Lithium niobate crystals were grown in 3D through localized heating by femtosecond laser irradiation deep inside 35Li2O-35Nb2O5-30SiO2 glass. Laser scanning speed and power density were systematically varied to control the crystal growth process and determine the optimal conditions for the formation of single crystal lines. EBSD measurements showed that, in principle, single crystals can be grown to unlimited lengths using optimal parameters. We successfully tuned the parameters to a growth mode where nucleation and growth occur upon heating and ahead of the scanning laser focus. This growth mode eliminates the problem reported in previous works of non-uniform polycrystallinity because of a separate growth mode where crystallization occurs during cooling behind the scanning laser focus. To our knowledge, this is the first report of such a growth mode using a fs laser. The crystal cross-sections possessed a symmetric, smooth lattice misorientation with respect to the c-axis orientation in the center of the crystal. Calculations indicate the observed misorientation leads to a decrease in the refractive index of the crystal line from the center moving outwards, opening the possibility to produce within glass a graded refractive index single crystal (GRISC) optically active waveguide.
This
study explores multiple fields as a mechanism of controlling
the orientation of the nucleation process, which is generally believed
to be a stochastic process, as observed in the equiaxed grain structure
of glass ceramics. Specifically, as a model system, Sb2S3 single crystals are grown on the surface of Sb-S-I
chalcogenide glass via laser crystallization. A spatial light modulator
is used to configure the beam shape, thermal gradient, and/or polarization
of the laser for controlling the orientation of Sb2S3 crystal seeds. We determine that the chemical and thermal
gradient can affect the crystal morphology but do not significantly
influence the crystal seed orientation. In contrast, the short crystal
axis along [010] has a preferential alignment along the direction
of polarization and perpendicular to the surface normal. Thus, we
conclude that polarization can be used as an effective tool for controlling
the nucleation and hence the orientation of Sb2S3 crystals on the surface of Sb-S-I chalcogenide glasses.
Practical applications of the recently demonstrated method of growing single-crystal architecture in glass by a femtosecond laser demand answers to two key questions: (1) How is the formation of a single crystal affected by the incongruent composition of glass? (2) Why are laser scanning speeds higher than a critical value necessary for obtaining single crystals in some cases, whereas smaller than a critical value are required in other systems? We have sought answers to both of these questions by investigating the effect of La 2 O 3 concentration on the crystallization of LaBGeO 5 in xLa 2 O 3 −B 2 O 3 −2GeO 2 glass as a model system that has been studied most extensively. The results show that for stoichiometric and La 2 O 3 -rich glass, a scanning speed above a critical value is required for fabricating LaBGeO 5 single crystal, while the opposite is true for the La 2 O 3 -deficient composition. The origin of these divergent behaviors is shown to be in the relative values of nucleation and growth rates and their temperature dependencies. This first systematic study illustrates the complex role of composition on the nucleation and growth mechanisms and provides a framework for determining the processing parameters needed for fabricating single-crystal architecture in a glass.
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