the Weyl-Berry-Lapidus conjectures
Here's a quick overview from John Baez
[sci.physics.research, 13 Dec 1996]:
In Kac's classic "can you hear the shape of drum?" puzzle you are
trying to reconstruct the geometry of a n-dimensional manifold
(possibly with boundary) from the eigenvalues of the Laplacian on that
manifold.
In lowbrow lingo, you're trying to figure out a shape
knowing the resonant frequencies at which it vibrates.
It's been known
ever since Weyl that you can figure out a bunch of interesting stuff
about the shape, which is why the puzzle is interesting. But recently
two 2-dimensional regions in the plane with different shapes were
discovered that have the same eigenvalues. (See Gorden, Webb, and
Wolpert, Bull. AMS 27 (1992), 134.) One says they are
"isospectral".
So no, you can't hear the shape of a drum! What about higher
dimensions? Well, actually some counterexamples in higher dimensions
were known before the 2d counterexamples. But it seems clear that from
the 2d counterexamples you can get counterexamples in all higher
dimensions. Just take the 2d shapes and take their cross product with
a fixed n-dimensional shape, like an n-dimensional torus.
By separation of variables the eigenvalues of the Laplacian on a 2d
shape determine the eigenvalues of the Laplacian on its cross product
with an n-dimensional torus so we obtain two different
(n+2)-dimensional shapes whose Laplacians have the same
eigenvalues.
[Someone subsequently asked "what other interesting stuff can be
deduced from the spectrum?"]
There will be lots of eigenvalues of the Laplacian, or resonant
frequencies, so let N(x) be the number of eigenvalues
less than x. N(x) grows asymptotically like
xn/2 where n is the dimension of
the drumhead. So the easiest thing to spot is the dimension of
the drumhead. Say that
N(x) = A x
n/2 + smaller error terms.
Then from the constant A you can figure out the area of
the drumhead. (Well, the term "area" is appropriate if the dimension
n is 2. If n = 3 we'd call it the volume, and so on.
Anyway, we can figure out how big the drumhead is.) But then there
are little correction terms to the above formula. If the boundary of
the drum is reasonably smooth, a more accurate formula is
N(x) = A xn/2 +
B x(n-1)/2 + smaller error terms
From the constant B you can figure out the length of the
boundary of the drumhead. (Well, the term "length" is appropriate
if the dimension n is 2. If n = 3 we'd call it the area,
and so on.) There is something called the Weyl-Berry conjecture about
what happens when the boundary of the drumhead is a fractal! Suppose
the drumhead has fractal dimension D. Then the Weyl-Berry
conjecture is that we should replace the above formula with
N(x) = A xn/2 +
B xD/2 + smaller error terms
My colleague here at UCR, Michel Lapidus, works on this sort of
thing. One of the subtleties is that there are different concepts of
"fractal dimension". The most well-known one, the Hausdorff
dimension, does not make the Weyl-Berry conjecture come out to be
universally valid: there are counterexamples. The Minkowski dimension
seems to work better, but as far as I know, the whole subject of drums
with fractal boundary becomes more and more complicated, the closer
and closer you look at it...
What else can you figure out? Well, if you generalize the problem a
bit and look at the eigenvalues of the Laplacian not on functions but
on p-forms, you can figure out a lot about the topology
of the drum, using de Rham theory. To be precise, you can figure out
its Betti numbers.
There is probably a lot more you can figure out, but I don't know
exactly what it is! For example, what do the still smaller correction
terms in the asymptotic formula above mean?...And what about
information obtained, not from the behavior
N(x) as x tends to infinity, but the from the
first few eigenvalues? I'm pretty sure they study this a bit in the
subject of "spectral geometry"...
The "Weyl conjecture" first appeared in the following article:
H. Weyl, "Uber die Abhangigkeit der Eigenschwingungen einer Membran
von deren Begrenzung", J. Angew. Math. 141 (1912) 1-11.
It concerned the asymptotic behaviour of the spectrum of eigenvalues
of the Laplacian on an open bounded subset of Rn
with "sufficiently smooth" boundary.
Here is an excerpt from M. Lapidus's survey article "Vibrations of
fractal drums, the Riemann hypothesis, waves in fractal media, and the
Weyl-Berry conjecture":

Berry, as a physicist motivated in part by the study of porous media
and the scattering of light from fractal surfaces,
then extended this to what became known as the Weyl-Berry conjecture
in the following papers:
M.V. Berry, "Distribution of modes in fractal resonators", from
Structural Stability in Physics (ed. W. Guttinger and H.
Eikemeier, Springer, Berlin, 1979) 51-53.
M.V. Berry, "Some geometric aspects of wave motion: wavefront
dislocations, diffraction catastrophes, diffractals", Geometry of
the Laplace Operator (eds. R. Osserman and A. Weinstein) Proceedings
of Symposia in Pure Mathematics 36 (AMS, 1980) 13-38.
This deals with the analogous problem of the spectral asymptotics
of the Laplacian, but on an open subset with fractal rather
than smooth boundary. Here is a further excerpt from the Lapidus
survey:

The Weyl-Berry conjecture, in its original form, was ultimately
disproved (by counterexample) in:
J. Brossard and R. Carmona, "Can one hear the dimension of a fractal",
Communications in Mathematical Physics 104 (1986) 103-122
The authors suggested that the Minkowski dimension was more appropriate
than the Hausdorff dimension for the boundary.
Lapidus reformulated the Weyl-Berry conjecture in
M.L. Lapidus, "Fractal drum, inverse spectral problems of elliptic
operators and a partial resolution of the Weyl-Berry conjecture",
Transactions of the American Mathematical Society 325
(1991) 465-529.

In this paper, Lapidus obtains a partial resolution of the
Weyl-Berry conjecture by establishing (in any dimension n
>1) remainder estimates for the asymptotics
of the eigenvalue counting function, expressed in terms of the
Minkowski (or box) dimension of the boundary. These estimates are
valid for Laplacians with Dirichlet or (under suitable hypotheses)
Neumann boundary conditions, and are also extended to higher order
elliptic operators (with possibly nonsmooth coefficients). Further,
families of examples are provided to show that these estimates are
sharp in any possible "fractal" (i.e., Minkowski) dimension.
In the following papers, the authors prove the case for n = 1
and establish unexpected and intruiging connections with the Riemann
zeta function:
M.L. Lapidus and C. Pomerance, "Fonction zeta de Riemann et conjecture de
Weyl-Berry pour les tambours fractals", C. R. Acad. Sci. Paris Ser. I
Math. 310 (1990) 343-348.
M.L. Lapidus and C. Pomerance, "The Riemann zeta-function and the
one-dimensional Weyl-Berry conjecture for fractal drums", Proceedings of
the London Mathematical Society (3) 66 (1993) 41-69.
"Based on his earlier work on the vibrations of 'drums with fractal
boundary', the first author has refined M.V. Berry's conjecture that
extended from the 'smooth' to the 'fractal' case H. Weyl's conjecture
for the asymptotics of the eigenvalues of the Laplacian on a bounded
open subset of Rn. We solve here in the
one-dimensional case (that is n = 1) this 'modified Weyl-Berry
conjecture'. We discover, in the process, some unexpected and
intriguing connections between spectral geometry, fractal geometry
and the Riemann zeta-function. We therefore show that one can 'hear'
(that is, recover from the spectrum) not only Minkowski fractal
dimension of the boundary - as was established previously by the
first author - but also, under the stronger assumptions of the
conjecture, its Minkowski content (a 'fractal' analogue of its
'length')."
In the following paper, the authors disprove the modified Weyl-Berry
conjecture for n > 1:
M.L. Lapidus and C. Pomerance, "Counterexamples to the modified Weyl-Berry
conjecture on fractal drums", Mathematical Proceedings of the Cambridge
Philosophical Society 119 (1996) 167-178.
The two families of counterexamples given suggest that to determine
the spectrum, more geometry of the drum is needed than just its volume
and the Minkowski dimension and content of its boundary.
M. Kac, "Can one hear the shape of a drum?", American Mathematical
Monthly (Slaught Memorial Papers No. 11) 73 (1966) 1-23.
B.D. Sleeman and Chen Hua, "An analogue of Berry's conjecture for
the phase in fractal obstacle scattering", IMA Journal of Applied
Mathematics 49 (1992) 193-200
B.D. Sleeman and Chen Hua, "The modified Weyl-Berry conjecture"
(preprint, 1991)
The following extensive survey contains probably the best
introduction to the history of these conjectures:
M.L. Lapidus, "Vibrations of fractal drums, the Riemann Hypothesis,
waves in fractal media, and the Weyl-Berry conjecture", in: Ordinary
and Partial Differential Equations (B.D. Sleeman and R.J. Jarvis,
eds.), vol. IV, Proc. Twelfth Internat. Conf. (Dundee, Scotland,
UK, June 1992), Pitman Research Notes in Math. Series 289
(Longman Scientific and Technical, 1993) 126-209.
This also documents an intriguing analogy between dynamical zeta
functions on hyperbolic manifolds and spectral zeta functions on
regions with fractal boundary.
In Part II of the above survey paper, are also formulated various
forms of the WBL conjectures in the important special cases of drums
with (approximately or possibly random) self-similar boundaries. In
particular, one has the following dichotomy: In the "nonlattice case"
(the generic case), the asymptotic second term of the eigenvalue
counting function N(x) is conjectured to be monotonic (and proportional
to xD/2), whereas in the "lattice case" (roughly
speaking, when the self-similar boundary has a large set of symmetries),
it is expected to be oscillatory, in a specific sense. (A sample of
references on work towards the above conjectures for drums with
self-similar boundary can be found, for example, in various places
in the book Fractal Geometry and Number Theory by M.L. Lapidus and
M. van Frankenhuysen.)
In that same survey paper by Lapidus, parallel conjectures are formulated
for drums with self-similar membranes, that is, for Laplacians on self-similar
fractals themselves rather on bounded open sets with self-similar boundaries.
These conjectures are specified (by means of a suitable notion of "spectral
dimension") and established in the following paper:
J. Kigami and M.L. Lapidus,
"Weyl's problem for the spectral distribution of Laplacians on p.c.f.
self-similar fractals", Commun. Math. Phys. 158 (1993), 93-125.
The partial analogue of Weyl's asymptotic formula for Laplacians on self-similar
fractals obtained in the above paper was significantly strengthened in the following
two papers:
M.L. Lapidus, "Analysis on fractals, Laplacians on self-similar sets,
noncommutative geometry and spectral dimensions", Topological Methods in Nonlinear
Analysis 4 (1994), 137-195.
J. Kigami and M.L. Lapidus, "Self-similarity of volume measures for Laplacians
on p.c.f. self-similar fractals", Commun. Math. Phys. 217 (2001), 165-180.
In the first of these papers, were constructed, by means of methods from operator
algebras and noncommutative geometry, (spectral) "volume measures" for fractals, viewed
in an important special case as an analogue on fractals of Riemannian volume measure.
In the second paper, for a smaller class of self-similar fractals, theses volume measures
were precisely identified and shown to be self-similar. In particular, for the homogeneous
Sierpinski gasket, this measure coincides with the natural Hausdorff measure on the fractal;
in general, however, it is different from it.
An important question: Lapidus and Pomerance unexpectedly related the (modified)
Weyl-Berry conjecture to the Riemann zeta function. Berry's best
known work links the zeta function and quantum chaos, and isn't
obviously linked to the Weyl-Berry conjecture. Is this further
Berry-zeta connection merely coincidental, or does it all stem from the
same root (spectral asymptotics)?
Lapidus provided the following answer:
"It is somewhat amusing that there does not seem to be any direct connection
between Michael Berry's work on the statistical distribution of the Riemann
zeros and the link with the Riemann zeta function discovered in the process
of resolving the modified Weyl-Berry conjecture in dimension 1. In
particular, the connection with the Riemann hypothesis discovered in my work
with Helmut Maier is completely independent. Indeed, the study of the
statistical distribution usually requires as a prerequisite that the Riemann
hypothesis is true.
Of course, there may be some interesting links between the general problem
of understanding the oscillations occurring in my work with Helmut Maier and
in the theory of complex dimensions developed in my joint book with Machiel
van Frankenhuysen. Michael Berry and I have discussed this issue on several
occasions and I have also thought about this for other reasons. (Most of my
heuristic conclusions about this very difficult problem are unpublished but
some comments are made about the possible connections between our theory of
complex dimensions of fractals and a (yet to be defined precisely, in
dimension larger than 2) dynamical system associated with fractal drums; see
section 10.4.3 (as well as 10.4.2) entitled "spectrum and periodic orbits"
of my joint book (with M-vF) "Fractal Geometry and Number Theory".
In summary, the answer to your question is "no". However, in the future, one
may discover a nice dynamical interpretation of our 'explicit formulas' and
of my (joint) reformulation of the Riemann Hypothesis. Hence, potentially,
one may eventually establish a link with the random matrix theoretic
approach to the statistical distribution of the Riemann zeros. For the
moment, however, this is out of reach and it is fair to say that the
subjects are totally distinct (and motivated by very different problems)
even though they both attempt to gain new information about different
aspects of the Riemann zeros."
[later note] "...some discussion of possible relations between the theory
of complex dimensions developed in the above-mentioned book Fractal Geometry
and Number Theory and some of the work on quantum chaos (including that
by Michael V. Berry) is given in Chapter 10 of that book (especially, Section 10.4).
I now have some further ideas on how these connections might occur but they are yet
to be written up..."
M.L. Lapidus and H. Maier, "Hypothese de Riemann, cordes fractales vibrantes
et conjecture de Weyl-Berry modifiee", C. R. Acad. Sci Paris Ser. I Math.
313 (1991) 19-24.
(Abstract) "Jointly with C. Pomerance, the first author has recently proved in
dimension one the "modified Weyl-Berry conjecture" formulated in his
earlier work on the vibrations of fractal drums. Here, we show, in
particular, that (still in dimension one) the converse of this
conjecture is not true in the "midfractal" case and that it is
true everywhere else if and only if the Riemann hypothesis is
true. We thus obtain a new characterization of the Riemann hypothesis
by means of a inverse spectral problem."
"As was the first author's hope at the beginning of his investigations
connecting fractal and spectral geometry with aspects of analytic
number theory, the above spectral characterization of the Riemann
hypothesis may shed new light on aspects of the theory of the Riemann
zeta-function."
See also the longer, related, paper:
M.L. Lapidus and H. Maier, "The Riemann hypothesis and inverse spectral
problems for fractal strings", Journal of the London Mathematical
Society (2) 52 (1995),
15-34.
By means of a suitable notion of generalised Minkowski content, many of the
above results (by Lapidus, Lapidus and Pomerance, as well as Lapidus and Maier)
were extended in the following papers to the situation where the fractality of
the boundary is governed by more general "gauge functions" than the usual power laws:
C.Q. He and M.L. Lapidus, "Generalized Minkowski content and the vibrations of
fractal drums and strings", Mathematical Research Letters 3 (1996) 31-40.
C.Q. He and M.L. Lapidus, "Generalized Minkowski content, spectrum of fractal drums,
fractal strings and the Riemann zeta function", Memoirs of the AMS
No. 608, 127 (1997), 1-97.
Moreover, mainly in the one-dimensional case, partly motivated by the above joint
works of Lapidus with Pomerance and with Maier, a detailed theory of complex
dimensions of fractal strings (defined as the poles of suitably defined 'geometric zeta
functions') was recently developed in the following book:
M.L. Lapidus and M. van Frankenhuysen, Fractal
Geometry and Number Theory: Complex dimensions of fractal strings and
zeros of zeta funtions, research monograph,
(Birkhauser, Boston, 2000).
In particular, a precise description of the geometric and spectral oscillations
of fractal strings is obtained in terms of the underlying complex dimensions via
suitable 'explicit formulas' (in the sense of number theory, but more general). Further,
the characterization of the Riemann hypothesis obtained by Lapidus and Maier is placed
in a broader and more conceptual framwork by means of the notion of complex
dimension, and is extended to a class of Dirichlet series including all those for which
Riemann's conjecture is expected to be true. Also, some new results concerning the vertical
ditribution of the zeros of Dirichlet series (including the Riemann zeta
function) are obtained via a detailed study of the interplay between the geometric and
spectral oscillations of certain generalized Cantor strings. Further references related
to this subject include:
M.L. Lapidus and M. van Frankenhuysen, "Complex dimensions of
fractal strings and oscillatory phenomena in fractal geometry and arithmetic", in:
Spectral Problems in
Geometry and Arithmetic (T. Branson, ed.), Contemporary Mathematics 237,
(AMS, 1999) 87-105.
M.L. Lapidus and M. van Frankenhuysen, "A prime number theorem for self-similar
flows and Diophantine approximation", in: Dynamical, Spectral and Arithmetic
Zeta Functions (M.L. Lapidus and M. van Frankenhuysen, eds.), Contemporary
Mathematics (AMS, 2001) (in press).
M.L. Lapidus and M. van Frankenhuysen, "Complex dimensions of self-similar fractal
strings and Diophantine approximation", preprint, June 2001.
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