Triple products of eigenfunctions and spectral geometry

[VERIFIED] Last updated by Joe Schaefer on Mon, 22 Apr 2024    source

Lawson's minimal surface ξ6,1 stereographically projected from S3 to R3


Joe Schaefer


Using elementary techniques from Geometric Analysis, Partial Differential Equations, and Abelian CC^* Algebras, we uncover a novel, yet familiar, global geometric invariant — namely the indexed set of integrals of triple products of eigenfunctions of the Laplace-Beltrami operator, to precisely characterize which isospectral closed Riemannian manifolds are isometric.


For a closed Riemannian manifold (M,g)(M,g), characterizing its class of non-isometric, isospectral manifolds is a type of Inverse Problem [DH11] in Spectral Geometry. Naïvely one might speculate that this class would always be empty. However, the academic literature is rich with decades-old constructions of specific pairings of counterexamples: beginning in 1964 with John Milnor’s 16-dimensional pair of non-isometric, isospectral flat tori [JM64], and continuing [CS92] towards the generic dimensional characterization of flat tori in Alexander Schiemann’s 1993 doctoral thesis [AS94] — replete with a computer aided search for the critical dim=3\dim = 3 case. A modern survey of the full flat tori history appears in [NRR22].

Along the way were insightful offshoots into more sophisticated, non-Euclidean symmetric covering spaces; constructing such isospectral, non-isometric “duets” involving nontrivial curvature tensors (and their spectrum-determined Euler characteristics in dimension 2 [MS67].) A prime example of this effort was Toshikazu Sunada’s 1985 [TS85] invention of a general-purpose covering space framework, which he then deployed in the same work to construct hyperbolic duets in dimensions 2 and 3.

For inhomogeneous Riemannian metrics, Carolyn Gordon discovered duets that are not even locally isometric [CG93].

Work continues in many related areas [DH11], such as determining topological characteristics of the class of isospectral, non-isometric manifolds in general (empty [ST80], finite [AS94], rigid [GK80], and compact [GZ97]) as a subset of different moduli spaces of Riemannian metrics.

What we offer in this article is a new perspective on a familiar tool: indexed Fourier coefficients of pairwise products of eigenfunctions as a discrete “algebraic/topological invariant” to complement the existing, discrete “analytic invariant” — the non-negative spectrum of the Laplace-Beltrami operator (herein referred to as the Laplacian) on L2(M,g)L^2(M,g). Combined, we observe the pair provides a “discrete global geometric representation” of the isometry classes of isospectral, closed Riemannian manifolds.



Given a (non-decreasing on the eigenvalues) orthonormal basis of eigenfunctions {ei}i=0\set{e^i}_{i=0}^{\infty} for the (non-negative) Laplacian ΔM\Delta_M on L2(M,g)L^2(M,g) associated with a closed Riemannian manifold (M,g)(M,g), define

Mi,j,k:=Meiejekˉgdx M^{i,j,k} := \int_M e^i e^j \bar{e^k} \sqrt{g} dx

To be isometric to (M,g)(M,g), it is a necessary and sufficient condition for another iosospectral closed Riemannian manifold to have an orthonormal basis of eigenfunctions (for its Laplacian) that both preserves the associated eigenvalues and possesses an invariant {Mi,j,k}\set{M^{i,j,k}} under each basis.

Symmetry plays an important role in computationally tractable cases [TF17] [LS18] [PS94], which is aptly illustrated in our flat tori Example below. However, the strength of our approach is perhaps best made apparent in the case of manifolds with the fewest number of Riemannian symmetries, which is the generic case often coinciding with the eigenvalues being unique (i.e., without nontrivial multiplicity.) In this instance, we offer the following


If every eigenvalue has multiplicity 11, given a pair of eigenvalue preserving orthormal bases as described in the hypothesis of the Theorem, the manifolds are isometric if and only if the {Mi,j,k}\set{M^{i,j,k}} for one basis agrees, up to absolute value in the individual terms, with the other basis.

The motivation for the study of {Mi,j,k}\set{M^{i,j,k}} is loosely derived from the study of the role of the linear multiplication operator Y:VVV((z))Y:V\otimes V\rightarrow V((z)) in the definition of a Vertex Operator Algebra [FBZ04] associated with a Chiral Conformal Field Theory. Here VV is the Vector Space of States and V((z))V((z)) is the space of formal Laurent series in zz with coefficients in VV. Since VV often comes equipped as a Hilbert Space with a traditional Fourier series orthonormal basis, indexing YY using the Fourier basis elements of VV is only slightly more involved than the Mi,j,kM^{i,j,k} case studied here, but quite similar in spirit. However a detailed comparison is out of scope for this article.

These results were first demonstrated during a similarly titled talk by the author at MSRI in 1997, but they appear here in published form for the first time.


Now with M,g,ei,Mi,j,kM,g,e^i,M^{i,j,k} as above, for fC(M)f \in C^\infty(M) and i0i \geq 0 note that the Fourier coefficients

f^(i):=Mf(x)eiˉ(x)g(x)dx    f(x)=i=0f^(i)ei(x)\begin{aligned} \hat{f}(i) &:= \int_M f(x)\bar{e^i}(x)\sqrt{g(x)}dx \\ \implies \\ f(x) &= \sum_{i=0}^{\infty}\hat{f}(i)e^i(x) \end{aligned}

since ff is uniquely representable as its rapidly converging Fourier Series (ΔM\Delta_M-specific Sobolev Embeddings [MT13] [RS75], together with Weyl’s Asymptotic Law [HW11], imply the terms in the sum are o(in)o(i^{-n}) uniformly in xx [LH68], nN\forall n\in\N.) Then we see that for f1,f2C(M)f_1, f_2 \in C^\infty(M), the Fourier coefficients of the pointwise product f1f2C(M)f_1 f_2 \in C^\infty(M) are

f1f2^(k)=i,jf1^(i)f2^(j)Mi,j,k    f1f2(x)=i,j,kf1^(i)f2^(j)Mi,j,kek(x)f1=f2p, p N    kf1^(k)ek(x)=i1,...,ip,kf2^(i1)...f2^(ip)Mi1,i2,i3Mi2,i3,i4...Mip1,ip,kek(x)\begin{aligned} \widehat{f_1 f_2}(k) &= \sum_{i,j}^\infty\hat{f_1}(i)\hat{f_2}(j)M^{i,j,k} \\ \implies \\ f_1f_2(x) &= \sum_{i,j,k}\hat{f_1}(i)\hat{f_2}(j)M^{i,j,k}e^k(x) \\ f_1 = f^p_2,\space p \space \in \N \implies \\ \sum_{k}\hat{f_1}(k)e^k(x) &= \sum_{i_1,...,i_p, k}\hat{f_2}(i_1)...\hat{f_2}(i_p)M^{i_1,i_2,i_3}M^{i_2,i_3,i_4}...M^{i_{p-1},i_p,k}e^k(x) \end{aligned}

and so, critically, any multivariate polynomial C[z1,,zl]\weierp \in \Complex[z_1,…,z_l] (on smooth functions) commutes with any spectrum-preserving Δ\Delta-eigenfunction orthonormal basis map FF that preserves {Mi,j,k}\set{M^{i,j,k}}:

C(M, Cl)C(M)FFl timesFC(N, Cl)C(N)\begin{CD} C^\infty(M,\space\Complex^l) @>\weierp >> C^\infty(M)\\ @V\underbrace{F\oplus\dots\oplus F}_{l\space\text{times}}VV @VVFV\\ C^\infty(N,\space\Complex^l) @>>\weierp > C^\infty(N) \end{CD}

Moreover if AMA\subset M is Borel-measurable, then the results above hold pointwise for the characteristic function of AA everywhere except along the boundary of AA: if f=f2f = f^2 and A:={xMf(x)=1}A:=\set{x\in M|f(x)=1},

if^(i)ei(x)=i,j,kf^(i)f^(j)Mi,j,kek(x)={1xA˚0xA˚\sum_{i}\hat{f}(i)e^i(x) = \sum_{i,j,k}\hat{f}(i)\hat{f}(j)M^{i,j,k}e^k(x) = \begin{cases} 1 & x \in \mathring{A} \\ 0 & x \in \mathring{A^\complement}\end{cases}

and by uniqueness, we have the following identity

f^(k)=i,jf^(i)f^(j)Mi,j,k  k0    f=f2 a.e.\begin{aligned} \hat{f}(k) &= \sum_{i,j}\hat{f}(i)\hat{f}(j)M^{i,j,k}\space\space \forall k\geq 0 \\ \iff f&=f^2 \space a.e. \end{aligned}

This implies any such basis map as above carries characteristic functions (as members of L2(M,g)L1(M,g)L^2(M,g)\subset L^1(M,g)) to characteristic functions in a measure-preserving fashion.

The point of these computations is to emphasize the fact that {Mi,j,k}\set{M^{i,j,k}} characterizes the Harmonic Analysis of the pointwise multiplication operator on C(M)C^\infty(M), which is a dense subalgebra of the Abelian CC^* algebra C(M)C(M), by the Stone-Weierstrass theorem.

For the rapid convergence of these above sums involving Mi,j,kM^{i,j,k}, note that products of eigenfunctions are smooth, so these Fourier coefficients decay as above (in each index). For more details, see Emmett Wyman’s work in 2022 with these coefficients as it relates to the triangle inequality on the eigenvalues [EW22].

Note: we may always assume

e0=M0,0,0=1/vol(M)    M0,j,k=Mj,0,k=δjk /vol(M)\begin{aligned} e^0 &= M^{0,0,0} = 1/\sqrt{vol(M)} \\ \implies \\ M^{0,j,k} &= M^{j,0,k} = \delta_{j-k}\space/\sqrt{vol(M)} \end{aligned}

where δi\delta_i is the Kronecker delta. Since vol(M)vol(M) is a spectral invariant [HW11], this information is already available from isospectrality considerations.

Proof of Theorem

For necessity, let F:(N,h)(M,g)F:(N,h)\rightarrow (M,g) be an isometry between closed Riemannian manifolds, and let the target orthonormal basis of eigenfunctions on L2(N,h)L^2(N,h) be the pull-back via FF of the orthonormal basis {ei}\set{e^i} on (M,g)(M,g) above. Since

Mi,j,k=Meiejekˉgdy=Nei(F(x))ej(F(x))ekˉ(F(x))hdx\begin{aligned} M^{i,j,k} &= \int_M e^i e^j \bar{e^k}\sqrt{g}dy \\ &= \int_N e^i(F(x)) e^j(F(x))\bar{e^k}(F(x))\sqrt{h}dx \end{aligned}

we are done with the necessity argument.

For sufficiency, we now consider the linear, bijective orthonormal eigenfunction basis map FF from C(M)C^\infty(M) to C(N)C^\infty(N) and note that from the calculations in the Preliminaries above, FF preserves pointwise products for smooth functions (and preserves characteristic functions when extended to L2(M,g)L^2(M,g)) by the premise that {Mi,j,k}\set{M^{i,j,k}} is invariant under this map.


F:C(M)C(N)F: C^\infty(M)\rightarrow C^\infty(N) preserves the uniform norm.

Proof of Lemma

Let {ai}\set{a_i} be a smooth partition of unity on MM.

1=iai(x)=i,jai^(j)ej(x)=jej(x)iai^(j)\begin{aligned} 1 &= \sum_i a_i(x) \\ &= \sum_{i,j} \hat{a_i}(j)e^j(x) \\ &= \sum_j e^j(x)\sum_i \hat{a_i}(j) \end{aligned}

Thus iai^(j)=δjvol(M)\sum_i\hat{a_i}(j) = \delta_j\sqrt{vol(M)} (Kronecker delta).

By the dominated convergence theorem,

limpjajp^(k)=˙j{aj=1}ekˉ(x)gdx\lim_{p\rightarrow\infty} \sum_j\hat{a^p_j}(k) = \int_{\dot{\bigcup}_j\set{a_j=1}}\bar{e^k}(x)\sqrt{g}dx

which is a characteristic function of positive measure on each disjoint subset {xMaj(x)=1}\set{x\in M | a_j(x) = 1}. This means the Lemma is proven for each aja_j, since the limiting characteristic function of a set with positive measure is preserved, and hence has uniform norm 1, as do all ajp, F(ajp)=F(aj)p, pNa_j^p,\space F(a_j^p)=F(a_j)^p,\space p\in\N, by Diagram (4).

Without loss of generality, we may apply the special case result shown for the smooth partition of unity {f/f,1f/f}\lbrace|f|/\lVert f \rVert_\infty, 1 - |f|/\lVert f\rVert_\infty\rbrace, where {xM f(x)=f} \set{x\in M|\space|f(x)| = \lVert f \rVert_\infty} has positive measure, and the Lemma is proven in full.

This means that on a dense set of C(M)C(M) (and C(N)C(N)), we have established FF as an isomorphism of Abelian CC^* algebras, and thus can be extended to an isomorphism of C(M)C(M) and C(N)C(N) in the same category.

Now we apply the Gelfand-Naimark Representation Theorem (in contravariant functor form) for Abelian CC^* algebras [JC19] to represent this isomorphism by a homeomorphism between NN and MM. Since it is bijective on smooth functions, it too must be smooth.

As this now diffeomorphism preserves eigenvalues and eigenfunctions (by hypothesis on FF), it must preserve the Laplacian on smooth functions. Hence it also must preserve the principal symbols of these same elliptic operators [MT13]. The principal symbols of the Laplacian are simply another means of expressing the Riemannian metric on the manifolds in question.

This completes the proof of the Theorem.

Discussion of Conjecture

With {M0i,j,k}\set{M_0^{i,j,k}} and {M1i,j,k}\set{M_1^{i,j,k}} representing the two triple-product sets for the bases {e0i}\set{e_0^i} and {e1i}\set{e_1^i}, let zi{1,1}z_i \in \set{-1,1} be the Z2\Z_2^\infty action on such an R\R-valued orthonormal basis {e1i}\set{e_1^i}. Thus, we need to choose ziz_i so that {zie1i}\set{z_ie_1^i} yields {M1i,j,k}={zizjzkM0i,j,k}\set{M_1^{i,j,k}} = \set{z_i z_j z_kM_0^{i,j,k}}.

We observe necessarily that

zk=M0i,i,k/M1i,i,k  i,kN,M0i,i,k0.z_k = M_0^{i,i,k} / M_1^{i,i,k} \,\, \forall i,k\in\N,\, ⋺ M_0^{i,i,k} \ne 0 \,.

Since for any given kk, M0i,i,kM_0^{i,i,k} cannot be identically 00 for all ii, this Formula for zkz_k requires both ii-independence, and sufficiency, to establish the basis map e0izie1ie_0^i \mapsto z_i e_1^i preserves {M0i,j,k}\set{M_0^{i,j,k}}. These aspects remain unknown.


Let {λi}Rn\set{\lambda_i} \subset \R^n be an indexed, rank nn lattice of Lie Algebra weights for the quotient space representation of g=Rn\frak{g}=\Reals^n as translation invariant (i.e., constant) vector fields on itself, when Rn\R^n is also viewed as g\frak{g}’s associated Lie Group over a torus defined by Rn/AZn,AGL(n,R)\Reals^n/A\Z^n, A \in GL(n,\Reals). These weights define integrable lifts of 1-forms over the torus that integrate to linear functionals <xλi, xRn\bra{x} \lambda_i\rangle,\space x\in\Reals^n as its Lie Group (covering the torus). These linear functionals can then be uniformly rescaled (by 2π12\pi \sqrt{-1}) and exponentiated to form multiplicative characters that descend to form an orthonormal basis of L2(Rn/AZn,dx)L^2(\Reals^n/A\Z^n,dx), with Lebesgue (Haar) measure dxdx.

Moreover, this basis simultaneously diagonalizes the flat torus’s Laplacian because the Laplacian is the image of a symmetric, negative-definite quadratic Casimir element under this (constant coefficient linear differential operator) quotient space representation of the universal enveloping algebra. Hence, its eigenvalues are in constant proportion (of 4π24\pi^2) to the Casimir-element-determined-length-squared of each character’s weight in the lattice.

We presently view the above basis

{e2π1xλi/detA}i=0\set{e^{2\pi\sqrt{-1}\langle{x}|\lambda_i\rangle}/\sqrt{|\det A|}}_{i=0}^\infty

to be our Theorem-applicable Fourier basis of orthonormal (multiplicative character) eigenfunctions (of this quotient representation of the (negative) Euclidean Casimir element) directly corresponding to {λi}\set{\lambda_i}. By our Theorem’s hypotheses, we must have i<j    λiλji < j \implies \lVert\lambda_i\rVert \leq \lVert\lambda_j\rVert (with the Euclidean norm on the weights).

Now we can compute

Mi,j,k={1/detAλi+λjλk=00otherwiseM^{i,j,k} = \begin{cases} 1/\sqrt{|\det A|} & \lambda_i + \lambda_j - \lambda_k = 0 \\ 0 & \text{otherwise} \end{cases}

As this Equation is linear on the weight lattice (A1)tZn={λi}(A^{-1})^t\Z^n = \set{\lambda_i}, only an L2L^2 orthonormal eigenfunction basis map which is induced from a volume-preserving invertible linear map between two such indexed, rank nn weight lattices will keep the “algebraic/topological” indexed data set {Mi,j,k}\set{M^{i,j,k}} invariant.

However, in order to apply our Theorem, it is essential that such a linear map BB be BO(n,R)B\in O(n,\Reals) on the weight lattice, because the induced L2L^2 eigenfunction basis map

{e2π1xBλi/detA}i=0\set{e^{2\pi\sqrt{-1}\langle x| B\lambda_i\rangle}/\sqrt{|\det A|}}_{i=0}^\infty

must also preserve the “analytic” invariants — the Casimir-element induced figure 4π2λi24\pi^2\lVert\lambda_i\rVert^2 for each indexed weight, i.e. the individual eigenvalues of the flat-tori’s Laplacian.

This representation-theoretical account [AK01] is exactly equivalent to the prior development of lattice congruence [NRR22] traditonally used to delineate isometry classes of flat tori. In fact, the matrix transpose of such a linear map BO(n,R)B\in O(n,\Reals), as described in the prior paragraph, is the contravariant Riemannian isometry between the tori, as provided by application of the Gelfand-Naimark Representation Theorem during the Proof of our Theorem.


The original research was funded in part by a gracious James Simons Research Award in 1995-1996, and the generous support of an Alfred P. Sloan Dissertation Fellowship in 1996-1997 at the University at Stony Brook.

The author would also like to thank Tanya Christiansen, Carolyn Gordon, Hamid Hezari, Harish Seshadri, and especially Leon Takhtajan for their technical assistance and review in the preparation of this manuscript for publication.