Abstract:
An apparatus for providing an optical display includes an optical substrate for propagating light received from a light source, a first set of one or more switchable diffractive elements in the substrate, and a second set of one or more switchable diffractive elements in the substrate. Each diffractive element in the second set corresponds to a diffractive element in the first set. Each of the diffractive elements in the first and second sets is configured to switch between on and off states. One of the states is for diffracting light and the other state for allowing light to pass through. Each of the first set of diffractive elements is configured to diffract the light at an angle for propagation in the substrate. Each of the second set of diffractive elements is configured to diffract the light for display.

Description:
BACKGROUND 
     The present disclosure relates generally to the field of display optics. More specifically, the disclosure relates to substrate guided optics. 
     Conventional solutions for wide field of view Head Mounted Displays (HMDs) (e.g., a helmet mounted display) and Head Up Displays (HUDs) generally include off-axis visors, combiners, and multiple complex tilted and decentered lenses. The field of view that can be achieved with conventional fixed diffractive components may be limited to less than about 30 degrees external angle. This limited field of view may not meet requirements for digital night vision systems and wide field of view HUDs or HMDs. 
     Conventional HMD optical designs, such as those for the Joint Helmet Mounted Cueing System (JHMCS), the Joint Strike Fighter (JSF), and the Eurofighter Typhoon, use complex tilted and decentered, aspheric plastic lenses. For example, the JSF HMD incorporates seven lenses in order to correct the off-axis aberrations induced by the visor. These lens elements are expensive, tolerance limited, and require precision tooling to assemble. 
     The optical performance of conventional visor-projected designs, typically fall off with exit pupil and field of view and barely meet the Modulation Transfer Function (MTF) performance required for night vision sensors. 
     A reduction in mass at the HMD system level is desirable for a number of reasons. To establish the effects of head supported mass during flight, the mass is multiplied by the aircraft acceleration. For high performance fighter aircraft pulling a 10 G turn, the mass of the HMD is multiplied by 10. Head supported mass also affects the induced neck loads during parachute deployment, HMD components, especially the optics, tend to be oriented forward and upward in the helmet. Neck strain during normal flight can be exacerbated by this forward center of mass, for example, induced neck forces during ejection and parachute deployment may be worsened by an upward and forward center of mass. 
     What is needed is an optical system having a lower mass. What is also needed is an optical system that does not need an IPD adjustment mechanism. What is also needed is an optical system having a smaller volume lens system. What is further needed is an optical system having a smaller volume display module. What is further still needed is an optical system having a lower cost. What is further still needed is an optical system without the need for a custom fit system. 
     SUMMARY 
     One exemplary embodiment of the disclosure relates to an apparatus for providing an optical display. The apparatus includes an optical substrate for propagating light received from a light source, a first set of one or more switchable diffractive elements in the substrate, and a second set of one or more switchable diffractive elements in the substrate. Each diffractive element in the second set corresponds to a diffractive element in the first set. Each of the diffractive elements in the first and second sets is configured to diffract light when switched off and allow light to pass through when switched on. Each of the first set of diffractive elements is configured to diffract the light at an angle for propagation in the substrate. Each of the second set of diffractive elements is configured to diffract the light for display. 
     Another exemplary embodiment of the disclosure relates to an apparatus for providing an optical display. The apparatus includes a substrate for propagating light received from a light source, a first set of one or more switchable Bragg gratings or holographic polymer dispersed liquid crystal devices in the substrate, and a second set of one or more switchable Bragg gratings or holographic polymer dispersed liquid crystal devices in the substrate. Each Bragg grating or liquid crystal device in the second set corresponds to a Bragg grating or liquid crystal device in the first set. Each of the Bragg gratings or liquid crystal devices in the first and second sets is configured to switch between on and off states, one of the states for diffracting light and the other state for allowing light to pass through. Each of the first set of Bragg gratings or liquid crystal devices is configured to diffract the light at an angle for propagation in the substrate. Each of the second set of Bragg gratings or liquid crystal devices is configured to diffract the light for display. 
     Another exemplary embodiment of the disclosure relates to an apparatus for providing an optical display. The apparatus includes means for propagating light received from a light source, means for diffracting light at an input or allowing light at the input to pass through based on a switching state, and means for diffracting propagated light to an output for display or allowing propagated light to pass through based on the switching state. Each means for diffracting propagated light corresponds to a means for diffracting light at an input. 
     It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory only, and are not restrictive of the invention as claimed. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       These and other features, aspects, and advantages of the present invention will become apparent from the following description, appended claims, and the accompanying exemplary embodiments shown in the drawings, which are briefly described below. 
         FIG. 1  is a diagram showing light passing through glass and air, according to an exemplary embodiment. 
         FIG. 2  is a diagram showing light passing through glass and a diffraction coupling, according to an exemplary embodiment. 
         FIG. 3  is a diagram showing light from a display device propagating through a waveguide, according to an exemplary embodiment. 
         FIG. 4  is a chart illustrating calculated external angles for a diffractive optical element that couples light into or out of a waveguide, according to an exemplary embodiment. 
         FIG. 5  is a chart illustrating calculated external angles for a diffractive optical element using two holograms to expand the field of view of a waveguide, according to an exemplary embodiment. 
         FIG. 6  is a diagram showing light propagating through a waveguide including multiple diffractive surfaces, according to an exemplary embodiment. 
         FIG. 7  is a diagram showing light propagating through a waveguide including multiple diffractive surfaces, according to another exemplary embodiment. 
         FIGS. 8A-8D  are diagrams showing light exiting the waveguide of  FIG. 7 , according to an exemplary embodiment. 
         FIG. 9  is a diagram showing multiple stacked instances of the waveguide of  FIG. 7 , according to an exemplary embodiment. 
         FIG. 10  is a top view of the waveguide of  FIG. 7 , according to an exemplary embodiment. 
         FIG. 11  is a top view of a waveguide having a laser input, according to an exemplary embodiment. 
     
    
    
     DETAILED DESCRIPTION 
     Referring to  FIG. 1 , a light wave  100  may pass through a glass or plastic layer  102  and an air layer  104 , according to an exemplary embodiment. The refractive index of glass/plastic  102  may be found using Snell&#39;s equation: Sine i/Sine r=refractive index. The largest angle of incidence in which light wave is refracted out of glass/plastic  102  is called the critical angle (r c ). In air, when i=90°, Sine r c =1/refractive index, so for propagation in a waveguide (parallel surfaces of optical medium) the allowable angle range is r c  to r=90°. Practically speaking, for substrate guided optics, the internal angle range is generally much smaller and equates to an external angle of about 20° to 30°. 
     Referring to  FIG. 2 , light enters a substrate or waveguide  200  and is diffracted by a diffraction grating  202  between a glass layer  204  and another glass layer  206 . Diffraction grating  202  adjusts the angle of the light passing through glass  204  so that the angle of the light as it meets the upper surface of glass  206  is beyond the critical angle and it reflects internally in waveguide  200 . The light will then pass back through grating  202  and glass layer  204  and exit into the air at a different point than it entered glass layer  204 . According to various exemplary embodiments, diffraction grating  202  may be a thick phase transmission hologram, a reflection hologram, a Bragg grating, binary or uniform optics, or another surface grating or diffractive surface. 
     For example, co-owned U.S. Pat. No. 5,856,842, which is herein incorporated by reference in its entirety, shows how light from a far field object (where the light is substantially collimated) can be coupled into a waveguide and out again by diffractive means, for example in a periscope. The far field object can also be created by a collimating lens in the same manner that an HMD or HUD images light from a display device, for example a CRT or flat panel display (e.g., an LCD display, a plasma display, etc.). The optics of the periscope may be used to displace the light from a collimating lens and can be used in an HMD, a HUD, or eyewear, for example a combiner in a conventional HMD or HUD. 
     Referring to  FIG. 3 , a simplified holographic waveguide  300  receives light transmitted from a display device  302  and through a collimating element  304 . The light passes through a glass (or optical plastic or other transparent) layer  306  and a diffractive element  308  (e.g., a holographic diffractive element), which is configured to diffract the light at a different angle. The diffracted light has an angle greater than the critical angle of a glass layer  310  and glass layer  306  and thus propagates internally to a second diffractive element  312 . Element  312  is configured to diffract the light out of waveguide  300 , for example to an eye location. Because the diffractive power of in-coupling diffractive surface  308  is the same as out-coupling diffractive surface  312 , the input and output angles are the same. This is generally true for any wavelength and thus there may be no chromatic aberration in the system. 
     Light propagation may be limited within a range of angles, for example the total internal reflection (TIR) is about 41 degrees to the substrate normal for glass. This range of angles can be extended slightly using a reflective coating, but this may diminish the transparency of the substrate. Light propagation may also be limited by light parallel to the surface (90 degrees to the surface normal). Light coupled into waveguide  300  using diffractive element  308  therefore has a range of angles that relates to the power of diffractive element  308  (e.g., diffraction grating line spacing) and refraction out of element  308 . 
     Referring to  FIG. 4 , these conditions have been tabulated in a chart  400  to show that the range of the external angles coupling into the waveguide or out of the waveguide may have a theoretical limit of about 30 degrees, according to an exemplary embodiment using BK-7 optical glass. Chart  400  shows an analysis of the external angles that can be employed versus the internal limits of the waveguide and how the range of external angles vary depending upon the grating spacing. Light propagates inside the waveguide (e.g., waveguide  300 ) between 90 degrees to the normal and the TIR angle of the substrate. In the illustrated example, the incidence angle in air at the substrate (field of view) is between −23.75 degrees and 4.39 degrees, giving a range of 28.14 degrees or less than 30 degrees. 
     The practical limit of the external angles is far less than 30 degrees. In another example, a limit of 20 degrees has been set for discussion purposes and as a representation of a reasonable limit for the angular bandwidth of a typical hologram. At system level, in order to expand the field of view well beyond about 20-30 degrees more than one hologram may be used. Each hologram diffracts light from a cone of external angles (e.g., about 20 degrees range) into the waveguide and propagates the light within the range of allowable angles supported by the waveguide (between 90 degrees and the TIR condition). However, the external angles of each hologram can be offset with respect to the other hologram by changing the diffractive power. 
     Referring to  FIG. 5 , a chart  500  illustrates that two holograms can couple light within the allowable angles of the substrate with external angles adding up to more than 30 or 40 degrees to expand the field of view of the system, according to an exemplary embodiment. If diffraction gratings  502  and  504  are applied, the field of view of the system in this example is expanded between about −59 degrees and about 6.57 degrees or to approximately 70 degrees (angle in air). 
     Referring to  FIG. 6 , a waveguide  600  includes two diffractive surfaces  602  and  604  in a substrate  606  to extend the field of view of the system, according to an exemplary embodiment. A light ray or wave  608  and a light ray  610  form a first field of view angle and both fall incident on diffractive surface  602 . A light ray  612  and a light ray  614  form a second field of view angle and fall incident on diffractive surfaces  602  and  604  causing the behavior of the light to be different (shown here as diverging light rays). If the light from rays  612  and  614  hit out-coupling diffractive surface  604 , the resultant image will be a double image. If the light is broad band (e.g. 50 nm from an LED), then the difference in diffractive power between in-coupling diffractive element  602  and out-coupling diffractive element  604  may also induce chromatic aberration. 
     Referring to  FIG. 7 , a waveguide  700  illustrates how in-coupling switchable diffractive elements and out-coupling diffractive elements can be paired up and switched in and out (on and off or vice versa) so that the output light does not suffer from image doubling and chromatic aberration, which would be present if trying to use non-switchable diffraction elements as discussed earlier. Waveguide  700  includes diffractive elements  702 ,  704 , and  706  (e.g., switchable diffractive elements such as electronically switchable Bragg gratings or Holographic Polymer Dispersed Liquid Crystal (HPDLC)) in substrate  708  at an input portion and diffractive elements  710 ,  712 , and  714  in substrate  708  at an output portion. Output diffractive elements  710 ,  712 , and  714  have the equal and opposite diffractive power as corresponding input diffractive elements  702 ,  704 , and  706 , respectively. In the illustrated exemplary embodiment, light is received by a collimating device  716  from three different angles. The input collimating lens generates a field of view that is needed for the optical display system (e.g., HMD, HUD, eyewear, etc.). According to some exemplary embodiments, the collimating lens may be integrated with diffractive elements  702 ,  704 ,  706 , while in other exemplary embodiments, the collimating lens may be separate. At any point in time, only one of each input element  702 ,  704 , or  706  may be operational or switched on along with its corresponding output element  710 ,  712 , or  714  and all elements may switch consecutively within the frame time of the system. Light does not couple into waveguide  700  until it hits a diffractive element ( 702 ,  704 , or  706 ) that is operational. Therefore, only light from one angle range is coupled into waveguide  700  at any one point in time. Further, light does not couple out of the substrate until it hits the diffraction element that is operational. 
     According to the illustrated example, a single parallel beam of light shown by dashed lines hits diffraction surface  702  and is diffracted into waveguide  700  until it hits complimentary diffractive surface  710  and is diffracted out of waveguide  700  at the same angle as it enters waveguide  700 . Because the input diffractive power is equal and opposite to the output diffractive power no chromatic aberration is induced in the system. It is noted that while the FIGURE illustrates use of three input and output switchable diffractive elements, according to other exemplary embodiments, more or fewer than three switchable diffractive elements may be used. It is also noted that while the FIGURE illustrates reception and output of light at three different angles, the figure does not include the light in the range between the three field angles shown. The light incident on each of the diffractive surfaces are in a range limited by the geometric limits described herein for a single fixed diffractive surface and are therefore in a range tabulated in  FIG. 4  and limited to about 30 degrees. 
     Referring to  FIGS. 8A-8D , a first order geometry of output holograms for a waveguide  800  is illustrated, according to an exemplary embodiment. For purposes of this example, the exit pupil of the system was set at about 15 mm (which is generally regarded as the minimum acceptable exit pupil of an HMD or eyewear although according to other exemplary embodiments exit pupils much greater than 15 mm may be used) with an eye-relief of about 25 mm (the minimum requirement for wearing aviator spectacles). The first order geometry plots a 60 degree field of view using three holograms  802 ,  804 , and  806 , each with a field of view of about 20 degrees.  FIG. 8A  shows the first order geometry for the central 20 degrees (plus and minus 10 degrees from normal),  FIG. 8B  shows the right 20 degrees (10 to 30 degrees from the left normal),  FIG. 8C  shows the left 20 degrees (−10 and −30 degrees from the right normal), and  FIG. 8D  shows the full 60 degrees of the holographic waveguide display with three overlapping holograms. The practical implementation of using multiple switchable diffractive surfaces in an HMD, HUD, or eyewear therefore includes overlapping switchable diffractive surfaces. This includes the illustration of  FIG. 7 , which shows a simplified version where the diffractive surfaces are adjacent to each other. 
     For an extended field of view and an extended exit pupil, the footprint of the light rays for exemplary 20 degree sections overlaps at waveguide  800 . The overlap may be decreased with increasing eye-relief and may be increased with increasing exit pupil size. For example, if the system has an exit pupil of 30 mm, then the overlap will be significant. Overlapping holograms cannot be employed within the same waveguide using conventional holographic material because the rays for each hologram would be indistinguishable from one another since they fall within the same range of internal waveguide angles. 
     According to some exemplary embodiments, multiple holograms that overlap with each other and are separated by an air space may be used, however, implementation of a mechanism for a curved visor or much greater field of view may be difficult and not lend itself to a low mass and mechanically stable solution. According to other exemplary embodiments, Switchable Bragg Gratings (SBG) (e.g., electronically switchable Bragg gratings) may be used as the diffractive element, for example as developed by SBG Labs, Inc. of Silicon Valley, Calif. According to other exemplary embodiments, switchable transmission holograms or switchable reflection holograms may be used to develop wider fields of view. 
     A waveguide (e.g., waveguide  700  or  800 ) may include multiple holograms (e.g., holograms  702 ,  704 , and  706  or holograms  802 ,  804 , and  806 ) of different powers. An SBG stack can be used that can be switched sequentially to build up the field of view of the optics This allows a setup of overlapping holograms as illustrated in  FIGS. 7 and 8 . 
     Referring to  FIG. 9 , a waveguide system  900  may include multiple stacks of SBG holograms  902 ,  904 , and  906  that are at least similar to each other, according to an exemplary embodiment. Such a system  900  may be used to generate color displays in sequential mode. Frame sequential color and frame sequential wide field of view have similar coordination between the display data, the illumination source, and the SBGs. Each SBG stacks  902 ,  904 , and  906  may be used to propagate a different color, for example, red, blue, and green. At any given point in time, one set of input and output holograms may be switched on to diffract light of a specific color and all holograms will switch within the frame time of the system at a rate sufficient so a human eye will not perceive flicker (e.g., about 16 milliseconds). According to other exemplary embodiments, different color schemes may be used or more or fewer than three switchable diffractive stacks may be used. 
     Referring to  FIG. 10 , while the waveguides have been illustrated as having single rows of diffractive elements thus far, according to other exemplary embodiments, a waveguide  10000  may include an in-coupling surface  1002  and an out-coupling diffractive surface  1004  that are paired up in a two dimensional array and have equal and opposite diffractive power. The input light may be generated using a collimating lens placed at exit pupil distance from the in-coupling diffractive array. The exit pupil of the lens may be of similar dimensions as for an HMD, HUD, or eyewear display system. The diffractive arrays concept may be used with broadband light sources and so lasers are not required in order to make the system work. It is noted that as in  FIG. 8 , due to the first order geometry of exit pupil and eye relief and the desire to have a contiguous field of view, overlapping switchable diffractive devices may be used in a practical implementation for an HMD, HUD, or eyewear. 
     According to other exemplary embodiments, the diffractive power on the input coupling diffractive elements can include additional diffractive power that can be used to color correct chromatic aberrations in the collimating lens. According to some exemplary embodiments, the waveguides described above may be used with a device that can be controlled to illuminate pixels at specific times. According to some exemplary embodiments, the waveguide system can utilize a beamsplitter in the middle of the sandwich to expand the exit pupil. Therefore, the input lens may be much smaller than for the exit pupil. 
     According to various exemplary embodiments, various light sources may be used to provide light waves to the waveguides described above. For example, a broad band light source such as an LED may be used with holographic waveguide displays. Chromatic dispersion induced by high power diffractive elements generally need to be negated by diffractive elements of equal and opposite power. In the case of a holographic waveguide display, this can be done by employing the same power diffractive element to couple light into and out of the waveguide. For an expanded field of view system employing switchable Bragg gratings, this same concept can be applied by using complimentary pairs of stacked SBGs for the in-coupling and out-coupling diffractive elements, as described above. 
     Referring to  FIG. 11 , compact and low cost lasers have become available (e.g. Necsel lasers available from Novalux, Inc. of San Francisco, Calif.) and represent an ideal light source for use with high diffractive power optics. Complimentary pairs of diffractive elements are not required for a holographic waveguide display  1100  employing one or more lasers, according to an exemplary embodiment. Because a laser has a very narrow spectrum, the diffractive power on an input coupling diffractive surface  1102  and an output coupling diffractive surface  1104  does not have to be balanced. Input diffractive elements  1102  are tiled 1, 2, 3 and the output diffractive elements are shown as columns A, B, C. In one example, the sequence of switching tiles may be 1 and 1A, then 1 and 1B, then 1 and 1C, then 2 and 2A, then 2 and 2B, etc. If the input device is a laser micro-mems scanner, which generally has a small field of view, the system may be able to expand this field of view sequentially using a high frame rate. The imaging device may also be a low resolution imager with a high frame rate, for example a ferro-electric crystal device. 
     Holographic lenses can be applied in the system that will reduce the size and mass of the final system. Lasers are highly efficient and already polarized, which enables low power HMDs, HUDs, or eyewear displays to be generated for applications such as soldier systems where battery power is a limiting factor. 
     Laser speckle is an issue that has hindered the introduction of laser illuminated. Easily recognizable as a sparkly or granular structure around uniformly illuminated rough surface, speckle arises from the high spatial and temporal coherence of Lasers. The resulting viewer distraction and loss of image sharpness has been an obstacle to commercialization of laser projectors. The benchmark for most applications is a speckle contrast of 1% (speckle contrast being defined as the ratio of the standard deviation of the speckle intensity to the mean speckle intensity). Mechanical methods such as rotating diffusers and vibrating screens suffer from problems of noise, mechanical complexity and size. Other passive techniques using diffractive, MEMs or holographic elements, microlens arrays and others have met with limited success. According to some exemplary embodiments, a despeckler based on an SBG that is compact, low cost, silent, easily integrated, and applicable to any type of laser display may be used, for example a despeckler developed by SBG Labs. This solution may also provide functions of beam combining, beam shaping, and homogenization integrated in a single module. 
     While the detailed drawings, specific examples, and particular configurations given describe preferred and exemplary embodiments, they serve the purpose of illustration only. The inventions disclosed are not limited to the specific forms shown. For example, the methods may be performed in any of a variety of sequence of steps or according to any of a variety of mathematical formulas. The hardware and software configurations shown and described may differ depending on the chosen performance characteristics and physical characteristics of the communications devices. For example, the type of system components and their interconnections may differ. The systems and methods depicted and described are not limited to the precise details and conditions disclosed. The figures show preferred exemplary operations only. The specific data types and operations are shown in a non-limiting fashion. Furthermore, other substitutions, modifications, changes, and omissions may be made in the design, operating conditions, and arrangement of the exemplary embodiments without departing from the scope of the invention as expressed in the appended claims.