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By S. Hutagalung

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1-17. , Rudolph, P. & Fukuda, T. (1998). “Czochralski growth of RE3Ga5SiO14 (RE=La, Pr, Nd) single crystals for the analysis of the influence of rare earth substitution on piezoelectricity” J. Crystal Growth, 191, pp. 746-753. , (1999). “Crystal Growth and Characterization of New Langasite-type Compounds for Piezoelecteic Applications” Proceedings of The 9th US-Japan on Dielectric and Piezoelectric Ceramics, held November 2-5, Rizzan Sea Park Hotel, Tancha Bay, Okinawa, Japan. , (1996). “Growth and characterization of lanthanum gallium silicate La3Ga5SiO14 single crystals for piezoelectric applications” J.

D) and (e) show the crystal structure along [100] and [120] showing asymmetry and symmetry, respectively. Dipole moment will be appeared in (d). Figure 11(a) shows equivalent series resistance as a function of vibration modes of resonators on the LGS and quartz single crystals (Shimamura, 1996). The resistance of LGS is one order smaller than that of quartz. So, as if the surface roughness of LGS is large, high frequency oscillation is easy. Moreover, as the equivalent series resistances at high vibration mode as 7th and 9th are small, LGS filter is useful for high frequency wave area filter.

45o 13 11 16 9 2 10 2 12 14 15 10 mm 8 3 6 7 4 5 1 2 (1) diamond anvils (2) beryllium diamond support disc (3) gasket (4) spacer ring (5) epoxy resin (6) adhesive (7) single crystal (8) ruby (9) hemispherical plate (10) disc-shaped plate (11) inclined adjusting screw (12) lateral-position adjusting screw (13) driver screw (14) lower sliding piston (15) cylindrical sleeve (16) upper stationary disc Fig. 20. Schematic cross section of diamond anvil cell. LGS Pressure (GPa) Atm. 03 Atm. 30 Table 6.

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