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A boundary-partition-based Voronoi diagram of d-dimensional balls: definition, properties, and applications
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  • Published: 06 May 2020

A boundary-partition-based Voronoi diagram of d-dimensional balls: definition, properties, and applications

  • Xianglong Duan1,
  • Chaoyu Quan2 &
  • Benjamin Stamm  ORCID: orcid.org/0000-0003-3375-483X3 

Advances in Computational Mathematics volume 46, Article number: 44 (2020) Cite this article

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Abstract

In computational geometry, different ways of space partitioning have been developed, including the Voronoi diagram of points and the power diagram of balls. In this article, a generalized Voronoi partition of overlapping d-dimensional balls, called the boundary-partition-based diagram, is proposed. The definition, properties, and applications of this diagram are presented. Compared to the power diagram, this boundary-partition-based diagram is straightforward in the computation of the volume of overlapping balls, which avoids the possibly complicated construction of power cells. Furthermore, it can be applied to characterize singularities on molecular surfaces and to compute the medial axis that can potentially be used to classify molecular structures.

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Funding

Open Access funding provided by Projekt DEAL. This work is partially supported by the National Natural Science Foundation of China (Grant No. 11901281).

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Author notes

    Authors and Affiliations

    1. Laboratoire de Mathématiques d’Orsay, Univ Paris-Sud 11, CNRS, Université Paris-Saclay, F-91405, Orsay, France

      Xianglong Duan

    2. SUSTech International Center for Mathematics, Southern University of Science and Technology, Shenzhen, China

      Chaoyu Quan

    3. Center for Computational Engineering Science, RWTH Aachen University, Aachen, Germany

      Benjamin Stamm

    Authors
    1. Xianglong Duan
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    2. Chaoyu Quan
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    3. Benjamin Stamm
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    Corresponding author

    Correspondence to Benjamin Stamm.

    Additional information

    Communicated by: Tomas Sauer

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    X. Duan and C. Quan are joint first authors who contributed equally to this article.

    Appendices

    Appendix 1. Proof of Claim 2.2

    First, we consider a sphere \(S_{i_{t}} \ni \mathbf {x}\) for a fixed 1 ≤ t ≤ m. According to the definition (24) and Eq. 26, we can compute

    $$ \begin{array}{llll} &\displaystyle|\zeta_{s}(x)-\mathbf{c}_{i_{t}}|^{2} - |\mathbf{x}-\mathbf{c}_{i_{t}}|^{2} \\ & \displaystyle{ = |x\mathbf{n}_{s}+\alpha(x)\mathbf{v}|^{2}-2\left( \mathbf{v}_{t}, x\mathbf{n}_{s}+\alpha(x)\mathbf{v}\right)}\\ & \displaystyle{ = \left( \alpha^{2}(x)|\mathbf{v}|^{2} + x^{2}\right)+ 2x\alpha(x)\left( \mathbf{n}_{s},\mathbf{v}\right)-2\alpha(x)(\mathbf{v},\mathbf{v}_{t})-2x(\mathbf{v}_{t},\mathbf{n}_{s})}\\ & \displaystyle{ =2\alpha(x)(\mathbf{v},\mathbf{v}-\mathbf{v}_{t})-2x(\mathbf{v}_{t},\mathbf{n}_{s})}\\ & \displaystyle{ = 2x\left[-(\mathbf{v}_{t},\mathbf{n}_{s}) + \frac{x}{|\mathbf{v}|^{2}(2-\alpha(x))}(\mathbf{v},\mathbf{v}-\mathbf{v}_{t})\right]}, \end{array} $$
    (56)

    where in the third and forth equality, we use the fact that α2(x)|v|2 + x2 = 2α(x)|v|2 and \(\left (\mathbf {n}_{s},\mathbf {v}\right ) =0\) as \(\mathbf {v}_{r}\in \mathcal A_{s}\).

    Since (x + λvt, ns) ≤ bs, ∀λ ≥ 0, we know that (vt, ns) ≤ 0. In the case of (vt, ns) < 0, according to Eq. 56, there exists a small enough number \(\varepsilon _{i_{t}}>0\) such that \(\forall x\in [0,\varepsilon _{i_{t}}]\),

    $$|\zeta_{s}(x)-\mathbf{c}_{i_{t}}|\geq |\mathbf{x}-\mathbf{c}_{i_{t}}|=r_{i_{t}}.$$

    Besides, in the case of (vt, ns) = 0 implying \(\mathbf {v}_{t} \in \mathcal {A}_{s}\), according to Eq. 28 and (56), we have ∀0 ≤ x ≤|v|,

    $$|\zeta_{s}(x)-\mathbf{c}_{i_{t}}|\geq |\mathbf{x}-\mathbf{c}_{i_{t}}|=r_{i_{t}}.$$

    In particular, when t = t0, we have both (vt, ns) = 0 and (v,v −vt) = 0. As a consequence,

    $$|\zeta_{s}(x)-\mathbf{c}_{i_{t}}|= |\mathbf{x}-\mathbf{c}_{i_{t}}|=r_{i_{t}},$$

    which means that \(\zeta _{s}(x) \in S_{i_{t_{0}}}\). So far, we have proved that \(\forall x\in [0,\varepsilon _{i_{t}}]\), ζs(x) does not lie in the interior of \(S_{i_{t}}\) and lies on the sphere \(S_{i_{t_{0}}}\).

    Second, we consider a sphere \(S_{j}\not \in \{S_{i_{1}}, S_{i_{2}},\ldots ,S_{i_{m}}\}\) that does not contain x. In this case, we have |x −cj|− rj > 0. Therefore, there exists a small number εj > 0 such that ∀x ∈ [0,εj],

    $$|\zeta_{s}(x)-\mathbf{x}|\leq\frac{1}{2}(|\mathbf{x}-\mathbf{c}_{j}|-r_{j}).$$

    This yields that ∀x ∈ [0,εj],

    $$|\zeta_{s}(x)-\mathbf{c}_{j}|\geq|\mathbf{x}-\mathbf{c}_{j}|-|\zeta_{s}(x)-\mathbf{x}|\geq\frac{1}{2}(|\mathbf{x}-\mathbf{c}_{j}|+r_{j})>r_{j}, $$

    that is to say, ζs(x) lies outside the sphere Sj.

    In summary, there exists a possibly small number ε > 0 such that ∀x ∈ [0,ε], ζs(x) does not cross any sphere Si and lies on the sphere \(S_{i_{t_{0}}}\), which implies that ζs(x) ∈Γ.

    Appendix 2. Proof of Claim 3.1

    Recall the definition of the face

    $$ F_{ij} := \text{conv}\left( {\gamma}_{i}^{(0)},\mathbf{c}_{\mathcal{I}(\gamma_{ij}^{(1)})}\right),\qquad 1\leq i\leq n_{0},~1\leq j\leq K_{i}. $$
    (57)

    Given a nondegenerate intersection point \(\gamma _{i}^{(0)}\) and the associated 1-patch \(\gamma _{ij}^{(1)}\), the (d − 1)-face Fij is actually a subset of \(\widetilde R_{0}\), since, according to Lemma 3, Fij is a subset of \(\mathcal {R}({\gamma }_{i}^{(0)})\). Further, taking any point \(\mathbf {y}\in \gamma _{ij}^{(1)}\), we have the following result:

    $$ \mathcal{R}(\mathbf{y}) = \text{conv}\left( \mathbf{y}, \mathbf{c}_{\mathcal{I}(\gamma_{ij}^{(1)})}\right) \subseteq \mathcal{R}\left( \gamma_{ij}^{(1)}\right). $$
    (58)

    As y tends to \(\gamma _{i}^{(0)}\), \(\mathcal {R}(\mathbf {y})\) tends to Fij. Any interior point of \(\mathcal {R}(\mathbf {y})\) has y as a unique closest point, which implies that the interior of \(\mathcal {R}(\mathbf {y})\) lies completely outside \(\widetilde {R}_{0}\). For any point x ∈ Fij, we can then find a sequence of points {xn} outside \(\widetilde {R}_{0}\) converging to x. Therefore, we have \(F_{ij} \subseteq \partial \widetilde {R}_{0}\).

    It is sufficient to prove that any point \(\mathbf {x}\in \partial \widetilde {R}_{0}\) belongs to either some face Fij or some set F0 with \(\dim (F_{0})\leq d-2\). \(\partial \widetilde {R}_{0}\) can be divided into two sets

    $$ U_{1} := \{\mathbf{x} \in \partial \widetilde{R}_{0}\mid \text{ all closest points of } \mathbf{x} \text{ belong to } \widetilde{P}_{0}\}, $$
    (59)

    and

    $$ U_{2} := \{\mathbf{x} \in \partial \widetilde{R}_{0}\mid \text{ there exists a closest point of } \mathbf{x} \text{ not contained in } \widetilde{P}_{0}\}. $$
    (60)

    In the following content, we prove that if x ∈ U1, then x belongs to a certain face Fij, while if x ∈ U2, then x belongs to F0 which will be defined later.

    Step 1: :

    In the case of x ∈ U1, we can find a sequence of points {xn} in Ω∖R0 such that xn tends to x. Correspondingly, there exists a sequence of points {an} on Γ, where an is one closest point of xn. Since x has finitely many closest points in \(\widetilde {P}_{0}\) and the total number of k-patches is finite, we can extract a subsequence of an such that this subsequence lies on some k-patch γ(k) with k ≥ 1 and converges to some nondegenerate intersection point \(\gamma _{i}^{(0)}\). Without loss of generality, we can therefore suppose that an tends to \(\gamma _{i}^{(0)}\) and an ∈ γ(k), ∀n. As a consequence, \(\gamma _{i}^{(0)}\) is on the boundary of γ(k) and further, there exists a 1-patch \(\gamma _{ij}^{(1)}\) on \(\overline \gamma ^{(k)}\), satisfying

    $$ \mathbf{c}_{\mathcal{I}(\gamma^{(k)})} \subseteq \mathbf{c}_{\mathcal{I}(\gamma_{ij}^{(1)})}. $$
    (61)

    Due to the fact that

    $$ \mathbf{x}_{n} \in \text{conv}\left( \mathbf{a}_{n},\mathbf{c}_{\mathcal{I}(\gamma^{(k)})}\right), $$
    (62)

    we then have

    $$ \mathbf{x} \in \text{conv}\left( \gamma_{i}^{(0)},\mathbf{c}_{\mathcal{I}(\gamma^{(k)})}\right) \subseteq \text{conv}\left( \gamma_{i}^{(0)},\mathbf{c}_{\mathcal{I}(\gamma_{ij}^{(1)})}\right) = F_{ij}, $$
    (63)

    by taking \(n\rightarrow \infty \).

    Step 2: :

    In the case of x ∈ U2, we want to prove that x belongs to some F0. According to the definition of U2, x has at least one closest point a that is not a nondegenerate intersection point. Here, we mention the fact that for any point y belonging to the open line segment \(\overline {\mathbf {a}\mathbf {x}}\) with endpoints a and x, a is the unique closest point of y on Γ, which can be easily proven by contradiction.

    On the one hand, if a is not an intersection point, then a lies on some k-patch γ(k) with k ≥ 1. According to Theorem 1, we know that

    $$ \mathcal{R}(\mathbf{a}) = \text{conv}\left( \mathbf{a}, \mathbf{c}_{\mathcal{I}({\gamma^{(k)}})}\right). $$
    (64)

    Considering that the latter convex hull, we obtain that \(\mathbf {x}\in \text {conv}(\mathbf {c}_{\mathcal {I}({\gamma ^{(k)}})})\) of dimension \(\dim (\text {conv}(\mathbf {c}_{\mathcal {I}({\gamma ^{(k)}})}))\leq d-2\), since otherwise, x will has a unique closest point on Γ. On the other hand, if a is a degenerate intersection point, then we have \(\mathbf {a} \in {\varLambda }_{\mathcal {I}(\mathbf {a})}\) with \(\dim \left ({\varLambda }_{\mathcal {I}(\mathbf {a})}\right ) \leq d-1\). Since \(\mathcal {R}(\mathbf {a})\subseteq {\varLambda }_{\mathcal {I}(\mathbf {a})}\) according to Theorem 1, it holds that \(\dim \left (\mathcal {R}(\mathbf {a})\right ) \leq d-1\). Here, we actually have \(\mathbf {a}\in \mathcal {R}(\mathbf {a})\) and \(\mathcal {R}(\mathbf {a})\) is a convex set from Lemma 3. Due to the fact mentioned above, we obtain that \(\mathbf {x} \in \mathcal {R}(\mathbf {a})\) only lies on \(\partial \mathcal {R}(\mathbf {a})\) of dimension \(\dim \left (\partial \mathcal {R}(\mathbf {a})\right ) \leq d-2\).

    As the number of k-patches and degenerate intersection points are finite, we can conclude that

    $$ \mathbf{x}\in \bigcup_{k\geq 1} \text{conv}(\mathbf{c}_{\mathcal{I}({\gamma^{(k)}})}) \bigcup_{\gamma_{i}^{(0)}\not\in \widetilde{P}_{0}} \partial\mathcal{R}(\gamma_{i}^{(0)}), \qquad \forall \mathbf{x}\in U_{2}, $$
    (65)

    where \(\gamma _{i}^{(0)}\) in the second union is taken as all degenerate intersection points. Note that the union on the right-hand side of Eq. 65 is of dimension less than or equal to d − 2. This implies that \(\dim (U_{2}) \leq d-2\). Therefore, we can define F0 = U2, which satisfies \(\dim (F_{0}) \leq d-2\).

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    Duan, X., Quan, C. & Stamm, B. A boundary-partition-based Voronoi diagram of d-dimensional balls: definition, properties, and applications. Adv Comput Math 46, 44 (2020). https://doi.org/10.1007/s10444-020-09765-3

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    • Received: 20 December 2018

    • Accepted: 24 January 2020

    • Published: 06 May 2020

    • DOI: https://doi.org/10.1007/s10444-020-09765-3

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    Keywords

    • Voronoi diagram
    • Power diagram
    • Partition of d-dimensional balls

    Mathematics Subject Classification (2010)

    • 52C07
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