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2015 | OriginalPaper | Buchkapitel

6. Completeness of Reidemeister-Type Moves on Labelled Apparent Contours

verfasst von : Giovanni Bellettini, Valentina Beorchia, Maurizio Paolini, Franco Pasquarelli

Erschienen in: Shape Reconstruction from Apparent Contours

Verlag: Springer Berlin Heidelberg

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Abstract

In this chapter we illustrate the results and report the figures from the paper [3]. More specifically, we shall prove that there exists a finite set of simple, or elementary, moves (also called rules) on labelled apparent contours, such that the following property holds: the images \(\Sigma _{1}\) and \(\Sigma _{2}\) of two stable embeddings of a closed smooth (not necessarily connected) surface M in \(\mathbb{R}^{3}\) are isotopic if and only if their apparent contours can be connected using finitely many isotopies of \(\mathbb{R}^{2}\), and a finite sequence of elementary moves or of their inverses (sometimes called “reverses”).

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Fußnoten
1
See Theorem 6.0.3 and Corollary 6.6.5 for a precise statement.
 
2
Namely, the fact that there are no other moves, besides those in the list of Sect. 6.1, necessary to connect two apparent contours of isotopic surfaces.
 
3
In [6, Definition 2] a different notion of equivalence between maps is introduced. Such a definition can be more suitable when the target space is the cartesian product of a two-dimensional manifold with \(\mathbb{R}\).
 
4
A realization in space of these moves involves two folds of the surface which can be “far one from the other”.
 
5
The move L can be realized in space by considering the surface in Fig. 1.​4, by gradually reducing the “hill”. The inverse of a move B can be realized by straightening the central part of a depression in a long “wave” with two parallels arcs corresponding to the crease and the valley of the wave.
 
6
Compare also with Definition 8.​1.​1.
 
7
See Chap. 5
 
8
See Theorem 2.​1.​14.
 
9
See, e.g., [9] and the references therein, or also [15, p. 597, 600, 601]. Usually, a stratified Morse function takes real values: for technical reasons, we consider here the slightly different case of a function taking values in \(\mathbb{S}^{1}\), but the definition is essentially the same.
 
10
Hence, the critical points of \(u_{\vert Y _{j}}^{}\) are nondegenerate.
 
11
By definition, points of Y 3 are considered as critical points of u.
 
12
The converse statement also holds true, as a consequence of the Isotopy Extension Theorem (see, for instance, [11, Theorem 1.3, p. 180], see also [19, pp. 157–201]). Namely, suppose that γ, e1 and e2 are as in (6.5). Then, γ induces an isotopy from e1(M) to \(\mathbb{R}^{3}\), which extends to an \(\mathbb{R}^{3}\)-ambient isotopy with compact support.
 
13
Notice that the map \(\alpha \in \mathcal{C}^{\infty }(\mathcal{S}, \mathbb{R}^{3}) \rightarrow F_{\alpha } \in \mathcal{C}^{\infty }(\mathcal{S},\mathcal{T} )\) is continuous.
 
14
Note also that, defining \(f_{\varphi _{t}}\) as in (2.​2), we have \(f_{\varphi _{t}}(x) = \#\{m \in M: F_{\gamma }(m,t) = (x,t)\}\) for any \((x,t) \in \mathcal{T}\).
 
15
For t ∈ [0, 1], we use the notation \(\tilde{\gamma }_{t}(\cdot ) =\tilde{\gamma } (\cdot,t)\) .
 
16
See, for instance, [8, p. 176, 177], and more generally [13, 14].
 
17
See [18, Proposition 5.4] for related problems.
 
18
To be more specific, [4, Fig. 9(row 1, column 1)] corresponds to move L; [4, Fig. 9(2,1)] corresponds to move B; [4, Fig. 9(3,1)] corresponds to move S; [4, Fig. 10(1,1)] corresponds to move K; [4, Fig. 10(1,2)] corresponds to move C; [4, Fig. 10(2,1)] corresponds to move T. Theorem [4, 3.2.3] is a simpler version of [4, Theorem 3.5.5], in which the height function is not considered, and hence is more close to Corollary 6.6.2. It follows by combining the classifications given by [10, 16, 21].
 
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Metadaten
Titel
Completeness of Reidemeister-Type Moves on Labelled Apparent Contours
verfasst von
Giovanni Bellettini
Valentina Beorchia
Maurizio Paolini
Franco Pasquarelli
Copyright-Jahr
2015
Verlag
Springer Berlin Heidelberg
DOI
https://doi.org/10.1007/978-3-662-45191-5_6

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