The present disclosure relates visual display devices and related components, modules, and methods.
Visual displays provide information to viewer(s) including still images, video, data, etc. Visual displays have applications in diverse fields including entertainment, education, engineering, science, professional training, advertising, to name just a few examples. Some visual displays such as TV sets display images to several users, and some visual display systems such s near-eye displays (NEDs) are intended for individual users.
An artificial reality system generally includes an NED (e.g., a headset or a pair of glasses) configured to present content to a user. The near-eye display may display virtual objects or combine images of real objects with virtual objects, as in virtual reality (VR), augmented reality (AR), or mixed reality (MR) applications. For example, in an AR system, a user may view images of virtual objects (e.g., computer-generated images (CGIs)) superimposed with the surrounding environment by seeing through a “combiner” component. The combiner of a wearable display is typically transparent to external light but includes some light routing optic to direct the display light into the user's field of view.
Because a display of HMD or NED is usually worn on the head of a user, a large, bulky, unbalanced, and/or heavy display device with a heavy battery would be cumbersome and uncomfortable for the user to wear. Consequently, head-mounted display devices can benefit from a compact and efficient configuration, including efficient light sources and illuminators providing illumination of a display panel, high-throughput combiner components, ocular lenses, and other optical elements in the image forming train.
Exemplary embodiments will now be described in conjunction with the drawings, which are not to scale, in which like elements are indicated with like reference numerals, and in which:
While the present teachings are described in conjunction with various embodiments and examples, it is not intended that the present teachings be limited to such embodiments. On the contrary, the present teachings encompass various alternatives and equivalents, as will be appreciated by those of skill in the art. All statements herein reciting principles, aspects, and embodiments of this disclosure, as well as specific examples thereof, are intended to encompass both structural and functional equivalents thereof. Additionally, it is intended that such equivalents include both currently known equivalents as well as equivalents developed in the future, i.e., any elements developed that perform the same function, regardless of structure.
As used herein, the terms “first”, “second”, and so forth are not intended to imply sequential ordering, but rather are intended to distinguish one element from another, unless explicitly stated. Similarly, sequential ordering of method steps does not imply a sequential order of their execution, unless explicitly stated.
AR and VR displays may use pupil-replicating lightguides to carry images to an eyebox and/or to illuminate display panels that generate images to be displayed. Herein the term “eyebox” means a geometrical area for the user's eye where a good-quality image may be observed by a user of the NED. A pupil-replicating lightguide may include grating structures for in-coupling a light beam into the lightguide, and/or for out-coupling portions of the light beam along the waveguide surface. In accordance with this disclosure, a grating structure of a pupil-replicating lightguide may include a tunable/switchable grating with switchable or tunable diffraction efficiency, grating pitch or grating period, blazing angle, etc. The terms “grating pitch” and “grating period” are used herein interchangeably. The term “tunable” encompasses both continuously tunable and switchable between two or more states. The term “diffraction efficiency” refers to aspects of the performance of the diffraction grating in terms of power throughput of the diffraction grating. In particular, the diffraction efficiency can be a measure of the optical power diffracted into a given direction compared to the power incident onto the diffractive element. In examples described herein, the diffraction efficiency is typically a measure of the optical power diffracted by the grating or a segment thereof in the first order of diffraction relative to the power incident onto the grating or the segment thereof. The term “output efficiency” as used herein refers to a fraction of the optical power of a light source of a display apparatus that is available to the user for viewing images.
An aspect of the present disclosure relates to a display system comprising a lightguide and an image light source coupled to the lightguide. The lightguide is configured to receive image light emitted by the image light source and to convey the image light received in a target field of view (FOV) of the display to an eyebox for presenting to a user. The term “field of view” (FOV), when used in relation to a display system, may refer to an angular range of light propagation supported by the system or visible to the user. A two-dimensional (2D) FOV may be defined by angular ranges in two orthogonal planes. For example, a 2D FOV of a NED device may be defined by two one-dimensional (1D) FOVs, which may be a vertical FOV, for example +\−20° relative to a horizontal plane, and a horizontal FOV, for example +\−30° relative to the vertical plane. With respect to a FOV of a NED, the “vertical” and “horizontal” planes or directions may be defined relative to the head of a standing person wearing the NED. Otherwise the terms “vertical” and “horizontal” may be used in the present disclosure with reference to two orthogonal planes of an optical system or device being described, without implying any particular relationship to the environment in which the optical system or device is used, or any particular orientation thereof to the environment.
Embodiments described herein relate to a pupil replicating lightguide operable to convey to a user different FOV portions at different time instances. Such lightguides include active, i.e. dynamically tunable, diffraction gratings configured to support a variable or switchable FOV and to enable adjusting one or more of the grating's properties to the particular FOV portion being displayed for providing an enhanced viewer experience. In some embodiments, an out-coupling (“output”) diffraction grating of a pupil-replicating lightguide may be segmented, with the segments individually switchable between a diffracting and a non-diffracting state depending on a FOV portion being displayed. By switching to a non-diffracting state a portion of an output grating that doesn't contribute to a FOV portion being currently displayed, grating-related artifacts, e.g. the “rainbow” in AR displays, can be reduced and the image brightness improved. Furthermore, the diffraction efficiency of a currently “FOV-contributing” subs-set of the grating segments may be adjusted to the FOV portion being conveyed, e.g. to provide enhanced image uniformity. In some embodiments, the FOV portion being displayed depends on a content of the image.
In some embodiments, an in-coupling (“input”) grating and an out-coupling (“output”) grating of a lightguide may be operable, i.e. their grating pitch simultaneously tuned, to quickly scan through a sequence of FOV portions of an image. In such embodiments, the image is presented to the viewer in a time-multiplexed manner, with the visual cortex of a viewer integrating the different FOV portions into a single image FOV; this approach may enable a greater overall FOV than can be instantaneously supported by the lightguide. By segmenting the output grating and selectively adjusting the diffraction efficiency of different segments during the FOV scan, the image brightness and/or uniformity of the lightguide may be further improved.
Accordingly, an aspect of the present disclosure provides a display apparatus for displaying images within a target field-of-view (FOV), the display apparatus comprising a lightguide for relaying image light carrying the images to an eyebox. The lightguide comprises a substrate of optically transparent material, the substrate comprising two opposing surfaces for guiding the image light in the substrate by reflections therefrom. The lightguide further comprises an output diffraction grating disposed in or upon the substrate and configured to diffract the image light out of the lightguide toward the eyebox, wherein the output diffraction grating has one or more electrically tunable characteristics and is operable to convey, to the eyebox, different FOV portions of the target FOV at different time instances. The display apparatus further comprises a controller configured to selectively tune the one or more electrically tunable characteristics in dependence on a FOV portion being conveyed.
In some implementations, the one or more electrically tunable characteristics may comprise a diffraction efficiency, and the output diffraction grating may comprise a plurality of grating segments disposed along the surfaces; the controller may be configured to selectively reduce the diffraction efficiency for one or more of the grating segments depending on the FOV portion being conveyed.
In some implementations, the one or more electrically tunable characteristics may comprise an output grating pitch, and the controller may be configured to selectively tune the output grating pitch in at least a segment of the output diffraction grating depending on the portion of the target FOV being displayed. The display apparatus may further comprise an input diffraction grating having an electrically tunable input grating pitch, with the controller configured to tune the electrically tunable input grating pitch in coordination with tuning the output grating pitch. In some of such implementations, the controller is configured to tune the input grating pitch, so as to direct beams of the image light from non-overlapping portions of the target FOV to propagate within the substrate at a same angle of incidence at the surfaces. In these or other implementations, the controller may be configured to tune the input grating pitch so that the image light propagates within the substrate at angles of incidence upon the opposing surfaces thereof smaller than 70 degrees for any FOV portion of the target FOV being conveyed.
Some implementations may comprise a source of the image light and an image processor for controlling the source depending on a content of the image, the image processor being operatively coupled to the controller, wherein the FOV portion being conveyed depends on the content of the image.
In any of the above implementations, the one or more electrically tunable characteristics of the output diffraction grating comprise a grating efficiency, and the controller may be configured to tune the grating efficiency depending on the FOV portion being displayed.
In some implementations, the display apparatus is configured for conveying, to the eyebox, an image in the target FOV sequentially portion by portion, and the controller is configured to at least once tune the one or more electrically tunable characteristics while the image is being displayed. In some of such implementations, the one or more electrically tunable grating characteristics being tuned comprise at least one of an output grating pitch in at least a segment of the output diffraction grating or diffraction efficiency in at least a segment of the output diffraction grating. In some of the above implementations, the output diffraction grating comprises a plurality of individually tunable grating segments, and the controller is configured to selectively tune at least one of the grating pitch or the diffraction efficiency for a subset of the individually tunable grating segments while the image is being displayed, the subset being dependent on the FOV portion being conveyed to the eyebox.
An aspect of the present disclosure provides a display apparatus for displaying an augmented reality (AR) image, the display apparatus comprising: an image projector for providing image light carrying the AR image, a lightguide, and a controller. The lightguide comprises a substrate of optically transparent material, the substrate comprising two opposing surfaces for guiding the image light in the substrate by reflections from the surfaces, and an output diffraction grating configured to diffract the image light out of the substrate for combining with ambient light carrying real scenery and for presenting the AR image to a user within a target field-of-view (FOV), wherein the output diffraction grating comprises a plurality of grating segments, each having an electrically variable diffraction efficiency. The controller is configured to selectively reduce the diffraction efficiency for one or more of the grating segments in dependence on a content of the AR image.
In some implementations of this aspect, the display apparatus is configured to present the AR image in a FOV portion of the target FOV dependent on the content of the AR image, and the controller is configured to switch the one or more grating segments to a substantially non-diffracting state when the one or more grating segments are disposed outside of the FOV portion presenting the AR image. In some implementations, the controller is configured to switch the one or more grating segments from the substantially non-diffracting state to a diffracting state when the content of the AR image changes. In some implementations, the controller may be configured to tune the diffraction efficiency of the one or more grating segments in the diffracting state.
An aspect of the present disclosure provides a method for displaying images to a user within a target field-of-view (FOV), comprising: a) coupling image light into a lightguide having an output region adjacent an eyebox; b) using an output diffraction grating located in the output region of the lightguide to convey to the eyebox different FOV portions of the image light at different time instances, the different FOV portions of the image light being conveyed within different portions of the target FOV; and c) tuning at least one of a grating pitch or a grating efficiency of the output diffraction grating in dependence on a FOV portion being conveyed to the eyebox.
In some implementations, the method may comprise selecting the FOV portion being conveyed depending on a content of the image. In some implementations the method may comprise selecting the FOV portion being conveyed depending on a location of the image content within the target FOV.
In some implementations, the method may comprise using the output diffraction grating to convey, to the eyebox over a frame time interval, the target FOV sequentially portion by portion, at least once during the frame time interval tuning the at least one of the grating pitch or the diffraction efficiency for the FOV portion being displayed.
In some implementations, the method may comprise i) using a scanning image projector to provide image light carrying the image to an input diffraction grating of the lightguide by sequentially scanning a beam of the image light through different portions of the target FOV over a frame time interval, the input diffraction grating tunable to couple the beam into the lightguide; and ii) tuning a pitch of each of the input diffraction grating and the at least a segment of the output diffraction grating in coordination with the scanning.
The image projector 103 may be embodied, for example, using a pixelated display panel, e.g. an LC micro display, optionally having suitable optics at its output. It may also be embodied using a light source, such as e.g. one or more light-emitting diodes (LED), superluminescent light-emitting diodes (SLED), side-emitting laser diodes, vertical-cavity surface-emitting laser diodes (VCSEL), etc., followed by an image beam scanner. The image light 101 provided by the projector 103 within the target FOV 110 is coupled into the substrate 125 by an input optical coupler, such as e.g. an input diffraction grating (IDG) 130 disposed in an input region of the lightguide as illustrated in
In some embodiments, the image projector 103 may project an image spanning up to the target FOV 110 sequentially portion by portion, each image portion carried by the image light in a corresponding FOV portion, e.g. 111, 112, or 113, with the controller 160 adjusting tuning the grating pitch of the IDG 130 and the ODG 140, or at least a segment thereof, for one or more of the FOV portions. In some embodiments, the controller 160 may tune the ODG 140 in dependence on image content being displayed in a current image frame; in some embodiments this may include e.g. deactivating a segment of the ODG 140, i.e. switching off, or at least substantially reducing the diffraction efficiency, of the segment, in dependence on an image content of the image being displayed. In some embodiments, e.g. when the image content is present only in a portion of the target FOV, the controller 160 may switch off, or at least substantially reduce the diffraction efficiency, of a segment of the ODG 140 that is outside of a FOV portion wherein the image content is present. Here “substantially” refers to a reduction by at least a factor of 5.
Referring to
Referring now to
Referring now to
Accordingly, in some embodiments a pupil-replicating lightguide includes a slab substrate for guiding light therein and an output grating supported by the substrate, wherein the output grating has a spatially variant tunable efficiency. The output grating may be controlled to out-couple light by a portion of the output grating to form an image only in a portion of a field of view. Such a pupil-replicating lightguide may be used in an AR display.
In some embodiments, a display apparatus such as those described above may have an output diffraction grating having at least a segment with an electrically tunable grating pitch. In some embodiments, the grating pitch of both the input and output diffraction gratings may be synchronously electrically tunable, e.g. in dependence on a FOV portion being displayed, so that rays of the image light are coupled in and out of the substrate at a same angle, thereby preserving the correspondence between the image FOV at the input coupler and the display FOV at seen from the eyebox, while potentially enhancing at least one of the output uniformity of the display or the FOV supported by the display.
In one embodiment, the lightguide 520 may represent the lightguide 120 of the display apparatus 100 of
By way of example, the display apparatus including the lightguide 520 may be configured so that when at a first time instance an image projector thereof, e.g. the image projector 103 shown in
At a second time instance, the image projector may generate image light 501b confined to the second FOV portion 10 of the FOV 505, as illustrated in
In other embodiments, the lightguide 520 having in-coupling and out-coupling diffraction gratings with a tunable pitch may be operated to display an image sequentially portion by portion, so that different portions of the image corresponding to different partial FOVs are being displayed at different time instances, each time adjusting the grating pitch synchronously in the IDG 530 and the ODG 540, or at least in some portions thereof, depending on the partial FOV being displayed. When the overall target FOV of the image is being scanned over a sufficiently short time, the sequentially displayed FOV portions of the image are integrated by a visual cortex of the viewer into a single image. Using this method, the overall FOV perceived by the viewer may be enhanced.
Referring to
The image projector 603 may be e.g. an LC display panel or another pixelated display configured to project images in the form of two-dimensional (2D) image frames. Each image frame is carried by the image light 601 in an angular domain, spanning a frame FOV 605, which is indicated in
The image projector 603 may project an image frame upon the IDG 630 in a time multiplexed manner, i.e. portion by portion sequentially in time. Each portion may be projected in a corresponding FOV portion of the frame FOV 605 for a fraction of a frame duration T, e.g. for a time interval Δt=T/N, to be perceived by the user as a single image spanning the frame FOV 605; here N is the number of FOV portions being sequentially transmitted per frame. An image processor 670 provides image information for each FOV portion to the projector 603, e.g. in a digital form, sequentially in time so that the whole frame is displayed over the frame duration T One of the image processor 670 and the image projector 603 may also be operatively connected to the controller 660 to provide information indicative of the FOV portion being displayed, with the controller 660 being configured to adjust the grating pitch of the IDG 630 and the ODG 640 as the FOV portion being displayed changes. Since at each moment in time the lightguide 620 conveys at most a portion of the full frame FOV 605, the frame FOV 605 may include an angular range that is broader than the angular range of light of the same color band that could be coupled into the substrate 632 by a diffraction grating with a fixed grating pitch based on the substrate's refractive index.
In an example embodiment illustrated in
The approach described above enables providing a large field of view display with a relatively low-index lightguide, which can potentially reduce the weight and/or cost of the display combiner. Furthermore for scanning displays, the output grating(s) may be synced with the instant scanning angle to improve the efficiency of light utilization.
Example embodiments described above include pupil-replicating or illuminating lightguides incorporating one or more grating structures that have variable, i.e. switchable or continuously tunable, grating pitch, also referred to as grating period, and/or variable diffraction efficiency. Some of such grating structures may have other tunable parameters, e.g. the blazing angle that defines the orientation of the grating grooves, or fringes, relative to the input/output surfaces of the lightguide. Some of such switchable or tunable gratings include a material with electrically tunable refractive index, such as but not exclusively a liquid crystal (LC) medium.
In some embodiments, the material of layer 1043 may contain LC medium, in which case the tunable diffraction grating 1040 may be referred to as an LC grating. The LC medium may include e.g. nematic-type liquid crystals. Nematic liquid crystals may be composed of rod-like molecules that may have non-zero dipole moments and can be approximately aligned by an electrical filed. In another example, the liquid-crystal medium may include cholesteric liquid crystals, in which a molecular stack has a twisted, helical or heliconical structure. The liquid-crystal medium may also include any suitable mixture of nematic liquid crystals, which may have larger, better defined dipole moments and relatively high birefringence, and cholesteric-type liquid crystals, which may have smaller dipole moments but may have the advantage of responding more quickly to changing electric fields. For example, a layer of nematic liquid crystals may be doped with chiral dopants, which may increase the response time of the nematic liquid crystals. The application of an electric field, e.g., by applying a suitable voltage between the electrodes 1041, may orient the dipole moments of LC molecules. For example, the application of an electric field to an LC layer, e.g. layer 1043, may cause the formation of a molecular orientation pattern of the LC molecules, e.g., for nematic liquid crystals, or may modify an existing orientation pattern of the LC molecules, e.g., for cholesteric liquid crystals.
In some embodiments grating 1040 may be an LC grating in which the period of the grating pattern is defined e.g. by pattering a photo-sensitive LC alignment layer, or by a surface relief pattern at an interface between the layer 1043 and a substrate. In the case of tunable surface relief gratings (SRG), LC molecules between the surface relief groves have a different refractive index than the material of the groves. In the absence of the electric field the LC molecules are aligned horizontally, i.e. parallel to the substrate and along the groves, diffracting light polarized along the groves. A voltage applied across the LC layer may align the LC molecules along the electric filed direction, i.e. normally to the layer, thereby substantially eliminating the diffraction.
The surface-relief grating structure 1104 may be polymer-based, e.g. it may be formed from a polymer having an isotropic refractive index np of about 1.5, for example. The LC fluid has an anisotropic refractive index. For light polarization parallel to a director of the LC fluid, i.e. to the direction of orientation of the nematic LC molecules 1110, the LC fluid has an extraordinary refractive index ne, which may be higher than an ordinary refractive index no of the LC fluid for light polarization perpendicular to the director. For example, the extraordinary refractive index ne may be about 1.7, and the ordinary refractive index no may be about 1.5, i.e. matched to the refractive index np of the surface-relief grating structure 1104.
When the voltage Vis not applied (left side of
In some embodiments of the LC surface-relief grating 1100, the surface-relief grating structure 1104 may be formed from an anisotropic polymer with substantially the same or similar ordinary no and extraordinary ne refractive indices as the LC fluid. When the LC director aligns with the optic axis of the birefringent polymer, the refractive index contrast is close to zero at any polarization of impinging light, and there is no diffraction. When the LC director is misaligned with the optic axis of the birefringent polymer e.g. due to application of an external electric field, the refractive index contrast is non-zero for any or most polarizations of the impinging light, and accordingly there is diffraction and beam deflection.
In some embodiments, the grating 1040 may be a holographic polymer-dispersed liquid crystal (H-PDLC) grating that may be manufactured by causing interference between two coherent laser beams in layer 1143, containing a photosensitive monomer/liquid crystal (LC) mixture, between the two electrodes 1041 having a conductive coating. Upon irradiation, a photoinitiator contained within the mixture initiates a free-radical reaction, causing the monomer to polymerize. As the polymer network grows, the mixture phase separates into polymer-rich and liquid-crystal rich regions. The refractive index modulation between the two phases causes light passing through the layer 1143 to be scattered in the case of traditional PDLC2 or diffracted in the case of H-PDLC. When an electric field is applied across the cell, the index modulation is removed and light passing through the cell is unaffected. A description of such tunable diffraction gratings, which may be switched on and off, is provided in an article entitled “Electrically Switchable Bragg Gratings from Liquid Crystal/Polymer Composites” by Pogue et al., Applied Spectroscopy, v. 54 No. 1, 2000, which is incorporated herein by reference in its entirety.
In some embodiments, the grating 1040 may be a polarization volume hologram (PVH) and/or a Pancharatnam—Berry phase (PBP) liquid crystal (LC) grating. Such gratings may be controlled either directly by applying an electric field to the LC layer, or indirectly by providing a serially coupled half-wave plate (HWP). When the electric field is applied to the LC layer, LC molecules are aligned in the electric field, changing effective refractive index, depending on polarization state of the impinging light.
In some embodiments, layer 1043 of the electrically tunable grating 1040 may include a flexoelectric LC. LC molecules typically are electrical dipoles having a non-zero dipole moment, which usually do not exhibit spontaneous polarization because of equal probability for the dipoles to point to two opposite directions respectively, but become polarized in an external electric field. However LC molecules that do not have a perfect rod-shaped structure, but have e.g. a bend-shaped or a pear-shaped structure, may exhibit spontaneous polarization, termed flexoelectric polarization or flexoelectric effect. In materials with a low dielectric anisotropy and a non-zero flexoelectric coefficient difference (e1-e3), where e1 and e3 are the splay and bent flexoelectric coefficients, respectively, electric fields exceeding certain threshold values may result in a transition from the homogeneous planar state to a spatially periodic one, producing a diffraction grating in layer 1043. The field-induced grating is characterized by rotation of the LC director about the alignment axis in the alignment layer(s) adjacent layer 1043, with the wavevector of the grating oriented perpendicular to the initial alignment direction. The rotation sign is defined by both the electric field vector and the sign of the (e1-e3) difference. The wavenumber characterizing the field-induced periodicity is increased linearly with the applied voltage starting from a threshold value of about it/d, where d is the thickness of the layer. Examples of suitable flexoelectric LC materials, and of LC gratings incorporating such materials that may be used in embodiments of the present disclosure, are described in e.g. in an article entitled “Dynamic and Photonic Properties of Field-Induced Gratings in Flexoelectric LC Layers” by Palto in Crystals 2021, 11, 894, and a U.S. Pat. No. 10,890,823, both of which being incorporated herein by reference in their entireties.
In some embodiments, layer 1043 of the electrically tunable grating 1040 having a variable grating period or a slant angle may include helical and helicoidal LC. Cholesteric LCs (CLC), which have intrinsic periodicity in the form of the helical supramolecular structure, may be obtained e.g. by doping the nematic LC matrix with chiral components. The LC molecules in the mixture may self-organize into a periodic helically twisted configuration including helical structures extending between the top and bottom surfaces of the LC layer 1043. Depending on a type of alignment conditions at the layer surfaces, the helical twist axes of the helical structures may be normal to the surfaces or tilt. The helical structures may form a volume grating that acts as a Bragg grating with the Bragg period equal to one half of the distance P, termed cholesteric pitch, along the helical axis where the LC director and the optic axis rotate by 360°. By varying the applied electrical field, the cholesteric pitch P and thus the Bragg period P/2 of the LC grating may be varied. In some embodiments of LC grating, e.g. some of those including a planar-aligned CLC layer, a diffractive pattern may appear when the applied electric field exceeds a threshold, and may vary in amplitude with the applied field, thereby enabling tuning the diffraction efficiency. In some embodiments a tunable LC grating may include oblique helicoidal LCs, in which the LC director is tilted at an oblique angle to the helical axis. Such LC gratings may have superior tunability because the applied electric field may tune the oblique angles and the pitch lengths in a relatively wide range without disturbing the helical axis orientation. Tunable gratings with oblique helicoidal LCs have been described e.g. in an article entitled “Electrooptic Response of Chiral Nematic Liquid Crystals with Oblique Helicoidal Director” by Xiang et al. Phys. Rev. Lett. 112, 217801, 2014, which is incorporated herein by reference in its entirety.
In at least some embodiments, an LC-based grating 1040 such as those described above may be polarization selective. Such gratings may selectively diffract a light beam having a first polarization, e.g. linear or circular, but transmit a light beam having a second, typically orthogonal, polarization with negligible diffraction. In such embodiments, the display apparatuses described above may operate with polarized image light, e.g. to enhance the display's efficiency, and/or may include various polarizers and polarization converters, such as e.g. quarter-wave plates (QWP), half-wave plates (HWP), a-plates, and lightguides incorporating the same.
Tunable diffraction gratings other than LC grating may also be used in the example embodiments described above. In some embodiments, switchable/tunable gratings may be formed on a surface of the lightguide by providing a surface acoustic wave as disclosed e.g. in an article entitled “Status of Leaky Mode Holography” by Smalley et al., Photonics 2021, 8, 29, 2 which is incorporated herein by reference in its entirety. Such diffraction gratings may be tunable in both the grating pitch, by tuning the frequency of the acoustic wave, and the diffraction efficiency, by tuning its amplitude.
Diffraction gratings with a tunable/switchable diffraction efficiency may also be implemented as fluidic gratings. A fluidic grating may include two immiscible fluid layers, like water and oil, whose interface deforms when a spatially inhomogeneous electric field is applied. The spatially inhomogeneous electric field may be provided e.g. by using spatially inhomogeneous and/or discrete electrodes.
Referring to
At least one of the first 1221 and second 1222 electrode structures may be patterned for imposing a spatially variant electric field onto the 1201 and second 1202 fluids. For example, in 12A and 12B, the first electrode 1221 is patterned, and the second electrodes 1222 is not patterned, i.e. the second electrodes 1222 is a backplane electrode. In the embodiment shown, both the first 1221 and second 1222 electrodes are substantially transparent. For example, the first 1221 and second 1222 electrodes may be indium tin oxide (ITO) electrodes.
The application of the spatially variant electric field causes the inter-fluid boundary 1203 to distort as illustrated in
Portions of a patterned electrode may be individually addressable. In some embodiments, the first electrode 1221 may be a continuous, non-patterned electrode coupled to a patterned dielectric layer for creating a spatially non-uniform electric field across the first 1201 and second 1202 fluids. Also in some embodiments, the backplane electrode is omitted, and the voltage is applied between the segmented electrodes themselves.
The thickness of the first 1221 and second 1222 electrodes may be e.g. between 10 nm and 50 nm. The materials of the first 1221 and second 1222 electrodes besides ITO may be e.g. indium zinc oxide (IZO), zinc oxide (ZO), indium oxide (TO), tin oxide (TO), indium gallium zinc oxide (IGZO), etc. The first 1201 and second 1202 fluids may have a refractive index difference of at least 0.1, and may be as high as 0.2 and higher. One of the first 1201 or second 1202 fluids may include polyphenylether, 1,3-bis(phenylthio)benzene, etc. The first 1211 and/or second 1212 substrates may include e.g. fused silica, quartz, sapphire, etc. The first 1211 and/or second 1212 substrates may be straight or curved, and may include vias and other electrical interconnects. The applied voltage may be varied in amplitude and/or duty cycle when applied at a frequency of between 100 Hz and 100 kHz. The applied voltage can change polarity and/or be bipolar. Individual first 1201 and/r second 1202 fluid layers may have a thickness of between 0.5-5 micrometers, more preferably between 0.5-2 micrometer.
To separate the first 1201 and second 1202 fluids, surfactants containing one hydrophilic end functional group and one hydrophobic end functional group may be used. The examples of a hydrophilic end functional group are hydroxyl, carboxyl, carbonyl, amino, phosphate, sulfhydryl. The hydrophilic functional groups may also be anionic groups such as sulfate, sulfonate, carboxylates, phosphates, for example. Non-limiting examples of a hydrophobic end functional group are aliphatic groups, aromatic groups, fluorinated groups. For example, when polyphenyl thioether and fluorinated fluid may be selected as a fluid pair, a surfactant containing aromatic end group and fluronirated end group may be used. When phenyl silicone oil and water are selected as the fluid pair, a surfactant containing aromatic end group and hydroxyl (or amino, or ionic) end group may be used. These are only non-limiting examples.
Referring to
In some embodiments, the method includes coupling, into the lightguide, image light carrying the images in an angular domain, and using an output diffraction grating to couple different FOV portions of the image light out of the lightguide at different time instances. In some embodiments, the method includes selecting the FOV portion being conveyed depending on an image content. In some embodiments, the method includes selecting the FOV portion being conveyed depending on a location of the image content within the target FOV. In some embodiments, the method includes using only a portion of an output area of the output grating to diffract the image light out of the lightguide depending on the FOV portion being conveyed.
In some embodiments, the method includes operating at least a segment of the output diffraction grating to convey, to the eyebox over a frame time interval, the target FOV sequentially portion by portion, at least once during the frame time interval tuning the at least one of the grating pitch or the diffraction efficiency for the FOV portion being displayed.
In some embodiments, the method includes switching the FOV portions being conveyed in synchronization with FOV portions being displayed by an image projector providing the images to the lightguide. In some embodiments, the method includes using a scanning image projector to provide image light carrying the image to an input diffraction grating of the lightguide by sequentially scanning a beam of the image light through different portions of the target FOV over a frame time interval, the input diffraction grating tunable to couple the beam into the lightguide, and tuning a pitch of each of the input diffraction grating and the at least a segment of the output diffraction grating in synchronization with the scanning.
Example embodiments described above have been described by way of example to assist in better understanding of salient features of their operation, and are capable of many variations and modifications. For example in some cases the example embodiments described above may be effective for monochromatic image light. For color images, the image light of different colors may be spatially and/or temporally multiplexed. In some embodiments, two or more stacked lightguides may be used to guide different color channels. In some embodiments, the grating pitch of the input and output couplers of the same lightguide may be tuned to accommodate different color channels in a time multiplexed manner. In at least some embodiments, more than one diffraction grating may be used to couple light out of the lightguide. Some embodiments may utilize more than one input diffraction grating and/or more than one output diffraction gratings, e.g. to support a 2D FOV. When two or more diffraction gratings are used for the in-coupling or the out-coupling, the gratings may be superimposed to form a 2D grating structure, e.g. at a same outer surface of the lightguide's substrate. In other embodiments, different in-coupling gratings or different out-coupling gratings may be disposed at the opposite outer surfaces of the substrate. Embodiments in which one or more input gratings or one or more output gratings are disposed in the bulk of the substrate are also within the scope of the present disclosure. In embodiments where the image light may get diffracted by N≥2 diffraction gratings with grating vectors ki, i=1, . . . , Nin succession, the grating periods of two or more of the diffraction gratings are adjusted so that the grating vectors ki, i=1, . . . , N, sum to zero, i.e. Σ1Nki=0, for every FOV portion being transmitted.
Embodiments of the present disclosure may include, or be implemented in conjunction with, an artificial reality system. An artificial reality system adjusts sensory information about outside world obtained through the senses such as visual information, audio, touch (somatosensation) information, acceleration, balance, etc., in some manner before presentation to a user. By way of non-limiting examples, artificial reality may include virtual reality (VR), augmented reality (AR), mixed reality (MR), hybrid reality, or some combination and/or derivatives thereof. Artificial reality content may include entirely generated content or generated content combined with captured (e.g., real-world) content. The artificial reality content may include video, audio, somatic or haptic feedback, or some combination thereof. Any of this content may be presented in a single channel or in multiple channels, such as in a stereo video that produces a three-dimensional effect to the viewer. Furthermore, in some embodiments, artificial reality may also be associated with applications, products, accessories, services, or some combination thereof, that are used to, for example, create content in artificial reality and/or are otherwise used in (e.g., perform activities in) artificial reality. The artificial reality system that provides the artificial reality content may be implemented on various platforms, including a wearable display such as an HMD connected to a host computer system, a standalone HMD, a near-eye display having a form factor of eyeglasses, a mobile device or computing system, or any other hardware platform capable of providing artificial reality content to one or more viewers.
Referring to
The purpose of the eye-tracking cameras 1404 is to determine position and/or orientation of both eyes of the user. The eyebox illuminators 1406 illuminate the eyes at the corresponding eyeboxes 1412, allowing the eye-tracking cameras 1404 to obtain the images of the eyes, as well as to provide reference reflections i.e. glints. The glints may function as reference points in the captured eye image, facilitating the eye gazing direction determination by determining position of the eye pupil images relative to the glints images. To avoid distracting the user with the light of the eyebox illuminators 1406, the latter may be made to emit light invisible to the user. For example, infrared light may be used to illuminate the eyeboxes 1412.
Turning to
In some embodiments, the front body 1502 includes locators 1508 and an inertial measurement unit (IMU) 1510 for tracking acceleration of the HMD 1500, and position sensors 1512 for tracking position of the HMD 1500. The IMU 1510 is an electronic device that generates data indicating a position of the HMD 1500 based on measurement signals received from one or more of position sensors 1512, which generate one or more measurement signals in response to motion of the HMD 1500. Examples of position sensors 1512 include: one or more accelerometers, one or more gyroscopes, one or more magnetometers, another suitable type of sensor that detects motion, a type of sensor used for error correction of the IMU 1510, or some combination thereof. The position sensors 1512 may be located external to the IMU 1510, internal to the IMU 1510, or some combination thereof.
The locators 1508 are traced by an external imaging device of a virtual reality system, such that the virtual reality system can track the location and orientation of the entire HMD 1500. Information generated by the IMU 1510 and the position sensors 1512 may be compared with the position and orientation obtained by tracking the locators 1508, for improved tracking accuracy of position and orientation of the HMD 1500. Accurate position and orientation is important for presenting appropriate virtual scenery to the user as the latter moves and turns in 3D space.
The HMD 1500 may further include a depth camera assembly (DCA) 1511, which captures data describing depth information of a local area surrounding some or all of the HMD 1500. The depth information may be compared with the information from the IMU 1510, for better accuracy of determination of position and orientation of the HMD 1500 in 3D space.
The HMD 1500 may further include an eye tracking system 1514 for determining orientation and position of user's eyes in real time. The obtained position and orientation of the eyes also allows the HMD 1500 to determine the gaze direction of the user and to adjust the image generated by the display system 1580 accordingly. The determined gaze direction and vergence angle may be used to adjust the display system 1580 to reduce the vergence-accommodation conflict. The direction and vergence may also be used for displays' exit pupil steering as disclosed herein. Furthermore, the determined vergence and gaze angles may be used for interaction with the user, highlighting objects, bringing objects to the foreground, creating additional objects or pointers, etc. An audio system may also be provided including e.g. a set of small speakers built into the front body 1502.
The present disclosure is not to be limited in scope by the specific embodiments described herein. Indeed, other various embodiments and modifications, in addition to those described herein, will be apparent to those of ordinary skill in the art from the foregoing description and accompanying drawings. Thus, such other embodiments and modifications are intended to fall within the scope of the present disclosure. Further, although the present disclosure has been described herein in the context of a particular implementation in a particular environment for a particular purpose, those of ordinary skill in the art will recognize that its usefulness is not limited thereto and that the present disclosure may be beneficially implemented in any number of environments for any number of purposes. Accordingly, the claims set forth below should be construed in view of the full breadth and spirit of the present disclosure as described herein.
This application claims priority from U.S. Provisional Patent Application No. 63/286,349 entitled “Active Gratings in Pupil-Replicated Displays and Illuminators”, and U.S. Provisional Patent Application No. 63/286,230 entitled “Active Fluidic Optical Element”, both filed on Dec. 6, 2021 and incorporated herein by reference in their entireties.
Number | Date | Country | |
---|---|---|---|
63286349 | Dec 2021 | US | |
63286230 | Dec 2021 | US |