2013
DOI: 10.1016/j.crhy.2013.08.004
|View full text |Cite
|
Sign up to set email alerts
|

Nanoscale studies of ferroelectric domain walls as pinned elastic interfaces

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

6
50
0

Year Published

2013
2013
2023
2023

Publication Types

Select...
9

Relationship

1
8

Authors

Journals

citations
Cited by 66 publications
(61 citation statements)
references
References 171 publications
6
50
0
Order By: Relevance
“…Successful switching was defined as a°180 PFM phase contrast between the two polarization states, and the presence of a well-defined ring feature corresponding to a decrease of PFM amplitude at the domain wall, characteristic of a columnar domain penetrating through the full film thickness. At both RH values, we recognize the previously-reported [12] linear (figure 2(c)) and logarithmic (figure 2(d)) dependence of domain size on tip bias and writing time, respectively. However, for comparable choice of writing parameters, domain radii at 44% RH (figure 2(b)) are almost twice as big as those obtained at 29% RH (figure 2(a)).…”
Section: Resultssupporting
confidence: 85%
See 1 more Smart Citation
“…Successful switching was defined as a°180 PFM phase contrast between the two polarization states, and the presence of a well-defined ring feature corresponding to a decrease of PFM amplitude at the domain wall, characteristic of a columnar domain penetrating through the full film thickness. At both RH values, we recognize the previously-reported [12] linear (figure 2(c)) and logarithmic (figure 2(d)) dependence of domain size on tip bias and writing time, respectively. However, for comparable choice of writing parameters, domain radii at 44% RH (figure 2(b)) are almost twice as big as those obtained at 29% RH (figure 2(a)).…”
Section: Resultssupporting
confidence: 85%
“…Experiments have focused primarily on the latter, more accessible regimes, using piezoresponse force microscopy (PFM) to image needle-like [8] or cylindrical [9] domains in single crystals and thin films. Such studies have demonstrated the creep-like lateral motion of domain walls pinned by defects [10][11][12], recently confirmed with atomic resolution by direct imaging of domain growth using transmission electron microscopy [13]. They also highlighted the crucial role of surface adsorbates [14][15][16][17], particularly water, which determine the electrostatic boundary conditions and thus the size, shape and growth rate of the domain [18][19][20].…”
Section: Introductionmentioning
confidence: 94%
“…At zero temperature this leads to the existence of a depinning force f dep , below which no motion takes place. At finite temperature T the combination of the applied force, collective pinning and thermal effects leads to an extremely rich dynamical behavior, which has been the focuss of many theoretical [1,2,5,6,9] and experimental studies [10][11][12][13][14][15][16].…”
mentioning
confidence: 99%
“…However, our experimental results shown in S1 suggested a ferroelectric switching rather than the motion of ferroelastic domain walls. Therefore, there could be a relatively strong pinning effect to the micro-ferroelastic domain walls in the present PMN-38%PT single crystal, which would originate from the existence of oxygen vacancy, topological defects or compositional variation in relaxor-based ferroelectrics [44][45][46][47]. with alternate !…”
mentioning
confidence: 99%