Journal of Inorganic Materials ›› 2025, Vol. 40 ›› Issue (2): 128-144.DOI: 10.15541/jim20240355
• REVIEW • Previous Articles Next Articles
TAO Guilong1,2(), ZHI Guowei2, LUO Tianyou2, OUYANG Peidong2, YI Xinyan3, LI Guoqiang1,2,3(
)
Received:
2024-07-27
Revised:
2024-09-12
Published:
2025-02-20
Online:
2024-11-25
Contact:
LI Guoqiang, professor. E-mail: msgli@scut.edu.cnAbout author:
TAO Guilong (1988-), male, PhD candidate. E-mail: ictgl@mail.scut.edu.cn
Supported by:
CLC Number:
TAO Guilong, ZHI Guowei, LUO Tianyou, OUYANG Peidong, YI Xinyan, LI Guoqiang. Progress on Key Technologies of Cavity-structured Thin Film Bulk Acoustic Wave Filter[J]. Journal of Inorganic Materials, 2025, 40(2): 128-144.
Filter type | SAW filter | BAW filter |
---|---|---|
Characteristic | High stability, low insertion loss (2-4 dB) | High stability, low insertion loss (0.8-1.5 dB), high power tolerance |
Applicable frequency range | 10 MHz-3 GHz | 1.5-6 GHz, the maximum up to over 10 GHz |
Advantage | Smaller than the traditional ceramic filter, flexible, mature technology, high reliability | Suitable for high frequency, insensitive to temperature changes, miniaturized vertical propagation in acoustic wave, decreased size according to frequency increase |
Limitation | Poor thermal stability, decreased Q-value when operating frequency exceeds 1.5 GHz | High manufacturing cost, complex manufacturing process |
Table 1 Technical characteristics of SAW filter and BAW filter
Filter type | SAW filter | BAW filter |
---|---|---|
Characteristic | High stability, low insertion loss (2-4 dB) | High stability, low insertion loss (0.8-1.5 dB), high power tolerance |
Applicable frequency range | 10 MHz-3 GHz | 1.5-6 GHz, the maximum up to over 10 GHz |
Advantage | Smaller than the traditional ceramic filter, flexible, mature technology, high reliability | Suitable for high frequency, insensitive to temperature changes, miniaturized vertical propagation in acoustic wave, decreased size according to frequency increase |
Limitation | Poor thermal stability, decreased Q-value when operating frequency exceeds 1.5 GHz | High manufacturing cost, complex manufacturing process |
Fig. 1 Operating principle of the L-type FBAR filter (a) Electrical characteristics of the idealized FBAR; (b) Fundamental unit of the L-type structure; (c) Transmission response
Fig. 2 FBAR and the equivalent circuit model of piezoelectric thin film (a) Schematic structure of FBAR; (b) Mason equivalent circuit model of the piezoelectric thin film
Fig. 7 Discretized model and electrode feed lines of BAW resonator[36] (a) Schematic representation of discretized resonator model; (b) Two resonators in series and connected by broad lead; (c) Single resonator connected by narrow lead
Fig. 8 3.55 GHz FBAR filter based on single-crystal and polycrystalline AlN[54] (a) Measured power sweep at right band edge of the filters; (b) Measured insertion loss of the filters versus input power
Fig. 11 Experimental results of FBAR filter fabricated with Al0.8Sc0.2N film[65] (a) Transmission response of FBAR filter; (b) Return loss of the FBAR filter
Fig. 12 Effect of Sc-dopant concentration on crystal quality and surface morphology of Al1−xScxN thin films[69] (a-c) TEM dark-field images and electron diffraction patterns for 10%, 31%, and 42% Sc content; (d-f) Corresponding SEM plane views
Fig. 13 Performance comparison of FBAR obtained by two-step (Sample 1) and single PVD (Sample 2) processes[86] (a) Frequency impedance characteristic curves; (b) Smith chart
Fig. 14 Schematic diagram for SABAR process[87] (a) Combination of PLD and MOCVD AlN film; (b) Bottom electrode and bonding layer sputtered on top of AlN layer; (c) Resonator structure
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