2001
DOI: 10.1201/9781420035704
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The Curve Shortening Problem

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Cited by 200 publications
(203 citation statements)
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“…It is expected intuitively that, depending on the convex initial curve, the flow (1) will either converge to a point, converge to a round circle S 1 , or expand to infinity, with each γ t remaining smooth and convex. This is indeed true due to Theorem 3.12 (see also Remark 3.14) of [Chou and Zhu 2001]. Moreover, for given initial data X 0 (ϕ) : S 1 → ‫ޒ‬ 2 , if we consider its homothetic class there exists a unique number > 0 (for convenience we call it the critical number of X 0 ) such that under the flow (1) with initial data λX 0 (ϕ), λ = , γ t will converge to the unit circle S 1 (without rescaling) smoothly as t → ∞.…”
Section: Introductionmentioning
confidence: 53%
See 1 more Smart Citation
“…It is expected intuitively that, depending on the convex initial curve, the flow (1) will either converge to a point, converge to a round circle S 1 , or expand to infinity, with each γ t remaining smooth and convex. This is indeed true due to Theorem 3.12 (see also Remark 3.14) of [Chou and Zhu 2001]. Moreover, for given initial data X 0 (ϕ) : S 1 → ‫ޒ‬ 2 , if we consider its homothetic class there exists a unique number > 0 (for convenience we call it the critical number of X 0 ) such that under the flow (1) with initial data λX 0 (ϕ), λ = , γ t will converge to the unit circle S 1 (without rescaling) smoothly as t → ∞.…”
Section: Introductionmentioning
confidence: 53%
“…According to [Chou and Zhu 2001], the critical number is obtained via a contradiction argument and for a given curve X 0 (ϕ) we do not know what it is. However, we can use the following theorem to give an estimate of (see Corollary 2.7).…”
Section: Estimate Of the Critical Numbermentioning
confidence: 99%
“…First we need to establish the following lemma. If M were orientable, this lemma would follow from basic results on curve shortening flow by curvature [17,8]; however, when M is not orientable, the geodesic curvature is not well-defined along the entire curve; hence we use the "disk flow" method devised in [19] which does not require orientability.…”
Section: 3mentioning
confidence: 99%
“…Contracting (t < 0) and expanding (t > 0) self-similar solutions (AbreshLanger [1], Brakke [10] and [14]) correspond to the vector field tuy. All these solutions are discussed in Chou-Zhu [13]. Finally, the contracting\expanding spirals corresponding to ws are discussed in [8] and Li [20].…”
Section: V(t) = [R-(a + L)t]^t Rx)mentioning
confidence: 99%