Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015...

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Lenses Lenses Real-time Rendering of Physically Based Optical Effect in Real-time Rendering of Physically Based Optical Effect in Theory and Practice Theory and Practice SIGGRAPH 2015 Course SIGGRAPH 2015 Course Masaki Kawase Masaki Kawase Silicon Studio, Corp. Silicon Studio, Corp. [email protected] [email protected]

Transcript of Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015...

Page 1: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

LensesLensesReal-time Rendering of Physically Based Optical Effect in Theory and PracticeReal-time Rendering of Physically Based Optical Effect in Theory and Practice

SIGGRAPH 2015 CourseSIGGRAPH 2015 Course

Masaki KawaseMasaki KawaseSilicon Studio, Corp.Silicon Studio, Corp.

[email protected]@siliconstudio.co.jp

Page 2: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Various Bokeh from PhotographsVarious Bokeh from Photographs

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Page 3: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

ContentsContents• Aberrations and Corrections• Residual Aberrations and Bokeh Characteristics• Phenomena of Multiple-Lens Systems• Conclusion

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Page 4: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

AberrationsAberrations and Correctionsand Corrections

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Optical AberrationsOptical Aberrations• Actual lenses do not image ideally

– Imperfect focus– Image distortion– Color dispersion– And more …

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Page 6: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Major AberrationsMajor 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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Page 7: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Monochromatic and Chromatic AberrationsMonochromatic 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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Page 8: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Details of Important AberrationsDetails of Important AberrationsWhich Affect BokehWhich Affect Bokeh

Page 9: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Spherical AberrationSpherical 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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Page 10: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Principle of Spherical AberrationPrinciple 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

Incident height

Page 11: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Spherical Lens BokehSpherical Lens Bokeh

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Spot diagrams

Front bokeh (sharp-edged) Back bokeh (soft-edged)

Optical axis

Circle ofleast confusion(a.k.a. COLC)

Page 12: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Corrections for Spherical AberrationCorrections 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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Page 13: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Example of Doublet Lens CorrectionExample 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

Page 14: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

ComparisonComparison

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Spherical lens Doublet lensSharper focusFlatter bokeh

Page 15: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Spherical Aberration ChartsSpherical Aberration Charts(Longitudinal Aberration Diagrams)(Longitudinal Aberration Diagrams)

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Y: Incident heig

ht Y: Incident heig

ht

Spherical lens Doublet lens

X: Amount of aberration

• Y-axis : Incident height (independent variable)• X-axis : Amount of spherical aberration (dependent variable)

Page 16: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Spherical Aberration ChartsSpherical Aberration Charts(Longitudinal Aberration Diagrams)(Longitudinal Aberration Diagrams)

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Without correction Doublet Triplet Aspherical

Incident height

Spherical Doublet Triplet Aspherical

Page 17: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Diagrams and BokehDiagrams and Bokeh• Closer to vertical line,

better correction– Sharper focus– Flatter bokeh

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Spherical Doublet Triplet Aspherical

Front bokeh

Back bokeh

Page 18: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Axial Chromatic AberrationAxial 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 CAPrinciple of Axial CA

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Focal length on each wavelength

Incident height

Page 20: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Bokeh of Axial CABokeh of Axial CA

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Spot diagrams of marginal rays

Front bokeh Back bokeh

Page 21: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Effects of Axial CAEffects 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

Page 22: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Correction of Axial Chromatic AberrationCorrection 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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Page 23: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Apochromatic triplet

Achromatic LensAchromatic 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.svgEgmason, https://commons.wikimedia.org/wiki/File:Apochromat_2.svg

Page 24: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Example of Achromatic Doublet CorrectionExample 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

Page 25: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Example of Achromatic Doublet BokehExample of Achromatic Doublet Bokeh

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Spot diagram of marginal rays

Front bokeh Back bokeh

Page 26: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

ComparisonComparison

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Axial chromatic aberration Residual chromatic aberrationa.k.a. secondary spectrum

Page 27: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Correction by Achromatic DoubletCorrection 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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Page 28: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Diagrams and Bokeh with Multiple WavelengthsDiagrams and Bokeh with Multiple Wavelengths

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Doublet lensSpherical lenswithout correction

Page 29: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Corrected Bokeh from AberrationsCorrected 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

Page 30: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Front Bokeh with Purple FringeFront Bokeh with Purple Fringe

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Front bokeh in photographs

Page 31: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Back Bokeh with Green FringeBack Bokeh with Green Fringe

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Back bokeh in photographs

Page 32: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Is Residual Aberration Visible or Not?Is Residual Aberration Visible or Not?

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Visible

Strongly visibleSlightly out of focus

with a large aperture

Large out of focuswith a small aperture

Less visible

Out-of-focus amount

Aperture

size

Focus Blurry

LargeS

mall

Smaller bokeh

Larger bokeh

Page 33: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Is Residual Aberration Visible or Not? (Cont’d)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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Page 34: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Residual Aberrations andResidual Aberrations andBokeh CharacteristicsBokeh Characteristics

Page 35: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Bokeh CharacteristicsBokeh 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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Page 36: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Various Bokeh from PhotographsVarious Bokeh from Photographs

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Page 37: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Phenomena of Multiple-Lens SystemsPhenomena of Multiple-Lens Systems

Page 38: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Multiple-Lens SystemsMultiple-Lens Systems• Actual optical system is composed of multiple lenses

in order to:– Correct aberrations– Zoom– Reduce focus breathing– Others

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Page 39: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Multiple-Lens vs. Single-LensMultiple-Lens vs. Single-Lens• More complex aberrations• Various bokeh characteristics• Different focus breathing• Variable maximum aperture• Optical Vignetting• And more …

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Page 40: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Focus BreathingFocus 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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Page 41: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Focal Length, Sensor Size and FOVFocal 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

Page 42: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Accurate FOV CalculationAccurate 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

Page 43: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Focusing MechanismsFocusing 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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Page 44: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Focusing Mechanism and Breathing ExamplesFocusing 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

Page 45: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Focusing Mechanism and Breathing ExamplesFocusing 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

Page 46: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Focusing Mechanism and Breathing ExamplesFocusing 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

Page 47: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Focal length is shrunk to 40% in this caseImage distance is also shrunk to 50%FOV becomes wider

Focusing Mechanism and Breathing ExamplesFocusing Mechanism and Breathing Examples

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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

Page 48: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Variable Aperture Zoom LensesVariable Aperture Zoom Lenses

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Narrow (60mm)Maximum aperture is f/4.0

Wide (12mm)Maximum aperture is f/2.8

Page 49: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Effective Aperture Diameter Effective Aperture Diameter ‘D’‘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 aperturediameter

Page 50: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Zooming Varies Virtual Image DiameterZooming Varies Virtual Image Diameter• To keep the exposure, narrower FOV requires larger

diameterD = f / F

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Wide (12mm) f/2.8D = 12/2.8 = ~4.2mm

Φ~4.2mm

Narrow (60mm) f/4D = 60/4 = 15mm

Φ15mm

Zoom lens12-60mm F2.8-4.0

Page 51: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Zoom Lens TypesZoom 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”

Page 52: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Examples of Zoom Lens ProductsExamples 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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Page 53: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Tendency of Actual LensesTendency 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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Page 54: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

ConclusionConclusion

Page 55: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

ConclusionConclusion• 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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Page 56: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

Conclusion (cont’d)Conclusion (cont’d)• Actual optical system is composed of multiple lenses

in 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

Page 57: Lenses Real-time Rendering of Physically Based Optical Effect in Theory and Practice SIGGRAPH 2015 Course Masaki Kawase Silicon Studio, Corp. masa@siliconstudio.co.jp.

ReferencesReferences• 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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