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On Courants nodal domain property for linear combinations of eigenfunctions (after P. B erard and B. Helffer). March 2019 Conference in honour of B.W. Schulze for his 75-th birthday. Bernard Helffer, Laboratoire de Math ematiques


  1. On Courant’s nodal domain property for linear combinations of eigenfunctions (after P. B´ erard and B. Helffer). March 2019 Conference in honour of B.W. Schulze for his 75-th birthday. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ e de Nantes. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  2. Abstract We revisit Courant’s nodal domain property for linear combinations of eigenfunctions. This property was proven by Sturm (1836) in the case of dimension 1. Although stated as true for the Dirichlet Laplacian in dimension > 1 in a footnote of the celebrated book of Courant-Hilbert (and wrongly attributed to H. Herrmann, a PHD student of R. Courant), it appears to be wrong. This was first observed by V. Arnold in the seventies. In this talk, we present simple and explicit counterexamples to this so-called ”Herrmann’s statement” for domains in R d , S 2 or T 2 . We also discuss the existence of a counterexample in a C ∞ , convex domain Ω in R 2 in relation with the analysis of the number of domains delimited by the level sets of a second eigenfunction for the Neumann problem. We finally discuss the question to have positive statements. This work has been done in collaboration with P. B´ erard. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  3. Introduction Let Ω ⊂ R d be a bounded open domain or, more generally, a compact Riemannian manifold with boundary. Consider the eigenvalue problem � − ∆ u = λ u in Ω , (1) B ( u ) = 0 on ∂ Ω , where B ( u ) is some boundary condition on ∂ Ω, so that we have a self-adjoint boundary value problem (including the empty condition if Ω is a closed manifold). � For example, D ( u ) = u ∂ Ω for the Dirichlet boundary condition, or � N ( u ) = ∂ u ∂ν | ∂ Ω for the Neumann boundary condition. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  4. Call H (Ω , B ) the associated self-adjoint extension of − ∆, and list its eigenvalues in nondecreasing order, counting multiplicities, 0 ≤ λ 1 (Ω , B ) < λ 2 (Ω , B ) ≤ λ 3 (Ω , B ) ≤ · · · (2) For any integer n ≥ 1, define the index τ (Ω , B , λ n ) = min { k | λ k (Ω , B ) = λ n (Ω , B ) } . (3) E ( λ n ) will denote the eigenspace associated with λ n . Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  5. The Courant nodal theorem For a real continuous function v on Ω, we define its nodal set Z ( v ) = { x ∈ Ω | v ( x ) = 0 } , (4) and call β 0 ( v ) the number of connected components of Ω \ Z ( v ) i.e., the number of nodal domains of v . Courant’s nodal Theorem (1923) For any nonzero u ∈ E ( λ n (Ω , B )) , β 0 ( u ) ≤ τ (Ω , B , λ n ) ≤ n . (5) Courant’s nodal domain theorem can be found in Courant-Hilbert [10]. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  6. The extended Courant nodal property Given r > 0, denote by L (Ω , B , r ) the space     � L (Ω , B , r ) = c j u j | c j ∈ R , u j ∈ E λ j (Ω , B )  . (6)  λ j (Ω , B ) ≤ r Extended Courant Property:= (ECP) We say that v ∈ L (Ω , B , λ n (Ω , B )) satisfies (ECP) if β 0 ( v ) ≤ τ (Ω , B , λ n ) . (7) A footnote in Courant-Hilbert [10] indicates that this property also holds for any linear combination of the n first eigenfunctions, and refers to the PhD thesis of Horst Herrmann (G¨ ottingen, 1932) [16]. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  7. Historical remarks : Sturm (1836), Pleijel (1956). 1. (ECP) is true for Sturm-Liouville equations. This was first announced by C. Sturm in 1833, [30] and proved in [31]. Other proofs were later on given by J. Liouville and Lord Rayleigh who both cite Sturm explicitly. 2. ˚ A. Pleijel mentions (ECP) in his well-known paper [26] on the asymptotic behaviour of the number of nodal domains of a Dirichlet eigenfunction associated with the n -th eigenvalue in a plane domain. At the end of the paper, he writes: “In order to treat, for instance the case of the free three-dimensional membrane ]0 , π [ 3 , it would be necessary to use, in a special case, the theorem quoted in [9].... However, as far as I have been able to find there is no proof of this assertion in the literature.” Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  8. Historical remarks: V. Arnold (1973-1979) As pointed out by V. Arnold [1], when Ω = S d , (ECP) is 3. related to Hilbert’s 16 − th problem. Arnold [2] mentions that he actually discussed the footnote with R. Courant, that (ECP) cannot be true, and that O. Viro produced in 1979 counter-examples for the 3-sphere S 3 , and any degree larger than or equal to 6, [32]. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  9. More precisely V. Arnold wrote: Having read all this, I wrote a letter to Courant: ”Where can I find this proof now, 40 years after Courant announced the theorem?”. Courant answered that one can never trust one’s students: to any question they answer either that the problem is too easy to waste time on, or that it is beyond their weak powers. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  10. And V. Arnold continues: The point is that for the sphere S 2 (with the standard Riemannian metric) the eigenfunctions (spherical functions) are polynomials. Therefore, their linear combinations are also polynomials, and the zeros of these polynomials are algebraic curves (whose degree is bounded by the number n of the eigenvalue). Therefore, from the generalized Courant theorem one can, in particular, derive estimates for topological invariants of the complements of projective real algebraic curves (in terms of the degrees of these curves). Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  11. ... And then it turned out that the results of the topology of algebraic curves that I had derived from the generalized Courant theorem contradict the results of quantum field theory. Nevertheless, I knew that both my results and the results of quantum field theory were true. Hence, the statement of the generalized Courant theorem is not true. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  12. Historical remarks: Gladwell-Zhu (2003) 4. In [12], Gladwell and Zhu refer to (ECP) as the Courant-Herrmann conjecture . They claim that this extension of Courant’s theorem is not stated, let alone proved, in Herrmann’s thesis or subsequent publications. They consider the case in which Ω is a rectangle in R 2 , stating that they were not able to find a counter-example to (ECP) in this case. They also provide numerical evidence that there are counter-examples for more complicated (non convex) domains. They suggest that may be the conjecture could be true in the convex case. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  13. Historical remarks: looking for the PHD thesis of H. Herrmann 5. Herrmann’s thesis has three parts. Only the second part was accepted by the evaluating committee for publication. This part does not contain any mention of (ECP). The first part, was published later in [17] in Math. Z. in 1936 in a different form. Finally, the third part was never published. The title of this chapter indicates that this part was devoted to the analysis of the Fourier-Robin problem and to analyze how the eigenvalues tend to the eigenvalues of the Dirichlet problem as the Robin parameter tends to + ∞ . Nothing to do with (ECP). The purpose in this talk is to provide simple counter-examples to the Extended Courant Property for domains in R d , S 2 or R 3 , including convex domains. No algebraic topology will be involved. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

  14. Some geometrical statements There are two statements of V. Arnold for which no proof is available. ◮ ECP is true for the sphere S 2 . ◮ ECP does not hold for other metrics on the sphere. Outside the (1 D )-case, the only known result is for R P 2 and was obtained by J. Leydold. Bernard Helffer, Laboratoire de Math´ ematiques Jean Leray, Universit´ On Courant’s nodal domain property for linear combinations of eigenfunctions e de Nantes.

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