Patent Application
20220357493
Reflective films including multiple polymeric layers are known. Examples of such films are mirrors and polarizers which include alternating polymeric layers in which the adjacent layers have different refractive indices.
Displays may exhibit variable black state reflectivity properties.
In some aspects of the present disclosure, a display system is provided. The display system can include a display including a plurality of pixels and configured to emit an image for viewing by a viewer and a reflective polarizer disposed on the display. For substantially normally incident light, for a primary wavelength λb, the reflective polarizer can transmit at least 60% of the incident light having a first polarization state x and reflect at least 60% of the incident light having an orthogonal second polarization state y, and for each of a first wavelength λuv and a second wavelength λbg, 0<λb-λuv≤100 nm and 0<λbg-λb≤100 nm, the reflective polarizer can transmit at least 40% of the incident light for each of the first and second polarization states. The display system can also include a retarder layer disposed between the reflective polarizer and the display, such that when a substantially white incident light is incident on the display system at an incident angle θ1, the display system reflects at least a portion of the incident light, after the incident light is reflected at least twice by the display as an exiting light propagating at an exit angle θ2 substantially equal to the incident angle, and a maximum difference between corresponding CIE 1931 color chromaticity coordinates x and y of the incident and exiting lights can be less than about 0.1 at least when the incident angle is substantially equal to zero.
In some aspects of the present disclosure, a display system is provided. The display system can include a display configured to emit an image in a visible wavelength range, and the display can include a blue pixel configured to emit blue light. The emitted blue light can have a blue peak at a blue wavelength λb in the visible wavelength range. The display system can also include a linear absorbing polarizer layer disposed on the display, a reflective polarizer disposed between the linear absorbing polarizer layer and the display, and a retarder layer disposed between the reflective polarizer and the display and having a deviation A from being a quarter-wave retarder. For a substantially normally incident light: for the blue wavelength Xb, the reflective polarizer can transmit at least 60% of light having a first polarization state and reflect at least 60% of light having an orthogonal second polarization state, for at least one wavelength less than λb, λb-λuv≤50 nm, and for each wavelength λ in the visible wavelength range, λ-λb≥50 nm, the reflective polarizer can transmit at least 40% of the incident light for each of the first and second polarization states. Δ can be Δb at the wavelength λb, and Δr at at least one red wavelength λr in the visible wavelength range, λr-λb≥100 nm, Δb≤Δr, and for the first polarization state, the linear absorbing polarizer can have a greater transmittance at the red wavelength λr than at the blue wavelength λb.
In some aspects of the present disclosure, a display system is provided. The display system can include an emissive display including a blue pixel configured to emit blue light having a blue peak at a blue wavelength λb, a green pixel configured to emit green light having a green peak at a green wavelength λg, and a red pixel configured to emit red light having a red peak at a red wavelength λr. The display system can also include a reflective polarizer disposed on the emissive display and a retarder layer disposed between the reflective polarizer and the emissive display and having a deviation Δ from being a quarter-wave retarder. For a substantially normally incident light: for the blue wavelength λb and for at least one infrared wavelength λir, the reflective polarizer transmits at least 60% of light having a first polarization state and reflects at least 60% of light having an orthogonal second polarization state, for each of the green and red wavelengths λg and λr, the reflective polarizer transmits at least 40% of the incident light for each of the first and second polarization states, and Δ is αb and αr at the respective blue and red wavelengths λr, and λr, Δb≤Δr. For light incident at at least one incident angle between about 10 and 60 degrees, and for the red wavelength λr, the reflective polarizer can transmit at least 50% of light having the first polarization state and reflect at least 50% of light having the second polarization state.
In the following description, reference is made to the accompanying drawings that form a part hereof and in which various embodiments are shown by way of illustration. The drawings are not necessarily to scale. It is to be understood that other embodiments are contemplated and may be made without departing from the scope or spirit of the present description. The following detailed description, therefore, is not to be taken in a limiting sense.
Wavelength and polarization dependent partial reflectors can be useful for improving reflected color properties, or black state properties, of an emissive display when the partial reflector is used in a circular polarizer of the emissive display. The partial reflectors may be reflective polarizers since the partial reflectors, in some embodiments, have different reflection properties for two orthogonal polarization states. The partial reflectors may be birefringent multilayer optical films with controlled band edges and tailored reflectivity with incidence angle.
In some embodiments, the optical stack 200 includes a plurality of elements in optical communication with each other including, but not limited to, a retarder layer 10, a linear absorbing polarizer 20 and a reflective polarizer 30. The reflective polarizer 30 can be disposed between, or substantially between, the linear absorbing polarizer 20 and the retarder layer 10. The reflective polarizer 30 can be bonded to the retarder layer 10 by a first adhesive layer 60 and the reflective polarizer 30 can be bonded to the linear absorbing polarizer 30 by a second adhesive layer 70.
One or both of the first adhesive layer 60 and the second adhesive layer 70 may be an optically clear adhesive (e.g., an adhesive having a haze as determined by the ASTM D1003-13 standard, for example, of less than about 5%, or less than about 2%, and a luminous transmittance as determined by the ASTM D1003-13 standard, for example, of at least about 80% or at least about 90%). In some embodiments, one or both of the first adhesive layer 60 and second adhesive layer 70 may include pressure-sensitive adhesives, UV-curable adhesives and/or polyvinyl alcohol-type adhesives.
The reflective polarizer 30 can be a multilayer optical film that includes an optical stack having a plurality of optical repeat units. Each optical repeat unit can include a plurality of polymer layers, such as first and second polymer layers. The multilayer optical film can include individual microlayers, where “microlayers” refer to layers sufficiently thin such that light reflected and/or transmitted at interfaces between such layers is primarily due to constructive or destructive interference to give the multilayer optical film desired reflective or transmissive properties. The microlayers can together represent one optical repeat unit (ORU) of the multilayer stack, an ORU being the smallest set of layers that recur in a repeating pattern throughout the thickness of the stack. The microlayers can have different refractive index characteristics so that some light is reflected at interfaces between adjacent microlayers. For optical films designed to reflect light at ultraviolet, visible, or near-infrared wavelengths, each microlayer typically has an optical thickness (i.e., a physical thickness multiplied by the relevant refractive index) of less than about 1 micrometer. In some cases, each microlayer has an optical thickness that is substantially equal to about ¼ of a corresponding wavelength. Thicker layers can, however, also be included, such as skin layers at the outer surfaces of the film, or protective boundary layers (PBL) disposed within the film that, for example, separate packets of microlayers. In some embodiments, only a single packet or stack of microlayers is included in a given optical film.
The linear absorbing polarizer 20 of the present disclosure can substantially transmit light having one polarization state, while substantially absorbing light having an orthogonal polarization state. One useful type of linear absorptive polarizer 20 is a dichroic polarizer. Dichroic polarizers are made, for example, by incorporating a dye into a polymer sheet that is then stretched in one direction. Dichroic polarizers can also be made by uniaxially stretching a semicrystalline polymer such as polyvinyl alcohol, then staining the polymer with an iodine complex or a dichroic dye, or by coating a polymer with an oriented dichroic dye. These polarizers often use polyvinyl alcohol as the polymer matrix for the dye. Dichroic polarizers generally have a large amount of absorption of light. In some embodiments, the linear absorbing polarizers are “weak” linear absorbing polarizers that have a contrast ratio (ratio of pass state transmission to block state transmission) of less than about 100:1, 10:1 or 5:1.
The retarder layer 10 can include films, coatings or a combination of films and coatings. Exemplary films include birefringent polymer film retarders, such as those available from Meadowlark Optics (Frederick, Colo.), for example. Exemplary coatings for forming a retarder layer include the linear photopolymerizable polymer (LPP) materials and the liquid crystal polymer (LCP) materials described in U.S. Pat. App. Pub. No. 2002/0180916 (Schadt et al.), U.S. Pat. App. Pub. No. 2003/028048 (Cherkaoui et al.), U.S. Pat. App. Pub. No. 2005/0072959 (Moia et al.) and U.S. Pat. App. Pub. No. 2006/0197068 (Schadt et al.), and in U.S. Pat. No. 6,300,991 (Schadt et al.). Suitable LPP materials include ROP-131 EXP 306 LPP and suitable LCP materials include ROF-5185 EXP 410 LCP, both available from ROLIC Technologies Ltd. (Allschwil, Switzerland).
Within the ultraviolet wavelength range 45, blue wavelength range 40, green wavelength range 41, red-infrared wavelength range 42, red wavelength range 43 and infrared wavelength range 44, respective ranges of deviations Δ can exist for different wavelengths λ. A deviation Δb min can be the minimum deviation at wavelength λb min among the range of deviations Δ within the blue wavelength range 40. A deviation Δg min can be the minimum deviation at wavelength λg min among the range of deviations Δ within the green wavelength range 41. A deviation Δri min can be the minimum deviation at wavelength λri min among the range of deviations Δ within the red-infrared wavelength range 42. In some embodiments, the minimum Δb min value is less than one or both of minima Δg min and Δri min.
In some embodiments, the reflective polarizer 30 transmits a portion of substantially normal incident light having a first polarization state x at one or more of the wavelengths λb, λg and λri within blue wavelength range 40, green wavelength range 41 and red-infrared wavelength range 42, respectively. In some embodiments, the first polarization state x can be substantially a linear polarization oriented along the x-axis, meaning that the electric field vector of light propagating along the z-axis is confined, or substantially confined, to the xz-plane. The reflective polarizer 30 can, in various implementations, transmit, transmit substantially, transmit about, or transmit at least 50%, 55%, 60%, 65%, 70%, 75%, 80%, 85%, 90% or 95% of substantially normal incident light having the first polarization state x at one or more of λb, λg and λri. While
In some embodiments, the reflective polarizer 30 reflects a portion of substantially normal incident light having a second polarization state y (orthogonal to the first polarization state x) at one or more of the wavelengths λb, λg and λri. In some embodiments, the second polarization state y can be substantially a linear polarization oriented along the y-axis, meaning that the electric field vector of light propagating along the z-axis is confined, or substantially confined, to the yz plane. The reflective polarizer 30 can, in various implementations, reflect, reflect substantially, reflect about, or reflect at least 50%, 55%, 60%, 65%, 70%, 75%, 80%, 85%, 90% or 95% of substantially normal incident light having the second polarization state y at one or more of λb, λg and λn.
In some embodiments, the reflective polarizer 30 transmits a portion of substantially normal incident light having the first polarization state x and/or the second polarization state y at one or more of λgri and λbg. λgri can be between λg and λri while λbg can be between λg and λb. The reflective polarizer 30 can, in various implementations, transmit, transmit substantially, transmit about, or transmit at least 50%, 55%, 60%, 65%, 70%, 75%, 80%, 85%, 90% or 95% of substantially normal incident light having the first polarization state x and/or the second polarization state y at one or more of λgri and λbg.
For substantially normally incident light, the linear absorbing polarizer layer 20 has an average transmittance Tb across the blue wavelength range 40, an average transmittance Tg across the green wavelength range 41 and an average transmittance Tri across the red-infrared wavelength range 42. In some embodiments, Tb is less than one or both of Tg and Tri.
Turning to
For an exemplary wavelength λb within the blue wavelength range 40, the reflective polarizer can, in various implementations, transmit, transmit substantially, transmit about, or transmit at least 50%, 55%, 60%, 65%, 70%, 75%, 80%, 85%, 90% or 95% of substantially normal incident light having a first polarization state x. In some embodiments, for the exemplary wavelength λb, the reflective polarizer can, in various implementations, reflect, reflect substantially, reflect about, or reflect at least 50%, 55%, 60%, 65%, 70%, 75%, 80%, 85%, 90% or 95% of substantially normal incident light having a second polarization state y orthogonal, or substantially orthogonal, to the first polarization state x, wherein an angle between the polarization states x, y, can be less than 2, 4, 6, 8, 10 or 20 degrees.
A wavelength λuv can be defined in an ultraviolet wavelength range 45 and a wavelength λbg can be defined between wavelength λb and λg within wavelength range 40 or wavelength range 41. In various implementations, 0<λb-λuv≤80, 85, 90, 95, 100, 105, 110, 115 or 120 nm and 0<λbg-λb≤80, 85, 90, 95, 100, 105, 110, 115 or 120 nm and the reflective polarizer 30 transmits, transmits substantially, transmits about, or transmits at least 20%, 25%, 30%, 35%, 40%, 45%, 50%, 55%, 60% or 65% of substantially normal incident light for each of the first polarization state x and the second polarization state y at one or more of λuv and λbg.
As best illustrated in
In some implementations, the incident light 100 and the exiting light 103 have substantially the same color coordinates so that the exiting light 103 is substantially as white as the substantially white incident light 100. In such implementations, a maximum difference between corresponding CIE 1931 color chromaticity coordinates x and y of the incident light 100 and exiting light 103 is less than about 0.1, or less than about 0.1, at least when the incident angle θ1 is substantially equal to zero.
In some embodiments, the reflective polarizer 30 and the retarder layer 10 are disposed between a viewer 90 and the display 80.
In some embodiments, the substantially white incident light 100 is reflected a first time by the display 80 as a first reflected light 101 after being transmitted by the reflective polarizer 30 and the retarder layer 10. The first reflected light 101 can be reflected a second time by the display 80 as a second reflected light 102 after being reflected by the reflective polarizer 30 and transmitted at least once by the retarder layer 10. The second reflected light 102 can exit the display 80 as the exiting light 103. In various embodiments, a maximum difference between corresponding CIE 1931 color chromaticity coordinates x and y of the incident light 100 and exiting light 103 is less than, or less than about, 0.08, 0.06, 0.04 or 0.02 at least when the incident angle θ1 is substantially equal to zero.
In various embodiments, a maximum difference between corresponding CIE 1931 color chromaticity coordinates x and y of the incident light 100 and exiting light 103 is less than about 0.01 for at least one incident angle greater than about 20, about 30 or about 40 degrees.
In some embodiments, the display system 300 includes a retarder layer 10. As described in detail above,
The display system 300 can also include a reflective polarizer 30 and, for substantially normally incident light, for at least one wavelength in an infrared wavelength range 44, the reflective polarizer 30 can transmit at least 40%, 45%, 50%, 55%, 60%, 65%, 70%, 75% or 80% of the incident light having a first polarization state x and can reflect at least 40%, 45%, 50%, 55%, 60%, 65%, 70%, 75% or 80% of the incident light having an orthogonal, or substantially orthogonal, second polarization state y.
In some embodiments, for each wavelength in the red wavelength range 43, the reflective polarizer 30 transmits a portion of the incident light for each of the first and second polarization states x, y. In various embodiments, for each wavelength in the red wavelength range 43, the reflective polarizer 30 transmits at least 20%, 25%, 30%, 35%, 40%, 45%, 50%, 55% or 60% of the incident light for each of the first and second polarization states x, y.
A linear absorbing polarizer layer 20 can also be included with the display system 300. In some embodiments, the linear absorbing polarizer layer 20 has a greater average optical transmittance in the red wavelength range 43 than in the blue wavelength range 40 for the first polarization state x. In some embodiments, the linear absorbing polarizer layer 20 has a greater average optical transmittance in the red wavelength range 43 than in the blue wavelength range 40 for the second polarization state y. In some embodiments, and as illustrated in
The display system 300 can include a linear absorbing polarizer layer 20 disposed on, proximate or adjacent the display 80, and a reflective polarizer 30 can be disposed between the linear absorbing polarizer layer 20 and the display 80. A retarder layer 10 can be disposed between, or substantially between, the reflective polarizer 30 and the display 80. As described above,
In some embodiments, for substantially normally incident light, for an exemplary blue wavelength λb, the reflective polarizer 30 transmits at least a portion of light having a first polarization state x, and reflects at least a portion of light having a second polarization state y. In some embodiments, for substantially normally incident light, for an exemplary blue wavelength λb, the reflective polarizer 30 transmits at least 40%, 45%, 50%, 55%, 60%, 65%, 70%, 75% or 80% of light having a first polarization state x, and reflects at least 40%, 45%, 50%, 55%, 60%, 65%, 70%, 75% or 80% of light having a second orthogonal, or substantially orthogonal, polarization state y.
Exemplary wavelengths λuv and λb are shown in
As described in detail above,
Further, in some embodiments, for the first polarization state y, the linear absorbing polarizer 20 has a greater transmittance at the red wavelength λr than at the blue wavelength λb. In some embodiments, the visible wavelength range extends from about 420 nm to about 650 nm.
In some embodiments, as best shown in
A reflective polarizer 30 can be disposed on the emissive display 80 and a retarder layer 10 can be disposed between, or substantially between, the reflective polarizer 30 and the emissive display 80. As described in detail above,
For substantially normal incident light, for the blue wavelength λb and for at least one infrared wavelength λir, the reflective polarizer 30 can transmit a portion of the incident light having a first polarization state x and can reflect a portion of the incident light having an orthogonal second polarization state y. In some embodiments, for substantially normal incident light, for the blue wavelength λb and for at least one infrared wavelength λir, the reflective polarizer 30 can transmit at least 40%, 45%, 50%, 55%, 60%, 65%, 70%, 75% or 80% of the incident light having a first polarization state x and can reflect at least 40%, 45%, 50%, 55%, 60%, 65%, 70%, 75% or 80% of the incident light having an orthogonal second polarization state y. As described above, light having the first polarization state x can be polarized orthogonally, or substantially orthogonally, to light having the second polarization state y.
In some embodiments, for each of the green and red wavelengths λg and λr, the reflective polarizer 30 transmits a portion of the incident light for each of the first and second polarization states x, y. In some embodiments, for each of the green and red wavelengths λg and λr, the reflective polarizer 30 transmits at least 20%, 25%, 30%, 35%, 40%, 45%, 50%, 55% or 60% of the incident light for each of the first and second polarization states x, y.
As described above,
In some embodiments, the emissive display is an Organic Light-Emitting Diode (OLED) display. In some embodiments, the emissive display is a Micro Light-Emitting Diode (μ-LED) display.
Example 1 and Comparative Example C1
A computational model was used to calculate reflection and transmission properties of a reflective polarizer. The computational model was driven by a 4×4 matrix solver routine based on the Berriman algorithm where the reflection and transmission matrix elements can be computed for an arbitrary stack of 1-dimensional layers, with each layer defined by its physical thickness and the by a dispersive refractive index tensor where each principal element of the refractive index tensor is a function of wavelength (λ). With this computational model, a 1-dimensional stack structure that represents an emissive display was defined and its reflection and transmission properties was computed.
A coordinate system for the computational model was defined, with a cartesian set of axes, x, y and z, shown in
With this computational stack model, the viewer-side reflection characteristics of an Organic LED (OLED) display was modelled with a stack structure of a glass layer (the exterior surface of the display) overtop a circular polarizer, composed of a display-quality iodine-type absorbing polarizer, overlaying a quarter-wave (λ/4) retarder, where the retarder had an extraordinary axis that lied midway between the principal in-plane axes of the absorbing polarizer. Further, underneath the retarder layer, was a dielectric layer, representing the thin-film encapsulant (TFE) which in turn overlaid an OLED emission surface including spatially organized array of voltage-driven blue, green and red emission “pixels” areas, surrounded by metallic-like transistor elements and conducting elements that function as the drivers for the emissive pixels that form the display.
Computation was performed with input from the computational stack model, to predict the degree of brightness increase of the intensity of the blue, green and red pixel emitted light from an OLED emission surface. These predictions were based on analysis of the stack-model-computed reflection and transmission coefficient spectra, coupled with an understanding of the reflection spectrum of the OLED emission surface. Analytic expressions were derived to predict pixel emission color and brightness change that results when a reflective polarizer is included in the circular polarizer of a modelled OLED display stack.
A multilayer optical film reflective polarizer was modeled that included a total of 44 optical repeat units (ORUs) that were modeled as being composed of alternating microlayers of 90/10 coPEN and low refractive index isotropic microlayers. The isotropic layers were modeled as being made as follows. A blend of polycarbonate and copolyesters (PCTg) is made as described in U.S. Pat. No. 10,185,068 (Johnson et al.) such that the index is about 1.57 and such that the layers remains substantially isotropic upon uniaxial orientation of the film. The PC:PCTg molar ratio is approximately 85 mol % PC and 15 mol % PCTg. The PC:PCTg is then blended with PETg at an 85:15 weight ratio ((PC:PCTg):PETg). The high index material, 90/10 coPEN, is referred to as material A, and the low index material is referred to as material B.
A thickness profile of microlayer A and B pairs, or ORUs, was mathematically generated. The phase thickness of the 1st A/B layer pair, is prescribed as 1/2λ0 (wavelength), wherein λ0 is in the deep blue, at approximately 420 nm wavelength. Adjacent A/B ORUs had their physical thicknesses adjusted to have a phase thickness of 1/2λi, where λi was incrementally larger than λ. Further adjoining A/B layer pairs had their phase thickness adjusted to be 1/2λi+1 and so on up through the entire optical film stack, until the last A/B layer pair is reached, with a phase thickness that was 1/2λN, where λN was approximately 580 nm. For this computational example, the film stack included a total of 44 A/B layer pairs, in a monotonic, non-linear A/B ORU profile. In addition, within each AB layer pair, both the A layer and B layer had an individual phase thickness that was 1/4λi.
The physical thickness profile for ORUs is shown in
The OLED can include a blue pixel configured to emit blue light having a blue peak at a blue wavelength of about 450 nm, a green pixel configured to emit green light having a green peak at a green wavelength of about 530 nm, and a red pixel configured to emit red light having a red peak at a red wavelength of about 630 nm. Representative values of the refractive index for the high index optical (HIO) layers (the birefringent 90/10 coPEN), denoted Nx, Ny, Nz along the x, y, z axes, respectively, and for the isotropic low index optical (LIO) layers (Niso is used to denote isotropic refractive indices), are shown in the following table:
Further, the model set-up defined a 400 micrometer glass layer followed by a display absorbing polarizer above the multilayer optical film reflective polarizer. The refractive indices for glass and the dielectric layer immediately above the OLED emission surface are shown in the following table.
The absorbing polarizer was modelled after a Sanritz display polarizer and assumed to be 10 micrometers thick. The refractive index (Niso) and the loss (Kx, Ky, Kz) for the absorbing polarizer are shown in the following table.
In the model, a quarter-wave retarder layer was situated below the reflective polarizer, with its extraordinary axis No, aligned midway at 45 degrees between the x-axis and the y-axis. The refractive index values for the retarder are shown in the following table, as are the deviation values Δ (in nanometers) from quarter-wave, at the representative wavelengths. Comparative Example C1 used a retarder that was approximately quarter wave at a green wavelength and Example 1 used a retarder that was approximately quarter wave at a blue wavelength. These retarder properties were manipulated in the model by changing the retarder thickness.
The OLED emission surface was defined in the model as having metal-like phase rotation properties upon reflection and with reflection coefficient values shown in the following table.
The absorption coefficients for all of the layers in the OLED model, except for the absorbing polarizer, were taken to be insignificantly small.
The computational model was set up to compute the ambient reflection for the circular polarizer. A D65 light source was incorporated in the computation. The CIE 1931 xy chromaticity coordinates for the D65 light source was x=0.3127 and y=0.3291. The normal incidence photopic reflectance for ambient D65 incident light was 7.66%. Chromaticity plots for the reflected light were computed and are shown in
Example 2 and Comparative Example C2
A reflective polarizer and circular polarizers including the reflective polarizer were modeled as in Example 1 and Comparative Example C1 for Example 2 and Comparative Example C2, respectively, except that the physical thickness of the optical repeat units used in the reflective polarizer had the physical thickness profile depicted in
The computational model was set up to compute the ambient reflection for the circular polarizer as described for Example 1. The normal incidence photopic reflectance for ambient D65 incident light was 6.81%. Chromaticity plots for the reflected light were computed and are shown in
Example 3 and Comparative Example C3
A reflective polarizer and circular polarizers including the reflective polarizer were modeled as in Example 1 and Comparative Example C1 for Example 3 and Comparative Example C3, respectively, except that the number of optical repeat units used in the reflective polarizer was reduced to 24 and the physical thickness of the optical repeat units had the physical thickness profile depicted in
The computational model was set up to compute the ambient reflection for the circular polarizer as described for Example 1. The normal incidence photopic reflectance for ambient D65 incident light was 8.06%. Chromaticity plots for the reflected light were computed and are shown in
Example 4 and Comparative Example C4
A reflective polarizer and circular polarizers including the reflective polarizer were modeled as in Example 1 and Comparative Example Cl for Example 4 and Comparative Example C4, respectively, except that the number of optical repeat units used in the reflective polarizer was reduced to 32 and the physical thickness of the optical repeat units had the physical thickness profile depicted in
The computational model was set up to compute the ambient reflection for the circular polarizer as described for Example 1. The normal incidence photopic reflectance for ambient D65 incident light was 8.06%. Chromaticity plots for the reflected light were computed and are shown in
Terms such as “about” will be understood in the context in which they are used and described in the present description by one of ordinary skill in the art. If the use of “about” as applied to quantities expressing feature sizes, amounts, and physical properties is not otherwise clear to one of ordinary skill in the art in the context in which it is used and described in the present description, “about” will be understood to mean within 5 percent of the specified value. A quantity given as about a specified value can be precisely the specified value. For example, if it is not otherwise clear to one of ordinary skill in the art in the context in which it is used and described in the present description, a quantity having a value of about 1, means that the quantity has a value between 0.95 and 1.05, and that the value could be 1.
Descriptions for elements in figures should be understood to apply equally to corresponding elements in other figures, unless indicated otherwise. Although specific embodiments have been illustrated and described herein, it will be appreciated by those of ordinary skill in the art that a variety of alternate and/or equivalent implementations can be substituted for the specific embodiments shown and described without departing from the scope of the present disclosure. This application is intended to cover any adaptations or variations of the specific embodiments discussed herein. Therefore, it is intended that this disclosure be limited only by the claims and the equivalents thereof.
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/IB2020/058946 | 9/24/2020 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 62906852 | Sep 2019 | US |
