Here are some unsolved mathematical problems with potential impact for neuroscience. Not all are tightly posed. Any feedback, not limited to brilliant ideas, is always appreciated and will be gratefully acknowledged.
spike metrics
multidimensional scaling of symmetric non-Euclidean spaces
nonlinear dynamics
isodipole textures
point processes
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Last revised: 3/15/07
Progress (8/2002) for combinations of Dspike and Dinterval: Perhaps any optimal path from spike train A to spike train B can be reorganized as an equal-cost path from spike train A to spike train X, then from X to B, in which A to X only uses the transformations of Dspike, and X to B only uses the transformations of Dinterval. Then, find a DP algorithm that finds X. Unfortunately, such reorganizations cannot be guaranteed. This idea makes use of the "algebraic" properties of the transformations. For general inspiration, see the algebraic dynamic programming work of Robert Giegerich.
I had hypothesized that for p = 1/2, one can always achieve an embedding with Euclidean geometry. (It is easy to show that p <= 1/2 is required for large q, and that p = 1 suffices for q = 0.) p = 1/2 also seemed plausible because a lattice of points in the Minkowski city block space -- which appears to be related to the spike time metric -- can be embedded in a Euclidean space with F(x)=x1/2, in a manner that preserves the metric. (For a k-dimensional lattice of N1N2...Nk points, then the dimension of the Euclidean space need be no larger than N1+N2+...+Nk-k. My interest is that the embedding requires a uniform power law transformation, independent of the number of points. This is not always possible for a non-euclidean manifold. The more general question of when a non-Euclidean manifold can be embedded in a distance-preserving (up to a power law transformation) manner in a Euclidean space, is an interesting one -- see multidimensional scaling of symmetric non-Euclidean spaces below.)
But it now (7/2000) is clear, due to the work of Dmitriy Aronov, that no exponent p>0 can guarantee a Euclidean embedding of a set of spike trains under the spike time metric. See the paper. Also, see this news flash.
Thus it would seem that no universal scale-free transformation of the distance suffices to embed the space of the spike time distance into Euclidean space.
It is well known that a Riemannian manifold can be embedded in a higher-dimensional Euclidean space in a topology-preserving manner. Here we ask about whether it is possible to find an embedding of a Riemannian manifold that preserves, or almost preserves, distance. That is, the geodesic distance between two points a and b, d(a,b), is required to be equal to some function of the Euclidean distance between the embedded images z(a) and z(b) of the points, namely, d(a,b)=F(|z(a)-z(b)|). So that the transformation is scale-free (as discussed above), we require F(x)=xp. We are interested in finding a power p that is independent of the number of points within the manifold to be embedded, an are not concerned whether the number of dimensions is finite or infinite.
Consider: (i) The Poisson process is often taken to be a good starting place for modeling spike trains. (ii) Spike trains from functionally related neurons are often positively or negatively correlated at short lags. But is it possible to construct a pair of point processes, each of which is Poisson when viewed in isolation, whose cross-correlation is negative at short lags? If it is impossible, can this be proven?
Note that it is easy to construct Poisson processes that are positively correlated at short lags. Two strategies:
(3/2001) Daniel Fisher.
His solution (which is a generalization of the second strategy above) is given here:
The A-to-B point process has
interval distribution
S=y[(a-1)2e-t + ((g-1)2-(a-1)2)e-gt - (g-1)(g-a)2t e-gt] with y=(g/a(g-1))2
and the B-to-A point process has interval distribution
R=z[delta(t) + (2(g-a) + (g-a)2t)e-at] with z=(a/g)2.
Take g > a > 1 with ln(g-a) - ln(a-1) < 1+ (a-1)/(g-a).
These conditions ensure that both R(t) and S(t) are positive and that the cross correlation (with mean subtracted)
has a minimum value
- (1-1/a) e-2/(g-a)
that is negative. By choosing both g and a large, one can get this minimum arbitrarily close to
-1. With these forms, the cross-correlation has a delta function component at t=0, is
large for small t, dips below zero for larger t and asymptotically
approaches zero from below for large t.
(3/15/07) An extensive analysis of these constructions, and of alternating Poisson processes in general, has been posted by Don Johnson. Download it.
Contributed (8/12/2002) by Dario Ringach: Griffiths et al., "Aspects of correlation in bivariate Poisson distributions and processes", Aust. J. Statist. 21, 238-255 (1979)