Abstract
It is well known that the Willmore flow of closed spherical immersions exists globally in time and converges if the initial datum has Willmore energy below
A Immersions into
H
2
with Sobolev regularity
The above definitions of the curvature, tangent vector and elastic energy also make sense for immersions
A curve
exists and, as in [8, (12)], one computes that
Moreover, as already computed in [12, (2.9)],
Consider immersions
Proof
The claim is due to (A.3) and the compact embedding
For immersions
Proof
After passing to a subsequence, without loss of generality,
It is a well-known fact that the product of a uniformly convergent sequence and a sequence that weakly converges in
B Energy estimates
We use the following two technical results from [31].
Consider immersions
Proof
Proposition 2.7 in [31] yields the claim for smooth immersions
Theorem B.2 ([31, Theorem 2.5])
Consider smooth immersions
then
C Monotonicity formula and estimates for
C
LY
(
p
,
τ
)
As it turns out, the underlying monotonicity formula in [25, Appendix B] from which Proposition 2.3 is concluded gives very useful exact identities for surfaces contained in spheres.
Since the integral in (2.5) only depends on the Dirichlet boundary conditions and as the Dirichlet boundary conditions of cylindrical surfaces of revolution are parallel circles with prescribed co-normal field,
First, recall Simon’s monotonicity formula in [25, Appendix B] for varifolds with boundary, cf. [32, (1.2)] and [18, Appendix A] for the versions without boundary.
Consider a 2-dimensional integral varifold 𝑉 in
writing
for all
For
One has that
To this end, we make the following construction. First, consider the parallel circles
Consider now an integer rectifiable 2-varifold
one has
Moreover, estimating
Using (C.1), one concludes
We now make a specific choice for
One has
Proof
First, consider any
Case 1:
we can parametrize 𝑀 by the surface of revolution associated to
Case 2:
Using that the Willmore energy is invariant with respect to scaling and translations, that
It holds that
Proof
To this end, simply note that (C.2) applied to
using that the support of
D Computation of
C
LY
rot
(
p
,
τ
)
and comparison to [11]
Returning to (1.6), for
and plugging this into (1.6) yields formula (1.7).
In particular, if one considers the case of horizontal boundary data, i.e.
also cf. [11, Theorem 1.2]. Next, adapting our methodology from the previous section, using Simon’s monotonicity formula, we show that the energy thresholds in (1.9) and [11, Theorem 1.1] are equivalent for all possible boundary conditions.
To this end, we rewrite the main players in defining the threshold in [11, Theorem 1.1] with this article’s notation.
If
We then have the following.
Writing
for
Especially, summing over
That is, recalling (1.6), the energy thresholds of Theorem 1.4 and [11, Theorem 1.1] coincide.
Proof of Proposition D.1
Suppose first of all that
In particular,
By (D.2), we have
Finally, if
and (D.3) also follows in this case. ∎
Acknowledgements
The author would like to thank Anna Dall’Acqua for helpful discussions and Sascha Eichmann for his comments on comparing Theorem 1.4 and [11, Theorem 1.1]. Moreover, the author is grateful to the referees for their valuable comments on the original manuscript.
-
Communicated by: Francesca Da Lio
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© 2025 Walter de Gruyter GmbH, Berlin/Boston
Articles in the same Issue
- Frontmatter
- Boundary behavior of solutions to fractional p-Laplacian equation
- Existence of distributional solutions to some quasilinear degenerate elliptic systems with low integrability of the datum
- A weakly coupled system of p-Laplace type in a heat conduction problem
- On the interior regularity criteria for the viscoelastic fluid system with damping
- On the L 1-relaxed area of graphs of BV piecewise constant maps taking three values
- On prescribing the number of singular points in a Cosserat-elastic solid
- Stability from rigidity via umbilicity
- Free boundary regularity in the fully nonlinear parabolic thin obstacle problem
- Calderón–Zygmund theory for strongly coupled linear system of nonlocal equations with Hölder-regular coefficient
- Inertial (self-)collisions of viscoelastic solids with Lipschitz boundaries
- A discrete crystal model in three dimensions: The line-tension limit for dislocations
- Two-dimensional graph model for epitaxial crystal growth with adatoms
- Global existence for the Willmore flow with boundary via Simon’s Li–Yau inequality
- Linearization in magnetoelasticity
- The fractional Hopf differential and a weak formulation of stationarity for the half Dirichlet energy
Articles in the same Issue
- Frontmatter
- Boundary behavior of solutions to fractional p-Laplacian equation
- Existence of distributional solutions to some quasilinear degenerate elliptic systems with low integrability of the datum
- A weakly coupled system of p-Laplace type in a heat conduction problem
- On the interior regularity criteria for the viscoelastic fluid system with damping
- On the L 1-relaxed area of graphs of BV piecewise constant maps taking three values
- On prescribing the number of singular points in a Cosserat-elastic solid
- Stability from rigidity via umbilicity
- Free boundary regularity in the fully nonlinear parabolic thin obstacle problem
- Calderón–Zygmund theory for strongly coupled linear system of nonlocal equations with Hölder-regular coefficient
- Inertial (self-)collisions of viscoelastic solids with Lipschitz boundaries
- A discrete crystal model in three dimensions: The line-tension limit for dislocations
- Two-dimensional graph model for epitaxial crystal growth with adatoms
- Global existence for the Willmore flow with boundary via Simon’s Li–Yau inequality
- Linearization in magnetoelasticity
- The fractional Hopf differential and a weak formulation of stationarity for the half Dirichlet energy