CA1297172C - Method of precisely adjusting the frequency of a piezoelectric resonator - Google Patents
Method of precisely adjusting the frequency of a piezoelectric resonatorInfo
- Publication number
- CA1297172C CA1297172C CA000557688A CA557688A CA1297172C CA 1297172 C CA1297172 C CA 1297172C CA 000557688 A CA000557688 A CA 000557688A CA 557688 A CA557688 A CA 557688A CA 1297172 C CA1297172 C CA 1297172C
- Authority
- CA
- Canada
- Prior art keywords
- resonator
- frequency
- insulating film
- appropriate fraction
- area
- 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.)
- Expired - Fee Related
Links
- 238000000034 method Methods 0.000 title claims abstract description 38
- 229920001721 polyimide Polymers 0.000 claims description 21
- CBENFWSGALASAD-UHFFFAOYSA-N Ozone Chemical compound [O-][O+]=O CBENFWSGALASAD-UHFFFAOYSA-N 0.000 claims description 8
- 238000000151 deposition Methods 0.000 claims description 7
- 239000010453 quartz Substances 0.000 claims description 7
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims description 7
- 238000013461 design Methods 0.000 claims description 4
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims description 3
- 229910052782 aluminium Inorganic materials 0.000 claims description 3
- 238000001020 plasma etching Methods 0.000 claims description 3
- 238000010894 electron beam technology Methods 0.000 claims description 2
- 238000010849 ion bombardment Methods 0.000 claims description 2
- 238000010943 off-gassing Methods 0.000 claims description 2
- 238000004544 sputter deposition Methods 0.000 claims description 2
- 230000007306 turnover Effects 0.000 claims description 2
- 238000001074 Langmuir--Blodgett assembly Methods 0.000 claims 2
- 230000000593 degrading effect Effects 0.000 abstract 1
- 239000010410 layer Substances 0.000 description 12
- 239000004642 Polyimide Substances 0.000 description 11
- 239000002356 single layer Substances 0.000 description 5
- 238000004140 cleaning Methods 0.000 description 3
- 238000010884 ion-beam technique Methods 0.000 description 2
- 238000002360 preparation method Methods 0.000 description 2
- 238000001771 vacuum deposition Methods 0.000 description 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000003486 chemical etching Methods 0.000 description 1
- 238000005520 cutting process Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000005442 molecular electronic Methods 0.000 description 1
- 239000000178 monomer Substances 0.000 description 1
- 239000011368 organic material Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 238000007747 plating Methods 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 238000010897 surface acoustic wave method Methods 0.000 description 1
- 238000010408 sweeping Methods 0.000 description 1
- UFHILTCGAOPTOV-UHFFFAOYSA-N tetrakis(ethenyl)silane Chemical compound C=C[Si](C=C)(C=C)C=C UFHILTCGAOPTOV-UHFFFAOYSA-N 0.000 description 1
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B05—SPRAYING OR ATOMISING IN GENERAL; APPLYING FLUENT MATERIALS TO SURFACES, IN GENERAL
- B05D—PROCESSES FOR APPLYING FLUENT MATERIALS TO SURFACES, IN GENERAL
- B05D1/00—Processes for applying liquids or other fluent materials
- B05D1/18—Processes for applying liquids or other fluent materials performed by dipping
- B05D1/20—Processes for applying liquids or other fluent materials performed by dipping substances to be applied floating on a fluid
- B05D1/202—Langmuir Blodgett films (LB films)
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y30/00—Nanotechnology for materials or surface science, e.g. nanocomposites
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y40/00—Manufacture or treatment of nanostructures
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H3/00—Apparatus or processes specially adapted for the manufacture of impedance networks, resonating circuits, resonators
- H03H3/007—Apparatus or processes specially adapted for the manufacture of impedance networks, resonating circuits, resonators for the manufacture of electromechanical resonators or networks
- H03H3/02—Apparatus or processes specially adapted for the manufacture of impedance networks, resonating circuits, resonators for the manufacture of electromechanical resonators or networks for the manufacture of piezoelectric or electrostrictive resonators or networks
- H03H3/04—Apparatus or processes specially adapted for the manufacture of impedance networks, resonating circuits, resonators for the manufacture of electromechanical resonators or networks for the manufacture of piezoelectric or electrostrictive resonators or networks for obtaining desired frequency or temperature coefficient
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10T—TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
- Y10T29/00—Metal working
- Y10T29/42—Piezoelectric device making
Abstract
ABSTRACT
The frequency of a piezoelectric resonator is precisely adjusted using monomolecular layer(s) of a thermally stable, low stress, uniform insulating film deposited on the active area of the resonator. The method is particularly suitable for precisely adjusting the frequencies of high frequency (i.e., very thin) resonators, and the frequencies of lateral field resonators, without degrading stability.
The frequency of a piezoelectric resonator is precisely adjusted using monomolecular layer(s) of a thermally stable, low stress, uniform insulating film deposited on the active area of the resonator. The method is particularly suitable for precisely adjusting the frequencies of high frequency (i.e., very thin) resonators, and the frequencies of lateral field resonators, without degrading stability.
Description
This invention relates to a method of precisely adjusting the frequency of a piezoelectric resonator.
Art established techniques such as vacuum deposition, have been used heretofore for adjusting the frequencies of conventional resonators. These techniques are discussed, for example, in U.S. Patent No. 4,107,349, issued August 15, 1978 to John R. Vig.
A difficulty has arisen however, in that the resonator art in the past several years has been extended to ultra high frequency (UHF) and lateral field (LF) resonators. No satisfactory techniques have existed heretofore for precisely adjusting the frequencies of UHF and LF resonators.
The general object of this invention is to provide a method of precisely adjusting the frequency of a piezoelectric resonator. A more particular object of the invention is to provide such a method where the piezoelectric resonator is a UHF
or LF resonator.
~9~ 2 It has now been found that the aforementioned objects can be attained using monomolecular layer(s) of a thermally stable, low stress, uniform insulating film deposited on the active area of the resonator.
More particularly, according to the invention, the frequency of a piezoelectric resonator is precisely adjusted by a method including the steps of: -(A) fabricating the resonator by means of art established techniques, (a) adjusting the frequency of the resonator with an accuracy that is equivalent to about +l atomic layer of quartz, (C) measuring the frequency of the resonator under a well defined set of experimental conditions, (D) depositing a monomolecular layer of a thermally stable, low stress, uniform insulating film on the active area of the resonator and outgassing the film thoroughly, (E) measuring the frequency of the resonator under the same set of experimental conditions as in step (C), (F) calculating the difference between the frequencies ~0 measured in steps (C) and (E) as the size of the step change in frequency for the particular resonator design and insulating film, (G) deciding on the frequency adjustment tolerance desired and converting that frequency adjustment tolerance to an insulating film area tolerance, and (H) removing the appropriate fraction of the insulating film area.
In step (A), the resonator is first fabricated by art ~X9~
established techniques including growing a suitable piezoelectric material as for example quartz, sweeping quartz, cutting, lapping, rounding, contouring, chemical etching, cleaning, depositing contacts, preparing an enclosure, rnounting, bonding, cleaning, baking, plating, etc.
In step (B), the frequency can be adjusted by art established techniques as for example, by vacuum deposition of a gold or aluminum film with an accuracy that is equivalent to about ~1 atomic layer of quartz. In general, for thickness field resonators, the insulating film can then be less than or about equal to one or two molecular layers. For lateral field resonators, more than a single layer may often be required. I
In step (C), the frequency of the resonator is measured under a well defined set of experimental conditions, as for example, conditions of temperature, pressure and load capacitance.
~ n step (D), a monomolecular layer of a thermally stable, low stress, uniform insulating film is deposited on the active area of the resonator and the film thoroughly outgassed. A
convenient method of depositing the film uses the Langmuir-~0 Blodgett (LB) technique. The LB technique can deposit a highlyordered monomolecular layer of the film. Thicker films can be `'built" one atomic layer at a time. Ls films are prepared by transferring floating organic monolayers onto solid substrates.
The preparation, properties and applications of LB films are reviewed in "An Applied Science Perspective of Langmuir-Blodgett Films" by G.G. Roberts, in ~dvances in Physics, Vol. 3~, pp 475-512, 1985. The low thermal stability of conventional L~ films have now been overcome with the preparation of polyimide LB films, as is described in the "Formation and Properties of Ultra Thin Polyimide Films Through the Langmuir-810dgett Technique" by MasazakU Uekita, Hiroshi Awaji and Makoto Murata, at the third International Symposium on Molecular Electronic Devices, Arlington, VA, 6-8 October 1986. A monolayer of polyimide LB film weighs about 0.55 times as much as a monolayer of quartz. Such an Ls film can, therefore, be very u~eful for adju~ting the frequency of quartz resonators.
In step (E), the frequency of the resonator is measured under the same set of experimental conditions as in step (C).
In step (F), the difference between the frequencies measured in steps (C) and (E) is calculated as the size of the step change in frequency for the particular resonator design and in~ulating film. For ultrahigh frequency re~onators, ~tress effects due to the film may need to be considered in the calculation.
In step (G), the frequency adjustment tolerance desired is decided and the frequency adjustment tolerance converted to an insulating film area tolerance.
In step (H), the appropriate fraction of the insulating area is removed. When the film is of an organic material, the appropriate fraction of the film can be removed by irradiating the appropriate area of the film with short wavelength ultraviolet light in the presence of oxygen, that is, by means of UV/ozone cleaning. The UV/ozone will remove the organic film wherever the resonator surface is exposed to UV/ozone. The UV/ozone treatment will leave behind a clean surface. The portion of the film that is shielded from the UV/ozone will remain on the resonator. For ~2~ 7~
example, the appropriate portion of the resonator surface can be exposed to ~V/ozone by means of a ~V-opaque non-reflecting mask, for example, one that is made of stainless steel. ~nother method is to raster a short wavelength UV laser as for example, an excimer laser~until the appropriate portion of the film is removed.
Other Methods of removing portions of the film are sputtering, ion bombardment, reactive ion etching, and by means of an electron beam. For example, one can form a precise polyimide pattern on the resonator surfaces by depositing as for example, by an ion beam assisted reaction, thin etch barrier layers from monomer vapors, such as tetravinylsilane, through a self supporting mask, on top of the polyimide films, then use oxygen-reactive ion etching for polyimide patterns development.
Other means of forming a precise polyimide pattern include rastering an elect~on beam or an ion beam in order to remove the appropriate fraction of the polyimide film.
A 100 MHz ~1 ppm resonator is needed for an oscillator intended for use in a radar system. It is therefore necessary to ~O adjust the frequency of a 100 MHz fundamental mode, AT-cut thickness field resonator to an accuracy of ~1 ppm by means of a polyimide Ls film. Tha approximate frequency change per monolayer of polyimide will be = (1.7 x lO 7)~ MHz b72 where ~ MHZ i~ the ~requency in megahert~. There~ore, = 17 ppm at lOO MHz. Therefore, in order to obtain frequency adjustment accuracy of +1 ppm, the area of the monolayer polyimide film must be controlled with an accuracy of about +1/17 atomic layer.
The 100 MHz fundamental mode AT-Cut resonator is first fabricated by art established techniques. Aluminum electrodes are deposited and the electrode thickness adjusted so that the resonator frequency is as close as possible and above 100 MHz when the resonator is in a vacuum and at its upper turnover temperature which is about 11~C. The measurement is made under well defined conditions of temperature, pressure, and load capacitance. That is, the temperature is 71C+2C, the pressure is below 10 ~ torr, and the load capacitance is 20pf~0.5pf. The fre~uency is found to be 100.~00864 ~Hz. Thus, the frequency must be lowered by 864 Hz. The 864 Hz corresponds to 8.64 ppm, or 8 ~ = 50.8% of an atomic layer of polyimide LB film. An atomic layer of polyimide LB film is then deposited onto the active area of the resonator;
49.2~ of the polyimide LB film deposited is then removed by means of irradiation with short wavelength ozone-generating UV light through a mask that permits the exposure o~ only 49.2% of the film to the uV/ozone. Subsequent to the UV irr~diation, the resonator frequency is found to be 99.999998 MHz.
In the foregoing embodiment, in lieu of the polyimide LB
film deposited, other thermally stable films deposited by other techniques could be used.
The method of the invention is applicable to bulk acoustic wave devices, surface acoustic wave devices, shallow bulk 3 ~ 7~
acoustic wave devices, and other piezoelectric resonators, delay lines, sensors, transducers, etc. . s I wish it to be understood that I do not desire to be 1.
limited to the exact details as described for obvious modifications will occur to a person skilled in the art.
Art established techniques such as vacuum deposition, have been used heretofore for adjusting the frequencies of conventional resonators. These techniques are discussed, for example, in U.S. Patent No. 4,107,349, issued August 15, 1978 to John R. Vig.
A difficulty has arisen however, in that the resonator art in the past several years has been extended to ultra high frequency (UHF) and lateral field (LF) resonators. No satisfactory techniques have existed heretofore for precisely adjusting the frequencies of UHF and LF resonators.
The general object of this invention is to provide a method of precisely adjusting the frequency of a piezoelectric resonator. A more particular object of the invention is to provide such a method where the piezoelectric resonator is a UHF
or LF resonator.
~9~ 2 It has now been found that the aforementioned objects can be attained using monomolecular layer(s) of a thermally stable, low stress, uniform insulating film deposited on the active area of the resonator.
More particularly, according to the invention, the frequency of a piezoelectric resonator is precisely adjusted by a method including the steps of: -(A) fabricating the resonator by means of art established techniques, (a) adjusting the frequency of the resonator with an accuracy that is equivalent to about +l atomic layer of quartz, (C) measuring the frequency of the resonator under a well defined set of experimental conditions, (D) depositing a monomolecular layer of a thermally stable, low stress, uniform insulating film on the active area of the resonator and outgassing the film thoroughly, (E) measuring the frequency of the resonator under the same set of experimental conditions as in step (C), (F) calculating the difference between the frequencies ~0 measured in steps (C) and (E) as the size of the step change in frequency for the particular resonator design and insulating film, (G) deciding on the frequency adjustment tolerance desired and converting that frequency adjustment tolerance to an insulating film area tolerance, and (H) removing the appropriate fraction of the insulating film area.
In step (A), the resonator is first fabricated by art ~X9~
established techniques including growing a suitable piezoelectric material as for example quartz, sweeping quartz, cutting, lapping, rounding, contouring, chemical etching, cleaning, depositing contacts, preparing an enclosure, rnounting, bonding, cleaning, baking, plating, etc.
In step (B), the frequency can be adjusted by art established techniques as for example, by vacuum deposition of a gold or aluminum film with an accuracy that is equivalent to about ~1 atomic layer of quartz. In general, for thickness field resonators, the insulating film can then be less than or about equal to one or two molecular layers. For lateral field resonators, more than a single layer may often be required. I
In step (C), the frequency of the resonator is measured under a well defined set of experimental conditions, as for example, conditions of temperature, pressure and load capacitance.
~ n step (D), a monomolecular layer of a thermally stable, low stress, uniform insulating film is deposited on the active area of the resonator and the film thoroughly outgassed. A
convenient method of depositing the film uses the Langmuir-~0 Blodgett (LB) technique. The LB technique can deposit a highlyordered monomolecular layer of the film. Thicker films can be `'built" one atomic layer at a time. Ls films are prepared by transferring floating organic monolayers onto solid substrates.
The preparation, properties and applications of LB films are reviewed in "An Applied Science Perspective of Langmuir-Blodgett Films" by G.G. Roberts, in ~dvances in Physics, Vol. 3~, pp 475-512, 1985. The low thermal stability of conventional L~ films have now been overcome with the preparation of polyimide LB films, as is described in the "Formation and Properties of Ultra Thin Polyimide Films Through the Langmuir-810dgett Technique" by MasazakU Uekita, Hiroshi Awaji and Makoto Murata, at the third International Symposium on Molecular Electronic Devices, Arlington, VA, 6-8 October 1986. A monolayer of polyimide LB film weighs about 0.55 times as much as a monolayer of quartz. Such an Ls film can, therefore, be very u~eful for adju~ting the frequency of quartz resonators.
In step (E), the frequency of the resonator is measured under the same set of experimental conditions as in step (C).
In step (F), the difference between the frequencies measured in steps (C) and (E) is calculated as the size of the step change in frequency for the particular resonator design and in~ulating film. For ultrahigh frequency re~onators, ~tress effects due to the film may need to be considered in the calculation.
In step (G), the frequency adjustment tolerance desired is decided and the frequency adjustment tolerance converted to an insulating film area tolerance.
In step (H), the appropriate fraction of the insulating area is removed. When the film is of an organic material, the appropriate fraction of the film can be removed by irradiating the appropriate area of the film with short wavelength ultraviolet light in the presence of oxygen, that is, by means of UV/ozone cleaning. The UV/ozone will remove the organic film wherever the resonator surface is exposed to UV/ozone. The UV/ozone treatment will leave behind a clean surface. The portion of the film that is shielded from the UV/ozone will remain on the resonator. For ~2~ 7~
example, the appropriate portion of the resonator surface can be exposed to ~V/ozone by means of a ~V-opaque non-reflecting mask, for example, one that is made of stainless steel. ~nother method is to raster a short wavelength UV laser as for example, an excimer laser~until the appropriate portion of the film is removed.
Other Methods of removing portions of the film are sputtering, ion bombardment, reactive ion etching, and by means of an electron beam. For example, one can form a precise polyimide pattern on the resonator surfaces by depositing as for example, by an ion beam assisted reaction, thin etch barrier layers from monomer vapors, such as tetravinylsilane, through a self supporting mask, on top of the polyimide films, then use oxygen-reactive ion etching for polyimide patterns development.
Other means of forming a precise polyimide pattern include rastering an elect~on beam or an ion beam in order to remove the appropriate fraction of the polyimide film.
A 100 MHz ~1 ppm resonator is needed for an oscillator intended for use in a radar system. It is therefore necessary to ~O adjust the frequency of a 100 MHz fundamental mode, AT-cut thickness field resonator to an accuracy of ~1 ppm by means of a polyimide Ls film. Tha approximate frequency change per monolayer of polyimide will be = (1.7 x lO 7)~ MHz b72 where ~ MHZ i~ the ~requency in megahert~. There~ore, = 17 ppm at lOO MHz. Therefore, in order to obtain frequency adjustment accuracy of +1 ppm, the area of the monolayer polyimide film must be controlled with an accuracy of about +1/17 atomic layer.
The 100 MHz fundamental mode AT-Cut resonator is first fabricated by art established techniques. Aluminum electrodes are deposited and the electrode thickness adjusted so that the resonator frequency is as close as possible and above 100 MHz when the resonator is in a vacuum and at its upper turnover temperature which is about 11~C. The measurement is made under well defined conditions of temperature, pressure, and load capacitance. That is, the temperature is 71C+2C, the pressure is below 10 ~ torr, and the load capacitance is 20pf~0.5pf. The fre~uency is found to be 100.~00864 ~Hz. Thus, the frequency must be lowered by 864 Hz. The 864 Hz corresponds to 8.64 ppm, or 8 ~ = 50.8% of an atomic layer of polyimide LB film. An atomic layer of polyimide LB film is then deposited onto the active area of the resonator;
49.2~ of the polyimide LB film deposited is then removed by means of irradiation with short wavelength ozone-generating UV light through a mask that permits the exposure o~ only 49.2% of the film to the uV/ozone. Subsequent to the UV irr~diation, the resonator frequency is found to be 99.999998 MHz.
In the foregoing embodiment, in lieu of the polyimide LB
film deposited, other thermally stable films deposited by other techniques could be used.
The method of the invention is applicable to bulk acoustic wave devices, surface acoustic wave devices, shallow bulk 3 ~ 7~
acoustic wave devices, and other piezoelectric resonators, delay lines, sensors, transducers, etc. . s I wish it to be understood that I do not desire to be 1.
limited to the exact details as described for obvious modifications will occur to a person skilled in the art.
Claims (13)
1. Method of precisely adjusting the frequency of a piezoelectric resonator, said method including the steps of:
(A) fabricating the resonator by means of art established techniques, (B) adjusting the frequency of the resonator with an accuracy that is equivalent to about ?1 atomic layer of quartz, (C) measuring the frequency of the resonator under a well defined set of experimental conditions, (D) depositing a monomolecular layer of a thermally stable, low stress, uniform insulating film on the active area of the resonator and outgassing the film thoroughly, (E) measuring the frequency of the resonator under the same set of experimental conditions as in step (C), (F) calculating the difference between the frequencies measured in steps (C) and (E) as the size of the step change in frequency for the particular resonator design and insulating film, (G) deciding on the frequency adjustment tolerance desired and converting that frequency adjustment tolerance to an insulating film area tolerance, and (H) removing the appropriate fraction of the insulating film area.
(A) fabricating the resonator by means of art established techniques, (B) adjusting the frequency of the resonator with an accuracy that is equivalent to about ?1 atomic layer of quartz, (C) measuring the frequency of the resonator under a well defined set of experimental conditions, (D) depositing a monomolecular layer of a thermally stable, low stress, uniform insulating film on the active area of the resonator and outgassing the film thoroughly, (E) measuring the frequency of the resonator under the same set of experimental conditions as in step (C), (F) calculating the difference between the frequencies measured in steps (C) and (E) as the size of the step change in frequency for the particular resonator design and insulating film, (G) deciding on the frequency adjustment tolerance desired and converting that frequency adjustment tolerance to an insulating film area tolerance, and (H) removing the appropriate fraction of the insulating film area.
2. Method according to Claim 1 wherein the resonator is a thickness field resonator.
3. Method according to Claim 1 wherein the resonator is a lateral field resonator.
4. Method according to Claim 1 wherein the well defined set of experimental conditions include temperature, pressure, and load capacitance.
5. Method according to Claim 1 wherein the insulating film deposited is a polyimide film.
6. Method according to Claim 5 wherein the polyimide film is deposited by the Langmuir-Blodgett technique.
7. Method according to Claim 1 wherein the appropriate fraction of the insulating film area is removed by UV/ozone treatment.
8. Method according to Claim 1 wherein the appropriate fraction of the insulating film area is removed by rastering a short wavelength UV laser until the appropriate portion of the film is removed.
9. Method according to Claim 1 wherein the appropriate fraction of the insulating film area is removed by rastering an electron beam until the appropriate portion of the film is removed.
10. Method according to Claim 1 wherein the appropriate fraction of the insulating film area is removed by sputtering.
11. Method according to Claim 1 wherein the appropriate fraction of the insulating film area is removed by ion bombardment.
12. Method according to Claim 1 wherein the appropriate fraction of the insulating film area is removed by reactive ion etching.
13. Method of adjusting the frequency of a 100 MHz fundamental mode, AT-cut thickness field resonator to an accuracy of ?1 ppm, said method including steps of:
(A) fabricating the 100 MHz fundamental mode, AT-cut thickness field resonator by means of art established techniques, (B) depositing aluminum electrodes and adjusting the electrode thickness so that the resonator frequency is as close as possible to and above 100 MHz when the resonator is in a vacuum and at its upper turnover temperature of about 71°C, (C) measuring the frequency of the resonator under well defined conditions of a temperature of 71°C?2°C, a pressure of below 10-6 torr, and a load capacitance of 20pf?0.5pf, (D) depositing a monomolecular layer of polyimide film obtained by the Langmuir-Blodgett technique onto the active area of the resonator, (E) measuring the frequency of the resonator under the same set of experimental conditions as in step (C), (F) calculating the difference between the frequencies measured in steps (C) and (E) as the size of the step change in frequency for the particular resonator design and polyimide film, (G) deciding on the frequency adjustment tolerance desired and converting that frequency adjustment to a polyimide film area tolerance, and (H) removing the appropriate fraction of the polyimide film area by means of irradiation with short wavelength ozone-generating ultraviolet light through a mask.
(A) fabricating the 100 MHz fundamental mode, AT-cut thickness field resonator by means of art established techniques, (B) depositing aluminum electrodes and adjusting the electrode thickness so that the resonator frequency is as close as possible to and above 100 MHz when the resonator is in a vacuum and at its upper turnover temperature of about 71°C, (C) measuring the frequency of the resonator under well defined conditions of a temperature of 71°C?2°C, a pressure of below 10-6 torr, and a load capacitance of 20pf?0.5pf, (D) depositing a monomolecular layer of polyimide film obtained by the Langmuir-Blodgett technique onto the active area of the resonator, (E) measuring the frequency of the resonator under the same set of experimental conditions as in step (C), (F) calculating the difference between the frequencies measured in steps (C) and (E) as the size of the step change in frequency for the particular resonator design and polyimide film, (G) deciding on the frequency adjustment tolerance desired and converting that frequency adjustment to a polyimide film area tolerance, and (H) removing the appropriate fraction of the polyimide film area by means of irradiation with short wavelength ozone-generating ultraviolet light through a mask.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US046,347 | 1987-05-06 | ||
US07/046,347 US4761298A (en) | 1987-05-06 | 1987-05-06 | Method of precisely adjusting the frequency of a piezoelectric resonator |
Publications (1)
Publication Number | Publication Date |
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CA1297172C true CA1297172C (en) | 1992-03-10 |
Family
ID=21942971
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CA000557688A Expired - Fee Related CA1297172C (en) | 1987-05-06 | 1988-01-29 | Method of precisely adjusting the frequency of a piezoelectric resonator |
Country Status (2)
Country | Link |
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US (1) | US4761298A (en) |
CA (1) | CA1297172C (en) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4931752A (en) * | 1987-09-30 | 1990-06-05 | Hewlett-Packard Company | Polyimide damper for surface acoustic wave device |
US5019451A (en) * | 1989-04-27 | 1991-05-28 | Edison Polymer Innovation Corp. | Non-centrosymmetric, multi-layer Langmuir-Blodgett films |
US5530408A (en) * | 1995-05-25 | 1996-06-25 | The United States Of America As Represented By The Secretary Of The Army | Method of making an oven controlled crystal oscillator the frequency of which remains ultrastable under temperature variations |
US6456173B1 (en) * | 2001-02-15 | 2002-09-24 | Nokia Mobile Phones Ltd. | Method and system for wafer-level tuning of bulk acoustic wave resonators and filters |
US6480074B1 (en) * | 2001-04-27 | 2002-11-12 | Nokia Mobile Phones Ltd. | Method and system for wafer-level tuning of bulk acoustic wave resonators and filters by reducing thickness non-uniformity |
Family Cites Families (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4252839A (en) * | 1976-12-29 | 1981-02-24 | Citizen Watch Company Limited | Tuning fork-type quartz crystal vibrator and method of forming the same |
US4107349A (en) * | 1977-08-12 | 1978-08-15 | The United States Of America As Represented By The Secretary Of The Army | Method of adjusting the frequency of piezoelectric resonators |
US4232239A (en) * | 1979-03-16 | 1980-11-04 | Motorola, Inc. | Frequency adjustment of piezoelectric resonator utilizing low energy oxygen glow device for anodizing electrodes |
US4396704A (en) * | 1981-04-22 | 1983-08-02 | Bell Telephone Laboratories, Incorporated | Solid state devices produced by organometallic plasma developed resists |
US4417948A (en) * | 1982-07-09 | 1983-11-29 | International Business Machines Corporation | Self developing, photoetching of polyesters by far UV radiation |
US4414059A (en) * | 1982-12-09 | 1983-11-08 | International Business Machines Corporation | Far UV patterning of resist materials |
US4654118A (en) * | 1986-03-17 | 1987-03-31 | The United States Of America As Represented By The Secretary Of The Army | Selectively etching microstructures in a glow discharge plasma |
-
1987
- 1987-05-06 US US07/046,347 patent/US4761298A/en not_active Expired - Fee Related
-
1988
- 1988-01-29 CA CA000557688A patent/CA1297172C/en not_active Expired - Fee Related
Also Published As
Publication number | Publication date |
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US4761298A (en) | 1988-08-02 |
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