real-time rendering of physically based optical effect in ......•bokeh is rich in variety...
TRANSCRIPT
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LensesReal-time Rendering of Physically Based Optical Effect in Theory and Practice
SIGGRAPH 2015 Course
Masaki Kawase
Silicon Studio, Corp.
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Various Bokeh from Photographs
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Contents
• Aberrations and Corrections
• Residual Aberrations and Bokeh Characteristics
• Phenomena of Multiple-Lens Systems
• Conclusion
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Aberrations and Corrections
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Optical Aberrations
• Actual lenses do not image ideally
– Imperfect focus
– Image distortion
– Color dispersion
– And more …
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Major Aberrations
• Monochromatic aberrations– Occur even with single-wavelength rays– Also known as Seidel's five aberrations
• Chromatic aberrations– Caused by dispersion
• The separation of visible light into its different colors • Different refractive indices in multi-wavelength rays
– Caused with multi-wavelength rays but:• Occurs as blur in monochrome film• Does not occur in color film with single-wavelength rays
– Such as Sodium-vapor Lamps
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Monochromatic and Chromatic Aberrations
• Monochromatic aberrations (Seidel's five aberrations)– Spherical Aberration (SA)
– Coma
– Field Curvature
– Astigmatism
– Distortion
• Chromatic aberrations (CA)– Lateral Chromatic Aberration (CA of Magnification)
– Longitudinal Chromatic Aberration (Axial CA)
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Details of Important AberrationsWhich Affect Bokeh
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Spherical Aberration
• The focal length deviation of rays parallel to the optical axis
• The aberration is caused by a spherical lens
– Spherical surfaces are:
• Not ideal for lenses
• Commonly used due to the high manufacturability
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Principle of Spherical Aberration
• The farther the rays are from the optical axis,the closer they intersect the optical axis
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Focal length of each incident height
Paraxial focal length
Optical axis
Incid
ent h
eig
ht
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Spherical Lens Bokeh
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Spot diagrams
Front bokeh (sharp-edged) Back bokeh (soft-edged)
Optical axis
Circle of
least confusion
(a.k.a. COLC)
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Corrections for Spherical Aberration
• Doublet lens– Pair of convex and concave lenses– Concave lens aberration cancels convex lens one– Cannot cancel perfectly
• Triplet lens– An additional lens to doublet– Still not perfect, but much better
• Aspherical lens– Surface is close to ideal– Expensive to make– Perfectly remove spherical aberration
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Example of Doublet Lens Correction
• More complicated bokeh than spherical
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Focal point of each incident height
Circle of least confusion plane
Front bokeh Back bokeh
Optical axis
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Comparison
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Spherical lens Doublet lens
Sharper focus
Flatter bokeh
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Spherical Aberration Charts(Longitudinal Aberration Diagrams)
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Y: In
cid
ent h
eig
ht
Y: In
cid
ent h
eig
ht
Spherical lens Doublet lens
X: Amount of aberration
• Y-axis : Incident height (independent variable)• X-axis : Amount of spherical aberration (dependent variable)
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Spherical Aberration Charts(Longitudinal Aberration Diagrams)
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Without correction Doublet Triplet Aspherical
Incid
ent h
eig
ht
Spherical Doublet Triplet Aspherical
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Diagrams and Bokeh
• Closer to vertical line,better correction
– Sharper focus
– Flatter bokeh
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Spherical Doublet Triplet Aspherical
Front bokeh
Back bokeh
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Axial Chromatic Aberration
• Differences of ray wavelengths cause aberration
• Refractive indices differ by wavelengths
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DrBob, https://en.wikipedia.org/wiki/File:Chromatic_aberration_lens_diagram.svg
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Principle of Axial CA
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Focal length on each wavelength
Incid
ent h
eig
ht
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Bokeh of Axial CA
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Spot diagrams of marginal rays
Front bokeh Back bokeh
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Effects of Axial CA
• Front bokeh shows red fringe
• Back bokeh shows blue fringe
• Relatively larger fringe around the focal point
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Out-of-focus images made by a magnifier
Front bokeh Back bokeh
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Correction of Axial Chromatic Aberration
• Achromatic lens
– Correction with doublet or triplet etc.
• Coupling of different dispersion property lenses
• Focusable multi-wavelength rays on a single point
• Cannot correct perfectly on all wavelengths
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Apochromatic triplet
Achromatic Lens
• Achromatic lens (Achromat)– Achromatic doublet etc.
– Focusable two wavelength rays on the same point
• e.g. red and blue
• Apochromatic lens (APO)– Apochromatic triplet etc.
– Generally focusable three wavelength rays• e.g. red, green and blue
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DrBob, https://commons.wikimedia.org/wiki/File:Lens6b-en.svg
Egmason, https://commons.wikimedia.org/wiki/File:Apochromat_2.svg
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Example of Achromatic Doublet Correction
• Cannot match all color focal points
– If you match red and blue, you cannot match others (green etc.)
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Focal plane on each wavelength
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Example of Achromatic Doublet Bokeh
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Spot diagram of marginal rays
Front bokeh Back bokeh
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Comparison
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Axial chromatic aberration Residual chromatic aberration
a.k.a. secondary spectrum
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Correction by Achromatic Doublet
• Doublet also corrects spherical aberration
• Combination bokeh of each character– Residual aberration of spherical aberration
• Soft / Sharp edge
• Dark center / sharp peak
– Residual aberration ofaxial chromatic aberration
• Concentric colored circles
• ⇒Complicated gradation
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*
=
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Diagrams and Bokeh with Multiple Wavelengths
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Doublet lensSpherical lens
without correction
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Corrected Bokeh from Aberrations
• Correction by achromatic doublets
– Widely used
– Typical correction example
• Soft purple fringe on front bokeh
• Sharp green fringe on back bokeh
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Front bokeh in photographs Back bokeh in photographs
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Front Bokeh with Purple Fringe
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Front bokeh in photographs
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Back Bokeh with Green Fringe
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Back bokeh in photographs
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Is Residual Aberration Visible or Not?
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Strongly visibleSlightly out of focus
with a large aperture
Large out of focuswith a small aperture
Less visible
Out-of-focus amount
Apertu
re s
ize
Focus Blurry
Larg
eS
mall
Smaller bokeh
Larger bokeh
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Is Residual Aberration Visible or Not? (Cont’d)
• Strongly visible
– Slightly out of focus with a large aperture
• Less visible
– Large out of focus with a small aperture
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Residual Aberrations andBokeh Characteristics
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Bokeh Characteristics
• Bokeh Characteristics vary by:
– Aberrations
– Residual aberrations
• Different corrections make different characteristics
• Residual aberrations are essentially undesired
– But they are characteristics of real photos
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Various Bokeh from Photographs
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Phenomena of Multiple-Lens Systems
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Multiple-Lens Systems
• Actual optical system is composed of multiple lensesin order to:
– Correct aberrations
– Zoom
– Reduce focus breathing
– Others
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Multiple-Lens vs. Single-Lens
• More complex aberrations
• Various bokeh characteristics
• Different focus breathing
• Variable maximum aperture
• Optical Vignetting
• And more …
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Focus Breathing• Focus breathing
– FOV varies when focusing
• Types of focus breathing– Single Lens
• Focusing by shifting lens or sensor– Focal length is constant and independent of focus distance
• At close focus, FOV becomes narrower– In spite of constant focal length
» Extend image distance (between lens and sensor)» While the F-number is the same, the effective F-number is larger (darker)
– Multiple-lens system• Breathing varies by the focusing mechanism
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Focal Length, Sensor Size and FOV
• Field of view is often explained as…– Depends on the ratio of sensor size and focal length
• fov = atan(h / 2f) * 2
• f = h / (tan(fov / 2) * 2)
• fov : field of view
• h : sensor size
• Not accurate– Accurate only when focusing on infinite distance
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f
do=∞ di = f
fov
hD
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Accurate FOV Calculation• Field of view
– Depends on the ratio of sensor size and image distance• fov = atan(h / 2di) * 2• di = h / (tan(fov / 2) * 2)
– Effective calculation only when a lens exists• fov = atan(h (do - f) / 2do f) * 2 • f = (do h / 2) / (tan(fov / 2) * do + h / 2)
• Effective F-number– Fe = di / D– Effective calculation only when a lens exists
• Fe = (1 + M) F• Fe = (di / f) F
• Focus distance is also required in order to calculate correctly– If the focal length is constant, FOV becomes narrower with finite focus
Optical magnification ‘M’M = di / do
M = f / (do – f) = di / f - 1
fovh
f
do <∞ di > f
D
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Focusing Mechanisms
• All-Group Focusing / Film-Back Focusing– Same mechanism as single-lens system– Used in old lenses– FOV becomes narrower when close focus
• An Effective F-number becomes decreased
• Front-Group Focusing– Used in old lenses– Usually FOV becomes narrower when close focus
• An Effective F-number becomes decreased
• Inner (Internal) / Rear Focusing– a.k.a. IF / RF– Used in recent zoom lenses– Usually FOV becomes wider when close focus (less expensive lenses)– No-breathing focus (relatively expensive lenses)
• An Effective F-number is constant
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Focusing Mechanism and Breathing Examples
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All-Group / Film-Back FocusingFOV becomes narrower
f
do di
fov
h
Inner Focusing (expensive lens)No breathingFocal length becomes shrunk
Infinite focus
Close focus
fov
h
f
do di
f
do=∞ di =f
fov
h
f
do=∞ di =f
fov
h
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Focusing Mechanism and Breathing Examples
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f=3
do=∞ di=3=f
fov
h
f=2
do=6=3f di=3=1.5f
fov
h
f=3
do=∞ di=3=f
fov
h
M = di / do = 1.0 M = di / do = 0.5
fov
h
f=3
do=6=2f di=6=2f
Infinite focus
Focus on 2f
Shift sensor to backward 2f (or shift lens)Focal length is constantEffective F-number becomes darker
Image distance is fixedFocal length is shrunk to 66.7%FOV and Effective F-number are constant
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Focusing Mechanism and Breathing Examples
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Typical Inner FocusingFOV becomes widerFocal length is largely shrunk
f
do di
fov
h
All-Group / Film-Back FocusingFOV becomes narrower
Infinite focus
Close focus
fov
h
f
do di
f
do=∞ di =f
fov
h
f
do=∞ di =f
fov
h
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Focal length is shrunk to 40% in this caseImage distance is also shrunk to 50%FOV becomes wider
Focusing Mechanism and Breathing Examples
47
fov
h
f=3
do=6=2f di=6=2f
f=3
do=∞ di=3=f
fov
h
f=1.2
do=6=5f di=1.5=1.25f
fov
h
f=3
do= ∞ di=3=f
fov
h
M = di / do = 1.0 M = di / do = 0.25
Infinite focus
Focus on 2f
Shift sensor to backward 2f (or shift lens)Focal length is constantEffective F-number becomes darker
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Variable Aperture Zoom Lenses
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Narrow (60mm)
Maximum aperture is f/4.0
Wide (12mm)
Maximum aperture is f/2.8
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Effective Aperture Diameter ‘D’
• Diameter of “Entrance Pupil”
– Virtual image of the aperture as seen from the front
– NOT a physical aperture diameter
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Effective aperture
diameter
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Zooming Varies Virtual Image Diameter
• To keep the exposure, narrower FOV requires larger diameter
D = f / F
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Wide (12mm) f/2.8
D = 12/2.8 = ~4.2mm
Φ~4.2mm
Narrow (60mm) f/4
D = 60/4 = 15mm
Φ15mm
Zoom lens
12-60mm F2.8-4.0
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Zoom Lens Types
• Fixed Aperture Zoom Lens– Minimum F-number is constant over the entire zoom range– Effective diameter is proportional to focal length (D = f / F)
• Variable Aperture Zoom Lens– Minimum F-number becomes larger as the FOV becomes narrower– Effective diameter is not proportional to focal length
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Narrow (60mm)
f/4.0
Wide (12mm)
f/2.8
*Note that the “Minimum F-number”
means the “Maximum Aperture”
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Examples of Zoom Lens Products• OLYMPUS D.ZUIKO (4/3“)
– 14-42mm F3.5-5.6– 12-60mm F2.8-4.0– 35-100mm F2.0 Fixed aperture
• CANON EF-S (APS-C)– 17-55mm F2.8 Fixed aperture– 18-135mm F3.5-5.6– 55-250mm F4.0-5.6
• DX NIKKOR (APS-C)– 17-55mm F2.8 Fixed aperture– 18-140mm F3.5-5.6– 55-200mm F4.0-5.6
• CANON EF (35mm)– 24-70mm F2.8 Fixed aperture– 70-200mm F2.8 Fixed aperture– 100-400mm F4.5-5.6
• FX NIKKOR (35mm)– 24-70mm F2.8 Fixed aperture– 70-200mm F2.8 Fixed aperture– 80-400mm F4.5-5.6
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Tendency of Actual Lenses
• Lower magnification zoom
• More expensive “Brighter lens”
• Higher magnification zoom
• Less expensive “Darker lens”
Minimum F-numbervaries a little
Minimum F-numbervaries a lot
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Conclusion
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Conclusion
• Actual lenses have various aberrations
– Many solutions correct aberrations
– Aberrations cannot be completely corrected
• Residual aberrations give bokeh its character
• Bokeh is rich in variety
– Different corrections show different representations
– Color fringes and gradation vary between front and back bokeh
– Conspicuousness: smaller out-of-focus > larger out of focus
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Conclusion (cont’d)
• Actual optical system is composed of multiple lensesin order to:– Correct aberrations
– Zoom
– Reduce focus breathing
• Many phenomena do not conform to single lens rules– Different focus breathing
– Different zooming aperture varying
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by different mechanisms
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References
• Kawase, M. “Camera, Optics Theory and Post Effects for Renderists.” Computer Entertainment Developers Conference, 2007.
• Kawase, M. “Optics Knowledge to Achieve Attractive Images.” Computer Entertainment Developers Conference, 2010.
• Trávník, J. “On Bokeh.” Jakub Trávník's resources. http://jtra.cz/stuff/essays/bokeh/index.html
• 安藤幸司『光と光の記録「レンズ編」』 AnfoWorld http://www.anfoworld.com/LensMF.html
• 吉田正太郎(1997)『カメラマンのための写真レンズの科学』地人書館.
• 永田信一(2002)『図解 レンズがわかる本』日本実業出版社.
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