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[[Image:Isospectral drums.svg|frame|right|Mathematically ideal drums with membranes of these two different shapes (but otherwise identical) would sound the same, because the [[eigenfrequency|eigenfrequencies]] are all equal, so the [[Timbre#Spectra|timbral spectra]] would contain the same overtones. This example was constructed by Gordon, Webb and Wolpert. Notice that both polygons have the same area and perimeter.]]
[[Image:Isospectral drums.svg|frame|right|Mathematically ideal drums with membranes of these two different shapes (but otherwise identical) would sound the same, because the [[eigenfrequency|eigenfrequencies]] are all equal, so the [[Timbre#Spectra|timbral spectra]] would contain the same overtones. This example was constructed by Gordon, Webb and Wolpert. Notice that both polygons have the same area and perimeter.]]


To '''hear the shape of a drum''' is to infer information about the shape of the [[drumhead]] from the sound it makes, i.e., from the list of [[overtones]], via the use of [[mathematics|mathematical]] theory. "Can One Hear the Shape of a Drum?" was the witty title of an article by [[Mark Kac]] in the [[American Mathematical Monthly]] 1966 (see the [[#References|references]] below)<ref name=a>{{cite journal|last=Kac|first=Mark|title=Can One Hear the Shape of a Drum?|journal=The American Mathematical Monthly|year=1966|month=April|volume=73|url=http://www.jstor.org/stable/2313748}}</ref>, but these questions can be traced back all the way to [[Hermann Weyl]].
To '''hear the shape of a drum''' is to infer information about the shape of the [[drumhead]] from the sound it makes, i.e., from the list of [[overtones]], via the use of [[mathematics|mathematical]] theory. "Can One Hear the Shape of a Drum?" was the witty title of an article by [[Mark Kac]] in the [[American Mathematical Monthly]] 1966 <ref name=hearshape>{{cite journal|last=Kac|authorlink=Mark Kac|first=Mark|title=Can One Hear the Shape of a Drum?|journal=[[American Mathematical Monthly]]|year=1966|month=April|volume=73|issue=4, part 2|pages=1&ndash23|doi=10.2307/2313748|jstor=2313748}}</ref>, but these questions can be traced back all the way to [[Hermann Weyl]].


The frequencies at which a drumhead can vibrate depend on its shape. The [[Helmholtz equation]] tells us the frequencies if we know the shape. These frequencies are the [[eigenvalues]] of the [[Laplacian]] in the region. A central question is: can they tell us the shape if we know the frequencies? No other shape than a square vibrates at the same frequencies as a square. Is it possible for two different shapes to yield the same set of frequencies? Kac did not know the answer to that question.
The frequencies at which a drumhead can vibrate depend on its shape. The [[Helmholtz equation]] tells us the frequencies if we know the shape. These frequencies are the [[eigenvalues]] of the [[Laplacian]] in the region. A central question is: can they tell us the shape if we know the frequencies? No other shape than a square vibrates at the same frequencies as a square. Is it possible for two different shapes to yield the same set of frequencies? Kac did not know the answer to that question.
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==The answer==
==The answer==
Almost immediately, [[John Milnor]] observed that a theorem due to [[Ernst Witt]] implied the existence of a pair of 16-dimensional tori that have the same eigenvalues but different shapes. However, the problem in two dimensions remained open until 1992, when Gordon, Webb, and Wolpert constructed, based on the [[Toshikazu Sunada|Sunada method]], a pair of regions in the plane that have different shapes but identical eigenvalues. The regions are non-[[convex polygon]]s (see picture). The proof that both regions have the same eigenvalues is rather elementary and uses the symmetries of the Laplacian. This idea has been generalized by Buser et al., 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.
Almost immediately, [[John Milnor]] observed that a theorem due to [[Ernst Witt]] implied the existence of a pair of 16-dimensional tori that have the same eigenvalues but different shapes. However, the problem in two dimensions remained open until 1992, when Gordon, Webb, and Wolpert constructed, based on the [[Toshikazu Sunada|Sunada method]], a pair of regions in the plane that have different shapes but identical eigenvalues<ref>{{cite journal|doi=10.1090/S0273-0979-1992-00289-6|first1=Carolyn|last1=Gordon|first2=David L.|last2=Webb|first3=Scott|last3=Wolpert|title=One Cannot Hear the Shape of a Drum|journal=Bulletin of the American Mathematical Society|volume=27|issue=1|year=1992|pages=134&ndash;138|url=http://www.ams.org/bull/1992-27-01/S0273-0979-1992-00289-6/home.html}}<ref>. The regions are non-[[convex polygon]]s (see picture). The proof that both regions have the same eigenvalues is rather elementary and uses the symmetries of the Laplacian. This idea has been generalized by Buser et al., 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 set|convex]] planar regions with [[analytic function|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<sup>∞</sup> 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 surfaces of a given genus does not admit a continuous isospectral flow through any point, and is compact in the Frechet–Schwartz topology.
On the other hand, [[Steve Zelditch]] proved that the answer to Kac's question is positive if one imposes restrictions to certain [[convex set|convex]] planar regions with [[analytic function|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<sup>∞</sup> 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 surfaces of a given genus does not admit a continuous isospectral flow through any point, and is compact in the Frechet–Schwartz topology.
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* [[Gassmann triple]]
* [[Gassmann triple]]
* [[Isospectral]]
* [[Isospectral]]
*[[Spectral geometry]]
* [[Spectral geometry]]
* <ref>an extension to [[iterated function system]] fractals {{cite journal|first1=W.|last1=Arrighetti|first2=G.|last2=Gerosa|contribution=Can you hear the fractal dimension of a drum?|arxiv=math.SP/0503748 |title=Applied and Industrial Mathematics in Italy|series=Series on Advances in Mathematics for Applied Sciences|volume=69|pages=65–75|publisher=World Scientific|year=2005|isbn=978-981-256-368-2}}</ref>
* <ref>{{cite journal|doi=10.1007/BF01210795|first1=Jean|last1=Brossard|first2=René|last2=Carmona|title=Can one hear the dimension of a fractal?|journal=Comm. Math. Phys.|volume=104|issue=1|year=1986|pages= 103&ndash;122|bibcode = 1986CMaPh.104..103B }}<ref>


==References==
==References==
<references />
<references />
* {{citation|first1=W.|last1=Arrighetti|first2=G.|last2=Gerosa|contribution=Can you hear the fractal dimension of a drum?|arxiv=math.SP/0503748 |title=Applied and Industrial Mathematics in Italy|series=Series on Advances in Mathematics for Applied Sciences|volume=69|pages=65–75|publisher=World Scientific|year=2005|isbn=978-981-256-368-2}}
* {{citation|doi=10.1007/BF01210795|first1=Jean|last1=Brossard|first2=René|last2=Carmona|title=Can one hear the dimension of a fractal?|journal=Comm. Math. Phys.|volume=104|issue=1|year=1986|pages= 103&ndash;122|bibcode = 1986CMaPh.104..103B }}
* {{citation|first1=Peter|last1=Buser|first2=John|last2=Conway|authorlink2=John Horton Conway|first3=Peter|last3=Doyle|first4=Klaus-Dieter|last4=Semmler|title=Some planar isospectral domains|journal=International Mathematics Research Notices|volume=9|year=1994|pages=391ff}}
* {{citation|first1=Peter|last1=Buser|first2=John|last2=Conway|authorlink2=John Horton Conway|first3=Peter|last3=Doyle|first4=Klaus-Dieter|last4=Semmler|title=Some planar isospectral domains|journal=International Mathematics Research Notices|volume=9|year=1994|pages=391ff}}
* {{citation | last=Chapman | first=S.J. | year=1995 | title=Drums that sound the same | journal=[[American Mathematical Monthly]] | issue=February | pages=124&ndash;138}}
* {{citation | last=Chapman | first=S.J. | year=1995 | title=Drums that sound the same | journal=[[American Mathematical Monthly]] | issue=February | pages=124&ndash;138}}
* {{cite journal|last=Giraud|first=Olivier|coauthors=[[Thas, Koen]]|title=Hearing shapes of drums - mathematical and physical aspects of isospectrality|journal=Reviews of Modern Physics|year=2010|volume=82|issue=3|pages=2213–2255|doi=10.1103/RevModPhys.82.2213|arxiv=1101.1239|bibcode=2010RvMP...82.2213G}}
* {{cite journal|last=Giraud|first=Olivier|coauthors=[[Thas, Koen]]|title=Hearing shapes of drums - mathematical and physical aspects of isospectrality|journal=Reviews of Modern Physics|year=2010|volume=82|issue=3|pages=2213–2255|doi=10.1103/RevModPhys.82.2213|arxiv=1101.1239|bibcode=2010RvMP...82.2213G}}
* {{citation|first1=Carolyn|last1=Gordon|first2=David|last2=Webb|title=You can't hear the shape of a drum|journal= [[American Scientist]] |volume=84|issue=January&ndash;February|pages=46&ndash;55}}
* {{citation|first1=Carolyn|last1=Gordon|first2=David|last2=Webb|title=You can't hear the shape of a drum|journal=[[American Scientist]] |volume=84|issue=January&ndash;February|pages=46&ndash;55}}
* {{citation|doi=10.1007/BF01231320|first1=C.|last1=Gordon|first2=D.|last2=Webb|first3=S.|last3=Wolpert|title=Isospectral plane domains and surfaces via Riemannian orbifolds|journal=Inventiones Mathematicae|volume=110|year=1992|issue=1|pages=1&ndash;22|bibcode = 1992InMat.110....1G }}
* {{citation|doi=10.1007/BF01231320|first1=C.|last1=Gordon|first2=D.|last2=Webb|first3=S.|last3=Wolpert|title=Isospectral plane domains and surfaces via Riemannian orbifolds|journal=Inventiones Mathematicae|volume=110|year=1992|issue=1|pages=1&ndash;22|bibcode = 1992InMat.110....1G }}
*{{citation |doi= 10.1090/S0273-0979-1992-00289-6 |first1= Carolyn | last1=Gordon | first2=David L. |last2=Webb |first3= Scott |last3=Wolpert |title=One Cannot Hear the Shape of a Drum |journal=Bulletin of the American Mathematical Society|volume= 27 |issue= 1 |year=1992 |pages= 134&ndash;138 |url=http://www.ams.org/bull/1992-27-01/S0273-0979-1992-00289-6/home.html}}
* {{citation|first=V. Ja.|last=Ivrii|title=The second term of the spectral asymptotics for a Laplace&ndash;Beltrami operator on manifolds with boundary|journal=Funktsional. Anal. i Prilozhen|volume=14|issue=2|year=1980|pages=25&ndash;34}} (In [[Russian language|Russian]]).
* {{citation|first=V. Ja.|last=Ivrii|title=The second term of the spectral asymptotics for a Laplace&ndash;Beltrami operator on manifolds with boundary|journal=Funktsional. Anal. i Prilozhen|volume=14|issue=2|year=1980|pages=25&ndash;34}} (In [[Russian language|Russian]]).
* {{citation|doi=10.2307/2313748|first=Mark|last=Kac|authorlink=Mark Kac|title=Can one hear the shape of a drum?|journal=[[American Mathematical Monthly]]|volume=73|issue=4, part 2|year=1966|pages=1&ndash;23|jstor=2313748}}
* {{citation|first=Michel L.|last=Lapidus|title=Can one hear the shape of a fractal drum? Partial resolution of the Weyl&ndash;Berry conjecture|journal=Geometric analysis and computer graphics (Berkeley, CA, 1988)|pages=119&ndash;126|series=Math. Sci. Res. Inst. Publ.|issue=17|publisher=Springer|publication-place=New York|year=1991}}
* {{citation|first=Michel L.|last=Lapidus|title=Can one hear the shape of a fractal drum? Partial resolution of the Weyl&ndash;Berry conjecture|journal=Geometric analysis and computer graphics (Berkeley, CA, 1988)|pages=119&ndash;126|series=Math. Sci. Res. Inst. Publ.|issue=17|publisher=Springer|publication-place=New York|year=1991}}
* {{citation|first=Michel L.|last=Lapidus|contribution=Vibrations of fractal drums, the [[Riemann hypothesis]], waves in fractal media, and the Weyl&ndash;Berry conjecture|title=Ordinary and Partial Differential Equations, Vol IV, Proc. Twelfth Internat. Conf. (Dundee, Scotland,UK, June 1992)|editors=B. D. Sleeman and R. J. Jarvis|series=Pitman Research Notes in Math. Series|volume=289|publisher=Longman and Technical|publication-place=London|year=1993|pages=126&ndash;209}}
* {{citation|first=Michel L.|last=Lapidus|contribution=Vibrations of fractal drums, the [[Riemann hypothesis]], waves in fractal media, and the Weyl&ndash;Berry conjecture|title=Ordinary and Partial Differential Equations, Vol IV, Proc. Twelfth Internat. Conf. (Dundee, Scotland,UK, June 1992)|editors=B. D. Sleeman and R. J. Jarvis|series=Pitman Research Notes in Math. Series|volume=289|publisher=Longman and Technical|publication-place=London|year=1993|pages=126&ndash;209}}

Revision as of 20:47, 29 December 2012

Mathematically ideal drums with membranes of these two different shapes (but otherwise identical) would sound the same, because the eigenfrequencies are all equal, so the timbral spectra would contain the same overtones. This example was constructed by Gordon, Webb and Wolpert. Notice that both polygons have the same area and perimeter.

To hear the shape of a drum is to infer information about the shape of the drumhead from the sound it makes, i.e., from the list of overtones, via the use of mathematical theory. "Can One Hear the Shape of a Drum?" was the witty title of an article by Mark Kac in the American Mathematical Monthly 1966 [1], but these questions can be traced back all the way to Hermann Weyl.

The frequencies at which a drumhead can vibrate depend on its shape. The Helmholtz equation tells us the frequencies if we know the shape. These frequencies are the eigenvalues of the Laplacian in the region. A central question is: can they tell us the shape if we know the frequencies? No other shape than a square vibrates at the same frequencies as a square. Is it possible for two different shapes to yield the same set of frequencies? Kac did not know the answer to that question.

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 λn the Dirichlet eigenvalues for D: that is, the eigenvalues of the Dirichlet problem for the Laplacian:

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 with clamped boundary.

Therefore the question may be reformulated as: what can be inferred on D if one knows only the values of λn? 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 manifolds, as well as for other elliptic differential operators such as the Cauchy–Riemann operator or Dirac operator. Other boundary conditions besides the Dirichlet condition, such as the Neumann boundary condition, can be imposed. See spectral geometry and isospectral as related articles.

The answer

Almost immediately, John Milnor observed that a theorem due to Ernst Witt implied the existence of a pair of 16-dimensional tori that have the same eigenvalues but different shapes. However, the problem in two dimensions remained open until 1992, when Gordon, Webb, and Wolpert constructed, based on the Sunada method, a pair of regions in the plane that have different shapes but identical eigenvaluesCite error: A <ref> tag is missing the closing </ref> (see the help page).

  • <ref>Brossard, Jean; Carmona, René (1986). "Can one hear the dimension of a fractal?". Comm. Math. Phys. 104 (1): 103–122. Bibcode:1986CMaPh.104..103B. doi:10.1007/BF01210795.<ref>

References

  1. ^ Kac, Mark (1966). "Can One Hear the Shape of a Drum?". American Mathematical Monthly. 73 (4, part 2): 1&ndash23. doi:10.2307/2313748. JSTOR 2313748. {{cite journal}}: Unknown parameter |month= ignored (help)
  • Buser, Peter; Conway, John; Doyle, Peter; Semmler, Klaus-Dieter (1994), "Some planar isospectral domains", International Mathematics Research Notices, 9: 391ff
  • Chapman, S.J. (1995), "Drums that sound the same", American Mathematical Monthly (February): 124–138
  • Giraud, Olivier (2010). "Hearing shapes of drums - mathematical and physical aspects of isospectrality". Reviews of Modern Physics. 82 (3): 2213–2255. arXiv:1101.1239. Bibcode:2010RvMP...82.2213G. doi:10.1103/RevModPhys.82.2213. {{cite journal}}: Unknown parameter |coauthors= ignored (|author= suggested) (help)
  • Gordon, Carolyn; Webb, David, "You can't hear the shape of a drum", American Scientist, 84 (January–February): 46–55
  • Gordon, C.; Webb, D.; Wolpert, S. (1992), "Isospectral plane domains and surfaces via Riemannian orbifolds", Inventiones Mathematicae, 110 (1): 1–22, Bibcode:1992InMat.110....1G, doi:10.1007/BF01231320
  • Ivrii, V. Ja. (1980), "The second term of the spectral asymptotics for a Laplace–Beltrami operator on manifolds with boundary", Funktsional. Anal. i Prilozhen, 14 (2): 25–34 (In Russian).
  • Lapidus, Michel L. (1991), "Can one hear the shape of a fractal drum? Partial resolution of the Weyl–Berry conjecture", Geometric analysis and computer graphics (Berkeley, CA, 1988), Math. Sci. Res. Inst. Publ. (17), New York: Springer: 119–126
  • Lapidus, Michel L. (1993), "Vibrations of fractal drums, the Riemann hypothesis, waves in fractal media, and the Weyl–Berry conjecture", Ordinary and Partial Differential Equations, Vol IV, Proc. Twelfth Internat. Conf. (Dundee, Scotland,UK, June 1992), Pitman Research Notes in Math. Series, vol. 289, London: Longman and Technical, pp. 126–209 {{citation}}: Unknown parameter |editors= ignored (|editor= suggested) (help)
  • Lapidus, Michel L.; Pomerance, Carl (1993), "The Riemann zeta-function and the one-dimensional Weyl-Berry conjecture for fractal drums", Proc. London Math. Soc. (3), 66 (1): 41–69, doi:10.1112/plms/s3-66.1.41
  • Lapidus, Michel L.; Pomerance, Carl (1996), "Counterexamples to the modified Weyl–Berry conjecture on fractal drums", Math. Proc. Cambridge Philos. Soc., 119 (1): 167–178, Bibcode:1996MPCPS.119..167L, doi:10.1017/S0305004100074053
  • Lapidus, M. L.; van Frankenhuysen, M. (2000), Fractal Geometry and Number Theory: Complex dimensions of fractal strings and zeros of zeta functions, Boston: Birkhauser. (Revised and enlarged second edition to appear in 2005.)
  • Milnor, John (1964), "Eigenvalues of the Laplace operator on certain manifolds", Proceedings of the National Academy of Sciences of the United States of America, 51: 542ff, Bibcode:1964PNAS...51..542M, doi:10.1073/pnas.51.4.542, PMC 300113, PMID 16591156
  • Sunada, T. (1985), "Riemannian coverings and isospectral manifolds", Ann. Of Math. (2), 121 (1): 169–186, doi:10.2307/1971195, JSTOR 1971195
  • Zelditch, S. (2000), "Spectral determination of analytic bi-axisymmetric plane domains", Geometric and Functional Analysis, 10 (3): 628–677, doi:10.1007/PL00001633

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