Math 2.0

Partial differential equations Existence theory Theorem

Holmgren's uniqueness theorem

Builds on Linear PDECharacteristic varietyAnalytic function

Statement

Let Ω⊆ℝn\Omega \subseteq \R^n be open, and let P=∑∣α∣≤maα(x) ∂αP = \sum_{\abs{\alpha} \le m} a_\alpha(x) \, \partial^\alpha be a linear differential operator of order mm whose coefficients aαa_\alpha are real-analytic on Ω\Omega. Let S⊆ΩS \subseteq \Omega be a real-analytic hypersurface and let x0∈Sx_0 \in S be a point at which SS is noncharacteristic for PP. Let U⊆ΩU \subseteq \Omega be an open neighbourhood of x0x_0, and let u∈Cm(U)u \in C^m(U) satisfy Pu=0P u = 0 in UU and ∂αu=0\partial^\alpha u = 0 on S∩US \cap U for all ∣α∣≤m−1\abs{\alpha} \le m - 1. Then u=0u = 0 in some neighbourhood of x0x_0.

Remarks

Equivalently, two CmC^m solutions of Pu=fP u = f with the same Cauchy data on SS coincide near x0x_0; here ff need not be analytic. The proof is by duality: one solves the adjoint equation P∗v=pP^{*} v = p for polynomials pp, with zero Cauchy data on a nearby analytic hypersurface, using the Cauchy–Kovalevskaya theorem. Integration by parts then shows that ∫u p=0\int u \, p = 0 on a lens-shaped region for every polynomial pp, and the Weierstrass approximation theorem gives u=0u = 0 there. Example: for the wave equation ∂t2u−∂x2u=0\partial_t^2 u - \partial_x^2 u = 0, the line t=0t = 0 is noncharacteristic, so a C2C^2 solution with u(0,x)=∂tu(0,x)=0u(0, x) = \partial_t u(0, x) = 0 vanishes near the line. The analyticity of the coefficients cannot simply be dropped: there are linear operators with smooth coefficients for which the Cauchy problem has nonzero solutions with zero data. Hörmander extended the theorem to distribution solutions and to C1C^1 hypersurfaces.

Going deeper

For a student

The theorem is a unique continuation result across noncharacteristic hypersurfaces. It applies to the Laplace, heat and wave equations, since their coefficients are constant. For the wave equation it is a step towards domain of dependence arguments. For the Laplace equation it shows that the Cauchy problem has at most one solution, even though it is not well posed. The noncharacteristic hypothesis matters: for the heat operator the line t=0t = 0 is characteristic, and Tychonoff's example gives a nonzero solution of the heat equation with zero initial values.

Reading path

To understand this page from the ground up, read these 4 pages in order. The foundations come first.

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  1. Analytic function concept
  2. Characteristic variety concept
  3. Linear PDE concept
  4. Holmgren's uniqueness theorem statement

Further reading

  1. Web https://en.wikipedia.org/wiki/Holmgren%27s_uniqueness_theorem
About this page
Tag1VVKF0Y19B
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Kindstatement, theorem
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MSC35A02, 35A20
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AboutLinear PDE
UsesLinear PDE, Characteristic variety, Analytic function
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