hearing the shape of a drum
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In theoretical mathematics, the conceptual problem of "hearing the shape of a drum" refers to the prospect of inferring information about the shape of a hypothetical idealized drumhead from the sound it makes when struck, i.e. from analysis of overtones. "Can One Hear the Shape of a Drum?" is the title of a 1966 article by Mark Kac in the ''
American Mathematical Monthly ''The American Mathematical Monthly'' is a peer-reviewed scientific journal of mathematics. It was established by Benjamin Finkel in 1894 and is published by Taylor & Francis on behalf of the Mathematical Association of America. It is an exposi ...
'' which made the question famous, though this particular phrasing originates with Lipman Bers. Similar questions can be traced back all the way to physicist
Arthur Schuster Sir Franz Arthur Friedrich Schuster (12 September 1851 – 14 October 1934) was a German-born British physicist known for his work in spectroscopy, electrochemistry, optics, X-radiography and the application of harmonic analysis to physics. S ...
in 1882. For his paper, Kac was given the Lester R. Ford Award in 1967 and the Chauvenet Prize in 1968. The frequencies at which a drumhead can vibrate depend on its shape. The
Helmholtz equation In mathematics, the Helmholtz equation is the eigenvalue problem for the Laplace operator. It corresponds to the elliptic partial differential equation: \nabla^2 f = -k^2 f, where is the Laplace operator, is the eigenvalue, and is the (eigen)fun ...
calculates the frequencies if the shape is known. These frequencies are the
eigenvalues In linear algebra, an eigenvector ( ) or characteristic vector is a vector that has its direction unchanged (or reversed) by a given linear transformation. More precisely, an eigenvector \mathbf v of a linear transformation T is scaled by a ...
of the
Laplacian In mathematics, the Laplace operator or Laplacian is a differential operator given by the divergence of the gradient of a scalar function on Euclidean space. It is usually denoted by the symbols \nabla\cdot\nabla, \nabla^2 (where \nabla is th ...
in the space. A central question is whether the shape can be predicted if the frequencies are known; for example, whether a Reuleaux triangle can be recognized in this way. Kac admitted that he did not know whether it was possible for two different shapes to yield the same set of frequencies. The question of whether the frequencies determine the shape was finally answered in the negative in the early 1990s by Carolyn S. Gordon, David Webb and Scott A. Wolpert.


Formal statement

More formally, the drum is conceived as an elastic membrane whose boundary is clamped. It is represented as a domain ''D'' in the plane. Denote by ''λ''''n'' the Dirichlet eigenvalues for ''D'': that is, the
eigenvalue In linear algebra, an eigenvector ( ) or characteristic vector is a vector that has its direction unchanged (or reversed) by a given linear transformation. More precisely, an eigenvector \mathbf v of a linear transformation T is scaled by a ...
s of the Dirichlet problem for the
Laplacian In mathematics, the Laplace operator or Laplacian is a differential operator given by the divergence of the gradient of a scalar function on Euclidean space. It is usually denoted by the symbols \nabla\cdot\nabla, \nabla^2 (where \nabla is th ...
: : \begin \Delta u + \lambda u = 0\\ u, _ = 0 \end Two domains are said to be isospectral (or homophonic) if they have the same eigenvalues. The term "homophonic" is justified because the Dirichlet eigenvalues are precisely the fundamental tones that the drum is capable of producing: they appear naturally as Fourier coefficients in the solution
wave equation The wave equation is a second-order linear partial differential equation for the description of waves or standing wave fields such as mechanical waves (e.g. water waves, sound waves and seismic waves) or electromagnetic waves (including light ...
with clamped boundary. Therefore, the question may be reformulated as: what can be inferred on ''D'' if one knows only the values of ''λ''''n''? Or, more specifically: are there two distinct domains that are isospectral? Related problems can be formulated for the Dirichlet problem for the Laplacian on domains in higher dimensions or on
Riemannian manifold In differential geometry, a Riemannian manifold is a geometric space on which many geometric notions such as distance, angles, length, volume, and curvature are defined. Euclidean space, the N-sphere, n-sphere, hyperbolic space, and smooth surf ...
s, as well as for other
elliptic differential operator In the theory of partial differential equations, elliptic operators are differential operators that generalize the Laplace operator. They are defined by the condition that the coefficients of the highest-order derivatives be positive, which im ...
s such as the Cauchy–Riemann operator or
Dirac operator In mathematics and in quantum mechanics, a Dirac operator is a first-order differential operator that is a formal square root, or half-iterate, of a second-order differential operator such as a Laplacian. It was introduced in 1847 by William Ham ...
. Other boundary conditions besides the Dirichlet condition, such as the
Neumann boundary condition In mathematics, the Neumann (or second-type) boundary condition is a type of boundary condition, named after Carl Neumann. When imposed on an ordinary or a partial differential equation, the condition specifies the values of the derivative app ...
, can be imposed. See spectral geometry and isospectral as related articles.


The answer

In 1964, John Milnor observed that a theorem on lattices due to Ernst Witt implied the existence of a pair of 16-dimensional flat tori that have the same eigenvalues but different shapes. However, the problem in two dimensions remained open until 1992, when Carolyn Gordon, David Webb, and Scott Wolpert constructed, based on the Sunada method, a pair of regions in the plane that have different shapes but identical eigenvalues. The regions are
concave polygon A simple polygon that is not convex is called concave, non-convex or reentrant. A concave polygon will always have at least one reflex interior angle—that is, an angle with a measure that is between 180° degrees and 360° degrees exclusive. ...
s. The proof that both regions have the same eigenvalues uses the symmetries of the Laplacian. This idea has been generalized by Buser, Conway, Doyle, and Semmler who constructed numerous similar examples. So, the answer to Kac's question is: for many shapes, one cannot hear the shape of the drum ''completely''. However, some information can be inferred. On the other hand, Steve Zelditch proved that the answer to Kac's question is positive if one imposes restrictions to certain
convex Convex or convexity may refer to: Science and technology * Convex lens, in optics Mathematics * Convex set, containing the whole line segment that joins points ** Convex polygon, a polygon which encloses a convex set of points ** Convex polytop ...
planar regions with analytic boundary. It is not known whether two non-convex analytic domains can have the same eigenvalues. It is known that the set of domains isospectral with a given one is compact in the C topology. Moreover, the sphere (for instance) is spectrally rigid, by Cheng's eigenvalue comparison theorem. It is also known, by a result of Osgood, Phillips, and Sarnak that the moduli space of
Riemann surface In mathematics, particularly in complex analysis, a Riemann surface is a connected one-dimensional complex manifold. These surfaces were first studied by and are named after Bernhard Riemann. Riemann surfaces can be thought of as deformed vers ...
s of a given genus does not admit a continuous isospectral flow through any point, and is compact in the Fréchet–Schwartz topology.


Weyl's formula

Weyl's formula states that one can infer the area ''A'' of the drum by counting how rapidly the ''λ''''n'' grow. We define ''N''(''R'') to be the number of eigenvalues smaller than ''R'' and we get : A = \omega_d^(2\pi)^d \lim_\frac, where ''d'' is the dimension, and \omega_d is the volume of the ''d''-dimensional unit ball. Weyl also conjectured that the next term in the approximation below would give the perimeter of ''D''. In other words, if ''L'' denotes the length of the perimeter (or the surface area in higher dimension), then one should have : N(R) = (2\pi)^\omega_d AR^ \mp \frac(2\pi)^\omega_ LR^ + o(R^). For a smooth boundary, this was proved by Victor Ivrii in 1980. The manifold is also not allowed to have a two-parameter family of periodic geodesics, such as a sphere would have.


The Weyl–Berry conjecture

For non-smooth boundaries, Michael Berry conjectured in 1979 that the correction should be of the order of : R^, where ''D'' is the
Hausdorff dimension In mathematics, Hausdorff dimension is a measure of ''roughness'', or more specifically, fractal dimension, that was introduced in 1918 by mathematician Felix Hausdorff. For instance, the Hausdorff dimension of a single point is zero, of a line ...
of the boundary. This was disproved by J. Brossard and R. A. Carmona, who then suggested that one should replace the Hausdorff dimension with the upper box dimension. In the plane, this was proved if the boundary has dimension 1 (1993), but mostly disproved for higher dimensions (1996); both results are by and Pomerance.


See also

* Gassmann triple * Isospectral * Spectral geometry * Vibrations of a circular membrane


Notes


References

* * * * * * * * (In Russian). * * * * . (Revised and enlarged second edition to appear in 2005.) * * * * *


External links


Simulation
showing solutions of the wave equation in two isospectral drums

by Toby Driscoll at the University of Delaware
Some planar isospectral domains
by Peter Buser, John Horton Conway, Peter Doyle, and Klaus-Dieter Semmler *
3D rendering of the Buser-Conway-Doyle-Semmler homophonic drums


by Ivars Peterson at the Mathematical Association of America web site * * {{DEFAULTSORT:Hearing The Shape Of A Drum Partial differential equations Spectral theory Drumming Mathematics papers