JPS57206117A - Miniature quartz oscillator - Google Patents
Miniature quartz oscillatorInfo
- Publication number
- JPS57206117A JPS57206117A JP9189981A JP9189981A JPS57206117A JP S57206117 A JPS57206117 A JP S57206117A JP 9189981 A JP9189981 A JP 9189981A JP 9189981 A JP9189981 A JP 9189981A JP S57206117 A JPS57206117 A JP S57206117A
- Authority
- JP
- Japan
- Prior art keywords
- oscillator
- oscillation mode
- caused
- oscillating
- displacement
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000010453 quartz Substances 0.000 title 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 title 1
- 230000010355 oscillation Effects 0.000 abstract 3
- 238000006073 displacement reaction Methods 0.000 abstract 2
- 230000000694 effects Effects 0.000 abstract 1
- 238000005259 measurement Methods 0.000 abstract 1
- 238000000034 method Methods 0.000 abstract 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
- H03H9/02—Details
- H03H9/05—Holders; Supports
- H03H9/0504—Holders; Supports for bulk acoustic wave devices
- H03H9/0514—Holders; Supports for bulk acoustic wave devices consisting of mounting pads or bumps
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
- H03H9/02—Details
- H03H9/125—Driving means, e.g. electrodes, coils
- H03H9/13—Driving means, e.g. electrodes, coils for networks consisting of piezoelectric or electrostrictive materials
- H03H9/132—Driving means, e.g. electrodes, coils for networks consisting of piezoelectric or electrostrictive materials characterized by a particular shape
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
- H03H9/15—Constructional features of resonators consisting of piezoelectric or electrostrictive material
- H03H9/17—Constructional features of resonators consisting of piezoelectric or electrostrictive material having a single resonator
- H03H9/19—Constructional features of resonators consisting of piezoelectric or electrostrictive material having a single resonator consisting of quartz
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
- H03H9/46—Filters
- H03H9/54—Filters comprising resonators of piezoelectric or electrostrictive material
- H03H9/56—Monolithic crystal filters
Landscapes
- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Abstract
PURPOSE:To obtain an oscillator using a secondary contour oscillation mode, by providing an appropriate electrode on an oscillator containing an oscillating part and a supporting part formed in a body. CONSTITUTION:A supporting part 13 has such measurement and shape with which the oscillation mode is hardly disturbed at an oscillating part 11 and at the same time the displacement is hardly caused at a sealed part 18. Thus an effect caused when the part 18 is joined mechanically and electrically can be avoided. Then an electrode shown in the figure is formed by a photolithographic technique on an oscillator in which the supporting part 13 with which no displacement is caused at the part 18 is unified with the oscillating part 11. In such way, an oscillator is obtained with a high resonance frequency that so far has the limitation just by the basic contour oscillation mode.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9189981A JPS57206117A (en) | 1981-06-15 | 1981-06-15 | Miniature quartz oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9189981A JPS57206117A (en) | 1981-06-15 | 1981-06-15 | Miniature quartz oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS57206117A true JPS57206117A (en) | 1982-12-17 |
Family
ID=14039409
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9189981A Pending JPS57206117A (en) | 1981-06-15 | 1981-06-15 | Miniature quartz oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS57206117A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01181215A (en) * | 1988-01-13 | 1989-07-19 | Kinseki Ltd | Crystal vibrator |
-
1981
- 1981-06-15 JP JP9189981A patent/JPS57206117A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01181215A (en) * | 1988-01-13 | 1989-07-19 | Kinseki Ltd | Crystal vibrator |
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