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Global solutions for a new geometric flow with rotational invariance
Boundary Value Problems volume 2017, Article number: 17 (2017)
Abstract
In this paper we introduce a new geometric flow with rotational invariance and prove the existence of a global solution.
1 Introduction
Since the last quarter of the 20th century, using partial differential equations to formulate and solve geometric problems has become a trend and a dominating force. A new area called geometric analysis was born. When looking back at the history of geometric analysis, one could see numerous success stories of utilizing differential equations to tackle important problems in geometry, topology, and physics. Typical and important examples would include Yau’s solution to the Calabi conjecture using the complex Monge-Ampère equation (see Yau [1]), Schoen’s solution of the Yamabe conjecture (see Schoen [2]), Schoen-Yau’s proof of the positive mass conjecture (see Schoen-Yau [3]), Donaldson’s work on 4-dimensional smooth manifolds using the Yang-Mills equation (see Donaldson [4]), and recently, Perelman’s solution to the century-old Poincaré conjecture using Hamilton’s beautiful theory on the Ricci flow, which is just a nonlinear version of the classical heat equation (see [5–7]). However, despite all these success, the equations studied and utilized in geometry so far are almost exclusively of elliptic or parabolic type. With few exceptions, hyperbolic equations have not yet found their way into the study of geometric or topological problems. More recently, Kong et al. introduced the hyperbolic geometric flow which is a fresh start of an attempt to introduce hyperbolic partial differential equations into the realm of geometry (see [8] or [9]). The kind of flow is a very natural tool to understand the wave character of metrics, the wave phenomenon of curvatures, the evolution of manifolds and their structures (see [10–12]).
In this paper, we introduce a new geometric flow with rotational invariance. This flow is described formally by a system of parabolic partial differential equations, essentially a coupled system of hyperbolic-parabolic partial differential equations with rotational invariance. More precisely, let \(\mathscr{S}_{t}\) be a family of hypersurfaces in the \((n+1)\)-dimensional Euclidean space \(\mathbb{R} ^{n+1}\) with coordinates \((x_{1},\ldots, x_{n+1})\), without loss of generality, we may assume that the family of hypersurfaces \(\mathscr{S}_{t}\) is given by
where \(x=(x_{1},\ldots,x_{n+1})^{T}\) is a vector-valued smooth function of t and \(\theta =(\theta_{1},\ldots,\theta_{n})\), the new flow considered here is given by the following evolution equation:
where \(f_{i}(\nu)\) (\(i=1,\ldots,n\)) are n given smooth functions, \({ \Delta =\sum^{n}_{i=1}\frac{\partial^{2} }{\partial \theta_{i}^{2}}}\) is the Laplacian operator, and \(\vert \bullet \vert \) stands for the norm of the vector • in \(\mathbb{R}^{n+1}\). It is easy to verify that equation (1.2) possesses the rotational invariance which plays an important role in the present paper.
We are interested in the deformation of a smooth closed hypersurface \(x=x_{0}(\theta_{1},\ldots,\theta_{n})\) under the flow (1.2), that is, we consider how the hypersurface \(x_{0}\) is smoothly deformed, say, embedded into a smooth family of hypersurfaces depending on a time parameter. This can be reduced to solve the Cauchy problem for (1.2) with the initial data
Obviously, in the present situation, \(x_{0}=x_{0}(\theta_{1},\ldots, \theta_{n})\) is a vector-valued periodic function, say, defined on \([0,1]^{n}\). In Section 2, we shall prove the following.
Theorem 1.1
If \(f\in C^{1}\), \(x_{0}\in L^{\infty }\) and \(\vert x_{0}(\theta_{1},\ldots,\theta_{n})\vert >0\), then the Cauchy problem (1.2), (1.3) admits a unique global smooth solution on \([0,\infty) \times \mathbb{R}^{n}\).
The paper is organized as follows. In Section 2 we prove the global existence and uniqueness of smooth solutions for the Cauchy problem (1.2), (1.3); in Section 3, we state conclusions obtained in the present paper and give some open problems.
2 Global existence and uniqueness of smooth solutions
This section is devoted to the global existence and uniqueness of smooth solution of the following equation:
where \(x=(x_{1},\ldots,x_{n})^{T}\) is the unknown vector-valued function, \(f(\nu)=(f_{1}(\nu),\ldots, f_{m}(\nu))^{T}\) is a given smooth vector-valued function, \({ \Delta =\sum^{m}_{i=1}\frac{\partial^{2} }{\partial \theta_{i}^{2}}}\) is the Laplacian operator, and \(\vert \bullet \vert \) stands for the norm of the vector • in \(\mathbb{R}^{n}\).
Let
Then it is easy to verify that equation (2.1) can be rewritten as
and
for smooth solutions.
We now consider the Cauchy problem for equation (2.1), equivalently, the system (2.1a)-(2.1b) with initial data
where \(r_{0}(\theta)\) is a given scalar function of θ, and \(P_{0}(\theta)\) is a given vector-valued function of θ. In the following, we first investigate the local existence of smooth solution of the above Cauchy problem.
As the standard way, let \(K(t,\theta)\) be the fundamental solution associated with the operator \({ \frac{\partial }{\partial t}-\triangle }\). That is to say,
Then the solution \(r=r(t,\theta)\) of the Cauchy problem
has the following integral representation:
where ∗ denotes the convolution with the space variables. We have the following.
Lemma 2.1
Assume that
then there exists a positive constant T such that the Cauchy problem (2.5) admits a unique smooth solution \(=r(t,\theta)\) on the strip
where
in which
where \(g_{j}=rf_{j}(r)\) (\(j=1,\ldots,m\)).
Proof
Set
and let \(\mathcal{T}\) be the following integral operator:
The solution \(r=r(t,\theta)\) can be obtained as the \(L^{\infty }\)-limit of the sequence \(\{r^{k}\}\) defined by
To prove the above statement, we first claim that, for any \(t\in [0,T]\), we have
In the following, we prove (2.14) by the method of induction.
When \(k=0\), we have
By Young’s inequality, we obtain
Now we assume that \(\Vert r^{k}(t,\theta)\Vert _{L^{\infty }}\leq (m+1)M\) (\(k\in \mathbb{N}\)) holds. We next prove
In fact,
Notice that
It follows from (2.18) that
This is the desired estimate (2.14). Thus, the proof of (2.14) is completed.
In the following, we prove that \(\{r^{k}(t,\theta)\}\) is uniformly convergent in the strip \((0,T]\times \mathbb{R}^{m}\). To do so, it suffices to show that
is uniformly convergent in the strip \((0,T]\times \mathbb{R}^{m}\).
In fact, we have
where
Noting
we obtain from (2.21)
By (2.9), we have
which implies that \({ \sum^{\infty }_{k=1} [ r^{k+1}(t,\theta)-r^{k}(t,\theta) ] }\) is uniformly convergent in the strip \((0,T]\times \mathbb{R}^{m}\). Therefore, \({ \lim_{k\rightarrow \infty }r^{k}(t,\theta)}\) gives the unique local solution of the Cauchy problem (2.5). Thus, the proof of Lemma 2.1 is completed. □
Lemma 2.2
Suppose that
and let \(M\stackrel{\triangle }{=}\Vert r_{0}\Vert _{L^{\infty }}\). Suppose furthermore that \(r(t,\theta)\) is the solution of Cauchy problem (2.5) on the strip \(\Pi_{T}\), then we have
Proof
It follows from the proof of Lemma 2.1 that
Introduce
where C and L are positive constants to be determined. By (2.27),
On the other hand,
Thus,
Choose sufficiently large C such that
and
for all \(t\in [0,T]\).
In the following, we prove that, for any \((t,\theta)\in (0,T)\times (-L,L)^{m}\), that
In fact, if (2.33) is not true, then we can define t̄ by
It is easy to see that there exists a point, denoted by \(\bar{\theta }\in (-L,L)^{m}\), such that
and
By (2.35)-(2.36), it follows from (2.30) that
Noting
we can choose a sufficiently large C such that
On the other hand, by the definition of \((\bar{t},\bar{\theta })\) we have
which is a contradiction. This proves (2.33).
Noting (2.27) and (2.33) and letting \(L\rightarrow \infty \) gives
Similarly, letting
we can prove
Combining (2.42) and (2.44) leads to
Thus, the proof of Lemma 2.2 is completed. □
By Lemma 2.1 and Lemma 2.2, we have the following.
Theorem 2.1
If \(f\in C^{1}\) and \(r_{0}\in L^{\infty }\), then the Cauchy problem (2.5) admits a unique global smooth solution on \([0,\infty)\times \mathbb{R}^{m}\).
Now we turn to a consideration of the Cauchy problem (2.1) (i.e., (2.1a)-(2.1b)), (2.3). We have the following.
Theorem 2.2
Under the assumptions of Theorem 1.1, the Cauchy problem (2.1), (2.3) admits a unique global smooth solution on \([0,\infty) \times \mathbb{R}^{m}\).
Proof
Noting (1.4), by the maximum principle we obtain the result that, on the existence domain of smooth solution, we have
On the one hand, we observe that, under the condition (2.46), equation (2.1) can be reduced to the system (2.1a)-(2.1b); on the other hand, we notice that, once \(r=r(t,\theta)\) is solved from the Cauchy problem (2.5), equation (2.1b) becomes linear. Therefore, Theorem 2.2 follows from Theorem 2.1 directly. □
3 Conclusions and open problems
In the present paper, we introduce a new geometric flow with rotational invariance. This flow is described formally by a system of hyperbolic partial differential equations with viscosity, essentially a coupled system of hyperbolic-parabolic partial differential equations with rotational invariance, which possesses very interesting geometric properties and dynamical behavior. We only investigate the global solutions for the flow equation (1.2) in the Euclidean space \(\mathbb{R}^{n}\) (\(n\ge 2\)), there are some fundamental and interesting problems. In particular, the following open problems seem to us to be more interesting and important: (i) use the flow equation (2.1) to investigate the deformation of a closed m-dimensional sub-manifold \(x_{0}=x_{0}(\theta_{1},\ldots,\theta_{m})\); (ii) find a suitable way to extend the results presented in this paper to the case of Riemannian manifolds instead of the Euclidean space \(\mathbb{R}^{n}\); (iii) introduce the theory of viscous shock waves to investigate geometric problems. These problems are worthy of study in the future.
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Acknowledgements
This research was supported by the Fundamental Research Funds for the Central Universities (2014QNA63), the Natural Science Foundation of Jiangsu Province (BK20150172) and the TianYuan Special Funds of the National Natural Science Foundation of China (11526191).
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Kong, DX., Ru, Q. Global solutions for a new geometric flow with rotational invariance. Bound Value Probl 2017, 17 (2017). https://doi.org/10.1186/s13661-017-0751-7
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DOI: https://doi.org/10.1186/s13661-017-0751-7