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| Content Provider | IEEE Xplore Digital Library |
|---|---|
| Author | Imbaud, J. Assoud, A. Bourquin, R. Boy, J.J. Galliou, S. Romand, J.P. |
| Copyright Year | 2007 |
| Description | Author affiliation: FEMTO-ST Inst. UMR CNRS 6174, Besancon (Imbaud, J.; Assoud, A.; Bourquin, R.; Boy, J.J.; Galliou, S.; Romand, J.P.) |
| Abstract | Materials in the LGT family are promising for designing bulk acoustic wave resonators with high quality factor. In our laboratory, we have manufactured a lot of planoconvex 10 MHz $5^{th}$ overtone Y-cut resonators using LGS (langasite $La_{3}Ga_{5}SiO_{14})$ and LGT (langatate $La_{3}Ga_{5.5}Ta_{0.5}O_{14})$ crystals. Our initial aim was to do noise measurements on these home-made resonators but problems occurred during manufacturing. It was the opportunity for further investigations. Indeed, we observed that the quality factor depends strongly on the energy trapping, the polishing method and the materials quality from one supplier to another. As for the quartz crystal, we have found that the material quality can be qualified by IR spectrometry whose resulting spectra exhibit absorption peaks more or less deep, linked to defects. These predominant criteria are not surprising but although they are nowadays quite well-defined in the case of quartz crystal resonators, they have to be defined again in the case of these LGS and LGT crystals. Then, a satisfying machining and polishing method has been first applied to elaborate high Q resonators. A comparison between different grades of LGS and LGT materials is established. In addition, LGT resonators are characterized by their motional parameters and frequency-temperature curves. Nevertheless, one of the main results is that the measured Q-f product is not the expected one. We present results of Q-factor versus radius of curvature and their comparison with the theoretical approach. It appears that an optimization should be performed. Right now the best resonator that we have made has got a Q-f product of 1.4 $10^{13}$ on its $5^{th}$ overtone (1.7 $10^{13}$ on its $9^{th}$ overtone). This result is slightly higher than the similar parameter obtained on a SC-cut quartz crystal resonator working at the same frequency. |
| Starting Page | 711 |
| Ending Page | 714 |
| File Size | 481526 |
| Page Count | 4 |
| File Format | |
| ISBN | 9781424406463 |
| ISSN | 10756787 |
| DOI | 10.1109/FREQ.2007.4319167 |
| Language | English |
| Publisher | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Publisher Date | 2007-05-29 |
| Publisher Place | Switzerland |
| Access Restriction | Subscribed |
| Rights Holder | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Subject Keyword | Crystalline materials Q factor Manufacturing Crystals Frequency Acoustic materials Acoustic waves Laboratories Noise measurement Infrared spectra |
| Content Type | Text |
| Resource Type | Article |
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