Color Conversion Film for Backlight Unit
20230061049 · 2023-03-02
Assignee
Inventors
Cpc classification
G02F1/133614
PHYSICS
G02F1/133606
PHYSICS
G02F1/133617
PHYSICS
G02F1/133611
PHYSICS
International classification
Abstract
A color conversion film for a backlight unit that includes an array of light emitting diodes. The color conversion film includes a substantially planar base portion, and a plurality of three-dimensional structures extending from the substantially planar base portion. Each of the three-dimensional structures has at least one sloped surface with a base angle of about 55°-75° relative to the substantially planar base portion. The color conversion film includes a material having a refractive index of about 1.5-1.7.
Claims
1-16. canceled
17. A color conversion film for a backlight unit comprising an array of light emitting diodes, the color conversion film comprising: a) a substantially planar base portion configured to receive light from a light source positioned below the substantially planar base portion; and b) a plurality of three-dimensional structures configured to extend from the substantially planar base portion in a direction away from the light source, each of the plurality of three-dimensional structures having at least one sloped surface at an angle Θ relative to the substantially planar base portion such that each of the plurality of three-dimensional structures comprises a decreasing cross-section as light travels away from the light source.
18. The color conversion film according to claim 17, wherein the substantially planar base portion has a thickness of up to about 15 μm.
19. The color conversion film according to claim 17, wherein the color conversion film comprises a material having a refractive index in a range of about 1.5-1.7.
20. The color conversion film according to claim 17, wherein the color conversion film comprises phosphor material.
21. The color conversion film according to claim 17, wherein the color conversion film comprises a material having quantum dots.
22. The color conversion film according to claim 17, wherein each of the plurality of three-dimensional structures is cone shaped.
23. The color conversion film according to claim 22, wherein a peak of at least one of the plurality of three-dimensional structures is truncated and/or rounded.
24. The color conversion film according to claim 17, wherein each of the plurality of three-dimensional structures is pyramid shaped.
25. The color conversion film according to claim 24, wherein a peak of at least one of the plurality of three-dimensional structures is truncated and/or rounded.
26. The color conversion film according to claim 17, wherein bases of the plurality of three-dimensional structures cover a majority of the substantially planar base portion.
27. The color conversion film according to claim 17, wherein bases of the plurality of three-dimensional structures are tiled together.
28. The color conversion film according to claim 17, wherein the plurality of three-dimensional structures comprises bases having widths in the range of about 30 μm to about 75 μm.
29. The color conversion film according to claim 17, wherein the angle Θ comprises an angle between 55°-75°.
30. The color conversion film according to claim 17, wherein the angle Θ comprises an angle of nominally 60°.
31. The color conversion film according to claim 17, wherein the angle Θ comprises an angle of nominally 70°.
32. A color conversion film for a backlight unit comprising an array of light emitting diodes, the color conversion film comprising: a) a substantially planar base portion configured to receive light from a light source positioned below the substantially planar base portion; and b) a plurality of three-dimensional structures configured to extending from the substantially planar base portion in a direction away from the light source, each of the plurality of three-dimensional structures having at least one sloped surface with a base angle relative to the substantially planar base portion such that each of the plurality of three-dimensional structures comprises a decreasing cross-section as light travels away from the light source.
33. The color conversion film according to claim 32, wherein the color conversion film comprises a material having quantum dots.
34. The color conversion film according to claim 32, wherein each of the plurality of three-dimensional structures has a cone shape.
35. The color conversion film according to claim 32, wherein each of the plurality of three-dimensional structures has a pyramid shape.
36. The color conversion film according to claim 32, wherein the substantially planar base portion has a thickness of up to about 15 μm
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0022] The components of the following figures are illustrated to emphasize the general principles of the present disclosure and are not necessarily drawn to scale, although at least one of the figures may be drawn to scale. Reference characters designating corresponding components are repeated as necessary throughout the figures for the sake of consistency and clarity.
[0023]
[0024]
[0025]
[0026]
DETAILED DESCRIPTION
[0027]
[0028] As also illustrated in
[0029]
[0030] The bases of the three-dimensional structures 334 desirably cover the majority, if not all, of the base portion 332, i.e., the three-dimensional structures 334 are tiled closely together. In an embodiment, the widths of the bases of the three-dimensional structures 334 may be in the range of about 30 μm to about 75 μm. The slopes of the side walls of the three-dimensional structures 334 should generally have relatively high angles, as represented by the angle θ in
[0031] For example, if the color conversion layer 330 contains a phosphor material and has a refractive index (n) of 1.6, and the material in contact with the steep sides of the three-dimensional structures 334 has a refractive index (n) of 1.5, then the slopes of the sides of the structures 334, represented by angle θ, should be ˜70 degrees relative to the base portion 332. This allows for the light rays that are almost normal (˜90 degrees), represented by arrow 200, to be guided by total internal reflection (TIR), whereas the low angle light rays, represented by arrow 210, will not be guided, which has the potential of equalizing the distances that each of the types of light rays 200, 210 travel in the color conversion material before exiting the color conversion layer 330 as light rays represented by arrows 400 and 410, respectively, in
[0032] The design of the three-dimensional structures 334 that equalize the relative absorptions of the blue light with different incident angles depends on the refractive index of the various materials in the adjacent layers, and also the thickness of the base portion 332 that includes a phosphor material or quantum dots, which in some embodiments may be optional. As understood by one of ordinary skill in the art, the thickness of the base portion 332 of the color conversional layer 330 with depend on, in part, the size and concentration of the phosphor particles or quantum dots in the material used for the color conversion layer 330, for example a lower concentration of color changing material would require larger structures to compensate
Modelled Performance
[0033] A variety of structures for the color conversion layer 330 were modelled to predict the absorption properties of the color conversion layer 330 with respect to blue light entering the color conversion layer 330 at different angles, which were grouped at 85°-90°, 80°-90°, 65°-70°, 50°-55°, and 42.5°-47.5°. An absorption value of 1.0 means the light is expected to be fully absorbed by the color conversion layer 330, and an absorption value of 0.0 means the light is not expected to be absorbed at all by the color conversion layer 330. Two different embedded phosphor structures with phosphor material having a refractive index of n=1.6 and n=1.7, and a surrounding material of n=1.5 were used, as well as two different base portion 332 thicknesses of 5 μm and 15 μm. A control having no three-dimensional structures was also modelled across the various incoming ray angles. The results of the modelling are listed in Tables I-IV below.
[0034] For the first set of data, the thickness of the base portion 332 of the color conversion layer 330 was set to 5 μm, the refractive index of the phosphor material in the color conversion layer 330 was set to 1.7, and the cladding material in the layer 340 above the three-dimensional structures 334 was set to 1.5 so that the difference (A) between the refractive indices was 0.2. The three-dimensional structures 334 were in the shapes of a four-sided pyramid (‘Pyramid”), a three-sided pyramid (“Tri-pyramid”), and a cone (“Cone”). The base taper angle θ was input at 45°, 60° and 70°. The results showing the effect of the shape of the three-dimensional structures 334, as well as the base taper angle θ of the three-dimensional structures 334 are listed in Table I.
TABLE-US-00001 TABLE I Predicted Absorption of Blue Light Rays by Color Conversion Layer with 5 μm Base Portion and Refractive Index Δ of 0.2 Taper 85°-90° 80°-90° 65°-70° 50°-55° 42.5°-47.5° Shape of Angle Incoming Incoming Incoming Incoming Incoming Ratio Structure θ (°) Rays Rays Rays Rays Rays 45°/90° None NA 0.18 0.18 0.19 0.21 0.22 1.25 Pyramid 45 0.43 0.43 0.52 0.56 0.53 1.33 Pyramid 60 0.67 0.69 0.65 0.64 0.65 0.97 Pyramid 70 0.94 0.94 0.76 0.72 0.75 0.80 Tri-pyramid 60 0.38 0.40 0.46 0.46 0.48 1.27 Tri-pyramid 70 0.63 0.61 0.55 0.53 0.55 0.88 Cone 60 0.65 0.66 0.65 0.66 0.67 1.03 Cone 70 0.97 0.97 0.77 0.45 0.77 0.85
[0035] The modelling results listed in Table I show the effect of the angle of the incoming light rays on the absorption by the color conversion layer 330. For the color conversion layer with no three-dimensional structures, there is more absorption at lower angles of incidence (i.e. near normal). The results also indicate that a color conversion layer 330 with three-dimensional structures 334 in the shape of a pyramid or cone, and a base taper angle θ of ˜60° are predicted to equalize the relative absorption of high angle and low angle rays of incoming blue light to a desired level. In other words, the structures in the shape of a pyramid or cone and a base taper angle θ of ˜60° should have the most consistent absorption of the incoming blue light across angles of incidence, which is desirable.
[0036] For the next set of data, the thickness of the base portion 332 of the color conversion layer 330 was increased to 15 μm. The refractive index of the material in the color conversion layer 330 was kept at 1.7, and the cladding material in the layer 340 above the three-dimensional structures 334 was kept at 1.5 (Δ=0.2). The results showing the effect of the shape of the three-dimensional structures 334, as well as the base taper angle θ of the three-dimensional structures 334 are listed in Table II.
TABLE-US-00002 TABLE II Predicted Absorption of Blue Light Rays by Color Conversion Layer with 15 μm Base Portion and Refractive Index Δ of 0.2 Taper 85°-90° 80°-90° 65°-70° 50°-55° 42.5°-47.5° Shape of Angle Incoming Incoming Incoming Incoming Incoming Ratio Structure θ (°) Rays Rays Rays Rays Rays 45°/90° None NA 0.44 0.44 0.46 0.50 0.52 1.19 Pyramid 45 0.61 0.61 0.68 0.72 0.74 1.21 Pyramid 60 0.77 0.78 0.77 0.77 0.78 1.02 Pyramid 70 0.96 0.96 0.84 0.82 0.85 0.88 Tri-pyramid 60 0.57 0.59 0.64 0.66 0.68 1.18 Tri-pyramid 70 0.75 0.73 0.70 0.70 0.72 0.97 Cone 60 0.76 0.77 0.76 0.78 0.80 1.05 Cone 70 0.94 0.94 0.85 0.84 0.86 0.91
[0037] The modelling results listed in Table II indicate that a color conversion layer 330 with three-dimensional structures 334 in the shape of a pyramid or cone, and a base taper angle θ of ˜60°, as well as a tri-pyramid with a base angle of θ of ˜70°, are predicted to equalize the relative absorption of high angle and low angle rays of incoming blue light to a desirable level.
[0038] For the next set of data, the thickness of the base portion 332 of the color conversion layer 330 was set to 5 μm, the refractive index of the material in the color conversion layer 330 was decreased to 1.6, and the cladding material in the layer 340 above the three-dimensional structures 334 was kept at 1.5 so that the difference (Δ) between the refractive indices was 0.1. The results showing the effect of the shape of the structures, as well as the base taper angle θ of the three-dimensional structures 334 are listed in Table III.
TABLE-US-00003 TABLE III Predicted Absorption of Blue Light Rays by Color Conversion Layer with 5 μm Base Portion and Refractive Index Δ of 0.1 Taper 85°-90° 80°-90° 65°-70° 50°-55° 42.5°-47.5° Shape of Angle Incoming Incoming Incoming Incoming Incoming Ratio Structure θ (°) Rays Rays Rays Rays Rays 45°/90° None NA 0.18 0.18 0.19 0.21 0.23 1.29 Pyramid 45 0.42 0.43 0.44 0.52 0.55 1.28 Pyramid 60 0.54 0.55 0.61 0.62 0.65 1.20 Pyramid 70 0.83 0.79 0.71 0.73 0.77 0.93 Tri-pyramid 60 0.36 0.36 0.41 0.44 0.46 1.28 Tri-pyramid 70 0.50 0.51 0.50 0.51 0.55 1.10 Cone 60 0.54 0.55 0.61 0.63 0.66 1.21 Cone 70 0.81 0.79 0.72 0.74 0.78 0.95
[0039] The modelling results listed in Table III indicate that a color conversion layer 330 with three-dimensional structures 334 in the shape of a pyramid or cone, and a base taper angle θ of ˜70° are predicted to equalize the relative absorption of high angle and low angle rays of incoming blue light to a desirable level.
[0040] For the next set of data, the thickness of the base portion 332 of the color conversion layer 330 was increased back to 15 μm, the refractive index of the material in the color conversion layer 330 was kept at 1.6, and the cladding material in the layer 340 above the three-dimensional structures 334 was kept at 1.5 (Δ=0.1). The results showing the effect of the shape of the three-dimensional structures 334, as well as the base taper angle θ of the three-dimensional structures 334 are listed in Table IV.
TABLE-US-00004 TABLE IV Predicted Absorption of Blue Light Rays by Color Conversion Layer with 15 μm Base Portion and Refractive Index Δ of 0.1 Taper 85°-90° 80°-90° 65°-70° 50°-55° 42.5°-47.5° Shape of Angle Incoming Incoming Incoming Incoming Incoming Ratio Structure θ (°) Rays Rays Rays Rays Rays 45°/90° None NA 0.44 0.44 0.46 0.51 0.54 1.22 Pyramid 45 0.61 0.61 0.63 0.70 0.72 1.20 Pyramid 60 0.68 0.69 0.74 0.76 0.79 1.15 Pyramid 70 0.88 0.86 0.80 0.83 0.86 0.97 Tri-pyramid 60 0.56 0.56 0.61 0.64 0.67 1.20 Tri-pyramid 70 0.65 0.66 0.67 0.69 0.73 1.11 Cone 60 0.69 0.69 0.74 0.77 0.79 1.16 Cone 70 0.87 0.85 0.81 0.83 0.86 0.99
[0041] The modelling results listed in Table IV indicate that a color conversion layer 330 with three-dimensional structures 334 in the shape of a pyramid or cone, and a base taper angle θ of ˜70° are predicted to equalize the relative absorption of high angle and low angle rays of incoming blue light to a desirable level.
[0042] A review of all of the modelling results indicates that as the difference between the refractive indices of the color conversion layer 330 and the layer in direct contact with the three-dimensional structures 334 increases, the optimal base angles θ for the three-dimensional structures 334 should decrease to achieve the desired equalization of the relative absorption of the high angle and low angle rays of incoming blue light. In addition, increasing the thickness of the base portion 332 of the color conversion layer 330 generally increases the absorption of the blue light, as expected. By adjusting the relative thickness of the base portion 332, the shape of the three-dimensional structures 334, and the refractive index of the color conversion material of the color conversion layer 330 and of the material in the layer 340 in contact with the three-dimensional structures 334, it is possible to equalize the absorption of the low and high angle light rays, or in some cases to actually have higher absorption of the low angle or normal light.
[0043] The three-dimensional structures 334 of the color conversion layer 330 according to embodiments described herein may be created using many techniques known in the art. For example, in an embodiment, the shape of the three-dimensional structures 334 may be cast onto a substrate using a suitable master mold, and thermally-curing polymer or ultraviolet (UV) light curing polymer, or the shape may be impressed into a thermoplastic substrate through compression molding or other molding, or may be created at the same time as the substrate using extrusion-embossing or injection molding. The three-dimensional structures 334 may be produced by replicating a master. For example, an optical diffuser may be made by replication of a master containing the desired shapes as described in U.S. Pat. No. 7,190,387 B2 to Rinehart et al., entitled “Systems And Methods for Fabricating Optical Microstructures Using a Cylindrical Platform and a Rastered Radiation Beam”; U.S. Pat. No. 7,867,695 B2 to Freese et al., entitled “Methods for Mastering Microstructures Through a Substrate Using Negative Photoresist”; and/or U.S. Pat. No. 7,192,692 B2 to Wood et al., entitled “Methods for Fabricating Microstructures by Imaging a Radiation Sensitive Layer Sandwiched Between Outer Layers”, assigned to the assignee of the present invention, the disclosures of all of which are incorporated herein by reference in their entireties as if set forth fully herein. The masters themselves may be fabricated using laser scanning techniques described in these patents, and may also be replicated to provide diffusers using replicating techniques described in these patents.
[0044] In an embodiment, the second substrate 340 may have its three-dimensional structures 344 created in the same manner described above with respect to the three-dimensional structures 334. The desired material(s) to be used for the color conversion layer 330 may then be applied to the three-dimensional structures 344 of the second substrate 340 and fill in the voids in between the three-dimensional structures 344 so that the color conversion layer 330 is formed with the three-dimensional structures 334 in between the three-dimensional structures 344.
[0045] Embodiments of the present invention mitigate the issues identified above caused by light coming into the color conversion layer at different angles by creating similar path-lengths through the color conversion layer, and as a result, similar absorptions. In order to achieve similar path lengths for high and low angle light, the color conversion layer includes three-dimensional structures containing, for example, phosphors or quantum dots, that guide the incoming low angle and normal light, and have a higher refractive index relative to the surrounding material. Each of the three-dimensional structures desirably has a wide base that faces the source of the blue light, and then a taper extended away from the source of the blue light, so that the three-dimensional structure has a decreasing cross-section as the light travels away from the light source.
[0046] The embodiments described herein represent a number of possible implementations and examples and are not intended to necessarily limit the present disclosure to any specific embodiments. Instead, various modifications can be made to these embodiments, and different combinations of various embodiments described herein may be used as part of the invention, even if not expressly described, as would be understood by one of ordinary skill in the art. Any such modifications are intended to be included within the spirit and scope of the present disclosure and protected by the following claims.