Patent Grant
11803003
The present disclosure relates to display systems and, more particularly, to augmented reality display systems comprising diffractive devices based on cholesteric liquid crystal.
Modern computing and display technologies have facilitated the development of systems for so called “virtual reality” or “augmented reality” experiences, in which digitally reproduced images or portions thereof are presented to a user in a manner wherein they seem to be, or may be perceived as, real. A virtual reality, or “VR”, scenario typically involves the presentation of digital or virtual image information without transparency to other actual real-world visual input; an augmented reality, or “AR”, scenario typically involves presentation of digital or virtual image information as an augmentation to visualization of the actual world around the user. A mixed reality, or “MR”, scenario is a type of AR scenario and typically involves virtual objects that are integrated into, and responsive to, the natural world. For example, an MR scenario may include AR image content that appears to be blocked by or is otherwise perceived to interact with objects in the real world.
Referring to
Systems and methods disclosed herein address various challenges related to AR and VR technology.
In a first aspect, an optical device comprises a plurality of waveguides formed over one another and having formed thereon respective diffraction gratings, wherein the respective diffraction gratings are configured to diffract visible light incident thereon into respective waveguides, such that visible light diffracted into the respective waveguides propagates therewithin. The respective diffraction gratings are configured to diffract the visible light incident on the respective waveguides into the respective waveguides within respective field of views (FOVs) with respect to layer normal directions of the respective waveguides. The respective FOVs are such that the plurality of waveguides are configured to diffract the visible light within a combined FOV that is continuous and greater than each of the respective FOVs.
In a second aspect, an optical system comprises a first waveguide having formed thereon a first diffraction grating. The first diffraction grating has a first period and is configured to diffract light having a first color that is incident on the first waveguide within a first FOV. The optical system additionally comprises a second waveguide having formed thereon a second diffraction grating. The second diffraction grating has a second period and is configured to diffract light having the first color that is incident on the second waveguide within a second FOV. The first and second diffraction gratings are configured to diffract the light having the first color within respective field of views (FOVs) into the respective waveguides with respect to layer normal directions of the respective waveguides. The respective FOVs are such that the first and second waveguides are configured to diffract the visible light having the first color within a combined FOV that is continuous and greater than each of the first and second FOVs.
In a third aspect, a display device comprises a first waveguide having formed thereon a first diffraction grating comprising liquid crystals, wherein the first diffraction grating is configured to diffract part of light having a first color incident thereon into the first waveguide. The first diffraction grating is additionally configured to pass therethrough part of the light having the first color incident thereon. The first diffraction grating is further configured to pass therethrough light having a second color. The display device additionally comprises a second waveguide having formed thereon a second diffraction grating comprising liquid crystals, wherein the second diffraction grating is configured to diffract the light having the second color into the second waveguide. The second diffraction grating is further configured to diffract the part of the light having the first color that has passed through the first diffraction grating into the second waveguide.
In a fourth aspect, a head-mounted display device is configured to project light to an eye of a user to display augmented reality image content. The head-mounted display device comprises a frame configured to be supported on a head of the user. The head-mounted display device additionally comprises a display disposed on the frame. At least a portion of the display comprises a plurality of waveguides. The waveguides are transparent and disposed at a location in front of the user's eye when the user wears the head-mounted display device such that the transparent portion transmits light from a portion of an environment in front of the user to the user's eye to provide a view of the portion of the environment in front of the user. The display further comprises one or more light sources and a plurality of diffraction gratings in the display configured to couple light from the light sources into the waveguides in the display. The waveguides and the diffraction gratings in the display comprise the waveguides and the diffraction gratings according to any one of first to third aspects.
Throughout the drawings, reference numbers may be re-used to indicate correspondence between referenced elements. The drawings are provided to illustrate example embodiments described herein and are not intended to limit the scope of the disclosure.
AR systems may display virtual content to a user, or viewer, while still allowing the user to see the world around them. Preferably, this content is displayed on a head-mounted display, e.g., as part of eyewear, that projects image information to the user's eyes. In addition, the display may also transmit light from the surrounding environment to the user's eyes, to allow a view of that surrounding environment. As used herein, it will be appreciated that a “head-mounted” display is a display that may be mounted on the head of a viewer.
With continued reference to
With continued reference to
With reference now to
It will be appreciated, however, that the human visual system is more complicated and providing a realistic perception of depth is more challenging. For example, many viewers of conventional “3-D” display systems find such systems to be uncomfortable or may not perceive a sense of depth at all. Without being limited by theory, it is believed that viewers of an object may perceive the object as being “three-dimensional” due to a combination of vergence and accommodation. Vergence movements (i.e., rotation of the eyes so that the pupils move toward or away from each other to converge the lines of sight of the eyes to fixate upon an object) of the two eyes relative to each other are closely associated with focusing (or “accommodation”) of the lenses and pupils of the eyes. Under normal conditions, changing the focus of the lenses of the eyes, or accommodating the eyes, to change focus from one object to another object at a different distance will automatically cause a matching change in vergence to the same distance, under a relationship known as the “accommodation-vergence reflex,” as well as pupil dilation or constriction. Likewise, a change in vergence will trigger a matching change in accommodation of lens shape and pupil size, under normal conditions. As noted herein, many stereoscopic or “3-D” display systems display a scene using slightly different presentations (and, so, slightly different images) to each eye such that a three-dimensional perspective is perceived by the human visual system. Such systems are uncomfortable for many viewers, however, since they, among other things, simply provide different presentations of a scene, but with the eyes viewing all the image information at a single accommodated state, and work against the “accommodation-vergence reflex.” Display systems that provide a better match between accommodation and vergence may form more realistic and comfortable simulations of three-dimensional imagery.
The distance between an object and the eye 210 or 220 may also change the amount of divergence of light from that object, as viewed by that eye.
Without being limited by theory, it is believed that the human eye typically can interpret a finite number of depth planes to provide depth perception. Consequently, a highly believable simulation of perceived depth may be achieved by providing, to the eye, different presentations of an image corresponding to each of these limited number of depth planes. The different presentations may be separately focused by the viewer's eyes, thereby helping to provide the user with depth cues based on the accommodation of the eye required to bring into focus different image features for the scene located on different depth plane and/or based on observing different image features on different depth planes being out of focus.
With continued reference to
In some embodiments, the image injection devices 360, 370, 380, 390, 400 are discrete displays that each produce image information for injection into a corresponding waveguide 270, 280, 290, 300, 310, respectively. In some other embodiments, the image injection devices 360, 370, 380, 390, 400 are the output ends of a single multiplexed display which may, e.g., pipe image information via one or more optical conduits (such as fiber optic cables) to each of the image injection devices 360, 370, 380, 390, 400. It will be appreciated that the image information provided by the image injection devices 360, 370, 380, 390, 400 may include light of different wavelengths, or colors (e.g., different component colors, as discussed herein).
In some embodiments, the light injected into the waveguides 270, 280, 290, 300, 310 is provided by a light projector system 520, which comprises a light module 530, which may include a light emitter, such as a light emitting diode (LED). The light from the light module 530 may be directed to and modified by a light modulator 540, e.g., a spatial light modulator, via a beam splitter 550. The light modulator 540 may be configured to change the perceived intensity of the light injected into the waveguides 270, 280, 290, 300, 310. Examples of spatial light modulators include liquid crystal displays (LCD) including a liquid crystal on silicon (LCOS) displays.
In some embodiments, the display system 250 may be a scanning fiber display comprising one or more scanning fibers configured to project light in various patterns (e.g., raster scan, spiral scan, Lissajous patterns, etc.) into one or more waveguides 270, 280, 290, 300, 310 and ultimately to the eye 210 of the viewer. In some embodiments, the illustrated image injection devices 360, 370, 380, 390, 400 may schematically represent a single scanning fiber or a bundle of scanning fibers configured to inject light into one or a plurality of the waveguides 270, 280, 290, 300, 310. In some other embodiments, the illustrated image injection devices 360, 370, 380, 390, 400 may schematically represent a plurality of scanning fibers or a plurality of bundles of scanning fibers, each of which are configured to inject light into an associated one of the waveguides 270, 280, 290, 300, 310. It will be appreciated that one or more optical fibers may be configured to transmit light from the light module 530 to the one or more waveguides 270, 280, 290, 300, 310. It will be appreciated that one or more intervening optical structures may be provided between the scanning fiber, or fibers, and the one or more waveguides 270, 280, 290, 300, 310 to, e.g., redirect light exiting the scanning fiber into the one or more waveguides 270, 280, 290, 300, 310.
A controller 560 controls the operation of one or more of the stacked waveguide assembly 260, including operation of the image injection devices 360, 370, 380, 390, 400, the light source 530, and the light modulator 540. In some embodiments, the controller 560 is part of the local data processing module 140. The controller 560 includes programming (e.g., instructions in a non-transitory medium) that regulates the timing and provision of image information to the waveguides 270, 280, 290, 300, 310 according to, e.g., any of the various schemes disclosed herein. In some embodiments, the controller may be a single integral device, or a distributed system connected by wired or wireless communication channels. The controller 560 may be part of the processing modules 140 or 150 (
With continued reference to
With continued reference to
The other waveguide layers 300, 310 and lenses 330, 320 are similarly configured, with the highest waveguide 310 in the stack sending its output through all of the lenses between it and the eye for an aggregate focal power representative of the closest focal plane to the person. To compensate for the stack of lenses 320, 330, 340, 350 when viewing/interpreting light coming from the world 510 on the other side of the stacked waveguide assembly 260, a compensating lens layer 620 may be disposed at the top of the stack to compensate for the aggregate power of the lens stack 320, 330, 340, 350 below. Such a configuration provides as many perceived focal planes as there are available waveguide/lens pairings. Both the out-coupling optical elements of the waveguides and the focusing aspects of the lenses may be static (i.e., not dynamic or electro-active). In some alternative embodiments, either or both may be dynamic using electro-active features.
In some embodiments, two or more of the waveguides 270, 280, 290, 300, 310 may have the same associated depth plane. For example, multiple waveguides 270, 280, 290, 300, 310 may be configured to output images set to the same depth plane, or multiple subsets of the waveguides 270, 280, 290, 300, 310 may be configured to output images set to the same plurality of depth planes, with one set for each depth plane. This can provide advantages for forming a tiled image to provide an expanded field of view at those depth planes.
With continued reference to
In some embodiments, the out-coupling optical elements 570, 580, 590, 600, 610 are diffractive features that form a diffraction pattern, or “diffractive optical element” (also referred to herein as a “DOE”). Preferably, the DOE's have a sufficiently low diffraction efficiency so that only a portion of the light of the beam is deflected away toward the eye 210 with each intersection of the DOE, while the rest continues to move through a waveguide via TIR. The light carrying the image information is thus divided into a number of related exit beams that exit the waveguide at a multiplicity of locations and the result is a fairly uniform pattern of exit emission toward the eye 210 for this particular collimated beam bouncing around within a waveguide.
In some embodiments, one or more DOEs may be switchable between “on” states in which they actively diffract, and “off” states in which they do not significantly diffract. For instance, a switchable DOE may comprise a layer of polymer dispersed liquid crystal, in which microdroplets comprise a diffraction pattern in a host medium, and the refractive index of the microdroplets may be switched to substantially match the refractive index of the host material (in which case the pattern does not appreciably diffract incident light) or the microdroplet may be switched to an index that does not match that of the host medium (in which case the pattern actively diffracts incident light).
In some embodiments, a camera assembly 630 (e.g., a digital camera, including visible light and infrared light cameras) may be provided to capture images of the eye 210 and/or tissue around the eye 210 to, e.g., detect user inputs and/or to monitor the physiological state of the user. As used herein, a camera may be any image capture device. In some embodiments, the camera assembly 630 may include an image capture device and a light source to project light (e.g., infrared light) to the eye, which may then be reflected by the eye and detected by the image capture device. In some embodiments, the camera assembly 630 may be attached to the frame 80 (
With reference now to
In some embodiments, a full color image may be formed at each depth plane by overlaying images in each of the component colors, e.g., three or more component colors.
In some embodiments, light of each component color may be outputted by a single dedicated waveguide and, consequently, each depth plane may have multiple waveguides associated with it. In such embodiments, each box in the figures including the letters G, R, or B may be understood to represent an individual waveguide, and three waveguides may be provided per depth plane where three component color images are provided per depth plane. While the waveguides associated with each depth plane are shown adjacent to one another in this drawing for ease of description, it will be appreciated that, in a physical device, the waveguides may all be arranged in a stack with one waveguide per level. In some other embodiments, multiple component colors may be outputted by the same waveguide, such that, e.g., only a single waveguide may be provided per depth plane.
With continued reference to
It will be appreciated that references to a given color of light throughout this disclosure will be understood to encompass light of one or more wavelengths within a range of wavelengths of light that are perceived by a viewer as being of that given color. For example, red light may include light of one or more wavelengths in the range of about 620-780 nm, green light may include light of one or more wavelengths in the range of about 492-577 nm, and blue light may include light of one or more wavelengths in the range of about 435-493 nm.
In some embodiments, the light source 530 (
With reference now to
The illustrated set 660 of stacked waveguides includes waveguides 670, 680, and 690. Each waveguide includes an associated in-coupling optical element (which may also be referred to as a light input area on the waveguide), with, e.g., in-coupling optical element 700 disposed on a major surface (e.g., an upper major surface) of waveguide 670, in-coupling optical element 710 disposed on a major surface (e.g., an upper major surface) of waveguide 680, and in-coupling optical element 720 disposed on a major surface (e.g., an upper major surface) of waveguide 690. In some embodiments, one or more of the in-coupling optical elements 700, 710, 720 may be disposed on the bottom major surface of the respective waveguide 670, 680, 690 (particularly where the one or more in-coupling optical elements are reflective, deflecting optical elements). As illustrated, the in-coupling optical elements 700, 710, 720 may be disposed on the upper major surface of their respective waveguide 670, 680, 690 (or the top of the next lower waveguide), particularly where those in-coupling optical elements are transmissive, deflecting optical elements. In some embodiments, the in-coupling optical elements 700, 710, 720 may be disposed in the body of the respective waveguide 670, 680, 690. In some embodiments, as discussed herein, the in-coupling optical elements 700, 710, 720 are wavelength selective, such that they selectively redirect one or more wavelengths of light, while transmitting other wavelengths of light. While illustrated on one side or corner of their respective waveguide 670, 680, 690, it will be appreciated that the in-coupling optical elements 700, 710, 720 may be disposed in other areas of their respective waveguide 670, 680, 690 in some embodiments.
As illustrated, the in-coupling optical elements 700, 710, 720 may be laterally offset from one another. In some embodiments, each in-coupling optical element may be offset such that it receives light without that light passing through another in-coupling optical element. For example, each in-coupling optical element 700, 710, 720 may be configured to receive light from a different image injection device 360, 370, 380, 390, and 400 as shown in
Each waveguide also includes associated light distributing elements, with, e.g., light distributing elements 730 disposed on a major surface (e.g., a top major surface) of waveguide 670, light distributing elements 740 disposed on a major surface (e.g., a top major surface) of waveguide 680, and light distributing elements 750 disposed on a major surface (e.g., a top major surface) of waveguide 690. In some other embodiments, the light distributing elements 730, 740, 750, may be disposed on a bottom major surface of associated waveguides 670, 680, 690, respectively. In some other embodiments, the light distributing elements 730, 740, 750, may be disposed on both top and bottom major surface of associated waveguides 670, 680, 690, respectively; or the light distributing elements 730, 740, 750, may be disposed on different ones of the top and bottom major surfaces in different associated waveguides 670, 680, 690, respectively.
The waveguides 670, 680, 690 may be spaced apart and separated by, e.g., gas, liquid, and/or solid layers of material. For example, as illustrated, layer 760a may separate waveguides 670 and 680; and layer 760b may separate waveguides 680 and 690. In some embodiments, the layers 760a and 760b are formed of low refractive index materials (that is, materials having a lower refractive index than the material forming the immediately adjacent one of waveguides 670, 680, 690). Preferably, the refractive index of the material forming the layers 760a, 760b is 0.05 or more, or 0.10 or less than the refractive index of the material forming the waveguides 670, 680, 690. Advantageously, the lower refractive index layers 760a, 760b may function as cladding layers that facilitate total internal reflection (TIR) of light through the waveguides 670, 680, 690 (e.g., TIR between the top and bottom major surfaces of each waveguide). In some embodiments, the layers 760a, 760b are formed of air. While not illustrated, it will be appreciated that the top and bottom of the illustrated set 660 of waveguides may include immediately neighboring cladding layers.
Preferably, for ease of manufacturing and other considerations, the material forming the waveguides 670, 680, 690 are similar or the same, and the material forming the layers 760a, 760b are similar or the same. In some embodiments, the material forming the waveguides 670, 680, 690 may be different between one or more waveguides, and/or the material forming the layers 760a, 760b may be different, while still holding to the various refractive index relationships noted above.
With continued reference to
In some embodiments, the light rays 770, 780, 790 have different properties, e.g., different wavelengths or different ranges of wavelengths, which may correspond to different colors. The in-coupling optical elements 700, 710, 720 each deflect the incident light such that the light propagates through a respective one of the waveguides 670, 680, 690 by TIR. In some embodiments, the in-coupling optical elements 700, 710, 720 each selectively deflect one or more particular wavelengths of light, while transmitting other wavelengths to an underlying waveguide and associated in-coupling optical element.
For example, in-coupling optical element 700 may be configured to deflect ray 770, which has a first wavelength or range of wavelengths, while transmitting rays 1242 and 1244, which have different second and third wavelengths or ranges of wavelengths, respectively. The transmitted ray 780 impinges on and is deflected by the in-coupling optical element 710, which is configured to deflect light of a second wavelength or range of wavelengths. The ray 790 is deflected by the in-coupling optical element 720, which is configured to selectively deflect light of third wavelength or range of wavelengths.
With continued reference to
With reference now to
In some embodiments, the light distributing elements 730, 740, 750 are orthogonal pupil expanders (OPE's). In some embodiments, the OPE's deflect or distribute light to the out-coupling optical elements 800, 810, 820 and, in some embodiments, may also increase the beam or spot size of this light as it propagates to the out-coupling optical elements. In some embodiments, the light distributing elements 730, 740, 750 may be omitted and the in-coupling optical elements 700, 710, 720 may be configured to deflect light directly to the out-coupling optical elements 800, 810, 820. For example, with reference to
Accordingly, with reference to
Stacked Waveguides with Combined Field of View
Providing an immersive experience to a user of waveguide-based display systems, e.g., various semitransparent or transparent display systems configured for virtual/augmented/mixed display applications described supra, depends on, among other things, various characteristics of light coupling into the waveguides of the display systems. For example, virtual/augmented/mixed display having increase field of view can potentially enhance the viewing experience. The field of view of the display depends on the angle of light output by the plurality of waveguides in the waveguides stack that are included in the eyepiece through which the viewer sees images projected into his or her eye. The angle of light output from the plurality of waveguides in turn depends, at least in part, on the acceptance angle of light coupled into the waveguide. As discussed above, in-coupling optical elements such as in-coupling gratings may be employed to couple light into the grating. In certain cases, however, only light having a limited range of angles can be coupled into a given waveguide using a given grating. This limited range of angles of acceptance of light by the waveguide, may also limit the range of angle output by the waveguide into the eye of the wearer, and thus potentially reduce the field of view for the wearer. This particular limitation, as well as designs for increasing the acceptance angle and thus the field of view, of the display are discussed below.
As described supra, e.g., in reference to
To achieve desirable characteristics of in-coupling of light into (or out-coupling of light from) the waveguides 270, 280, 290, 300, 310, the optical elements 570, 580, 590, 600, 610 configured as diffraction gratings can be formed of a material having structures that are configured to control various optical properties, including diffraction properties. The desirable diffraction properties include, among other properties, spectral selectivity, angular selectivity, polarization selectivity, high spectral bandwidth and high diffraction efficiencies, and a wide field of view (FOV), among other properties.
To achieve one or more of these and other advantages, various examples described herein include a plurality of waveguides formed over one another and having formed thereon respective diffraction gratings. The diffraction gratings are configured to diffract visible light incident thereon into respective waveguides, such that visible light diffracted into the waveguides propagates within each of the waveguides, for example, by total internal reflection. The diffraction gratings are configured to diffract the visible light into the respective waveguides when the visible light is incident thereon within respective ranges of angles, or field of views (FOVs) (e.g., with respect to layer normal directions of the respective waveguides). The respective FOVs provided by the individual diffraction gratings and waveguides are such that the waveguides, when stacked together, have an aggregate acceptance angle or FOV that is continuous and greater than the individual FOVs provided by the diffraction gratings and waveguides separately.
As described herein, visible light may include light having one or more wavelengths in various color ranges, including red, green, or blue color ranges. As described herein, red light may include light of one or more wavelengths in the range of about 620-780 nm, green light may include light of one or more wavelengths in the range of about 492-577 nm, and blue light may include light of one or more wavelengths in the range of about 435-493 nm. Thus, visible may include light of one or more wavelengths in the range of about 435 nm-780 nm.
As described herein, structures configured to diffract light, such as diffraction gratings, may diffract light in a transmission mode and/or reflection mode. As described herein, structures that are configured to diffract light in transmission mode refer to structures in which the intensity of diffracted light on the opposite side of the structures as the light-incident side is greater, e.g., at least 10% greater, 20% greater or 30% greater, compared to the intensity of diffracted light on the same side of the structures as the light-incident side. Conversely, structures that are configured to diffract light in reflection mode refer to structures in which the intensity of diffracted light on the same side of the structures as the light-incident side is greater, e.g., at least 10% greater, 20% greater or 30% greater, compared to the intensity of diffracted light on the opposite side of the structures as the light-incident side.
In operation, when an incident light beam 1016, e.g., visible light, is incident on the diffraction grating 1008 at an angle of incidence a measured relative to a plane normal 1012 that is normal or orthogonal to the surface 1008S extending in the y-z plane, the diffraction grating 1008 at least partially diffracts the incident light beam 1016 as a diffracted light beam 1024 at a diffraction angle θ measured relative to the surface normal 1012 and at least partially transmits the incident light as a transmitted light beam 1020. As described herein, a light beam that is incident at an angle in a clockwise direction relative to the plane normal 1012 (i.e., on the right side of the plane normal 1012) as in the illustrated embodiment is referred to as having a negative α (α<0), whereas a light beam that is incident at an angle in a counter-clockwise direction relative to the plane normal 1012 (i.e., on the left side of the plane normal) is referred to as having a positive α (α>0). When the diffracted light beam 1024 is diffracted at a diffraction angle θ that exceeds a critical angle θTIR for occurrence of total internal reflection in the waveguide 1004, the diffracted light beam 1024 propagates in along the x-axis under total internal reflection (TIR) until the diffracted light beam 1024 reaches the optical element 1012, which can correspond to one of light distributing elements (730, 740, 750,
As further described elsewhere in the specification, a suitable combination of the material and the structure of the diffraction grating 1016 may be selected such that a particular range (Δα) of angle of incidence α, referred to herein as a range of angle of acceptance or a field-of-view (FOV), is obtained. According to various embodiments, the diffraction grating 1008 and the waveguide 1004 are arranged such that Δα exceeds 20 degrees (e.g., +/−10 degrees), 30 degrees (e.g., +/−15 degrees), 40 degrees (e.g., +/−20 degrees) or 50 degrees (e.g., +/−25 degrees), or is within a range of angles defined by any of these values, including symmetric and asymmetric ranges about the plane normal 1012, e.g., at 0 degrees. As described herein. the desired range Δα may be described by a range of angles spanning negative and/or positive values of a, outside of which the diffraction efficiency falls off by more than 10%, 25%, more than 50%, or more than 75%, relative to the diffraction efficiency at α=0. Having the Δα within the range in which the diffraction efficiency is relatively high and constant may be desirable, e.g., where a uniform intensity of diffracted light is desired within the Δα. Thus, the Δα is associated with the angular bandwidth of the diffraction grating 1016, such that the incident light beam 1016 within the Aa is efficiently diffracted by the diffraction grating 1016 at a diffraction angle θ with respect to the surface normal 1012 (e.g., the y-z plane) that exceeds θTIR, and that the diffracted light propagates within the waveguide 1004 under total internal reflection (TIR).
In various embodiments, the diffraction grating 1008 (and the optical element 1012) is formed of a material whose refractive index (n1) or an effective refractive index is higher than the refractive index n2 of the waveguide 1004; i.e., n1>n2. In some embodiments, the waveguide 1004 may correspond to the waveguides 310, 300, 290, 280, 270 (
According to certain embodiments, the diffraction grating 1008 may have periodic structures having a period Λa. The period Λa repeats, or substantially repeats, at least twice at regular intervals across the waveguide 1004 in a lateral direction (e.g., x, y directions). In other words, the period Λa may be the distance between identical points of directly neighboring repeating structures. According to various embodiments, the period Λa may correspond to that formed by arrangements of liquid crystals, as described elsewhere in the application. In various embodiments, the Λa may be smaller than the wavelength that the grating 1008 is configured to diffract, and may be smaller than a wavelength, or any wavelength, in the range of about 435 nm-780 nm. In some embodiments configured to diffract at least red light, the Λa may be less than a wavelength (or any wavelength) in the range of about 620-780 nm. In some other embodiments configured to diffract at least green light, the Λa may be less than a wavelength (or any wavelength) in the range of about 492-577 nm. In some other embodiments configured to diffract at least blue light, the Λa may be less than a wavelength (or any wavelength) in the range of about 435-493 nm. Alternatively, according to various embodiments, the Λa may be in the range of 10 nm to 1 μm, including 10 nm to 500 nm or 300 nm to 500 nm. It will be appreciated that the diffraction gratings disclosed herein may be utilized to diffract light and may be part of the display system 250 (
Without being bound to any theory, in some embodiments, the Λa may have a value that is less than a ratio mλ/(sin α+n2 sin θ), where m is an integer (e.g., 1, 2, 3 . . . ) and each of α, n2 and θ has a value described throughout the specification. For example, a may be within the range Δα exceeding 40 degrees, n2 may be in the range of 1-2, and θ may be in the range of 40-80 degrees.
In some embodiments, the Λa may be substantially constant across the surface 1008S of the grating 1008. However, embodiments are not so limited and in some other embodiments, Λa may vary across the surface 1008S.
As described above, the field-of-view (FOV), or Δα, corresponds to a range of angles of incident light that can be coupled into a waveguide and cause TIR. As discussed above, this range of angles can also affect and correspond to the range of angles of light output by the waveguides and the eyepiece and thus affect the field-of-view experienced by the viewer when viewing images through the display. In order to couple incident light into the waveguide and to propagate therewithin under TIR, the light incident on the waveguide 1004 may be directed within the range of acceptance angles or FOV, Δα, which, among other things, is dependent on the refractive index n2 of the material of the waveguide 1004, and the refractive index n1 of the material of the diffraction grating 1008. For example, the FOV (Δα) of a waveguide 1004 comprising a glass substrate with a refractive index of 1.5 can be about 30 degrees. When the gratings are designed to produce a symmetric FOV, the FOV or range of accepted angles for the glass substrate can be within ±15 degrees in one dimension. In the following, various embodiments are described in which a combined range of accepted angles or an effective FOV for a stack of waveguides is extended relative to the individual component waveguides, which may have different and/or smaller FOVs relative to the effective FOV of the stack of waveguides.
As described herein, a combined, aggregate or an effective FOV of a plurality of waveguides, e.g., a stack of waveguides, refers to, for a given color, a range of continuous FOV resulting from the combination of FOVs of the individual waveguides. When the FOVs overlap, the range of continuous FOV include, e.g., can be a sum of, non-overlapping portions of the FOVs of individual waveguides. For example, if a first waveguide having a first diffraction grating formed thereon has α1 from −5 to 20 degrees (i.e., Δα1=25 degrees) for light with a given color, and a second waveguide having a second diffraction grating formed thereon has α2 from −20 to 5 degrees (i.e., Δα2=25 degrees) for the given color, the complementary FOV for the given color from the stack is 40 degrees.
Display devices according to various embodiments include a plurality of waveguides formed over one another and having formed thereon respective diffraction gratings, wherein the diffraction gratings are configured to diffract visible light incident thereon into respective waveguides, such that visible light diffracted into the respective waveguides propagates within each of the respective waveguides to be guided therein by total internal reflection. The diffraction gratings are configured to diffract the visible light into the respective waveguides within different FOVs, with respect to a layer normal direction of the waveguide, where the respective FOVs are such that the waveguides have a combined FOV that is continuous and greater than each of the individual respective FOVs.
In the illustrated embodiment, the first and second waveguides 1004, 1104 are in a stacked arrangement and interposed by a separator 1106, and have substantially parallel directions of propagation (e.g., x-direction) under total internal reflection.
The first and second waveguides 1004, 1104 and the corresponding first and second diffraction gratings 1008, 1012 are similar to each other except, the first and second diffraction gratings 1004, 1108 have different periods Λ1, Λ2, respectively and are configured to diffract light having different wavelength while having the same general color (i.e., red, green, or blue). However, embodiments are not so limited, and the first and second diffraction gratings 1004, 1108 can have substantially the same period and be configured to diffract light having the same wavelength.
Additionally, the first waveguide 1004 coupled to the first diffraction grating 1008 is configured to diffract light having a first, e.g., a positive a (having a counterclockwise angle with respect to the plane normal 1012), whereas the second waveguide 1104 coupled to the second diffraction grating 1108 is configured to diffract light having a different, e.g., a negative a (having a clockwise angle with respect to the plane normal 1012). However, embodiments are not so limited. For example, the first and second waveguides 1004 and 1104 can both be configured to diffract positive or negative but different angles of incidence. Other variations are possible. For example, either of the first and second waveguides 1004 and 1104 can be configured to diffract positive or negative angles or both, and the ranges of angles Δα1 and Δα2 can be the same or different in magnitude.
The first diffraction grating 1008 is configured to partially diffract and to partially transmit visible light 1116, 1124 incident thereon, respectively. In the illustrated embodiment, the first diffraction grating 1008 is configured to partially diffract the visible light 1116 incident thereon within the first FOV (Δα1), and to partially transmit therethrough the visible light 1124 incident thereon within the second FOV (Δα2). The second diffraction grating 1108 is configured to receive light 1128 partially transmitted through the first diffraction grating 1008 as an incident light, and to at least partially diffract the light 1128 into partially diffracted light 1132.
In the illustrated embodiment, the first and second diffraction gratings 1008 and 1108 are configured to diffract light having the same color. That is, each of the first and second diffraction gratings 1008 and 1108 is configured to diffract light having one or more wavelengths in the same color range (red, green, or blue color range) within the wavelength range of about 435 nm-780 nm. In various embodiments, the first and second diffraction gratings 1008 and 1108 can be configured to diffract light having the same or different wavelengths within in the range of about 620-780 nm for red color, to diffract light having the same or different wavelengths within in the range of about 492-577 nm for green color, or to diffract light having the same or different wavelengths within in the range of about range of about 435-493 nm for blue color.
In some embodiments, the first and second diffraction gratings 1008 and 1108 may be configured to diffract particular wavelengths by configuring the respective periods Λ1, Λ2. Without being bound to any theory, under some circumstances, the period A may be generally related to α, n2, θ and λ by the following equation:
Λa(sin α+n2 sin θ)=mλ, [1]
where m is an integer (e.g., 1, 2, 3 . . . ) and α, n2, θ, and λ are angle of incidence, refractive index of the waveguide, angle of the diffracted light and the wavelength of the light, respectively, and may have values described elsewhere in the specification. Other types of diffractive optical element and possible holographic optical element can be used.
Still referring to
Still referring to the illustrated embodiment of
Still referring to
The first diffraction grating 1008 at least partially transmits the incident light 1124 as transmitted light 1128, which in turn becomes incident light on the second diffraction grating 1108 having the second period Λ2 at an angle of incidence α2. The second diffraction grating 1108 in turn at least partially diffracts the light 1128 as diffracted light 1132 at a second diffraction angle θ2. The second waveguide 1104 has a second waveguide index of refraction n2-2 such that when the light 1128 is incident on the surface 11085 within the Δα2, the second wave guide 1104 diffracts the light 1128 at a diffraction angle that exceeds a critical angle θTIR-2 for occurrence of total internal reflection in the waveguide 1104. The resulting diffracted light 1132 propagates along the x-axis under total internal reflection (TIR) until the light reaches the optical element 1112.
Thus, while the first waveguide 1004 having formed thereon the first diffraction grating 1008 and the second waveguide 1104 having formed thereon the first diffraction grating 1108 individually have Δα1 and Δα2, respectively, when stacked as illustrated in the portion of the display device 1100, the resulting stacked waveguides 1004, 1104 have a combined FOV that is continuous and greater than respective FOVs Δα1, Δα2, of the component waveguides 1004, 1104.
In the illustrated embodiment, the diffraction gratings 1008 and 1108 have suitable lengths in the x-direction and partially or fully overlap each other in the x-direction, such that the overlapping portion is sufficient for the incident light 1124 within Δα2 to traverse both the first and second diffraction gratings 1008 and 1108.
In the illustrated embodiment, to have the combined FOV with high diffraction efficiency, it will be appreciated that the first diffraction grating 1008 is configured to diffract the incident light 1116 within the Δα1 with high diffraction efficiency, while being configured to at least partially transmit the incident light 1124, and the second diffraction grating 1108 is configured to diffract its incident light 1128 within the Δα2 with high diffraction efficiency. According to embodiments, the first and second diffraction gratings 1008 and 1108 are configured to diffract incident light 1116 and 1124 within Δα1 and Δα2, respectively, with diffraction efficiency exceeding about 20%, 40%, 60% or 80%, or having a percentage in any range defined by any of these values, according to embodiments. According to embodiments, the first diffraction grating 1008 is configured to transmit the incident light 1124 within the Δα2 with transmission efficiency exceeding about 20%, 40%, 60% or 80% or having a percentage in any range defined by any of these values, according to embodiments.
In some embodiments, Δα1 and Δα2 may partially overlap. According to embodiments, Δα1 and Δα2 overlap by less than 20%, 40%, 60% or 80% or a percentage in any range defined by any of these values, on the basis of Δα1 or Δα2, or by less than 5°, 10°, 15°, or 20° or a value in any range defined by any of these values, according to embodiments.
In one example, the first waveguide 1004 is configured to couple light having α1 from 0 to 30 degrees (i.e., Δα1=30 degrees) and a green wavelength (e.g., 530 nm) into the first waveguide 1004, while the second waveguide 1104 is configured to couple light having the same green wavelength and α2 from −30 to 0 degrees (i.e., Δα2=30 degrees). The resulting combined FOV can be as high as 60 degrees.
Still referring to
However, unlike the display device 1100 illustrated above with respect to
Referring to
Referring to
In summary, referring to
In summary, referring to
Unlike the embodiment illustrated with respect to
In the illustrated embodiment, to configure each of the first and second diffraction gratings 1008 and 1208 to diffract light having one or more wavelengths corresponding to different colors (red, green, or blue), the respective Λ1 and Λ2 may be selected to be different and smaller than the wavelengths the gratings 1008 and 1208 are configured to diffract. Thus, where the first and second diffraction gratings 1008 and 1208 are configured to diffract a green light and a red light, respectively, the Λ1 and Λ2 may be selected to be less than a wavelength (or any wavelength) within different ranges of about 492-577 nm for green color and about 620-780 nm for red color, respectively. In addition, where the first and second diffraction gratings 1008 and 1208 are configured to diffract a blue light and a green light, respectively, the Λ1 and Λ2 may be selected to be less than a wavelength (or any wavelength) within different ranges of about 435-493 nm for blue color and about light 492-577 nm for green color, respectively.
Referring to
The first diffraction grating 1016 at least partially transmits the incident light 1124 incident thereon at an angle of incidence α2 and having the first color and λ1 as a transmitted light 1128, which in turn becomes light 1128 incident on the second diffraction grating 1208 having the second period Λ2. The second diffraction grating 1208 at least partially diffracts the light 1128 incident within the Δα2 as diffracted light 1232 at a second diffraction angle θ2. The second waveguide 1204 has a second waveguide index of refraction n2-2 such that when the light 1128 is incident within the Δα2, the second wave guide 1204 diffracts the light 1128 at a diffraction angle that exceeds a critical angle θTIR-2 for occurrence of total internal reflection in the waveguide 1204. The resulting diffracted light 1232 propagates in along the x-axis under total internal reflection (TIR) until the light reaches the optical element 1212 and exits therethrough.
Referring to
Thus, by stacking the first waveguide 1004 having formed thereon the first diffraction grating 1008 having the first period Λ1, and the second waveguide 1204 having formed thereon the second diffraction grating 1208 having the second period Λ2, the first diffraction grating 1008 is configured to diffract light having the first color and λ1 and within Δα1, the second diffraction grating 1208 is configured to diffract light having the first color and λ1 and within Δα2, and the second diffraction grating 1208 is further configured is configured to diffract light having the second color and λ2 and within at least Δα1. The resulting stack has a combined FOV greater than respective field of views (FOVs) Δα1, Δα2 of the component waveguides 1004, 1204. Also, the second waveguide propagate more than one color potentially reducing the number of waveguides in the stack.
In the illustrated embodiment, referring to
Still referring to
In some embodiments, Δα1 and Δα2 may partially overlap. According to embodiments, Δα1 and Δα2 overlap by less than 20%, 40%, 60% or 80%, or by a percentage within any range defined by any of these values, on the basis of Δα1 or Δα2, or by less than 5°, 10°, 15°, or 20°, or by a value in a range defined by any of these values, according to embodiments.
In one example, the first waveguide 1004 can be configured with the first diffraction grating 1008 having Λ1=380 nm to couple a green light (e.g., 530 nm) having α1 from −5 to 20 degrees (i.e., Δα1=25 degrees) into the first waveguide 1004. The second waveguide 1204 can be configured with the second diffraction grating 1208 having Λ2=465 nm to couple the green light (e.g., 530 nm) having α2 from −20 to 5 degrees (i.e., Δα2=25 degrees) into the second waveguide 1204. The resulting combined FOV is 40 degrees, which is a significant improvement over either Δα1=25 degrees or Δα2=25 degrees. In addition, second waveguide 1204 configured with the second diffraction grating 1208 having Λ2=465 nm can couple red light (e.g., 650 nm) having α1 from −5 to 20 degrees (i.e., Δα1=25 degrees) into the second waveguide 1204. Thus, the stack can be used to project a green-color image (e.g., at 530 nm) having a combined FOV of 40 degrees, as well as a red-color image (e.g., at 650 nm) having an FOV of 25 degrees.
Similar to the display device 1200 illustrated above with respect to
In operation, referring to coupling of light having λ1, when incident light 1116, e.g., visible light each having a first color and λ1, is incident on the first diffraction grating 1008 at an angle of incidence α1, the first diffraction grating 1008 at least partially diffracts the incident light 1116. In particular, the first waveguide 1004 has a first waveguide index of refraction n2-1 such that when the incident light 1116 is incident on its surface within Δα1, the first waveguide 1004 diffracts the incident light 1116 at a diffraction angle that exceeds a critical angle θTIR-1 for occurrence of total internal reflection in the waveguide 1004, such that the diffracted light 1120 propagates along the x-axis under total internal reflection (TIR).
The first diffraction grating 1008 at least partially transmits the incident light 1124 of the first color and λ1 which in turn becomes incident on the second diffraction grating 1208 having the second period Λ2 at an angle of incidence α2. The second diffraction grating 1208 at least partially diffracts the light 1224 of the first color and wavelength within the Δα2 as diffracted light 1232. In particular, the second waveguide 1204 has a second waveguide index of refraction n2-2 such that when the light 1128 of the first color and wavelength is incident on the surface 1208S within the Δα2, the second wave guide 1204 diffracts the light 1124 at a diffraction angle that exceeds a critical angle θTIR-2 for occurrence of total internal reflection in the waveguide 1204, such that the diffracted light 1232 propagates along the x-axis under total internal reflection (TIR).
Referring to coupling of light having λ2, when incident light 1226 and 1224, e.g., visible light having a second color and λ2, is incident on the first diffraction grating 1008, the first diffraction grating 1008 substantially transmits the incident light 1226 and 1224, which in turn becomes incident on the second diffraction grating 1208 at α1 within Δα1 and α2 within Δα2, respectively. The second waveguide 1204 has a second waveguide index of refraction n2-2 such that when the light 1226 of the second color and wavelength is incident on its surface within Δα1, the second wave guide 1204 diffracts the light 1226 of the second color and wavelength at a diffraction angle that exceeds a critical angle θTIR-2 for occurrence of total internal reflection in the second waveguide 1204, such that the diffracted light 1236 of the second color and wavelength propagates along the x-axis under total internal reflection (TIR). On the other hand, the second diffraction grating 1208 substantially transmits the light 1224 of the second color and wavelength, which in turn becomes incident on the third diffraction grating 1308 at α2 within Δα2. The third waveguide 1304 has a third waveguide index of refraction n2-3 such that when the light 1224 of the second color and wavelength is incident on its surface within Δα2, the third wave guide 1304 diffracts the light 1224 of the second color and wavelength at a diffraction angle that exceeds a critical angle θTIR-3 for occurrence of total internal reflection in the third waveguide 1304, such that the diffracted light 1324 of the second color and wavelength propagates along the x-axis under total internal reflection (TIR).
Referring to coupling of light having λ3, when incident light 1316 and 1324, e.g., visible light having a third color and λ3, is incident on the first and second diffraction gratings 1008, 1208, the first and second diffraction gratings 1008, 1208 substantially transmit the incident light 1316 and 1324, which in turn becomes incident on the third diffraction grating 1308 at α1 within Δα1 and α2 within Δα2, respectively. The third waveguide 1304 has a third waveguide index of refraction n2-3 such that when the light 1316 is incident on its surface within the Δα1, the third wave guide 1304 diffracts the light 1316 at a diffraction angle that exceeds a critical angle θTIR-3 for occurrence of total internal reflection in the third waveguide 1304, such that the diffracted light 1328 propagates along the x-axis under total internal reflection (TIR). On the other hand, the third diffraction grating 1308 substantially transmits the light 1324, which in turn becomes incident on the fourth diffraction grating 1408 at α2 within Δα2. The fourth waveguide 1404 has a fourth waveguide index of refraction n2-4 such that when the light 1324 is incident on its surface within the Δα2, the fourth wave guide 1404 diffracts the light 1324 at a diffraction angle that exceeds a critical angle θTIR-4 for occurrence of total internal reflection in the fourth waveguide 1404, such that the diffracted light 1332 propagates along the x-axis under total internal reflection (TIR).
Still referring to
Thus, by stacking the first through fourth waveguides 1004, 1204, 1304, 1404 having formed thereon respective diffraction gratings 1008, 1208, 1308, 1408 having respective periods Λ1, Λ2, Λ3, Λ4, the first waveguide 1004 is configured to diffract light having the first color and λ1 and within Δα1, and the second waveguide 1204 is configured to diffract light having the first color and λ1 and within Δα2, such that a combined FOV greater than respective field of views FOVs Δα1, Δα2 of the component first and second waveguides 1004, 1204, is achieved for light having the first color (e.g., blue) at λ1. Similarly, the second waveguide 1204 is configured to diffract light having the second color and λ2 and within Δα1 and the third waveguide 1304 is configured to diffract light having the second color and λ2 and within Δα2, such that a combined FOV greater than respective field of views FOVs Δα1, Δα2 of the component second and third waveguides 1204, 1304 is achieved for light having the second color (e.g., green) at λ2. Similarly, the third waveguide 1304 is configured to diffract light having the third color and λ2 and within Δα1, and the fourth waveguide 1404 is configured to diffract light having the third color λ3 and within Δα2, such that a combined FOV greater than respective field of views FOVs Δα1, Δα2 of the component third and fourth waveguides 1304, 1404 is achieved for light having the third color (e.g., red) at λ3.
Notably, some waveguides operate on multiple colors and corresponding wavelengths. In some cases, less waveguide are therefore potentially used. The stack may thus be simpler and possibly smaller and lighter and less expensive or at least less complex.
Stacked Waveguides with Combined Field of View Based on Liquid Crystal-Based Diffraction Gratings
As described supra, various embodiments include a plurality of waveguides formed over one another, e.g., in a stacked configuration, and having formed thereon respective diffraction gratings, where the respective diffraction gratings are configured to diffract visible light incident thereon into respective waveguides, such that visible light diffracted into the respective waveguides propagates within each of the respective waveguides. The respective diffraction gratings are configured to diffract the visible light into the respective waveguides within respective field of views (FOVs) with respect to a layer normal direction of the respective waveguide, wherein the respective FOVs are such that the waveguides have a combined FOV that is continuous and greater than each of the respective FOVs. In the following, embodiments of diffraction gratings based on liquid crystals and waveguides having the liquid-crystal diffraction gratings are described. The waveguides and the diffraction gratings are configured to achieve the particular arrangements described above, including wavelength selectivity of diffraction and transmission, as well as their FOV, for forming the stacked waveguides with combined FOVs.
Generally, liquid crystals possess physical properties that may be intermediate between conventional fluids and solids. While liquid crystals are fluid-like in some aspects, unlike most fluids, the arrangement of molecules within liquid crystals exhibits some structural order. Different types of liquid crystals include thermotropic, lyotropic, and polymeric liquid crystals. Thermotropic liquid crystals disclosed herein can be implemented in various physical states, e.g., phases, including a nematic state/phase, a smectic state/phase, a chiral nematic state/phase or a chiral smectic state/phase.
As described herein, liquid crystals in a nematic state or phase can have calamitic (rod-shaped) or discotic (disc-shaped) organic molecules that have relatively little positional order, while having a long-range directional order with their long axes being roughly parallel. Thus, the organic molecules may be free to flow with their center of mass positions being randomly distributed as in a liquid, while still maintaining their long-range directional order. In some implementations, liquid crystals in a nematic phase can be uniaxial; i.e., the liquid crystals have one axis that is longer and preferred, with the other two being roughly equivalent. In other implementations, liquid crystals can be biaxial; i.e., in addition to orienting their long axis, the liquid crystals may also orient along a secondary axis.
As described herein, liquid crystals in a smectic state or phase can have the organic molecules that form relatively well-defined layers that can slide over one another. In some implementations, liquid crystals in a smectic phase can be positionally ordered along one direction. In some implementations, the long axes of the molecules can be oriented along a direction substantially normal to the plane of the liquid crystal layer, while in other implementations, the long axes of the molecules may be tilted with respect to the direction normal to the plane of the layer.
Herein and throughout the disclosure, nematic liquid crystals are composed of rod-like molecules with the long axes of neighboring molecules approximately aligned to one another. To describe this anisotropic structure, a dimensionless unit vector n called the director, may be used to describe the direction of preferred orientation of the liquid crystal molecules.
Herein and throughout the disclosure, a tilt angle or a pre-tilt angle 1 can refer to an angle measured in a plane perpendicular to a major surface (in an x-y plane) of the liquid crystal layers or of the substrate, e.g., the x-z plane, and measured between an alignment direction and the major surface or a direction parallel to the major surface, e.g., the x-direction.
Herein and throughout the disclosure, an azimuthal angle or a rotation angle φ is used to describe an angle of rotation about a layer normal direction, or an axis normal to a major surface of a liquid crystal layer, which is measured in a plane parallel to a major surface of the liquid crystal layers or of the substrate, e.g., the x-y plane, and measured between an alignment direction, e.g., an elongation direction or the direction of the director, and a direction parallel to the major surface, e.g., the y-direction.
Herein and throughout the disclosure, when an angle such as the rotation angle φ or a pre-tilt angle Φ are referred to as being substantially the same between different regions, it will be understood that an average alignment angles can, for example, be within about 1%, about 5% or about 10% of each other although the average alignment can be larger in some cases.
Herein and throughout the specification, a duty cycle can, for example, refers to a ratio between a first lateral dimension of a first region having liquid crystal molecules aligned in a first alignment direction, and the grating period of the zone having the first region. Where applicable, the first region corresponds to the region in which the alignment of the liquid crystals does not vary between different zones.
As describe herein, liquid crystals in a nematic state or a smectic state can also exhibit chirality. Such liquid crystals are referred to as being in a chiral phase or a cholesteric phase. In a chiral phase or a cholesteric phase, the liquid crystals can exhibit a twisting of the molecules perpendicular to the director, with the molecular axis parallel to the director. The finite twist angle between adjacent molecules is due to their asymmetric packing, which results in longer-range chiral order.
As described herein, liquid crystals in a chiral smectic state or phase can be configured such that the liquid crystal molecules have positional ordering in a layered structure, with the molecules tilted by a finite angle with respect to the layer normal. In addition, chirality can induce successive azimuthal twists of the liquid crystal molecules with respect to a direction perpendicular to the layer normal from one liquid crystal molecule to the next liquid crystal molecule in the layer normal direction, thereby producing a spiral twisting of the molecular axis along the layer normal.
As described herein and throughout the disclosure, a chiral structure refers to a plurality of liquid crystal molecules in a cholesteric phase that extend in a direction, e.g., a direction perpendicular to the director such as a layer depth direction, and are successively rotated or twisted in a rotation direction, e.g., clockwise or counterclockwise. In one aspect, the directors of the liquid crystal molecules in a chiral structure can be characterized as a helix having a helical pitch.
As described herein, liquid crystals in a cholesteric phase displaying chirality can be described as having a chiral pitch, or a helical pitch (p), which corresponds to a length in the layer depth direction corresponding to a net rotation angle of the liquid crystal molecules of the chiral structures by one full rotation in the first rotation direction. In other words, the helical pitch refers to the distance over which the liquid crystal molecules undergo a full 360° twist. The helical pitch (p) can change, e.g., when the temperature is altered or when other molecules are added to a liquid crystal host (an achiral liquid host material can form a chiral phase if doped with a chiral material), allowing the helical pitch (p) of a given material to be tuned accordingly. In some liquid crystal systems, the helical pitch is of the same order as the wavelength of visible light. As described herein, liquid crystals displaying chirality can also be described as having a twist angle, or a rotation angle (ϕ), which can refer to, for example, the relative azimuthal angular rotation between successive liquid crystal molecules in the layer normal direction, and as having a net twist angle, or a net rotation angle, which can refer to, for example, the relative azimuthal angular rotation between an uppermost liquid crystal molecule and a lowermost liquid crystal molecule across a specified length, e.g., the length of a chiral structure or the thickness of the liquid crystal layer.
According to various embodiments described herein, liquid crystals having various states or phases as described above can be configured to offer various desirable material properties, including, e.g., birefringence, optical anisotropy, and manufacturability using thin-film processes. For example, by changing surface conditions of liquid crystal layers and/or mixing different liquid crystal materials, grating structures that exhibit spatially varying diffraction properties, e.g., gradient diffraction efficiencies, can be fabricated.
As described herein, “polymerizable liquid crystals” may refer to liquid crystal materials that can be polymerized, e.g., in-situ photopolymerized, and may also be described herein as reactive mesogens (RM).
It will be appreciated that the liquid crystal molecules may be polymerizable in some embodiments and, once polymerized, may form a large network with other liquid crystal molecules. For example, the liquid crystal molecules may be linked by chemical bonds or linking chemical species to other liquid crystal molecules. Once joined together, the liquid crystal molecules may form liquid crystal domains having substantially the same orientations and locations as before being linked together. For ease of description, the term “liquid crystal molecule” is used herein to refer to both the liquid crystal molecules before polymerization and to the liquid crystal domains formed by these molecules after polymerization.
According to particular embodiments described herein, photo-polymerizable liquid crystal materials can be configured to form Bragg-reflective structures, e.g., a diffraction grating, whose material properties, including birefringence, chirality, and ease for multiple-coating, can be utilized to create diffraction gratings with different material properties, e.g., birefringence, chirality, and thickness, which can result in different optical properties, e.g., diffraction efficiency, wavelength selectivity and off-axis diffraction angle selectivity, to name a few.
Optical properties of a grating are determined by the physical structures of the grating (e.g., the periodicity, the depth, and the duty cycle), as well as material properties of the grating (e.g., refractive index, absorption, and birefringence). When liquid crystals are used, optical properties of the grating can be controlled by controlling, e.g., molecular orientation or distribution of the liquid crystal materials. For example, by varying molecular orientation or distribution of the liquid crystal material across the grating area, the grating may exhibit graded diffraction efficiencies. Such approaches are described in the following, in reference to the figures.
In the following, various embodiments of cholesteric liquid crystal diffraction gratings (CLCGs) that are optimized for various optical properties are described. Generally, diffraction gratings have a periodic structure, which splits and diffracts light into several beams travelling in different directions. The directions of these beams depend, among other things, on the period of the periodic structure and the wavelength of the light. To optimize certain optical properties, e.g., diffraction efficiencies, for certain applications such as in-coupling optical elements (1008, 1208 in
As described supra, liquid crystal molecules of a cholesteric liquid crystal (CLC) layer in a chiral (nematic) phase or a cholesteric phase is characterized by a plurality of liquid crystal molecules that are arranged to have successive azimuthal twists of the director as a function of position in the film in a normal direction, or a depth direction, of the liquid crystal layer. As described herein, the liquid crystal molecules that arranged to have the successive azimuthal twists are collectively referred to herein as a chiral structure. As described herein, an angle (ϕ) of azimuthal twist or rotation is described as the angle between the directors the liquid crystal molecules, as described supra, relative to a direction parallel to the layer normal. The spatially varying director of the liquid crystal molecules of a chiral structure can be described as forming a helical pattern in which the helical pitch (p) is defined as the distance (e.g., in the layer normal direction of the liquid crystal layer) over which the director has rotated by 360°, as described above. As described herein, a CLC layer configured as a diffraction grating has a lateral dimension by which the molecular structures of the liquid crystals periodically repeat in a lateral direction normal to the depth direction. This periodicity in the lateral direction is referred to as a grating period (Λ).
According to various embodiments described herein, a diffraction grating comprises a cholesteric liquid crystal (CLC) layer comprising a plurality of chiral structures, wherein each chiral structure comprises a plurality of liquid crystal molecules that extend in a layer depth direction by at least a helical pitch and are successively rotated in a first rotation direction. The helical pitch is a length in the layer depth direction corresponding to a net rotation angle of the liquid crystal molecules of the chiral structures by one full rotation in the first rotation direction. The arrangements of the liquid crystal molecules of the chiral structures vary periodically in a lateral direction perpendicular to the layer depth direction
Without being bound to any theory, under a Bragg-reflection condition, the wavelength of the incident light (λ) may be proportional to the mean or average refractive index (n) of a CLC layer and to the helical pitch (p), and can be expressed as satisfying the following condition under some circumstances:
λ≈np [2]
In addition, the bandwidth (Δλ) of Bragg-reflecting wavelengths may be proportional to the birefringence Δn (e.g., the difference in refractive index between different polarizations of light) of CLC layer and to the helical pitch (p), and can be expressed as satisfying the following condition under some circumstances:
Δλ=Δn·p [3]
In various embodiments described herein, the bandwidth Δλ is about 60 nm, about 80 nm or about 100 nm.
According to various embodiments, a peak reflected intensity within a visible wavelength range between, e.g., about 390 nm and about 700 nm, or within a near infrared wavelength range between, e.g., about 700 nm and about 2500 nm, can exceed about 60%, about 70%, about 80% or about 90%. In addition, according to various embodiments, the full width at half maximum (FWHM) can be less than about 100 nm, less than about 70 nm, less than about 50 nm or less than about 20 nm.
n·sin(θ)=λ/Λ+sin(θinc), [4]
where θinc is the incident angle relative to the direction of layer normal, θ is the reflection angle relative to the direction of layer normal and n is a reflective index of a medium in which the reflected beam propagates. When the CLC layer 1158 is illuminated with the incident beam 1216 at an off-axis angle, the reflection spectrum may be shifted toward shorter wavelengths. According to various embodiments disclosed herein, the ratio λ/Λ can have a value between 0.5 and 0.8, between 0.6 and 0.9, between 0.7 and 1.0, between 0.8 and 1.1, between 0.9 and 1.2, between 1.0 and 1.6, between 1.1 and 1.5, or between 1.2 and 1.4.
Without being bound to any theory, the off-axis angle at which the CLC layer 1158 is configured to Bragg-reflect with high efficiency can also depend on the helical pitch p of the chiral structures.
Referring to
As illustrated, the second CLC layer 1358B is configured such that when a second incident light beam 1316B is directed to an incident surface of the CLC layer 1358B at a second off-axis angle θinc,2 different from the first off-axis angle θinc,1 a second reflected light beam 1320B having a second reflection angle θ2 different from the first reflection angle θ1 is generated As illustrated, the CLC layer 1358B is further configured to have a second range 1324B of off-axis angles, similar to the first range 1324A described above with respect to
As described supra, for various applications including in-coupling and out-coupling of light, a wave guide device can be configured to propagate light by total internal reflection (TIR).
sin(θC)=1/nt [5]
where nt is the refractive index of the waveguide 1604. According to various embodiments, nt may be between about 1 and about 2 between about 1.4 and about 1.8 or between about 1.5 and about 1.7. For example, the waveguide may comprise a polymer such as polycarbonate or a glass.
Thus, as described above with respect to
As described above with respect to
Additional Aspects
In a 1st example, an optical device comprises a plurality of waveguides formed over one another and having formed thereon respective diffraction gratings, wherein the respective diffraction gratings are configured to diffract visible light incident thereon into respective waveguides, such that visible light diffracted into the respective waveguides propagates therewithin. The respective diffraction gratings are configured to diffract the visible light into the respective waveguides within respective field of views (FOVs) with respect to layer normal directions of the respective waveguides. The respective FOVs are such that the plurality of waveguides are configured to diffract the visible light within a combined FOV that is continuous and greater than each of the respective FOVs.
In a 2nd example, in the optical device of the 1st example, the plurality of waveguides are formed of a material whose refractive index is smaller than an effective refractive index of the respective diffraction gratings, such that the visible light diffracted into the respective waveguides propagates therewithin under total internal reflection.
In a 3rd example, in the optical device of the 1st or 2nd examples, the plurality of waveguides are in a stacked arrangement and are configured to propagate the visible light in substantially parallel directions under total internal reflection.
In a 4th example, in the optical device of the 1st to 3rd examples, wherein different ones of the respective diffraction gratings are disposed to overlap each other in a lateral direction perpendicular to the layer normal directions.
In a 5th example, in the optical device of any one of the 1st to 4th examples, different ones of the respective FOVs do not overlap by more than 20% on the basis of a sum of the different ones of the respective FOVs.
In a 6th example, in the optical device of any one of the 1st to 5th examples, the plurality of waveguides includes a first waveguide having formed thereon a first diffraction grating configured to partially diffract and to partially transmit the visible light incident thereon, and includes a second waveguide having formed thereon a second diffraction grating configured to at least partially diffract the transmitted visible light from the first diffraction grating incident thereon.
In a 7th example, in the optical device of the 6th example, the first and second diffraction gratings have different periods and are configured to diffract visible light having different wavelengths while having the same color.
In an 8th example, in the optical device of the 6th example, the first and second diffraction gratings have substantially the same period and are configured to diffract visible light having substantially the same wavelength.
In a 9th example, in the optical device of the 6th example, the first and second diffraction gratings have different periods and are configured to diffract visible light having different wavelengths and different colors.
In a 10th example, in the optical device of the 9th example, the first diffraction grating has a first period and is configured to diffract visible light having a first color, and the second grating has a second period and is configured to diffract visible light having the first color and visible light having a second color.
In an 11th example, in the optical device of the 10th example, the first color corresponds to a shorter wavelength compared to the second color.
In a 12th example, in the optical device of the 10th or 11th examples, the first diffraction grating is configured to partially diffract visible light having the first color incident thereon within a first FOV, and to partially transmit the visible light having the first color incident thereon within a second FOV, and the second diffraction grating is configured to at least partially diffract the visible light having the first color partially transmitted through the first diffraction grating.
In a 13th example, in the optical device of the 12th example, the first diffraction grating is configured to substantially transmit the visible light having the second color, and the second diffraction grating is configured to at least partially diffract the visible light having the second color incident within the first FOV.
In a 14th example, in the optical device of the 13th example, the optical device further comprises a third waveguide having formed thereon a third diffraction grating having a third period and configured to diffract visible light having a third color, wherein the second color corresponds to a shorter wavelength compared to the third color.
In a 15th example, in the optical device of the 14th example, the second diffraction grating is configured to at least partially transmit the visible light having the second color, and the third diffraction grating is configured to receive and to at least partially diffract within the second FOV the partially transmitted visible light having the second color from the second diffraction grating.
In a 16th example, in the optical device of the 15th example, the first and second diffraction gratings are configured to substantially transmit the visible light having the third color, and the third diffraction grating is configured to at least partially diffract within the first FOV the visible light having the third color that is transmitted through the first and second diffraction gratings.
In a 17th example, an optical system comprises a first waveguide having formed thereon a first diffraction grating. The first diffraction grating has a first period and is configured to diffract light having a first color and incident on the first waveguide within a first FOV. The optical system additionally comprises a second waveguide having formed thereon a second diffraction grating. The second diffraction grating has a second period and is configured to diffract light having the first color and incident on the second waveguide within a second FOV. The first and second diffraction gratings are configured to diffract the light having the first color within respective field of views (FOVs) into the respective waveguides with respect to layer normal directions of the respective waveguides. The respective FOVs are such that the first and second waveguides are configured to diffract the visible light having the first color within a combined FOV that is continuous and greater than each of the first and second FOVs.
In an 18th example, in the optical system of the 17th example, the first waveguide and the second waveguide are in a stacked configuration, the first waveguide is configured to receive the light having the first color prior to the second waveguide, and the first period is shorter than the second period.
In a 19th example, in the optical system of the 18th example, the second diffraction grating is configured to diffract the light having the first color within the second FOV after substantially transmitting through the first diffraction grating without substantially diffracting.
In a 20th example, in the optical system of the 19th example, the first diffraction grating is configured to substantially transmit therethrough without substantially diffracting the light having the second color, wherein the light having the second color has a longer wavelength compared to the light having the first color.
In a 21st example, in the optical system of the 20th example, the second diffraction grating is configured to diffract the light having the second color within the second FOV to be guided in the waveguide.
In a 22nd example, in the optical system of the 17th example, each of the first and second diffraction gratings comprises a cholesteric liquid crystal (CLC) layer.
In a 23rd example, in the optical system of the 20th example, the CLC layer comprises a plurality of chiral structures, wherein each chiral structure comprises a plurality of liquid crystal molecules that extend in a layer depth direction by at least a helical pitch and are successively rotated in a first rotation direction. The helical pitch is a length in the layer depth direction corresponding to a net rotation angle of the liquid crystal molecules of the chiral structures by one full rotation in the first rotation direction. Arrangements of the liquid crystal molecules of the chiral structures vary periodically in a lateral direction perpendicular to the layer depth direction.
In a 24th example, in the optical system of the 20th example, each chiral structure comprises at least three calamitic liquid crystal molecules that are elongated along different elongation directions.
In a 25th example, a display device comprises a first waveguide having formed thereon a first diffraction grating comprising liquid crystals, wherein the first diffraction grating is configured to diffract part of light having a first color incident thereon into the first waveguide. The first diffraction grating is additionally configured to pass therethrough part of the light having the first color incident thereon. The first diffraction grating is further configured to pass therethrough light having a second color. The display device additionally comprises a second waveguide having formed thereon a second diffraction grating comprising liquid crystals, wherein the second diffraction grating is configured to diffract the light having the second color into the second waveguide. The second diffraction grating is further configured to diffract the part of the light having the first color that has passed through the first diffraction grating.
In a 26th example, in the display device of the 25th example, first diffraction grating is configured diffract light having the first color within a first range of angles of incidence relative to a layer normal, and the first diffraction grating is configured to pass therethrough the light having the first color within a second range of angles of incidence relative to the layer normal.
In a 27th example, in the display device of the 26th example, the second diffraction grating is configured diffract the light having the second color incident thereon within the first range of angles, and the second diffraction grating is configured to diffract the light having the first color incident thereon within the second range of angles of incidence
In a 28th example, in the display device of the 27th example, the first range of angles and the second range of angles do not overlap by more than 20% on the basis of a sum of the first range of angles and the second range of angles.
In a 29th example, in the display device of any one of the 25th to 28th examples, the first color corresponds to a shorter wavelength compared to the second color.
In a 30th example, in the display device of any one of the 25th to 29th examples, the first diffraction grating comprises periodically varying liquid crystals arranged to have a first period in a lateral direction, and the second diffraction grating comprises periodically varying liquid crystals arranged to have a second period in the lateral direction greater than the first period.
In a 31st example, in the display device of the 30th example, one or both of the first diffraction grating and the second diffraction grating are configured to diffract light having a wavelength and has a period in a lateral direction such that a wavelength/period ratio (λ/Λ) is between about 0.3 and 2.3.
In a 32nd example, in the display device of the 30th example, one or both of the first diffraction grating and the second diffraction grating are configured to diffract light having a wavelength and has a period such that the period is less than the wavelength by 1 nm to 250 nm.
In a 33rd example, in the display device of any one of the 25th to 32nd examples, the liquid crystals comprise cholesteric liquid crystals.
In a 34th example, in the display device of the 33rd example, the liquid crystals of the first diffraction grating has a helical pitch smaller than that of the liquid crystals of the second diffraction grating.
In a 35th example, in the display device of any one of the 25th to 34th examples, one or both of the first diffraction grating and the second diffraction grating are configured to diffract light into the respective waveguides transmissively.
In a 36th example, in the display device of any one of the 25th to 34th examples, one or both of the first diffraction grating and the second diffraction grating are configured to diffract light into the respective waveguides reflectively.
In a 37th example, in the display device of any one of the 25th to 36th examples, the first color is green and the second color is red.
In a 38th example, in the display device of any one of the 25th to 36th examples, the first color is blue and the second color is green.
In a 39th example, a head-mounted display device is configured to project light to an eye of a user to display augmented reality image content. The head-mounted display device comprises a frame configured to be supported on a head of the user. The head-mounted display device additionally comprises a display disposed on the frame. At least a portion of the display comprises a plurality of waveguides. The waveguides are transparent and disposed at a location in front of the user's eye when the user wears the head-mounted display device such that the transparent portion transmits light from a portion of an environment in front of the user to the user's eye to provide a view of the portion of the environment in front of the user. The display further comprises one or more light sources and a plurality of diffraction gratings in the display configured to couple light from the light sources into the waveguides in the display. The waveguides and the diffraction gratings in the display comprise the waveguides and the diffraction gratings according to any one of 1st to 38th examples.
In a 40th example, in the device of the 39th example, the one or more light sources comprises a fiber scanning projector.
In a 41st example, in the device of the 39th or 40th examples, the display is configured to project light into the user's eye so as to present image content to the user on a plurality of depth planes.
Additional Considerations
In the embodiments described above, augmented reality display systems and, more particularly, spatially varying diffraction gratings are described in connection with particular embodiments. It will be understood, however, that the principles and advantages of the embodiments can be used for any other systems, apparatus, or methods with a need for the spatially varying diffraction grating. In the foregoing, it will be appreciated that any feature of any one of the embodiments can be combined and/or substituted with any other feature of any other one of the embodiments.
Unless the context clearly requires otherwise, throughout the description and the claims, the words “comprise,” “comprising,” “include,” “including” and the like are to be construed in an inclusive sense, as opposed to an exclusive or exhaustive sense; that is to say, in the sense of “including, but not limited to.” The word “coupled”, as generally used herein, refers to two or more elements that may be either directly connected, or connected by way of one or more intermediate elements. Likewise, the word “connected”, as generally used herein, refers to two or more elements that may be either directly connected, or connected by way of one or more intermediate elements. Additionally, the words “herein,” “above,” “below,” “infra,” “supra,” and words of similar import, when used in this application, shall refer to this application as a whole and not to any particular portions of this application. Where the context permits, words in the above Detailed Description using the singular or plural number may also include the plural or singular number, respectively. The word “or” in reference to a list of two or more items, that word covers all of the following interpretations of the word: any of the items in the list, all of the items in the list, and any combination of one or more of the items in the list. In addition, the articles “a,” “an,” and “the” as used in this application and the appended claims are to be construed to mean “one or more” or “at least one” unless specified otherwise.
As used herein, a phrase referring to “at least one of” a list of items refers to any combination of those items, including single members. As an example, “at least one of: A, B, or C” is intended to cover: A, B, C, A and B, A and C, B and C, and A, B, and C. Conjunctive language such as the phrase “at least one of X, Y and Z,” unless specifically stated otherwise, is otherwise understood with the context as used in general to convey that an item, term, etc. may be at least one of X, Y or Z. Thus, such conjunctive language is not generally intended to imply that certain embodiments require at least one of X, at least one of Y and at least one of Z to each be present.
Moreover, conditional language used herein, such as, among others, “can,” “could,” “might,” “may,” “e.g.,” “for example,” “such as” and the like, unless specifically stated otherwise, or otherwise understood within the context as used, is generally intended to convey that certain embodiments include, while other embodiments do not include, certain features, elements and/or states. Thus, such conditional language is not generally intended to imply that features, elements and/or states are in any way required for one or more embodiments or whether these features, elements and/or states are included or are to be performed in any particular embodiment.
While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the disclosure. Indeed, the novel apparatus, methods, and systems described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the methods and systems described herein may be made without departing from the spirit of the disclosure. For example, while blocks are presented in a given arrangement, alternative embodiments may perform similar functionalities with different components and/or circuit topologies, and some blocks may be deleted, moved, added, subdivided, combined, and/or modified. Each of these blocks may be implemented in a variety of different ways. Any suitable combination of the elements and acts of the various embodiments described above can be combined to provide further embodiments. The various features and processes described above may be implemented independently of one another, or may be combined in various ways. No element or combinations of elements is necessary or indispensable for all embodiments. All suitable combinations and subcombinations of features of this disclosure are intended to fall within the scope of this disclosure.
This application is a divisional of U.S. patent application Ser. No. 15/926,920 filed on Mar. 20, 2018 entitled “STACKED WAVEGUIDES HAVING DIFFERENT DIFFRACTION GRATINGS FOR COMBINED FIELD OF VIEW,” which claims the priority benefit of U.S. Provisional Patent Application No. 62/474,529 filed on Mar. 21, 2017 entitled “STACKED WAVEGUIDES HAVING DIFFERENT DIFFRACTION GRATINGS FOR COMBINED FIELD OF VIEW,” which are incorporated by reference herein in their entirety.
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| Number | Date | Country | |
|---|---|---|---|
| 20220155525 A1 | May 2022 | US |
| Number | Date | Country | |
|---|---|---|---|
| 62474529 | Mar 2017 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | 15926920 | Mar 2018 | US |
| Child | 17590482 | US |
