METHOD AND DEVICE FOR PRODUCING A COMPUTER-GENERATED HOLOGRAM, A HOLOGRAM AND A LIGHTING DEVICE FOR A VEHICLE

Abstract

A method for producing a computer-generated hologram, including the method steps of generating a reference beam, generating an object beam, imprinting computer-generated information pertaining to the hologram to the object beam, and overlapping of the object beam and the reference beam on or in a photosensitive recording medium for imprinting the hologram, wherein successively a plurality of portions of the photosensitive recording medium are simultaneously impinged upon with the object beam and the reference beam to produce a plurality of sub-holograms, and wherein the angle of incidence at which the reference beam is incident on the surface of a first portion of the recording medium is different from the angle of incidence at which the reference beam impinges upon the surface of a second portion of the recording medium.

Claims

1. A method for producing a computer-generated hologram, the method comprising: generating a reference beam; generating an object beam; imprinting computer-generated information pertaining to the hologram to the object beam; and overlapping the object beam and the reference beam on or in a photosensitive recording medium for imprinting the hologram, wherein successively a plurality of sections of the photosensitive recording medium are each simultaneously impinged upon by the object beam and the reference beam to produce a plurality of sub-holograms, and wherein an angle of incidence at which the reference beam is incident on the surface of a first portion of the recording medium is different from an angle of incidence at which the reference beam is incident on the surface of a second portion of the recording medium.

2. The method according to claim 1, wherein the reference beam is reflected onto the portions of the recording medium by a reflector or a parabolic reflector.

3. The method according to claim 2, wherein different radial distances between the optical axis of the reflector and the point of incidence of the reference beam on the reflector and different angles of incidence of the reference beam are generated on the surfaces of the portions of the recording medium.

4. The method according to claim 1, wherein the photosensitive recording medium has a planar surface.

5. The method according to claim 1, wherein the photosensitive recording medium is moved between an exposure with the object beam and the reference beam for generating a first sub-hologram and an exposure with the object beam and the reference beam for generating a second sub-hologram in a plane parallel to the planar surface of the recording medium.

6. The method according to claim 5, wherein the optical axis of the parabolic reflector lies in the plane or is aligned parallel to the plane in which the photosensitive recording medium is moved between the generation of two sub-holograms.

7. The method according to claim 1, wherein the produced computer-generated hologram is a transmission hologram or a reflection hologram or an edge-lit-hologram.

8. The method according to claim 1, wherein the produced computer-generated hologram serves as a master hologram for the production of hologram replicas.

9. A device for producing a computer-generated hologram, comprising a light source for generating a light beam; optical splitter to split the light beam generated by the light source into an object beam and a reference beam; modulater to imprint hologram-related information to the object beam; and an optical device for overlapping the object beam and the reference beam on or in a photosensitive recording medium for imprinting the hologram, wherein in the operation of the device successively a plurality of portions of the photosensitive recording medium are simultaneously impinged upon with the object beam and the reference beam to generate sub-holograms, and wherein the optical device serving for overlapping the object beam and the reference beam is designed such that an angle of incidence at which the reference beam is incident on the surface of a first portion of the recording medium is different from an angle of incidence at which the reference beam impinges upon the surface of a second portion of the recording medium.

10. The device according to claim 9, wherein the light source is a laser light source.

11. The device according to claim 9, wherein the optical device serving for the overlapping of object beam and reference beam comprises a reflector or a parabolic reflector from which, during operation of the device, the reference beam is reflected onto the photosensitive recording medium.

12. The device according to claim 9, wherein the device comprises an adjuster to move the photosensitive recording medium between an exposure with the object beam and the reference beam to generate a first sub-hologram and an exposure with the object beam and the reference beam to generate a second sub-hologram, wherein the adjuster is adapted to move the recording medium in a plane parallel to the planar surface of the recording medium.

13. The device according to claim 9, wherein the device further comprises a modulater for imprinting hologram-related information to the object beam, wherein the modulater is an LC display or an LC display operated in a reflection arrangement, which generates phase shifts between different portions of the object beam.

14. A hologram, in particular a hologram replica, produced by a method according to claim 1, wherein the hologram is provided to a curved surface and/or for use with a light source having a predetermined divergence.

15. A lighting device for a vehicle, in particular a headlight for a vehicle, comprising a hologram according to claim 14, wherein the lighting device includes a curved surface on which the hologram is disposed.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0022] The present invention will become more fully understood from the detailed description given hereinbelow and the accompanying drawings which are given by way of illustration only, and thus, are not limitive of the present invention, and wherein:

[0023] FIG. 1 is a perspective view of a portion of a device according to the invention;

[0024] FIG. 2 is a schematic sectional view of a reconstruction of a hologram according to the invention; and

[0025] FIG. 3 is a schematic sectional view of a reconstruction of a hologram according to the invention.

DETAILED DESCRIPTION

[0026] In the exemplary embodiment depicted in FIG. 1, a hologram formed of a plurality of sub-holograms is to be imprinted to a photosensitive recording medium 1 shown only schematically. The sub-holograms can be arranged side by side in a two-dimensional matrix in an x and a y direction. Photosensitive recording media 1 may consist of conventional media used in the generation of holograms. The recording medium 1 may, for example, be formed as a film that is disposed on a transparent substrate, not shown. The photosensitive recording medium 1 has a planar surface and extends in an x-y plane.

[0027] The embodiment of a device according to the invention partially shown schematically in FIG. 1 further comprises a laser light source, which generates a laser beam which is split by an optical device into an optical beam 2 and a reference beam 3. The device further comprises a modulator, which may be formed as an LC display in a reflection arrangement. The LC display can be controlled as a function of computer-generated data which relates to the creation of individual sub-holograms.

[0028] The object beam 2 can be widened onto the LC display by an optical device. As a function of the data controlling the LC display, the LC display can change the phase of portions of the object beam 2 during reflection, so that portions of the object beam 2 can exhibit a phase shift relative to other parts of the object beam 2. As a result, the object beam 2 is imprinted with information pertaining to a sub-hologram.

[0029] The device further comprises a parabolic reflector 4 facing the photosensitive recording medium 1. In this case, the optical axis 5 of the reflector 4 extends in the x-direction through the x-y plane of the planar surface of the recording medium 1. In particular, the focal point 6 of the parabolic reflector 4 is in the x-y plane of the planar surface of the recording medium 1.

[0030] Laser beams disposed in parallel with the optical axis of the parabolic reflector 4, i.e., extending in the negative x-direction, are focused into the focal point 6 of the parabolic reflector 4, wherein the angle at which they enter into the photosensitive recording medium 1 is dependent on the position in which they impinge on the reflector 4.

[0031] FIG. 1 depicts three exemplary reference beams 3, 3, 3, each of which are incident on the reflector 4 in the negative x-direction and thereby are spaced differently from the optical axis 5 of the reflector 4. Accordingly, also the angle at which they impinge on the recording medium 1 is different.

[0032] The reference beam 3 in FIG. 1 impinging on the reflector 4 far above the optical axis 5 impinges on the surface of the recording medium 1 at a comparatively wide angle of incidence to the x-y plane. In contrast, the angle of incidence , at which the reference beam 3 in FIG. 1 impinging on the reflector 4 is incident on the surface of the recording medium 1 further down or closer to the optical axis 5, is significantly smaller than the angle of incidence . A variation of the position of the reference beam 3, 3 thus results in a change in the angle of incidence , at which the reference beam 3, 3 is incident on the recording medium 1, and thus in a change in the orientation of the Bragg planes in the hologram and in a change in the angle of incidence at which the hologram can later be reconstructed.

[0033] The object beam 2 is not reflected on the reflector 4 but instead moves in the positive z-direction upward directly into the recording medium 1 and is superimposed there by the reference beam 3, 3, 3. By interference with the reference beam 3, 3, 3, a hologram is written into the photosensitive recording medium 1 in a conventional manner.

[0034] The reflector 4 takes on two functions. On the one hand it serves to focus the reference beam 3, 3, 3 onto or into the recording medium 1 and on the other hand, it allows for a change in the angle of incidence of the reference beam 3, 3, 3. In this case, the recording medium 1 is displaceably mounted in an x-y plane in the focal point of the reflector 4. For this purpose, an adjuster for moving the photosensitive recording medium 1 are provided.

[0035] For the manufacture of the hologram, the recording medium 1 can be positioned in the x-y plane in such a manner that the object beam 2 and the reference beam 3, 3, 3 overlap on a first portion of the surface of the recording medium 1 so as to imprint a first sub-hologram. To this end, the object beam 2 is imprinted with the information pertaining to the first sub-hologram.

[0036] After reading the first sub-hologram, the recording medium 1 is shifted in the x-y plane until the object beam 2 and the reference beam 3, 3, 3 overlap on a second portion of the surface of the recording medium 1 so as to imprint a second sub-hologram. To this end, the object beam 2 is imprinted with the information pertaining to the second sub-hologram.

[0037] In this manner, all sub-holograms are gradually read into the recording medium 1.

[0038] By means of the reference beam impinging upon the side of the reflector 4 facing away from the object beam 2, reflection holograms can be written. This corresponds to the superposition of the object beam 2 in FIG. 1 with the upper reference beam 3 or the reference beam 3 arranged slightly further down.

[0039] By means of the reference beam 3 impinging upon the side of the reflector 4 facing the object beam 2, transmission holograms can be written. This corresponds to the superposition of the object beam 2 in FIG. 1 with the reference beam 3 disposed below the recording medium 1.

[0040] By means of the reference beam 3 impinging upon the reflector 4 in the vicinity of the optical axis 5, an angle of incidence can be achieved that corresponds to the critical angle of the total reflection at the interface between the recording medium 1 and the environment. This is the case for the reference beam 3. Thus, edge-lit-holograms of both categories, transmission and reflection, can also be produced.

[0041] The flexibility in the imprinting of the holograms at different angles allows for a targeted adaptation to divergent light sources. FIG. 2 shows as a divergent light source a light emitting diode (LED) 7 and the outgoing light 8 or the wavefronts 9 of the light 8. If, despite the divergence of the light 8, the proportions 10 of the first diffraction order of the hologram reconstructed by the light 8 are to move upward in FIG. 2 in the same direction, the Bragg planes 11 of the hologram for different sub-holograms must be at a different angle to the surface of the recording medium 1. For example, in FIG. 2, the angle .sub.1 of the right Bragg planes 11 is significantly larger than the angle .sub.2 of the left Bragg planes 11.

[0042] It should be noted at this point that in FIG. 2 and FIG. 3, instead of the thin recording medium 1 only a comparatively thick plate is shown. This can be a transparent substrate to which the recording medium 1, for example, is applied in the form of a thin film.

[0043] With the device according to FIG. 1 or by means of the inventive method, suitable angles of incidence of the reference beam 3, 3, 3 onto the recording medium 1 can be selected during the writing of the hologram into the recording medium 1 so as to achieve suitable inclinations of the Bragg planes 11 in the hologram. The inclination of the Bragg planes 11 suitable for the divergent light source can be taken into account in the production of the computer-generated hologram without having to use the light emitting diode 7 itself in the writing process.

[0044] In the exemplary reconstruction according to FIG. 3, a light emitting diode 7 is likewise used as a divergent light source. The recording medium 1 or a substrate carrying the recording medium 1 is not planar but curved or has a curved surface.

[0045] The Bragg planes 11 of individual sub-holograms already mutually inclined due to the divergent light source must have an additional change in inclination due to the curvature of the recording medium 1 containing the hologram. This is illustrated in FIG. 3 by the effective Bragg planes 12, which represent the change in the Bragg planes due to the curvature of the recording medium 1 serving as the hologram carrier. This change in angle of the effective Bragg planes 12 when the recording medium 1 is bent relative to a planar surface 13 shown by way of example in FIG. 3 can already be taken into account in the writing process without having to use a curved recording medium in the writing process.

[0046] The computer-generated hologram produced with the device according to FIG. 1 or by means of the method according to the invention can serve as a master hologram for the production of hologram replicas. For example, the hologram replicas can be read into a thin flexible film. This film can then be applied, for example, to a curved surface of a lighting device, in particular a headlight.

[0047] The invention being thus described, it will be obvious that the same may be varied in many ways. Such variations are not to be regarded as a departure from the spirit and scope of the invention, and all such modifications as would be obvious to one skilled in the art are to be included within the scope of the following claims.