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Instant Dehazing of Images using Polarization
Yoav Schechner, Srinivasa Narasimhan, Shree Nayar Department of Computer Science Columbia University Sponsors: DARPA HID, Morin Foundation, NSF
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Imaging through Haze Recover: Previous work Object + haze layers
clear day moderate haze very hazy Previous work Pure image processing Grewe & Brooks ’98, Kopeika ’98 Oakley & Satherley ’98 Physics based Nayar & Narasimhan ’99 Polarization filtering Shurcliff & Ballard ’64 Object + haze layers Scene structure Info about the aerosols Recover: Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Imaging through Haze object R A direct T
camera object radiance R Airlight A scattering direct transmission T Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Multiplicative & additive models Color
Airlight A camera object radiance R scattering direct transmission T 1 z 1 z z is a function of (x,y) Multiplicative & additive models - similar dependence Color
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Polarization and Haze A
polarizer direct transmission Along the line of sight, polarization state is distance invariant Assume: The object is unpolarized @ all orientations camera Plane of rays determines airlight components A > _ + Airlight degree of polarization p=0 unpolarized = p=1 polarized =0 Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Life is tough… Trivial case I
Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar Life is tough… I Trivial case … still, there is a dominant polarization
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Experiment I = A T/2 + Best polarized image
Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Experiment = I T/2 + A Worst polarized image
Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Polarization measurement
polarizer camera 180 o 3 general measurements suffice Polarization vector determination
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Model Recovery )/p e I R + = / ) ( e R T = A + = 2 / T I A
camera object radiance R airlight A transmission T + = 2 / T I A 2 input images: Recovery for known A p , βz e I R - + = / ) ( radiance )/p z 1 b depth I A _ βz e R T - = transmission ÷ ø ö ç è æ A 1 airlight + p polarization degree
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airlight polarization
Model saturated airlight A airlight polarization p camera 2 input images: Recovery for known A p , βz e I R - + = / ) ( radiance )/p z 1 b depth I + = 2 / T I A A transmission βz e R T - = airlight ÷ ø ö ç è æ - = βz e A 1 _ A + p polarization degree
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Dehazing Experiment I Best polarized image
Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Dehazing Experiment R Dehazed image
Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Range map ( ) = pA I e 1 log depth component images Airlight
- = pA I e z 1 b log depth component images Airlight saturation polarization p
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Aerosol distribution º å b b depends on the wavelength l l
Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar l 400 600 500 700 nm b Fog, heavy dust Rayleigh (air) Red b ) x,y z ( Green Blue å ) ( x,y z Blue b Green Red
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Dehazing Experiment I Best polarized image
Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Dehazing Experiment R Dehazed image
Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Range map Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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Conclusion Fast Acquisition Vision through Haze Depth
from Polarization Aerosol Size l b Instant Dehazing: Yoav Schechner, Srinivasa Narasimhan, Shree Nayar
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