Math 2.0

Global analysis, analysis on manifolds Spectral geometry Example

Laplacian eigenvalues of the round sphere

Builds on SphereLaplace–Beltrami operatorSpherical harmonics

Example

Let Sn⊂ℝn+1S^n \subset \R^{n+1} be the unit sphere with its round metric, n≥1n \ge 1, and let Δ=−div⁡grad⁡\Delta = -\operatorname{div} \operatorname{grad} be its Laplace–Beltrami operator. Its eigenvalues are λk=k(k+n−1),k=0,1,2,….\lambda_k = k(k + n - 1), \quad k = 0, 1, 2, \ldots. The λk\lambda_k-eigenspace consists of the restrictions to SnS^n of the homogeneous harmonic polynomials of degree kk on ℝn+1\R^{n+1}, the spherical harmonics of degree kk. Its dimension is (n+kn)−(n+k−2n),\binom{n + k}{n} - \binom{n + k - 2}{n}, with the convention that the second term is 00 when k<2k < 2.

Check of the eigenvalue: write a homogeneous harmonic polynomial of degree kk as P=rkYP = r^k Y with r=∣x∣r = \abs{x} and YY a function on SnS^n. In polar coordinates the Euclidean Laplacian is ∂r2+nr∂r−1r2Δ\partial_r^2 + \frac{n}{r} \partial_r - \frac{1}{r^2} \Delta. Applied to PP it gives rk−2(k(k−1)+nk)Y−rk−2ΔY=0r^{k-2} \big( k(k-1) + nk \big) Y - r^{k-2} \Delta Y = 0, so ΔY=k(k+n−1)Y\Delta Y = k(k + n - 1) Y. These eigenfunctions span a dense subspace of L2(Sn)L^2(S^n), so there are no other eigenvalues.

For S2S^2 the eigenvalues are k(k+1)k(k+1) with multiplicity 2k+12k + 1. For k=1k = 1 the eigenfunctions are the restrictions of the coordinate functions x1,…,xn+1x_1, \ldots, x_{n+1}, with eigenvalue nn.

Remarks

Since the unit sphere has Ricci curvature (n−1)(n - 1) times the metric, the first nonzero eigenvalue nn shows that the bound in the Lichnerowicz–Obata theorem is attained. The multiplicities grow like a constant times kn−1k^{n-1}, which agrees with Weyl's law.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Spherical_harmonics
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Instance ofSpectrum of the Laplace–Beltrami operator
UsesSphere, Laplace–Beltrami operator, Spherical harmonics

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