TY - JOUR
T1 - Domain structure and phase transitions in epitaxial KNbO3 thin films studied by in situ second harmonic generation measurements
AU - Gopalan, Venkatraman
AU - Raj, Rishi
PY - 1996
Y1 - 1996
N2 - Epitaxial thin films of KNbO3 were deposited on SrTiO3 (100) substrate by laser ablation. In the orthorhombic phase, the four possible domain variants in the KNbO3 (110) film growth plane were determined to be KNbO3[11̄0]∥SrTiO3[001], [001̄], [010], and [01̄0] denoted as X+, X-, Y+, and Y-, respectively. Using a fundamental beam of 1064 nm transmitted normal to the film, the second harmonic generation (SHG) signal at 532 nm was measured and correlated to the area fractions AX+, AX-, AY+, and AY- of the four domain variants X+, X-, Y+, and Y-, respectively, in the growth plane of the film. At room temperature, the area fractions δAx=AX+-AX- and δAy=AY+-AY- were determined to be ∼3.3% and ∼2.2%, respectively. In-situ SHG measurements revealed the phase transitions to be 210±10°C for orthorhombic-tetragonal and 450±10°C for tetragonal-cubic transitions. In the tetragonal phase (between 210°C and 450°C) the KNbO3 〈100〉∥SrTiO3 〈100〉. The use of SHG as a sensitive, non-destructive and real-time probe of phase transitions and evolution of domains in ferroelectric thin films is demonstrated.
AB - Epitaxial thin films of KNbO3 were deposited on SrTiO3 (100) substrate by laser ablation. In the orthorhombic phase, the four possible domain variants in the KNbO3 (110) film growth plane were determined to be KNbO3[11̄0]∥SrTiO3[001], [001̄], [010], and [01̄0] denoted as X+, X-, Y+, and Y-, respectively. Using a fundamental beam of 1064 nm transmitted normal to the film, the second harmonic generation (SHG) signal at 532 nm was measured and correlated to the area fractions AX+, AX-, AY+, and AY- of the four domain variants X+, X-, Y+, and Y-, respectively, in the growth plane of the film. At room temperature, the area fractions δAx=AX+-AX- and δAy=AY+-AY- were determined to be ∼3.3% and ∼2.2%, respectively. In-situ SHG measurements revealed the phase transitions to be 210±10°C for orthorhombic-tetragonal and 450±10°C for tetragonal-cubic transitions. In the tetragonal phase (between 210°C and 450°C) the KNbO3 〈100〉∥SrTiO3 〈100〉. The use of SHG as a sensitive, non-destructive and real-time probe of phase transitions and evolution of domains in ferroelectric thin films is demonstrated.
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U2 - 10.1063/1.115922
DO - 10.1063/1.115922
M3 - Article
AN - SCOPUS:0030568370
SN - 0003-6951
VL - 68
SP - 1323
EP - 1325
JO - Applied Physics Letters
JF - Applied Physics Letters
IS - 10
ER -