2006
DOI: 10.1016/j.jcrysgro.2005.12.116
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Crystal growth and characterization of Nd, Mg co-doped near-stoichiometric LiNbO3

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Cited by 19 publications
(10 citation statements)
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“…Nevertheless, the k eff being greater than unity is not common. In the earlier report by Nakamura et al [22], 0.12 mol% was reported in Nd, Mg:SLN. However, concentration in the LT crystal grown from 0.3 mol% Nd 3+ doped melt was also measured to be 5.6 Â 10 19 ions cm À 3 [23] in the crystal for which k eff was calculated to be 0.9.…”
Section: Resultsmentioning
confidence: 80%
“…Nevertheless, the k eff being greater than unity is not common. In the earlier report by Nakamura et al [22], 0.12 mol% was reported in Nd, Mg:SLN. However, concentration in the LT crystal grown from 0.3 mol% Nd 3+ doped melt was also measured to be 5.6 Â 10 19 ions cm À 3 [23] in the crystal for which k eff was calculated to be 0.9.…”
Section: Resultsmentioning
confidence: 80%
“…Here, we examine a micro-resonator disc of LiNbO 3 having a radius r = 2 mm and height h = 1 mm, placed on an aluminum thermostat. LiNbO 3 has a density of ρ = 4.648 g/cm 3 [ 34 ], yielding to a mass m of about 0.058 g. Its thermodynamic properties are the specific heat C = 0.63 J/(g·K) and the thermal conductivity k = 3.92 W/(m·K) [ 35 ]. If THz radiation is directed onto the top surface of the microdisc, it will first be largely absorbed by the crystal, and then reflected by the Al thermostat and, finally, further absorbed by the crystal.…”
Section: Theorymentioning
confidence: 99%
“…The thermal conductivity components at different temperatures were calculated according to the relevant equation, and are shown in CrystEngComm Paper of 5.97 W (m K) −1 for SLN, 5.62 W (m K) −1 for MgOSLN, 40 3.75 W (m K) −1 for CLN and 4.63 W (m K) −1 for MgOCLN. 32 These results are likely to be caused by a very small amount of intrinsic defects in the crystal, which could also lead to more phonon scattering.…”
Section: Thermal Propertiesmentioning
confidence: 99%