Display device and a method for illuminating a light modulator array of a display device

An image projector device or a virtual display device may comprise a light modulator array to generate an image. The modulator array may be e.g. Liquid Crystal on Silicon (LCOS) chip or a digital micromirror device (DMD). A modulator array which does not emit light itself needs further means to provide light.

Spatial variations in the intensity of the illuminating light affect the quality of the displayed image.

Patent application US 2002/0176054A1 discloses a light pipe to provide a uniform light beam for illuminating an LCOS imager.

U.S. Pat. No. 7,152,977 discloses a diffuser for homogenizing illuminating light for an LCOS imager.

U.S. Pat. No. 6,814,442 discloses a virtual display comprising a light guide plate to illuminate a reflective imager.

An object of the invention is to provide a display device. Another object of the invention is to provide a method for illuminating a light modulator array of a display device.

According to a first aspect of the invention, there is provided a device for displaying images, said device comprising:

a light source to emit light, an illuminating unit to provide illuminating light by distributing light emitted from said light source, a reflective light modulator array comprising a plurality of pixels for modulating said illuminating light, and imaging optics to focus or collimate light modulated by said pixels, wherein said illuminating unit comprises a substrate having two surfaces separated by a substantially constant distance, said substrate further comprising: an in-coupling portion to couple light of said light source into said substrate to form a waveguided beam which is confined to said substrate by total internal reflections at said surfaces, an integrating portion to reduce spatial variations in the intensity of said waveguided beam, and an out-coupling portion to provide said illuminating light by coupling light of said waveguided beam out of said substrate through one of said surfaces.

According to a second aspect of the invention, there is provided a method for displaying images comprising

coupling light through an in-coupling portion to a substrate of an illuminating unit to form a waveguided beam which is confined to said substrate by total internal reflections on two surfaces of said substrate, said surfaces being separated by a substantially constant thickness. transmitting said waveguided beam through an integrating portion of said substrate in order to reduce spatial variations in the intensity of said waveguided beam, coupling light of said in-coupled beam out of said substrate through at least one of said surfaces by an out-coupling portion of said illuminating unit in order to provide illuminating light, reflecting and modulating said illuminating light by pixels of a reflective light modulator array, and

focusing or collimating light reflected from said pixels in order to display said images.

The illuminating unit provides a cost-effective and compact way to homogenize the illuminating light and to distribute the illuminating light to the modulator array.

The spatial distribution of out-coupling efficiency of the out-coupling portion may be non-uniform in order to improve the quality of the displayed images.

In an embodiment, the spatial distribution of the out-coupling efficiency of the out-coupling portion is arranged to reduce vignetting.

In an embodiment, the spatial distribution of the out-coupling efficiency of the out-coupling portion is arranged to reduce stray light.

In an embodiment, the out-coupling portion comprises out-coupling elements which are arranged to direction-selectively couple light out of the substrate in order to provide energy-efficient angular distribution of the illuminating light. In other words, the out-coupling elements may have a high efficiency for coupling light propagating in a predetermined direction within said substrate out of said substrate, wherein the elements have a lower efficiency for coupling light propagating in other directions out of said substrate.

The out-coupling elements may be e.g. prisms, diffractive gratings, or holograms.

In an embodiment, several light sources may be arranged side by side to emit light into the same substrate. The light sources may have different colors in order to implement a color display.

In an embodiment, the illuminating unit may comprise several stacked substrates in order to implement a color display. For example, the out-coupling portion of a first substrate may be arranged to provide red light. Green light emitted by the out-coupling portion of a second substrate may be transmitted through the out-coupling portion of said first substrate.

The embodiments of the invention and their benefits will become more apparent to a person skilled in the art through the description and examples given herein below, and also through the appended claims.

In the following examples, the embodiments of the invention will be described in more detail with reference to the appended drawings, in which

FIG. 1 shows, in a side view, a display device comprising an illuminating unit,

FIG. 2 a shows, in a side view, reflective light modulator,

FIG. 2 b shows an image formed by the reflective light modulator of FIG. 2 a,

FIG. 3 a shows, in a side view, the display device acting as a projecting device,

FIG. 3 b shows, in a side view, the display device acting as a virtual display,

FIG. 4 shows, in a side view, an illuminating unit, wherein light is coupled into the edge of said unit,

FIG. 5 shows, in a side view, an illuminating unit, wherein light is coupled through an upper surface into said unit,

FIG. 6 shows, in a three-dimensional view, a diffractive beam expander,

FIG. 7 shows, in a top view, a diffractive beam expander,

FIG. 8 a shows, in a side view, an illuminating unit comprising a plurality of stacked substrates, wherein light is coupled into the edges of said substrates,

FIG. 8 b shows, in a side view, an illuminating unit comprising a plurality of stacked substrates, wherein light is coupled through the surfaces of said substrates,

FIG. 9 a shows, in a side view, propagation of light rays modulated by a first pixel of the modulator, said first pixel being at the center of the modulator,

FIG. 9 b shows, in a side view, propagation of light rays modulated by a first pixel of the modulator, said first pixel being near the side of the modulator,

FIG. 10 a shows, in a top view, a plurality of light out-coupling elements of the illuminating unit,

FIG. 10 b shows, in a three-dimensional view, an out-coupling portion comprising a plurality of prisms,

FIG. 10 c shows, in a three-dimensional view, an out-coupling portion comprising a plurality of diffractive zones having different diffractive properties,

FIG. 10 d shows, in a three-dimensional view, the direction of a light ray coupled out of the substrate by an out-coupling element,

FIG. 11 a shows, by way of example, radiance of an out-coupling element as a function of zenith angle of a light ray provided by an out-coupling element,

FIG. 11 b shows by way of example, radiance of an out-coupling element as a function of zenith angle of a light ray provided by an out-coupling element,

FIG. 12 a shows, in a side view, direction-selective coupling of light out of the substrate,

FIG. 12 b shows, by way of example, radiant emittance of an out-coupling element as a function of zenith angle of a light ray impinging on said out-coupling element.

FIG. 13 shows, in a side view, a virtual display device comprising a diffractive beam expander to expand the viewing aperture of said device,

FIG. 14 shows, in a three dimensional view, a bi-ocular virtual display device, and

FIG. 15 shows, in a side view, a display device comprising a curved polarizing beam splitter.

Referring to FIG. 1 , a display device 500 may comprise an illuminating unit 100 , a light source 110 , a two-dimensional reflective modulator array 210 , and imaging optics 280 . The illuminating unit 100 comprises a waveguiding substrate 7 , an integrating portion 102 , and an out-coupling portion 30 . In-coupled light is confined to the substrate 7 by total internal reflections (TIR), i.e. light is waveguided within the substrate 7 . Light emitted by the light source 110 is coupled into the substrate e.g. through the edge of said substrate 7 . The light is reflected several times on the surfaces of the substrate in the integrating portion 102 . Consequently, the integrating portion 102 may act as an optical integrator to reduce variations in spatial intensity distribution of light propagating within said substrate 7 before it is coupled out of the substrate 7 . Out-coupled light B 2 , B 3 provided by the out-coupling portion 30 may impinge on the modulator array 210 . Light B 4 , B 5 may be reflected from each pixel PX 1 of the modulator array 210 towards the imaging optics 280 , depending on the state of said pixel PX 1 . Each pixel PX 1 may be in a reflecting state or in a non-reflecting state. In certain cases the pixels PX 1 may also be set into a partially reflecting state. The imaging optics 280 focuses or collimates light B 43 , B 5 reflected from the modulator array 210 , providing a focused or collimated light beam B 6 . AX 1 denotes the optical axis of the imaging optics 280 .

Illuminating light B 2 , B 3 provided by the illuminating unit 100 may be arranged to impinge to all pixels PX 1 of the modulator array 210 .

In order to provide sufficient homogenization of light B 1 propagating inside the integrating portion 102 , the ratio of the length L 1 of said integrating portion 102 to the thickness d 1 of said integrating portion 102 may be greater than or equal to 10, preferably greater than 50 (see also FIGS. 4 and 5 ). Said ratio may even be greater than or equal to 200 to attain a high degree of homogenization.

As the integrating portion 102 and the out-coupling portion 30 are implemented on the same substrate 7 , the optical coupling between the integrating portion 102 and the out-coupling portion 30 is almost perfect. Consequently, the thickness d 1 may be reduced without compromising the optical coupling efficiency between the integrating portion and the out-coupling portion 30 . The size of the illuminating unit 100 may be kept compact. There is not need to align the integrating portion 102 with respect to the substrate 7 .

Directions SX, SY and SZ are orthogonal. The surfaces 41 , 42 of the substrate 7 may be substantially parallel to a plane defined by the directions SX and SZ (See FIG. 10 d ).

The width of the substrate 7 , and in particular the width of the integrating portion 102 (in the direction SZ) may be greater than or equal to 10 times the thickness d 1 of said integrating portion 102 in order to allow lateral spreading of the in-coupled light B 1 .

In particular, the display device 500 may comprise a polarizing beamsplitter 250 , which is arranged to provide a substantially polarized illuminating beam B 3 by reflecting a predetermined polarization of out-coupled light beam B 2 . Light having the other polarization state may be transmitted through the beamsplitter 250 . The illuminating beam B 3 impinges on the pixels PX 1 of the modulator array 210 . Light B 4 is reflected from the pixels PX 1 towards the beamsplitter 250 . Light reflected from a polarization-rotating pixel PX 1 may be transmitted through the beamsplitter 250 providing a transmitted beam B 5 . The imaging optics 280 focuses or collimates the light B 5 , providing a focused or collimated beam B 6 . Light rays reflected from those pixels which maintain the original polarization of the light B 3 do not pass through the beamsplitter 250 to the imaging optics 280 , but are reflected towards the illuminating unit 100 again.

In particular, the beamsplitter 250 , the modulator array 210 , and the imaging optics 280 may be arranged so that the optical axis AX 1 of the imaging optics 280 passes approximately through the center of the active area of the modulator array 210 , such that the modulator array 210 is substantially perpendicular to the axis AX 1 , and such that the reflecting plane of the beamsplitter 250 is substantially at a 45 degree angle with respect to said optical axis AX 1 .

Referring to FIG. 2 a , the modulator array 210 may be a liquid crystal on silicon array, i.e. an LCOS-array. The LCOS array comprises a reflective layer 208 and liquid crystal layer 209 .

Referring to FIG. 2 b , an image 605 may be formed on the modulator array 210 by changing the states of individual pixels PX 1 . The state of a pixel PX 1 may be changed e.g. by changing the orientation of liquid crystals by applying a voltage to electrodes.

The LCOS array is especially suitable for use in the arrangement shown in FIG. 1 . The LCOS array is polarization changing, and allows effective use of the polarizing beamsplitter 250 . The polarizing beamsplitter 250 allows substantially perpendicular illumination. Consequently, a light ray, which is transmitted through a miniature portion on the liquid crystal layer 209 , is reflected back substantially through the same miniature portion. Thus, the interfering effect of adjacent pixels is minimized when compared to a situation in which the illuminating rays impinge on the modulator array 210 e.g. at an angle of 30 degrees.

The device 500 may also arranged in an off-axis configuration comprising a first polarizer to polarize the illuminating beam B 3 , and a second polarizer for the reflected beam B 4 . The modulator array 210 may be inclined with respect to the optical axis AX 1 of the imaging optics 280 .

The modulator array 210 may also be digital micromirror device (DMD), i.e. a micromirror array comprising a plurality of mechanically movable miniature mirrors. In that case the device 500 may be implemented without the polarizers.

The substrate 7 may comprise or consist of e.g. polycarbonate, polymethyl methacrylate (PMMA), or glass.

Referring to FIG. 3 a , the display device 500 may be an image projector. The imaging optics 280 may focus light B 6 on an external screen 800 in order to project a real image 810 to said screen. Light reflected from each pixel PX 1 of an image is substantially focused into a corresponding spot on the screen 800 . The distance between the device 500 and the screen may be e.g. several meters, and the displayed image 810 may be viewed by several persons.

Referring to FIG. 3 b , the display device 500 may be a virtual display. The imaging optics 280 may be arranged to collimate light reflected from each pixel PX 1 of an image. An image typically comprises several pixels PX 1 . The collimated beams B 6 corresponding to the several pixels, and which impinge on the eye E 1 of a viewer, create an impression of a virtual image 710 located at an infinite distance from the viewer (See FIG. 14 ).

The optical power level required in case of the image projector ( FIG. 3 a ) is by several orders of magnitude greater than in case of the virtual display ( FIG. 3 b ).

Referring to FIG. 4 , the illuminating unit 100 comprises a waveguiding substrate 7 . The substrate 7 has two surfaces 41 , 42 . The surfaces are separated by a substantially constant distance d 1 . The surfaces 41 , 42 may be substantially planar or curved. The substrate 7 may be e.g. cut from a sheet of plastics having substantially constant thickness d 1 . The substrate may even be flexible.

In case of substantially planar surfaces 41 , 42 , the surfaces 41 , 42 are substantially parallel. Thus, consecutive total internal reflections on the surfaces 41 , 42 do not substantially change the divergence of the beam B 1 propagating within the substrate 7 .

In case of the curved surfaces 41 , 42 , the surfaces 41 , 42 are substantially parallel in the local sense, i.e. locally parallel. In other words, those portions of the surfaces 41 , 42 which are opposite each other are substantially parallel.

Light B 0 provided by a light source 110 may be coupled into the substrate 7 through an edge 43 to form an out-coupled light beam B 2 , which may comprise light rays LR 2 a , LR 2 b , LRe. The edge 43 may be substantially perpendicular to the surfaces 41 , 42 . B 1 denotes in-coupled light waveguided within the substrate 7 . The in-coupled light B 1 is confined to said substrate 7 by total internal reflections (TIR) at said surfaces 41 , 42 . Light is coupled out of the substrate 7 by an out-coupling portion 30 . The out-coupling portion 30 may comprise e.g. a diffraction grating or a prism structure.

Lenses, mirrors and/or gratings may be positioned between the edge 43 and the light source 110 in order to modify intensity distribution of the in-coupled light B 1 . A lens surface or grating may be implemented directly on the edge 43 .

Two or more light sources 110 may be arranged side by side to emit light of different colors into the same substrate 7 .

Referring to FIG. 5 , light B 0 of the light source 110 may be coupled into the substrate 7 through one of the surfaces 41 , 42 by using an in-coupling portion 10 . The in-coupling portion 10 may be e.g. a diffraction grating or a prism structure. The surfaces 41 , 42 are separated by the substantially constant distance d 1 . The surfaces 41 , 42 may be substantially planar or curved.

The illuminating unit 100 may be a diffractive beam expander 50 comprising a diffractive in-coupling portion 10 and a diffractive out-coupling portion 30 .

L 1 denotes the distance between the in-coupling portion 10 and the out-coupling portion 30 , i.e. the length of the integrating portion 102 ( FIG. 1 ). d 1 denotes the thickness of the substrate 7 . The ratio L 1 /d 1 may be selected to be e.g. greater than or equal to 200 so as to effectively smooth out spatial variations in the intensity of the in-coupled beam B 1 .

Lenses, mirrors and/or gratings may be positioned between the light source 110 and the in-coupling portion 10 in order to modify intensity distribution of the in-coupled light B 1

Two or more light sources 110 may be arranged side by side to emit light of different colors into the same substrate 7 .

The substrate 7 of the illuminating unit 100 may be planar or slightly curved. The substrate 7 may have a substantially constant thickness d 1 at least over the integrating portion 102 and the out-coupling portion 30 . The substrate 7 may be e.g. cylindrically curved. The substrate 7 may be e.g. cut from a sheet of constant thickness d 1 . The in-coupling portion 10 and the out-coupling portion 30 may be implemented e.g. by embossing on the surfaces 41 , 42 of the substrate.

Referring to FIG. 6 , a diffractive beam expander 50 may be arranged to expand the dimensions of a narrow light beam B 0 in two directions. A narrow beam B 0 emitted by the light source 110 has a dimension W 0 in the direction SZ and a dimension H 0 in the direction SX. An in-coupling grating 10 provides an in-coupled beam B 1 by diffracting light of the beam B 0 . An intermediate grating 20 provides an expanded beam V 1 by diffracting light of said in-coupled beam B 1 . Also the expanded beam is waveguided within the substrate 7 . The expanded beam V 1 has a greater dimension than the narrow beam B 0 in the direction SX. The out-coupling grating 30 provides an out-coupled illuminating beam B 2 by diffracting light of the expanded beam V 1 . The dimensions H 2 and W 2 of the out-coupled beam B 2 are greater than the dimensions of the original narrow beam B 0 . The gratings 10 , 20 , 30 may comprise a plurality of substantially linear diffractive features, e.g. ridges and grooves.

U.S. Pat. No. 6,580,529 discloses such a diffractive beam expander for expanding an exit pupil in two dimensions. The patent discloses also a display device based on said beam expander.

Patent application US 2006/0126182 discloses a diffractive beam expander comprising a first diffractive element to couple light into a substrate, a second diffractive element to couple light out of the substrate, and an intermediate diffractive element to diffract in-coupled light towards the second diffractive element. The intermediate diffractive element has a substantially periodic pattern composed of substantially linear elements for producing conical diffraction.

Referring to FIG. 7 , a diffractive beam expander 50 may comprise a first deflecting portion 21 a and a first restoring portion 21 b . The deflecting portion 21 a provides a deflected beam U 1 by diffracting light of the in-coupled beam B 1 . The restoring portion 21 b provides a restored beam V 1 by diffracting light of said deflected beam U 1 . The beams U 1 and V 1 are waveguided within the substrate 7 . The restored beam V 1 together with an undiffracted part of the original in-coupled beam B 1 forms an enlarged beam, which has a greater dimension in the direction SZ than the original in-coupled beam B 1 . The out-coupling grating 30 provides expansion also in the direction SX.

The diffractive beam expander 50 may further comprise a second deflecting portion 22 a and a restoring portion 22 b . The second deflecting portion 22 a provides a second deflected beam U 2 , and the second restoring portion 22 b provides a second restored beam V 2 . The restored beams V 1 and V 2 form an expanded beam which may be coupled out of the substrate by the out-coupling grating 30 .

The portions 21 a and 22 b may be on a first side of a reference plane PLN 1 , and the portions 22 a and 21 b may be on a second side of a reference plane PLN 1 . The reference plane PLN 1 is substantially perpendicular to the gratings 10 , 30 , and consequently it appears as a line in FIG. 7 . The deflected beams U 1 and U 2 may pass through said plane PLN 1 .

The gratings 10 , 21 a , 21 b , 22 a , 21 b , 30 may comprise a plurality of substantially linear diffractive features, e.g. ridges and grooves.

The diffractive beam expander 50 of FIG. 7 may also be implemented without the deflecting and restoring gratings 21 a , 21 b , 22 a , 21 b . In that case the in-coupling grating 10 may have curved diffractive features. To provide beam expansion in two directions. Also the out-coupling grating 30 may have curved diffractive features.

Referring to FIG. 8 a , the illuminating unit 100 may comprise two or more stacked substrates 7 a , 7 b , 7 c . Light provided by the out-coupling portion 30 b of the second substrate 7 b may be arranged to pass through the first substrate 7 a , in particular through the out-coupling portion 30 a of said substrate 7 a . In particular, the out-coupling portion 30 a may be at least partially light-transmitting at the wavelengths provided by the second out-coupling portion 30 b.

Light provided by the out-coupling portion 30 c of a third substrate may be arranged to pass through the substrates 7 a and 7 b . Light for the substrates may be provided using different light sources 110 a , 110 b , 110 c . The first substrate 7 a may be arranged to transmit red color, the second substrate 7 b may be arranged to transmit green color, and the third substrate 7 c may be arranged to transmit blue color.

The light sources 110 a , 110 b , 110 c may be arranged to emit light in sequential order, and the modulator array 210 may be synchronized with the operation of the light sources 110 a , 110 b , 110 c in order to display multi-color images.

Light sources having different colors may also be arranged to emit light into the same substrate 7 .

Referring to FIG. 8 b , light may be coupled into the substrates 7 a , 7 b , 7 c by using in-coupling portions 10 a , 10 b , 10 c.

FIG. 9 a shows illumination of a pixel PX 1 which is located at the center of the modulator array 210 . The angle between the reflecting surface of the beamsplitter 250 and the optical axis AX 1 is substantially equal to 45 degrees. The out-coupling portion 30 provides light rays LR 2 a and LR 2 b . The beamspitter 250 reflects and polarizes the light of the rays LR 2 a and LR 2 b and provides polarized rays LR 3 a and LR 3 b . The pixel PX 1 reflects the light of the rays LR 3 a and LR 3 b and provides reflected rays LR 5 a and LR 5 b . Both reflected rays LR 5 a and LR 5 b impinge on the aperture of the imaging optics 280 .

(x 1 ,z 1 ) denotes the coordinates of a first light-emitting point on the out-coupling portion 30 . (x 2 ,z 2 ) denotes a second light-emitting point on the out-coupling portion 30 . The light ray LR 2 a is emitted from the first point and the ray LR 2 b from the second point. The light ray LR 2 a has a zenith angle θ LR2a , and an azimuth angle θ LR2a (not shown in FIG. 9 a ). The light ray LR 2 b has a zenith angle θ LR2b , and an azimuth angle φ LR2b (not shown in FIG. 9 a ).

FIG. 9 b shows illumination of a second pixel PX 2 which is located at the edge of the modulator array 210 . The beamspitter 250 reflects and polarizes the light of the rays LR 2 c and LR 2 d and provides two polarized rays LR 3 c and LR 3 d . The pixel PX 1 reflects the light of the rays LR 3 c and LR 3 d and provides reflected rays LR 5 c and LR 5 d . However, the reflected ray LR 5 c does not impinge on the aperture of the imaging optics 280 . Consequently, optical power of the ray LR 5 c is wasted, and the ray LR 5 c may even cause harmful stray light effects.

In case of FIG. 9 b , only a part of the optical power of the illuminating beam B 2 , B 3 contributes to the forming of the image. This may cause relative darkening of the peripheral portions of a displayed image. This phenomenon is known as “vignetting”.

Vignetting and/or stray light effects may be reduced by tailoring the angular out-coupling efficiencies at different locations on the out-coupling portion and/or the lateral intensity distribution of the in-coupled beam B 1 in the direction SZ.

By comparing FIGS. 9 a and 9 b , it may be noticed that the optical power of the ray LR 2 d should be higher than the optical power of the ray LR 2 b in order to provide substantially similar brightness at the center of the displayed image and at the periphery of the displayed image. This may be attained by selecting a higher diffraction efficiency, at the location (x 1 ,z 1 ) in the direction of the ray LR 2 d than in the direction of the ray LR 2 b . x 1 denotes a coordinate in the direction SX and z 1 denotes a coordinate in the direction SZ ( FIGS. 10 a and 10 d ).

The optical power of the ray LR 2 c appears to be wasted. Consequently, the diffraction efficiency in the direction LR 2 c may be selected to be substantially lower than in the direction LR 2 a , at the location (x 2 ,z 2 ). x 2 denotes a coordinate in the direction SX and z 2 denotes a coordinate in the direction SZ ( FIGS. 10 a and 10 d ). In particular, the diffraction efficiency in the direction LR 2 d may be selected to be substantially equal to zero in order to avoid losing energy and in order to minimize stray light effects.

The light ray LR 2 c has a zenith angle θ LR2c , and an azimuth angle φ LR2c (not shown in FIG. 9 a ). The light ray LR 2 d has a zenith angle θ LR2d , and an azimuth angle φ LR2d (not shown in FIG. 9 a ).

Referring to FIG. 10 a , the out-coupling portion 30 may comprise a plurality of out-coupling elements F 30 . The location of each feature may be specified by the coordinates x and z. The elements F 30 may be e.g. reflective or refractive prisms, diffractive gratings, or holograms.

The out-coupling elements F 30 change the direction of the waveguided light B 1 so that it may escape through the upper 41 and/or lower surface 42 of the substrate 7 .

The spatial distribution of out-coupling efficiency over said out-coupling portion 30 may be non-uniform in order to provide advantageous spatial and/or directional radiance distribution.

The efficiency of coupling light out of the substrate 7 may be selected to be greater near the periphery of the out-coupling portion 30 than near the center of the out-coupling portion e.g. in order to reduce vignetting.

Referring to FIG. 10 b , the out-coupling elements F 30 may be prisms. The height h 1 of the prisms may be lower near the center of said out-coupling portion 30 than near the periphery of said out-coupling portion 30 in order to tailor the spatial and directional radiance distribution provided by the out-coupling portion 30 , e.g. in order to reduce vignetting.

The surface of the substrate 7 between adjacent prisms may be substantially flat. Consequently, the fractional area covered by prisms may be smaller than 100%, e.g. in the range of 10% to 90%. The fractional area covered by prisms on an unit area at a predetermined location (x,z) means the ratio of summed base area of said prisms on said unit area to the whole area of said unit area.

The out-coupling portion 30 may comprise prisms which are arranged such that the fractional area covered by prisms is lower near the center of said out-coupling portion 30 than near the periphery of said out-coupling portion 30 e.g. in order to reduce vignetting.

The prisms may also be reflective. For example, inclined facets of the prisms may be coated with a reflective coating, or arranged such that light may be reflected by total internal reflection in a predetermined direction.

Referring to FIG. 10 c , the out-coupling portion 30 may comprise diffractive features, in particular diffractive grooves and/or ridges. The out-coupling elements F 30 may be zones which comprise diffractive features, in particular diffractive grooves and/or ridges. The out-coupling elements F 30 may have different diffractive properties in order to tailor the spatial and directional radiance distribution provided by the out-coupling portion 30 . The out-coupling elements F 30 may be arranged on the out-coupling portion 30 to form a substantially continuous diffractive surface.

The out-coupling elements F 30 may comprise diffractive features such that the diffraction efficiency of said out-coupling portion 30 is lower near the center of said out-coupling portion 30 than near the periphery of said out-coupling portion 30 .

The diffraction efficiency of an unit area, in a predetermined diffraction order, means the ratio of out-coupled optical power diffracted in said diffraction order from said unit area to optical power impinging on said unit area.

Each element F 30 may have its own angular diffraction efficiency. For example, grating period, profile form, profile height, blaze angle, refractive index difference and/or fill factor of a diffractive element F 30 may be selected to implement a desired angular distribution of radiance at a predetermined location (x,z) on the out-coupling portion 30 .

In particular, a greater out-coupling efficiency near the periphery may be implemented e.g. so that out-coupling elements F 30 may have diffractive ridges, wherein the height of said diffractive ridges is smaller near the center of said out-coupling portion 30 than near the periphery of said out-coupling portion 30 .

The radiance of an element F 30 , and consequently also the local out-coupling efficiency may also be adjusted e.g. by choosing the area of an individual element F 30 with respect to the total area of the out-coupling portion 30 . Thus, the out-coupling portion 30 may comprise a plurality of small grating areas having a substantially smooth non-diffracting surface between said grating areas.

A zenith angle θ of a light ray or a light beam is the angle between the direction of said light ray and the direction −SY. The direction −SY is opposite the direction SY. The light ray has a projection on a plane defined by the directions SX and SZ. An azimuth angle φ is the angle between said projection PR 2 and the direction SX.

FIG. 10 d shows zenith θ LR2 and azimuth φ LR2 angles of a light ray LR 2 . The light ray LR 2 may be provided by an out-coupling element F 30 having coordinates X and Z. The zenith angle θ LR2 is the angle between the direction of the light rays LR 2 and the direction −SY. The direction −SY is opposite the direction SY. The light ray LR 2 has a projection PR 2 on a plane defined by the directions SX and SZ. The azimuth angle φ LR2 is the angle between said projection PR 2 and the direction SX.

FIG. 11 a shows, by way of example, the radiance L(x 2 ,z 2 ,θ LR2 , φ LR2 ) of a light-out-coupling element F 30 in the direction specified by the zenith angle θ LR2 and azimuth angle φ LR2 at the location (x 2 ,z 2 ) of FIGS. 9 a and 9 b , as a function of the zenith angle θ LR2 of an out-coupled light ray. Radiance L means the power emitted per unit solid angle per unit source area. The unit of radiance L is Watts per steradian per square metre (Wsr −1 m −2 ).

As was noticed from FIG. 9 b , the light of the light ray LR 2 c will not reach the aperture of the imaging optics 280 , and therefore the light ray LR 2 d should have an increased power to reduce vignetting. The radiance at the angle θ LR2d may be arranged to be higher than at the angle θ LR2b in order to reduce vignetting.

FIG. 11 b shows, by way of example, the radiance L(x 1 ,z 1 ,θ LR2 , φ LR2 ) of a light-out-coupling element F 30 at the location (x 1 ,z 1 ) of FIGS. 9 a and 9 b as a function of the zenith angle θ LR2 of an out-coupled light ray. As was noticed from FIG. 9 b , light of the light ray LR 2 c will not reach the aperture of the imaging optics 280 , and therefore the radiance L may have a low value in the direction corresponding to said light ray LR 2 c , i.e. at the zenith angle θLR 2 c . The radiance at the angle θLR 2 c may be arranged to be substantially lower than at the angle θLR 2 a.

In particular, the out-coupling efficiency E(x,z,θ LR2 ,φ LR2 ) of coupling light out of the substrate at the location (x,z) in the direction specified by the angles θ LR2 ,φ LR2 may be selected such that the desired form of the radiance curve may be attained. The efficiency E(x,z,θ LR2 ,φ LR2 ) is the ratio of a first optical power to a second optical power, wherein said first optical power is an optical power impinging on a small area dxdz on the substrate side, and said second optical power is the optical power of light coupled out of the substrate from said small area dxdz in the direction having a zenith angle θ LR2 , and azimuth angle φ LR2 .

The efficiencies E(x,z,θ LR2 ,φ LR2 ) of the out-coupling elements F 30 for coupling light out of the substrate may be selected such that an optical power P TOT illuminating a pixel PX 1 near the center of the modulator array 210 is lower than an optical power P TOT illuminating a pixel PX 2 near the edge of said modulator array 210 .

In particular, the efficiencies E(x,z,θ LR2 ,φ LR2 ) of the out-coupling elements F 30 for coupling light out of the substrate may be selected such that more than 60% of the optical power P TOT illuminating a pixel PX 2 at the edge of said modulator array 210 is reflected towards an aperture of the imaging optics 280 . Even more than 80% of the light of the peripheral pixel PX 2 may be reflected towards the aperture of the imaging optics 280 .

Referring to FIG. 12 a , the in-coupled beam B 1 may comprise a plurality of light rays LR 11 , LR 12 , LR 13 , each having their own zenith angles θ LR11 , θ LR12 , θ LR13 . The light rays shown in FIG. 11 impinge on the same out-coupling element F 30 at a location (x,z). The out-coupling element F 30 may be arranged to couple only light of the ray LR 12 out of the substrate, and reflect the remaining rays LR 11 and LR 13 back into the substrate 7 substantially without reducing their optical power. In other words, the out-coupling element F 30 may be arranged to couple light out of the substrate direction-selectively.

The light beam B 1 may comprise a nearly infinite number of light rays LR 11 , LR 12 , LR 13 propagating in different directions.

FIG. 12 b shows, by way of example, the radiant emittance M(x,z) as a function of the zenith angle θ LR1 of a light ray impinging on an out-coupling element F 30 at a location (x,z). Radiant emittance M means the optical power emitted from a surface. The unit of the emittance M is Watts per square meter (W/m2). It is assumed hypothetically in FIG. 12 b that the optical power of the impinging ray is independent of the zenith angle, and that only one ray or a perfectly collimated beam impinges on the out-coupling element F 30 at a time. The radiant emittance M may have a maximum value for a light ray LR 12 having a zenith angle θ LR12 , and a lower value for rays having zenith angles θ LR11 and θ LR12 .

The out-coupling elements F 30 may be arranged to direction-selectively couple light of a light ray LR 12 propagating in a predetermined direction within said substrate 7 out of said substrate, wherein said out-coupling elements F 30 are arranged to couple light propagating in other directions out of said substrate 7 to a lesser degree.

Referring to FIG. 13 , the device 500 , which comprises at least the illumination unit 100 , the modulator array 210 , and the imaging optics 280 , may also be called as an optical engine. A display device 501 may comprise a diffractive beam expander 300 to expand the exit pupil of the optical engine 500 . Consequently, the viewer has a considerable freedom to move the display device 501 with respect to his eye E 1 in the directions SX, SY, and SZ, while still being able to see the whole displayed virtual image. The diameter of the aperture of the imaging optics 280 may also be considerably reduced. Consequently, the device 501 may be implemented using smaller, lighter and possibly cheaper lenses.

Light reflected from a predetermined pixel PX 1 is collimated by the imaging optics 280 to provide a substantially collimated beam B 6 propagating in a predetermined direction. Light of the beam B 6 is coupled into the substrate 307 of the beam expander 300 by an in-coupling grating 310 . An out-coupling grating 330 provides an output beam B 7 by diffracting light of the in-coupled beam out of the substrate 307 . The output beam B 7 is also substantially collimated and substantially parallel to the beam B 6 . Consequently, a plurality of enlarged beams B 7 corresponding to a plurality of pixels PX 1 on the modulator array 210 provide the same virtual image as the beams B 6 provided by the imaging optics 280 . The gratings 310 , 330 of the diffractive beam expander 300 may be arranged, for example, as shown in FIG. 7 .

The diffractive beam expander 300 may be e.g. an expander disclosed in the patent application US 2006/0126182.

The diffractive beam expander 300 may be e.g. an expander disclosed in the patent application PCT/FI2007/050322.

The diffractive beam expander 300 may be e.g. an expander disclosed in the patent application PCT/FI2006/050590.

Referring to FIG. 14 , a display device 501 may also be bi-ocular in order to display virtual images to both eyes E 1 , E 2 of a viewer. The beams B 7 provide for a viewer an impression of a virtual image 710 displayed at an infinite distance from the viewer.

There are several ways to implement a bi-ocular display. The substrate 307 of the diffractive beam expander 300 shown of FIG. 13 may comprise a second out-coupling grating 330 b ( FIG. 14 ) to provide enlarged beams B 7 also for the left eye E 2 of the viewer. The beam B 6 shown in FIG. 13 may be distributed to two separate diffractive beam expanders 300 , each having its own out-coupling grating 330 . Two optical engines 500 may be attached to each other, wherein each optical engine 500 has its own diffractive beam expander 300 . Two optical engines 500 may be attached to each other without a diffractive beam expander 300 .

The use of two optical engines 500 allows displaying stereo images.

Referring to FIG. 15 , the display device 500 may comprise a curved polarizing beam splitter 250 in order to reduce the size of the device 500 and/or in order to improve the image quality.

Light rays LR 2 a , LR 2 b coupled out of the substrate 7 may impinge on the curved beam splitter 250 . A part of the light is transmitted through the splitter and a part of the light is transmitted towards the modulator array 210 . Light rays LR 3 a , LR 3 b may impinge on a pixel PX 1 and may be reflected from said pixel, providing reflected rays LR 4 a , LR 4 b . If the pixel PX 1 has changed the polarization of reflected light, then a part of the light of the rays LR 4 a , LR 4 b may be transmitted through the splitter 250 forming rays LR 5 a , LR 5 b . Light of the rays LR 5 a , LR 5 b may be focused or collimated by the imaging optics 280 to provide image-forming light rays LR 6 a , LR 6 b.

The angular distribution of radiance and/or spatial distribution of radiance over the out-coupling portion 30 may be selected such that optical power P TOT illuminating a pixel PX 1 near the center of the modulator array 210 is lower than optical power P TOT illuminating a pixel PX 2 near the edge of said modulator array 210 , in order to reduce or eliminate vignetting.

The angular distribution of radiance and/or spatial distribution of radiance on the out-coupling portion 30 may be selected such that a greater fraction of optical power reflected from the peripheral pixels PX 2 impinges on the effective aperture of the imaging optics 280 , when compared with a situation when the spatial intensity distribution on the out-coupling portion 30 is uniform and when each point of the out-coupling portion 30 provides substantially the same angular radiance distribution.

The curved beams splitter 250 may be curved in one dimension, i.e. cylindrically curved. In that case the imaging optics 280 may comprise cylindrical optics in order to form a sharp image.

The curved beams splitter 250 may be curved in two dimensions, i.e. it may be doubly curved. The splitter 250 may form a part of a spherical, ellipsoid or paraboloid surface.

Display devices comprising a curved polarizing beam splitter has been described e.g. in U.S. Pat. No. 6,486,997.

Display devices comprising a curved polarizing beam splitter has been described e.g. in U.S. Pat. No. 7,206,134.

The display device 500 may further comprise e.g. a data processing unit, memory and communications unit to provide access to a mobile telephone network, internet or local area network. The display device 500 may be or may be a part of a device selected from the following list: a display module connectable to a further device, portable device, device with wireless telecommunicating capabilities, imaging device, mobile phone, gaming device, music recording/playing device (based on e.g. MP3-format), remote control transmitter or receiver, navigation instrument, measuring instrument, target finding device, aiming device, navigation device, personal digital assistant (PDA), communicator, portable internet appliance, hand-held computer, accessory to a mobile phone.

The drawings are schematic. For the person skilled in the art, it will be clear that modifications and variations of the devices and methods according to the present invention are perceivable. The particular embodiments described above with reference to the accompanying drawings are illustrative only and not meant to limit the scope of the invention, which is defined by the appended claims.