2010
DOI: 10.1016/j.jmmm.2010.07.001
|View full text |Cite
|
Sign up to set email alerts
|

Defect driven multiferroicity in Gd doped BiFeO3 at room temperature

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

3
11
0

Year Published

2011
2011
2024
2024

Publication Types

Select...
10

Relationship

0
10

Authors

Journals

citations
Cited by 51 publications
(14 citation statements)
references
References 50 publications
3
11
0
Order By: Relevance
“…All loops exhibit a finite exchange bias field and vertical symmetry with visibly greater saturation and remanent magnetization if compared to what has been previously reported [23,[48][49][50][51][52]. As an example the M-H curve of NBFSO materials for x= 0.10 shows remanent magnetization (M r ) 4.05 Am 2 /kg and coercive field (H C ) 0.08 T at room temperature.…”
Section: Resultssupporting
confidence: 50%
“…All loops exhibit a finite exchange bias field and vertical symmetry with visibly greater saturation and remanent magnetization if compared to what has been previously reported [23,[48][49][50][51][52]. As an example the M-H curve of NBFSO materials for x= 0.10 shows remanent magnetization (M r ) 4.05 Am 2 /kg and coercive field (H C ) 0.08 T at room temperature.…”
Section: Resultssupporting
confidence: 50%
“…Therefore, it allows current to pass through when a high voltage is applied [22][23][24]. Currently, great efforts have been made to improve electrical properties by doping with rare-earth elements such as: lanthanum [25][26][27][28][29], praseodymium [30,31], samarium [32][33][34][35], europium [36][37][38][39], gadolinium [40,41], dysprosium [42,43] and neodymium (Nd) [44][45][46][47][48]. Among these rare-earth elements, the employment of Nd as a dopant in BiFeO 3 thin films/ceramics has shown an improvement in ferroelectric and ferromagnetic properties [49,50].…”
Section: Introductionmentioning
confidence: 99%
“…These characteristics are unrepeatable, taking into account that most magnetic ferroelectrics possess coexisting spin and dipole order only well below room temperature. At room temperature, BiFeO3 single crystal has distorted rhombohedral (R) structure with lattice parameter of (ar=3.96Å and ar=89.41 Å) [7]. The magnetic ordering is G-type with a weak canting moment with a 62 nm spin cycloid [8].…”
Section: Introductionmentioning
confidence: 99%