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428 Chapter 8 THE UBIQUITY OF PRIME NUMBERS<br />

say at n = N, then one expects 2N complex zeros of the resulting, degree-<br />

2N polynomial in x. But in practice, only some of these 2N zeros are real<br />

(i.e., such that 1<br />

2 + ix is on the Riemann critical line). For large N, and<br />

again experimentally, the rest of the polynomial’s zeros are “expelled” a good<br />

distance away from the critical line. The Riemann hypothesis, if it is to be<br />

cast in language appropriate to the Hermite expansion, must somehow address<br />

this expulsion of nonreal polynomial zeros away from the real axis. Thus<br />

the Riemann hypothesis can be cast in terms of quantum dynamics in some<br />

fashion, and it is not out of the question that this kind of interdisciplinary<br />

approach could be fruitful.<br />

An anecdote cannot be resisted here; this one concerns the field of<br />

engineering. Peculiar as it may seem today, the scientist and engineer van<br />

der Pol did, in the 1940s, exhibit tremendous courage in his “analog”<br />

manifestation of an interesting Fourier decomposition. An integral used by<br />

van der Pol was a special case (σ =1/2) of the following relation, valid for<br />

s = σ + it, σ ∈ (0, 1) [Borwein et al. 2000]:<br />

∞<br />

ζ(s) =s e<br />

−∞<br />

−σω (⌊e ω ⌋−e ω ) e −iωt dω.<br />

Van der Pol actually built and tested an electronic circuit to carry out the<br />

requisite transform in analog fashion for σ =1/2, [van der Pol 1947]. In today’s<br />

primarily digital world it yet remains an open question whether the van der<br />

Pol approach can be effectively used with, say, a fast Fourier transform to<br />

approximate this interesting integral. In an even more speculative tone, one<br />

notes that in principle, at least, there could exist an analog device—say an<br />

extremely sophisticated circuit—that sensed the prime numbers, or something<br />

about such numbers, in this fashion.<br />

At this juncture of our brief interdisciplinary overview, a word of caution<br />

is in order. One should not be led into a false presumption that theoretical<br />

physicists always endeavor to legitimize the prevailing conjectural models of<br />

the prime numbers or of the Riemann ζ function. For example, in the study<br />

[Shlesinger 1986], it is argued that if the critical behavior of ζ corresponds to<br />

a certain “fractal random walk” (technically, if the critical zeros determine a<br />

Levy flight in a precise, stochastic sense), then fundamental laws of probability<br />

are violated unless the Riemann hypothesis is false.<br />

In recent years there has been a flurry of interdisciplinary activity—<br />

largely computational—relating the structure of the primes to the world<br />

of fractals. For example, in [Ares and Castro 2004] an attempt is made to<br />

explain hidden structure of the primes in terms of spin-physics systems and<br />

the Sierpiński gasket fractal; see also Exercise 8.26. A fascinating approach<br />

to a new characterization of the primes is that of [van Zyl and Hutchinson<br />

2003], who work out a quantum potential whose eigenvalues (energy levels)<br />

are the prime numbers. Then they find that the fractal dimension of said<br />

potential is about 1.8, which indicates surprising irregularity. We stress that<br />

such developments certainly sound theoretical on the face of it, and some of

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