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Globally Optimal Affine and Metric Upgrades in Stratified Autocalibration

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Globally Optimal Affine and Metric Upgrades in Stratified Autocalibration Globally Optimal Affine and Metric Upgrades in Stratified Autocalibration Manmohan Chandrakery Sameer Agarwalz David Kriegmany Serge Belongiey [email protected] [email protected] [email protected] [email protected] y University of California, San Diego z University of Washington, Seattle Abstract parameters of the cameras, which is commonly approached by estimating the dual image of the absolute conic (DIAC). We present a practical, stratified autocalibration algo- A variety of linear methods exist towards this end, how- rithm with theoretical guarantees of global optimality. Given ever, they are known to perform poorly in the presence of a projective reconstruction, the first stage of the algorithm noise [10]. Perhaps more significantly, most methods a pos- upgrades it to affine by estimating the position of the plane teriori impose the positive semidefiniteness of the DIAC, at infinity. The plane at infinity is computed by globally which might lead to a spurious calibration. Thus, it is im- minimizing a least squares formulation of the modulus con- portant to impose the positive semidefiniteness of the DIAC straints. In the second stage, the algorithm upgrades this within the optimization, not as a post-processing step. affine reconstruction to a metric one by globally minimizing This paper proposes global minimization algorithms for the infinite homography relation to compute the dual image both stages of stratified autocalibration that furnish theoreti- of the absolute conic (DIAC). The positive semidefiniteness cal certificates of optimality. That is, they return a solution at of the DIAC is explicitly enforced as part of the optimization most away from the global minimum, for arbitrarily small . process, rather than as a post-processing step. Our solution approach relies on constructing efficiently min- For each stage, we construct and minimize tight convex imizable, tight convex relaxations to non-convex programs, relaxations of the highly non-convex objective functions in using them in a branch and bound framework [13, 27]. a branch and bound optimization framework. We exploit A crucial concern in branch and bound algorithms is the the problem structure to restrict the search space for the exponential dependence of the worst case time complexity DIAC and the plane at infinity to a small, fixed number of on the number of branching dimensions. In this paper, we branching dimensions, independent of the number of views. exploit the inherent problem structure to restrict our branch- Experimental evidence of the accuracy, speed and scala- ing dimensions to a small, fixed, view-independent number, bility of our algorithm is presented on synthetic and real data. which allows our algorithms to scale gracefully with an in- MATLAB code for the implementation is made available to crease in the number of views. the community. A significant drawback of local methods is that they criti- cally depend on the quality of a heuristic intialization. We use chirality constraints derived from the scene to compute 1 Introduction a theoretically correct initial search space for the plane at This paper proposes practical algorithms that provably solve infinity, within which we are guaranteed to find the global well-known formulations for both affine and metric upgrade minimum [8, 9]. Our initial region for the metric upgrade stages of stratified autocalibration to their global minimum. is intuitively specifiable as conditions on the intrinsic pa- The affine upgrade, which is arguably the more difficult rameters and can be wide enough to include any practical step in autocalibration, is succintly computable by estimating cases. the position of the plane at infinity in a projective reconstruc- While we provide a unified framework for a global solu- tion, for instance, by solving the modulus constraints [19]. tion to stratified autocalibration, in several ways, our con- Previous approaches to minimizing the modulus constraints structions are general enough to find application in domains for several views rely on local, descent-based methods with beyond multiple view geometry. random reinitializations. These methods are not guaranteed In summary, our main contributions are the following: to perform well for such non-convex problems. Moreover, in our experience, a highly accurate estimate of the plane at • Highly accurate recovery of the plane at infinity in a infinity is imperative to obtain a usable metric reconstruction. projective reconstruction by global minimization of the The metric upgrade step involves estimating the intrinsic modulus constraints. • Highly accurate estimation of the DIAC by globally 2.2 Modulus Constraints solving the infinite homography relation. Noting that the infinite homography is conjugate to a rotation matrix and must have eigenvalues of equal moduli, one can • A general exposition on novel convexification methods relate the roots of its characteristic polynomial for global optimization of non-convex programs. > 3 2 det(λI − (Ai − aip )) = λ − αiλ + βiλ − γi: (3) The outline of the rest of the paper is as follows. Sec- tion 2 describes background relevant to autocalibration and to derive the so called modulus constraint [19]: Section 3 outlines the related prior work. Section 4 is a brief 3 3 overview of branch and bound algorithms. Sections 5 and 6 γiαi = βi ; (4) describe our global optimization algorithms for estimating the DIAC and the plane at infinity respectively. Section 7 where αi; βi; γi are affine functions of the coordinates presents experiments on synthetic and real data and Section 8 fp1; p2; p3g of the plane at infinity. Three views suffice 3 concludes with a discussion of further extensions. to restrict the solution space to a 4 = 64 possibilities (ac- tually 21, see [23]), which can in theory be extracted using 2 Background continuation methods. Unless stated otherwise, we will denote 3D world points 2.3 Chirality bounds on plane at infinity X by homogeneous 4-vectors and 2D image points x by Chirality constraints demand that the reconstructed scene homogeneous 3-vectors. Given the images of n points in points lie in front of the camera. While a general projective m views, a projective reconstruction fP; Xg computes the transformation may result in the plane at infinity splitting the Euclidean scene fP^i; X^ jg up to a 4 × 4 homography: scene, a quasi-affine transformation is one that preserves the convex hull of the scene points X and camera centers C.A −1 transformation Hq that upgrades a projective reconstruction Pi = P^iH ; Xj = HX^ j: to quasi-affine can be computed by solving the so-called A camera matrix is denoted by K[Rjt] where K is an upper chiral inequalities. A subsequent affine centering, Ha, guar- antees that the plane at infinity in the centered quasi-affine triangular matrix that encodes the intrinsic parameters and −> frame, v = (HaHq) π1, cannot pass through the origin. (R; t) constitute exterior orientation. A more detailed discus- > sion of the material in this section can be found in [10]. So it can be parametrized as (v1; v2; v3; 1) and bounds on vi in the centered quasi-affine frame can be computed by 2.1 The Infinite Homography Relation solving six linear programs: q> q> We can always perform the projective reconstruction such min = max vi s.t. Xj v > 0; Ck v > 0; (5) that P1 = [Ij0]. Let the first world camera be P1 = K1 [Ij0]. b q q Then H has the form where Xj and Ck are points and camera centers in the quasi- affine frame, j = 1; : : : ; n and k = 1; : : : ; m. We refer the K1 0 reader to [8, 18] for a thorough treatment of the subject. H = > (1) −p K1 1 3 Previous work > where π1 = (p; 1) is the location to which the plane Approaches to autocalibration [6] can be broadly classified at infinity moves in the projective reconstruction from its as direct and stratified. Direct methods seek to compute a canonical position (0; 0; 0; 1)>. The aim of autocalibration metric reconstruction by estimating the absolute conic. This is to recover the plane at infinity and the intrinsic parameters. is encoded conveniently in the dual quadric formulation of Let Pi = [Aijai] where Ai is 3 × 3 and ai is a 3 × 1 vector. autocalibration [12, 28], whereby an eigenvalue decompo- Let bPi = Ki [Rijti]. Then, for the case of constant intrinsic sition of the estimated dual quadric yields the homography parameters (Ki = K), we have that relates the projective reconstruction to Euclidean. Linear methods [20] as well as more elaborate SQP based optimiza- ∗ > ∗ > > ! = (Ai − aip )! (Ai − aip ) (2) tion approaches [28] have been proposed to estimate the dual quadric, but perform poorly with noisy data. Methods such where !∗ = KK> denotes the dual image of the absolute as [16] which are based on the Kruppa equations (or the conic (DIAC). Equality here is up to a scale factor. Since fundamental matrix), are known to suffer from additional i > H1 = (Ai − aip ) is precisely the homography induced ambiguities [25]. between the views P1 = [Ij0] and Pi = [Aijai] by the plane This work primarily deals with a stratified approach to at infinity (p; 1)>, it is called the infinite homography. autocalibration [19]. It is well-established in literature that, in the absence of prior information about the scene, esti- and the actual subdivision itself are essentially heuristic. We mating the plane at infinity represents the most significant consider the rectangle with the smallest minimum of flb as challenge in autocalibration [9]. The modulus constraints the most promising to contain the global minimum and sub- [19] propose a necessary condition for the coordinates of the divide it into k = 2 rectangles along the largest dimension. plane at infinity. Local minimization techniques are used A key consideration when designing bounding functions is in [19] to minimize a noisy overdetermined system in the the ease with which they can be estimated .
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