VIDEO HOLOGRAM AND DEVICE FOR RECONSTRUCTING VIDEO HOLOGRAMS

• US 20110026089A1
• Filed: 10/12/2010
• Published: 02/03/2011
• Est. Priority Date: 11/13/2002
• Status: Active Grant

• Current Assignee: SeeReal Technologies GmbH (SeeReal Technologies S.A.)
• Original Assignee: SeeReal Technologies GmbH (SeeReal Technologies S.A.)
• Inventors: Schwerdtner, Armin
• Granted Patent: US 8,174,744 B2
• Time in Patent Office: Days
• US Class Current: 359/9
• CPC Class Codes: G03H 1/08 Synthesising holograms, i.e. holograms synthesized from objects or objects from hologramsusing electric digital computers G06F; G06T
• CPC Class Codes: G03H 1/16 using Fourier transform G03H1/10, G03H1/12, G03H1/14 take precedence; analogue computers G06G, e.g. G06G7/19
• CPC Class Codes: G03H 1/2286 Particular reconstruction light G03H1/24 takes precedence; Beam properties
• CPC Class Codes: G03H 1/2294 Addressing the hologram to an active spatial light modulator
• CPC Class Codes: G03H 2001/0858 Cell encoding wherein each computed values is represented by at least two pixels of the modulator, e.g. detour phase coding
• CPC Class Codes: G03H 2001/2236 Details of the viewing window
• CPC Class Codes: G03H 2001/2242 Multiple viewing windows
• CPC Class Codes: G03H 2001/2271 RGB holobject
• CPC Class Codes: G03H 2210/30 3D object
• CPC Class Codes: G03H 2222/22 Spatial coherence
• CPC Class Codes: G03H 2222/34 Multiple light sources
• CPC Class Codes: G03H 2226/05 Means for tracking the observer

Abstract

The invention relates to video holograms and devices for reconstructing video holograms, comprising an optical system having a light source, lens and the video hologram having cells arranged in a matrix or a regular pattern with at least one opening per cell, the phase or amplitude of said opening being controllable. The holographic video representations of expanded spatial objects can be achieved in a wide viewing area in real time using controllable displays, whereby the objects are either computer-generated or created by different means. The space-bandwidth product (SBP) of the hologram is thus reduced to a minimum and the periodicity interval of the Fourier spectrum is used as a viewing window on the inverse transformation plane, through which the object is visible in the preceding space. The mobility of the viewer(s) is achieved by tracking the viewing window.

Claims

1. A method for reconstructing a three-dimensional scene using a reconstruction device including a light source, an optical system and a hologram encoded on a hologram-bearing medium having a matrix of cells;

the hologram-bearing medium and the optical system being illuminated by the light source; and

the optical system imaging the light source into an image plane of the light source;

the method comprising the steps of

(i) the optical system generating an inverse Fourier transform of the hologram encoded on the hologram-bearing medium at the image plane of the light source;

(ii) providing a viewing window at the image plane of the light source, the viewing window being the location where an observer places at least one eye to view the holographic reconstruction representing the three-dimensional scene; and

(iii) forming the holographic reconstruction of the three-dimensional scene from the hologram encoded in the hologram bearing medium within a reconstruction frustum stretching between the hologram-bearing medium and the viewing window.

2. The method of claim 1, wherein the viewing window is positioned in relation to an eye of an observer.

3. The method of claim 1 in which the holographic reconstruction of the three-dimensional scene is made up of multiple discrete points and the hologram on the hologram-bearing medium comprises the limited region with information needed to reconstruct one such single point in the reconstruction, the point being visible from the viewing window, and is characterized in that the limited region:

(a) is encoded with information for that single point in the reconstruction and

(b) is the only limited region in the hologram encoded with information for that point, and

(c) is restricted in size to form a portion of the entire hologram, the size being such that multiple reconstructions of that point caused by higher diffraction orders are not visible at the viewing window.

4. The method of claim 3 in which the limited region has been generated by a projection from the viewing window through the single point onto the hologram-bearing medium.

5. The method of claim 1 comprising the step of time sequentially re-encoding a hologram on the hologram-bearing medium for one eye and then the other eye of an observer.

6. The method of claim 1 in which the holographic reconstruction representing the three-dimensional scene is described by the Fresnel transform of the hologram being encoded in the hologram-bearing medium and the holographic reconstruction representing the three-dimensional scene is not described by the Fourier transform of the hologram being encoded in the hologram-bearing medium.

7. The method of claim 1 in which the size of the viewing window is calculated by a computing means in dependence of the extension of the periodicity interval of the hologram bearing medium.

8. The method of claim 1 in which the size of the viewing window is smaller than the size of the hologram-bearing medium.

9. The method of claim 1 in which there are separate viewing windows, one for each eye of the observer.

10. The method of claim 9 in which each viewing window is approximately 1 cm×

1 cm.

11. The method of claim 9 in which the locations of an observer'"'"'s eyes are tracked and the positions of the viewing windows are altered so that the observer can maintain a view through each viewing window even when moving his or her head.

12. The method of claim 1 in which the light source includes one or more individual light sources.

13. The method of claim 1, in which the light source is a line-shaped light source.

14. The method of claim 1, in which the light source is a real light source.

15. The method of claim 1, in which the light source is a point light source.

16. The method of claim 1, wherein several light sources are turned on to generate viewing windows for several observers.

17. The method of claim 1, wherein information required to determine the position of the light source is provided by at least one position sensor that measures the position of the observer.

18. The method of claim 1 comprising the steps of assigning a first viewing window to a first eye of a viewer and also assigning a second viewing window to the other eye of the viewer, the second viewing window being generated using a second light source.

19. The method of claim 18, wherein the optical system and the hologram-bearing medium are arranged so that higher diffraction orders of the hologram for the first viewing window have a zero point or an intensity minimum at the position of the second viewing window.

20. The method according to claim 19, wherein the hologram-bearing medium is re-encoded for the second eye at the same time as the second viewing window is generated.

21. The method of claim 1, wherein the holographic reconstruction is in color, and wherein the hologram-bearing medium is composed of cells arranged in a regular pattern with at least three openings per cell, representing the three primary colors, the phase or the amplitude or the phase and the amplitude of light from the light source being controllable by said openings by encoding the hologram into the hologram bearing medium, and said openings being encoded individually for each primary color.

22. The method of claim 1, wherein a color reconstruction is achieved by at least three reconstructions in the individual primary colors, generated sequentially.

23. The method of claim 1, in which the hologram-bearing medium is a TFT display.

24. The method of claim 1 in which the hologram-bearing medium controls phase of light of the light source.

25. The method of claim 1 in which the hologram-bearing medium controls amplitude of light of the light source.

26. The method of claim 1 in which the hologram-bearing medium controls phase and amplitude of light of the light source.