Ex Parte Donofrio et alDownload PDFPatent Trial and Appeal BoardNov 9, 201613018013 (P.T.A.B. Nov. 9, 2016) Copy Citation UNITED STA TES p A TENT AND TRADEMARK OFFICE APPLICATION NO. FILING DATE 13/018,013 0113112011 65106 7590 MYERS BIGEL, PA P.O. BOX 37428 RALEIGH, NC 27627 11/14/2016 FIRST NAMED INVENTOR Matthew Donofrio 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. 5308-1381 7782 EXAMINER NADAV,ORI ART UNIT PAPER NUMBER 2811 NOTIFICATION DATE DELIVERY MODE 11/14/2016 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): uspto@myersbigel.com PTOL-90A (Rev. 04/07) UNITED STATES PATENT AND TRADEMARK OFFICE BEFORE THE PATENT TRIAL AND APPEAL BOARD Ex parte MATTHEW DONOFRIO, 1 John Adam Edmond, James Ibbetson, David Todd Emerson, Michael John Bergmann, Kevin Haberern, Raymond Rosado, and Jeffrey Carl Britt Appeal2015-003587 Application 13/018,013 Technology Center 2800 Before MARK NAGUMO, CHRISTOPHER L. OGDEN, and JEFFREY R. SNAY, Administrative Patent Judges. NAGUMO, Administrative Patent Judge. DECISION ON APPEAL Matthew Donofrio, John Adam Edmond, James Ibbetson, David Todd Emerson, Michael John Bergmann, Kevin Haberern, Raymond Rosado, and Jeffrey Carl Britt ("Cree") timely appeal 1 The real party in interest is identified as Cree, Inc. ("Cree"). (Appeal Brief, filed 31 October 2014 ("Br."), 2.) Appeal2015-003587 Application 13/018,013 under 35 U.S.C. § 134(a) from the Final Rejection2 of claims 1, 3-10, 16, 18-28, 62, and 64. 3 We have jurisdiction. 35 U.S.C. § 6. We reverse. OPINION A. Introduction4 The subject matter on appeal relates to "horizontal" white light emitting diodes ("LEDs") having oblique substrate sidewalls coated with a conformal phosphor layer comprising a phosphor having a specified average equivalent particle diameter, d50. The '013 Specification reveals that such LEDs provide relatively high brightness with relatively low angular variation. Moreover, a relatively high ratio of yellow phosphor to (more expensive) red phosphor may be used, resulting in a cost savings. (Spec. 12 [0051].) As Slater5 explains, white light may be produced from an ultraviolet light em1ttmg LED by combining red, green, and blue light emitted by phosphors placed on or near the ultraviolet light emitting LED. (Slater, col. 3, 11. 28--44.) In particular, as shown in Slater Figure lB (next page), 2 Office action mailed 30 May 2014 ("Final Rejection"; cited as "FR"). 3 Remaining copending claims 11-15, 29-33, 35-39, 63, and 65 have been withdrawn from consideration (FR 1, § 5a), and are not before us. 4 Application 13/018,013, Horizontal light emitting diodes including phosphor particles, filed 31 January 2011. We refer to the '"013 Specification," which we cite as "Spec." 5 Seen. 13, infra, for the complete citation. Slater is incorporated into the '013 Specification by reference. (Spec. 9 [0038].) 2 Appeal2015-003587 Application 13/018,013 conventional white LED devices have a diode region 1106 on first face lOOa of a substrate 100. Blue or ultraviolet light emitted from diode region 1107 is conducted out of the device through transparent substrate 100 and then through phosphor layer 120 on second face lOOb as well as vertical side faces lOOc and oblique side faces lOOd. {Slater Figures lB (left) and 2B (right) are shown below} 120} {Fig. lB shows a prior art LED with diode layer 110 and vertical side walls 1 OOc coated with nonconformal phosphor layer 120} 220_\ /~uuuuu t'::::::==~~~:::.:.:.~:.:~\ 1'X./ 200b \\ ~ \ ·. . . \ 200d 200 200d.J 1 OOe 2ooa1 200e-,: ~---------- """"4 ••••••w""""""""w<-y«««« ....... ~ \..210 {Fig. 2B shows an LED with diode layer 210 and oblique sidewalls 200d coated with conformal phosphor layer 220} According to Slater, it may be difficult to obtain sufficient coverage of phosphor coating 120 on vertical walls 1 OOc without excessive coating on 6 Throughout this Opinion, for clarity, labels to elements are presented in bold font, regardless of their presentation in the original document. 7 The nature of the diode region, i.e., whether "horizontal" (the anode and cathode ohmic contacts to the p-type layer and then-type layer, respectively, extend along the first face of the diode region) (Spec. 1 [0004], 11 [0044]) or "vertical" (the anode and cathode ohmic contacts are on opposite faces of the diode region) (id. at 11 [0044]) does not appear to be critical to the operation of white light LEDs of the invention. 3 Appeal2015-003587 Application 13/018,013 oblique portions lOOd; and still poor coverage on second face lOOb may be obtained. (Slater, col. 5, 11. 51-62.) As a result, too much blue emission from diode region 110 may be emitted through second face 100, while too little yellow secondary emission may be transmitted through the excessively thick coating on face lOOd. (Id. at col. 5, 1. 62, through col. 6, 1. 6.) The practical effect is said to be reduced conversion efficiency and a large angular dependence of Color Correlated Temperature ("CCT"). (Id. at col. 6, 11. 6-9.) In contrast, the oblique sidewalls shown in Slater Figure 2B are said to permit a conformal coating, which is said to "produce a desired spectrum of light, while also allowing more radiant flux to be emitted from the phosphor-coated LED." (Id. at 11. 14--16.) According to the '013 Specification, "[i]t is well known that larger phosphor particles are generally more efficient in light conversion than small sized phosphor particles." (Spec. 9 [0039].) However, the Specification explains; large phosphor particles may also have a lower light scattering efficiency than smaller phosphor particles which "may produce a high angular variation in Correlated Color Temperature (CCT), which is typical in white LEDs using large particulate size phosphor particles for brightness boost." (Id.) The variability of maximum change in CCT is referred to as "max delta CCT," or "max dCCt." (Id. at 20 [0076].) Cree reports that, contrary to expectations, a conformal phosphor layer having phosphor particles limited to an average equivalent particle 4 Appeal2015-003587 Application 13/018,013 diameter d50 8 of between about 10 µm and about 20 µm "provide[ s] relatively high brightness with relatively low angular variation." (Spec. 10 [0040].) Figure 1, reproduced below, illustrates an embodiment of the claimed light emitting diode 100. "'-- 1' 2n va 114 120 112 n ,.>120c ' ""'t'- -11o'b\ HOa 100 180 "182.a I ) !~:::::::-::::::::-::;:::-:::]-! --~18-)2~~--lB_;2b~1-36-=~:-::::~~~~I~ 170 1J2 FIG. l 1J4 {Fig. 1 shows packaged white LED 200 in cross section} Active diode region 110 comprises first face llOa and second face llOb, between which are located n-type region 112 and p-type region 114, which are connected by conductive vias 172 and 162, respectively, to cathode ohmic contact 170 and anode contact 160, 8 The symbol "d50," denoting the "average equivalent particle diameter," indicates that 50 mass% of the particles have a smaller diameter. (Spec. 10, [0041].) 5 Appeal2015-003587 Application 13/018,013 respectively, which lie in the plane of first face llOa. Light emitted from diode region 110 travels through substrate 120 and excites, e.g., blue, yellow, and red phosphor particles 142 in conformal phosphor layer 140 on oblique faces 120a and on outer face 120b of substrate 120. The mixed colors of the emitted light combine to form white light, which is gathered and transmitted to the external world by lens 190. Sole independent Claim 1 reads: A light emitting diode [100] comprising: a diode region [110] having first [llOa] and second [llOb] opposing faces and including therein an n-type layer [112] and a p-type layer [114]; an anode contact [160] that ohmically contacts the p-type layer [114] and extends on the first face [llOa]; a cathode contact [170] that ohmically contacts the n-type layer [112] and that also extends on the first face [llOa]; a transparent substrate [120] on the second face [llOb ], the transparent substrate including an inner face [120c] adjacent the second face [llOb], an outer face [120b] remote from the second face [llOb] and a sidewall [120a] that extends from the outer face [120b] to the inner face [120c]; and a conformal layer [140] that comprises phosphor [142] having an average equivalent particle diameter d50 of between about JOµm and about 20µm, on the outer face [120b] and extending on the sidewall [120a] oblique to the inner face [120c]. (Claims App., Br. 15; some indentation, paragraphing, bracketed labels to Fig. 1, and emphasis added.) 6 Appeal2015-003587 Application 13/018,013 The Examiner maintains the following ground of rejection9: Claims 1, 3-10, 16, 18-28, 62, and 64 stand rejected under 35 U.S.C. § 103(a) in view of the combined teachings of Donofrio, 10 Ishii, 11 Sakane, 12 and Slater. 13 B. Discussion Findings of fact throughout this Opinion are supported by a preponderance of the evidence of record. As will be seen, we need focus only on the limitations recited in claim 1. Cree contends first that the Examiner erred harmfully in concluding that it would have been prima facie obvious to combine the teachings of Donofrio regarding LED structures that "may incorporate wavelength conversion material such as a phosphor" (Donofrio 1 [0004], last sentence) 9 Examiner's Answer mailed 28 November 2014 ("Ans."). 10 Matthew Donofrio et al., Semiconductor light emitting diodes having reflective structures and methods of fabricating same, U.S. Patent Application Publication 2009/0283787 Al (2009), now U.S. Patent No. 8,368,100 (5 February 2013), assigned to Cree, Inc., the real party in interest in this Appeal. 11 Tsutomu Ishii et al., White LED lamp, backlight, light emitting device, display device and illumination device, U.S. Patent Application Publication 2011/0006334 Al (2011), based on an application filed 19 February 2009, now U.S. Patent No. 8,471,283 (25 June 2013). 12 Kenji Sakane et al., Phosphor and manufacturing method for the same, and light source, U.S. Patent No. 7,476,337 B2 (2009). 13 David B. Slater, Jr., and Gerald H. Negley, Phosphor-coated light emitting diodes including tapered sidewalls, andfabrication methods therefore, U.S. Patent No. 6,853,010 B2 (2005) (assigned to Cree, Inc., the real-party-in- interest). 7 Appeal2015-003587 Application 13/018,013 with the teachings of Slater regarding a conformal layer of phosphor on the outer face and oblique sidewalls of a substrate, wherein phosphor particles have an average equivalent particle diameter d50 of between about 10 µm and about 20 µmas disclosed by Ishii or Sakane. (Br. 3---6.) Although the Examiner does overstate the teachings of Donofrio to the extent that Donofrio is found to teach that "a conformal phosphor layer can be incorporated into the LED structure" (FR 3, 11. 7-8), this error is harmless in context. Donofrio teaches an LED assembly with transparent substrate 120 having outer face 120b and oblique side walls 120a that extend from outer face 120b to the inner face 120c, as shown in Donofrio Figure 12, reproduced below. {Donofrio Fig. 12 shows a cross section of an LED mounted on a substrate} The similarity between the shape of Donofrio' s substrate 120 and the substrate 200 illustrated by Slater in Fig. 2B, supra, together with the similar disclosed optical function, would have suggested the application of a conformal coating even in the absence of Donofrio' s express invitation to incorporate a wavelength conversion material into the LED. 8 Appeal2015-003587 Application 13/018,013 As for the selection of phosphor particles having a d50 between about 10 µm and about 20 µm, the teachings of Ishii that the average grain size of phosphor powders should be greater than 10 µm to avoid lowered light extracting efficiency (Ishii 5 [O 104]-[O106]) provides a sufficient reasonable expectation of successfully using particles in the range required by the claims. Similarly, the teachings of Sakane that d50 for phosphor particles should be 20 µm or less (Sakane, col. 9, 1. 65, through col. 10, 1. 10, cited by the Examiner in the Examiner's Answer (Ans., para. bridging 10- 11) would have provided further reason to select particles within the required range. 14 The silence of Ishii and Sakane regarding oblique sidewalls (Br. 5) is of no moment, given that both Donofrio-and, more critically, Slater-teach oblique sidewalls, the latter emphasizing the improved spectral and radiant flux obtained by being able to coat oblique sidewalls with a conformal phosphor-containing layer. Cree argues further that the Examiner erred in not giving sufficient weight to the evidence of unexpected results. (Br. 7-11.) First, as shown in Figure 8, reproduced on the following page, when applied to substrates having vertical walls, the larger d50 = 15 µm phosphor particles provide a mean max dCCT of about 7 500, compared to smaller d50 = 5.5 µm phosphor particles, which provide a mean max dCCT of about 3000. (Spec. 20 [0077].) This is consistent with the effect of larger scattering particles discussed in the '013 Specification and summarized supra. 14 It has not escaped our notice that Sakane recommends a most preferred range of "3.0 µm or more and 15 µm or less" (Sakane, col. 10, 11. 17-18.) 9 Appeal2015-003587 Application 13/018,013 {Figure 8 is shown below} ·X ••• ,.,,., •• rr·,···· ~~T4-.,,.~ ! , ,,.,.,,.,t.<." . ' ,:, ·~ Ii. ~~CCopy with citationCopy as parenthetical citation