Ex Parte Savchenko et alDownload PDFPatent Trial and Appeal BoardFeb 26, 201913365574 (P.T.A.B. Feb. 26, 2019) Copy Citation UNITED STA TES p A TENT AND TRADEMARK OFFICE APPLICATION NO. 13/365,574 89941 7590 HONEYWELL/S&S Patent Services 115 Tabor Road P.O.Box 377 FILING DATE 02/03/2012 02/28/2019 MORRIS PLAINS, NJ 07950 FIRST NAMED INVENTOR Arthur Savchenko UNITED STATES DEPARTMENT OF COMMERCE United States Patent and Trademark Office Address: COMMISSIONER FOR PATENTS P.O. Box 1450 Alexandria, Virginia 22313-1450 www .uspto.gov ATTORNEY DOCKET NO. CONFIRMATION NO. H0033422-5772/1121-521US1 4341 EXAMINER PARK,HYUND ART UNIT PAPER NUMBER 2865 NOTIFICATION DATE DELIVERY MODE 02/28/2019 ELECTRONIC Please find below and/or attached an Office communication concerning this application or proceeding. The time period for reply, if any, is set in the attached communication. Notice of the Office communication was sent electronically on above-indicated "Notification Date" to the following e-mail address(es): patentservices-us@honeywell.com pairdocketing@ssiplaw.com PTOL-90A (Rev. 04/07) UNITED STATES PATENT AND TRADEMARK OFFICE BEFORE THE PATENT TRIAL AND APPEAL BOARD Ex parte AR THUR SA VCHENKO and FRED PETRI Appeal2017-011855 Application 13/365,574 1 Technology Center 2800 Before ADRIENE LEPIANE HANLON, TERRY J. OWENS, and BRIAND. RANGE, Administrative Patent Judges. HANLON, Administrative Patent Judge. DECISION ON APPEAL A. STATEMENT OF THE CASE The Appellants filed an appeal under 35 U.S.C. § 134(a) from an Examiner's decision finally rejecting claims 1, 3-7, and 9-12. 2 We have jurisdiction under 35 U.S.C. § 6(b). 1 The real party in interest is said to be Honeywell International Inc. Appeal Brief dated March 13, 2017 ("App. Br."), at 3. 2 Claims 13 and 14, which are also pending, have been objected to as depending from a rejected base claim. The Examiner indicates that claims 13 and 14 would be allowable if rewritten in independent form including all of the limitations of the base claim and any intervening claims. Final Office Action dated August 12, 2016 ("Final Act."), at 7. Appeal2017-011855 Application 13/365,574 We AFFIRM-IN-PART. Independent claims 1 and 7 are reproduced below from the Claims Appendix to the Appeal Brief. Claim 1: A system comprising: a first resonator coupled between a proof mass and a support base on a first side of the proof mass and the support base; a second resonator coupled between the proof mass and the support base on a second side of the proof mass and the support base, wherein the first and second resonators comprise double-ended tuning forks (DETFs ); a first oscillator configured to generate a first drive signal at a first frequency based on a first resonant mode of the first resonator; a second oscillator configured to generate a second drive signal at a second frequency based on a second resonant mode of the first resonator; a third oscillator configured to generate a third drive signal at a third frequency based on a first resonant mode of the second resonator; a fourth oscillator configured to generate a fourth drive signal at a fourth frequency based on a second resonant mode of the second resonator; a first drive mechanism configured to cause the first resonator to resonate at the first and second resonant modes based on the generated first and second drive signals; a second drive mechanism configured to cause the second resonator to resonate at the first and second resonant modes based on the generated third and fourth drive signals; and a processing device configured to generate an acceleration value based on signals outputted by the first and second resonators. App. Br. 20 (emphasis added). Claim 7: A method comprising: 2 Appeal2017-011855 Application 13/365,574 using a first oscillator, driving a first resonator to resonate at a first resonant mode; using a second oscillator, driving the first resonator to resonate at a second resonant mode; using a third oscillator, driving a second resonator to resonate at the first resonant mode; using a fourth oscillator, driving the second resonator to resonate at the second resonant mode, wherein the first and second resonators comprise double-ended tuning forks (DETFs); and at a processing device, generating an acceleration value based on signals outputted by the first and second resonators. App. Br. 22 (emphasis added). Claims 1, 3-7, and 9-12 stand rejected underpre-AIA 35 U.S.C. § 103(a) as unpatentable over Loper, Jr. 3 in view of Tudor et al. 4 B. DISCUSSION 1. Claims 1 and 3---6 Claim 1 recites a system comprising, inter alia, "a first resonator coupled between a proof mass and a support base on a first side of the proof mass and the support base" and "a second resonator coupled between the proof mass and the support base on a second side of the proof mass and the support base." App. Br. 20 ( emphasis added). The Appellants argue that Loper does not disclose first and second resonators coupled between a proof mass and a support base on first and second sides, respectively, of the proof mass and the support base, as recited in claim 1. App. Br. 10. 3 US 4,258,572, issued March 31, 1981 ("Loper"). 4 M. J. Tudor & S. P. Beeby, Resonant Microsensors: Fundamentals and State of the Art, 9 Sensors and Materials 457-71 (1997) ("Tudor"). 3 Appeal2017-011855 Application 13/365,574 Loper discloses an accelerometer comprising, inter alia, first resonator 20 and second resonator 22 coupled to proof mass 14 and support base 10 on oppositely disposed ends of the respective proof mass and support base. Loper Figure 1 is reproduced below. Loper Figure 1 is a pictorial representation of the disclosed accelerometer. The Examiner finds that the first and second oppositely disposed ends of the proof mass and the support base correspond to the claimed first and second sides, respectively, of the proof mass and the support base. See Final Act. 3 (finding that the first side of the proof mass and the support base is the left side in Fig. 1 and the second side of the proof mass and the support base is the right side in Fig. 1 ). 5 During prosecution, the PTO applies to the verbiage of the proposed claims the broadest reasonable meaning of the words in their ordinary usage as they 5 Final Office Action dated August 12, 2016. 4 Appeal2017-011855 Application 13/365,574 would be understood by one of ordinary skill in the art, taking into account whatever enlightenment by way of definitions or otherwise that may be afforded by the written description contained in the applicant's specification. In re Morris, 127 F.3d 1048, 1054 (Fed. Cir. 1997). In this case, the Appellants disclose that "[ o ]ne DETF [ double-ended tuning fork] 36 is attached to a top of the proof mass 30 and the base section 32 and the other DETF 38 is attached to a bottom of the proof mass 30 and the base section 32." Spec. ,r 7 ( emphasis added). Consistent with that disclosure, Appellants' Figure 1, reproduced below, depicts first resonator 36 and second resonator 38 coupled on opposite swfaces of proof mass 30 and support base 32. Appellants' Figure 1 is a partial perspective view of an exemplary vibrating beam accelerometer. Based on the Appellants' Specification, we interpret the term "side" in claim 1 to mean a surface. We, therefore, interpret "a first side of the proof mass and the support base" to be a first surface of the proof mass and the support base and "a second side of the proof mass and the support base" to be a second surface of the 5 Appeal2017-011855 Application 13/365,574 proof mass and the support base, wherein the first surface is different from the second surface. See App. Br. 20. The Examiner has failed to show that Loper's resonators 20 and 22 are coupled to different surfaces of proof mass 14 and support base 10. Likewise, the Examiner has failed to establish that coupling Loper's resonators 20 and 22 to different surfaces of proof mass 14 and support base 10 would have been obvious to one of ordinary skill in the art based on the prior art of record. For those reasons, the obviousness rejection of claims 1 and 3-6 is not sustained. 2. Claims 7 and 9-12 a. Claims 7, 9, and 102 Claim 7 recites that "the first and second resonators comprise double-ended tuning forks (DETFs)." App. Br. 22. The Examiner finds that Loper's accelerometer comprises, inter alia, first and second resonators 20 and 22, respectively, comprising a pair of quartz crystals. Final Act. 5. The Examiner, however, finds that the resonators are not double- ended tuning forks (DETFs) as recited in claim 7. Final Act. 5. The Examiner finds Tudor discloses that a double-ended tuning fork (DETF) resonator is "one of the better choice[ s] for being used in acceleration analysis ... where double ended tuning forks are known for having improved performance 6 The Appellants argue, "[ fJor reasons analogous to those discussed above with respect to claim 1 (Group 1), the Examiner failed to establish that Loper in view of Tudor discloses the method of independent claim 7." App. Br. 17. In contrast to claim 1, however, claim 7 does not recite that the first and second resonators are coupled between a proof mass and a support base on first and second sides, respectively, of the proof mass and the support base, and claim 7 does not recite first and second drive mechanisms. Therefore, we address the Appellants' arguments directed to claim 1 on pages 5-13 of the Appeal Brief with the exception of arguments directed to those two limitations. 6 Appeal2017-011855 Application 13/365,574 characteristics." Final Act. 5. The Examiner also finds Tudor discloses various resonator materials, including single crystal silicon and single crystal quartz, wherein "quartz crystal exhibit[ s] linear temperature coefficient [ of] zero for certain modes in certain crystal orientation[s]." Final Act. 5. The Examiner concludes that it would have been obvious to one of ordinary skill in the art to replace Loper's quartz crystal resonators with first and second resonators compris[ing] double-ended tuning forks made of quartz crystals, since not only[] would [it] simply amount to substituting one known type of resonator with another known type of the same crystal material, but also due to the improved performance characteristics of the sensor system with reduction in temperature effect, as a result of said substitution. Final Act. 5---6 ( emphasis added). The Appellants contend that Tudor discloses fundamental resonator geometries that include bridges, such as the bridge disclosed in Loper, and more complex resonator geometries that include DETFs. App. Br. 8-9. Because "Tudor describes DETFs as a 'more complex resonator geometr[y ], "' the Appellants argue that replacing Loper's bridge resonators with Tudor's DETFs is "not a simple substitution of one known type of resonator for another." App. Br. 9. There is no dispute on this record that Tudor discloses that known resonator geometries include bridges and DETFs. Tudor, Section 4.1. Moreover, Tudor discloses that DETFs were known to be used in accelerometers. Tudor, Section 3.2; see also Ans. 3--4 (citing Tudor, Section 3.2).7 Thus, a preponderance of the evidence supports the Examiner's finding that the proposed modification of Loper's accelerometer is nothing more than substituting one known type of 7 Examiner's Answer dated July 28, 2017. 7 Appeal2017-011855 Application 13/365,574 resonator for another known type of resonator, wherein both resonators were known to be used in accelerometers. 8 Next, the Appellants argue that Tudor does not disclose or suggest a DETF made of quartz crystals. App. Br. 6. In response, the Examiner recognizes that Tudor does not expressly describe a DETF made of a single quartz crystal. Ans. 4. The Examiner, however, explains that it would have been obvious to one of ordinary skill in the art to not only use a DETF in Loper's accelerometer but also to use a DETF made of a single crystal quartz based on the various advantages disclosed in Tudor. Ans. 5; see also Tudor, Section 5. The Appellants argue: [ A ]t least because Tudor describes that it is common for resonators to be fabricated from polysilicon, and that there are limited machining processes available for quartz crystals as compared to silicon, one of ordinary skill in the art would likely have avoided the use of quartz crystals for fabrication of these "more complex resonators," such as DETFs according to Tudor. App. Br. 6 (footnote omitted). The Appellants also argue that one of ordinary skill in the art would not have fabricated a DETF from a quartz crystal because Tudor discloses that electronics cannot be integrated in quartz and quartz wafers are more expensive than silicon wafers. 9 App. Br. 7. 8 Because a preponderance of the evidence of record supports the Examiner's first reason for modifying Loper's accelerometer, it is not necessary to address the Examiner's second, alternative reason for modifying Loper's accelerometer (i.e., to improve performance characteristics of the sensor system with a reduction in temperature effect). Final Act. 6. 9 Notably, the Appellants do not disclose the material of the DETF described in their Specification. 8 Appeal2017-011855 Application 13/365,574 The Appellants' arguments are not persuasive of reversible error. First, Tudor does not disclose that a DETF could not be fabricated from a quartz crystal using an existing machining process, and the Appellants do not direct us to any evidence establishing that it would have been outside the level of ordinary skill in the art to fabricate a DETF from a quartz crystal using an existing process. Second, the Appellants do not direct us to any disclosure in Loper indicating that electronics are integrated in Loper's first and second resonators. Third, cost does not carry much weight in an obviousness analysis. See In re F arrenkopf, 713 F .2d 714, 718 (Fed. Cir. 1983) ("That a given combination would not be made by businessmen for economic reasons does not mean that persons skilled in the art would not make the combination because of some technological incompatibility."). The Appellants also argue that the modification proposed by the Examiner would change the principle of operation of Loper's accelerometer. App. Br. 8. The Appellants argue that Loper utilizes a pair of piezoelectric crystals (i.e., quartz) "'each having two independent resonant modes, each sensitive to acceleration effects but exhibiting substantially different temperature sensitivities."' App. Br. 8. The Appellants argue that the quartz crystals of Loper's accelerometer "separate 'the effects of temperatures and strain in order to obtain an accurate temperature compensated measure of acceleration."' App. Br. 7. The Appellants argue that Tudor, on the other hand, does not disclose or suggest that a DETF has particular qualities related to temperature sensitivities. App. Br. 7. The Examiner finds that the basic concept of Loper "is that it uses different temperature sensitivities in different modes inherent in single crystal quartz to obtain temperature corrected acceleration values." Ans. 6 (italics added). The Examiner finds that Tudor "discusses this same temperature behavior of single 9 Appeal2017-011855 Application 13/365,574 crystal quartz inherent in different modes." Ans. 6 ( citing Tudor, Section 5); see also Tudor, Section 5 ( disclosing that the linear temperature coefficient of frequency for quartz "is zero for certain modes in certain crystal orientations"). Therefore, the Examiner finds that the proposed substitution would not have modified the operation of Loper's accelerometer because a single crystal quartz DETF "would have yielded the same temperature sensitivities along different modes, and the temperature compensated acceleration values would have been the result." Ans. 6. The Appellants do not direct us to any evidence to the contrary. In sum, a preponderance of the evidence of record supports the Examiner's conclusion of obviousness. Therefore, the obviousness rejection of claims 7, 9, and 10 is sustained. 10 b. Claims 11 and 1211 Claim 11 reads as follows: Claim 11: The method of Claim 10, further comprising: at a first analog-to-digital converter (ADC) and digital counter, converting the output of the first bandpass filter to a first digital frequency; at a second analog-to-digital converter (ADC) and digital counter, converting the output of the second bandpass filter to a second digital frequency; 10 The Appellants indicate that "[ c ]laims 9 and 10 depend from claim 7, and therefore include the subject matter of claim 7 ." App. Br. 17. Therefore, the Appellants argue that "[ f]or at least the reasons stated above with respect to claim 7, the Examiner failed to establish a prima facie case of obviousness with respect to claims 9 and 10." App. Br. 17. 11 The Appellants argue that the Examiner has failed to show that Loper in view of Tudor discloses or suggests the method of claim 11 "for reasons analogous to those stated above with respect to claim 4 [] and claim 5." App. Br. 18. 10 Appeal2017-011855 Application 13/365,574 at a third analog-to-digital converter (ADC) and digital counter, converting the output of the third bandpass filter to a third digital frequency;and at a fourth analog-to-digital converter (ADC) and digital counter, converting the output of the fourth bandpass filter to a fourth digital frequency. App. Br. 23 (emphasis added). Claim 12 depends from claim 11. App. Br. 23. The Examiner finds Loper discloses that dual mode oscillator 31, which drives crystal 20, comprises a first bandpass filter (i.e., notch filter 36) and a second bandpass filter (i.e., notch filter 40). Final Act. 6. Although not expressly described in Loper, the Examiner finds that dual mode oscillator 50, which drives crystal 22, has a corresponding structure, and thus, comprises a third bandpass filter and a fourth bandpass filter as claimed. Final Act. 6. The Appellants argue: [T]he Examiner has not shown that one having ordinary skill in the art would have understood the notch filters disclosed by Loper to have been bandpass filters. Indeed, Loper discloses that the "notch filter 36 [] attenuates or rejects the C mode resonant frequency of the crystal 20" and the "filter 40 [] rejects the B mode resonant frequency of the crystal 20." The descriptions of a notch filter, which reject a particular frequency as described in Loper, would not be understood by one of ordinary skill in that art as providing a disclosure or suggestion of a bandpass filter as recited in claim [ 11]. App. Br. 13-14 (footnotes omitted; italics added). Consistent with the Appellants' argument, the Examiner finds that a notch filter "is a filter known in the art as a filter that rejects 'particular' frequencies within a certain range, and band passes frequencies outside that range." Ans. 9 (italics added). The Examiner recognizes that a bandpass filter, on the other hand, operates in a different manner. See Ans. 8 (finding that a bandpass filter "is known in the art as a filter that passes 'particular' frequencies within a certain range, and 11 Appeal2017-011855 Application 13/365,574 rejects (attenuates) frequencies outside that range" (italics added)). Nonetheless, the Examiner explains: If the particular frequency range to pass/reject is not predetermined or known, then both the bandpass filter and notch filter would be interpreted under broadest reasonable interpretation as the same, since both types of filters band pass[] and band reject[] frequency ranges in general terms. It is the relative relationship to a predetermined band of frequency range that distinguishes one type of filter from another. Since the claims simply generically recite[] filtering the signal and nothing more, and Loper discloses a filter that band-pass[ es] bands of frequency ranges (other than the C mode band that was rejected), Loper discloses a bandpass filter and filtering signals, as claimed. Ans. 9-10. In response, the Appellants direct our attention to their Specification which is said to disclose that "bandpass filters 160, 162, 172, 17 4 are chosen according to the two resonant frequency modes experienced by the DETFs 136, 138. Outputs from the filters 160, 162, 172, 174 are turned into digital frequency values by analog-to-digital converters (ADC) with digital counters 164, 166, 176, 178." Reply Br. 11 ( original emphasis omitted). 12 The Appellants explain: In this example of Appellant's specification, the bandpass filters are specifically chosen according to the two resonant frequency modes experienced by the DETFs, and the outputs from these bandpass filters are turned into the digital frequency values which are sent to a processor in order to generate acceleration values based on the digital frequency values. As such, one of ordinary skill in the art would understand that the function of the bandpass filters is to pass the resonant frequencies associated with the DETFs, and to filter out ranges of other frequencies, which is different from the operations performed by a notch filter in rejecting or attenuating the frequency 12 Reply Brief dated September 27, 2017. 12 Appeal2017-011855 Application 13/365,574 associated with the notch frequency of the notch filter, while allowing other frequencies to pass through the notch filter. Reply Br. 11-12 (emphasis added). Therefore, the Appellants argue that one of ordinary skill in the art would not understand Loper's notch filters to be bandpass filters as recited in claim 11. Reply Br. 12. The Appellants' argument is persuasive of reversible error. The record on appeal establishes that the claimed bandpass filter operates in a different manner than Loper's notch filter. Therefore, the obviousness rejection of claims 11 and 12 is not sustained. C. DECISION The Examiner's decision rejecting claims 1, 3---6, 11, and 12 under pre-AIA 35 U.S.C. § 103(a) as unpatentable over Loper in view of Tudor is reversed. The Examiner's decision rejecting claims 7, 9, and 10 under pre-AIA 35 U.S.C. § 103(a) as unpatentable over Loper in view of Tudor is affirmed. No time period for taking any subsequent action in connection with this appeal may be extended under 37 C.F.R. § 1.136(a)(l )(iv). AFFIRMED-IN-PART 13 Copy with citationCopy as parenthetical citation