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Non-line-of-sight Imaging with Partial
Occluders and Surface Normals
Felix Heide1,2, Matthew O’Toole1,3, Kai Zang1, David B. Lindell1, Steven Diamond1, Gordon Wetzstein1
1Stanford University 2Princeton University 3CMU
ACM SIGGRAPH 2019
Non-line-of-sight Imaging
Non-line-of-sight Imaging
Hidden Objects Behind Hidden Objects
Experimental Non-line-of-sight Imaging
Experimental Non-line-of-sight Imaging
Reconstruction (TV-Prior):
Simulated Transients :
𝑡 [ps]
Partially-Occluded
Non-line-of-sight Imaging
Reconstruction (TV-Prior):
Time-tagged Photon Counts – Transient Images
Experimental measurements Photograph of hidden scene
𝑡 [ps]
Measurement Slice Reconstruction
Transient Image Slice
Non-line-of-sight Imaging
[1] Velten et al. (2012)
[2] Gupta et al. (2012)
[3] Wu et al. (2012)
[4] Buttafava et al. (2015)
[5] O’Toole et al. (2018)
[6] Lindell et al.(2019)
Direct Pulsed
Measurement
[1] Katz et al. (2012)
[2] Katz et al. (2014)
[3] Smith et al. (2018)
[4] Kadambi et al. (2016)
[5] Heide et al. (2015)
Coherent and Modulated
Measurment
Accurate Image Formation Models
and Priors
[1] Xin et al. (2019)
[2] Thrampoulidis et al. (2019)
[3] Tancik et al. (2018)
[4] Chen et al. (2019)
Tracking using
Intensity Imaging
[1] Klein et al. (2012)
[2] Smith et al. (2018)
[3] Boger-Lombard and Katz (2018)
[4] Bouman et al.
Non-line-of-sight Imaging
[1] Velten et al. (2012)
[2] Gupta et al. (2012)
[3] Wu et al. (2012)
[4] Buttafava et al. (2015)
[5] O’Toole et al. (2018)
[6] Lindell et al.(2019)
Direct Pulsed
Measurement
[1] Katz et al. (2012)
[2] Katz et al. (2014)
[3] Smith et al. (2018)
[4] Kadambi et al. (2016)
[5] Heide et al. (2015)
Coherent and Modulated
Measurment
Accurate Image Formation Models
and Priors
[1] Xin et al. (2019)
[2] Thrampoulidis et al. (2019)
[3] Tancik et al. (2018)
[4] Chen et al. (2019)
Tracking using
Intensity Imaging
[1] Klein et al. (2012)
[2] Smith et al. (2018)
[3] Boger-Lombard and Katz (2018)
[4] Bouman et al.
Image Formation Without Occlusions *
* ( or explicitly requires them )
Continuous Image Formation without
Occlusions
Steered Laser
& SPAD
Detector
Scanned Wall
Area
x′i
y′
Confocal Measurements:
𝑡 [ps]
j 𝜌j
x
y
z
Path Length
Gating
Voxel
Volume
Continuous Image Formation with
Occlusions
Steered Laser
& SPAD
Detector
Scanned Wall
Area
x′i
y′
j
Confocal Measurements:
𝑡 [ps]
Visibility
Factors
Voxel
Volume
Normal
Factors
x
y
z
Path
Gating
j
Steered Laser
& SPAD
Detector
Scanned Wall
Area
x′i
y′
j Confocal Measurements:
𝑡 [ps]
Visibility
Factors
Voxel
Volume
Normal
Factors
x
y
z
Path
Gating
Continuous Image Formation with
Occlusions
Steered Laser
& SPAD
Detector
Scanned Wall
Area
x′i
y′
Confocal Measurements:
𝑡 [ps]
Retro
Reflection
n
Diffuse
Reflection
Visibility
Factors
Voxel
Volume
Normal
Factors
𝜔
x
y
z
j
Continuous Image Formation with Normals
Full Continuous Image Formation
Model
Steered Laser
& SPAD
Detector
Scanned Wall
Area
x′i
y′
Confocal Measurements:
𝑡 [ps]
Retro
Reflection
n
Diffuse
Reflection
𝜔
x
y
z
j
Factorized Transient Light Transport
Continuous Model:
Discretize
Measurement
𝑥′
, 𝑦′
, 𝑡:
Discrete
Model:
Discretize Space
𝑥′
, 𝑦′
, 𝑥, 𝑦, 𝑧:
Discretized Operator Size
Discrete
Model:
Steered Laser
& SPAD
Detector
Scanned Wall
Area
𝑁
𝑁
𝑁
𝑁
𝑁
i
j
How much light can get
reflected from j to i ?
vij
Wall
pos.
Vol pos.
j
i
Visualization of the Visibility Matrix
Ground Truth Scene Visibility Term for
Pixel Position indicated on the leftViewing direction towards wall
Discretized Operator Size
Discrete
Model:
Steered Laser
& SPAD
Detector
Scanned Wall
Area
𝑁
𝑁
𝑁
𝑁
𝑁
i
j
How does forshortening at j
reduce the light back to i ?
𝜔
nj
Nij
Vol pos.
j
i
Wall
pos.
Copy across all time-stamps.
Copy Matrix:
Time-dependent Transport.
Sampling Matrix:
Discretized Operator Size
Discrete
Model:
Visibility Matrix:
Steered Laser
& SPAD
Detector
Scanned Wall
Area
𝑁
𝑁
𝑁
𝑁
𝑁
i
j
Normal Matrix:𝜔
nj
Matrix-Free
Implementation
Recover Factorized Transient Light Transport
Discrete
Model:
Optimization
Problem:
Spherical Normal
Parametrization
MAP Estimate
Regularizer (Prior)
Memory Limitations
Visibility Vars:
Steered Laser
& SPAD
Detector
Scanned Wall
Area
𝑁
𝑁
𝑁
𝑁
𝑁
i
j
Normal Vars:
Proposed Method:
Backprojection:
Matrix-Free Inverse:
For a volume of 643
Matlab (CPU) ~ 500GB and 2h
For a volume of 403
Cuda (GPU) ~ 14GB and 180s
Occluded Hidden Scene in 2D
2D Setup
Geometry:
No
Occlusion
Proposed
Measuremen
t
Detector
Occluded Hidden Scene in 2D
Backprojection
Method
Filtered
Backprojection
Linear Inverse
Method
Proposed
Approach
Ground
Truth
2D Setup
Geometry:
Detector
Occluded Hidden Scene in 3D
Filtered
Backprojection
Linear Inverse
Method
Proposed
Approach
Ground
Truth
Partially Occluded Hidden Scene in 3D
Filtered
Backprojection
Linear Inverse
Method
Proposed
Approach
Ground
Truth
Transient Measurement
𝑡 [ps]
Backprojection
Method
Filtered Backprojection
Method
Linear Inverse
Method
Proposed
Approach
Albedo Reconstructions
Backprojection
Method
Filtered Backprojection
Method
Linear Inverse
Method
Proposed
Approach
More Difficult Albedo Reconstructions
Backprojection
Method
Linear Inverse
Method
Proposed
Approach
Self-Occlusions
Estimated Normals
Physical Measurement Setup
Single Photon Avalanche Detector
MPD PD-100
100 𝜇𝑚 active area
Relay Optics
75mm achromatic
doublet lens
Beam-Splitter in Coaxial Alignment
Short-Pulsed Laser Illumination (50ps FWHM)
AlphaLas
PICOPOWER-LD-670-50
Scanning Galvo Mirror System
Illumination Path
Detection Path
Backprojection
Method
Linear Inverse
Method
Proposed
Approach
Experimental Reconstruction Results
LCT
Method
Scene PhotographMeasurement
Slice
Backprojection
Method
Linear Inverse
Method
Proposed
Approach
Experimental Reconstruction Results
LCT
Method
Scene Photograph
Backprojection
Method
Linear Inverse
Method
Proposed
Approach
Experimental Reconstruction Results
LCT
Method
Scene Photograph
Backprojection
Method
Linear Inverse
Method
Proposed
Approach
Experimental Reconstruction Results
LCT
Method
Scene Photograph
Backprojection
Method
Linear Inverse
Method
Proposed
Approach
Experimental Reconstruction Results
LCT
Method
Estimated NormalsScene Photograph
Future Directions
Scattering Media and
Active Sources
Learned Visibility Matrices
And Scene Representations
1
6
4
1
2
8
2
5
6
1
2
8
3
2
6
4
5
1
2
2
5
6
3
2
Higher-Order Bounces
Every Surface Becomes a “Sensor”
Non-line-of-sight Imaging with Partial
Occluders and Surface Normals
Felix Heide1,2, Matthew O’Toole1,3, Kai Zang1, David B. Lindell1, Steven Diamond1, Gordon Wetzstein1
1Stanford University 2Princeton University 3CMU
ACM SIGGRAPH 2019

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Non-line-of-sight Imaging with Partial Occluders and Surface Normals | TOG 2019