REVIEW 2 major objections 4 minor 19 references
Construction of High Codimension Ancient Mean Curvature Flows
T0 review · 2 major / 4 minor · reviewed 2026-08-14 · deepseek-v4-flash
Pith's one-line read For every positive integer m, a compact ancient curve shortening flow in R^{2m} exists whose image spans the full space.
desk verdict Sound explicit construction with a fixable factor error in the entropy proof, but the central example is not new; the paper's value lies in the entropy computation, product construction, and honest discussion of overlap. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is the torus curve, a curve on a product of $m$ circles $S^1(r^{k_1^2})\times\cdots\times S^1(r^{k_m^2})$ with coordinate functions $r^{k_j^2}\cos(k_j\theta)$ and $r^{k_j^2}\sin(k_j\theta)$. Its defining property is that the speed $|\partial_\theta\gamma|$ is independent of $\theta$, so the vector Laplacian acts as a pure second derivative in $\theta$; substituting into $\partial_t\gamma=\Delta_\gamma\gamma$ collapses the entire high-codimension flow to a single first-order ODE for $r(t)$. The ancient solution of that ODE, obtained by inverting $F(r)=\frac12\sum_j r^{2k_j^2}=-t$, is what makes the construction work.
What would settle it
For $m=2$, $k_1=1$, $k_2=2$, let $r(t)$ solve $\frac12(r^2+r^8)=-t$ and define $\gamma_t$ by formula (2.1); evaluate both sides of $\partial_t\gamma_t=\Delta_{\gamma_t}\gamma_t$ at $\theta=\pi/4$ and $t=-1$. If the two sides differ, the ancient-flow claim for this example is false; if they agree, the reduction is consistent.
Extended reading notes
Core claim
The central object is the torus curve $\gamma_t(\theta) = (r^{k_1^2}\cos(k_1\theta), r^{k_1^2}\sin(k_1\theta), \ldots, r^{k_m^2}\cos(k_m\theta), r^{k_m^2}\sin(k_m\theta))$, which winds $k_j$ times around the $j$-th circle $S^1(r^{k_j^2})$. Because $|\partial_\theta\gamma_t|^2 = \sum_{j=1}^m k_j^2 r^{2k_j^2}$ is independent of $\theta$, the curve Laplacian is $|\partial_\theta\gamma_t|^{-2}\partial_\theta^2$, so the mean curvature flow equation $\partial_t\gamma = \Delta_\gamma\gamma$ reduces to the scalar ODE $r' = -r\,/\,\sum_{j=1}^m k_j^2 r^{2k_j^2}$. The paper proves this ODE has a unique positive solution on $(-\infty,0)$ with $r\to\infty$ as $t\to-\infty$ and $r\to0$ as $t\to0$, yielding an ancient flow. The coordinate functions are linearly independent, so $\gamma_t$ spans $\mathbb{R}^{2m}$; rescaling shows the tangent flow at $-\infty$ is the multiplicity-$k_m$ circle and at $0$ the multiplicity-$k_1$ circle. Consequently $\sup_t\lambda(\gamma_t) = k_m\lambda(S^1)$. Adding one linear coordinate to the same Ansatz gives eternal helix-type solutions in odd-dimensional spaces with infinite entropy, and products of torus curves give $n$-dimensional ancient mean curvature flows of high codimension.
Load-bearing premise
The reduction to a single ODE rests on the curve being parametrized with speed independent of $\theta$, so that the curve Laplacian is a pure second derivative in $\theta$; if that failed, the coordinate functions would not close under the flow, and the whole construction would collapse.
Editorial extensions
If this is right
- Ancient curve shortening flows in Euclidean space need not be planar: for each $m$ there is one in $\mathbb{R}^{2m}$ spanning the full space.
- Products of these curves produce compact $n$-dimensional ancient mean curvature flows that also span the full space, and further products with Euclidean factors give finite-entropy ancient solutions in every dimension and codimension except curves lying in odd-dimensional Euclidean spaces.
- The entropy of the $m$-frequency torus curve is exactly $k_m\lambda(S^1)$, matching the linear-in-dimension entropy growth that the conjectured sharp constant predicts.
- Setting $k_1=1$ makes the tangent flow at time $0$ a single round circle even though the curve has arbitrarily high codimension; the tangent flow at $0$ alone cannot bound codimension.
- The example yields the lower bound $\lambda(S^1)C_1\ge 2$ for the constant in the known entropy-codimension bound and motivates the conjecture that the sharp value is $C_1=2/\lambda(S^1)$.
Reading between the lines
- If the conjectured sharp constant is correct, any ancient curve shortening flow whose image truly spans $\mathbb{R}^N$ must have entropy at least $(N/2)\lambda(S^1)$; testing this inequality on multi-frequency or perturbed torus curves would give evidence without classifying all ancient flows.
- The identity $F(r)+t=0$ makes the construction essentially algebraic, so these solutions may serve as explicit blow-up models; one could perturb the Ansatz by small non-sinusoidal Fourier modes and check whether the ODE reduction survives to first order.
- The same constant-speed idea may generalize to higher-dimensional submanifolds formed from orthogonal products of such curves, with entropy becoming a product of winding numbers; whether the resulting flows remain ancient is a testable extension.
- Varying the frequencies $k_j$ gives a family of ancient flows with the same ambient dimension but different entropies, which may help calibrate any future sharp bound.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper constructs a family of closed curves in R^{2m} with coordinate functions r(t)^{k_j^2} times trigonometric monomials of frequency k_j, and proves that for an explicitly defined function r(t) these curves solve the curve shortening flow on (-∞,0). The main existence result is Theorem 1.1; the paper also identifies the tangent flows at 0 and -∞, computes the entropy as k_m λ(S^1), constructs analogous noncompact helix solutions in R^{2m+1}, and takes products to obtain higher-dimensional ancient mean curvature flows. The appendix gives an ODE existence proof. The authors state in Remark 1.3 that the main construction was already discovered by Altschuler–Altschuler–Angenent–Wu in [AAAW13].
Significance. The construction itself is clean, self-contained, and machine-checkable in the sense that the Laplacian reduction is valid because |∂_θ γ_t| is θ-independent, and the ODE solution is proved from scratch in the appendix. If the entropy computation is corrected, the paper provides explicit non-planar ancient curve shortening flows with computable entropy and explicit tangent flows, which is a useful addition to the small set of known high-codimension ancient flows and directly motivates the sharp-constant conjecture for a Colding–Minicozzi codimension bound. However, because the central existence result is already present in [AAAW13], the incremental value of the paper rests on the entropy computation, the helix variant, the product construction, and the conjectures; the authors are honest about this priority issue, but it should be reflected in the framing.
major comments (2)
- [Corollary 2.3] The displayed Gaussian integral in the proof of the lower bound has a measure-factor error. For sγ_t, with A = Σ_j r^{2k_j^2} and B = Σ_j k_j^2 r^{2k_j^2}, the correct computation is (4π)^{-1/2} ∫_{sγ_t} e^{-|x|^2/4} dH^1 = s√π √B exp(-s^2 A/4), because the dilation multiplies the arclength element by s and |∂_θ γ_t| = √B. The manuscript writes a factor √B in the denominator instead of the numerator. As printed, the choice s̃ = √2 A^{-1/2} gives an expression that tends to 0 as t → -∞, so the claimed lower bound does not follow. Replacing the denominator by √B makes the displayed limit correct and gives k_m λ(S^1). Since this corollary is the basis for the entropy applications and Conjecture 2.4, the proof must be corrected.
- [Section 2.3, proof of Theorem 1.2] The proof of Theorem 1.2 is one sentence: 'Take the product of n appropriately chosen torus curves.' This is not sufficient as written, because a product of n torus curves in R^{2m} would lie in R^{2mn}; to obtain a submanifold of R^{2m}, the torus-curve factors must be chosen with ambient dimensions that sum to 2m, and the nondegeneracy of the resulting product must be checked. The statement is plausible and the fix is straightforward, but the proof should be completed explicitly.
minor comments (4)
- [Section 2.1, between (2.2) and (2.3)] The Laplacian formula Δ_{γ_t} = |∂_θ γ_t|^{-2} ∂_θ^2 is used because |∂_θ γ_t| is θ-independent; this fact is correct for the given coordinate functions, but it should be stated explicitly as the justification rather than left implicit.
- [Proposition 2.2] The tangent flows are described as 'the multiplicity k_m circle' and 'the multiplicity k_1 circle' without specifying the radius; the limiting circles have radius √2, as expected for self-shrinking circles, and this should be stated for clarity.
- [Corollary 2.3, upper bound] The upper-bound argument uses monotonicity of entropy to conclude sup_t λ(γ_t) = lim_{t→-∞} λ(γ_t); this is standard for closed mean curvature flows, but a citation or one-line justification would improve rigor.
- [Remark 1.3 and abstract add-on] The add-on remark about [AAAW13] appears twice, once after the abstract and once as Remark 1.3; for a journal submission this should be integrated into the introduction in a single place.
Circularity Check
No circularity: the construction is verified from scratch by direct Laplacian computation and an explicit ODE solution; the acknowledged overlap with AAAW13 is a priority issue, not a circular dependency.
full rationale
The derivation is self-contained. Equation (2.1) defines the torus curves γ_t, and Proposition 2.1 verifies the curve shortening flow equation by computing both sides: since |∂_θγ_t|^2 = Σ k_j^2 r^{2k_j^2} is θ-independent, the curve Laplacian is |∂_θγ_t|^{-2}∂_θ^2, and ∂_tγ_t matches Δ_{γ_t}γ_t exactly when r satisfies the ODE (2.5). The ODE is solved explicitly in Theorem A.1 via the conserved quantity F(r)=½Σ r^{2k_j^2}=-t, which also yields the required asymptotics r→∞ as t→−∞ and r→0 as t→0. No parameter is fitted to the target theorem, and no conclusion is assumed as an input. The prior discovery by Altschuler–Altschuler–Angenent–Wu is disclosed in the abstract and in Remark 1.3, but it is not used as a proof ingredient, so the overlap is a novelty/priority concern, not circularity. The entropy computation in Corollary 2.3 appears to have a measure-factor typo in the displayed Gaussian integral (√B in the denominator instead of the numerator), but the stated limit k_mλ(S^1) follows from the corrected formula; this is a correctness/typo issue, not a circular reduction. Overall, the paper's central existence claim does not reduce by construction to its own inputs.
Assumptions & free parameters
assumptions (6)
- standard math The Laplacian on a curve with θ-independent speed equals |∂_θγ|^{-2}∂_θ^2.
- domain assumption Mean curvature flow equation ∂_t x = Δ x for immersed submanifolds.
- standard math Entropy is monotone nonincreasing along mean curvature flow (Huisken monotonicity).
- standard math The product formula Δ_{M1×M2} = Δ_{M1} + Δ_{M2}.
- domain assumption Colding-Minicozzi Theorem 0.6/0.9 as cited external results on dimension bounds.
- standard math The implicit equation F(r) = -t has a unique positive solution on t ∈ (-∞,0) because F is strictly monotone.
Cite this review
Pith. "Pith review of Construction of High Codimension Ancient Mean Curvature Flows." pith.science (2026). https://pith.science/paper/IZCJSHWZ
@misc{pith2026190802688,
author = {Pith},
title = {Pith review of: Construction of High Codimension Ancient Mean Curvature Flows},
year = {2026},
howpublished = {\url{https://pith.science/paper/IZCJSHWZ}},
note = {Machine review of arXiv:1908.02688}
}
read the original abstract
We construct a class of compact ancient solutions to the mean curvature flow in Euclidean space with high codimension. In particular, we construct higher codimensional ancient curve shortening flows. Moreover, we characterize the asymptotic behavior of these solutions. Add on remark: the construction in this paper has been discovered by Altschuler D.-Altschuler S.-Angenent-Wu in [AAAW13].
Reference graph
Works this paper leans on
-
[1]
Dylan J. Altschuler, Steven J. Altschuler, Sigurd B. Angenent, and Lani F. Wu. The zoo of solitons for curve shortening in R^n . Nonlinearity , 26(5):1189--1226, 2013
work page 2013
-
[2]
Unique asymptotics of ancient convex mean curvature flow solutions
Sigurd Angenent, Panagiota Daskalopoulos, and Natasa Sesum. Unique asymptotics of ancient convex mean curvature flow solutions. J. Differential Geom. , 111(3):381--455, 2019
2019
-
[3]
Uniqueness of convex ancient solutions to mean curvature flow in R^3
Simon Brendle and Kyeongsu Choi. Uniqueness of convex ancient solutions to mean curvature flow in R^3 . Invent. Math. , 217(1):35--76, 2019
2019
-
[4]
Ancient low entropy flows, mean convex neighborhoods, and uniqueness
Kyeongsu Choi, Robert Haslhofer, and Or Hershkovits. Ancient low entropy flows, mean convex neighborhoods, and uniqueness. arXiv preprint arXiv:1810.08467 , 2018
arXiv 2018
-
[5]
Ildefonso Castro and Ana M. Lerma. The C lifford torus as a self-shrinker for the L agrangian mean curvature flow. Int. Math. Res. Not. IMRN , (6):1515--1527, 2014
2014
-
[6]
Colding and William P
Tobias H. Colding and William P. Minicozzi, II. Generic mean curvature flow I : generic singularities. Ann. of Math. (2) , 175(2):755--833, 2012
2012
-
[7]
Minicozzi, II
Tobias Holck Colding and William P. Minicozzi, II. Uniqueness of blowups and ojasiewicz inequalities. Ann. of Math. (2) , 182(1):221--285, 2015
2015
-
[8]
Ancient gradient flows of elliptic functionals
Kyeongsu Choi and Christos Mantoulidis. Ancient gradient flows of elliptic functionals. arXiv preprint arXiv:1902.07697 , 2019
arXiv 1902
Show all 19 references
-
[9]
Minicozzi, II
Tobias Holck Colding and William P. Minicozzi, II. Complexity of parabolic systems. arXiv preprint arXiv:1903.03499 , 2019
1903 arXiv
-
[10]
Minicozzi, II
Tobias Holck Colding and William P. Minicozzi, II. Regularity of elliptic and parabolic systems. arXiv preprint arXiv:1905.00085 , 2019
1905 arXiv
-
[11]
Minicozzi, II, and Erik Kj r Pedersen
Tobias Holck Colding, William P. Minicozzi, II, and Erik Kj r Pedersen. Mean curvature flow. Bull. Amer. Math. Soc. (N.S.) , 52(2):297--333, 2015
2015
-
[12]
Classification of compact ancient solutions to the curve shortening flow
Panagiota Daskalopoulos, Richard Hamilton, and Natasa Sesum. Classification of compact ancient solutions to the curve shortening flow. J. Differential Geom. , 84(3):455--464, 2010
2010
-
[13]
Ancient solutions of the mean curvature flow
Robert Haslhofer and Or Hershkovits. Ancient solutions of the mean curvature flow. Comm. Anal. Geom. , 24(3):593--604, 2016
2016
-
[14]
Convex ancient solutions of the mean curvature flow
Gerhard Huisken and Carlo Sinestrari. Convex ancient solutions of the mean curvature flow. J. Differential Geom. , 101(2):267--287, 2015
2015
-
[15]
Hamiltonian stationary cones and self-similar solutions in higher dimension
Yng-Ing Lee and Mu-Tao Wang. Hamiltonian stationary cones and self-similar solutions in higher dimension. Trans. Amer. Math. Soc. , 362(3):1491--1503, 2010
2010
-
[16]
Mean curvature flow in higher codimension: introduction and survey
Knut Smoczyk. Mean curvature flow in higher codimension: introduction and survey. In Global differential geometry , volume 17 of Springer Proc. Math. , pages 231--274. Springer, Heidelberg, 2012
2012
-
[17]
Codimension bounds and rigidity of ancient mean curvature flow by the tangent flow at -
Douglas Stryker and Ao Sun. Codimension bounds and rigidity of ancient mean curvature flow by the tangent flow at - . (In preparation)
-
[18]
Long-time existence and convergence of graphic mean curvature flow in arbitrary codimension
Mu-Tao Wang. Long-time existence and convergence of graphic mean curvature flow in arbitrary codimension. Invent. Math. , 148(3):525--543, 2002
2002
-
[19]
Evolution of curves and surfaces by mean curvature
Brian White. Evolution of curves and surfaces by mean curvature. In Proceedings of the I nternational C ongress of M athematicians, V ol. I ( B eijing, 2002) , pages 525--538. Higher Ed. Press, Beijing, 2002
2002
Reviewed August 14, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.