Optical systems including light-guide optical elements with two-dimensional expansion

Information

  • Patent Grant
  • 11448816
  • Patent Number
    11,448,816
  • Date Filed
    Tuesday, April 20, 2021
    3 years ago
  • Date Issued
    Tuesday, September 20, 2022
    a year ago
Abstract
An optical system including a light-guide optical element (LOE) with first and second sets (204, 206) of mutually-parallel, partially-reflecting surfaces at different orientations. Both sets of partially-reflecting surfaces are located between parallel major external surfaces. A third set of at least partially-reflecting surfaces (202), deployed at the coupling-in region, receive image illumination injected from a projector (2) with an optical aperture having a first in-plane width and direct the image illumination via reflection of at least part of the image illumination at the third set of at least partially-reflective facets towards the first set of partially-reflective facets with an effective optical aperture having a second width larger than the first width.
Description
FIELD AND BACKGROUND OF THE INVENTION

The present invention relates to optical systems and, in particular, it concerns an optical system including a light-guide optical element (LOE) for achieving optical aperture expansion.


Many near-eye display systems include a transparent light-guide optical element (LOE) or “waveguide” placed before the eye of the user, which conveys an image within the LOE by internal reflection and then couples out the image by a suitable output coupling mechanism towards the eye of the user. The output coupling mechanism may be based on embedded partial reflectors or “facets”, or may employ a diffractive pattern. The description below will refer primarily to a facet-based coupling-out arrangement, but it should be appreciated that various features of the invention are also applicable to diffractive arrangements.


Two-dimensional aperture expansion within a waveguide employing internal orthogonal facets was described in FIG. 13 of U.S. Pat. No. 6,829,095 B2, which is reproduced here as FIG. 1A. Reference numerals referring to the prior art drawings are presented here in parentheses. Light from projector (20) propagates within the waveguide and is reflected by facets (22a)-(22c) towards facets (23), which couple the light out towards an observer.


PCT publication WO 2019/142177 A1 discloses a similar concept employing non-orthogonal facets. FIGS. 2 and 29 of the PCT publication are reproduced here as FIGS. 1B and 1C, respectively. The first set of facets, here denoted (32), are non-orthogonal, so only one mode of propagation is reflected. The two configurations illustrated differ as to whether the regions containing the two sets of facets are overlapping (FIG. 1B) or non-overlapping (FIG. 1C).


SUMMARY OF THE INVENTION

The present invention is an optical system.


According to the teachings of an embodiment of the present invention there is provided, an optical system for directing image illumination injected at a coupling-in region towards a user for viewing, the optical system comprising a light-guide optical element (LOE) formed from transparent material, the LOE comprising: (a) a first region containing a first set of planar, mutually-parallel, partially-reflecting surfaces having a first orientation; (b) a second region containing a second set of planar, mutually-parallel, partially-reflecting surfaces having a second orientation non-parallel to the first orientation; (c) a set of mutually-parallel major external surfaces, the major external surfaces extending across the first and second regions such that both the first set of partially-reflecting surfaces and the second set of partially-reflecting surfaces are located between the major external surfaces, wherein the second set of partially-reflecting surfaces are at an oblique angle to the major external surfaces so that a part of image illumination propagating within the LOE by internal reflection at the major external surfaces from the first region into the second region is coupled out of the LOE towards the user, and wherein the first set of partially-reflecting surfaces are oriented so that a part of image illumination propagating within the LOE by internal reflection at the major external surfaces from the coupling-in region is deflected towards the second region, wherein the optical system further comprises a third set of planar, mutually-parallel, at least partially-reflecting surfaces deployed at the coupling-in region, the third set of at least partially-reflecting surfaces being deployed to receive image illumination injected from a projector with an optical aperture having a first width measured parallel to the major external surfaces and to direct the image illumination via reflection of at least part of the image illumination at the third set of at least partially-reflective facets towards the first set of partially-reflective facets with an effective optical aperture having a second width measured parallel to the major external surfaces, the second width being larger than the first width.


According to a further feature of an embodiment of the present invention, the third set of at least partially-reflecting surfaces has a first sequence of successively-increasing reflectivities in an order in which the image illumination reaches them, and wherein the first set of partially-reflecting surfaces has a second sequence of successively-increasing reflectivities in an order in which the image illumination reaches them, the second sequence starting at a reflectivity smaller than a last reflectivity of the first sequence.


According to a further feature of an embodiment of the present invention, a last reflectivity of the first sequence of successively-increasing reflectivities is greater than 90%.


According to a further feature of an embodiment of the present invention, a majority of the image illumination directed towards the first set of partially-reflecting surfaces undergoes exactly one reflection from the third set of at least partially-reflecting surfaces.


According to a further feature of an embodiment of the present invention, a majority of the image illumination directed towards the first set of partially-reflecting surfaces undergoes two reflections from the third set of at least partially-reflecting surfaces.


According to a further feature of an embodiment of the present invention, the third set of at least partially-reflecting surfaces are integrated as part of the LOE and located between the major external surfaces.


According to a further feature of an embodiment of the present invention, the third set of at least partially-reflecting surfaces are parallel to the first set of partially-reflecting surfaces.


According to a further feature of an embodiment of the present invention, the third set of at least partially-reflecting surfaces are non-parallel to the first set of partially-reflecting surfaces.


According to a further feature of an embodiment of the present invention, an inter-surface spacing of the third set of at least partially-reflecting surfaces is smaller than an inter-surface spacing of the first set of partially-reflecting surfaces.


According to a further feature of an embodiment of the present invention, a surface area of each at least partially-reflecting surface of the third set of at least partially-reflecting surfaces is smaller than a surface area of each partially-reflecting surface of the first set of partially-reflecting surfaces.


According to a further feature of an embodiment of the present invention, the first region and the second region are non-overlapping.


According to a further feature of an embodiment of the present invention, there is also provided an image projector for projecting a collimated image having an angular field of view about an optical axis, the image projector being optically coupled to the LOE so as to introduce the collimated image into the LOE via the third set of at least partially-reflecting surfaces at the coupling-in region as a propagating image propagating within the LOE by internal reflection at the major external surfaces, the propagating image being partially reflected by the first set of partially-reflecting surfaces to generate a deflected propagating image propagating within the LOE by internal reflection at the major external surfaces, the deflected propagating image being partially reflected by the second set of partially-reflecting surfaces to generate a coupled-out image directed outwards from one of the major external surfaces towards the user.





BRIEF DESCRIPTION OF THE DRAWINGS

The invention is herein described, by way of example only, with reference to the accompanying drawings, wherein:



FIG. 1A, discussed above, corresponds to FIG. 13 of U.S. Pat. No. 6,829,095 B2;



FIGS. 1B and 1C, discussed above, correspond to FIGS. 2 and 29 of PCT Patent Application Publication No. WO 2019/142177 A1, respectively;



FIGS. 2A and 2B are schematic isometric views of an optical system implemented using a light-guide optical element (LOE), constructed and operative according to the teachings of the present invention, illustrating a top-down and a side-injection configuration, respectively;



FIGS. 3A and 3B are schematic illustrations of the effects of different spacing of partially-reflecting internal surfaces on redirection of image illumination from a projector with a given optical aperture width from a first direction to a second direction within a substrate;



FIG. 4A is a schematic front view of a light-guide optical element (LOE) according to the teachings of an embodiment of the present invention, illustrating three-stage expansion of an optical aperture from a projector to illumination coupled-out towards a viewer;



FIGS. 4B and 4C are schematic isometric representations of two implementations of the LOE of FIG. 4A using partially-reflecting internal surfaces that are orthogonal and oblique, respectively, for the first two stages of aperture expansion;



FIGS. 5A and 5B are schematic front and isometric views, respectively, of a variant implementation of the LOE of FIG. 4A in which partially-reflecting internal surfaces for performing two stages of optical aperture expansion are deployed in regions which are at least partially overlapping;



FIG. 6 is a schematic representation in angular space (polar coordinates) of the relative directions of the image illumination through various stages of propagation through the LOE of FIG. 4C;



FIGS. 7A and 7B are schematic front views of two further variant implementations of the LOE of FIG. 4A illustrating options for lateral injection of image illumination;



FIG. 8A is a schematic representation of a production sequence for the LOE of FIG. 4A;



FIG. 8B is a schematic representation of a production sequence for the LOE of FIG. 5A;



FIG. 9 is a schematic front view of a further variant implementation of the LOE of FIG. 4A in which the geometrical form of the LOE regions is modified;



FIGS. 10A and 10B are schematic front and isometric views, respectively, of a further variant implementation of the LOE of FIG. 4A employing a rectangular waveguide section for a preliminary stage of optical aperture expansion;



FIGS. 11A and 11B are schematic isometric views before and after assembly, respectively, of a further variant implementation of the LOE of FIG. 4A employing a slab with internal at least partially-reflecting facets for a preliminary stage of optical aperture expansion without light guiding by TIR; and



FIGS. 12A and 12B are schematic isometric views before and after assembly, respectively, of a further variant implementation of the LOE of FIG. 4A employing a slab with internal at least partially-reflecting facets for a preliminary stage of optical aperture expansion with light guiding by surfaces non-parallel with the major surfaces of the LOE.





DESCRIPTION OF THE PREFERRED EMBODIMENTS

Certain embodiments of the present invention provide an optical system including a light-guide optical element (LOE) for achieving optical aperture expansion for the purpose of a head-up display, such as a near-eye display, which may be a virtual reality display, or more preferably an augmented reality display.


An exemplary implementation of a device in the form of a near-eye display, generally designated 10, employing an LOE 12 according to the teachings of an embodiment of the present invention, is illustrated schematically in FIGS. 2A and 2B. The near-eye display 10 employs a compact image projector (or “POD”) 14 optically coupled so as to inject an image into LOE (interchangeably referred to as a “waveguide,” a “substrate” or a “slab”) 12 within which the image light is trapped in one dimension by internal reflection at a set of mutually-parallel planar external surfaces. The light impinges of a set of partially-reflecting surfaces (interchangeably referred to as “facets”) that are parallel to each other, and inclined obliquely to the direction of propagation of the image light, with each successive facet deflecting a proportion of the image light into a deflected direction, also trapped/guided by internal reflection within the substrate. This first set of facets are not illustrated individually in FIGS. 2A and 2B, but are located in a first region of the LOE designated 16. This partial reflection at successive facets achieves a first dimension of optical aperture expansion.


In a first set of preferred but non-limiting examples of the present invention, the aforementioned set of facets are orthogonal to the major external surfaces of the substrate. In this case, both the injected image and its conjugate undergoing internal reflection as it propagates within region 16 are deflected and become conjugate images propagating in a deflected direction. In an alternative set of preferred but non-limiting examples, the first set of partially-reflecting surfaces are obliquely angled relative to the major external surfaces of the LOE. In the latter case, either the injected image or its conjugate forms the desired deflected image propagating within the LOE, while the other reflection may be minimized, for example, by employing angularly-selective coatings on the facets which render them relatively transparent to the range of incident angles presented by the image whose reflection is not needed.


The first set of partially-reflecting surfaces deflect the image illumination from a first direction of propagation trapped by total internal reflection (TIR) within the substrate to a second direction of propagation, also trapped by TIR within the substrate.


The deflected image illumination then passes into a second substrate region 18, which may be implemented as an adjacent distinct substrate or as a continuation of a single substrate, in which a coupling-out arrangement (either a further set of partially reflective facets or a diffractive optical element) progressively couples out a proportion of the image illumination towards the eye of an observer located within a region defined as the eye-motion box (EMB), thereby achieving a second dimension of optical aperture expansion. The overall device may be implemented separately for each eye, and is preferably supported relative to the head of a user with the each LOE 12 facing a corresponding eye of the user. In one particularly preferred option as illustrated here, a support arrangement is implemented as an eye glasses frame with sides 20 for supporting the device relative to ears of the user. Other forms of support arrangement may also be used, including but not limited to, head bands, visors or devices suspended from helmets.


It is a particularly preferred feature of certain embodiments of the present invention that the optical system further includes a third set of planar, mutually-parallel, at least partially-reflecting surfaces (“facets”) deployed at the coupling-in region. The third set of facets are not shown individually in FIGS. 2A and 2B, but are designated by region 15. The third set of facets are deployed to receive image illumination injected from projector 14 with an optical aperture having a first width measured parallel to the major external surfaces of the LOE 12 and to direct the image illumination via reflection of at least part of the image illumination by the facets in region 15 towards the first set of partially-reflective facets in region 16 with an effective optical aperture having a second, larger width measured parallel to the major external surfaces of the LOE. The significance of this aperture expansion will be discussed further below.


The third set of facets 15 are interposed in the optical path between projector 14 and first set of facets 16 at the coupling region. The phrase “at the coupling region” is used herein to encompass both a case in which the third set of facets are incorporated into the LOE at the coupling region and where the third set of facets are external to the LOE, with both of these options being exemplified in detail below.


Reference is made herein in the drawings and claims to an X axis which extends horizontally (FIG. 2A) or vertically (FIG. 2B), in the general extensional direction of the first region of the LOE, and a Y axis which extends perpendicular thereto, i.e., vertically in FIG. 2A and horizontally in FIG. 2B.


In very approximate terms, the first LOE, or first region 16 of LOE 12, may be considered to achieve aperture expansion in the X direction while the second LOE, or second region 18 of LOE 12, achieves aperture expansion in the Y direction. It should be noted that the orientation as illustrated in FIG. 2A may be regarded as a “top-down” implementation, where the image illumination entering the main (second region) of the LOE enters from the top edge, whereas the orientation illustrated in FIG. 2B may be regarded as a “side-injection” implementation, where the axis referred to here as the Y axis is deployed horizontally. In the remaining drawings, the various features of certain embodiments of the present invention will be illustrated in the context of a “top-down” orientation, similar to FIG. 2A. However, it should be appreciated that all of those features are equally applicable to side-injection implementations, which also fall within the scope of the invention. In certain cases, other intermediate orientations are also applicable, and are included within the scope of the present invention except where explicitly excluded.


The POD employed with the devices of the present invention is preferably configured to generate a collimated image, i.e., in which the light of each image pixel is a parallel beam, collimated to infinity, with an angular direction corresponding to the pixel position. The image illumination thus spans a range of angles corresponding to an angular field of view in two dimensions.


Image projector 14 includes at least one light source, typically deployed to illuminate a spatial light modulator, such as an LCOS chip. The spatial light modulator modulates the projected intensity of each pixel of the image, thereby generating an image. Alternatively, the image projector may include a scanning arrangement, typically implemented using a fast-scanning mirror, which scans illumination from a laser light source across an image plane of the projector while the intensity of the beam is varied synchronously with the motion on a pixel-by-pixel basis, thereby projecting a desired intensity for each pixel. In both cases, collimating optics are provided to generate an output projected image which is collimated to infinity. Some or all of the above components are typically arranged on surfaces of one or more polarizing beam-splitter (PBS) cube or other prism arrangement, as is well known in the art.


Optical coupling of image projector 14 to LOE 12 may be achieved by any suitable optical coupling, such as for example via a coupling prism with an obliquely angled input surface, or via a reflective coupling arrangement, via a side edge and/or one of the major external surfaces of the LOE. Where third set of facets 15 is external to the LOE, the third set of facets are preferably integrated with the coupling-in arrangement, as will be exemplified below with reference to FIGS. 11A-11C, below. Further details of the coupling-in configuration are not critical to the invention, and are shown here only schematically.


It will be appreciated that the near-eye display 10 includes various additional components, typically including a controller 22 for actuating the image projector 14, typically employing electrical power from a small onboard battery (not shown) or some other suitable power source. It will be appreciated that controller 22 includes all necessary electronic components such as at least one processor or processing circuitry to drive the image projector, all as is known in the art.


Turning now to FIGS. 3A and 3B, this illustrates schematically the geometry of image illumination from a projector having a certain width of optical aperture with the first set of partially-reflecting internal surfaces. In order to obtain uniform light illumination, the width of the projector's aperture 100 must be such that the reflected rays from one facet are contiguous with the reflected rays from the next facet to avoid black lines in the display. In some cases, it is desirable that there is sufficient overlap that each viewing direction receives a reflection from two or more facets, and most preferably from a constant number of facets across the aperture, thereby enhancing uniformity of the viewed image. FIGS. 3A and 3B illustrate cases in which different number of facets (102 and 109) are illuminated by a beam from projector 2 with aperture width 100. The reflected light (104, 106, 110 and 108) propagates toward the other facets (not shown in this figure). Preferably a complete and constant number of facets are illuminated. In FIG. 3A the number varies between 2 and 3, while in FIG. 3B it is constant, with two facets contributing to the output across the entire aperture. The wider the aperture 100, the more facets are illuminated the more uniform is the image transmitted.


For a predefined facet spacing the aperture width must be modified accordingly to generate a uniform image. A large facet spacing therefore dictates use of a large aperture. Tight spacing of facets across waveguide increases production complexity and cost. On the other hand, producing a large aperture projector increases projector size. These conflicting design considerations are reconciled according to an aspect of the present invention by performing a preliminary stage of optical aperture expansion between the projector and what was referred to above as the first set of facets. This is achieved using an additional set of facets (referred to herein as the “third set of at least partially-reflecting internal surfaces”).



FIG. 4A shows schematically a front view of a waveguide according to this aspect of the present invention. The aperture of projector 2 is small. The two arrows originating from this projector represent light rays of the edges of this aperture. The light from this projector is coupled into waveguide section 200 having facets 202 (which are the preliminary, additional and “third” set of facets). As the light propagates in this section 200, its lateral aperture dimension (“width”) in the plane of the LOE expands as it is partially redirected by reflections from successive facets 202 towards section 207 that includes facets 204 (referred to above as the “first” set of facets). The light reflected from facets 204 is redirected towards section 209 that includes facets 206 (referred to above as the “second” set of facets), to be coupled out towards the viewer.



FIG. 4B shows isometric view of FIG. 4A. Here it can be seen that the section 200 has same width (waveguide thickness) as 207 and 209, so that sections 200, 207 and 209 are integrated within a contiguous LOE, sandwiched between mutually-parallel external surfaces. The guidance throughout these sections is by total internal reflection (TIR) from these external surfaces. The transmission of light between the sections is preferably without disturbance or discontinuity, and the separating lines shown between the sections in various views (e.g., the front views of FIGS. 4A, 5A, 7A, 7B and 9) is for ease of understanding.


Facets 206 are designed to transmit scenery light, allowing the viewer a direct view of an external scene beyond the LOE, and therefore have relatively low reflectivity, typically below 50%. In some configurations facets 204 are also designed to transmit scenery light, and therefore also have relatively low reflectivity, typically below 50%. In other configurations where facets 204 are not part of the “viewing area” of the LOE, higher reflectivities may be used. Facets 202 preferably are outside the viewing area of the LOE and therefore do not need to transmit scenery. High reflectivity is therefore preferably used in order to obtain high efficiency of light transmission. Preferably, the last facet 211 in region 200 has a high reflectivity of at least 90%, and preferably 100% reflectivity. Since section 200 is not designed to transmit scenery light, it is preferably covered (not shown) so no external light passes through it. Alternatively, this section 200 of the waveguide is coated with reflective coating such as silver.


In order to provide relatively uniform image illumination intensity across the optical aperture, one or more of the sets of partially-reflecting surfaces, and preferably each set, most preferably has a sequence of successively-increasing reflectivities in an order in which the image illumination reaches them. By way of example, for waveguide region 200, a sequence of 3 facets having 33%, 50% and 100% reflectivity are effective to reflect roughly a third of the incident illumination from each successive surface. Similar for a sequence of 4 facets, 25%, 33%, 50% and 100% values are effective to reflect roughly a quarter of the incident illumination from each surface. For facets which are within a viewing area through which the viewer observes an external scene, the reflectivity values are lower, and the proportional increase between facets is smaller, but the underlying concept of the increasing sequence to compensate for a lower proportion of illumination intensity remaining within the propagating image illumination remains the same. (Where the ideal reflectivity values for successive facets are relatively close, two or more successive facets in a region of the LOE may be implemented with the same reflectivity value as a manufacturing simplification, but the sequence is still referred to as “successively increasing” since it is monotonically increasing, to provide the above effect of enhanced uniformity.) Thus, for example, facets 204 have a second sequence of successively-increasing reflectivities in an order in which the image illumination reaches them, where the second sequence starts at a reflectivity smaller than a last reflectivity of the first sequence (of facets 204).


In the configuration of FIG. 4A, a majority of the image illumination directed towards facets 204 undergoes exactly one reflection from facets 202. The spacing of the facets 202 is close, ensuring continuity of the image illumination redirected towards facets 204 across an expanded effective aperture, as illustrated by the bounding arrows shown in LOE section 207. This allows the use of a larger spacing for facets 204, thereby reducing production complexity and costs for the larger portion of the waveguide. For, example if the facets 202 expand the aperture by a factor of 3 (using 3 facets with progressive increasing reflectivity) then facets 204 can have roughly three times the spacing compared without section 200. In more general terms, the spacing of facets 204 is typically larger than the spacing of facets 202. Additionally, the surface area of facets 202 is typically smaller than that of facets 204. As a result, only a relatively small volume of closely-spaced facets needs to be produced, while complexity and production costs for the majority of the LOE structure are reduced.



FIG. 4B shows facets in sections 200 and 207 to be perpendicular to the major external surfaces of the waveguide. FIG. 4C shows an alternative implementation according to which the facets of both sections 200 and 207 of the waveguide are at an oblique angle to the major surfaces of the LOE, referred to here as “twisted facets”.



FIGS. 5A and 5B are analogous to FIGS. 4A and 4C, but illustrate that facets 204 and 206 may optionally be implemented in at least partially overlapping regions of the waveguide, in a manner analogous to the corresponding options taught in WO 2019/142177 A1, referred to above. The input aperture expansion section 200 is preferably implemented so as to span a majority, and preferably the full thickness, of the LOE, as shown in FIG. 5B.



FIG. 6 illustrates the image reflections for the facets in angular space. This description is for twisted facets as described in FIG. 4C and in FIG. 5. The light is coupled into waveguide 200 as 1930A into one of images 6L or 6R. These two images represent back and forth TIR reflection from the major surfaces of the LOE as the image illumination propagates along aperture expansion section 200. Reflection by facets 202 is represented as 1938 onto 4R and 4L. These are the images propagating by TIR along section 207. In this non-limiting but particularly preferred configuration, facets 202 are parallel to facets 204, so the reflection by facets 204 towards section 209 is also along 1938 from 4R to 6L. Here 6L and 6R also represent images propagating along section 209. In other words, the images propagating in section 200 and 209 are here the same in angular space. The reflection by facets 206 within section 209 coupling out towards the observer is represented as 1934 from guided image 6R to output coupled image 8.


Circles 39 represent the TIR cutoff of the waveguide and are parallel to the plane of the waveguide. It is apparent the images 4L and 4R are diagonal to the plane of the waveguide, i.e., with the sides of the rectangular image in angular space parallel and perpendicular to the major surfaces of the substrate, while images 6L and 6R are aligned parallel to the surfaces of the waveguide. Practically it is typically more convenient to construct a projector 2 for parallel coupling in than for diagonal. As a result, coupling in through waveguide section 200 contributes to simplicity of the projector implementation, and can therefore be of advantage even via a small number of high-reflectivity facets that do not necessarily significantly expand the effective optical aperture of the projector.


Ergonomic consideration could dictate injection the image from the side of the waveguide, as shown in FIGS. 7A and 7B. In this case, a first facet 210 is advantageously implemented with a high reflectivity in order to achieve approximate uniformity between the image illumination transmitted by the first facet and that reflected by the subsequent facets. For example, if only two facets exist in section 200, the first facet will have 50% reflectivity and the second 100%. However, if there are four facets then the first will have 75% reflectivity (25% transmittance), the second 33%, the third 50% and the last (210) 100%. Alternatively, facet 210 may be implemented with 100% so that all transmission into section 207 is from the subsequent facets.


The configuration presented in FIG. 7A is based on coupling in from 1930B (referring to the angular space illustration of FIG. 6) onto facet 210 that reflects 1938 to 6L. Further propagation is as described before.



FIG. 7B shows an equivalent configuration where the facets in section 200 are at an opposite orientation to enable different position of the projector 2.


In the side-injection cases, the first facet 210 functions primarily as a coupling-in facet, and is an exception to the successively-increasing reflectivities of facets along the sequence of facets, with the “sequence” beginning from the second facet. In these cases, a majority of the image illumination directed towards facets 204 undergoes two reflections from facets 202.



FIG. 8A illustrates schematically a method for integrating a waveguide with sections as described in FIGS. 4A-4C. A set of coated plates 253 is glued together to form a stack 254 and sliced 255a to generate the facet section required for section 207. A set of coated plates 250 is glued together to form a stack 251 and sliced diagonally to generate the facet section required for section 209, shown as 252a, and a third set of coated plates 256 is glued together to form a stack 257 which is sliced to generate section 258a (the facets required for section 200). The three sections are combined 260a and glued 262a. The glue is index matched to the waveguide so minimal perturbation introduced to the light as it passes between the sections. A thin cover glass 264 is preferably glued on both sides of the waveguide, and optionally further polished, to generate waveguide 266a having smooth parallel TIR surfaces.



FIG. 8B shows a similar manufacturing process suitable for the architecture described in FIGS. 5A and 5B. Sections 252b, 255b and 258b are produced in the same manner as shown in FIG. 8A, but where 258b is twice the thickness as the others. 252b and 255b are stacked while 258B is placed from the side as shown in 260b. The sections are glued together 262b and transparent cover glasses 264 are glued as covers, optionally with further polishing, to generate a single waveguide 266b.


If it is desired to incorporate two overlapping sets of facets within a single layer, this may be done according to the technique explained in the above-referenced WO 2019/142177 A1 with reference to FIG. 11, where the resulting waveguide section containing two sets of facets is combined with the section 258b (corresponding to the facets of section 200) attached to the side prior to addition of the cover sheets.


Although shown thus far as rectangular waveguide sections, it should be noted that the shape of the sections can change according to the propagation of the guided light. By way of one non-limiting example, depending on the geometry of the image propagation, expanding of the image illumination within the waveguide may in some cases require broadening of sections 200 and 207 along the propagation path, resulting in a waveguide form as illustrated in FIG. 9.


Although illustrated thus far as an integrated part of an LOE guided in one dimension, the preliminary stage of aperture expansion may optionally be implemented in various additional configurations which are unguided, guided on different axes, or guided in two dimensions, as will now be exemplified by the non-limiting examples of FIGS. 10A-12B.


In the non-limiting example of FIGS. 10A and 10B, section 200 is implemented as a rectangular waveguide section 270 which guides the image illumination in two dimensions during the preliminary aperture expansion, prior to injection of the expanded aperture image illumination into waveguide section 107. An air gap 295 or some optical layer emulating an air gap is preferably provided to maintain internal reflection within waveguide section 270 except where coupled out. Examples of such 2D waveguide structures may be found in U.S. Pat. No. 10,133,070 and will not be described here in detail.



FIGS. 11A and 11B illustrate a further option according to which the coupling-in aperture expansion facets are provided without guiding of the image illumination by TIR. In this case, facets 202 are provided in a first section 280 which is wider than the rest of the waveguide 207. In this configuration, the light in 280 is unguided and propagates through 280 while expanding in both dimensions. In this configuration the coupling into waveguide 207 is preferably achieved via a coupling prism 285. FIG. 11A shows 280 separated from 285 for clarity. The angled orientation of 280 and coupling prism 285 facilitate uniform illumination along the thickness (vertical as shown) dimension of 207. FIG. 11B shows 280 after attachment to coupling-in prism 285.



FIG. 12A shows a further variant implementation according to which the first stage of aperture expansion via facets 202 is provided in a first section 290 that is guided in one dimension that is not parallel to waveguide 207. FIG. 12B shows placement of section 290 on top of a coupling prism 285 where an air-gap 295 is provided in order to preserve TIR guidance within section 290.


In all respects other than those explicitly described here, the arrangement of first set of partially-reflecting internal surfaces 204 and the second set of partially-reflecting internal surfaces 206 within a common waveguide may be implemented according to the range of options described in parallel PCT patent application no. PCT/M2019/157572, which is unpublished as of the filing date of this application and does not constitute prior art.


In all of the front views illustrated herein, the aperture expansion of the present invention is represented schematically by parallel arrows indicating the span of the optical aperture for a given ray direction corresponding to a central pixel on the optical axis of a collimated image. The optical axis is not actually within the X-Y plane, but rather has a Z-component into the page chosen such that the entire range of angles in the depth dimension of the field of view (FOV) undergo total internal reflection at the major substrate surfaces. For simplicity of presentation, the graphic representations herein, and the description thereof, relate only to the in-plane (X-Y) component of the light ray propagation directions, referred to herein as the “in-plane component” or the “component parallel to the major external surfaces of the LOE.”


As mentioned above in the context of FIG. 3B, all of the above principles can also be applied to “sideway” configurations, where an image is injected from a POD located laterally outside the viewing area and is spread by a first set of facets vertically and then by a second set of facets horizontally for coupling into the eye of the user. All of the above-described configurations and variants should be understood to be applicable also in a side-injection configuration.


Throughout the above description, reference has been made to the X axis and the Y axis as shown, where the X axis is either horizontal or vertical, and corresponds to the first dimension of the optical aperture expansion, and the Y axis is the other major axis corresponding to the second dimension of expansion. In this context, X and Y can be defined relative to the orientation of the device when mounted on the head of a user, in an orientation which is typically defined by a support arrangement, such as the aforementioned glasses frame of FIGS. 3A and 3B.


Although the invention has been illustrated thus far in the context of a preferred but non-limiting example of a near-eye display, it should be noted that embodiments of various aspects of the invention may be used to advantage in other application including, but not limited to, head-up displays (HUDs). One subset of HUDs of particular interest are HUDs for vehicles.


It will be appreciated that the above descriptions are intended only to serve as examples, and that many other embodiments are possible within the scope of the present invention as defined in the appended claims.

Claims
  • 1. An optical system for directing image illumination from an image projector towards a user for viewing, the optical system comprising: (a) an image projector for projecting a collimated image having an angular field of view about an optical axis, said collimated image having a projector optical aperture;(b) a light-guide optical element (LOE) formed from transparent material, said LOE comprising: (i) a first region containing a first set of planar, mutually-parallel, partially-reflecting surfaces having a first orientation;(ii) a second region containing a second set of planar, mutually-parallel, partially-reflecting surfaces having a second orientation non-parallel to said first orientation;(iii) a set of mutually-parallel major external surfaces, said major external surfaces extending across said first and second regions such that both said first set of partially-reflecting surfaces and said second set of partially-reflecting surfaces are located between said major external surfaces; and(iv) a coupling-in surface having a coupling-in optical aperture, said coupling-in surface being positioned such that a collimated image introduced via said coupling-in surface propagates within said LOE by internal reflection at said major external surfaces, is partially reflected by said first set of partially-reflecting surfaces to generate a deflected propagating image propagating within said LOE by internal reflection at said major external surfaces, and is partially reflected by said second set of partially-reflecting surfaces to generate a coupled-out image directed outwards from one of said major external surfaces towards the user,
  • 2. The optical system of claim 1, wherein said coupling-in surface is obliquely angled relative to said major external surfaces.
  • 3. The optical system of claim 2, wherein said aperture expanding arrangement further comprises a pair of mutually-parallel external faces, said third set of partially-reflecting surface being located between said external faces, one of said external faces being deployed in facing relation to said coupling-in surface, with an air gap between said external face and said coupling-in surface.
  • 4. The optical system of claim 1, wherein said third set of at least partially-reflecting surfaces has a first sequence of successively-increasing reflectivities in an order in which the image illumination reaches them, and wherein said first set of partially-reflecting surfaces has a second sequence of successively-increasing reflectivities in an order in which the image illumination reaches them, said second sequence starting at a reflectivity smaller than a last reflectivity of said first sequence.
  • 5. The optical system of claim 4, wherein a last reflectivity of said first sequence of successively-increasing reflectivities is greater than 90%.
  • 6. The optical system of claim 1, wherein a majority of the image illumination arriving at said first set of partially-reflecting surfaces has undergone exactly one reflection from said third set of at least partially-reflecting surfaces.
  • 7. The optical system of claim 1, wherein a majority of the image illumination arriving at said first set of partially-reflecting surfaces has undergone two reflections from said third set of at least partially-reflecting surfaces.
  • 8. The optical system of claim 1, wherein said first region and said second region are non-overlapping.
US Referenced Citations (288)
Number Name Date Kind
2748659 Geffcken et al. Jun 1956 A
2795069 Hardesty Jun 1957 A
2886911 Hardesty May 1959 A
3491245 Hardesty Jan 1970 A
3626394 Nelson et al. Dec 1971 A
3667621 Barlow Jun 1972 A
3677621 Smith Jul 1972 A
3737212 Antonson et al. Jun 1973 A
3802763 Cook et al. Apr 1974 A
3857109 Pilloff Dec 1974 A
3873209 Schinke et al. Mar 1975 A
3940204 Withrington Feb 1976 A
4084883 Eastman et al. Apr 1978 A
4191446 Arditty et al. Mar 1980 A
4309070 St Leger Searle Jan 1982 A
4331387 Wentz May 1982 A
4516828 Steele May 1985 A
4613216 Herbec et al. Sep 1986 A
4711512 Upatnieks Dec 1987 A
4715684 Gagnon Dec 1987 A
4775217 Ellis Oct 1988 A
4798448 Van Raalte Jan 1989 A
4805988 Dones Feb 1989 A
4932743 Isobe et al. Jun 1990 A
4978952 Irwin Dec 1990 A
5033828 Haruta Jul 1991 A
5076664 Migozzi Dec 1991 A
5096520 Faris Mar 1992 A
5157526 Kondo et al. Oct 1992 A
5231642 Scifres et al. Jul 1993 A
5301067 Bleier et al. Apr 1994 A
5353134 Michel et al. Oct 1994 A
5367399 Kramer Nov 1994 A
5369415 Richard et al. Nov 1994 A
5453877 Gerbe et al. Sep 1995 A
5543877 Takashi et al. Aug 1996 A
5555329 Kuper et al. Sep 1996 A
5619601 Akashi et al. Apr 1997 A
5650873 Gal et al. Jul 1997 A
5680209 Maechler Oct 1997 A
5724163 David Mar 1998 A
5751480 Kitagishi May 1998 A
5764412 Suzuki et al. Jun 1998 A
5829854 Jones Nov 1998 A
5883684 Millikan et al. Mar 1999 A
5896232 Budd et al. Apr 1999 A
5919601 Nguyen et al. Jul 1999 A
5966223 Yaakov et al. Oct 1999 A
5982536 Swan Nov 1999 A
6021239 Minami et al. Feb 2000 A
6052500 Takano et al. Apr 2000 A
6091548 Chen Jul 2000 A
6144347 Mizoguchi et al. Nov 2000 A
6222676 Togino et al. Apr 2001 B1
6322256 Inada et al. Nov 2001 B1
6324330 Stites Nov 2001 B1
6349001 Spitzer Feb 2002 B1
6362861 Hertz et al. Mar 2002 B1
6384982 Spitzer May 2002 B1
6388814 Tanaka May 2002 B2
6404550 Yajima Jun 2002 B1
6404947 Matsuda Jun 2002 B1
6490104 Gleckman et al. Dec 2002 B1
6509982 Steiner Jan 2003 B2
6542307 Gleckman Apr 2003 B2
6556282 Jamieson et al. Apr 2003 B2
6577411 David Jun 2003 B1
6580529 Amitai et al. Jun 2003 B1
6671100 McRuer Dec 2003 B1
6690513 Hulse et al. Feb 2004 B2
6710902 Takeyama Mar 2004 B2
6775432 Basu Aug 2004 B2
6791760 Janeczko et al. Sep 2004 B2
6798579 Robinson et al. Sep 2004 B2
6829095 Amitai Dec 2004 B2
6942925 Lazarev et al. Sep 2005 B1
7016113 Choi et al. Mar 2006 B2
7021777 Amitai Apr 2006 B2
7088664 Kim et al. Aug 2006 B2
7175304 Wadia et al. Feb 2007 B2
7205960 David Apr 2007 B2
7355795 Yamazaki et al. Apr 2008 B1
7391573 Amitai Jun 2008 B2
7418170 Mukawa et al. Aug 2008 B2
7430355 Heikenfeld et al. Sep 2008 B2
7446170 Milovan et al. Nov 2008 B2
7457040 Amitai Nov 2008 B2
7577326 Amitai Aug 2009 B2
7643214 Amitai Jan 2010 B2
7672055 Amitai Mar 2010 B2
7724443 Amitai May 2010 B2
7751122 Amitai Jul 2010 B2
7778508 Hirayama Aug 2010 B2
7949214 Dejong May 2011 B2
7995275 Maeda et al. Aug 2011 B2
8000020 Amitai Aug 2011 B2
8004765 Amitai Aug 2011 B2
8035872 Ouchi Oct 2011 B2
8096439 Amitai et al. Jan 2012 B2
8405573 Lapidot et al. Mar 2013 B2
8432614 Amitai Apr 2013 B2
8643948 Amitai et al. Feb 2014 B2
8655178 Capron et al. Feb 2014 B2
8666208 Amirparviz et al. Mar 2014 B1
8736963 Robbins et al. May 2014 B2
8743464 Amirparviz Jun 2014 B1
8913865 Bennett Dec 2014 B1
9025253 Hadad et al. May 2015 B2
9248616 Amitai Feb 2016 B2
9551880 Amitai Jan 2017 B2
9568738 Mansharof et al. Feb 2017 B2
9804396 Amitai Oct 2017 B2
9805633 Zheng Oct 2017 B2
9933684 Brown et al. Apr 2018 B2
10048499 Amitai Aug 2018 B2
10437066 Dobschal Oct 2019 B2
10480725 Streppel Nov 2019 B2
10480772 Joiris Nov 2019 B2
10480775 Yamada Nov 2019 B2
20020015233 Park Feb 2002 A1
20020191297 Gleckman et al. Dec 2002 A1
20030007157 Hulse et al. Jan 2003 A1
20030020006 Janeczko et al. Jan 2003 A1
20030063042 Friesem et al. Apr 2003 A1
20030090439 Spitzer et al. May 2003 A1
20030165017 Amitai Sep 2003 A1
20030197938 Schmidt et al. Oct 2003 A1
20030218718 Moliton et al. Nov 2003 A1
20040032660 Amitai Feb 2004 A1
20040033528 Amitai Feb 2004 A1
20040085649 Repetto et al. May 2004 A1
20040137189 Tellini et al. Jul 2004 A1
20040233534 Nakanishi et al. Nov 2004 A1
20050018308 Cassarly et al. Jan 2005 A1
20050078388 Amitai Apr 2005 A1
20050083592 Amitai Apr 2005 A1
20050084210 Cha Apr 2005 A1
20050174641 Greenberg Aug 2005 A1
20050174658 Long et al. Aug 2005 A1
20050180687 Amitai Aug 2005 A1
20050265044 Chen et al. Dec 2005 A1
20060126182 Levola Jun 2006 A1
20060268421 Shimizu et al. Nov 2006 A1
20070070859 Hirayama Mar 2007 A1
20070086712 Shani Apr 2007 A1
20070091445 Amitai Apr 2007 A1
20070097513 Amitai May 2007 A1
20070155277 Amitai Jul 2007 A1
20080025667 Amitai Jan 2008 A1
20080094586 Hirayama Apr 2008 A1
20080106775 Amitai et al. May 2008 A1
20080151379 Amitai Jun 2008 A1
20080186604 Amitai Aug 2008 A1
20080198471 Amitai Aug 2008 A1
20080278812 Amitai Nov 2008 A1
20080285140 Amitai Nov 2008 A1
20090052046 Amitai Feb 2009 A1
20090052047 Amitai Feb 2009 A1
20090097127 Amitai Apr 2009 A1
20090122414 Amitai May 2009 A1
20090153437 Aharoni Jun 2009 A1
20090190222 Simmonds et al. Jul 2009 A1
20100067110 Amitai et al. Mar 2010 A1
20100111472 DeJong May 2010 A1
20100171680 Lapidot et al. Jul 2010 A1
20100202128 Saccomanno Aug 2010 A1
20100278480 Vasylyev et al. Nov 2010 A1
20100291489 Moskovits et al. Nov 2010 A1
20120039576 Dangel et al. Feb 2012 A1
20120147361 Mochizuki et al. Jun 2012 A1
20120179369 Lapidot et al. Jun 2012 A1
20120206817 Totani Aug 2012 A1
20130229717 Amitai Sep 2013 A1
20130276960 Amitai Oct 2013 A1
20130279017 Amitai Oct 2013 A1
20130321432 Burns et al. Dec 2013 A1
20130334504 Thompson et al. Dec 2013 A1
20130335975 Park Dec 2013 A1
20140003762 Macnamara Jan 2014 A1
20140043688 Schrader et al. Feb 2014 A1
20140118613 Amitai et al. May 2014 A1
20140118836 Amitai et al. May 2014 A1
20140118837 Amitai et al. May 2014 A1
20140126051 Amitai et al. May 2014 A1
20140126052 Amitai et al. May 2014 A1
20140126056 Amitai et al. May 2014 A1
20140126057 Amitai et al. May 2014 A1
20140126175 Amitai et al. May 2014 A1
20140185142 Gupta et al. Jul 2014 A1
20140226215 Komatsu et al. Aug 2014 A1
20150016777 Abovitz et al. Jan 2015 A1
20150081313 Boross et al. Mar 2015 A1
20150138451 Amitai May 2015 A1
20150138646 Tatsugi May 2015 A1
20150160529 Popovich et al. Jun 2015 A1
20150198805 Mansharof et al. Jul 2015 A1
20150205140 Mansharof et al. Jul 2015 A1
20150205141 Mansharof et al. Jul 2015 A1
20150219834 Nichol et al. Aug 2015 A1
20150277127 Amitai Oct 2015 A1
20150293360 Amitai Oct 2015 A1
20150338655 Sawada et al. Nov 2015 A1
20160116743 Amitai Apr 2016 A1
20160170212 Amitai Jun 2016 A1
20160170213 Amitai Jun 2016 A1
20160170214 Amitai Jun 2016 A1
20160187656 Amitai Jun 2016 A1
20160234485 Robbins et al. Aug 2016 A1
20160341964 Amitai Nov 2016 A1
20160349518 Amitai et al. Dec 2016 A1
20170045744 Amitai Feb 2017 A1
20170052376 Amitai Feb 2017 A1
20170052377 Amitai Feb 2017 A1
20170075119 Schultz et al. Mar 2017 A1
20170242249 Wall Aug 2017 A1
20170315358 Masuda Nov 2017 A1
20170336636 Amitai et al. Nov 2017 A1
20170343822 Border et al. Nov 2017 A1
20170357095 Amitai Dec 2017 A1
20170363799 Ofir et al. Dec 2017 A1
20170371160 Schultz Dec 2017 A1
20180039082 Amitai Feb 2018 A1
20180067315 Amitai et al. Mar 2018 A1
20180157057 Gelberg et al. Jun 2018 A1
20180210202 Danziger Jul 2018 A1
20180267317 Amitai Sep 2018 A1
20180275384 Danziger et al. Sep 2018 A1
20180284448 Matsuki Oct 2018 A1
20180292592 Danziger Oct 2018 A1
20180292599 Ofir et al. Oct 2018 A1
20180373039 Amitai Dec 2018 A1
20190011710 Amitai Jan 2019 A1
20190056600 Danziger et al. Feb 2019 A1
20190064518 Danziger Feb 2019 A1
20190155035 Amitai May 2019 A1
20190170327 Eisenfeld et al. Jun 2019 A1
20190208187 Danziger Jul 2019 A1
20190212487 Danziger et al. Jul 2019 A1
20190227215 Danziger et al. Jul 2019 A1
20190278086 Ofir Sep 2019 A1
20190285900 Amitai Sep 2019 A1
20190293856 Danziger Sep 2019 A1
20190339530 Amitai Nov 2019 A1
20190346609 Eisenfeld Nov 2019 A1
20190361240 Gelberg Nov 2019 A1
20190361241 Amitai Nov 2019 A1
20190377187 Rubin et al. Dec 2019 A1
20190391408 Mansharof Dec 2019 A1
20200033572 Danziger et al. Jan 2020 A1
20200041713 Danziger Feb 2020 A1
20200081246 Olkkonen Mar 2020 A1
20200089001 Amitai et al. Mar 2020 A1
20200110211 Danziger et al. Apr 2020 A1
20200120329 Danziger Apr 2020 A1
20200133008 Amitai Apr 2020 A1
20200150330 Danziger et al. May 2020 A1
20200183159 Danziger Jun 2020 A1
20200183170 Amitai et al. Jun 2020 A1
20200200963 Eisenfeld et al. Jun 2020 A1
20200209667 Sharlin et al. Jul 2020 A1
20200241308 Danziger et al. Jul 2020 A1
20200249481 Danziger et al. Aug 2020 A1
20200278557 Greenstein et al. Sep 2020 A1
20200285060 Amitai Sep 2020 A1
20200292417 Lobachinsky et al. Sep 2020 A1
20200292744 Danziger Sep 2020 A1
20200292819 Danziger et al. Sep 2020 A1
20200310024 Danziger et al. Oct 2020 A1
20200326545 Amitai et al. Oct 2020 A1
20200371311 Lobachinsky et al. Nov 2020 A1
20210003849 Amitai et al. Jan 2021 A1
20210018755 Amitai Jan 2021 A1
20210033773 Danziger et al. Feb 2021 A1
20210033774 Tanaka Feb 2021 A1
20210033862 Danziger et al. Feb 2021 A1
20210033872 Rubin et al. Feb 2021 A1
20210055218 Aldaag et al. Feb 2021 A1
20210055466 Eisenfeld Feb 2021 A1
20210055561 Danziger et al. Feb 2021 A1
20210063733 Ronen Mar 2021 A1
20210072553 Danziger et al. Mar 2021 A1
20210099691 Danziger Apr 2021 A1
20210109351 Danziger et al. Apr 2021 A1
20210116367 Gelberg et al. Apr 2021 A1
20210141141 Danziger et al. May 2021 A1
20210157150 Amitai May 2021 A1
20210165231 Gelberg et al. Jun 2021 A1
20210239898 Danziger et al. Aug 2021 A1
Foreign Referenced Citations (72)
Number Date Country
101542346 Sep 2009 CN
107238928 Oct 2017 CN
1422172 Nov 1970 DE
19725262 Dec 1998 DE
102013106392 Dec 2014 DE
0365406 Apr 1990 EP
0380035 Aug 1990 EP
0399865 Nov 1990 EP
0543718 May 1993 EP
0566004 Oct 1993 EP
1158336 Nov 2001 EP
1180711 Feb 2002 EP
1326102 Jul 2003 EP
1385023 Jan 2004 EP
1485747 Dec 2004 EP
1562066 Aug 2005 EP
0770818 Apr 2007 EP
1779159 May 2007 EP
2530510 Dec 2012 EP
2496905 Jun 1982 FR
2638242 Apr 1990 FR
2721872 Jan 1996 FR
2220081 Dec 1989 GB
2272980 Jun 1994 GB
2278222 Nov 1994 GB
2278888 Dec 1994 GB
2002539498 Nov 2002 JP
2003140081 May 2003 JP
2003536102 Dec 2003 JP
2004527801 Sep 2004 JP
2005084522 Mar 2005 JP
2011-028141 Feb 2011 JP
201809798 Mar 2018 TW
9510106 Apr 1995 WO
9815868 Apr 1998 WO
9952002 Oct 1999 WO
0004407 Jan 2000 WO
0063738 Oct 2000 WO
0127685 Apr 2001 WO
0195025 Dec 2001 WO
0195027 Dec 2001 WO
02082168 Oct 2002 WO
03058320 Jul 2003 WO
03081320 Oct 2003 WO
2004109349 Dec 2004 WO
2005024485 Mar 2005 WO
2005024491 Mar 2005 WO
2005024969 Mar 2005 WO
2005093493 Oct 2005 WO
2005124427 Dec 2005 WO
2006013565 Feb 2006 WO
2006085308 Aug 2006 WO
2006085309 Aug 2006 WO
2006085310 Aug 2006 WO
2006087709 Aug 2006 WO
2006098097 Sep 2006 WO
2007054928 May 2007 WO
2007093983 Aug 2007 WO
2008023367 Feb 2008 WO
2008129539 Oct 2008 WO
2008149339 Dec 2008 WO
2009009268 Jan 2009 WO
2009074638 Jun 2009 WO
2011130720 Oct 2011 WO
2013065656 May 2013 WO
2013175465 Nov 2013 WO
2015081313 Jun 2015 WO
2016103251 Jun 2016 WO
2016132347 Aug 2016 WO
2017106873 Jun 2017 WO
2017199232 Nov 2017 WO
WO-WO-2018206848 Nov 2018 WO
Non-Patent Literature Citations (1)
Entry
Da-Yong et al., “A Continuous Membrance Micro Deformable Mirror Based on Anodic Bonding of SOI to Glass Water”, Microsystem Technologies, Micro and Nanosystems Information Storage and Processing Systems, vol. 16, No. 10, May 20, 2010 pp. 1765-1769.
Related Publications (1)
Number Date Country
20210239898 A1 Aug 2021 US
Provisional Applications (1)
Number Date Country
62796107 Jan 2019 US
Continuations (1)
Number Date Country
Parent 16638495 US
Child 17234885 US