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Light Field Light Field

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Light Field. Modeling a desktop. Image Based Rendering. Fast Realistic Rendering without 3D models. Start from Ray Tracing. Rendering is about computing color along each ray. Sampling Rays. Sampling Rays by Taking Pictures. Rendering as Ray Resampling. Ray space. - PowerPoint PPT Presentation

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Page 1: Light Field

Light FieldLight Field

Page 2: Light Field

Modeling a desktopModeling a desktop

Page 3: Light Field
Page 4: Light Field

Image Based RenderingImage Based Rendering

Fast Realistic Rendering without 3D models

Page 5: Light Field

Start from Ray TracingStart from Ray Tracing

Rendering is about computing color along each ray

Page 6: Light Field

Sampling RaysSampling Rays

Page 7: Light Field

Sampling Rays by Taking PicturesSampling Rays by Taking Pictures

Page 8: Light Field

Rendering as Ray ResamplingRendering as Ray Resampling

Page 9: Light Field

Ray spaceRay space

How to parameterize the ray space

How to sample and resample rays

Page 10: Light Field

Two Plane ParameterizationTwo Plane Parameterization

Page 11: Light Field

Stanford Camera ArrayStanford Camera Array

Page 12: Light Field

Light Field RenderingLight Field Rendering

Very Fast

Page 13: Light Field

Light Field RenderingLight Field Rendering

4D interpolation

Page 14: Light Field

Dynamic Reparameterized Light Fields

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Dynamic Reparameterized Light Fields

• Move to desired new focal surface• Create a new 4D space with new focal surface• Recove ray with Reparameterization

• (u, v, s, t) => (u, v, f, g)F

Page 16: Light Field

Dynamic Reparameterized Light Fields

• Recover ray r• Resample from ray (s’, t’, f, g) and (s’’, t’’, f, g)• Interpolation, reconstruction with filter, … , etc

Page 17: Light Field

Dynamic Reparameterized Light Fields

• Change the shape of focal surface • Gives focus on 3D object rather than planes

Page 18: Light Field

Dynamic Reparameterized Light Fields

Page 19: Light Field

Dynamic Reparameterized Light Fields

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Variable Apertures

• Also can generate variable aperture• Aperture

– Control amount of light– Control depth of fields

• Aperture Filter: – Control how many cameras are used to resample a required ray– Larger apertures produce images with narrow range of focus

Page 21: Light Field

Aperture Filters

Page 22: Light Field

Variable Apertures

Page 23: Light Field

Variable Apertures

Page 24: Light Field

Marc Levoy

Stanford multi-camera array

• 640 × 480 pixels ×30 fps × 128 cameras

• synchronized timing

• continuous streaming

• flexible arrangement

Page 25: Light Field

Marc Levoy

Ways to use large camera arrays

• widely spaced light field capture

• tightly packed high-performance imaging

• intermediate spacing synthetic aperture photography

Page 26: Light Field

Marc Levoy

Intermediate camera spacing:synthetic aperture photography

Page 27: Light Field

Marc Levoy

Example using 45 cameras[Vaish CVPR 2004]

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Page 29: Light Field

Tiled camera array

• world’s largest video camera

• no parallax for distant objects

• poor lenses limit image quality

• seamless mosaicing isn’t hard

Can we match the image quality of a cinema camera?

Page 30: Light Field

Tiled panoramic image(before geometric or color calibration)

Page 31: Light Field

Tiled panoramic image(after calibration and blending)

Page 32: Light Field

Tiled camera array

• world’s largest video camera

• no parallax for distant objects

• poor lenses limit image quality

• seamless mosaicing isn’t hard

• per-camera exposure metering

• HDR within and between tiles

Can we match the image quality of a cinema camera?

Page 33: Light Field

same exposure in all cameras

individually metered

checkerboardof exposures

Page 34: Light Field

Marc Levoy

High-performance photography as multi-dimensional sampling

• spatial resolution

• field of view

• frame rate

• dynamic range

• bits of precision

• depth of field

• focus setting

• color sensitivity

Page 35: Light Field

Light field photography using a handheld plenoptic camera

Ren Ng, Marc Levoy, Mathieu Brédif,Gene Duval, Mark Horowitz and Pat Hanrahan

Stanford University

Page 36: Light Field

Marc Levoy

What’s wrong with conventional cameras?

Aperture

Page 37: Light Field

Marc Levoy

Capture the light field inside a camera

125*125 μm

500 microns

Aperture

Page 38: Light Field

Marc Levoy

Conventional versus light field camera

uv-plane st-plane

Page 39: Light Field

Marc Levoy

Conventional versus light field camera

uv-planest-plane

Page 40: Light Field

Prototype camera

4000 × 4000 pixels ÷ 292 × 292 lenses = 14 × 14 pixels per lens

Contax medium format camera Kodak 16-megapixel sensor

Adaptive Optics microlens array 125μ square-sided microlenses

Page 41: Light Field

Marc Levoy

Light Field in a Single Exposure

Page 42: Light Field

Marc Levoy

Light Field in a Single Exposure

Page 43: Light Field

Marc Levoy

Light field inside a camera body

Page 44: Light Field

Marc Levoy

Digitally stopping-down

• stopping down = summing only the central portion of each microlens

Σ

Σ

Page 45: Light Field

Marc Levoy

Digital refocusing

• refocusing = summing windows extracted from several microlenses

Σ

Σ

Page 46: Light Field

Marc Levoy

Example of digital refocusing

Page 47: Light Field

Marc Levoy

Refocusing portraits

Page 48: Light Field

Marc Levoy

Action photography

Page 49: Light Field

Extending the depth of field

conventional photograph,main lens at f / 22

conventional photograph,main lens at f / 4

Page 50: Light Field

Marc Levoy

Scene-dependent focal plane

Σ

Depth from focus problem

Interactive solution [Agarwala 2004]

Page 51: Light Field

Marc Levoy

Extending the depth of field

conventional photograph,main lens at f / 22

conventional photograph,main lens at f / 4

light field, main lens at f / 4,after all-focus algorithm

[Agarwala 2004]

Page 52: Light Field

Marc Levoy

A digital refocusing theorem

• an f / N light field camera, with P × P pixels under each microlens, can produce views as sharp as an f / (N × P) conventional camera

• these views can be focused anywhere within the depth of field of the f / (N × P) camera

Page 53: Light Field

Marc Levoy

Prior work

• integral photography– microlens array + film

– application is autostereoscopic effect

• [Adelson 1992]– proposed this camera

– built an optical bench prototype using relay lenses

– application was stereo vision, not photography

Page 54: Light Field

Marc Levoy

Digitally moving the observer

• moving the observer = moving the window we extract from the microlenses

Σ

Σ

Page 55: Light Field

Marc Levoy

Example of moving the observer

Page 56: Light Field

Marc Levoy

Moving backward and forward

Page 57: Light Field

Marc Levoy

Implications

• cuts the unwanted link between exposure(due to the aperture) and depth of field

• trades off (excess) spatial resolution for ability to refocus and adjust the perspective

• sensor pixels should be made even smaller, subject to the diffraction limit

36mm × 24mm ÷ 2.5μ pixels = 266 megapixels

20K × 13K pixels

4000 × 2666 pixels × 20 × 20 rays per pixel

• Application in microscope