cvpr cvpr2013 cvpr2013-219 knowledge-graph by maker-knowledge-mining

219 cvpr-2013-In Defense of 3D-Label Stereo


Source: pdf

Author: Carl Olsson, Johannes Ulén, Yuri Boykov

Abstract: It is commonly believed that higher order smoothness should be modeled using higher order interactions. For example, 2nd order derivatives for deformable (active) contours are represented by triple cliques. Similarly, the 2nd order regularization methods in stereo predominantly use MRF models with scalar (1D) disparity labels and triple clique interactions. In this paper we advocate a largely overlooked alternative approach to stereo where 2nd order surface smoothness is represented by pairwise interactions with 3D-labels, e.g. tangent planes. This general paradigm has been criticized due to perceived computational complexity of optimization in higher-dimensional label space. Contrary to popular beliefs, we demonstrate that representing 2nd order surface smoothness with 3D labels leads to simpler optimization problems with (nearly) submodular pairwise interactions. Our theoretical and experimental re- sults demonstrate advantages over state-of-the-art methods for 2nd order smoothness stereo. 1

Reference: text


Summary: the most important sentenses genereted by tfidf model

sentIndex sentText sentNum sentScore

1 s e Abstract It is commonly believed that higher order smoothness should be modeled using higher order interactions. [sent-5, score-0.16]

2 For example, 2nd order derivatives for deformable (active) contours are represented by triple cliques. [sent-6, score-0.161]

3 Similarly, the 2nd order regularization methods in stereo predominantly use MRF models with scalar (1D) disparity labels and triple clique interactions. [sent-7, score-0.557]

4 In this paper we advocate a largely overlooked alternative approach to stereo where 2nd order surface smoothness is represented by pairwise interactions with 3D-labels, e. [sent-8, score-0.399]

5 Contrary to popular beliefs, we demonstrate that representing 2nd order surface smoothness with 3D labels leads to simpler optimization problems with (nearly) submodular pairwise interactions. [sent-12, score-0.429]

6 One reason for their popularity is that when applying movemaking algorithms such as α-expansion [4] or fusion moves [8] they often result in submodular moves, allowing efficient computation using min-cut/max-flow algorithms [4]. [sent-18, score-0.333]

7 Many basic optimization methods for stereo use scalar (1D) disparity labels. [sent-19, score-0.369]

8 ca regularization potentials assign higher cost to surfaces with larger tilt [4]. [sent-27, score-0.165]

9 To address more general scenes our paper follows the popular trend of using 2nd derivative surface regularization for stereo [9, 15]. [sent-29, score-0.308]

10 [15] retain the scalar disparity labels while using triple-cliques to penalize 2nd derivatives of the reconstructed surface. [sent-32, score-0.384]

11 In contrast, Li and Zucker [9] use 3D-labels corresponding to tangent planes to encode 2nd order disparity map smoothness as pairwise interactions. [sent-35, score-0.776]

12 The first term computes the difference of the disparity assignment, and the disparity predicted by the neighboring tangent plane. [sent-38, score-0.817]

13 ) The second term penalizes the (squared) angular difference between neighboring tangent plane normals. [sent-40, score-0.459]

14 [15] that only use a disparity estimate at each pixel, the approach by Li and Zucker [9] requires discretization of a much larger label space. [sent-44, score-0.243]

15 As shown in [15], this specific approach results in disparity maps that are inferior to those of Woodford et al. [sent-46, score-0.243]

16 The discussed limitations of [9] may have helped to promote the general perception of triple interactions of scalar disparity labels as a superior approach for modeling 2nd order smoothness. [sent-47, score-0.443]

17 This makes it possible to precompute and penalize 2nd order smoothness via 111777223088 a unary term. [sent-50, score-0.203]

18 There is however no smoothness interaction between models and therefore it is not possible to combine local models into global ones. [sent-51, score-0.15]

19 In this paper we propose a new 3D-label stereo algorithm encoding 2nd order smoothness of the disparity map with pairwise interactions. [sent-53, score-0.529]

20 We show how to properly measure 2nd derivative of the reconstructed surface using pairwise cliques when the labels are tangent planes. [sent-55, score-0.498]

21 Instead of using a fixed set of locally precomputed tangents, we adaptively generate new surface proposals based on the current surface estimate. [sent-56, score-0.316]

22 [15] we show that our formulation is submodular when using planar proposals, and verify experimentally that Roof duality [11] labels much more pixels for general proposals with our formulation. [sent-59, score-0.378]

23 We show that the use of even higher order labels (that encode higher order derivatives) further extends the class of submodular functions. [sent-61, score-0.222]

24 In addition we present a version of our method that works with depth rather than disparity and, therefore, does not require rectified cameras. [sent-62, score-0.43]

25 The possibility to decrease the energy for each fusion move is an attractive feature, however there is no guarantee on how many variables will be labeled in each fusion move. [sent-91, score-0.317]

26 For submodular fusion moves we are guaranteed to label all variables. [sent-95, score-0.333]

27 A Second Order Multi-View Stereo Smoothness Prior for In this section we present a second order smoothness prior for dense multi-view stereo reconstruction. [sent-98, score-0.223]

28 To each viewing ray we will assign a plane that locally represents the surface geometry close to the ray. [sent-101, score-0.334]

29 The intersection between the ray and the plane will be the estimated 3D point. [sent-102, score-0.165]

30 By interpreting the planes as a tangents of the viewed 3D surface we can encourage smooth solutions by penalizing neighboring 3D-points that deviate largely from neighboring tangents. [sent-103, score-0.485]

31 Rectified Cameras and Disparity Maps We will start by assuming that the cameras have been rectified, since this allows us to work in disparity space. [sent-106, score-0.279]

32 gT pheix goal no tfh hsete irmeoa gise t Io estimate the function D : I R that gives a disparity value → feostri emaacthe pixel ninc ttihoen image. [sent-111, score-0.264]

33 →To R Re tahchat pixel p we wariillty assign a tangent plane that locally approximates this function. [sent-112, score-0.401]

34 We can think of these tangents as samples of the disparity function and its derivatives. [sent-113, score-0.368]

35 By the function TpD : I R we → twioilnl mean tsh dee tangent sa. [sent-114, score-0.243]

36 o→n o Rf wthee whole image, that is TpD (x) = D (p) + ∇D (p)T (x − p), (4) where D (p) and ∇D (p) is the assigned disparity and disparity gradient (dw ∇ithD respect htoe athssei image csopoarridtyina anted system) at pixel p. [sent-116, score-0.507]

37 We define a pairwise interaction between neighboring pixels as Vpq = |TpD (q) − D (q) |, (5) That is, Vpq measures the curve’s deviation from the tangent plane, see Figure 1. [sent-117, score-0.384]

38 Intuitively, if the surface is smooth then 111777223 919 for parallel viewing rays. [sent-118, score-0.194]

39 (7) That is, Vpq measures the second derivative at p in direction q p of the underlying disparity function. [sent-123, score-0.332]

40 However directly penalizing 2nd derivative of the depth function is not a good idea. [sent-128, score-0.228]

41 In general the projection of a plane will not yield a linear depth function unless the camera is affine (which can be seen from (11) below). [sent-129, score-0.213]

42 Therefore we will instead measure the deviation from the tangent plane along the viewing ray. [sent-131, score-0.417]

43 = 1 and ap ∈ R we denote the tangent plane ∈at p given by =the 1 equation npTx + ap = 0. [sent-138, score-0.349]

44 between the viewing ray at q and the tangent plane at p. [sent-140, score-0.476]

45 We let Tpd : I R+ → abet qth aen depth tfaunncgetinotn olfa nthee a tangent plane atd point p, t Rhat is, Q? [sent-141, score-0.456]

46 We can calculate the tangent function using Tpd(q) = −npTapqh. [sent-143, score-0.243]

47 (11) (Here we are assuming that the viewing ray is not completely contained in the tangent plane. [sent-144, score-0.37]

48 In contrast disparity is inversely proportional to depth and will therefore be linear. [sent-146, score-0.35]

49 Given the estimated tangent plane at p and the depth at q the interaction computes the distance between the estimated 3D point and the tangent plane along the view- ing ray. [sent-154, score-0.853]

50 The smoothness term will penalize deviations from planes and thereby encourage solutions with small second derivatives. [sent-155, score-0.29]

51 Submodularity of Fusion Moves In this section we will show that fusion moves [8] with our interactions are often submodular. [sent-158, score-0.226]

52 Given a current disparity function D and a proposal function P the fusion move a flluonwcsti pixels aton change tphoesiarl l a fbuenlcst ifornom P Pth teh tangents of D to the tangents of P. [sent-159, score-0.705]

53 In what follows we will use Vpq(D, P) = |TpD (q) − P (q) | , (13) to mean the penalty for assigning p the tangent plane from D and q the tangent plane from P. [sent-160, score-0.723]

54 Candidate Planes We first show that fusion moves where the candidate function P is a plane result in submodular terms. [sent-165, score-0.439]

55 1 If the proposal P is a plane then the fusion wPirothp any function Df t hise a rsoupbomsaold Pula isr move. [sent-168, score-0.293]

56 General Candidates Next we derive some more general sufficient conditions for submodularity of the fusion move. [sent-173, score-0.183]

57 2ca Ivef) b botehtw Deen a p a Pnd a q eth ceonn vtehxe (inorte raaltcetironnasVpq and Vqp are submodular for the fusion move. [sent-176, score-0.263]

58 To see this we first note that if both D and P are convex othe sne they are e b foitrhs tb nooutned ethda ftr iofm b obtehlo Dw by dth Peir a tangent planes. [sent-177, score-0.243]

59 (26) In the case of a plane proposal P we see that min(Vpq(D, D), t) ≤ (27) min ? [sent-191, score-0.203]

60 Epq(D, D) +Epq(P, P) ≤ Epq(D, P) +Epq(P, D), (30) showing that planar proposals also generate submodular interactions with this energy. [sent-201, score-0.391]

61 General Order Smoothness Priors In Section 2 we used tangent planes to create our smoothness prior. [sent-210, score-0.441]

62 For example, if we to each pixel assign a quadratic function instead of a tangent we have an interaction that penalizes 3rd derivatives. [sent-215, score-0.365]

63 1it is easy to see that if our proposals fulfill ApP (q) = P (q) , (32) then the fusion move will be submodular. [sent-218, score-0.301]

64 For example if we only use the zero order expansion (constant functions/ fronto-parallel planes) then we find that fusion moves with constant depth proposals are submodular. [sent-220, score-0.482]

65 eWriem weniltls use n beoitghh tbhoer disparity v cehrosisoenn (Section 2. [sent-234, score-0.243]

66 Depth Depth, 1st derivative Depth, 1st, 2nd derivative . [sent-242, score-0.178]

67 Constant functions Constant 1st derivative Constant 2nd derivative . [sent-245, score-0.178]

68 Characterization of Pairwise interactions, unary terms and submodular proposals for different types of labels. [sent-248, score-0.336]

69 (a) - Image, (b) - depth map using only the data term, (c) - depth map computed with regularization. [sent-251, score-0.258]

70 (a) × - Image, (b) - depth map using only the data term, (c) - depth map computed with The data term Ep is a unary term that depends on the tangent plane at p. [sent-255, score-0.718]

71 For each depth we use a planar homography hto\ project one Fofo trh eea neighboring images ainnator thhoem coegnrtearimage. [sent-257, score-0.218]

72 In principle we could make the NCC depend on the tilt of the tangent as well, however storing the samples of such a function would require lots of memory. [sent-261, score-0.281]

73 We also add an extra cost to assignments of planes which are roughly parallel to the viewing rays. [sent-265, score-0.224]

74 We us the extra cost (1 − npTvp)2k, (34) where np is the normal of the plane assigned to p and vp 111777333422 is the direction of the viewing ray in p (in the 3D space the viewing ray direction will be p/ ? [sent-267, score-0.399]

75 1 Proposal Generation To generate proposals we use similar heuristics to those of [15]. [sent-275, score-0.155]

76 • • To generate planar proposals we randomly select a point annerda a espm laanll neighborhood. [sent-276, score-0.214]

77 Using tmhel y be ssetl eloctca al maximum of the normalized cross correlation for each viewing ray we create a 3D cloud to the neighborhood and fit a plane using RANSAC. [sent-277, score-0.262]

78 • We use a filtering process that takes the current assignment, computes gth per corresponding 3 thDe points, aa sndsi gfnoreach pixel fits a plane to its neighboring 3D points. [sent-279, score-0.179]

79 Finally we have a proposal that just incFrienaaslelys/decreases the depth/disparity of all proposals with a small random step size. [sent-280, score-0.221]

80 For their data sets we computed a depth map for the middle image (nr 4) and used the remaining 6 images to compute the cross correlations needed for the data term. [sent-284, score-0.158]

81 The effects of the regularization term can be seen by comparing the surface generated from the data term without regularization (b) and the one with regularization (c) (the data term is particularly weak in the bowling data set because of the large texture less region). [sent-287, score-0.394]

82 GlobalStereo also penalize second derivative but use triple cliques with scalar disparity labels. [sent-292, score-0.512]

83 The comparison is performed on the Middlebury data set consisting of stereo pairs of rectified images. [sent-294, score-0.172]

84 In the fusion moves we use ”improve” [11] after running RD to label all unlabelled variables. [sent-319, score-0.236]

85 First we consider the Segpln-proposals which are 14 piecewise planar proposals generated from a segmentation (see [15]). [sent-321, score-0.253]

86 In Figure 4 we started from the same randomized disparity function with tangents parallel to the image plane. [sent-322, score-0.389]

87 We kept track of how many variables where unlabeled after RD for both methods and presented the numbers in Table 2 and the resulting disparity maps in Figure 4. [sent-324, score-0.269]

88 Note that the fusion move for our method is only submodular if we fuse one planar function at a time. [sent-325, score-0.347]

89 The SegPln proposals are piecewise planar and the regularization at transitions between planes may not be submodular. [sent-326, score-0.406]

90 We also test our regularization on the full pipeline of GlobalStereo which uses all three types of proposals (Segpln, SameUni and Smooth). [sent-327, score-0.212]

91 (b-d) are estimated disparity maps after fusing the 14 SegPln proposals. [sent-331, score-0.271]

92 In (f-h) we present the unlabelled variables summed over all 14 proposals scaled 0–14. [sent-332, score-0.226]

93 TsukubaVenusTeddyConesAverage Non occ All Disc Non occ All Disc Non occ All Disc Non occ All Disc Our4. [sent-334, score-0.236]

94 M Tidhed ceblaussreys [ are non goc thcleu sdaemd regions, aalsl , pixels iasn bde regions near depth d%is ocfo nptiixneulsiti beesi. [sent-364, score-0.153]

95 Conclusions In this paper we advocated a largely overlooked approach to stereo with 2nd order smoothness regularization. [sent-384, score-0.253]

96 In contrast to popular approaches where triple cliques are used for representing 2nd order surface derivatives, we proposed to use pairwise interactions with 3Dlabels. [sent-385, score-0.288]

97 We showed that this leads to simpler optimization problems and in many cases (nearly) submodular fusion moves. [sent-386, score-0.286]

98 (a) - Image, (b) - depth map using only the data term, (c) (c) - depth map computed with regularization. [sent-406, score-0.258]

99 (a) - Image, (b) - depth map using only the data term, (c) - depth map computed with regularization. [sent-408, score-0.258]

100 Global stereo reconstruction under second order smoothness priors. [sent-499, score-0.223]


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tfidf for this paper:

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