Patent Grant
11740496
This disclosure generally relates to illumination from light modulation devices, and more specifically relates to control of privacy display and high efficiency display.
Privacy displays provide image visibility to a primary user that is typically in an on-axis position and reduced visibility of image content to a snooper, that is typically in an off-axis position. A privacy function may be provided by micro-louvre optical films that transmit some light from a display in an on-axis direction with low luminance in off-axis positions. However such films have high losses for head-on illumination and the micro-louvres may cause Moiré artefacts due to beating with the pixels of the spatial light modulator. The pitch of the micro-louvre may need selection for panel resolution, increasing inventory and cost.
Switchable privacy displays may be provided by control of the off-axis optical output.
Control may be provided by means of luminance reduction, for example by means of switchable backlights for a liquid crystal display (LCD) spatial light modulator. Display backlights in general employ waveguides and edge emitting sources. Certain imaging directional backlights have the additional capability of directing the illumination through a display panel into viewing windows. An imaging system may be formed between multiple sources and the respective window images. One example of an imaging directional backlight is an optical valve that may employ a folded optical system and hence may also be an example of a folded imaging directional backlight. Light may propagate substantially without loss in one direction through the optical valve while counter-propagating light may be extracted by reflection off tilted facets as described in U.S. Pat. No. 9,519,153, which is incorporated by reference herein in its entirety.
In a known privacy display the privacy mode is provided by the addition of a removable louver film, such as marketed by 3M Corporation, which may not be reliably or easily fitted or removed by users and therefore in practice, is not assiduously attached by the user every time they are outside the office. In another known privacy display the control of privacy mode is electronically activated but control is vested in the user who must execute a keystroke to enter privacy mode.
According to a first aspect of the present disclosure, there is provided an illumination apparatus comprising: at least one light source arranged to provide input light; a waveguide arrangement comprising at least a first waveguide that extends across a plane and comprises: first and second opposed light guiding surfaces arranged to guide light along the first waveguide, the second light guiding surface being arranged to guide light by total internal reflection; and an input end arranged between the first and second light guiding surfaces and extending in a lateral direction between the first and second light guiding surfaces, the first waveguide being arranged to receive the input light from the at least one light source through the input end, and being arranged to cause light from the at least one light source to exit from the first waveguide through the second light guiding surface by breaking total internal reflection; and an optical turning film component comprising: an input surface arranged to receive the light exiting from the first waveguide, the input surface extending across the plane; and an output surface facing the input surface, wherein the input surface comprises: an array of prismatic elements each comprising a pair of facets defining a ridge therebetween, the ridges extending along an array of lines across the plane in which the input surface extends, wherein the prismatic elements are arranged to deflect the light exiting the first waveguide, the deflection varying in at least one direction across the plane so that the deflected light is directed towards a common optical window in front of the illumination apparatus.
The lines may be curved across the plane so that the deflection varies in a direction that is orthogonal to an optical axis that is normal to the plane, and corresponds to the lateral direction. Advantageously uniformity may be increased in the lateral direction.
The facets may have respective facet angles, defined between a normal to the facet and a normal to the plane, that may vary across the array so that the deflection further varies in a direction orthogonal to the optical axis, and corresponds to a direction that is orthogonal to the lateral direction, so that the deflected light may be directed towards a further, common optical window in front of the illumination apparatus. Facet angles of respective facets, defined between a normal to the facet and a normal to the plane, may vary across the array so that the deflection varies in a direction orthogonal to an optical axis that is normal to the plane, the direction corresponding to a direction orthogonal to the lateral direction. Advantageously uniformity may be increased across the illumination apparatus in the direction orthogonal to the lateral direction.
The first mentioned common optical window and the further common optical window may be defined at different distances in front of the illumination apparatus. Advantageously a wider range of locations for which uniformity is increased is provided.
The first mentioned common optical window and the further common optical window may be defined at the same distance in front of the illumination apparatus. Advantageously the uniformity for an observer at or near the optical window is increased.
The facets may have respective facet angles, defined between a normal to the facet and a normal to the plane, that may vary across the array so that the deflection varies in a direction that is orthogonal to an optical axis normal to the plane and corresponds to a direction orthogonal to the lateral direction.
The lines of the array may have an arithmetic mean tangential angle projected on to the plane of 0° from the lateral direction. Advantageously uniformity may be increased for an on-axis observer.
The lines of the array may have an arithmetic mean tangential angle projected on to the plane that is inclined at more than 0° from the lateral direction. Advantageously uniformity may be increased for an off-axis observer.
The optical turning film component may have a rectangular shape across the plane and the lateral direction may be along a major or minor axis of the rectangular shape. Advantageously a rectangular shape for use in landscape or portrait orientations may be illuminated.
The output surface may be planar. Advantageously the cost of fabrication of the optical turning film component may be reduced.
The facets may have respective facet angles, defined between a normal to the facet and a normal to the plane may be between 40° and 70°, preferably between 42.5° and 65° and more preferably between 42.5° and 62.5°. Advantageously light cones may be directed to desirable optical window locations while achieving increased uniformity.
At least some of the facets may have respective facet angles, defined between a normal to the facet and a normal to the plane, of between 52.5° and 62.5°. In respect of at least some of the facets may have respective facet angles, defined between a normal to the facet and a normal to the plane, of between 42.5° and 52.5°. At least some of the facets may have a respective facet angle, defined between a normal to the facet and a normal to the plane, of between 40° and 52.5°. Advantageously displays may be provided with first and second viewing locations with increased uniformity.
In each pair of facets, a first facet may have a normal on the internal side of the input surface that is inclined towards the input end of the first waveguide and a second facet has a normal on the internal side of the input surface that may be inclined away from the input end of the first waveguide, the first facets having respective facet angles, defined between the normal to the facet and a normal to the plane, that vary across the array so that the deflection varies in a direction that is orthogonal to an optical axis normal to the plane and corresponds to a direction orthogonal to the lateral direction.
The first facets may have respective facet angles, defined between a normal to the facet and a normal to the plane, of between 52.5° and 62.5°. The second facets may have respective facet angles, defined between the normal to the facet and a normal to the plane, that are constant across the array. The second facets may have respective facet angles, defined between the normal to the facet and a normal to the plane, that vary across the array. The second facets may have respective facet angles, defined between a normal to the facet and a normal to the plane, of between 40° and 52.5°. The first facets may have respective facet angles, defined between the normal to the facet and a normal to the plane, that increase across the array with distance from the input end, and the second facets having respective facet angles, defined between the normal to the facet and a normal to the plane, that decrease across the array with distance from the input end. The first facets may have respective facet angles, defined between a normal to the facet and a normal to the plane, of between 42.5° and 52.5° and the second facets have respective facet angles, defined between a normal to the facet and a normal to the plane, of between 42.5° and 52.5°. Advantageously uniformity may be increased.
At least one light source may comprise an array of light sources arrayed across the input end. Advantageously the size of the source may be increased.
The common optical window may be aligned with an optical axis that extends from the centre of the optical turning film component normal to the plane. Advantageously the uniformity may be increased for an on-axis observer.
The common optical window may be offset from an optical axis that extends from the centre of the optical turning film component normal to the plane. Advantageously the uniformity may be increased for an off-axis observer.
The waveguide may further comprise a second input end arranged between the first and second light guiding surfaces opposite to the first mentioned input end, and the illumination apparatus further may comprise at least one second light source arranged to input light into the waveguide through the second input end in an opposite direction from the at least one first mentioned light source. Advantageously first and second illumination profiles may be provided.
The illumination apparatus may further comprise at least one second light source arranged to provide input light in an opposite direction from the at least one first mentioned light source as viewed along the optical axis normal to the plane; the waveguide arrangement may further comprise a second waveguide that extends across the same plane as the first waveguide and may comprise: first and second opposed light guiding surfaces arranged to guide light along the first waveguide, the second light guiding surface being arranged to guide light by total internal reflection; and an input end arranged between the first and second light guiding surfaces and extending in a lateral direction between the first and second light guiding surfaces, the second waveguide being arranged to receive the input light from the at least one second light source through the input end, and being arranged to cause light from the at least one second light source to exit from the second waveguide through the second light guiding surface by breaking total internal reflection, and the input surface of the optical turning film component being arranged to receive the light exiting from the first waveguide and the second waveguide. Advantageously uniformity may be increased.
The lines may be straight and the facets may have respective facet angles, defined between a normal to the facet and a normal to the plane, that vary across the array so that the deflection varies in a direction that is orthogonal to the optical axis and corresponds to a direction orthogonal to the lateral direction so that the deflected light from each input end is directed towards respective common optical windows in front of the illumination apparatus. Advantageously the first and second illumination profiles may provide increased brightness and uniformity across the illumination apparatus.
The deflected light through each input end may be directed towards the same common optical window in front of the illumination apparatus. The respective common optical windows may be in the same location in front of the illumination apparatus. Advantageously display brightness may be increased. Uniformity may be further increased.
The respective common optical windows may be in different locations in front of the illumination apparatus. Advantageously multiple viewing locations with increased uniformity may be provided.
The lines may be curved so that the deflected light input through the first end may be directed towards a common optical window in front of the illumination apparatus and the deflected light input through the second end may be directed towards a virtual common optical window behind the illumination apparatus. Advantageously uniformity may be increased for at least one of the light sources.
The illumination apparatus further comprising a control system may be arranged to control the at least one first light source and the at least one second light source independently. In one mode of operation the control system may be arranged to provide illumination from both the at least one first light source and the at least one second light sources so as to increase spatial uniformity of illumination across the illumination device for at least one viewing location. Advantageously the illumination apparatus may be arranged to switch between at least two different illumination profiles while achieving increased uniformity.
The waveguide may be arranged to cause light from the at least one first light source and the at least one second light source to exit from the waveguide with different angular distributions. Advantageously an illumination apparatus may be arranged to provide illumination for narrow and wider illumination profiles.
The waveguide may be arranged to cause light from the at least one first light source and the at least one second light source to exit from the waveguide with a common angular distribution. Advantageously multiple optical windows may be provided for multiple users or uniformity may be further increased.
The illumination apparatus may comprise: at least one first light source arranged to provide input light; at least one second light source arranged to provide input light in an opposite direction from the at least one first light source, a waveguide arrangement arranged to receive the input light from the at least one first light source and the at least one second light source and to cause light from the at least one first light source and the at least one second light source to exit from the waveguide arrangement by breaking total internal reflection, wherein the waveguide arrangement comprises at least one waveguide; and an optical turning film component comprising: an input surface arranged to receive the light exiting from a waveguide through a light guiding surface of the waveguide by breaking total internal reflection, the input surface extending across the plane; and an output surface facing the input surface, wherein the input surface comprises: an array of prismatic elements each comprising a pair of facets defining a ridge therebetween, the ridges extending along an array of lines across the plane in which the input surface extends, wherein the prismatic elements are arranged to deflect the light exiting the waveguide, the deflection varying in at least one direction across the plane so that the deflected light is directed towards a common optical window in front of the illumination apparatus.
The waveguide arrangement may comprise; a waveguide extending across a plane and comprising: first and second opposed light guiding surfaces arranged to guide light along the optical waveguide, the second light guiding surface being arranged to guide light by total internal reflection, and first and second input ends arranged between the first and second light guiding surfaces and extending in a lateral direction between the first and second light guiding surfaces; wherein the at least one first light source is arranged to input light into the waveguide through the first input end and the at least one second light source is arranged to input light into the waveguide through the second input end, and the waveguide is arranged to cause light from the at least one first light source and the at least one second light source to exit from the waveguide through one of the first and second light guiding surfaces by breaking total internal reflection. Advantageously thickness and cost may be reduced.
The waveguide arrangement may comprise: a first waveguide extending across a plane and comprising first and second opposed light guiding surfaces arranged to guide light along the optical waveguide, the second light guiding surface being arranged to guide light by total internal reflection; and a first input end arranged between the first and second light guiding surfaces and extending in a lateral direction between the first and second light guiding surfaces; wherein the at least one first light source is arranged to input light into the first waveguide through the first input end, and the first waveguide is arranged to cause light from the at least one first light source to exit from the first waveguide through one of the first and second light guiding surface by breaking total internal reflection; a second waveguide extending across the plane in arranged in series with the first waveguide and comprising first and second opposed light guiding surfaces arranged to guide light along the optical waveguide, the second light guiding surface being arranged to guide light by total internal reflection, and a second input end arranged between the first and second light guiding surfaces and extending in a lateral direction between the first and second light guiding surfaces; wherein the at least one second light source is arranged to input light into the second waveguide through the second input end, and the second waveguide is arranged to cause light from the at least one second light source to exit from the second waveguide through one of the first and second light guiding surfaces by breaking total internal reflection, and wherein the first and second waveguides are oriented so that at least one first light source and at least one second light source input light into the first and second waveguides in opposite directions. Advantageously luminance uniformity may be increased.
According to a second aspect of the present disclosure, there is provided a backlight apparatus comprising: an illumination apparatus according to the first aspect; and a rear reflector arranged to receive light exiting from the first surface of waveguide and direct it back through the waveguide. Advantageously efficiency of collection of light from the illumination apparatus is increased.
According to a third aspect of the present disclosure, there is provided a display apparatus comprising: a backlight apparatus according to the second aspect; and a spatial light modulator arranged to receive light from the backlight apparatus. Advantageously a display may be provided with high uniformity for desirable viewing locations. The viewing locations may be controlled by switching of the backlight light sources. The size of the illumination cones may be varied, to achieve switchable display viewing freedom.
The display apparatus may further comprise: at least one display polariser arranged on a side of the spatial light modulator; an additional polariser arranged on the same side of the spatial light modulator as the display polariser; and at least one polar control retarder arranged between the display polariser and the additional polariser, wherein the at least one polar control retarder may include a switchable liquid crystal retarder comprising a layer of liquid crystal material. Advantageously a switchable privacy display may be provided with a privacy mode and public mode of operation. The polar control retarder may cooperate with a switchable backlight to achieve increased viewing freedom in a public mode of operation. Uniformity of privacy mode security factor may be increased.
According to a fourth aspect of the present disclosure, there is provided a vehicle having a display apparatus according to the third aspect mounted therein. Advantageously occupants may be illuminated with high efficiency and may be provided with high luminance uniformity.
According to a fifth aspect of the present disclosure, there is provided an optical turning film component comprising: an input surface for receiving light exiting from a waveguide through a light guiding surface of the waveguide by breaking total internal reflection, the input surface extending across a plane; and an output surface facing the input surface, wherein the input surface comprises: an array of prismatic elements each comprising a pair of facets defining a ridge therebetween, the ridges extending along an array of lines across the plane in which the input surface extends, wherein the prismatic elements may be arranged to deflect the light exiting the waveguide, the deflection varying in at least one direction across the plane so that the deflected light is directed towards a common optical window in front of the illumination apparatus.
According to a sixth aspect of the present disclosure, there is provided illumination apparatus comprising: a waveguide extending across a plane and comprising: first and second opposed light guiding surfaces arranged to guide light along the optical waveguide, the second light guiding surface being arranged to guide light by total internal reflection, and an input end arranged between the first and second light guiding surfaces and extending in a lateral direction between the first and second light guiding surfaces; at least one light source arranged to input light into the waveguide through the input end, wherein the waveguide is arranged to cause light from the light sources to exit from the waveguide through the second light guiding surface by breaking total internal reflection; and an optical turning film component comprising: an input surface arranged to receive the light exiting from the waveguide, the input surface extending across the plane; and an output surface facing the input surface, wherein the input surface comprises: an array of prismatic elements each comprising a pair of facets defining a ridge therebetween, the ridges extending along an array of lines across the plane in which the input surface extends, wherein the prismatic elements are arranged to deflect the light exiting the waveguide, the deflection varying in at least one direction across the plane so that the deflected light is directed towards a common optical window in front of the illumination apparatus. The illumination apparatus may provide light to a common spatial location across at least part of the illumination apparatus. An observer viewing the illumination apparatus at or near the common optical window may advantageously be provided with increased uniformity of luminance across the illumination apparatus. An environmental illumination apparatus may provide a focused illumination region at a desirable working distance.
Embodiments of the present disclosure may be used in a variety of optical systems. The embodiments may include or work with or in cooperation with a variety of illuminators, environmental lighting, interior and exterior automotive illumination, projectors, projection systems, optical components, displays, microdisplays, computer systems, processors, self-contained projector systems, visual and/or audio-visual systems and electrical and/or optical devices. Aspects of the present disclosure may be used with practically any apparatus related to optical and electrical devices, optical systems, presentation systems or any apparatus that may contain any type of optical system. Accordingly, embodiments of the present disclosure may be employed in optical systems, devices used in visual and/or optical presentations, visual peripherals and so on and in computing environments.
Before proceeding to the disclosed embodiments in detail, it should be understood that the disclosure is not limited in its application or creation to the details of the particular arrangements shown, because the disclosure is capable of other embodiments. Moreover, aspects of the disclosure may be set forth in different combinations and arrangements to define embodiments unique in their own right. Also, the terminology used herein is for the purpose of description and not of limitation.
These and other advantages and features of the present disclosure will become apparent to those of ordinary skill in the art upon reading this disclosure in its entirety.
Embodiments are illustrated by way of example in the accompanying FIGURES, in which like reference numbers indicate similar parts, and in which:
Terms related to optical retarders for the purposes of the present disclosure will now be described.
In a layer comprising a uniaxial birefringent material there is a direction governing the optical anisotropy whereas all directions perpendicular to it (or at a given angle to it) have equivalent birefringence.
The optical axis of an optical retarder refers to the direction of propagation of a light ray in the uniaxial birefringent material in which no birefringence is experienced. This is different from the optical axis of an optical system which may for example be parallel to a line of symmetry or normal to a display surface along which a principal ray propagates.
For light propagating in a direction orthogonal to the optical axis, the optical axis is the slow axis when linearly polarized light with an electric vector direction parallel to the slow axis travels at the slowest speed. The slow axis direction is the direction with the highest refractive index at the design wavelength. Similarly the fast axis direction is the direction with the lowest refractive index at the design wavelength.
For positive dielectric anisotropy uniaxial birefringent materials the slow axis direction is the extraordinary axis of the birefringent material. For negative dielectric anisotropy uniaxial birefringent materials the fast axis direction is the extraordinary axis of the birefringent material.
The terms half a wavelength and quarter a wavelength refer to the operation of a retarder for a design wavelength λ0 that may typically be between 500 nm and 570 nm. In the present illustrative embodiments exemplary retardance values are provided for a wavelength of 550 nm unless otherwise specified.
The retarder provides a phase shift between two perpendicular polarization components of the light wave incident thereon and is characterized by the amount of relative phase, Γ, that it imparts on the two polarization components; which is related to the birefringence Δn and the thickness d of the retarder by
Γ=2·π·Δn·d/λ0 eqn. 1
In eqn. 1, Δn is defined as the difference between the extraordinary and the ordinary index of refraction, i.e.
Δn=ne−n0 eqn. 2
For a half-wave retarder, the relationship between d, Δn, and λ0 is chosen so that the phase shift between polarization components is ΓF=π. For a quarter-wave retarder, the relationship between d, Δn, and λ0 is chosen so that the phase shift between polarization components is Γ=π/2.
The term half-wave retarder herein typically refers to light propagating normal to the retarder and normal to the spatial light modulator.
Some aspects of the propagation of light rays through a transparent retarder between a pair of polarisers will now be described.
The state of polarisation (SOP) of a light ray is described by the relative amplitude and phase shift between any two orthogonal polarization components. Transparent retarders do not alter the relative amplitudes of these orthogonal polarisation components but act only on their relative phase. Providing a net phase shift between the orthogonal polarisation components alters the SOP whereas maintaining net relative phase preserves the SOP. In the current description, the SOP may be termed the polarisation state.
A linear SOP has a polarisation component with a non-zero amplitude and an orthogonal polarisation component which has zero amplitude.
A linear polariser transmits a unique linear SOP that has a linear polarisation component parallel to the electric vector transmission direction of the linear polariser and attenuates light with a different SOP.
Absorbing polarisers are polarisers that absorb one polarisation component of incident light and transmit a second orthogonal polarisation component. Examples of absorbing linear polarisers are dichroic polarisers.
Reflective polarisers are polarisers that reflect one polarisation component of incident light and transmit a second orthogonal polarisation component. Examples of reflective polarisers that are linear polarisers are multilayer polymeric film stacks such as DBEF™ or APF™ from 3M Corporation, or wire grid polarisers such as ProFlux™ from Moxtek. Reflective linear polarisers may further comprise cholesteric reflective materials and a quarter waveplate arranged in series.
A retarder arranged between a linear polariser and a parallel linear analysing polariser that introduces no relative net phase shift provides full transmission of the light other than residual absorption within the linear polariser.
A retarder that provides a relative net phase shift between orthogonal polarisation components changes the SOP and provides attenuation at the analysing polariser.
In the present disclosure an ‘A-plate’ refers to an optical retarder utilizing a layer of birefringent material with its optical axis parallel to the plane of the layer.
A ‘positive A-plate’ refers to positively birefringent A-plates, i.e. A-plates with a positive Δn.
In the present disclosure a ‘C-plate’ refers to an optical retarder utilizing a layer of birefringent material with its optical axis perpendicular to the plane of the layer. A ‘positive C-plate’ refers to positively birefringent C-plate, i.e. a C-plate with a positive Δn. A ‘negative C-plate’ refers to a negatively birefringent C-plate, i.e. a C-plate with a negative Δn.
‘O-plate’ refers to an optical retarder utilizing a layer of birefringent material with its optical axis having a component parallel to the plane of the layer and a component perpendicular to the plane of the layer. A ‘positive O-plate’ refers to positively birefringent O-plates, i.e. O-plates with a positive Δn.
Achromatic retarders may be provided wherein the material of the retarder is provided with a retardance Δn·d that varies with wavelength λ as
Δn·d/λ=κ eqn. 3
where κ is substantially a constant.
Examples of suitable materials include modified polycarbonates from Teijin Films. Achromatic retarders may be provided in the present embodiments to advantageously minimise colour changes between polar angular viewing directions which have low luminance reduction and polar angular viewing directions which have increased luminance reductions as will be described below.
Various other terms used in the present disclosure related to retarders and to liquid crystals will now be described.
A liquid crystal cell has a retardance given by Δn·d where Δn is the birefringence of the liquid crystal material in the liquid crystal cell and d is the thickness of the liquid crystal cell, independent of the alignment of the liquid crystal material in the liquid crystal cell.
Homogeneous alignment refers to the alignment of liquid crystals in switchable liquid crystal displays where molecules align substantially parallel to a substrate. Homogeneous alignment is sometimes referred to as planar alignment. Homogeneous alignment may typically be provided with a small pre-tilt such as 2 degrees, so that the molecules at the surfaces of the alignment layers of the liquid crystal cell are slightly inclined as will be described below. Pretilt is arranged to minimise degeneracies in switching of cells.
In the present disclosure, homeotropic alignment is the state in which rod-like liquid crystalline molecules align substantially perpendicularly to the substrate. In discotic liquid crystals homeotropic alignment is defined as the state in which an axis of the column structure, which is formed by disc-like liquid crystalline molecules, aligns perpendicularly to a surface. In homeotropic alignment, pretilt is the tilt angle of the molecules that are close to the alignment layer and is typically close to 90 degrees and for example may be 88 degrees.
In a twisted liquid crystal layer a twisted configuration (also known as a helical structure or helix) of nematic liquid crystal molecules is provided. The twist may be achieved by means of a non-parallel alignment of alignment layers. Further, cholesteric dopants may be added to the liquid crystal material to break degeneracy of the twist direction (clockwise or anti-clockwise) and to further control the pitch of the twist in the relaxed (typically undriven) state. A supertwisted liquid crystal layer has a twist of greater than 180 degrees. A twisted nematic layer used in spatial light modulators typically has a twist of 90 degrees.
Liquid crystal molecules with positive dielectric anisotropy are switched from a homogeneous alignment (such as an A-plate retarder orientation) to a homeotropic alignment (such as a C-plate or O-plate retarder orientation) by means of an applied electric field.
Liquid crystal molecules with negative dielectric anisotropy are switched from a homeotropic alignment (such as a C-plate or O-plate retarder orientation) to a homogeneous alignment (such as an A-plate retarder orientation) by means of an applied electric field.
Rod-like molecules have a positive birefringence so that ne>no as described in eqn. 2. Discotic molecules have negative birefringence so that ne<no.
Positive retarders such as A-plates, positive O-plates and positive C-plates may typically be provided by stretched films or rod-like liquid crystal molecules. Negative retarders such as negative C-plates may be provided by stretched films or discotic like liquid crystal molecules.
Parallel liquid crystal cell alignment refers to the alignment direction of homogeneous alignment layers being parallel or more typically antiparallel. In the case of pre-tilted homeotropic alignment, the alignment layers may have components that are substantially parallel or antiparallel. Hybrid aligned liquid crystal cells may have one homogeneous alignment layer and one homeotropic alignment layer. Twisted liquid crystal cells may be provided by alignment layers that do not have parallel alignment, for example oriented at 90 degrees to each other.
Transmissive spatial light modulators may further comprise retarders between the input display polariser and the output display polariser for example as disclosed in U.S. Pat. No. 8,237,876, which is herein incorporated by reference in its entirety. Such retarders (not shown) are in a different place to the passive retarders of the present embodiments. Such retarders compensate for contrast degradations for off-axis viewing locations, which is a different effect to the luminance reduction for off-axis viewing positions of the present embodiments.
Terms related to privacy display appearance will now be described.
A private mode of operation of a display is one in which an observer sees a low contrast sensitivity such that an image is not clearly visible. Contrast sensitivity is a measure of the ability to discern between luminances of different levels in a static image. Inverse contrast sensitivity may be used as a measure of visual security, in that a high visual security level (VSL) corresponds to low image visibility.
For a privacy display providing an image to an observer, visual security may be given as:
VSL=(Y+R)/(Y−K) eqn. 4
where VSL is the visual security level, Y is the luminance of the white state of the display at a snooper viewing angle, K is the luminance of the black state of the display at the snooper viewing angle and R is the luminance of reflected light from the display.
Panel contrast ratio is given as:
C=Y/K eqn. 5
For high contrast optical LCD modes, the white state transmission remains substantially constant with viewing angle. In the contrast reducing liquid crystal modes of the present embodiments, white state transmission typically reduces as black state transmission increases such that
Y+K˜P·L eqn. 6
The visual security level may then be further given as:
where off-axis relative luminance, P is typically defined as the percentage of head-on luminance, L at the snooper angle and the display may have image contrast ratio C and the surface reflectivity is ρ.
The off-axis relative luminance, P is sometimes referred to as the privacy level. However, such privacy level P describes relative luminance of a display at a given polar angle compared to head-on luminance, and is not a measure of privacy appearance.
The display may be illuminated by Lambertian ambient illuminance I. Thus in a perfectly dark environment, a high contrast display has VSL of approximately 1.0. As ambient illuminance increases, the perceived image contrast degrades, VSL increases and a private image is perceived.
For typical liquid crystal displays the panel contrast C is above 100:1 for almost all viewing angles, allowing the visual security level to be approximated to:
VSL=1+I·ρ/(π·P·L) eqn. 8
The perceptual image security may be determined from the logarithmic response of the eye, such that the security factor, S is given by:
S=log10(V) eqn. 9
Desirable limits for S were determined in the following manner. In a first step a privacy display device was provided. Measurements of the variation of privacy level, P(θ) of the display device with polar viewing angle and variation of reflectivity ρ(θ) of the display device with polar viewing angle were made using photopic measurement equipment. A light source such as a substantially uniform luminance light box was arranged to provide illumination from an illuminated region that was arranged to illuminate the privacy display device along an incident direction for reflection to a viewer positions at a polar angle of greater than 0° to the normal to the display device. The variation I(θ) of illuminance of a substantially Lambertian emitting lightbox with polar viewing angle was determined by measuring the variation of recorded reflective luminance with polar viewing angle considering the variation of reflectivity ρ(θ). The measurements of P(θ), r(θ) and I(θ) were used to determine the variation of Security Factor S(θ) with polar viewing angle along the zero elevation axis.
In a second step a series of high contrast images were provided on the privacy display including (i) small text images with maximum font height 3 mm, (ii) large text images with maximum font height 30 mm and (iii) moving images.
In a third step each observer (with eyesight correction for viewing at 1000 mm where appropriate) viewed each of the images from a distance of 1000 mm, and adjusted their polar angle of viewing at zero elevation until image invisibility was achieved for one eye from a position near on the display at or close to the centre-line of the display. The polar location of the observer's eye was recorded. From the relationship S(θ), the security factor at said polar location was determined. The measurement was repeated for the different images, for various display luminance Ymax, different lightbox illuminance I(q=0), for different background lighting conditions and for different observers.
From the above measurements S<1.0 provides low or no visual security, 1.0≤S<1.5 provides visual security that is dependent on the contrast, spatial frequency and temporal frequency of image content, 1.5≤S<1.8 provides acceptable image invisibility (that is no image contrast is observable) for most images and most observers and S>1.8 provides full image invisibility, independent of image content for all observers.
In comparison to privacy displays, desirably wide-angle displays are easily observed in standard ambient illuminance conditions. One measure of image visibility is given by the contrast sensitivity such as the Michelson contrast which is given by:
M=(Imax−Imin)/(Imax+Imin) eqn. 10
and so:
M=((Y+R)−(K+R))/((Y+R)+(K+R))=(Y−K)/(Y+K+2·R) eqn. 11
Thus the visual security level (VSL), is equivalent (but not identical to) 1/M. In the present discussion, for a given off-axis relative luminance, P the wide-angle image visibility, W is approximated as
W=1/VSL=1/(1+I·ρ/(π·P·L)) eqn. 12
In the present discussion the colour variation Δε of an output colour (uw′+Δu′, vw′+Δv′) from a desirable white point (uw′, vw′) may be determined by the CIELUV colour difference metric, assuming a typical display spectral illuminant and is given by:
Δε=(Δu′2+Δv′2)1/2 eqn. 13
Catadioptric elements employ both refraction and reflection, which may be total internal reflection or reflection from metallised surfaces.
The structure and operation of various directional display devices will now be described. In this description, common elements have common reference numerals. It is noted that the disclosure relating to any element applies to each device in which the same or corresponding element is provided. Accordingly, for brevity such disclosure is not repeated.
A switchable privacy display apparatus will now be described.
Display apparatus 100 comprises a backlight apparatus 20; and a spatial light modulator 48 arranged to receive light from the backlight apparatus 20.
In the present disclosure, the spatial light modulator 48 may comprise a liquid crystal display comprising substrates 212, 216, and liquid crystal layer 214 having red, green and blue pixels 220, 222, 224. The spatial light modulator 48 has an input display polariser 210 and an output display polariser 218 on opposite sides thereof. The output display polariser 218 is arranged to provide high extinction ratio for light from the pixels 220, 222, 224 of the spatial light modulator 48. Typical polarisers 210, 218 may be absorbing polarisers such as dichroic polarisers.
Optionally a reflective polariser 208 may be provided between the input display polariser 210 and backlight 20 to provide recirculated light and increase display efficiency. Advantageously efficiency may be increased.
The backlight apparatus 20 comprises a rear reflector 3; and an illumination apparatus 110. The illumination apparatus comprises a waveguide arrangement comprising waveguide 1, and optical turning film component 50 and arranged to receive light exiting from the first surface of waveguide 1 and direct it back through the waveguide 1.
The waveguide 1 further comprises a second input end 4 arranged between the first and second light guiding surfaces 6, 8 opposite to the first mentioned input end 2, and the illumination apparatus 110 further comprises at least one second light source 17 arranged to input light into the waveguide 1 through the second input end 4. In further embodiments described hereinbelow the second light source 17 may be omitted. Advantageously cost and bezel width may be reduced.
Optical stack 5 may comprise diffusers, optical turning film components and other known optical backlight structures. Asymmetric diffusers, that may comprise asymmetric surface relief features for example, may be provided in the optical stack 5 with increased diffusion in the elevation direction in comparison to the lateral direction may be provided. Advantageously image uniformity may be increased.
Display apparatus 100 further comprises: at least one display polariser that is the output polariser 218 arranged on a side of the spatial light modulator 48 that in
The display polariser 218 and the additional polariser 318 have electric vector transmission directions 219, 319 that are parallel, and orthogonal to the input polariser 210 transmission direction 211. Reflective polariser 302 further has a polarisation transmission direction 303 that is aligned parallel to the polarisation transmission directions 219, 319.
In
Polar control retarder 300 is arranged between the display polariser 218 and the additional polariser 318, the at least one polar control retarder 300 including a switchable liquid crystal retarder 301 comprising a layer 214 of liquid crystal material. Polar control retarders 300 comprise: (i) a switchable liquid crystal retarder 301 comprising a layer 314 of liquid crystal material arranged between transparent support substrates 312, 316 and arranged between the display polariser 218 and the additional polariser 318; and (ii) at least one passive compensation retarder 330.
The display further comprises a control system arranged to independently control the at least one first light source 15 arrayed across an input end of the waveguide 1 and the at least one second light source 17 arrayed across an input end of the waveguide 1. The light sources 15, 17 are arranged to provide input light to a waveguide 1.
Control of the polar control retarders is achieved by means of driver 350 to change the operating voltage across the liquid crystal layer 314. Controller 352 is provided to control the driver 350 and controller 354 that further controls the driving of light sources 15, 17.
The display device 100 is arranged to display an image and capable of operating in at least a public mode and a privacy mode, wherein in the privacy mode the privacy function is provided and the visibility of the image to an off-axis viewer is reduced compared to the public mode and the visibility of the image to the primary user in an on-axis position remains visible in both the privacy and public modes. The control system 350, 352, 354 selectively operates the display device 100 in the public mode or the privacy mode for at least one region of the displayed image, typically the entire displayed image. Such display device may be used in applications such as but not limited to switchable privacy displays such as laptops, monitors, TV, cell phone, tablets, wearable displays, ATM displays and automotive displays.
It may be desirable to provide a high efficiency display with high uniformity of luminance.
It would be desirable that light cones 415C, 415L, 415R, 415U, 415D are each directed to a common direction.
The structure of an exemplary waveguide will now be described.
Waveguide 1 is an optical waveguide that extends across a plane (x-y plane in
The first and second light guiding surfaces 6, 8 are arranged to guide light by total internal reflection. In the embodiment of
Waveguide 1 comprises an input end 2 arranged between the first and second light guiding surfaces 6, 8 and extending in a lateral direction (along the x-axis) between the first and second light guiding surfaces 6,8.
The at least one light source 15 comprises an array of light sources 15 that are arrayed across the lateral direction (that is parallel to the x-axis in the present embodiment). At least one light source 15 is arranged to input light into the waveguide through the input end 2. Light source may comprise an array of light sources, such as an LED array.
The operation of an illumination apparatus 110 will now be described.
Illumination apparatus 110 comprises: a waveguide 1 extending across a plane (x-y plane) and comprising: first and second opposed light guiding surfaces 6, 8 arranged to guide light along the optical waveguide 1.
The second light guiding surface 8 is arranged to guide light by total internal reflection.
An input end 2 is arranged between the first and second light guiding surfaces 6, 8 and extending in a lateral direction between the first and second light guiding surfaces 6, 8.
At least one light source 15 arranged to input light into the waveguide 1 through the input end 2, wherein the waveguide 1 is arranged to cause light from the light sources 15 to exit from the waveguide 1 through the second light guiding surface 8 by breaking total internal reflection.
The optical turning film component 50 comprises: an input surface 56 arranged to receive the light exiting from the waveguide 1, the input surface 56 extending across the plane (x-y plane); and an output surface 58 facing the input surface 56. The input surface 56 comprises: an array of prismatic elements 52, each comprising a pair of facets 53 defining a ridge 54 therebetween. The output surface 58 is planar. For each pair of facets 53A, 53B, the first facet 53A has a normal nA on the internal side of the input surface 56 that is inclined towards a first side 52 of the optical turning film 50 and a second facet 53B has a normal nB on the internal side of the input surface 56 that is inclined towards a second side 53 of the optical turning film 50 opposite to from the first end 52, the first facets 53A having respective facet angles α, defined between the normal to the facet 53A and a normal (z-direction) to the plane (x-y plane), that vary across the array so that the deflection varies in a direction that is orthogonal (y-direction) to an optical axis 199 normal to the plane (z-direction) and corresponds to a direction orthogonal (y-direction) to the lateral direction (x-direction).
Incident rays 415 on the surface 8 of waveguide 1 have angles of incidence at the surface 8 that are less than the critical angle at the said surface 8. Light cone 415 is determined at least in part by the collimation of the light rays 415 from light sources 15 that breaks internal reflection at the surface 8.
Grazing output light rays 415G are output from the waveguide 1 with a cone angle 415 and substantially uniform output angle across the plane (x-y plane) of the waveguide 1.
The prismatic elements 51 of the optical turning film component 50 are arranged to deflect the light 415G exiting the waveguide 1, the deflection varying in at least one direction across the plane (x-y plane).
Near the upper edge of the display, light rays 415G are refracted by facets 53BU with facet angle βU and reflected by total internal reflection at facets 53AU with surface normal direction nAU with facet angle αU such that output light ray 415U is directed towards a window 26A at a window distance ZwA from the illumination apparatus 110. In at least one cross sectional plane (y-z plane in
In the present disclosure optical window 26A refers to the directing of light by illumination apparatus 110 from light sources such as sources 15 to defined spatial regions in a window plane 197, that is at the window distance ZwA from the illumination apparatus. The optical window 26 may also be referred to as an optical pupil. An observation from a location within the optical window provides light rays with common or substantially common optical properties from across the illumination apparatus 110.
The use of the term optical window 26 in the present embodiments is distinct and different from the use of the term window when used to refer to sheets or panes of glass or other transparent material such as plastics for use in house windows, car windows and windscreens, and other types of protective windows. Such sheets or panes do not contribute to the creation of desirable viewing regions with improved uniformity as described herein.
Similarly near the centre of the display, light rays 415G are refracted by facets 53BC with facet angle βC and reflected by total internal reflection at facets 53AC with surface normal direction nAC with facet angle αC such that output light ray 415C is directed towards a window 26A in the window plane 197A at a window distance ZwA from the illumination apparatus 110.
Similarly near the lower edge of the display, light rays 415G are refracted by facets 53BD with facet angle βD and reflected by total internal reflection at facets 53AD with surface normal direction nAC with facet angle αD such that output light ray 415D is directed towards a window 26A in the window plane 197A at a window distance ZwA from the illumination apparatus 110.
Facet angles α, β may vary continuously with location across the length of the optical turning film component. The deflected light rays 415U, 415C, 415D are directed towards a common optical window 26A in front of the illumination apparatus 110.
The operation of the optical turning film component with ridges 54 that are arranged as straight lines will now be further described.
Facet angles α, β of respective facets 53, defined between a normal to the facet 53 and a normal (z-direction) to the plane (x-y plane), vary across the array so that the deflection varies in a direction (y-direction) that is orthogonal to an optical axis 199 that is normal to the plane (x-y plane), the direction corresponding to a direction (y-direction) that is orthogonal to the lateral direction (x-direction).
The lines are straight and facet 53 angles of respective facets 53, defined between a normal to the facet 53 and a normal to the plane (x-y plane), vary across the array so that the deflection varies in a direction that is orthogonal to the optical axis 199 corresponding to a direction that is orthogonal to the lateral direction.
The lines of the array have an arithmetic mean tangential angle projected on to the plane (x-y plane) of 0° from the lateral direction, that is the lines are parallel to the x-axis direction that is the lateral direction in the present embodiment.
Thus the rays 415G are directed by the optical turning film component 50 towards the common window 26A. Light rays 415UL, 415CL, 415DL from the upper, central and lower parts of the left edge region of the optical turning film are located to the window 26A at a location corresponding to the lateral location of the left edge region in the lateral direction. Light rays 415UC, 415CC, 415DC from the upper, central and lower parts of the central region of the optical turning film are located to the window 26A at a location in the lateral corresponding to the lateral location of the central region in the lateral direction. Light rays 415UR, 415CR, 415DR from the upper, central and lower parts of the right edge region of the optical turning film are located to the window 26A at a location in the lateral corresponding to the lateral location of the right edge region in the lateral direction.
In the embodiment of
The embodiment of
It may be desirable to provide an optical window with reduced extent in the direction that is orthogonal to the lateral direction.
The curved facets have surface normal directions nAK, nAC, nAL that vary across the width of the optical turning film 50, that is the surface normal directions vary in the lateral direction along a ridge such that light rays 415G from the waveguide 1 are directed towards a common window 26B in a window plane 197B at a distance ZWB from the optical turning film component 50 of the illumination apparatus 110.
The optical window 26B has a cone width defined by cone 415 in direction orthogonal to the lateral direction and an extent determined by the cone width 415 and the height of the optical turning film component 50, and is thus orthogonal to the optical window 26A illustrated in
In the embodiment of
The orientation of the lines of the array is described by facet peak 54 rotations γ where γR is rotation at the right side of the display γC is the rotation in the centre and ye is the rotation at the left edge. The arithmetic mean tangential angle projected on to the plane (x-y plane) is the average rotation γ across the lateral direction.
The lines of the array may alternatively have an arithmetic mean tangential angle that is inclined at more than 0° from the lateral direction. Such an arrangement achieves an offset ZOB that is non-zero. Advantageously the nominal window 26B location may be set for off-axis illumination with desirable properties as will be described further hereinbelow.
It may be desirable to provide a common optical window for all points across the illumination apparatus 110.
The facet surfaces 53 are provided to achieve operation for rays 415G as illustrated in both
The first mentioned common optical window 26A and the further common optical window 26B are defined the same distance in front of the illumination apparatus 110, achieving common optical window 26AB. Advantageously increased uniformity of output is achieved across the whole of the illumination apparatus 110 from observation locations within the optical window 26AB.
The first mentioned common optical window 26A and the further common optical window 26B are defined at different distances ZWA, ZWB in front of the illumination apparatus 110. Further as described above, the offset ZOA may be provided by facet 53 angle selection and offset ZOB may be achieved by selection of the arithmetic mean tangential angle projected on to the plane (x-y plane) of the inclination of the lines formed by the ridges 54 of the array. Advantageously increased uniformity may be achieved for two different nominal observation distances and angular locations.
The operation of the illumination apparatus 110 in a backlight 20 of a display apparatus 100 will now be described. For the purposes of the present description the backlights 20 are further referred to as pupillated backlights, that is backlights that provide optical windows 26.
Light source array 15 is arranged at the lower edge of the backlight and rays 415L, 415R are directed towards optical window 26A that has an extent in the lateral direction as described above. In typical operation, the window distance between the backlight 20 and the window plane 197 is arranged to be greater than the typical observer location.
In an illustrative example, a laptop display of diagonal size 14 inches is arranged with a window distance ZWA of 700 mm, while the nominal observer location is in plane 145 at a distance ZV of 500 mm. The window distance ZWA may be arranged by design of waveguide 1 and facets 53 to be at a nominal snooper distance which may for example be 700 mm.
The window 26B may be at substantially the same distance as the window 26A illustrated in
As will be described further in an illustrative example below, the arrangement of
Desirably the nominal user 45 plane 145 is closer to the backlight 20 than the window plane 197. In operation the user 45 sees an image that has increased uniformity in comparison to unpupillated backlights (i.e. backlights which do not provide a common optical window 26, or in other words provide a common optical window at optical infinity). When the observer moves to the right side of the display, the display maintains increased brightness on the right side of the display in comparison to the left side. By way of comparison, if the nominal observer distance ZV is arranged to be greater than the window distance ZWA, ZWB then as the observer moves to the right from the central optical axis 199, the right side of the display becomes darker than the left side of the image. Such a variation with observer position is typically considered unnatural and undesirable.
Further, the snooper 47 is desirably arranged at or further than the window distance ZWA, ZWB. Such an arrangement provides increased uniformity of security factor across the display area in comparison to unpupillated backlights.
In alternative embodiments the windows 26A, 26B may be at different distances from the backlight 20, such as illustrated in
Features of the embodiment of
An illustrative embodiment will now be described.
Polar region 65 represents the field of view of the border of a 14″ laptop display viewed by a head-on observer at 500 mm and polar region 67 represents the field of view of the border of the display viewed by an off-axis snooper at 45 degrees and a distance along the normal 199 of 600 mm.
In prior art unpupillated displays, the luminance contours vary across the field of view. Thus a prior art display with such an unpupillated backlight has a central luminance of 100% and less than 50% luminance in the upper right and upper left corners. It would be desirable to increase the luminance uniformity for such a backlight profile.
In an illustrative embodiment of the arrangements of
In the present embodiments, facet angles of respective facets 53, defined between a normal to the facet 53 and a normal (z-direction) to the plane (x-y plane) may be between 40° and 70° preferably between 42.5° and 65°, and more preferably between 42.5° and 62.5° as will be further described with reference to
Further a polar control retarder 300 is provided as illustrated in
Image uniformity can be assessed by comparing variation of luminance across the display for the viewing positions in polar space 29A˜M as indicated.
Comparing
The operation of the display in privacy mode to an observer 45 and snooper 47 will now be described.
The variation of uniformity of security factor S with viewing location will now be described.
By way of comparison
In the graphs of
Comparing
It would be desirable to provide a public mode of operation with higher luminance at off-axis positions.
In comparison to the embodiments of
The deflected light through each input end 2, 4 is directed towards the same common optical window 26 in front of the illumination apparatus 110. As the deflection of the light rays 415, 417 is dominated by the reflection rather than the refraction, the present embodiments achieve pupillation of light rays and provide optical windows 27A. Thus light rays 417U, 415U may be directed in similar directions by means of facet angle selection γA, γB as described elsewhere herein.
Such an arrangement can be used in a switchable privacy display further comprising polar control retarders 300 and polariser 318 of
Alternatively such an arrangement can be used in a switchable high efficiency display of
The pupillation of
The operation of the display backlight 20 for light rays 417G from the second end onto curved facets will now be described.
The lines of the ridges are curved so that the deflected light input through the first end is directed towards a common optical window 27A in front of the illumination apparatus 110 and the deflected light input through the second end 4 is directed towards a virtual common optical window 27B behind the illumination apparatus 110, in the plane 197B.
Exemplary light rays 417CD, 417CC, 417CU illustrate that the backlight 20 illuminates towards the user 45 and snooper 47, appearing to originate from the virtual optical window 27B. The luminance profile of
Alternative arrangements of operation of a display comprising different optical windows will now be described further.
In comparison to the arrangement of
Features of the embodiments of
Alternative arrangements of waveguide 1 will now be described.
In comparison to the waveguide 1 of
Advantageously the cost and complexity of the waveguides 1 may be reduced.
It may be desirable to provide first and second optical windows 26, 27 that have the same or similar size.
In an alternative embodiment, the waveguide 1 is arranged to cause light from the at least one first light source 15 and the at least one second light source 17 to exit from the waveguide 1 with a common angular distribution, such that angular distributions 425, 427 are the same.
The waveguides 1 of
The optical windows 26A, 26B may be arranged in the same location that may be an on-axis location (centred around optical axis 199) or an off-axis location. The control system is arranged to provide illumination from both the at least one first light source 15 and the at least one second light source 17 so as to increase spatial uniformity of illumination across the illumination device for at least one viewing location. In such an arrangement, the outputs from both waveguides 1 are combined by the optical turning film component 50. Waveguides 1 may have non-uniformities of extraction in the direction orthogonal to the lateral direction, that is dependent on distance from the light source 15, so that such a combination may achieve improved extraction efficiency. Advantageously uniformity of luminance may be increased.
Such an output may be suitable for application to a vehicle as illustrated in
Light input from the first light source 15 correspondingly produces a similar high luminance profile in the region of the field of view 67 for the passenger 47.
Such a backlight 20 may provide a display 100 that is visible to a driver at night-time, advantageously with low stray light to the remainder of the cabin. Further such a backlight 20 when illuminated by light source 15 only may provide high luminance to the passenger 47 and not to the driver. Such a backlight 20 may advantageously provide some degree of image privacy to the driver 45. In another mode of operation both light sources 15, 17 may be illuminated so that fields of view 65, 67 may both be illuminated. Advantageously a high efficiency display 100 may be provided.
It may be desirable to increase the uniformity of input light on to the optical turning film 50.
In comparison to
The optical turning film component 50 comprises: an input surface 56 arranged to receive the light exiting from the waveguide 1, the input surface 56 extending across the plane (x-y plane); and an output surface 58 facing the input surface 56. The input surface 56 comprises: an array of prismatic elements 52 each comprising a pair of facets 53 defining a ridge 54 therebetween. The output surface 58 is planar. For each pair of facets 53A, 53B, the first facet 53A has a normal nA on the internal side of the input surface 56 that is inclined towards a first side 52 of the optical turning film 50 and a second facet 53B has a normal nB on the internal side of the input surface 56 that is inclined towards a second side 53 of the optical turning film 50 opposite to from the first end 52, the first facets 53A having respective facet angles α, defined between the normal to the facet 53A and a normal (z-direction) to the plane (x-y plane), that vary across the array so that the deflection varies in a direction that is orthogonal (y-direction) to an optical axis 199 normal to the plane (z-direction) and corresponds to a direction orthogonal (y-direction) to the lateral direction (x-direction).
In comparison to the embodiment of
Considering a viewing arrangement similar to that illustrated in
For a position x from one edge of the turning film component 50 of width L, the relative position across the turning film component 50 is given by x/L.
In a first illustrative embodiment of
Light rays 415B are directed towards a common window 26A that is inclined to optical axis 199 by refraction at facets 53A and total internal reflection at the facets 53B. The window distance ZwA may be shorter than the window distance ZWB. For example the distance ZWA may be near the passenger 45 nominal viewing distance while the distance ZWB may be at infinity. Advantageously the complexity of the tooling for forming the prismatic array is reduced. Typically the distance ZWA is arranged to be greater than the nominal passenger distance to advantageously achieve desirable luminance uniformity variations with lateral passenger 45 location.
Considering facets 53A, 53B at least some of the facets 53A have respective facet angles α1, α2, defined between a normal to the facet and a normal (z-direction) to the plane (x-y plane), of between 52.5° and 62.5°. In respect of at least some of the facets 53B have respective facet angles β2, defined between a normal to the facet and a normal (z-direction) to the plane (x-y plane), of between 42.5° and 52.5°. In another embodiment at least some of the facets β1 have respective facet angle, defined between a normal to the facet and a normal (z-direction) to the plane (x-y plane), of between 40° and 52.5°.
In each pair of facets 53A, 53B, a first facet 53A has a normal on the internal side of the input surface that is inclined towards the input end 2 of the first waveguide 1A and a second facet 53B has a normal on the internal side of the input surface that is inclined away from the input end 2A of the first waveguide 1A, the first facets 53A having respective facet angles α, defined between the normal to the facet and a normal (z-direction) to the plane (x-y plane), that vary across the array 50 so that the deflection varies in a direction that is orthogonal to an optical axis 199 normal (z-direction) to the plane (x-y plane) and corresponds to a direction orthogonal to the lateral direction.
Referring to
In an alternative arrangement, the first facets 53A have respective facet angles α2, defined between a normal to the facet and a normal (z-direction) to the plane (x-y plane), of between 52.5° and 62.5° and the second facets 53B have respective facet angles β2, defined between the normal to the facet and a normal (z-direction) to the plane (x-y plane), that vary across the array. The second facets 53B have respective facet angles, defined between a normal to the facet and a normal (z-direction) to the plane (x-y plane), of between 40° and 52.5°. Advantageously pupillation may be provided to a second display user, achieving increased uniformity.
In an alternative embodiment, both the facet angles α2, β2 vary with relative position x/L. Light rays 415A are directed towards a common window 26A that is inclined around a 45° angle to optical axis 199 by refraction at the facets 53B and total internal reflection at facets 53A. Light rays 415B are directed by refraction at the facets 53A and total internal reflection at the facets 53B towards a common optical window 26B that is near to optical axis 199.
The deflected light from each input end 2A, 2B is directed towards respective common optical windows 26A, 26B in front of the illumination apparatus. The respective common optical windows 26A, 26B are in different locations in front of the illumination apparatus.
In alternative arrangements wherein the common optical windows 26A, 26B are in the same location, increased brightness and uniformity may be achieved and for example switching between a narrow angle and wide angle mode of operation may advantageously be achieved.
In arrangements wherein the common optical windows are in different locations, different viewing locations may be provided, advantageously with increased brightness and uniformity.
Advantageously as both light rays 415A, 415B are directed to a common optical windows 26A, 26B by total internal reflection at facets 53A, 53B respectively, pupillation may be achieved with similar window distances ZWA, ZWB compared to the embodiment of
A backlight 20 suitable for use in a switchable privacy display 100 of the type illustrated in
In an alternative embodiment of
Referring to
A backlight 20 suitable for use in a central automotive display 100 of the type illustrated in
Embodiments of waveguide facets will now be described.
In an illustrative embodiment the angle 39A may be 55 degrees. More generally, the angle 39A may be at least 40 degrees and at most 70 degrees, preferably may be at least 45 degrees and at most 65 degrees and more preferably may be at least 50 degrees and at most 60 degrees.
In operation, most light rays 415Ba from the waveguide 1B are refracted and pass through the waveguide 1A with a small deviation. However some light rays 415Bb that are output from the waveguide 1B refract through the gently sloping facet 32A and are incident on the internal face of the steeply sloping facet 36A at which the light rays 415Bb undergo total internal reflection. The steeply sloping facet 36A has a surface normal direction 37A such that the totally internally reflected light rays 415Bb are in the same or a similar direction to the light rays 415Ba. Advantageously stray light is reduced and brightness is increased.
By way of comparison with the alternative of
In operation light rays 415Bb are reflected by total internal reflection at the facet 36A and may be redirected within the waveguide 1A as illustrated. Such light rays 415Bb may provide increased stray light in undesirable polar directions that are different to the polar directions for light rays 415Ba. Luminance may be increased in undesirable polar directions, and security level of the display may be degraded.
Further light sources 17 may be provided.
Light rays 415A with cones 425A are directed to a first optical window 26A, such as near to a passenger 47 while light rays 415B with cones 425B are directed to a second optical window 26B, such as near to a driver 45. Further light rays 417A with cones 427A are directed to the second optical window 26B, while light rays 417B with cones 427B are directed to the first optical window 26A.
In comparison to the arrangement of
The respective common optical windows 26A, 26B may be in the same location in front of the illumination apparatus. Advantageously brightness and uniformity may be increased.
It may be desirable to provide an optical window 26 with multiple luminance maxima.
The lines of ridges 54A are curved in the plane of the optical turning film component 50 while the lines of the ridges 54B are linear in the plane. As illustrated in
The pupillation of the linear ridges 54B may provide an extended window 26B such that uniformity is increased for the observer 47 with field of view 67.
In alternative embodiments both ridges 54A, 54B may have lines that are linear in the plane. Advantageously visibility of Moiré may be reduced.
In alternative embodiments either or both ridges 54A, 54B may have ridges that are curved. Advantageously uniformity may be increased for both users 45, 47.
In the embodiment and alternative embodiments of
In the alternative embodiment of
In comparison to the light turning film component 50 of
In comparison to the arrangement of
It may be desirable to provide different outputs for different regions of a display.
First light source 15 comprises first and second parts 15A, 15B and second light source 17 comprises first and second parts 17A, 17B. Waveguide 1 may be of the type illustrated elsewhere herein, or may be first and second waveguides 1A, 1B for example as illustrated in
Light rays 415A propagating within the waveguide 1 are input with an expanding cone in the lateral direction. The microstructures on the surfaces 6, 8 of the waveguide 1 adjust the ray 415A propagation directions to achieve some collimation in the lateral direction and thus illumination regions 475A are provided with limited extent in the lateral direction. Such collimation can achieve partial illumination of the backlight in regions 475A that are determined by the location of the light source along the first input end 2.
Similarly light rays 417B propagating within the waveguide 1 are input with an expanding cone in the lateral direction. Some collimation is provided in the lateral direction and thus illumination regions 477B are provided with limited extent in the lateral direction. Such collimation can achieve partial illumination of the backlight in regions 477B that are determined by the location of the light source along the input end 4.
By control of light sources 15A, 15B and 17A, 17B, the directionality of output may be different for different regions of the backlight 20. In an illustrative example, in one mode of operations, the left side of the display 100 may be arranged for high image visibility to both users 45, 47 and the right side of the display 100 may be provided for high image security factor to a snooper 47 with high image visibility to the user 45. In other illustrative modes of operation, the whole display 100 may be arranged to be seen by both users 45, 47 or the whole display 100 may be arranged to be private to the user 45.
The number of light sources 15A-N may be adjusted to increase the number of addressable regions of display control.
It may be desirable to provide a curved display.
In comparison to the embodiments described elsewhere herein, the backlight 20C is curved. For comparison purposes the backlight 20F that is the backlight 20C before curving is illustrated. The backlight 20F is provided with a waveguide 1, and optical turning film component 50 that is pupillated in at least one axis (by means of variable tilt facets 53, by means of curved ridges 54 or both) to provide an optical window 26F in a window plane 197F as described elsewhere herein. After curving, backlight 20C provides a modified optical window 26C in a modified window plane 197C that is closer to the backlight than the optical window 26F.
Advantageously the curvature of the display can be provided for comfortable viewing by the user 45, and the optical window 26C can be provided for desirable image uniformity and variation of uniformity with user 45 location. Further in a privacy display, increased uniformity of security factor can be provided to off-axis snooper 47.
Operation of the switchable retarders of
When the layer 314 of liquid crystal material 414 is driven to operate in the privacy mode, the retarders 300 provide no overall transformation of polarisation component 360 to output light rays 400 passing therethrough along an axis perpendicular to the plane of the switchable retarder, but provides an overall transformation of polarisation component 361 to light rays 415 passing therethrough for some polar angles which are at an acute angle to the perpendicular to the plane of the retarders.
Polarisation component 360 from the output polariser 218 is transmitted by reflective polariser 302 and incident on retarders 300. On-axis light has a polarisation component 362 that is unmodified from component 360 while off-axis light has a polarisation component 364 that is transformed by the retarders 300. At a minimum, the polarisation component 361 is transformed to a linear polarisation component 364 and absorbed by additional polariser 318. More generally, the polarisation component 361 is transformed to an elliptical polarisation component, that is partially absorbed by additional polariser 318.
The polar distribution of light transmission illustrated in
Features of the embodiment of
Advantageously, a privacy display is provided that has low luminance to an off-axis snooper while maintaining high luminance for an on-axis observer.
The operation of the reflective polariser 302 for light from ambient light source 604 will now be described for the display operating in privacy mode.
Ambient light source 604 illuminates the display device 100 with unpolarised light. Additional polariser 318 transmits light ray 410 normal to the display device 100 with a first polarisation component 372 that is a linear polarisation component parallel to the electric vector transmission direction 319 of the additional polariser 318.
In both states of operation, the polarisation component 372 remains unmodified by the retarders 300 and so transmitted polarisation component 382 is parallel to the transmission axis of the reflective polariser 302 and the output polariser 218, so ambient light is directed through the spatial light modulator 48 and lost.
By comparison, for ray 412, off-axis light is directed through the retarders 300 such that polarisation component 374 incident on the reflective polariser 302 may be reflected. Such polarisation component is re-converted into component 376 after passing through retarders 300 and is transmitted through the additional polariser 318.
Thus when the layer 314 of liquid crystal material is in the second state of said two states, the reflective polariser 302 provides no reflected light for ambient light rays 410 passing through the additional polariser 318 and then the retarders 300 along an axis perpendicular to the plane of the retarders 300, but provides reflected light rays 412 for ambient light passing through the additional polariser 318 and then the retarders 300 at some polar angles which are at an acute angle to the perpendicular to the plane of the retarders 300; wherein the reflected light 412 passes back through the retarders 300 and is then transmitted by the additional polariser 318.
The retarders 300 thus provide no overall transformation of polarisation component 380 to ambient light rays 410 passing through the additional polariser 318 and then the retarder 300 along an axis perpendicular to the plane of the switchable retarder, but provides an overall transformation of polarisation component 372 to ambient light rays 412 passing through the absorptive polariser 318 and then the retarders 300 at some polar angles which are at an acute angle to the perpendicular to the plane of the retarders 300.
The polar distribution of light reflection illustrated in
In the public mode of operation, the control system 710, 752, 350 is arranged to switch the switchable liquid crystal retarder 301 into a second retarder state in which a phase shift is introduced to polarisation components of light passing therethrough along an axis inclined to a normal (z-direction) to the plane (x-y plane) of the switchable liquid crystal retarder 301.
By way of comparison, solid angular extent 415D may be substantially the same as solid angular extent 415B in a public mode of operation. Such control of output solid angular extents 415C, 415D may be achieved by synchronous control of the sets 15, 17 of light sources and the at least one switchable liquid crystal retarder 300.
Advantageously a privacy mode may be achieved with low image visibility for off-axis viewing and a large solid angular extent may be provided with high efficiency for a public mode of operation, for sharing display imagery between multiple users and increasing image spatial uniformity.
Additional polariser 318 is arranged on the same output side of the spatial light modulator 48 as the display output polariser 218 which may be an absorbing dichroic polariser. The display polariser 218 and the additional polariser 318 have electric vector transmission directions 219, 319 that are parallel. As will be described below, such parallel alignment provides high transmission for central viewing locations.
A transmissive spatial light modulator 48 arranged to receive the output light from the backlight; an input polariser 210 arranged on the input side of the spatial light modulator between the backlight 20 and the spatial light modulator 48, an output polariser 218 arranged on the output side of the spatial light modulator 48; an additional polariser 318 arranged on the output side of the output polariser 218; and a switchable liquid crystal retarder 300 comprising a layer 314 of liquid crystal material arranged between the at least one additional polariser 318 and the output polariser 218 in this case in which the additional polariser 318 is arranged on the output side of the output polariser 218; and a control system 710 arranged to synchronously control the light sources 15, 17 and the at least one switchable liquid crystal retarder 300.
Control system 710 further comprises control of voltage controller 752 that is arranged to provide control of voltage driver 350, in order to achieve control of switchable liquid crystal retarder 301.
Features of the embodiment of
Advantageously, a privacy display is provided that has high reflectivity to an off-axis snooper while maintaining low reflectivity for an on-axis observer. As described above, such increased reflectivity provides enhanced privacy performance for the display in an ambiently illuminated environment.
Operation in the public mode will now be described.
Features of the embodiment of
When the liquid crystal retarder 301 is in a first state of said two states, the polar control retarder 300 provides no overall transformation of polarisation component 360, 361 to output light passing therethrough perpendicular to the plane of the switchable retarder 301 or at an acute angle to the perpendicular to the plane of the switchable retarder 301. That is polarisation component 362 is substantially the same as polarisation component 360 and polarisation component 364 is substantially the same as polarisation component 361. Thus the angular transmission profile of
Thus when the liquid crystal retarder 301 is in the first state of said two states, the retarders 300 provide no overall transformation of polarisation component 372 to ambient light rays 412 passing through the additional polariser 318 and then the retarders 300, that is perpendicular to the plane of the retarders 300 or at an acute angle to the perpendicular to the plane of the retarders 300.
In operation in the public mode, input light ray 412 has polarisation state 372 after transmission through the additional polariser 318. For both head-on and off-axis directions no polarisation transformation occurs and thus the reflectivity for light rays 415 from the reflective polariser 302 is low. Light ray 412 is transmitted by reflective polariser 302 and lost in the display polarisers 218, 210 or the backlight of
Features of the embodiment of
Advantageously in a public mode of operation, high luminance and low reflectivity is provided across a wide field of view. Such a display can be conveniently viewed with high contrast by multiple observers.
Other types of switchable privacy display will now be described.
A display device 100 that may be switched between privacy and public modes of operation comprises an imaging waveguide and an array of light sources as described in U.S. Pat. No. 9,519,153, which is incorporated by reference herein in its entirety. The imaging waveguide images an array of light sources to optical windows that may be controlled to provide high luminance on-axis and low luminance off-axis in a privacy mode, and high luminance with a large solid angle cone for public operation.
As may be used herein, the terms “substantially” and “approximately” provide an industry-accepted tolerance for its corresponding term and/or relativity between items. Such an industry-accepted tolerance ranges from zero percent to ten percent and corresponds to, but is not limited to, component values, angles, et cetera. Such relativity between items ranges between approximately zero percent to ten percent.
While various embodiments in accordance with the principles disclosed herein have been described above, it should be understood that they have been presented by way of example only, and not limitation. Thus, the breadth and scope of this disclosure should not be limited by any of the above-described exemplary embodiments, but should be defined only in accordance with any claims and their equivalents issuing from this disclosure. Furthermore, the above advantages and features are provided in described embodiments, but shall not limit the application of such issued claims to processes and structures accomplishing any or all of the above advantages.
Additionally, the section headings herein are provided for consistency with the suggestions under 37 CFR 1.77 or otherwise to provide organizational cues. These headings shall not limit or characterize the embodiment(s) set out in any claims that may issue from this disclosure. Specifically and by way of example, although the headings refer to a “Technical Field,” the claims should not be limited by the language chosen under this heading to describe the so-called field. Further, a description of a technology in the “Background” is not to be construed as an admission that certain technology is prior art to any embodiment(s) in this disclosure. Neither is the “Summary” to be considered as a characterization of the embodiment(s) set forth in issued claims. Furthermore, any reference in this disclosure to “invention” in the singular should not be used to argue that there is only a single point of novelty in this disclosure. Multiple embodiments may be set forth according to the limitations of the multiple claims issuing from this disclosure, and such claims accordingly define the embodiment(s), and their equivalents, that are protected thereby. In all instances, the scope of such claims shall be considered on their own merits in light of this disclosure, but should not be constrained by the headings set forth herein.
| Number | Name | Date | Kind |
|---|---|---|---|
| 3914022 | Kashnow | Oct 1975 | A |
| 4059916 | Tachihara et al. | Nov 1977 | A |
| 4586790 | Umeda et al. | May 1986 | A |
| 4621898 | Cohen | Nov 1986 | A |
| 4974941 | Gibbons et al. | Dec 1990 | A |
| 5005108 | Pristash et al. | Apr 1991 | A |
| 5035491 | Kawagishi et al. | Jul 1991 | A |
| 5126882 | Oe et al. | Jun 1992 | A |
| 5608550 | Epstein et al. | Mar 1997 | A |
| 5658490 | Sharp et al. | Aug 1997 | A |
| 5671994 | Tai et al. | Sep 1997 | A |
| 5715028 | Abileah et al. | Feb 1998 | A |
| 5779337 | Saito et al. | Jul 1998 | A |
| 5791757 | O'Neil et al. | Aug 1998 | A |
| 5808784 | Ando et al. | Sep 1998 | A |
| 5835166 | Hall et al. | Nov 1998 | A |
| 5854872 | Tai | Dec 1998 | A |
| 5894361 | Yamazaki et al. | Apr 1999 | A |
| 5914760 | Daiku | Jun 1999 | A |
| 5997148 | Ohkawa | Dec 1999 | A |
| 6055103 | Woodgate et al. | Apr 2000 | A |
| 6099758 | Verrall et al. | Aug 2000 | A |
| 6144433 | Tillin et al. | Nov 2000 | A |
| 6169589 | Kaneko | Jan 2001 | B1 |
| 6204904 | Tillin et al. | Mar 2001 | B1 |
| 6222672 | Towler et al. | Apr 2001 | B1 |
| 6280043 | Ohkawa | Aug 2001 | B1 |
| 6364497 | Park et al. | Apr 2002 | B1 |
| 6379016 | Boyd et al. | Apr 2002 | B1 |
| 6392727 | Larson et al. | May 2002 | B1 |
| 6437915 | Moseley et al. | Aug 2002 | B2 |
| 6731355 | Miyashita | May 2004 | B2 |
| 6752505 | Parker et al. | Jun 2004 | B2 |
| 7067985 | Adachi | Jun 2006 | B2 |
| 7072096 | Holman et al. | Jul 2006 | B2 |
| 7163319 | Kuo et al. | Jan 2007 | B2 |
| 7227602 | Jeon et al. | Jun 2007 | B2 |
| 7366392 | Honma et al. | Apr 2008 | B2 |
| 7524542 | Kim et al. | Apr 2009 | B2 |
| 7528893 | Schultz et al. | May 2009 | B2 |
| 7528913 | Kobayashi | May 2009 | B2 |
| 7633586 | Winlow et al. | Dec 2009 | B2 |
| 7660047 | Travis et al. | Feb 2010 | B1 |
| 7766534 | Iwasaki | Aug 2010 | B2 |
| 7834834 | Takatani et al. | Nov 2010 | B2 |
| 7970246 | Travis et al. | Jun 2011 | B2 |
| 7991257 | Coleman | Aug 2011 | B1 |
| 8070346 | Maeda et al. | Dec 2011 | B2 |
| 8098350 | Sakai et al. | Jan 2012 | B2 |
| 8154686 | Mather et al. | Apr 2012 | B2 |
| 8228476 | Shibazaki | Jul 2012 | B2 |
| 8237876 | Tan et al. | Aug 2012 | B2 |
| 8249408 | Coleman | Aug 2012 | B2 |
| 8262271 | Tillin et al. | Sep 2012 | B2 |
| 8469575 | Weber et al. | Jun 2013 | B2 |
| 8646931 | Choi et al. | Feb 2014 | B2 |
| 8801260 | Urano et al. | Aug 2014 | B2 |
| 8848132 | O'Neill et al. | Sep 2014 | B2 |
| 8939595 | Choi et al. | Jan 2015 | B2 |
| 8973149 | Buck | Mar 2015 | B2 |
| 9195087 | Terashima | Nov 2015 | B2 |
| 9274260 | Urano et al. | Mar 2016 | B2 |
| 9304241 | Wang et al. | Apr 2016 | B2 |
| 9324234 | Ricci et al. | Apr 2016 | B2 |
| 9448355 | Urano et al. | Sep 2016 | B2 |
| 9501036 | Kang et al. | Nov 2016 | B2 |
| 9519153 | Robinson et al. | Dec 2016 | B2 |
| 9541698 | Wheatley et al. | Jan 2017 | B2 |
| 9798169 | Su et al. | Oct 2017 | B2 |
| 10054732 | Robinson et al. | Aug 2018 | B2 |
| 10067726 | Wakamoto et al. | Sep 2018 | B2 |
| 10126575 | Robinson et al. | Nov 2018 | B1 |
| 10146093 | Sakai et al. | Dec 2018 | B2 |
| 10216018 | Fang et al. | Feb 2019 | B2 |
| 10288914 | Chung et al. | May 2019 | B2 |
| 10303030 | Robinson et al. | May 2019 | B2 |
| 10401638 | Robinson et al. | Sep 2019 | B2 |
| 10424232 | Schubert et al. | Sep 2019 | B2 |
| 10488705 | Xu et al. | Nov 2019 | B2 |
| 10527775 | Yang et al. | Jan 2020 | B2 |
| 10627670 | Robinson et al. | Apr 2020 | B2 |
| 10649248 | Jiang et al. | May 2020 | B1 |
| 10649259 | Lee et al. | May 2020 | B2 |
| 10712608 | Robinson et al. | Jul 2020 | B2 |
| 10802356 | Harrold et al. | Oct 2020 | B2 |
| 10935714 | Woodgate et al. | Mar 2021 | B2 |
| 10948648 | Ihas et al. | Mar 2021 | B2 |
| 10976578 | Robinson et al. | Apr 2021 | B2 |
| 11016341 | Robinson et al. | May 2021 | B2 |
| 11070791 | Woodgate et al. | Jul 2021 | B2 |
| 11079645 | Harrold et al. | Aug 2021 | B2 |
| 11079646 | Robinson et al. | Aug 2021 | B2 |
| 11092851 | Robinson et al. | Aug 2021 | B2 |
| 11099433 | Robinson et al. | Aug 2021 | B2 |
| 11099448 | Woodgate et al. | Aug 2021 | B2 |
| 11237417 | Woodgate et al. | Feb 2022 | B2 |
| 11327358 | Robinson et al. | May 2022 | B2 |
| 11366358 | Wu et al. | Jun 2022 | B2 |
| 11442316 | Woodgate et al. | Sep 2022 | B2 |
| 20010024561 | Cornelissen et al. | Sep 2001 | A1 |
| 20020015300 | Katsu et al. | Feb 2002 | A1 |
| 20020024529 | Miller et al. | Feb 2002 | A1 |
| 20020171793 | Sharp et al. | Nov 2002 | A1 |
| 20030030764 | Lee | Feb 2003 | A1 |
| 20030058381 | Shinohara et al. | Mar 2003 | A1 |
| 20030089956 | Allen et al. | May 2003 | A1 |
| 20030107686 | Sato et al. | Jun 2003 | A1 |
| 20030117792 | Kunimochi et al. | Jun 2003 | A1 |
| 20030169499 | Bourdelais et al. | Sep 2003 | A1 |
| 20030214615 | Colgan et al. | Nov 2003 | A1 |
| 20030222857 | Abileah | Dec 2003 | A1 |
| 20040015729 | Elms et al. | Jan 2004 | A1 |
| 20040100598 | Adachi et al. | May 2004 | A1 |
| 20040125430 | Kasajima et al. | Jul 2004 | A1 |
| 20040141107 | Jones | Jul 2004 | A1 |
| 20040145703 | O'Connor et al. | Jul 2004 | A1 |
| 20040223094 | Hamada et al. | Nov 2004 | A1 |
| 20040240777 | Woodgate et al. | Dec 2004 | A1 |
| 20040264910 | Suzuki et al. | Dec 2004 | A1 |
| 20050002174 | Min et al. | Jan 2005 | A1 |
| 20050111100 | Mather et al. | May 2005 | A1 |
| 20050117186 | Li et al. | Jun 2005 | A1 |
| 20050135116 | Epstein et al. | Jun 2005 | A1 |
| 20050157225 | Toyooka et al. | Jul 2005 | A1 |
| 20050190326 | Jeon et al. | Sep 2005 | A1 |
| 20050190329 | Okumura | Sep 2005 | A1 |
| 20050213348 | Parikka et al. | Sep 2005 | A1 |
| 20050219693 | Hartkop et al. | Oct 2005 | A1 |
| 20050243265 | Winlow et al. | Nov 2005 | A1 |
| 20050259205 | Sharp et al. | Nov 2005 | A1 |
| 20050270798 | Lee et al. | Dec 2005 | A1 |
| 20060066785 | Moriya | Mar 2006 | A1 |
| 20060082702 | Jacobs et al. | Apr 2006 | A1 |
| 20060098296 | Woodgate et al. | May 2006 | A1 |
| 20060146405 | MacMaster | Jul 2006 | A1 |
| 20060203162 | Ito et al. | Sep 2006 | A1 |
| 20060215244 | Yosha et al. | Sep 2006 | A1 |
| 20060244884 | Jeon et al. | Nov 2006 | A1 |
| 20060262255 | Wang et al. | Nov 2006 | A1 |
| 20060262258 | Wang et al. | Nov 2006 | A1 |
| 20060262558 | Cornelissen | Nov 2006 | A1 |
| 20060268207 | Tan et al. | Nov 2006 | A1 |
| 20060285040 | Kobayashi | Dec 2006 | A1 |
| 20070008471 | Wang et al. | Jan 2007 | A1 |
| 20070024970 | Lub et al. | Feb 2007 | A1 |
| 20070030240 | Sumiyoshi et al. | Feb 2007 | A1 |
| 20070035964 | Olczak | Feb 2007 | A1 |
| 20070047254 | Schardt et al. | Mar 2007 | A1 |
| 20070064163 | Tan et al. | Mar 2007 | A1 |
| 20070139772 | Wang | Jun 2007 | A1 |
| 20070223251 | Liao | Sep 2007 | A1 |
| 20070268427 | Uehara | Nov 2007 | A1 |
| 20070285775 | Lesage et al. | Dec 2007 | A1 |
| 20080008434 | Lee et al. | Jan 2008 | A1 |
| 20080068329 | Shestak et al. | Mar 2008 | A1 |
| 20080068862 | Shimura | Mar 2008 | A1 |
| 20080129899 | Sharp | Jun 2008 | A1 |
| 20080158491 | Zhu et al. | Jul 2008 | A1 |
| 20080158912 | Chang et al. | Jul 2008 | A1 |
| 20080205066 | Ohta et al. | Aug 2008 | A1 |
| 20080285310 | Aylward et al. | Nov 2008 | A1 |
| 20080316198 | Fukushima et al. | Dec 2008 | A1 |
| 20090009894 | Chuang | Jan 2009 | A1 |
| 20090040426 | Mather et al. | Feb 2009 | A1 |
| 20090085894 | Gandhi et al. | Apr 2009 | A1 |
| 20090086509 | Omori et al. | Apr 2009 | A1 |
| 20090109381 | Haruyama | Apr 2009 | A1 |
| 20090109703 | Chen et al. | Apr 2009 | A1 |
| 20090128735 | Larson et al. | May 2009 | A1 |
| 20090128746 | Kean et al. | May 2009 | A1 |
| 20090135623 | Kunimochi | May 2009 | A1 |
| 20090174843 | Sakai et al. | Jul 2009 | A1 |
| 20090213147 | Sagardoyburu et al. | Aug 2009 | A1 |
| 20090213298 | Mimura et al. | Aug 2009 | A1 |
| 20090213305 | Ohmuro et al. | Aug 2009 | A1 |
| 20090244415 | Ide | Oct 2009 | A1 |
| 20100002296 | Choi et al. | Jan 2010 | A1 |
| 20100014313 | Tillin et al. | Jan 2010 | A1 |
| 20100066960 | Smith et al. | Mar 2010 | A1 |
| 20100128200 | Morishita et al. | May 2010 | A1 |
| 20100149459 | Yabuta et al. | Jun 2010 | A1 |
| 20100177113 | Gay et al. | Jul 2010 | A1 |
| 20100187704 | Hsu et al. | Jul 2010 | A1 |
| 20100205667 | Anderson et al. | Aug 2010 | A1 |
| 20100214324 | Broughton et al. | Aug 2010 | A1 |
| 20100238376 | Sakai et al. | Sep 2010 | A1 |
| 20100283930 | Park et al. | Nov 2010 | A1 |
| 20100289989 | Adachi et al. | Nov 2010 | A1 |
| 20100295755 | Broughton et al. | Nov 2010 | A1 |
| 20100328438 | Ohyama et al. | Dec 2010 | A1 |
| 20110018860 | Parry-Jones et al. | Jan 2011 | A1 |
| 20110032483 | Hruska et al. | Feb 2011 | A1 |
| 20110176089 | Ishikawa et al. | Jul 2011 | A1 |
| 20110241573 | Tsai et al. | Oct 2011 | A1 |
| 20110241983 | Chang | Oct 2011 | A1 |
| 20110255304 | Kinoshita | Oct 2011 | A1 |
| 20110286222 | Coleman | Nov 2011 | A1 |
| 20110321143 | Angaluri et al. | Dec 2011 | A1 |
| 20120002121 | Pirs et al. | Jan 2012 | A1 |
| 20120020078 | Chang | Jan 2012 | A1 |
| 20120086875 | Yokota | Apr 2012 | A1 |
| 20120120351 | Kawata | May 2012 | A1 |
| 20120127573 | Robinson et al. | May 2012 | A1 |
| 20120147026 | Gass et al. | Jun 2012 | A1 |
| 20120147280 | Osterman et al. | Jun 2012 | A1 |
| 20120170315 | Fan et al. | Jul 2012 | A1 |
| 20120188792 | Matsumoto et al. | Jul 2012 | A1 |
| 20120212414 | Osterhout et al. | Aug 2012 | A1 |
| 20120235891 | Nishitani et al. | Sep 2012 | A1 |
| 20120294037 | Holman et al. | Nov 2012 | A1 |
| 20120299913 | Robinson et al. | Nov 2012 | A1 |
| 20120314145 | Robinson | Dec 2012 | A1 |
| 20120320311 | Gotou et al. | Dec 2012 | A1 |
| 20120327101 | Blixt et al. | Dec 2012 | A1 |
| 20130039062 | Vinther et al. | Feb 2013 | A1 |
| 20130057807 | Goto et al. | Mar 2013 | A1 |
| 20130100097 | Martin | Apr 2013 | A1 |
| 20130107174 | Yun et al. | May 2013 | A1 |
| 20130120817 | Yoon et al. | May 2013 | A1 |
| 20130128165 | Lee et al. | May 2013 | A1 |
| 20130242231 | Kurata et al. | Sep 2013 | A1 |
| 20130242612 | Lee et al. | Sep 2013 | A1 |
| 20130278544 | Cok | Oct 2013 | A1 |
| 20130293793 | Lu | Nov 2013 | A1 |
| 20130300985 | Bulda | Nov 2013 | A1 |
| 20130307831 | Robinson et al. | Nov 2013 | A1 |
| 20130308339 | Woodgate et al. | Nov 2013 | A1 |
| 20130321340 | Seo et al. | Dec 2013 | A1 |
| 20130328866 | Woodgate et al. | Dec 2013 | A1 |
| 20140009508 | Woodgate et al. | Jan 2014 | A1 |
| 20140022619 | Woodgate et al. | Jan 2014 | A1 |
| 20140071382 | Scardato | Mar 2014 | A1 |
| 20140098418 | Lin | Apr 2014 | A1 |
| 20140098558 | Vasylyev | Apr 2014 | A1 |
| 20140104147 | Nakahara et al. | Apr 2014 | A1 |
| 20140111760 | Guo et al. | Apr 2014 | A1 |
| 20140132887 | Kurata | May 2014 | A1 |
| 20140133181 | Ishida et al. | May 2014 | A1 |
| 20140140091 | Vasylyev | May 2014 | A1 |
| 20140140095 | Yuki et al. | May 2014 | A1 |
| 20140176873 | Shinohara et al. | Jun 2014 | A1 |
| 20140185322 | Liao | Jul 2014 | A1 |
| 20140201844 | Buck | Jul 2014 | A1 |
| 20140211125 | Kurata | Jul 2014 | A1 |
| 20140232836 | Woodgate et al. | Aug 2014 | A1 |
| 20140232960 | Schwartz et al. | Aug 2014 | A1 |
| 20140240344 | Tomono et al. | Aug 2014 | A1 |
| 20140240828 | Robinson et al. | Aug 2014 | A1 |
| 20140240839 | Yang et al. | Aug 2014 | A1 |
| 20140268358 | Kusaka et al. | Sep 2014 | A1 |
| 20140286043 | Sykora et al. | Sep 2014 | A1 |
| 20140286044 | Johnson et al. | Sep 2014 | A1 |
| 20140289835 | Varshavsky et al. | Sep 2014 | A1 |
| 20140340728 | Taheri | Nov 2014 | A1 |
| 20140361990 | Leister | Dec 2014 | A1 |
| 20140367873 | Yang et al. | Dec 2014 | A1 |
| 20150035872 | Shima et al. | Feb 2015 | A1 |
| 20150055366 | Chang et al. | Feb 2015 | A1 |
| 20150116212 | Freed et al. | Apr 2015 | A1 |
| 20150177447 | Woodgate et al. | Jun 2015 | A1 |
| 20150177563 | Cho et al. | Jun 2015 | A1 |
| 20150185398 | Chang et al. | Jul 2015 | A1 |
| 20150205157 | Sakai et al. | Jul 2015 | A1 |
| 20150268479 | Woodgate et al. | Sep 2015 | A1 |
| 20150286061 | Seo et al. | Oct 2015 | A1 |
| 20150286817 | Haddad et al. | Oct 2015 | A1 |
| 20150293273 | Chen et al. | Oct 2015 | A1 |
| 20150293289 | Shinohara et al. | Oct 2015 | A1 |
| 20150301400 | Kimura et al. | Oct 2015 | A1 |
| 20150338564 | Zhang et al. | Nov 2015 | A1 |
| 20150346417 | Powell | Dec 2015 | A1 |
| 20150346532 | Do et al. | Dec 2015 | A1 |
| 20150355490 | Kao et al. | Dec 2015 | A1 |
| 20150378085 | Robinson et al. | Dec 2015 | A1 |
| 20160054508 | Hirayama et al. | Feb 2016 | A1 |
| 20160103264 | Lee et al. | Apr 2016 | A1 |
| 20160132721 | Bostick et al. | May 2016 | A1 |
| 20160147074 | Kobayashi et al. | May 2016 | A1 |
| 20160154259 | Kim et al. | Jun 2016 | A1 |
| 20160216420 | Gaides et al. | Jul 2016 | A1 |
| 20160216540 | Cho et al. | Jul 2016 | A1 |
| 20160224106 | Liu | Aug 2016 | A1 |
| 20160238869 | Osterman et al. | Aug 2016 | A1 |
| 20160259115 | Kitano et al. | Sep 2016 | A1 |
| 20160334898 | Kwak et al. | Nov 2016 | A1 |
| 20160349444 | Robinson et al. | Dec 2016 | A1 |
| 20160356943 | Choi et al. | Dec 2016 | A1 |
| 20160357046 | Choi et al. | Dec 2016 | A1 |
| 20170003436 | Inoue et al. | Jan 2017 | A1 |
| 20170031206 | Smith et al. | Feb 2017 | A1 |
| 20170085869 | Choi et al. | Mar 2017 | A1 |
| 20170090103 | Holman | Mar 2017 | A1 |
| 20170090237 | Kim et al. | Mar 2017 | A1 |
| 20170092187 | Bergquist | Mar 2017 | A1 |
| 20170092229 | Greenebaum et al. | Mar 2017 | A1 |
| 20170115485 | Saito et al. | Apr 2017 | A1 |
| 20170123241 | Su et al. | May 2017 | A1 |
| 20170139110 | Woodgate et al. | May 2017 | A1 |
| 20170168633 | Kwak et al. | Jun 2017 | A1 |
| 20170205558 | Hirayama et al. | Jul 2017 | A1 |
| 20170236494 | Sommerlade et al. | Aug 2017 | A1 |
| 20170269283 | Wang et al. | Sep 2017 | A1 |
| 20170269285 | Hirayama et al. | Sep 2017 | A1 |
| 20170276960 | Osterman et al. | Sep 2017 | A1 |
| 20170315423 | Serati et al. | Nov 2017 | A1 |
| 20170329399 | Azam et al. | Nov 2017 | A1 |
| 20170336661 | Harrold et al. | Nov 2017 | A1 |
| 20170339398 | Woodgate et al. | Nov 2017 | A1 |
| 20170343715 | Fang et al. | Nov 2017 | A1 |
| 20170363798 | Hirayama et al. | Dec 2017 | A1 |
| 20170363913 | Yi | Dec 2017 | A1 |
| 20180011173 | Newman | Jan 2018 | A1 |
| 20180014007 | Brown | Jan 2018 | A1 |
| 20180052346 | Sakai et al. | Feb 2018 | A1 |
| 20180082068 | Lancioni et al. | Mar 2018 | A1 |
| 20180095581 | Hwang et al. | Apr 2018 | A1 |
| 20180113334 | Fang et al. | Apr 2018 | A1 |
| 20180188576 | Xu et al. | Jul 2018 | A1 |
| 20180188603 | Fang et al. | Jul 2018 | A1 |
| 20180196275 | Robinson et al. | Jul 2018 | A1 |
| 20180210243 | Fang et al. | Jul 2018 | A1 |
| 20180210253 | Kashima | Jul 2018 | A1 |
| 20180231811 | Wu | Aug 2018 | A1 |
| 20180252949 | Klippstein et al. | Sep 2018 | A1 |
| 20180259799 | Kroon | Sep 2018 | A1 |
| 20180259812 | Goda et al. | Sep 2018 | A1 |
| 20180284341 | Woodgate et al. | Oct 2018 | A1 |
| 20180321523 | Robinson et al. | Nov 2018 | A1 |
| 20180321553 | Robinson et al. | Nov 2018 | A1 |
| 20180329245 | Robinson et al. | Nov 2018 | A1 |
| 20180364526 | Finnemeyer et al. | Dec 2018 | A1 |
| 20190086706 | Robinson et al. | Mar 2019 | A1 |
| 20190121173 | Robinson et al. | Apr 2019 | A1 |
| 20190154896 | Yanai | May 2019 | A1 |
| 20190196235 | Robinson et al. | Jun 2019 | A1 |
| 20190196236 | Chen et al. | Jun 2019 | A1 |
| 20190197928 | Schubert et al. | Jun 2019 | A1 |
| 20190215509 | Woodgate et al. | Jul 2019 | A1 |
| 20190227366 | Harrold et al. | Jul 2019 | A1 |
| 20190235304 | Tamada et al. | Aug 2019 | A1 |
| 20190250458 | Robinson et al. | Aug 2019 | A1 |
| 20190278010 | Sakai et al. | Sep 2019 | A1 |
| 20190293858 | Woodgate et al. | Sep 2019 | A1 |
| 20190293983 | Robinson et al. | Sep 2019 | A1 |
| 20190353944 | Acreman et al. | Nov 2019 | A1 |
| 20190361165 | Chang et al. | Nov 2019 | A1 |
| 20200026125 | Robinson et al. | Jan 2020 | A1 |
| 20200041839 | Robinson et al. | Feb 2020 | A1 |
| 20200110301 | Harrold | Apr 2020 | A1 |
| 20200159055 | Robinson et al. | May 2020 | A1 |
| 20200185590 | Malhotra et al. | Jun 2020 | A1 |
| 20200218101 | Ihas et al. | Jul 2020 | A1 |
| 20200225402 | Ihas et al. | Jul 2020 | A1 |
| 20200233142 | Liao et al. | Jul 2020 | A1 |
| 20210033898 | Woodgate et al. | Feb 2021 | A1 |
| 20210116627 | Tsuji | Apr 2021 | A1 |
| 20210149233 | Robinson et al. | May 2021 | A1 |
| Number | Date | Country |
|---|---|---|
| 2222313 | Jun 1998 | CA |
| 1125943 | Oct 2003 | CN |
| 1776484 | May 2006 | CN |
| 101042449 | Sep 2007 | CN |
| 101256251 | Sep 2008 | CN |
| 101454712 | Jun 2009 | CN |
| 101518095 | Aug 2009 | CN |
| 101681061 | Mar 2010 | CN |
| 103473494 | Dec 2013 | CN |
| 103688211 | Mar 2014 | CN |
| 104133292 | Nov 2014 | CN |
| 104303085 | Jan 2015 | CN |
| 104321686 | Jan 2015 | CN |
| 104380177 | Feb 2015 | CN |
| 204740413 | Nov 2015 | CN |
| 105842909 | Aug 2016 | CN |
| 106104372 | Nov 2016 | CN |
| 106415342 | Feb 2017 | CN |
| 209171779 | Jul 2019 | CN |
| 1956423 | Aug 2008 | EP |
| 2037318 | Mar 2009 | EP |
| 2405542 | Mar 2005 | GB |
| 2418518 | Mar 2006 | GB |
| 2428100 | Jan 2007 | GB |
| 2428345 | Jan 2007 | GB |
| 2482065 | Jan 2012 | GB |
| 2486935 | Sep 2013 | GB |
| S58143305 | Aug 1983 | JP |
| H01130783 | Sep 1989 | JP |
| H11174489 | Jul 1999 | JP |
| 2005316470 | Nov 2005 | JP |
| 2005345799 | Dec 2005 | JP |
| 2006139160 | Jun 2006 | JP |
| 2007501966 | Feb 2007 | JP |
| 2007148279 | Jun 2007 | JP |
| 2007273288 | Oct 2007 | JP |
| 2009020293 | Jan 2009 | JP |
| 2011103241 | May 2011 | JP |
| 2014032953 | Feb 2014 | JP |
| 2014099363 | May 2014 | JP |
| 20120011228 | Feb 2012 | KR |
| 20130046116 | May 2013 | KR |
| 1020150021937 | Mar 2015 | KR |
| 1020170013915 | Feb 2017 | KR |
| 1020170040565 | Apr 2017 | KR |
| 101990286 | Jun 2019 | KR |
| M537663 | Mar 2017 | TW |
| I612360 | Jan 2018 | TW |
| 2005071449 | Aug 2005 | WO |
| 2006030702 | Mar 2006 | WO |
| 2008001896 | Jan 2008 | WO |
| 2008078764 | Jul 2008 | WO |
| 2008093445 | Aug 2008 | WO |
| 2009008406 | Jan 2009 | WO |
| 2009011199 | Jan 2009 | WO |
| 2010021926 | Feb 2010 | WO |
| 2010143705 | Dec 2010 | WO |
| 2014011328 | Jan 2014 | WO |
| 2014130860 | Aug 2014 | WO |
| 2015040776 | Mar 2015 | WO |
| 2015057625 | Apr 2015 | WO |
| 2015143227 | Sep 2015 | WO |
| 2015157184 | Oct 2015 | WO |
| 2015190311 | Dec 2015 | WO |
| 2015200814 | Dec 2015 | WO |
| 2016195786 | Dec 2016 | WO |
| 2017050631 | Mar 2017 | WO |
| 2017117570 | Jul 2017 | WO |
| 2018035492 | Feb 2018 | WO |
| 2018178790 | Oct 2018 | WO |
| 2018208618 | Nov 2018 | WO |
| 2019055755 | Mar 2019 | WO |
| 2019067846 | Apr 2019 | WO |
| 2019147762 | Aug 2019 | WO |
| Entry |
|---|
| CN-201880042320.X Notification of the Third Office Action from the Chinese Patent Office dated Dec. 30, 2022. |
| CN-201980082757.0 Notification of the 1st Office Action of the Chinese Patent Office dated Dec. 5, 2022. |
| JP2020-540724 Non-Final Notice of Reasons for Rejection dated Jan. 4, 2023. |
| JP-2020-540797 Non-Final Notice of Reasons for Rejection from the Japan Patent Office dated Dec. 6, 2022. |
| PCT/US2022/045030 International search report and written opinion of the international searching authority dated Jan. 3, 2023. |
| EP-20754927.0 Extended European Search Report of European Patent Office dated Sep. 19, 2022. |
| EP19771688.9 Notification of the First Office Action dated Mar. 6, 2023. |
| JP2020-550747 Non-Final Notice of Reasons for Rejection dated Mar. 29, 2023. |
| KR10-2020-7010753 Notice of Preliminary Rejection dated Feb. 17, 2023. |
| Chiu, et al, “Advanced Hyoer-Viewing Angle Controllable LCD”, 39-1 / M.-H. Chiu Invited Paper; AUO Technology Center, AU Optronics Corp., Hsinchu, Taiwan, SID 2021 Digest, ISSN 0097-996X/21/5202-0543, pp. 543-545. |
| PCT/US2021/029958 International search report and written opinion of the international searching authority dated Aug. 10, 2021. |
| PCT/US2021/043435 International search report and written opinion of the international searching authority dated Nov. 1, 2021. |
| PCT/US2021/043444 International search report and written opinion of the international searching authority dated Nov. 1, 2021. |
| Robson, et al. “Spatial and temporal contrast-sensitivity functions of the visual system”, J. Opt. Soc. Amer., vol. 56, pp. 1141-1142 (1966). |
| Simonyan et al., “Very Deep Convolutional Networks For Large-Scale Image Recognition”, ICLR 2015. |
| Weindorf et al., “Active Circular Polarizer OLED E-Mirror”, Proceedings of the Society for Information Display 25th Annual Symposium of Vehicle Displays, Livonia, MI, pp. 225-237, Sep. 25-26, 2018. |
| Adachi, et al. “P-228L: Late-News Poster: Controllable Viewing-Angle Displays using a Hybrid Aligned Nematic Liquid Crystal Cell”, ISSN, SID 2006 Digest, pp. 705-708. |
| Brudy et al., “Is Anyone Looking? Mitigating Shoulder Surfing on Public Displays through Awareness and Protection”, Proceedings of the International Symposium On Persuasive Displays (Jun. 3, 2014), pp. 1-6. |
| Cheng, et al., “Fast-Response Liquid Crystal Variable Optical Retarder and Multilevel Attenuator,” Optical Engineering 52 (10), 107105 (Oct. 16, 2013). (Year: 2013). |
| CN201680061632.6 Notification of the First Office Action dated Sep. 14, 2021. |
| CN201780030715.3 Notification of the First Office Action dated Jan. 21, 2020. |
| CN201880042320.X Notification of the First Office Action dated May 25, 2021. |
| CN201880073578.6 Notification of the First Office Action dated Aug. 27, 2021. |
| CN-201980020303.0—Notification of the First Office Action dated Dec. 16, 2021. |
| EP-16860628.3 Extended European Search Report of European Patent Office dated Apr. 26, 2019. |
| EP-17799963.8 Extended European Search Report of European Patent Office dated Oct. 9, 2019. |
| EP-18855604.7 Extended European Search Report of European Patent Office dated Jun. 1, 2021. |
| EP-18857077.4 Extended European Search Report of European Patent Office dated Jun. 16, 2021. |
| EP-19743619.9 Extended European Search of European Patent Office dated Nov. 23, 2021. |
| EP-19743701.5 Extended European Search Report of European Patent Office dated Nov. 24, 2021. |
| EP19771688.9 Extended European Search Report of European Patent Office dated Dec. 2, 2021. |
| EP-19825448.4 Extended European Search Report of European Patent Office dated Mar. 10, 2022. |
| Gass, et al. “Privacy LCD Technology for Cellular Phones”, Sharp Laboratories of Europe Ltd, Mobile LCD Group, Feb. 2007, pp. 45-49. |
| Ishikawa, T., “New Design for a Highly Collimating Turning Film”, SID 06 Digest, pp. 514-517. |
| JP2019-561773 Non-Final Notice of Reasons for Rejection dated Mar. 22, 2022. |
| Kalantar, et al. “Backlight Unit With Double Surface Light Emission,” J. Soc. Inf. Display, vol. 12, Issue 4, pp. 379-387 (Dec. 2004). |
| PCT/US2016/058695 International search report and written opinion of the international searching authority dated Feb. 28, 2017. |
| PCT/US2017/032734 International search report and written opinion of the international searching authority dated Jul. 27, 2017. |
| PCT/US2018/031206 International search report and written opinion of the international searching authority dated Jul. 20, 2018. |
| PCT/US2018/031218 International search report and written opinion of the international searching authority dated Jul. 19, 2018. |
| PCT/US2018/051021 International search report and written opinion of the international searching authority dated Nov. 21, 2018. |
| PCT/US2018/051027 International search report and written opinion of the international searching authority dated Nov. 30, 2018. |
| PCT/US2018/053328 International search report and written opinion of the international searching authority dated Nov. 30, 2018. |
| PCT/US2018/059249 International search report and written opinion of the international searching authority dated Jan. 3, 2019. |
| PCT/US2018/059256 International search report and written opinion of the international searching authority dated Jan. 3, 2019. |
| PCT/US2019/014889 International search report and written opinion of the international searching authority dated May 24, 2019. |
| PCT/US2019/014902 International search report and written opinion of the international searching authority dated Jun. 25, 2019. |
| PCT/US2019/023659 International search report and written opinion of the international searching authority dated Jun. 10, 2019. |
| PCT/US2019/038409 International search report and written opinion of the international searching authority dated Sep. 19, 2019. |
| PCT/US2019/038466 International search report and written opinion of the international searching authority dated Nov. 5, 2019. |
| PCT/US2019/042027 International search report and written opinion of the international searching authority dated Oct. 15, 2019. |
| PCT/US2019/054291 International search report and written opinion of the international searching authority dated Jan. 6, 2020. |
| PCT/US2019/059990 International search report and written opinion of the international searching authority dated Feb. 28, 2020. |
| PCT/US2019/066208 International search report and written opinion of the international searching authority dated Feb. 27, 2020. |
| PCT/US2020/017537 International search report and written opinion of the international searching authority dated Apr. 29, 2020. |
| PCT/US2020/040686 International search report and written opinion of the international searching authority dated Nov. 20, 2020. |
| PCT/US2020/044574 International search report and written opinion of the international searching authority dated Oct. 21, 2020. |
| PCT/US2020/053863 International search report and written opinion of the international searching authority dated Mar. 12, 2021. |
| PCT/US2020/060155 International search report and written opinion of the international searching authority dated Feb. 5, 2021. |
| PCT/US2020/060191 International search report and written opinion of the international searching authority dated Feb. 8, 2021. |
| PCT/US2020/063638 International search report and written opinion of the international searching authority dated Mar. 2, 2021. |
| PCT/US2020/064633 International search report and written opinion of the international searching authority dated Mar. 15, 2021. |
| PCT/US2021/029937 International search report and written opinion of the international searching authority dated Aug. 6, 2021. |
| PCT/US2021/029944 International search report and written opinion of the international searching authority dated Aug. 3, 2021. |
| PCT/US2021/029947 International search report and written opinion of the international searching authority dated Aug. 10, 2021. |
| PCT/US2021/029954 International search report and written opinion of the international searching authority dated Aug. 10, 2021. |
| CN201980030279.9 Notification of the First Office Action dated Mar. 29, 2022. |
| EP-19881483.2 Extended European Search Report of European Patent Office dated Aug. 5, 2022. |
| JP2020-509511 Non-Final Notice of Reasons for Rejection dated Jul. 19, 2022. |
| Nelkon et al., “Advanced Level Physics”, Third edition with SI units, Heinemann Educational Books LTD, London, 1970. |
| TW107132221 First Office Action dated Apr. 28, 2022. |
| EP-20835231.0 Extended European Search Report of European Patent Office dated May 15, 2023. |
| PCT/US2023/012240 International search report and written opinion of the international searching authority dated Apr. 27, 2023. |
| PCT/US2023/012243 International search report and written opinion of the international searching authority dated May 10, 2023. |
| Number | Date | Country | |
|---|---|---|---|
| 20220404654 A1 | Dec 2022 | US |
| Number | Date | Country | |
|---|---|---|---|
| 63114054 | Nov 2020 | US | |
| 63112823 | Nov 2020 | US | |
| 63058314 | Jul 2020 | US |
| Number | Date | Country | |
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| Parent | 17387071 | Jul 2021 | US |
| Child | 17739996 | US |
