TY - GEN
T1 - Intrinsic defects pinned at the domain wall in lithium niobate
AU - Stone, G.
AU - Steigerwald, H.
AU - Buse, K.
AU - Sohler, W.
AU - Gopalan, Venkatraman
AU - Phillpot, S.
AU - Dierolf, V.
PY - 2011/9/6
Y1 - 2011/9/6
N2 - Ferroelectric domain engineering is a powerful technique that can be used to create nonlinear optical devices based on quasi-phase matching. However, creating domains smaller than 1m poses significant challenges. This is partially due to an incomplete understanding of the properties of the ferroelectric domains; particularly in regards to the interaction of the domain wall and intrinsic defects, which determine the domain shapes and growth dynamics. Such defects are present in large numbers in congruent LiNbO3 crystals due to lithium deficiency. Due to the ionic nature of these intrinsic defects, they constitute defect dipoles that can be oriented in different ways in respect to the ferroelectric axis. In particular, after a domain inversion at room temperature these dipoles may not reorient along with the ferroelectric polarization and find themselves in an energetically unfavorable, frustrated, alignment that creates strain in the material. It has been found that such strain is released over time and by thermal treatments as shown by the observation of characteristic shifts in the Raman spectra [1].
AB - Ferroelectric domain engineering is a powerful technique that can be used to create nonlinear optical devices based on quasi-phase matching. However, creating domains smaller than 1m poses significant challenges. This is partially due to an incomplete understanding of the properties of the ferroelectric domains; particularly in regards to the interaction of the domain wall and intrinsic defects, which determine the domain shapes and growth dynamics. Such defects are present in large numbers in congruent LiNbO3 crystals due to lithium deficiency. Due to the ionic nature of these intrinsic defects, they constitute defect dipoles that can be oriented in different ways in respect to the ferroelectric axis. In particular, after a domain inversion at room temperature these dipoles may not reorient along with the ferroelectric polarization and find themselves in an energetically unfavorable, frustrated, alignment that creates strain in the material. It has been found that such strain is released over time and by thermal treatments as shown by the observation of characteristic shifts in the Raman spectra [1].
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U2 - 10.1109/CLEOE.2011.5942847
DO - 10.1109/CLEOE.2011.5942847
M3 - Conference contribution
AN - SCOPUS:80052274341
SN - 9781457705335
T3 - 2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference, CLEO EUROPE/EQEC 2011
BT - 2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference, CLEO EUROPE/EQEC 2011
T2 - 2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference, CLEO EUROPE/EQEC 2011
Y2 - 22 May 2011 through 26 May 2011
ER -