Nanoco Technologies Ltd. v. Samsung Electronics Co., Ltd. et al

Filing 1

COMPLAINT against Samsung Advanced Institute of Technology, Samsung Display Co., Ltd., Samsung Electronics America, Inc., Samsung Electronics Co., Ltd., Samsung Electronics Co., Ltd. Visual Display Division ( Filing fee $ 400 receipt number 0540-7664317.), filed by Nanoco Technologies Ltd.. (Attachments: # 1 Civil Cover Sheet, # 2 Exhibit 1, # 3 Exhibit 2, # 4 Exhibit 3, # 5 Exhibit 4, # 6 Exhibit 5, # 7 Exhibit 6, # 8 Exhibit 7, # 9 Exhibit 8, # 10 Exhibit 9, # 11 Exhibit 10, # 12 Exhibit 11, # 13 Exhibit 12, # 14 Exhibit 13, # 15 Exhibit 14)(Henry, Claire)

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Exhibit 5 USOO968.0068B2 (12) United States Patent (10) Patent No.: VO et al. US 9,680,068 B2 (45) Date of Patent: (54) QUANTUM DOT FILMS UTILIZING Jun. 13, 2017 (2013.01); B32B 2307/7242 (2013.01); B82Y MULT-PHASE RESNS 20/00 (2013.01); Y10T 156/10 (2015.01) (71) Applicant: Nanoco Technologies, Ltd., Manchester (58) Field of Classification Search CPC ...... H01L 33/502: C09K11/703: C09K11/02 See application file for complete search history. (72) Inventors: Cong-Duan Vo, Manchester (GB); (56) (GB) References Cited Imad Naasani, Manchester (GB); Amilcar Pillay Narrainen, Manchester (GB) U.S. PATENT DOCUMENTS 2010, 0123155 A1* (73) Assignee: Nanaco Technologies Ltd., Manchester 5, 2010 Pickett ................... B82Y 15.00 3f2011 Picket et al. 3/2011 Pickett et al. 2013, OO75692 A1 (*) Notice: 2011/0068321 A1 2011/0068322 A1 (GB) 3/2013 Naasani et al. Subject to any disclaimer, the term of this patent is extended or adjusted under 35 U.S.C. 154(b) by 312 days. FOREIGN PATENT DOCUMENTS EP (21) Appl. No.: 14/460,008 (22) Filed: O 2, 2009 Ramasamy et al. Materials Science in semiconductor Processing 42 O 2016) 334-343. Prior Publication Data US 2015/OO47765 A1 2028248 A1 OTHER PUBLICATIONS Aug. 14, 2014 (65) 257/98 SAG. Male, 2007, 19, 6581.* Feb. 19, 2015 Parlak et al. ACS Appl. Mater. Interfaces 2011, 3, 4306-4314.* Supporting information of Parlak 2011.* Wang et al. Langmuir 2005, 21, 2465-2473.* Related U.S. Application Data (60) Provisional application No. 61/865,692, filed on Aug. 14, 2013. * cited by examiner Primary Examiner — Mark Kaucher (74) Attorney, Agent, or Firm — Blank Rome LLP (51) Int. Cl. B82. 20/00 (2011.01) (57) HOIL 33/50 B32B 37/24 C09K II/70 C09K II/02 (2010.01) (2006.01) (2006.01) (2006.01) Multi-phase polymer films containing quantum dots (QDS) are described herein. The films have domains of primarily hydrophobic polymer and domains of primarily hydrophilic polymer. QDS, being generally more stable within a hydro (52) U.S. Cl. CPC ............ HOIL 33/504 (2013.01); B32B 37/24 (2013.01); C09K II/02 (2013.01); C09K II/703 (2013.01); HOIL 33/502 (2013.01); B32B 2037/243 (2013.01); B32B 2307/418 ABSTRACT phobic matrix, are dispersed primarily within the hydropho bic domains of the films. The hydrophilic domains tend to be effective at excluding oxygen. 1 Claim, 4 Drawing Sheets 2OO 2O3 U.S. Patent Jun. 13, 2017 Sheet 1 of 4 US 9,680,068 B2 104 2O3 U.S. Patent Jun. 13, 2017 Sheet 2 of 4 US 9,680,068 B2 : T08 008 Z98 U.S. Patent Jun. 13, 2017 Sheet 3 of 4 ` ZOG`&` ** .** ** *** <<. *** ** *** *** * **. & US 9,680,068 B2 U.S. Patent Jun. 13, 2017 on 8 N Sheet 4 of 4 US 9,680,068 B2 s f g 8. x: 3. anese: x, i US 9,680,068 B2 1. 2 larly, as phosphor films for down-converting light emitted QUANTUM DOT FILMS UTILIZING from a solid-state LED semiconductor material. MULT-PHASE RESNS FIELD OF THE INVENTION The invention relates to materials comprising light emit ting semiconductor quantum dots (QDs), and more specifi cally, multi-phase polymer films incorporating QDS. BACKGROUND Light-emitting diodes (LEDs) are becoming more impor tant to modern day life and it is envisaged that they will become one of the major applications in many forms of lighting such as automobile lights, traffic signals, general lighting, liquid crystal display (LCD) backlighting and dis play screens. Currently, LED devices are typically made from inorganic solid-state semiconductor materials. The material used to make the LED determines the color of light produced by the LED. Each material emits light with a particular wavelength spectrum, i.e., light having a particu lar mix of colors. Common materials include AlGaAS (red), AlGalnP (orange-yellow-green), and AlGalnN (green-blue). LEDs that produce white light, which is a mixture of fundamental colors (e.g., red, green and blue) or that pro duce light not available using the usual LED semiconductor materials are needed for many applications. Currently the most usual method of color mixing to produce a required color, such as white, is to use a combination of phospho rescent materials that are placed on top of the Solid-state LED whereby the light from the LED (the “primary light') is absorbed by the phosphorescent material and then re emitted at a different frequency (the “secondary light'). The phosphorescent material “down converts” a portion of the primary light. Current phosphorescent materials used in down convert ing applications typically absorb UV or blue light and convert it to light having longer wavelengths, such as red or green light. A lighting device having a blue primary light Source. Such as a blue-emitting LED, combined with sec ondary phosphors that emit red and green light, can be used to produce white light. The most common phosphor materials are solid-state semiconductor materials, such as trivalent rare-earth doped oxides or halophosphates. White emission can be obtained by blending a blue light-emitting LED with a green phos 10 15 an emulsion. A film is formed of the emulsion, which can then be cured to form a solid film. 25 30 35 40 45 phor such as, SrGaSa:Eu" and a red phosphor such as, SrSisNis:Eu" or a UV light-emitting LED plus a yellow phosphor such as, Sr.P.O., Eu"; Mu", and a blue-green BRIEF DESCRIPTION OF THE DRAWINGS The foregoing Summary as well as the following detailed description will be better understood when read in conjunc tion with the appended drawings. For the purpose of illus tration only, there is shown in the drawings certain embodi ments. It is understood, however, that the inventive concepts disclosed herein are not limited to the precise arrangements and instrumentalities shown in the drawings. FIG. 1 is a schematic illustration of a prior art use of a film containing QDs to down-convert light emitted by a LED. FIG. 2 is a schematic illustration of a QD-containing polymer sandwiched between transparent sheets. FIG. 3 is a schematic illustration of a two-phase film having a QD-compatible phase and an oxygen-excluding phase. FIG. 4 is a flowchart illustrating the steps of making a two-phase film. FIG. 5 is a plot of QD quantum yields in various films. FIG. 6 illustrates stability studies of two-phase LMA/ epoxy films. DESCRIPTION phosphor. White LEDs can also be made by combining a blue LED with a yellow phosphor. Several problems are associated with solid-state down converting phosphors. Color control and color rendering may be poor (i.e., color rendering index (CRI)<75), resulting in light that is unpleasant under many circumstances. Also, it is difficult to adjust the hue of emitted light; because the characteristic color emitted by any particular phosphor is a function of the material the phosphor is made of. If a suitable material does not exist, then certain hues may simply be 50 unavailable. There is thus a need in the art for down 60 There has been substantial interest in exploiting the properties of compound semiconductor particles with dimensions on the order of 2-50 nm, often referred to as quantum dots (QDS) or nanocrystals. These materials are of commercial interest due to their size-tunable electronic properties that can be exploited in many commercial appli 55 converting phosphors having greater flexibility and better color rendering than presently available. cations. The most studied of semiconductor materials have been the chalcogenides II-VI materials namely ZnS, ZnSe, CdS, CdSe, CdTe; especially CdSe due to its tunability over the visible region of the spectrum. Reproducible methods for the large-scale production of these materials have been devel oped from “bottom up' techniques, whereby particles are prepared atom-by-atom, i.e., from molecules to clusters to particles, using 'wet' chemical procedures. Two fundamental factors, both related to the size of the SUMMARY 65 Films containing QDs are described herein. The films may be used as components for LED lighting devices, particu The films are formed from two or more polymer materi als, for example, two or more polymer resins. The films at least partially phase-separate. Such that some domains within a film are primarily one of the polymer materials and other domains within the film are primarily the polymer material. One of the polymer materials is chosen to be highly compatible with the QDs. Another of the polymer materials is highly effective at excluding oxygen. As a result, the multi-domain films include QD-rich domains of QDs dis persed in the QD-compatible polymer, those domains being Surrounded by QD-poor domains of the oxygen-excluding polymer. Thus, the QDs are suspended in a medium with which they are highly compatible and are protected from oxygen by the oxygen-excluding domains. Methods of making such films are also described herein. According to some embodiments, QDS are suspended in a Solution of a first polymer resin (i.e., a QD-compatible resin). The QD suspension is then added to a solution of the second polymer resin (the oxygen-excluding resin), yielding individual semiconductor nanoparticles, are responsible for their unique properties. The first is the large surface-to volume ratio. As particles become smaller, the ratio of the US 9,680,068 B2 3 number of Surface atoms to those in the interior increases. This leads to the Surface properties playing an important role in the overall properties of the material. The second factor is a change in the electronic properties of the material when the material is very small in size. At extremely small sizes quantum confinement causes the materials band gap to gradually increase as the size of the particles decrease. This effect is a consequence of the confinement of an electron in a box giving rise to discrete energy levels similar to those observed in atoms and molecule rather than a continuous band as observed in the corresponding bulk semiconductor material. Thus, the “electron and hole' produced by the absorption of electromagnetic radiation are closer together than they would be in the corresponding macrocrystalline material. This leads to a narrow bandwidth emission that depends upon the particle size and composition of the nanoparticle material. QDs therefore have higher kinetic energy than the corresponding macrocrystalline material and consequently the first excitonic transition (band gap) increases in energy with decreasing particle diameter. QD nanoparticles of a single semiconductor material tend to have relatively low quantum efficiencies due to electron hole recombination occurring at defects and dangling bonds situated on the nanoparticle Surface, which may lead to 10 15 25 non-radiative electron-hole recombinations. One method to eliminate Such defects and dangling bonds on the inorganic Surface of the QD is to grow a second inorganic material, having a wider band-gap and Small lattice mismatch to that of the core material, epitaxially on the surface of the core particle, producing a “core-shell particle. Core-shell par ticles separate any carriers confined in the core from surface 30 states that would otherwise act as non-radiative recombina tion centers. One example is QDS having a ZnS shell grown on the surface of a CdSe core. Rudimentary QD-based light-emitting devices have been made by embedding colloidally produced QDs in an opti cally clear LED encapsulation medium, typically a silicone or an acrylate, which is then placed on top of a Solid-state LED. The use of QDs potentially has some significant advantages over the use of the more conventional phos phors, such as the ability to tune the emission wavelength, strong absorption properties, improved color rendering, and low scattering. For the commercial application of QDS in next-generation light-emitting devices, the QDS are preferably incorporated into the LED encapsulating material while remaining as fully mono-dispersed as possible and without significant loss of quantum efficiency. The methods developed to date are problematic, not least because of the nature of current LED encapsulants. QDS can agglomerate when formulated into current LED encapsulants, thereby reducing the optical performance of the QDs. Moreover, once the QDs are incorporated into the LED encapsulant, oxygen can migrate through the encapsulant to the surfaces of the QDs, which can lead to photo-oxidation and, as a result, a drop in quantum yield (QY). One way of addressing the problem of oxygen migration to the QDs has been to incorporate the QDs into a medium with low oxygen permeability to form “beads of such a material containing QDs dispersed within the bead. The QD-containing beads can then be dispersed within an LED encapsulant. Examples of such systems are described in U.S. patent application Ser. No. 12/888,982, filed Sep. 23, 2010 (Pub. No.: 2011/0068322) and Ser. No. 12/622,012, filed Nov. 19, 2009 (Pub. No.: 2010/0123155), the entire contents of which are incorporated herein by reference. 35 40 45 50 55 60 65 4 Films containing QDs are described herein. FIG. 1 illus trates a prior art embodiment 100, wherein a QD-containing film 101 is disposed on a transparent substrate 102. Such a film can be useful, for example, to down-convert primary light 103 from a primary light source 104 by absorbing primary light 103 and emitting secondary light 105. A portion 106 of primary light may also be transmitted through the film and Substrate so that the total light emanating from the film and substrate is a mixture of the primary and secondary light. QD-containing films, such as film 101 in FIG. 1, may be formed by dispersing QDS in a polymer resin material and forming films of the material using generally any method of preparing polymer films known in the art. It has been found that QDs are generally more compatible with hydrophobic resins, such as acrylates, compared to more hydrophilic resins, such as epoxies. Thus, polymer films made of QDS dispersed in acrylates tend to have higher initial quantum yields (QYs) than QD films using hydrophilic resins such as epoxy resins. However, acrylates tend to be permeable to oxygen, while epoxy resin polymers and similar hydrophilic polymers tend to be better at excluding oxygen. One alternative for achieving high QY associated with QD-containing hydrophobic films, while also maintaining stability of the QY over time, is to insulate the film from oxygen by Sandwiching the film between gas barrier sheets, as illustrated in FIG. 2. FIG. 2 illustrates a panel 200 having a polymer film 201 contained between gas barrier sheets 202 and 203. The polymer film 201 contains QDs dispersed throughout. Gas barrier sheets 202 and 203 serve to prevent oxygen from contacting the dispersed QDS. However, even in an embodiment as illustrated in FIG. 2, oxygen can permeate into the film at edges 204, resulting in a deterio ration of the QY of the film. One solution to this problem is to seal edges 204 with an oxygen barrier. However, doing so adds cost to the produc tion of panel 200. Another option is to use a polymer 201 that is less permeable to oxygen. But as explained above, QDS are generally less compatible with Such polymer resins, and therefore the optical properties of devices utilizing such polymers are less than ideal. Multi-phase films utilizing at least a first phase (phase 1) resin that is compatible with the QD material and at least a second phase (phase 2) resin that is efficient at rejecting O are described herein. FIG. 3 illustrate a plan view of such a film 300, wherein QDS 301 are dispersed in a first polymer phase 302, which is typically a hydrophobic material such as an acrylate resin. Regions of the first polymer phase are dispersed throughout a second polymer phase 303, which is typically an oxygen-impermeable material Such as epoxy. The multi-phase films described herein overcome many of the problems described above. The phase 1 resin is compat ible with the QDs and therefore allows a high initial QY. The phase 2 resin is impermeable to oxygen, and therefore protects the QDs from oxidation without the need to seal the edges of the panel. As used herein, the term “film' includes, not only 2-dimensional (i.e. flat) sheets, as illustrated in FIGS. 1-3, but can also include 3-dimensional shapes. FIG. 4 is a flowchart illustrating steps of a method of preparing multi-phase films as described herein. The QDs are dispersed in a solution of the phase 1 resin (or resin monomer) 401. As described above, the phase 1 resin is generally a hydrophobic resin, such as acrylate resins. Examples of Suitable phase 1 resins include, poly(methyl (meth)acrylate), poly(ethyl(meth)acrylate), poly(n-propyl (meth)acrylate), poly(butyl(meth)acrylate), poly(n-pentyl (meth)acrylate), poly(n-hexyl(meth)acrylate), poly US 9,680,068 B2 5 (cyclohexyl(meth)acrylate), poly(2-ethyl hexyl(meth) acrylate), poly(octyl(meth)acrylate), poly(isooctyl(meth) acrylate), poly(n-decyl(meth)acrylate), poly(isodecyl(meth) acrylate), poly(lauryl(meth)acrylate), poly(hexadecyl(meth) acrylate), poly(octadecyl(meth)acrylate), poly(isobornyl (meth)acrylate), poly(isobutylene), polystyrene, poly (divinyl benzene), polyvinyl acetate, polyisoprene, polycarbonate, polyacrylonitrile, hydrophobic cellulose based polymers like ethyl cellulose, silicone resins, poly (dimethyl siloxane), poly(vinyl ethers), polyesters or any hydrophobic host material Such as wax, paraffin, vegetable oil, fatty acids and fatty acid esters. Generally, the phase 1 resin can be any resin that is compatible with the QDs. The phase 1 resin may or may not be cross-linked or cross-linkable. The phase 1 resin may be a curable resin, for example, curable using UV light. In addition to the QDS and phase 1 resin (or resin monomer), the solution of 401 may further include one or more of a photoinitiator, a cross-linking agent, a polymerization cata lyst, a refractive index modifier (either inorganic one such as ZnS nanoparticles or organic one Such as high refractive index monomers or poly(propylene Sulfide)), a filler Such as fumed silica, a scattering agent Such as barium sulfate, a Viscosity modifier, a Surfactant or emulsifying agent, or the 6 are incorporated herein by reference. The QDs were added to a degassed vial, the toluene evaporated, and the resultant Solid QD re-dispersed in degassed lauryl methacrylate (LMA, 2.64 mL) containing IRG819/IRG651 (Igracure(R) 5 photoinitiators (9/18 mg). Trimethylolpropane trimethacry late (TMPTM) crosslinker (0.32 mL) was added. The mix ture was further stirred for 30 min under nitrogen affording phase 1 resin. Films of QDs in phase 1 resin were laminated between 3M gas barrier layers on an area limited by a 19 10 mmx 14 mmx0.051 mm plastic spacer. The film was cured with a Mercury lamp for 1 min. Stability testing of the QY of the QDS in phase 1 resin is represented by square data points in the plot illustrated in FIG. 5. 15 Example 1B Two-phase resin was prepared by mixing 148 microliters of the phase 1 resin with 0.5 mL degassed epoxy (Epotek, 20 OG142) and the mixture was mechanically stirred for 3 min at 100 rpm under nitrogen. 60 Microliters of the two-phase resin was then laminated between 3M gas barrier layers on an area limited by a 19 mmx 14 mmx0.051 mm plastic spacer. The film was cured with a Mercury lamp for 1 min. like. 25 Stability testing of the QY of the QDs in two-phase resin The QD-phase 1 resin dispersion can then be mixed with comprising acrylate (phase 1) and epoxy (Epotek OG142, a solution of the phase 2 resin (or resin monomer) 402. As phase 2) is represented by diamond-shaped data points in the explained above, the phase 2 resin is a better oxygen barrier plot illustrated in FIG. 5. than the phase 1 resin. The phase 2 resin is generally a Example 2 hydrophilic resin. The phase 2 resin may or may not be 30 cross-linkable. The phase 2 resin may be a curable resin, for example, curable using UV light. Examples of phase 2 resins Green InP/ZnS QDs (120 Optical Density (OD)) were include epoxy-based resins, polyurethanes-based resins, prepared as described in U.S. patent application Ser. No. hydrophilic (meth)acrylate polymers, polyvinyl alcohol, 13/624,632, filed Sep. 23, 2011. The QDs were added to a poly(ethylene-co-vinyl alcohol), polyvinyl dichloride, sili- 35 degassed vial and dispersed in degassed lauryl methacrylate cones, polyimides, polyesters, polyvinyls, polyamides, (LMA, 2.64 mL) containing IRG819/IRG651 photoinitia enphenolics, cyanoacrylates, gelatin, water glass (sodium tors (9/18 mg). TMPTM crosslinker (0.32 mL) was added. silicate), PVP (Kollidon). The solution of phase 2 resin may The mixture was further stirred for 30 min under nitrogen also include one or more of a photoinitiator, a cross-linking affording phase 1 resin. Two-phase resin was prepared by agent, a polymerization catalyst, a Surfactant or emulsifying 40 mixing 148 microliters of the phase 1 resin with 0.5 mL degassed polyurethane acrylate (Dymax OP4-4-26032) and agent, or the like. According to some embodiments, the phase 1-phase 2 the mixture was mechanically stirred for 3 min at 100 rpm mixture forms an emulsion 403, typically and emulsion of under nitrogen. 60 Microliters of the two-phase resin was phase 1 resin Suspended in phase 2 resin. The emulsion then laminated between 3M gas barrier layers on an area composition can be adjusted by adjusting the relative con- 45 limited by a 19 mmx14 mmx0.051 mm plastic spacer. The centrations of phase 1 and phase 2 resins, the rate of Stirring film was cured with a Mercury lamp for 1-5 min. Stability of the mixture, the relative hydrophobicity of the resins, and testing of the QY of the QDs in two-phase resin comprising the like. One or more emulsifying agents, Surfactants, or acrylate (phase 1) and polyurethane acrylate (Dymax OP-4other compounds useful for Supporting stable emulsions 26032, phase 2) is represented by triangle-shaped data may be used. 50 points in the plot illustrated in FIG. 5. According to certain embodiments, such as the embodi Example 3 ment illustrated in FIG. 2, the resin mixture is laminated between gas barrier films 404. Examples of gas barrier films Green InP/ZnS QDs (120 Optical Density (OD)) were include FTB3-50 (available from 3M, St. Paul, Minn.) and GX50W or GX25W (available from Toppan Printing Co., 55 prepared as described in U.S. patent application Ser. No. 13/624,632, filed Sep. 23, 2011. The QDs were re-dispersed LT, Japan). Upon curing 405, the laminated resin film yields a polymer film having regions of phase 1 polymer, contain in degassed lauryl methacrylate (LMA, 1.2 mL) by Stirring ing QDS, dispersed throughout phase 2 polymer, as illus under nitrogen overnight. IRG819 photoinitiator (3 mg) was trated in FIG. 3. dissolved in 0.6 mL of the QD dispersion in LMA. TMPTM 60 crosslinker (0.073 mL) was then added. The mixture was EXAMPLES further stirred for 30 min under nitrogen, affording phase 1 resin with QD concentration at 89.2 OD/mL. Two-phase Example 1A resin was obtained by mixing 67 microliters of phase 1 resin with 0.43 mL degassed epoxy (Epotek, OG142), upon which Green InP/ZnS QDs (120 Optical Density (OD)) were 65 the mixture was mechanically stirred for 3 min at 100 rpm prepared as described in U.S. patent application Ser. No. under nitrogen. 60 Microliters of the two-phase resin was 13/624,632, filed Sep. 23, 2011, the entire contents of which then laminated between 3M gas barrier layers on an area US 9,680,068 B2 8 7 limited by a 19 mm x 14 mmx0.051 mm plastic spacer. The films were cured with a Mercury lamp for 1 min. Example 4 Green InP/ZnS QDs (120 Optical Density (OD)) were prepared as described in U.S. patent application Ser. No. 13/624,632, filed Sep. 23, 2011. The QDs were dispersed in degassed lauryl methacrylate (LMA, 2.64 mL) containing IRG819/IRG651 photoinitiators (9/18 mg) by stirring under nitrogen overnight. TMPTM crosslinker (0.32 mL) was Effect of Refractive Index of Phase 2 Resin (RI of phase 1 resin = 1.47). Sam Initial Initial Phase 2 5 1 60 69 Urethane 2-phase 2-phase QY EQE 1.47 60 72 1.55 S4 59 1.58 69 Urethane 10 69 acrylate (Dymax OP4 4-26032) Epoxy (Epotek OG142) 59 58 15 25 30 35 40 45 50 As shown in Table 1, when the RI of the first phase and that of the second phase are matched, the initial QY and EQE of the film is maximized. When there is mismatch between the RIs of the first and second phase resins, the initial QY and EQE of the film is reduced. Thus, it is beneficial, where possible, to use first and second phase resins that have closely matched RIs. According to some embodiments, the RIs of the two resins differ by less than about 5%. According to some embodiments, the RIs of the two resins differ by less than about 1%. Accordingly, additives such as Surfactants, viscosity modifiers, monomers, light scattering agents, and other inorganic Surface tension modifiers may be used to adjust the RI of one or both phases so that the RIs match. Such additives may also be used to minimize chemical interaction between the phases. Moreover, chemical anti-oxidants (di laurylthiodipropionate, octadecylsulfide, octadecanethiol, cholesteryl palmitate, Zinvisible, ascorbic acid palmitate, alpha tocopherol, BHA, BHT, octane thiol, lipoic acid, gluthathion, sodium metabisulfite, trioctyl phosphine (TOP), tetradecylphosphonic acids, polyphenols) may be added to one or both phases to minimize the degradation of QDS around the edges of the two-phase/gas barrier encapsulated QD films. The inventive concepts set forth herein are not limited in their application to the construction details or component arrangements set forth in the above description or illustrated in the drawings. It should be understood that the phraseology and terminology employed herein are merely for descriptive purposes and should not be considered limiting. It should further be understood that any one of the described features may be used separately or in combination with other fea tures. Other invented Systems, methods, features, and advan tages will be or become apparent to one with skill in the art upon examining the drawings and the detailed description herein. It is intended that all such additional systems, methods, features, and advantages be protected by the accompanying claims. What is claimed is: 55 and above T70 606 for at least 2000 hours. Effect of Refractive Index of Phase 2 Resin The phase 1 LMA resin used in the above Examples has a refractive index (RI) of 1.47. Table 1 illustrates the effect of the RI of the phase 2 resin effects the optical properties of the two-phase films. RI of cured Phase 2 Resin QY EQE Resin acrylate (OP4 4-20639) added. The mixture was further stirred for 30 min under nitrogen affording phase 1 resin. Non-crosslinkable, non Viscous acrylate phase 2 resin was prepared by dissolving 10.1 mg IRG819 in deoxygenated glycidyl methacrylate (GMA, 1 mL). Non-crosslinkable, viscous acrylate phase 2 resin was prepared by dissolving polyvinylidene chloride (PVDC, Saran F310, 1.5 g) in deoxygenated GMA/IRG819/ IRG651 (8.5 mL/57.5 mg/115.3 mg) solution. Two-phase resin was obtained by mixing 148 microliters of the phase 1 resin with 0.5 mL degassed phase 2 resin and the mixture was mechanically stirred for 3 min at 100 rpm under nitrogen. 60 microliters of the two-phase resin was then either added to the well of a 19 mmx14 mm glass plate or laminated between 3M gas barrier layers on an area limited by a 19 mmx14mmx0.051 mm plastic spacer. The film was finally cured with Mercury lamp for 5 min. Stability of Resin Films FIG. 5 is a plot illustrating the quantum yield of resin films of QDs upon exposure to a blue backlight unit (BLU) for amounts of time (time, in days, denoted on the X-axis). The QY of green QDs in a single-phase LMA resin, as prepared in Example la above, is represented by Square data points 501. The single-phase resin film has an initial QY of about 60%, but the QY drops substantially during the first week of exposure. Diamond-shaped data points 502 represent the QY of a two-phase film of LMA/epoxy resin containing QDS pre pared as describe in Example 1b above. The initial QY of the LMA/epoxy two-phase film is also about 60%, but unlike that of the single-phase film, the QY of the two-phase film remains constant over the time period of the experiment. The stability of the QY indicates that the two-phase film effec tively prevents oxidation of the QDs. Triangle-shaped data points 503 represent QY a two phase film of QDs in LMA/polyurethane acrylate, as pre pared in Example 2 above. The initial QY of the LMA/ polyurethane acrylate film is about 45% and remains stable for over three months. FIG. 6 illustrates stability studies of the two-phase LMA/epoxy film prepared in Example 1b. LED intensity 601, efficacy 602, photoluminescence inten sity 603, QD/LED ratio 604, and % EQE 605 remain stable ple 60 1. A method of preparing a film, the method comprising: forming an emulsion comprising a first phase that com prises a first polymer and quantum dots and a second phase that comprises a second polymer; depositing the emulsion between gas barrier sheets to form a film; and curing the first and second polymers. k k k k k

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