No‐Heating Deposition of Ferroelectric x %YO 1.5 –(100− x %)(Hf 1− y Zr y )O 2 Films
The no‐heating deposition of x %YO 1.5 –(100− x %)(Hf 1− y Zr y )O 2 ( x = 0−0.09, y = 0, 0.25, 0.50, and 1) is achieved using a radio‐frequency magnetron sputtering method. To investigate the crystal structure and ferroelectric properties, epitaxial films are grown on (111)‐oriented indium tin ox...
Gespeichert in:
Veröffentlicht in: | Physica status solidi. A, Applications and materials science Applications and materials science, 2023-07, Vol.220 (14) |
---|---|
Hauptverfasser: | , , , , , |
Format: | Artikel |
Sprache: | eng |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | The no‐heating deposition of
x
%YO
1.5
–(100−
x
%)(Hf
1−
y
Zr
y
)O
2
(
x
= 0−0.09,
y
= 0, 0.25, 0.50, and 1) is achieved using a radio‐frequency magnetron sputtering method. To investigate the crystal structure and ferroelectric properties, epitaxial films are grown on (111)‐oriented indium tin oxide (ITO)/(111) Y‐stabilized zirconia (YSZ) substrates. The ferroelectric orthorhombic phase is obtained for the 5–7%YO
1.5
–95–93%HfO
2
and 5%YO
1.5
–95% (Hf
0.75
Zr
0.25
)O
2
films. The field‐induced phase transition from tetragonal to orthorhombic is confirmed for the 8%YO
1.5
–92%HfO
2
and 5%YO
1.5
–95%(Hf
0.50
Zr
0.50
)O
2
films. The remnant polarization (
P
r
) and coercive field (
E
c
) are 12–19 μC cm
−2
and 2,000–2,500 kV cm
−1
, respectively. The piezoelectric response of 1 μm thick films is investigated for 6%YO
1.5
–94% HfO
2
, 7%YO
1.5
–93%HfO
2
, and 5%YO
1.5
–95%(Hf
0.50
Zr
0.50
)O
2
films, which have piezoelectric coefficients (
d
33
) of 1.0, 3.3, and 5.0 pm V
−1
, respectively. These results show no‐heating deposition of
x
%YO
1.5
–(100−
x
%)(Hf
1−
y
Zr
y
)O
2
films with ferroelectric and piezoelectric properties. |
---|---|
ISSN: | 1862-6300 1862-6319 |
DOI: | 10.1002/pssa.202300100 |