WO2022069727A1 - Optical projection with combined beams - Google Patents

Optical projection with combined beams Download PDF

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Publication number
WO2022069727A1
WO2022069727A1 PCT/EP2021/077147 EP2021077147W WO2022069727A1 WO 2022069727 A1 WO2022069727 A1 WO 2022069727A1 EP 2021077147 W EP2021077147 W EP 2021077147W WO 2022069727 A1 WO2022069727 A1 WO 2022069727A1
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WO
WIPO (PCT)
Prior art keywords
light
beams
image plane
imager
optical
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
PCT/EP2021/077147
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English (en)
French (fr)
Inventor
Dries Jan DOORNAERT
Bart Henri Johanna Maximus
Raveen Kumaran
Dirk Leontina Maes
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Barco NV
Original Assignee
Barco NV
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Filing date
Publication date
Application filed by Barco NV filed Critical Barco NV
Priority to US18/247,249 priority Critical patent/US12591170B2/en
Priority to JP2023520063A priority patent/JP7646985B2/ja
Priority to EP21786463.6A priority patent/EP4222557A1/en
Priority to CA3197042A priority patent/CA3197042A1/en
Priority to CN202180076248.4A priority patent/CN116547603A/zh
Publication of WO2022069727A1 publication Critical patent/WO2022069727A1/en
Anticipated expiration legal-status Critical
Priority to JP2024212183A priority patent/JP2025060627A/ja
Ceased legal-status Critical Current

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Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B21/00Projectors or projection-type viewers; Accessories therefor
    • G03B21/14Details
    • G03B21/20Lamp housings
    • G03B21/2006Lamp housings characterised by the light source
    • G03B21/2013Plural light sources
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B21/00Projectors or projection-type viewers; Accessories therefor
    • G03B21/005Projectors using an electronic spatial light modulator but not peculiar thereto
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B21/00Projectors or projection-type viewers; Accessories therefor
    • G03B21/14Details
    • G03B21/20Lamp housings
    • G03B21/2006Lamp housings characterised by the light source
    • G03B21/2033LED or laser light sources
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B21/00Projectors or projection-type viewers; Accessories therefor
    • G03B21/14Details
    • G03B21/20Lamp housings
    • G03B21/2053Intensity control of illuminating light
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B21/00Projectors or projection-type viewers; Accessories therefor
    • G03B21/14Details
    • G03B21/20Lamp housings
    • G03B21/2066Reflectors in illumination beam
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B21/00Projectors or projection-type viewers; Accessories therefor
    • G03B21/14Details
    • G03B21/20Lamp housings
    • G03B21/208Homogenising, shaping of the illumination light

Definitions

  • the invention relates to combining beams of light.
  • One example application of the invention is to illuminate a projector imager.
  • This invention has many aspects. These include:
  • Some aspects of the invention supply light for high intensity highlights in projected images by combining plural light beams in which light is steered to highlight locations in an image plane.
  • the plural light beams may illuminate the same set of one or more imagers.
  • An advantage of some such embodiments is to substantially increase a light budget available for highlighting.
  • An advantage of some such embodiments is increased reliability of spatial phase modulators that may be used for light steering which may be achieved by splitting optical power among plural phase modulators.
  • the technology described herein may be applied for example to provide a projected image having highlights with a total light flux budget of at least 4000 lumen over a 15000 lumen baseline in a large size cinema screen.
  • Some aspects of the invention provide an optical assembly comprising plural spatial phase modulators, each illuminated by a light beam from a highly collimated light source.
  • a control system may set each of the phase modulators to apply phase shifts so as to steer light to a common target or image plane.
  • the light steered by each phase modulator may provide a light field at the target that includes areas of greater light intensity and areas of less light intensity.
  • the light fields may overlap at the target and may be co-registered so that corresponding areas in the overlapping light fields are superposed.
  • the combination of the light steered by the different phase modulators may be effected by directing light from the different phase modulators to converge at an acute angle ⁇ .
  • the combined light field at the target may, for example illuminate an imager (such as a spatial amplitude modulator of any suitable type).
  • angles between the optical axes of each phase modulator to the common target image are smaller than 1/2, 1/3, 1/4, 1/5, 1/6, etc. of a maximum boundary of an acceptance angle of an optical system that includes the imager.
  • at least one optical diffuser is provided in an optical path between the common target and the imager. The optical diffuser may increase an angular spread of the combined steered light.
  • One aspect of the invention provides a projection system comprising one or more light sources operative to emit light and optical elements arranged to direct the light from the one or more light sources in two or more separate collimated beams.
  • Each of the beams illuminates the active area of the imager.
  • the beams converging onto the image plane at an acute angle not exceeding 10 degrees.
  • the optical elements include a spatial light modulator arranged to modulate the light of at least one of the beams.
  • At least one modulated light beam (e.g. a light beam that is modulated by a spatial phase modulator) is combined with a base light beam (e.g. a beam that provides uniform illumination).
  • the modulated light beam and the base light beam preferably have similar coverage in angular space. This advantageously allows for light from both the modulated light beam and the base light beam to be diffused using the same optical diffuser thereby increasing the angular extent of the combined modulated and base light beams without severe loss of light outside of an acceptance angle of a downstream optical system.
  • a holographic diffuser is provided in an optical path of the base light beam.
  • the holographic diffuser acts as a static or “frozen” phase grating.
  • a base light beam having coverage in angular space that is similar to that of a modulated light beam is generated by collecting light from a separate light source (e.g. a laser light source) into an optical fiber (e.g. an optical fiber having a numerical aperture (“NA”) 0.2 and about 2x1 mm cut). Light from the optical fiber and light from the modulated light beam may be projected (e.g. imaged) onto a common target image plane.
  • a separate light source e.g. a laser light source
  • NA numerical aperture
  • Figure 1 is a schematic illustration of a projection system according to an example embodiment of the invention.
  • Figure 2 is a schematic representation of an example angular space.
  • Figure 3A is a schematic representation of an example arrangement of footprints in an angular space with two beams.
  • Figure 3B is a schematic representation of an example arrangement of footprints in an angular space with four beams.
  • Figures 3C to 3H are schematic representations of example arrangements of footprints in an angular space.
  • Figure 4 is a schematic illustration of a projection system according to an example embodiment of the invention.
  • Figure 5A is a schematic illustration of an optical arrangement according to an example embodiment of the invention.
  • Figure 5B is a schematic illustration of an optical arrangement according to an example embodiment of the invention.
  • Figure 5C is a plan view of an optical arrangement according to an example embodiment of the invention.
  • Figure 5D is a schematic side elevation view of an optical arrangement according to an example embodiment of the invention.
  • Figure 6A is a schematic illustration of an optical arrangement according to an example embodiment of the invention.
  • Figure 6B schematically illustrates an example light path.
  • Figure 7A is a schematic illustration of an optical arrangement according to an example embodiment of the invention.
  • Figure 7B is a schematic illustration of an optical arrangement according to an example embodiment of the invention.
  • Figure 7C is a schematic illustration of an optical arrangement according to an example embodiment of the invention.
  • Figures 8A and 8B are top and side elevation views of an optical assembly according to an example embodiment of the invention.
  • Figure 9 is a schematic illustration of an optical apparatus according to an example embodiment of the invention.
  • imager is any device that is operable to impart a desired image (an image may be any pattern) to a beam of light.
  • a spatial light modulator may be used as an imager.
  • an imager may be used to modulate light incident from one or more light sources according to image data to project images according to the image data onto a screen.
  • spatial light modulator or “SLM” is a device that operates to apply different alterations to a property of light at different locations.
  • a SLM comprises an array of controllable elements or “pixels” that are individually operable to alter a property of light at a corresponding pixel location.
  • Properties of light that may be altered by a SLM include amplitude (light intensity), polarization and phase.
  • a SLM may modulate light that is transmitted through the SLM (e.g. light is incident on one face of the SLM and modulated light is emitted from another opposing face of the SLM).
  • a SLM may modulate light that is reflected from one face of the SLM (e.g. light is incident on one face of the SLM and modulated light is emitted from the same face of the SLM).
  • spatial amplitude modulator or “SAM” means a type of SLM that is operable to controllably alter amplitude of light.
  • SAMs are liquid crystal panels (also called LCDs), liquid crystal on silicon (LCoS) devices and digital mirror devices (“DMDs”) device.
  • a “spatial phase modulator” or “SPM” is a type of SLM that is operable to controllably alter the phase of light.
  • SPMs are LCoS devices and deformable mirrors. Some embodiments apply SPMs that have a pitch (i.e. a spacing between adjacent pixels in rows and/or columns) of about 10 ⁇ m or less.
  • Some SLMs operate only to modulate light amplitude. Some SLMs operate to modulate light phase. Some SLMs operate to modulate both light amplitude and light phase. Operation of some SLMs may be dynamically controlled in real time to:
  • f-number is a dimensionless number that can be used to characterize an optical system, f-number is a ratio of a focal length of the optical system to a diameter of an entrance pupil of the optical system.
  • “highlight beam” as used herein includes a beam of light that produces a non- uniform light field which includes one or more highlights at a target area.
  • the target area may for example be a screen or image plane onto which the highlight beam is incident.
  • the highlight beam may include areas having higher illumination intensities and areas having lower illumination intensities.
  • a highlight beam may for example result from light steering.
  • modulate means to vary a property of something.
  • Light can be modulated temporally or spatially.
  • Example properties of light that may be modulated include amplitude (brightness or intensity), phase and polarization state.
  • Spatial modulation of light can be achieved by selectively attenuating light at spatial locations (e.g. pixels) and/or by steering light.
  • Light steering involves steering light that would otherwise illuminate some spatial locations to other spatial locations.
  • Light steering may be achieved, for example, using variable lenses, variable mirrors and/or phase modulators (e.g. SPMs).
  • a phase pattern applied by a SPM may direct incident light to selected regions in an image plane. Interference between different parts of the directed light may result in some locations in the image plane having more light (i.e.
  • the phase pattern applied by the SPM may effectively steer or direct incident light away from certain regions in the image plane and/or steer or direct the incident light so that light is concentrated in certain regions in the image plane.
  • NA numerical aperture
  • acceptance angle for an optical system is a solid angle for which light rays entering the optical system with directions lying within in the solid angle will pass through the optical system. Solid angle may be measured in steradians.
  • etendue is a number that characterizes how "spread out" light is in area and angle. From the point of view of an optical system the etendue may be defined as the area of an entrance pupil of the optical system times the acceptance angle (as defined herein) of the optical system.
  • One aspect of this invention relates to combining plural light beams.
  • An example application is to combine beams of light from different light sources onto an imager in a light projection system.
  • some or all of the beams of light are modulated light.
  • the modulation of the modulated light may be time varying.
  • the techniques described herein are applied to produce dynamic illumination of a projector imager.
  • plural beams may be modulated and then combined to illuminate the imager with light that varies with intensity over an active surface of the imager.
  • the modulation applied to the beams may be controlled to match images that the imager is controlled to display.
  • the different beams of light may each be modulated by a different SLM and then combined as described herein to illuminate an imager (or combined for some other purpose).
  • the modulation of the modulated light of one or more beams may be set on a frame-by-frame or scene-by-scene basis.
  • the imager may be controlled by image data comprising video frames and the modulation applied to the beams may vary for the different frames.
  • one or more of the beams is a base light beam.
  • a base light beam may, for example, provide uniform illumination or illumination that is modulated in a static (non-time-varying) way.
  • the base beam(s) may supply enough light to an imager to project a desired image and one or more other beams may be modulated to supply extra light for highlights.
  • some or all of the combined beams of light are premodulated according to image data such that more light is provided in areas of an imager that correspond to brighter parts of an image to be displayed and less light is provided in areas of the imager that correspond to dimmer parts of the image.
  • An example application of the present technology is to illuminate at least one area of an imager or other target with modulated light that has high intensity at selected locations.
  • a SLM may have a reduced life span or may be damaged or destroyed if it is used to modulate light having an intensity greater than the SLM is designed for. This problem may be avoided by combining two or more lower-intensity beams of light that are each modulated by a separate SLM.
  • Another problem that may be avoided or reduced by combining plural beams of light is that it may be desirable to use plural lower-power light sources to generate the light instead of a single higher-power light source. This may be motivated for example by cost, availability, and/or thermal management issues.
  • the energy of the combined beams may be spread over the plural SLMs.
  • This arrangement may permit the use of less-expensive SLMs and/or simplify thermal management (e.g. to keep the operating temperature of the SLMs within a desired range) and/or extend the expected mean time between failures of the SLMs.
  • the plural SLMs comprise a total of N SLMs where each SLM is illuminated by, and is operable to modulate, a beam of light having an intensity that is about 1/N of the desired total averaged intensity of the combined beams.
  • Embodiments which combine light from plural SLMs can facilitate providing high intensity illumination of a projector imager with light of the wavelength and polarization of the beams.
  • Another problem is that, in some applications it is desirable to combine different beams of light that may not consistently or at all have different spectra or different polarizations that would permit combination of the different beams using conventional light combiners such as a dichroic mirror (which may be used to combine two beams of light having different wavelengths) or a polarizing beam splitter (which may be used to combine two beams of light having different polarizations).
  • a dichroic mirror which may be used to combine two beams of light having different wavelengths
  • a polarizing beam splitter which may be used to combine two beams of light having different polarizations.
  • a typical dichroic mirror cannot be used to efficiently combine beams that have the same wavelength or wavelengths that differ from one another by less than at least about 10nm.
  • a typical polarizing beam splitter which may be used to combine beams, operates most efficiently for orthogonal polarization states.
  • an imager is of a type that requires illumination by light having a specific polarization and it is desired to combine two light beams of the same colour and the same polarization.
  • different beams of light that have spectra and polarization states that are either the same or very close to the same or not consistently different (i.e. sometimes they are the same or nearly the same) may be combined.
  • the beams of light may all have the same specific polarization (e.g. a polarization direction matched with a polarization direction required by an imager).
  • the plural light beams may have the same or effectively the same wavelength and the same or a similar polarization.
  • effectively the same wavelength means that at least 95% or at least 98% of the energy of the plural light beams is within a wavelength band that spans no more than 30 nm or no more than 20 nm or no more than 10nm - thereby making it impractical and/or inefficient to use a dichroic element to efficiently combine the light beams.
  • first and second light beams have “similar polarization states” if a polarizing beam splitter set to pass a maximum amount of the light energy of the first light beam will also pass at least 50% or at least 70% or at least 85% of a maximum amount of the light energy of the second light beam that the polarizing beam splitter can pass- thereby making it impractical or inefficient to use a polarizing beam splitter as a light combiner to combine the light of the first and second light beams (without first adjusting polarization states of the first and/or second light beams to be more nearly orthogonal using additional optical elements).
  • the methods and apparatus described herein are applied to combine two beams of light that have the same circular polarization state.
  • the light of the beams that are combined is:
  • the beams that are combined comprise light that:
  • the light in the plural light beams is generated by plural corresponding light sources.
  • each of the light beams is spatially modulated by a corresponding monochrome SLM (i.e. a SLM that does not include colour filters to allow separate control of light of different primary colours).
  • a corresponding monochrome SLM i.e. a SLM that does not include colour filters to allow separate control of light of different primary colours.
  • the beams that are combined comprise light that is coherent.
  • the beams that are combined collectively comprise light of slightly different wavelengths.
  • the light may be light from laser sources that emit light of a combination of slightly different wavelengths. This helps in de-speckling.
  • SLMs are provided by phase modulators (e.g. SPMs) which are each controlled to steer light of one of the beams and different ones of the beams are made up of narrow band light having slightly different wavelengths.
  • SPMs phase modulators
  • Each of the SLMs may be controlled to steer the light of the corresponding beam based on the wavelength of light in the corresponding beam.
  • SLMs will work better (e.g. more efficiently steer the light) if the wavelengths of light in the corresponding beam are within a small range around the wavelength(s) that each of the SLMs is set for (e.g. within about ⁇ 10nm of a wavelength for which an SLM is set to steer).
  • Fig. 1 schematically illustrates a projection system 10 according to an example embodiment of the present invention.
  • First and second light beams 12A and 12B (generally and collectively beams 12) converge on an image plane 13 at a relative angle ⁇ .
  • may be a small angle.
  • a is about 10 degrees or less or about 5 degrees or less.
  • Each of light beams 12 arrives at image plane 13 at an angle that is within an acceptance angle 11 of an optical system of which image plane 13 is a part.
  • Light beams 12A and 12B respectively comprise light emitted by light sources 14A and 14B modulated by SLMs 15A and 15B (generally and collectively SLMs 15) and optionally passed through sets of one or more optical elements 16A and 16B.
  • Optical elements 16A and 16B may, for example comprise one or more lenses, mirrors, prisms, filters, free space, or the like.
  • SLMs 15 comprise spatial phase modulators that are controlled to exhibit patterns of phase shifts that cause light incident on SLMs 15 to be steered onto image plane 13. In this manner light incident on SLMs 15 may be concentrated at locations on image plane 13 at which greater light intensity is desired and/or steered away from locations on image plane 13 at which lower light intensity is desired.
  • Pixels of SLMs 15 may be set to present a phase pattern that causes a desired level of focus of a pattern of light onto image plane 13. In some such embodiments no additional focusing optics are provided to focus light from beams 12 onto image plane 13. Focus may be provided, for example by setting pixels of the phase modulators to emulate a focusing lens in combination with optics for desired light steering.
  • a control system for the phase modulators may comprise a data processor configured to deliver control signals to set pixels of the phase modulators to have a desired phase pattern.
  • the data processor may, for example process image data to determine a desired light steering pattern and drive the phase modulators to steer light to achieve the desired light steering pattern.
  • SLMs 15 are phase modulators and are controlled to steer light.
  • light steering using phase modulators may be implemented in any of the embodiments described herein.
  • each SLM 15 is individually driven and/or controlled.
  • light in different beams 12 corresponds to different colours (e.g. red, green, and blue).
  • Each colour may have a different target profile (e.g. different light intensity profile, different polarization, etc.).
  • light in different beams 12 has different intensity profiles (e.g. light in beam 12A has a first intensity profile and light in beam 12B has a second intensity profile different from the first intensity profile) that when combined result in a desired target light intensity profile.
  • Light in the different beams 12 which comprise different intensity profiles may be the same colour or may be of different colours.
  • a single SLM 15 or a set of SLMs 15 may be driven to produce a beam (or beams) 12 having the target characteristics desired for the corresponding colour.
  • a first set of SLMs 15 may be driven to produce a desired beam 12 corresponding to red light
  • a second set of SLMs 15 may be driven to produce a desired beam 12 corresponding to green light
  • a third set of SLMs 15 may be driven to produce a desired beam 12 corresponding to blue light.
  • the individual SLMs 15 may be driven collectively (i.e. all of the SLMs in the set are controlled in the same manner) or individually (i.e.
  • different SLMs 15 are controlled differently to create a combined image at image plane 13 that could not (or would be very difficult) to obtain if all SLMs 15 were controlled in the same manner or a single SLM 15 was used.
  • different SLMs 15 may be individually controlled to steer light in beams 12 differently to create a desired image at image plane 13.
  • light beams corresponding to the different colours are combined using dichroic combination (e.g. with dichroic mirrors which pass one wavelength band and reflect another). After such combination the light beams corresponding to the different colours will share a common optical axis and therefore the same spot location in angular space.
  • dichroic combination e.g. with dichroic mirrors which pass one wavelength band and reflect another.
  • Light in beams 12 combines to create a combined image at image plane 13 which is spaced apart from SLMs 15.
  • Light in beams 12 may have any combination of the characteristics described above. In some embodiments which have significant commercial application beams 12 comprise light having the same polarization and wavelength.
  • Light beams 12 overlap at image plane 13.
  • light beams 12 all illuminate the same area on image plane 13.
  • the light of each of light beams 12 is modulated with the same pattern and at image plane 13 light beams 12 are registered with one another so that in each part of the image formed at image plane 13 the same parts of the patterns in each of light beams 12 overlap and reinforce one another.
  • the image at image plane 13 provides dynamic illumination to an optical system 17.
  • optical system 17 comprises a projector imager 19.
  • SLMs 15 may be controlled to modulate the light in beams 12.
  • SLMs 15 may be each controlled to apply the same modulation to the corresponding beam 12.
  • the modulation may, for example be determined at least in part from image data defining an image to be displayed by projection system 10.
  • projector imager 19 is positioned very close to or coincides with image plane 13. In some embodiments projector imager 19 is positioned farther from image plane 13.
  • An optional optical system 18 comprising a set of one or more optical elements may be provided to direct light from image plane 13 to projector imager 19. The light incident on projector imager 19 is further modulated by projector imager 19 and projected by a projection lens 20.
  • light beams 12 are shaped to illuminate a region of a specific size and shape at image plane 13.
  • an eventual image may have a particular aspect ratio.
  • an aspect ratio (width:height) of 16:9 is common.
  • Light beams 12 may, for example have an aspect ratio of 16:9 when they arrive at image plane 13.
  • light beams 12 have an aspect ratio when they arrive at image plane 13 that matches an aspect ratio of imager 19.
  • angular footprints of SLMs 15 may vary dynamically. Additionally, or alternatively, the angular footprints may not be constant over an entire image on image plane 13. To minimize adverse effects, optical system 17 may be chosen to telecenter an average steering profile of SLMs 15.
  • the present technology is not limited to two beams 12 but may be practiced with any suitable number of beams 12 (e.g. 2, 3, 4, 5, 6, 7, 8 beams, etc.).
  • Angular space is a representation in which radial distance from an origin to a point represents an angle and an angular position of the point around the origin represents azimuth. Angular space may be defined for a particular optical system such that the origin corresponds to an optical axis of an entrance pupil of the optical system (e.g. optical system 17 described elsewhere herein).
  • Fig 2. shows an example angular space.
  • Origin 21 indicates an angle corresponding to an optical axis.
  • Dashed circles 22A, 22B, 22C represent specific angles relative to the optical axis. Different points around any one of dashed circles 22 correspond to different azimuthal directions.
  • circles 22A, 22B, 22C could respectively represent angles of one, two and three degrees relative to the optical axis or angles of two, four and six degrees relative to the optical axis.
  • Solid circle 23 indicates the boundary of the acceptance angle for the optical system. Light incident on an entrance pupil of the optical system at an angle greater than the acceptance angle indicated by circle
  • Light incident on an entrance pupil having the same incident angle relative to the optical axis as well as the same azimuthal angle corresponds to the same point in angular space (e.g. two parallel rays correspond to the same point in angular space, all points in real space that are located along a ray emanating from a center of the entrance pupil of the optical system may be associated to the ame point in angular space, etc.).
  • patches 24A and 24B respectively represent footprints in angular space of light rays that originate from SLM 15A and SLM 15B (collectively or generally footprints 24).
  • SLMs 15 can be positioned in real space so that their footprints 24 in angular space are close to one another. This can be done while allowing the positions of SLMs 15 to be separated by any distance in real space.
  • SLMs 15 may be tilted to be perpendicular to the direction of the corresponding beams 12. SLMs 15 may optionally all be tilted by the same amount or may individually be tilted by different amounts.
  • any number of SLMs 15 may be arranged in real space to deliver light to imager 19 (or another target) as long as their footprints 24 in angular space are within the acceptance angle of the optical system in question (e.g. optical system 17) - i.e. within circle 23 in the example of Fig. 2.
  • the angles between beams 12 e.g. angle ⁇
  • the angles between beams 12 may be chosen freely as long as the footprints 24 corresponding to beams 12 are within the acceptance angle e.g. the angle indicated by circle 23. In embodiments in which there are more than two beams 12, it is optional but not required that all of beams 12 combine with the same angle.
  • the angles between beams 12 may be selected to accommodate physical limitations of hardware and/or to facilitate desired image quality. For any number of beams 12 it is generally beneficial to arrange beams 12 so that the combining angle ⁇ is minimized. Combining beams 12 with a small angle ⁇ can help by:
  • Image quality improvements may be achieved by placing an optical diffuser 13A in or close to image plane 13.
  • Diffuser 13A scatters light that is incident on the diffuser through a range of angles.
  • the angular scattering characteristics of diffuser 13A may be chosen such that light from footprints 24 in angular space is mixed and angular space is more nearly filled, with minimal light falling outside the acceptance angle.
  • a strength of diffuser 13A may be selected to fill the acceptance angle (i.e. f- number) of the optical system (e.g. optical system 17) as described elsewhere herein.
  • projector system 10 comprises plural diffusers 13A.
  • a first diffuser may be placed in or close to image plane 13 and a second diffuser may be placed in or close to projector imager 19.
  • the light scattering provided by the plural diffusers 13A is additive (linearly or non-linearly). Different ones of the plural diffusers may be identical or may have at least one property that is different from other ones of the plural diffusers. A desired amount of light scattering may be achieved by scattering the light by plural diffusers 13A.
  • projector system 10 may comprise at least one additional optical relay between image plane 13 and projector imager 19.
  • a diffuser 13A may be placed in or close to a plane of the additional optical relay.
  • a projector system 10 comprises three different image planes 13 (e.g. one image plane for each of 3 colour channels).
  • projector system 10 may comprise a first image plane 13 corresponding to a red colour channel, a second image plane 13 corresponding to a green colour channel and a third image plane 13 corresponding to a blue colour channel.
  • a diffuser 13A may be placed in or close to each of the three image planes 13.
  • Such projector system 10 may also comprise an additional optical relay between the image planes 13 and projector imager 19.
  • the additional optical relay may combine the beams from the three image planes 13 (e.g. using dichroic mirrors).
  • a diffuser 13A is optionally provided in or close to a plane of the additional optical relay.
  • diffuser 13A is rotationally symmetric (i.e. it scatters light equally in all directions). In some other embodiments diffuser 13A is asymmetric and scatters light more strongly in some directions than in others.
  • Diffuser 13A may enhance safety by limiting the maximum radiance of light at any specific angle.
  • diffuser 13A may reduce laser speckle (when beams 12 comprise coherent light - e.g. were light sources 14 provide narrow band laser illumination).
  • diffuser 13A is an asymmetric diffuser.
  • such an asymmetric diffuser may scatter light less along an axis along which angular footprints are combined while scattering light more along an axis that is orthogonal to the axis along which the angular footprints are combined.
  • Figures 3A and 3B respectively illustrate example arrangements for footprints 24 in angular space for the case of two and four beams 12.
  • footprints 24A and 24B are spaced on either side of the origin in angular space.
  • the angular spread of light incident at image plane 13 is increased, resulting in enlarged effective footprints 25A and 25B which respectively correspond to footprints 24A and 24B.
  • Effective footprints 25A and 25B overlap at region 26.
  • footprints 24-1 through 24-4 are clustered near the origin in angular space.
  • the angular spread of light incident at image plane 13 is increased, resulting in enlarged effective footprints 25-1 through 25-4 which respectively correspond to footprints 24-1 through 24-4.
  • Effective footprints 25- 1 through 25-4 overlap at regions 26.
  • Figs. 3A and 3B illustrate that the presence of a diffuser 13A can increase coverage of angular space.
  • the overlap 26 between effective footprints 25 may be increased and the amount of the available angular space inside the acceptance angle (i.e. inside circle 23) is increased.
  • diffuser 13A scatters light through too large an angle ⁇ nd/or if footprints 24 are located too close to circle 23, a significant amount of light from beams 12 may be scattered at angles outside of the acceptance angle (for which angles the light cannot be effectively utilized).
  • FIGs. 3C through 3H illustrate one benefit of arranging beams 12 to converge with a small angle ⁇ and providing footprints 24 close to the origin in angular space.
  • 3D and 3E centers of footprints 24A and 24B are separated by angles a0, a1 and a2 respectively with ⁇ 0 ⁇ ⁇ 1 ⁇ ⁇ 2. This results in the highest angle (outermost) parts of footprints 24 being separated from circle 23 by corresponding angles d0, d1 and d2, where d0>d1>d2.
  • the proximity of footprints 24 to circle 23 limits the degree to which the acceptance angle (angular space inside circle 23) can be filled by providing a diffuser to spread light of beams 12 through a wider range of angles without wasting light by having some light spread to angles that are outside of the acceptance angle (outside of circle 23).
  • Fig. 3F shows that when footprints 24 are close to the origin in angular space it is possible to apply a diffuser that spreads light through a relatively wide angle to obtain effective footprints 25A and 25B that fill much of the angular space within circle 23 without significant spill over of light outside of circle 23. The spreading of light also causes a large area of overlap 26 between effective footprints 25A and 25B.
  • Fig. 3G shows that when footprints 24 are moved away from the origin in angular space the maximum angle of scattering that the diffuser can provide without spill over of light outside of circle 23 is reduced.
  • effective footprints 25A and 25B still fill much of the angular space within circle 23 but less completely than in Fig. 3F.
  • the area of overlap 26 between effective footprints 25A and 25B is also reduced relative to Fig. 3F.
  • Fig. 3H shows that when footprints 24 are still further from the origin of angular space the maximum angle of scattering that the diffuser can provide without spill over of light outside of circle 23 is reduced further to the point that effective footprints 25A and 25B no longer overlap and also effective footprints 25A and 25B occupy a relatively small part of the area within circle 23.
  • Increasing overlap in angular space between footprints 24 advantageously increases the likelihood of seeing a combination of light from the different SLMs 15 from an increased number of viewing angles. Typically, increasing overlap in angular space between footprints 24 additionally assists with reducing speckle. If the optical system (e.g. optical system 17) comprises an asymmetric aperture, light from one or more SLMs 15 will be cut disproportionately more than from one or more other SLMs 15.
  • the optical system e.g. optical system 17
  • systems as described herein include optical elements that fold light beams 12 such that light beams 12 converge on image plane 13 at angle ⁇ (as shown for example in Fig. 1) while SLMs 15 and/or light sources 14 are not aligned with the parts of light beams 12 that converge on image plane 13.
  • as shown for example in Fig. 1
  • SLMs 15 and/or light sources 14 are not aligned with the parts of light beams 12 that converge on image plane 13.
  • Fig. 4 shows a system in which light modulated by light modulators 15A and 15B is redirected to form beams 12A and 12B that converge toward image plane 13 at angle ⁇ .
  • One or more optical elements may be provided to redirect the light. In the illustrated embodiment the redirection is provided by a prism 30. From the point of view of optical system 17, light modulators 15A and 15B appear to be at locations 15A’ and 15B’ respectively.
  • Fig. 4 advantageously allows flexibility in the positioning of SLMs 15 and can facilitate smaller angles a between different beams 12.
  • the actual size of a SLM is often greater than the active area of the SLM.
  • Fig. 4 shows that the apparent positions 15A’ and 15B’ can be located so that the active areas appear to be immediately next to one another even though the packaging 37 of SLMs 15A and 15B extends outside the active area 38.
  • Light for beams 12 is provided by one or more light sources 14.
  • one light source 14 provides light for plural beams 12.
  • light for each beam 12 is provided by a separate light source 14.
  • Light sources 14 may be of any of a wide variety of types. Light sources 14 may be selected based on technical factors such as desired optical power output, desired wavelength or spectral composition, desired polarization state (as well as factors such as cost, durability, size, power requirements, operating temperature range, etc.).
  • light sources 14 comprise lasers. In some embodiments light sources 14 comprise solid state light emitters such as semiconductor lasers, laser diodes, light emitting diodes, etc.
  • a light source 14 emits unpolarized light.
  • Unpolarized light may, for example, be obtained by combining light from two lasers having orthogonal polarizations or by passing light from a laser through an optical element such as an optical fiber that depolarizes the laser light.
  • the light from light source 14 is well collimated.
  • a desired degree of collimation may be achieved for example by using a light source such as a suitable laser that emits collimated light or by providing collimating optics.
  • SLMs 15 Light from light source(s) 14 is directed to SLMs 15 for modulation.
  • SLMs 15 are reflection type SLMs (e.g. LCoS devices)
  • light from a light source 14 is directed onto an active area of a SLM 15 where the light is modulated and specularly reflected.
  • the reflected modulated light is then provided as a beam 12 which travels to image plane 13 where it combines with light from other beams 12 as described herein.
  • light source 14 is
  • Figure 5A shows a simple embodiment in which light is directed from opposite sides of image plane 13 to illuminate active areas of each SLM 15 (e.g. beam 45A illuminates SLM 15A and beam 45B illuminates SLM 15B). After being reflected by SLMs 15 the light is directed in beams 12 (e.g. beams 12A and 12B) which converge toward image plane 13.
  • beams 12 e.g. beams 12A and 12B
  • the arrangement illustrated in Fig. 5A can be inconvenient due to optical and mechanical constraints.
  • Figure 5B shows an optical arrangement 50 which is one example of a way to illuminate the active areas of SLMs 15 to yield beams 12.
  • Optical arrangement 50 provides a 3D folded light path which facilitates positioning of components.
  • Optical arrangement 50 also illustrates how a single light source 14 may illuminate active areas of two SLMs.
  • Optical arrangement 50 also illustrates how the light directed to plural SLMs may be made to have the same polarization.
  • light source 14 emits a collimated beam of unpolarized light.
  • the light passes to a polarizing beamsplitter 51.
  • a portion of the light having one polarization (usually one half of the light) passes through polarizing beamsplitter 51 to a mirror 52.
  • the rest of the light is reflected by polarizing beamsplitter 51.
  • the light is reflected by SLMs 15A and 15B to provide beams 12A and 12B respectively which converge at angle ⁇ toward image plane 13.
  • Arrangement 50 may be constructed to cause the polarization state of beams 53A, 53B to be the same. This can be achieved by providing an optical element 54 (e.g. a wave plate) that changes the polarization state of one of beams 53A, 53B to match the polarization state of the other one of beams 53A, 53B.
  • optical element 54 (or multiple optical elements 54) change(s) the polarization state of both of beams 53A, 53B. For example the polarization direction of one of beams 53A, 53B may be rotated by 90 degrees or the polarization direction of both of beams 53A, 53B may be rotated by 45 degrees.
  • beams 53A and 53B are folded relative to beams 12. Beams 53 form an angle ⁇ with beams 12. ⁇ may for example be about 20 degrees. ⁇ may be chosen such that beams 53 and beams 12 overlap only for a short distance. This structure can facilitate relatively unobstructed access to image plane 13 as well as easy coupling to light source 14. In the illustrated optical arrangement 50 beams 53A and 53B do not cross one another.
  • Fig. 5C is a plan view of another example optical arrangement 55.
  • optical arrangement 55 provides an optical path formed with a 3D fold.
  • illumination beams 56A and 56B (generally and collectively beams 56) from light sources 14A and 14B respectively cross each other at angle ⁇ before reaching prism 57 which redirects beams 56 to corresponding SLMs 15A and 15B. Beams 56 cross at location 58.
  • Fig. 5D is a schematic side elevation view of optical arrangement 55. As indicated schematically in Fig. 5D the light in beams 56 from light sources 14 angles toward prism 57 and beams 12 leave prism 57 at an angle to converge at image plane 13. In some embodiments image plane 13 is directly below the location 58 at which beams 56 cross. Optical arrangement 55 does not rely on tilting SLMs 15 to direct beams 12 to converge at angle ⁇ .
  • optical arrangement 55 angle ⁇ is defined by the orientations of beams 56. Light can be incident on SLMs 15 perpendicularly in at least one plane. Thus optical arrangement 55 may provide reduced parallelogram distortion (i.e. distortion resulting from the SLM 15 being illuminated from a direction that is not normal to the plane of the SLM panel).
  • light delivered to illuminate SLMs 15 may be folded by a fold angle ⁇ relative to light beams 12 that are delivered to an image plane 13.
  • Fold angle ⁇ may be in a different plane from angle ⁇ by which beams 12 converge.
  • the fold by angle ⁇ can facilitate making the location at which beams 12 converge on image plane 13 to be physically separated from light beams which deliver light to SLMs 15 (e.g. beams 53 or 56).
  • fold angle ⁇ is chosen to be relatively large (e.g. at least 9 degrees or at least 12 degrees or at least 15 degrees or at least 18 degrees). In some embodiments angle ⁇ is about 20°.
  • Fig. 6A shows an optical arrangement 60 which includes a total internally reflecting (TIR) prism set 62.
  • TIR prism set 62 comprises a first part 62A and a second part 62B separated by a small gap 62C of a material (e.g. air) that has a lower index of refraction than that of parts 62A and 62B.
  • First and second prism parts 62A and 62B may, for example be made out of glass, fused silica or other optical materials.
  • An incoming light beam 61 can enter TIR prism set 62 at face 63 of first part 62A.
  • First part 62A causes beam 61 to be displaced and to change angle.
  • the light is totally internally reflected at interfaces of first part 62A before the light exits TIR prism set 62 and is delivered to SLM 15.
  • SLM 15 is mounted directly to first part 62A of TIR prism set 62.
  • TIR prism set 62 causes outgoing beam 12 to be oriented at an angle ⁇ relative to incoming beam 61 (e.g. may appear as if beam 61 was reflected by a SLM at position 15’).
  • angle ⁇ in Fig. 6A
  • ⁇ ’ is less than 50% of ⁇ .
  • is about 20 degrees and ⁇ ’ is about 8 degrees.
  • a TIR prism set may be used in conjunction with other optical arrangements as described herein.
  • the same TIR prism set may be used to guide plural light beams modulated by plural SLMs 15.
  • Additional SLMs may be included by placing the SLMs side by side or in an array in the same plane, by using a prism (e.g. a prism 30) or in any other manner described herein.
  • Fig. 7 A shows an optical arrangement 70 that includes a TIR prism set 62 and a pair of SLMs 15A and 15B.
  • Illumination light beams 61 A and 61 B (which may be provided as described elsewhere herein or in any other manner) travel through first part 62A.
  • Beams 12 that have interacted with SLMs 15A and 15B travel back into TIR prism set 62 and leave TIR prism set 62 with an angle ⁇ relative to light beams 61 .
  • illumination light beams 61 A and 61 B may be oriented at angles so that they converge by angle ⁇ .
  • beams 61A and 61B illumination reach SLMs 15 at directions determined by two angles, ⁇ and ⁇ ’.
  • may be about 5 degrees and ⁇ ’ may be about 8 degrees.
  • face 65 of TIR prism set 62 may be formed to cause beams 12 to converge at angle ⁇ . This may be done, for example by forming face 65 as a concave dihedral.
  • Face 63 of TIR prism set 62 may be formed to adjust the relative angles of incoming beams 61A and 61 B. For example, if beams 61 A and 61 B are converging when they reach face 63, face 63 may have angled facets that receive each of beams 61 and adjust beams 61 to be parallel or to have another desired angular relationship.
  • the facets may make face 63 convex. In some embodiments the facets make face 63 concave.
  • Fig. 7B shows an example optical arrangement 72 in which face 63 of TIR prism set 62 comprises two facets 63A and 63B that are angled relative to one another by a dihedral angle.
  • Beam 61 A enters face 63 at facet 63A
  • beam 63B enters face 63 at facet 63B.
  • Refraction of beams 61 A and 61 B at facets 63A and 63B respectively may reduce or eliminate convergence of beams 61A and 61B and/or cause beams 61A and 61 B to encounter SLMs 15A and 15B in a perpendicular direction in the plane of beams 61A and 61 B.
  • face 65 of TIR prism set 62 has facets 65A and 65B. Facets 65A and 65B are angled relative to one another. Beam 12A exits at facet 65A and beam 12B exits at facet 65B. Facets 65A and 65B may be angled to adjust beams 12A and 12B to converge at a desired angle ⁇ . For example facets 65A and 65B may be angled so that face 65 is convex and refraction of beams 12A and 12B at facets 65A and 65B makes beams 12A and 12B more convergent. In some embodiments beams 12A and 12B are parallel inside TIR prism set 62.
  • a TIR prism set 62 may be designed such that two or more SLMs 15 are directly mounted onto TIR prism set 62.
  • SLMs 15 may be put side by side or in an array on face 64 of TIR prism set 62.
  • a prism that functions like prism 30 described elsewhere herein is integrated with TIR prism set 62. Such constructions may reduce losses by eliminating some air/glass interfaces. Also providing a prism 30 that is fixed to or unitary with a TIR prism set 62 may maintain alignment more reliably than separate parts.
  • Fig. 7C shows an example optical arrangement 73.
  • Optical arrangement 73 is the same as optical arrangement 72 shown in Fig. 7B except that optical arrangement 73 comprises prism 30.
  • Figs. 8A and 8B are top and side elevation views of an example optical arrangement 80 that includes a TIR prism set 62 which supports plural SLMs 15.
  • SLMs 15 may be in direct contact with a face of TIR prism set 62.
  • face 64 of TIR prism set 62 is extended to include integral prisms 82A and 82B.
  • Rear faces of prisms 82A and 82B are at 45 degrees to an axis of TIR prism set 62.
  • SLMs 15A and 15B are mounted to side faces of integrated prisms 82A and 82B respectively.
  • SLMs 15 may have panel dimensions of about 15.5x8 mm 2 ; and/or
  • a distance from a SLM panel 15 to image plane 13 may be about 150mm; and/or • An f-number of a projection optical system 17 may be about F/4.5 which corresponds to a radius in angular space of about 6.4°; and/or
  • a footprint 24 may span half angles in angular space of about 1 .6° x 0.85°;
  • a double angular footprint may span half angles in angular space of about 1.6° x 2.1° (0.85+0.85+0.4);
  • a diffuser 13A may scatter light into a cone having a half angle of about 4°;
  • a half angle for converging beams 12 may be about 2.50° (corresponding to angle ⁇ being about 5°).
  • apparatus combines a highlight beam with a base light beam at or upstream from an imager.
  • the base light beam may be combined with the highlight beam using the same angled geometry described herein (e.g. in any of Figs. 4 to 8B).
  • the base light beam may uniformly illuminate the imager.
  • the base light beam may have an etendue that is comparable to the modulated light beam(s) with which it is combined.
  • the etendues (or areas in angular space) of the base light beam and the modulated light beam are the same or similar (e.g. 10% or less difference).
  • Fig. 9 shows apparatus 90 according to an example embodiment in which a base light beam 92 is combined at an imager 94 with a modulated light beam 96.
  • base light beam 92 is made up of light from a light source 95.
  • Base light beam 92 may be homogenized and collimated to provide uniform illumination of imager 94.
  • the optical path followed by base light beam 92 includes a holographic diffuser 98 that acts as a “frozen phase grating” making a fixed full screen pattern on imager 94.
  • base light beam 92 is created by illuminating a holographic diffuser 98 with a highly collimated light source.
  • base light beam 92 comprises white light.
  • the optical path taken by the base light beam has the same construction as the optical path taken by the modulated light beam (including that the light source is highly collimated) except that a SLM (e.g. an SPM) in the optical path of the base light beam is configured to with a phase pattern that presents a “frozen phase grating” such that base light beam 92 illuminates the target (e.g. image plane 13) with a fixed light pattern (e.g. a uniform light pattern).
  • SLM is replaced with a holographic diffuser (e.g. holographic diffuser 98) that acts as a “frozen phase grating”.
  • the light source may, for example be a light source that can put all of its output light into a fiber of dimensions on the order of 400x240 ⁇ m and NA 0.2.
  • a base light beam is realized by homogenizing light from a separate (laser) light source, for example by passing the light through an optical fiber with a rectangular cut and then projecting a magnified image of the rectangular cut onto target image 13.
  • the collimated light source may, for example, be a light source that can put all of its output light into a fiber of dimensions on the order of 2x 1.2mm and NA 0.2.
  • SLMs 15 may be controlled (e.g. by applying an appropriate phase pattern) to direct unwanted light away from an image plane or image (e.g image plane 13).
  • SLMs 15 may be controlled to direct the unwanted light onto an aperture or apertures which can absorb the unwanted light. This advantageously can create high quality black regions of an image.
  • the unwanted light is directed onto a cooled aperture.
  • light beams are aligned relative to one another and SLMs 15 such that the following conditions are satisfied:
  • a mismatch between unmodulated beams of light is compensated for by applying a corrective phase pattern to one or more SLMs 15. Additionally, or alternatively, applying a corrective phase pattern to a particular SLM 15 may compensate for performance defects present in the particular SLM 15.
  • positions and/or orientations of components of the apparatus described herein are dynamically adjusted to align or re-align the components as desired.
  • the components may be coupled to automatically adjusting supports such as gimbals, movable mounting mechanisms, etc. which can vary the position or orientation of a coupled component.
  • plural apparatuses according to any of the embodiments described herein are each applied to produce modulated light of a corresponding one of a plurality of different corresponding colours (e.g. red, green or blue).
  • the modulated light of the different colours may be combined to yield a full colour image having a desired colour gamut. Any suitable technology may be used to combine the modulated light of the different colours.
  • the invention includes, without limitation, the following enumerated example embodiments:
  • a projection system comprising: one or more light sources operative to emit light; optical elements arranged to direct the light from the one or more light sources in two or more separate collimated beams, each of the beams illuminating the active area of the imager, the beams converging onto the image plane at an acute angle not exceeding 10 degrees; wherein the optical elements include a spatial light modulator arranged to modulate the light of at least one of the beams.
  • the projection system according to example embodiment 1 or any other example embodiment herein comprising an imager having an active area that coincides with or is adjacent to the image plane.
  • each of the light beams has an aspect ratio when they arrive at the image plane that matches an aspect ratio of the imager.
  • the projection system according to example embodiment 1 or any other example embodiment herein comprising an optical system having an entrance pupil that coincides with or is adjacent to the image plane.
  • the projector system according to example embodiment 1 or any other example embodiment herein comprising an optical diffuser located in or adjacent to the image plane.
  • the optical elements comprise a TIR prism set, the beams enter the TIR prism set with a relative angle of more than 10 degrees and the beams exit the prism at the acute angle.
  • TIR prism set is formed with a concave dihedral and the beams enter the TIR prism set at respective facets of the concave dihedral.
  • a projector system comprising: one or more light sources operable to emit first and second beams of monochromatic collimated light, the first and second beams having wavelengths that are the same or differ by not more than 10 nm; a first spatial light modulator (SLM) illuminated in an optical path of the first beam of light; a second SLM located in an optical path of the second beam of light; wherein the first and second beams of light overlap at an image plane that coincides with or is imaged onto a projector imager.
  • SLM spatial light modulator
  • the projector according to example embodiment 9 or any other example embodiment herein comprising a controller connected to control the first and second spatial phase modulators to steer light in the respective first and second beams away from one or more areas on the image plane and/or to concentrate light from the respective first and second beams at one or more selected highlight areas on the image plane.
  • An apparatus for generating images including highlights comprising: a first spatial light modulator (SLM) in a first optical path of a first beam of light; a frozen phase grating in a second optical path of a second beam of light; wherein the first and second optical paths bring the first and second beams of light to converge and overlap at an image plane; a controller configured to control the first spatial light modulator to steer the light of the first beam toward highlight areas in the image plane.
  • SLM spatial light modulator
  • the apparatus according to example embodiment 13 or any other example embodiment herein comprising an optical system having an entrance pupil at or adjacent to the image plane, the optical system having an acceptance angle wherein the light from the first and second beams incident on the image plane is within the acceptance angle.
  • optical system comprises projection optics and a projection imager and the image plane coincides with or is imaged onto the projection imager.
  • a projector system comprising: a plurality of spatial light modulators (SLMs) operable as phase modulators, each of the SLMs illuminated by a light beam, each of the SLMs configured to steer a respective corresponding light beam to a common target image plane; wherein the light steered to the common target image plane illuminates a an imager in the optical path.
  • SLMs spatial light modulators
  • the projector system according to example embodiment 15 or any other example embodiment herein comprising a controller configured to control each of the SLMs to concentrate light from the corresponding light beam at selected highlight locations on the image plane. 17.
  • controller is configured to cause at least one of the highlight locations for one of the light beams to be at a highlight location that does not coincide on the image plane with any of the highlight locations for one or more other ones of the light beams.
  • An apparatus according to example embodiment 20 or any other example embodiment herein wherein the angles between directions of incidence of the first and second beams on the image plane and a normal to the image plane is no more than 1/3 of the angle corresponding to the boundary of the acceptance angle of the imager.
  • An apparatus according to any one of example embodiment s 1 or 3 to 6 or any other example embodiment herein comprising at least one diffuser in the optical path between the image plane and the imager that increases the angular spread of the combined beam of light.
  • An apparatus according to any one of example embodiment s 1, 8, 12, 16 or any other example embodiment herein wherein the beams of light are modulated to illuminate at least one region of the image plane with light having an intensity that is greater than an intensity of light illuminating another region of the image plane.
  • An apparatus according to any of example embodiment s 1 to 29 or any other example embodiment herein wherein the SLMs are configured to modulate the beams of light to dynamically illuminate a projector imager.
  • An apparatus according to any one of example embodiment s 1 to 30 or any other example embodiment herein wherein the plural beams of light are modulated and then combined to illuminate the imager with light that varies with intensity over an active surface of the imager.
  • An apparatus according to example embodiment 31 to 34 or any other example embodiment herein wherein the imager is controlled to process image data comprising video frames and the modulation applied to the beams varies for the different frames.
  • An apparatus according to any one of example embodiment s 1 to 35 or any other example embodiment herein wherein the beams of light which are combined comprise unpolarised light.
  • An apparatus according to any one of example embodiment s 1 to 35 or any other example embodiment herein wherein the beams of light which are combined comprise light having a polarization that varies in space and/or time
  • An apparatus according to any one of example embodiment s 1 to 35 or any other example embodiment herein wherein the beams of light which are combined comprise light having a fixed polarization.
  • An apparatus according to any one of example embodiment s 1 to 38 or any other example embodiment herein wherein the beams that are combined comprise light that: is monochrome; has a bandwidth of 18 nm or less or 12 nm or less or 5 nm or less or 3 nm or less; has a wavelength that is the same for the different beams; and/or has a wavelength that differs from that of the other beams by not more than 5 nm or 10 nm or 15 nm.
  • An apparatus according to any one of example embodiment s 1 to 39 or any other example embodiment herein wherein the beams of light that are combined comprise light that is coherent.
  • An apparatus according to any one of example embodiment s 1 to 40 or any other example embodiment herein wherein the beams of light that are combined converge on the image plane at a relative angle ⁇ .
  • optical elements comprise one or more lenses, mirrors, prisms, filters and free space.
  • An apparatus according to any one of example embodiment s 1 to 49 or any other example embodiment herein wherein the light of each of the light beams is modulated with the same pattern and at the image plane the light beams are registered with one another so that in each part of the image formed at the image plane the same parts of the patterns in each of the light beams overlap and reinforce one another.
  • An apparatus according to any one of example embodiment s 1 to 50 or any other example embodiment herein wherein the image at the image plane provides dynamic illumination to an optical system.
  • An apparatus according to any one of example embodiment s 1 to 53 or any other example embodiment herein wherein the modulation applied by each SLM is determined at least in part from image data defining an image to be displayed by the apparatus.
  • An apparatus comprising an optical system positioned between the imager and the image plane, the optical system comprising a set of one or more optical elements operable to direct light from the image plane to the imager.
  • An apparatus according to any one of example embodiment s 1 to 58 or any other example embodiment herein wherein the light beams are shaped to illuminate a region of a specific size and shape at the image plane. 60. An apparatus according to example embodiment 59 or any other example embodiment herein wherein the light beams have an aspect ratio that matches an aspect ratio of the imager.
  • An apparatus according to any one of example embodiment s 70 to 74 or any other example embodiment herein wherein filling of the angular space up to the boundary of the acceptance angle is optimized by varying properties of the diffuser.
  • An apparatus comprising one or more optical elements arranged to bend or fold the light beams such that the light beams converge on the image plane at angle a while the SLMs and/or light sources are not aligned with the parts of the light beams that converge on the image plane.
  • An apparatus according to example embodiment 77 or any other example embodiment herein wherein at least one of the one or more optical elements that bend or fold the light beams comprises a prism.
  • An apparatus according to any one of example embodiment s 1 to 79 or any other example embodiment herein wherein light for each beam is provided by a separate light source.
  • An apparatus according to any one of example embodiment s 79 to 81 or any other example embodiment herein wherein the one or more light sources comprise lasers.
  • An apparatus according to any one of example embodiment s 79 to 81 or any other example embodiment herein wherein the one or more light sources comprise solid state light emitters.
  • An apparatus according to example embodiment 83 or any other example embodiment herein wherein the solid state light emitters consist of one or more of lasers, laser diodes and light emitting diodes.
  • Apparatus for illuminating a target area comprising: at least one light source arranged to direct light to a plurality of spatial light modulators the spatial light modulators operable to output beams of modulated light wherein the beams of modulated light are arranged to converge to the target area with a converging angle a and to create overlapping light fields at the target area.
  • Apparatus according to example embodiment 91 or any other example embodiment herein comprising an optical diffuser at or near to the target area wherein the optical diffuser is operative to scatter light from the beams of modulated light within the acceptance angle.
  • Apparatus comprising: plural spatial phase modulators, each illuminated by a light beam from a highly collimated light source; a control system configured to set each of the phase modulators to apply phase shifts so as to steer light to a common target or image plane to provide a corresponding light field at the target that includes areas of greater light intensity and areas of less light intensity; wherein the light fields overlap at the target and are co-registered so that corresponding areas in the overlapping light fields are superposed.
  • the apparatus according to example embodiment 98 or 99 or any other example embodiment herein comprising an imager located to be illuminated by the combined light field at the target.
  • the apparatus according to any of example embodiment s 98 to 102 or any other example embodiment herein comprising at least one optical diffuser provided in an optical path between the common target and the imager.
  • a method for supplying light for high intensity highlights in projected images comprising combining plural light beams in which light is steered to highlight locations in an image plane wherein the plural light beams may illuminate the same set of one or more imagers.
  • a method for supplying light for high intensity highlights in projected images comprising at an imager combining at least one modulated light beam generated with an apparatus according to any one of the example embodiment s herein with a base light beam.
  • an optical path of the base light beam comprises a SLM configured as a frozen phase grating.
  • connection means any connection or coupling, either direct or indirect, between two or more elements; the coupling or connection between the elements can be physical, logical, or a combination thereof;
  • Control systems e. g. for controlling SLMs, SAMs or SPMs may be implemented using specifically designed hardware, configurable hardware, programmable data processors configured by the provision of software (which may optionally comprise “firmware”) capable of executing on the data processors, special purpose computers or data processors that are specifically programmed, configured, or constructed to perform one or more steps in a method as explained in detail herein and/or combinations of two or more of these.
  • specifically designed hardware are: logic circuits, application-specific integrated circuits (“ASICs”), large scale integrated circuits (“LSIs”), very large scale integrated circuits (“VLSIs”), and the like.
  • Examples of configurable hardware are: one or more programmable logic devices such as programmable array logic (“PALs”), programmable logic arrays (“PLAs”), and field programmable gate arrays (“FPGAs”).
  • PALs programmable array logic
  • PLAs programmable logic arrays
  • FPGAs field programmable gate arrays
  • Examples of programmable data processors are: microprocessors, digital signal processors (“DSPs”), embedded processors, graphics processors, math co-processors, general purpose computers, server computers, cloud computers, mainframe computers, computer workstations, and the like.
  • DSPs digital signal processors
  • embedded processors graphics processors
  • math co-processors general purpose computers
  • server computers cloud computers
  • mainframe computers mainframe computers
  • computer workstations and the like.
  • one or more data processors in a control circuit for a projector may implement methods as described herein by executing software instructions in a program memory accessible to the processors.
  • a component e.g. an optical element, modulator, light source, lens, assembly, device, arrangement, etc.
  • reference to that component should be interpreted as including as equivalents of that component any component which performs the function of the described component (i.e. , that is functionally equivalent), including components which are not structurally equivalent to the disclosed structure which performs the function in the illustrated exemplary embodiments of the invention.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Optics & Photonics (AREA)
  • Projection Apparatus (AREA)
  • Liquid Crystal (AREA)
  • Transforming Electric Information Into Light Information (AREA)
PCT/EP2021/077147 2020-10-02 2021-10-01 Optical projection with combined beams Ceased WO2022069727A1 (en)

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US18/247,249 US12591170B2 (en) 2020-10-02 2021-10-01 Optical projection with combined beams
JP2023520063A JP7646985B2 (ja) 2020-10-02 2021-10-01 ビームを組み合わせた光学投影
EP21786463.6A EP4222557A1 (en) 2020-10-02 2021-10-01 Optical projection with combined beams
CA3197042A CA3197042A1 (en) 2020-10-02 2021-10-01 Optical projection with combined beams
CN202180076248.4A CN116547603A (zh) 2020-10-02 2021-10-01 利用组合光束的光学投影
JP2024212183A JP2025060627A (ja) 2020-10-02 2024-12-05 ビームを組み合わせた光学投影

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CA3095177A CA3095177A1 (en) 2020-10-02 2020-10-02 Optical projection with combined beams
US202063119580P 2020-11-30 2020-11-30
US63/119,580 2020-11-30

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JP2025060627A (ja) 2025-04-10
US12591170B2 (en) 2026-03-31
CA3095177A1 (en) 2022-04-02
EP4222557A1 (en) 2023-08-09
CN116547603A (zh) 2023-08-04
CA3197042A1 (en) 2022-04-07
JP7646985B2 (ja) 2025-03-18
US20230375906A1 (en) 2023-11-23

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