Display of 3D Holoscopic content on ... - Brunel University

Display of 3D Holoscopic content on ... - Brunel University Display of 3D Holoscopic content on ... - Brunel University

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ICT Project ong>3Dong> VIVANT– Deliverable 6.4 Contract no.: 248420 ong>Displayong> ong>ofong> ong>3Dong> ong>Holoscopicong> Content on Auto-stereoscopic ong>Displayong> Figure 1: Multiview auto-stereoscopic display. Slanted Lenticular optics LCD Panel Figure 2: The Slanted arrangement ong>ofong> the lenticular lens and pixels in the multiview auto-stereoscopic displays. 2.2 ong>3Dong> HOLOSCOPIC DISPLAYS ong>3Dong> ong>Holoscopicong> imaging (also known as Integral imaging) is a technique that is capable ong>ofong> creating and encoding a true volume spatial optical model ong>ofong> the object scene in the form ong>ofong> a planar intensity distribution by using unique optical components. It is akin to holography in that ong>3Dong> information recorded on a 2D medium can be replayed as a full ong>3Dong> optical model, however, in contrast to holography, coherent light sources are not required. This conveniently allows more conventional live capture and display procedures to be adopted. With recent progress in the theory and microlens manufacturing, integral imaging is becoming a practical and prospective ong>3Dong> display technology and is attracting much interest in the ong>3Dong> area. To record a ong>3Dong> ong>Holoscopicong> image a regularly spaced array ong>ofong> small lenslets closely packed together in contact with an image sensor (as shown in figure 3). Each lenslet views the scene at a slightly different angle to its neighbour and therefore a scene is captured from many view points and parallax information is recorded. After processing, if the photographic transparency is re-registered with the original recording array and illuminated by diffuse white light from the rear, the object will be constructed in space by the intersection ong>ofong> ray bundles emanating from each ong>ofong> the lenslets. A ong>3Dong> ong>Holoscopicong> image is recorded in a regular block pixel pattern. The planar intensity distribution representing a ong>3Dong> ong>Holoscopicong> image is comprised ong>ofong> 2D array ong>ofong> M×M micro-images due to the structure ong>ofong> the microlens array used in the capture and replay. The rectangular aperture at the front ong>ofong> the camera and the regular structure ong>ofong> the hexagonal microlenses array used in the hexagonal grid (recording microlens array) gives rise to a regular ‘brick structure’ in the intensity distribution as illustrated in Figure 4. 6

ICT Project ong>3Dong> VIVANT– Deliverable 6.4 Contract no.: 248420 ong>Displayong> ong>ofong> ong>3Dong> ong>Holoscopicong> Content on Auto-stereoscopic ong>Displayong> Recording Medium Microlens Array Figure 3: Recording ong>ofong> a ong>3Dong> ong>Holoscopicong> Image. The replay ong>ofong> the ong>3Dong> Integral images is achieved by placing a microlens array on the top ong>ofong> the recoded planar intensity distributions as shown in figure 5. The microlens array has to match exactly the structure ong>ofong> the planar intensity distribution. Figure 4: Recorded ong>3Dong> ong>Holoscopicong> ong>contentong> showing a 2D Array ong>ofong> micro-images. 7

ICT Project <str<strong>on</strong>g>3D</str<strong>on</strong>g> VIVANT– Deliverable 6.4<br />

C<strong>on</strong>tract no.:<br />

248420<br />

<str<strong>on</strong>g>Display</str<strong>on</strong>g> <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>3D</str<strong>on</strong>g> <str<strong>on</strong>g>Holoscopic</str<strong>on</strong>g> C<strong>on</strong>tent <strong>on</strong><br />

Auto-stereoscopic <str<strong>on</strong>g>Display</str<strong>on</strong>g><br />

Figure 1: Multiview auto-stereoscopic display.<br />

Slanted<br />

Lenticular optics<br />

LCD Panel<br />

Figure 2: The Slanted arrangement <str<strong>on</strong>g>of</str<strong>on</strong>g> the lenticular lens and pixels in the multiview auto-stereoscopic displays.<br />

2.2 <str<strong>on</strong>g>3D</str<strong>on</strong>g> HOLOSCOPIC DISPLAYS<br />

<str<strong>on</strong>g>3D</str<strong>on</strong>g> <str<strong>on</strong>g>Holoscopic</str<strong>on</strong>g> imaging (also known as Integral imaging) is a technique that is capable <str<strong>on</strong>g>of</str<strong>on</strong>g> creating<br />

and encoding a true volume spatial optical model <str<strong>on</strong>g>of</str<strong>on</strong>g> the object scene in the form <str<strong>on</strong>g>of</str<strong>on</strong>g> a planar intensity<br />

distributi<strong>on</strong> by using unique optical comp<strong>on</strong>ents. It is akin to holography in that <str<strong>on</strong>g>3D</str<strong>on</strong>g> informati<strong>on</strong><br />

recorded <strong>on</strong> a 2D medium can be replayed as a full <str<strong>on</strong>g>3D</str<strong>on</strong>g> optical model, however, in c<strong>on</strong>trast to<br />

holography, coherent light sources are not required. This c<strong>on</strong>veniently allows more c<strong>on</strong>venti<strong>on</strong>al live<br />

capture and display procedures to be adopted. With recent progress in the theory and microlens<br />

manufacturing, integral imaging is becoming a practical and prospective <str<strong>on</strong>g>3D</str<strong>on</strong>g> display technology and is<br />

attracting much interest in the <str<strong>on</strong>g>3D</str<strong>on</strong>g> area.<br />

To record a <str<strong>on</strong>g>3D</str<strong>on</strong>g> <str<strong>on</strong>g>Holoscopic</str<strong>on</strong>g> image a regularly spaced array <str<strong>on</strong>g>of</str<strong>on</strong>g> small lenslets closely packed together in<br />

c<strong>on</strong>tact with an image sensor (as shown in figure 3). Each lenslet views the scene at a slightly<br />

different angle to its neighbour and therefore a scene is captured from many view points and parallax<br />

informati<strong>on</strong> is recorded. After processing, if the photographic transparency is re-registered with the<br />

original recording array and illuminated by diffuse white light from the rear, the object will be<br />

c<strong>on</strong>structed in space by the intersecti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> ray bundles emanating from each <str<strong>on</strong>g>of</str<strong>on</strong>g> the lenslets.<br />

A <str<strong>on</strong>g>3D</str<strong>on</strong>g> <str<strong>on</strong>g>Holoscopic</str<strong>on</strong>g> image is recorded in a regular block pixel pattern. The planar intensity distributi<strong>on</strong><br />

representing a <str<strong>on</strong>g>3D</str<strong>on</strong>g> <str<strong>on</strong>g>Holoscopic</str<strong>on</strong>g> image is comprised <str<strong>on</strong>g>of</str<strong>on</strong>g> 2D array <str<strong>on</strong>g>of</str<strong>on</strong>g> M×M micro-images due to the<br />

structure <str<strong>on</strong>g>of</str<strong>on</strong>g> the microlens array used in the capture and replay. The rectangular aperture at the fr<strong>on</strong>t <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

the camera and the regular structure <str<strong>on</strong>g>of</str<strong>on</strong>g> the hexag<strong>on</strong>al microlenses array used in the hexag<strong>on</strong>al grid<br />

(recording microlens array) gives rise to a regular ‘brick structure’ in the intensity distributi<strong>on</strong> as<br />

illustrated in Figure 4.<br />

6

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