Ex Parte Tu et alDownload PDFPatent Trial and Appeal BoardAug 30, 201613094262 (P.T.A.B. Aug. 30, 2016) Copy Citation UNITED STATES PATENT AND TRADEMARK OFFICE 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 APPLICATION NO. FILING DATE FIRST NAMED INVENTOR ATTORNEY DOCKET NO. CONFIRMATION NO. 13/094,262 04/26/2011 Chang-Ching Tu SLA2987 1279 55286 7590 08/31/2016 SHARP LABORATORIES OF AMERICA, INC. C/O LAW OFFICE OF GERALD MALISZEWSKI P.O. BOX 270829 SAN DIEGO, CA 92198-2829 EXAMINER HOSSAIN, MOAZZAM ART UNIT PAPER NUMBER 2898 MAIL DATE DELIVERY MODE 08/31/2016 PAPER 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. PTOL-90A (Rev. 04/07) UNITED STATES PATENT AND TRADEMARK OFFICE _________ BEFORE THE PATENT TRIAL AND APPEAL BOARD __________ Ex parte CHANG-CHING TU, LIANG TANG, JIANDONG HUANG, and APOSTOLOS T. VOUTSAS __________ Appeal 2014-002217 Application 13/094,262 Technology Center 2800 ___________ Before ADRIENE LEPIANE HANLON, CATHERINE Q. TIMM, and JAMES C. HOUSEL, 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 from a final rejection of claims 1–18 and 22–25. We have jurisdiction under 35 U.S.C. § 6(b). We REVERSE and enter new grounds of rejection. Independent claims 1, 18, and 25 are pending in the instant Application. Independent claim 1 is reproduced below from the Claims Appendix of the Appeal Brief dated July 31, 2013 (“App. Br.”). The limitations at issue are italicized. Appeal 2014-002217 Application 13/094,262 2 1. A method for fabricating a colloidal silicon quantum dot (SiQD) visible spectrum light-emitting diode (LED), the method comprising: forming a transparent first electrode; forming a hole-injection layer overlying the first electrode; forming a hole-transport layer overlying the hole-injection layer; forming a single SiQD layer overlying and in contact with the hole-transport layer, where each SiQD has a diameter of less than about 6 nanometers (nm); forming an electron-transport layer overlying and in contact with the single SiQD layer; and, forming a second electrode overlying the electron-transport layer. App. Br. 18 (emphasis added). The claims on appeal stand rejected as follows: (1) claims 1, 4, 8, 10, 11, 17, 18, 22, 24, and 25 under 35 U.S.C. § 102(e) as anticipated by Cho et al.;1 (2) claims 2 and 3 under 35 U.S.C. § 103(a) as unpatentable over Cho in view of Huang et al.;2 (3) claims 5, 7, 9, 12, 13, 16, and 23 under 35 U.S.C. § 103(a) as unpatentable over Cho; (4) claim 6 under 35 U.S.C. § 103(a) as unpatentable over Cho in view of Heeger et al.;3 and 1 US 2010/0213438 A1, published August 26, 2010 (“Cho”). 2 US 2011/0032743 A1, published February 10, 2011 (“Huang”). 3 US 2009/0126779 A1, published May 21, 2009 (“Heeger”). Appeal 2014-002217 Application 13/094,262 3 (5) claims 14 and 15 under 35 U.S.C. § 103(a) as unpatentable over Cho in view of Kwon et al.4 B. DISCUSSION 1. Rejections (1) – (5) The dispositive issue on appeal is: Did the Examiner reversibly err in finding that the colloidal silicon quantum dot (SiQD) visible spectrum light- emitting diode (LED) described in Cho comprises a single SiQD layer as recited in independent claims 1, 18, and 25? Referring to Cho Figure 2, reproduced below, the Examiner finds Cho describes a SiQD visible spectrum LED comprising, inter alia, single SiQD layer 16. Final 3, 6, 7.5 Cho Figure 2 depicts a cross-sectional view of an embodiment of a quantum dot (QD) light emitting device. 4 US 2007/0215856 A1, published September 20, 2007 (“Kwon”). 5 Final Office Action dated March 14, 2013. Appeal 2014-002217 Application 13/094,262 4 The Appellants argue that layer 16 is not a single SiQD layer.6 Rather, the Appellants argue that layer 16 is a multilayer comprised of first SiQD sublayer 17 and second SiQD sublayer 18 wherein one side of SiQD sublayer 17 is in contact with hole-transport layer (HTL) 15 and a second side of SiQD sublayer 17 is in contact with second SiQD sublayer 18, not electron-transport layer (ETL) 20 as claimed. Likewise, the Appellants argue that one side of SiQD sublayer 18 is in contact with SiQD sublayer 17, not hole transport layer 15 as claimed. App. Br. 7. The Appellants also argue that Cho’s SiQD sublayers 17 and 18 are made in separate steps from different materials and have different electrical properties and thus are not a single SiQD layer as claimed. App. Br. 7–8 (referring to Cho Fig. 3). The Appellants rely on a Declaration of Dr. David R. Evans dated April 30, 2013 (“Evans Decl.) to support their argument. App. Br. 9; see Evans Decl. ¶ 4 (“[Cho] Fig. 3 shows that QD light emitting layer 17 has a different energy band than QD light emitting layer 18. It is impossible for a single SiQD layer to have two different energy bands.”).7 We find the Appellants’ arguments are supported by the record. In an attempt to show that the “single layer SiQD layer” recited in claims 1, 18, and 25 encompasses more than one layer as in Cho’s multilayer 16, the Examiner directs our attention to steps 708f–708h in Appellants’ Figure 7B and finds multiple coatings are applied. Ans. 4. We disagree. Steps 708a–708h merely disclose a process for forming a SiQD suspension (step 708f) and 6 A reference is anticipatory when it discloses each and every element of the claimed invention, arranged or combined in the same way as in the claim. In re Gleave, 560 F.3d 1331, 1334 (Fed. Cir. 2009) (citations omitted). 7 Dr. Evans states, “In contrast, the Applicant’s device is able to bridge the energy gap between hole and electron-transport layers using a single SiQD layer having a single energy band, see Applicant’s Figs. 3A and 5A.” Evans Decl. ¶ 4. Appeal 2014-002217 Application 13/094,262 5 subsequently spin-coating the suspension of SiQDs on hole-transport layer 106. See Spec. 10, l. 21–11, l. 6; Reply Br. 2.8 The Examiner also directs our attention to steps 708k–708m in Appellants’ Figures 7A–7B which describes forming electron and hole barrier gaps. Ans. 4–5. Significantly, the Examiner does not direct us to any evidence showing that the electron and hole barrier gaps formed in steps 708j–708m each comprise a separate SiQD layer. Finally, the Examiner finds that the shell of the core/shell SiQDs is “formed by coating sub-layer as described in [page] 10, Lns. 18–20.” Ans. 5. According to the Appellants’ Specification, “[i]n one aspect, Step 708 forms the SiQD layer using core/shell SiQDs, where the cores are Si.” Spec. 10, ll. 18– 20 (emphasis added). We find that one of ordinary skill in the art would have understood that the shells surround the Si cores and are integral therewith. Thus, it is not clear on this record how the shell of the core/shell SiQDs forms a separate sub-layer as found by the Examiner. Independent claim 25 recites the following additional limitation: wherein an electron energy barrier gap of the single SiQD layer is between the electron energy barrier gap of the hole-transport layer and the electron energy bandgap of the electron-transport layer. App. Br. 25. The Appellants contend that Appellants’ Figures 3A and 5A illustrates the limitation. App. Br. 10. The Appellants argue that Cho does not disclose the additional limitation recited in claim 25: Cho’s Fig. 3 describes a first SiQD layer 17 with an electron energy barrier gap of about 4.3 eV, which is not in between the electron energy barrier gap of the hole-transport layer 15, which is 2.3 eV, and 8 Reply Brief dated November 12, 2013. Appeal 2014-002217 Application 13/094,262 6 the electron energy barrier gap of the electron-transport layer 20, which is 4.0 eV. Likewise, Cho’s second SiQD layer 18 has an electron energy barrier gap of about 4.8 eV, which is not between 2.3 and 4.0 eV. App. Br. 10 (emphasis omitted). In response, the Examiner directs our attention to Cho Figure 10 and contends that QD sub-layer 17a satisfies the relationship recited in claim 25 (i.e., ETL>QD>HTL). Ans. 11. However, remaining QD sub-layers 17b and 18 do not satisfy the claimed relationship. For the reasons set forth above, the § 102(e) rejection is not sustained. As for the § 103(a) rejections on appeal, the Examiner does not explain, in any detail, why a single SiQD layer would have been obvious to one of ordinary skill in the art based on the disclosure of Cho either alone or in combination with the remaining prior art of record. Therefore, the § 103(a) rejections are not sustained. 2. New grounds of rejection a. Claims 1, 4, 8, 10, 11, 17, 18, 22, and 24 Claims 1, 4, 8, 10, 11, 17, 18, 22, and 24 are rejected under 35 U.S.C. § 102(e) as anticipated by Cho. Cho discloses: The energy band structure of FIG. 3 shows an embodiment of a QD-LED in which the first electrode (anode) 14 is formed of ITO, the second electrode (cathode) 22 is formed of Al, the HIT [hole-injection layer] 13 is formed of PEDOT, the HTL 15 is formed of TFB, the ETL 20 is formed of TiO2, and the QD containing layer 17 (QD layer 1) having a band level shifted by a surface exchange process is formed between the QD light emitting layer 18 (emitting layer (“EML”), QD layer 2) and the HTL 15. . . . When the QD-LED is formed to have the band structure shown in FIG. 3, compared to the case when the Appeal 2014-002217 Application 13/094,262 7 QD containing layer 17 is not included, the band offset of the QD- LED having the band structure shown in FIG. 3 may be reduced . . . . Cho ¶ 97 (emphasis added). Based on the foregoing, we find Cho not only describes a QD-LED comprising, inter alia, two QD layers, i.e., QD containing layer 17 and QD light emitting layer 18, but also describes a QD-LED, as illustrated in Cho Figure 2, wherein the QD containing layer 17 is omitted. Thus, we find Cho describes a QD-LED comprising, inter alia, a single SiQD layer (i.e., QD light emitting layer 18) as recited in claims 1 and 18. See also Cho ¶ 7 (“A typical quantum dot light emitting device . . . has a basic structure of three layers, that is: a QD light emitting layer, and a hole transport layer . . . and an electron transport layer . . . which are respectively located at either end of the QD light emitting layer.”). The Appellants do not direct us to any error in the Examiner’s findings as to claims 4, 8, 10, 11, 17, 22, and 24. See App. Br. 9–10. Therefore, we adopt the Examiner’s findings as to claims 4, 8, 10, 11, 17, 22, and 24 on pages 4–7 of the Final Office Action. b. Claims 2 and 3 Claims 2 and 3 are rejected under 35 U.S.C. § 103(a) as unpatentable over Cho in view of Huang. The Appellants do not direct us to any error in the Examiner’s findings of fact or dispute that the limitations recited in claims 2 and 3 would have been obvious to one of ordinary skill in the art based on the combined teachings of Cho and Huang. See App. Br. 11–12. Therefore, we adopt the Examiner’s findings of fact and conclusions of law as to claims 2 and 3 on pages 8–10 of the Final Office Action. c. Claims 5, 7, 9, 12, 13, 16, and 23 Appeal 2014-002217 Application 13/094,262 8 Claims 5, 7, 9, 12, 13, 16, and 23 are rejected under 35 U.S.C. § 103(a) as unpatentable over Cho. The Appellants do not direct us to any error in the Examiner’s findings of fact or dispute that the limitations recited in claims 5, 7, 9, 16, and 23 would have been obvious to one of ordinary skill in the art based on the teachings of Cho. See App. Br. 12–13. Therefore, we adopt the Examiner’s findings of fact and conclusions of law as to claims 5, 7, 9, 16, and 23 on pages 10–12 and 14–16 of the Final Office Action. As to claims 12 and 13, the Appellants argue that “claims 12–13 recite a relationship between SiQD particle diameters and energy barrier gap values. Cho fails to describe a relationship between SiQD diameters and energy barrier gap values.” App. Br. 13. According to the Appellants’ Specification: In [one] aspect, forming the SiQD layer in Step 708 [in Figure 7A] includes the following substeps. . . . Step 708l forms a hole energy barrier gap between the hole-transport layer and the SiQD layer of less than, or equal to 0.9 electron volts (eV) [as recited in claims 9, 13, and 23]. Step 708m forms a hole energy barrier gap between the SiQD layer and the electron-transport layer of greater than, or equal to 1.5 eV [as recited in claims 9, 13, and 23]. More explicitly, the Step 708 forms the SiQD layer using SiQDs having a diameter in a range between 3 and 6 nm, then . . . Step 708l forms a hole energy barrier gap between the hole-transport layer and the SiQD layer of less than, or equal to 0.4 eV [as recited in claim 12], and Step 708m forms a hole energy barrier gap between the SiQD layer and the electron-transport layer of greater than, or equal to 2eV [as recited in claim 12]. Alternatively, if Step 708 forms the SiQD layer using SiQDs having a diameter in a range between 1 and 2 nm, then . . . Step 708l forms a hole energy barrier gap between the hole-transport layer and the SiQD layer of less than, or equal to 0.9 eV [as recited in claims 9, Appeal 2014-002217 Application 13/094,262 9 13, and 23]. Step 708m forms a hole energy barrier gap between the SiQD layer and the electron-transport layer of greater than, or equal to 1.5 eV [as recited in claims 9, 13, and 23]. Spec. 11, l. 21–12, l. 24 (emphasis added). Based on the foregoing, we find the Appellants appear to teach that the diameter of the SiQDs dictates (1) the hole energy barrier gap value between the hole-transport layer and the single SiQD layer and (2) the hole energy barrier gap value between the single SiQD layer and the electron-transport layer. Thus, we find the range of SiQD diameters recited in claim 12 necessarily results in the hole energy barrier gap values recited in claim 12 and the range of SiQD diameters recited in claim 13 necessarily results in the hole energy barrier gap values recited in claims 9, 13, and 23. Cho discloses that the QDs in QD light emitting layer 18 may have a diameter of about 1 nm–10 nm. Cho ¶ 59. That range encompasses the ranges recited in claims 12 and 13. Thus, we find the range of QD diameters disclosed in Cho necessarily results in a range of hole energy barrier gap values that encompasses the hole energy barrier gap values recited in claims 9, 12, 13, and 23. See In re Peterson, 315 F.3d 1325, 1330 (Fed. Cir. 2003) (“when, as here, the claimed ranges are completely encompassed by the prior art, the conclusion [of prima facie obviousness] is even more compelling than in cases of mere overlap”). d. Claim 6 Claim 6 is rejected under 35 U.S.C. § 103(a) as unpatentable over Cho in view of Heeger. The Appellants do not direct us to any error in the Examiner’s findings of fact or dispute that the limitation recited in claim 6 would have been obvious to one of ordinary skill in the art based on the combined teachings of Cho and Appeal 2014-002217 Application 13/094,262 10 Heeger. See App. Br. 14. Therefore, we adopt the Examiner’s findings of fact and conclusions of law as to claim 6 on pages 16–17 of the Final Office Action. e. Claims 14 and 15 Claims 14 and 15 are rejected under 35 U.S.C. § 103(a) as unpatentable over Cho in view of Kwon. The Appellants do not direct us to any error in the Examiner’s findings of fact or dispute that the limitations recited in claims 14 and 15 would have been obvious to one of ordinary skill in the art based on the combined teachings of Cho and Kwon. See App. Br. 14–15. Therefore, we adopt the Examiner’s findings of fact and conclusions of law as to claims 14 and 15 on pages 18–19 of the Final Office Action. C. DECISION We reverse the Examiner’s decision and enter the following new grounds of rejection under 37 C.F.R. § 41.50(b): Claims 1, 4, 8, 10, 11, 17, 18, 22, and 24 are rejected under 35 U.S.C. § 102(e) as anticipated by Cho. Claims 2 and 3 are rejected under 35 U.S.C. § 103(a) as unpatentable over Cho in view of Huang. Claims 5, 7, 9, 12, 13, 16, and 23 are rejected under 35 U.S.C. § 103(a) as unpatentable over Cho. Claim 6 is rejected under 35 U.S.C. § 103(a) as unpatentable over Cho in view of Heeger. Claims 14 and 15 are rejected under 35 U.S.C. § 103(a) as unpatentable over Cho in view of Kwon. According to 37 C.F.R. § 41.50(b), the Appellants, WITHIN TWO MONTHS FROM THE DATE OF THE DECISION, must exercise one of the Appeal 2014-002217 Application 13/094,262 11 following two options with respect to the new grounds of rejection to avoid termination of the appeal as to the rejected claims: (1) Reopen prosecution. Submit an appropriate amendment of the claims so rejected or new Evidence relating to the claims so rejected, or both, and have the matter reconsidered by the examiner, in which event the prosecution will be remanded to the examiner. . . . (2) Request rehearing. Request that the proceeding be reheard under § 41.52 by the Board upon the same Record. . . . No time period for taking any subsequent action in connection with this appeal may be extended under 37 C.F.R. § 1.136(a)(1). REVERSED; 37 C.F.R. § 41.50(b) Copy with citationCopy as parenthetical citation