multilayer architecture. Special attention is given to monitoring switching events in buried ferroic domain-and domain-wall distributions by SHG, thus opening new avenues towards the determination of the domain dynamics. Another aspect studied by SHG is the role of strain. We will finally show that by integrating SHG into the ongoing thin film deposition process, we can monitor the emergence of ferroic order and properties in situ, while they emerge during growth. Our review closes with an outlook, emphasizing the present underrepresentation of ferroic switching dynamics in the study of ferroic oxide heterostructures.
“…For its ferroelectricity at room temperature, BFO has been widely studied . An antisymmetric DMI in BFO gives rise to a weak ferromagnetic moment, which is usually used for magnetoelectric coupling and may induce the field‐free SOT switching. However, the DMI coupling can only occur in some special situations .…”
Recently, magnetization switching driven by spin–orbit torque (SOT) has been intensely studied. However, it is still a challenge to effectively control the spin Hall angle (SHA) and critical current density for SOT switching. With the help of multiferroic BiFeO3 (BFO) thin films, a method to adjust SHA and the switching current is proposed. The BFO‐based heterostructures with opposite spontaneous polarization fields show huge changes in both perpendicular magnetic anisotropy and SOT‐induced magnetization switching. The variation of the effective SHAs for the heterostructures with opposite polarizations is estimated to be 272%, which can be attributed to the distribution of oxygen vacancies inside the BFO films. The possible applications of these structures in memory and reconfigurable logic devices are also demonstrated.
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