Synthesizers for electronic music combine simple waves to create complex sounds. Similarly, we create quasiperiodic structures from simple sinusoidal waves. I presented a first attempt in the post “quasiperiodic designs from superposition of waves“. A more complete method is discussed here.

Somehow, I am trying to make up a Fourier series for quasiperiodic tilings. You can get a good idea about Fourier series from “An Intuitive Explanation of Fourier Theory” at http://cns-alumni.bu.edu/~slehar/fourier/fourier.html. Or have at least a look at the pictures if you don’t like the hard math.

We first look at periodic functions in one dimension. If we want mirror-symmetry at x=0 we can begin with a simple set of cosine functions f(x) = cos(k x). To get more details we can add higher harmonics

f(x)=a_1 cos(k x) + a_2 cos(2k x) + a_3 cos(3k x) + ...

Choosing the right coefficients a we can approximately synthesize any periodic mirror-symmetric function f(x). Here, the spatial frequencies of the waves correspond to periodically spaced points k, 2k, 3k, ….

In two dimensions periodic functions can be made up similarly. With

f(x,y)=cos(k x) + cos(k y)

we already have a square lattice with four-fold rotational symmetry. Adding higher harmonics gives

f(x,y)=a_10 [cos(k x)+cos(k y)] + a_11 [cos(kx+ky)+cos(kx-ky)] +a_20 [cos(2kx)+cos(2ky)] + ...

This can approximate the colors of any periodic picture with four-fold rotational symmetry. Now the frequencies form a square lattice with the points (k,0), (0,k), (k,k), (k,-k), (2k,0), (0,2k) and so on. It is important that all these waves fit to the basic wave and the corresponding square tessellation.

What changes for waves and functions that should fit to a quasiperiodic tiling of n-fold rotational symmetry ? As done in earlier posts, we can use a set of n cosine waves with the same size k for the frequencies. Their directions are regularly spaced. But this is simply a basic set and we might want to have higher “harmonics”. Then we know that their frequencies can not make a periodic lattice. Instead they are the corner points of a quasiperiodic tiling.

Take as an example eight-fold rotational symmetry. The basic set of waves is

f(x,y)=cos(kx)+cos[k(x+y)/sqrt(2)]+cos(ky)+cos[k(x-y)/sqrt(2)].

Their frequencies (k,0), (k/sqrt(2),k/sqrt(2), (0,k) and (k/sqrt(2),-k/sqrt(2)) already do not agree with a square lattice. Instead they are corner points of an Ammann-Beenker tiling with tiles of edge length equal to k. Thus we might use the Ammann-Beenker tiling to choose the frequencies for a synthesis of quasiperiodic structures and tilings with eight-fold rotational symmetry. At first sight we seem to running in circles.

Actually we get interesting new results. The point (k,0) lies at an obtuse angle of one of the eight rhombs making a star around (0,0). It is also a corner of a square. The diagonally opposed point of the square lies at ([1+sqrt(2)]k,0) and thus we have a set of waves with higher frequency

g(x,y)=cos([1+sqrt(2)]kx)+cos[k(x+y)[1+1/sqrt(2)]] +cos([1+sqrt(2)]ky)+cos[k(x-y)[1+1/sqrt(2)]],

which fits nicely with the basic waves f(x,y), see the figure below. Note that the frequencies are larger by the irrational factor (1+sqrt(2)). This is not at all “harmonic”.

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