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

8.24. It is a highly instructive exercise to cast Algorithm 8.5.2 into a detailed<br />

form that incorporates our brief overview and the various details from the<br />

literature (including the considerations of Exercise 8.23).<br />

A second task that lives high on the pedagogical ladder is to emulate a<br />

QTM with a standard TM program implementation, in a standard language.<br />

Of course, this will not result in a polynomial-time factorer, but only because<br />

the TM does what a QTM could do, yet the former involves an exponential<br />

slowdown. For testing, you might start with input numbers along the lines of<br />

Exercise 8.23. Note that one still has unmentioned options. For example, one<br />

could emulate very deeply and actually model quantum interference, or one<br />

could just use classical arithmetic and FFTs to perform the algebraic steps of<br />

Algorithm 8.5.2.<br />

8.8 Research problems<br />

8.25. Prove or disprove the claim of physicist D. Broadhurst that the number<br />

P = 29035682 ∞<br />

dx<br />

514269<br />

x906 <br />

sin(x ln 2) 1<br />

sinh(πx/2) cosh(πx/5) +8sinh2 <br />

(πx/5)<br />

0<br />

is not only an integer, but in fact a prime number. This kind of integral<br />

shows up in the theory of multiple zeta functions, which theory in turn has<br />

application in theoretical physics, in fact in quantum field theory (and we<br />

mean here physical fields, not the fields of algebra!).<br />

Since the 1st printing of the present book, Broadhurst has used a publicly<br />

available primality-proof package to establish that P is indeed prime. One<br />

research extension, then, is to find—with proof—an even larger prime having<br />

this kind of trigonometric-integral representation.<br />

8.26. Here we explore a connection between prime numbers and fractals.<br />

Consider the infinite-dimensional Pascal matrix P with entries<br />

<br />

i + j<br />

Pi,j = ,<br />

i<br />

for both i and j running through 0, 1, 2, 3, ...; thus the classical Pascal<br />

triangle of binomial coefficients has its apex packed into the upper-left corner<br />

of P , like so:<br />

⎛<br />

1 1 1 1<br />

⎞<br />

···<br />

⎜ 1<br />

⎜<br />

P = ⎜ 1<br />

⎜<br />

⎝ 1<br />

.<br />

2<br />

3<br />

4<br />

.<br />

3<br />

6<br />

10<br />

.<br />

4<br />

10<br />

20<br />

.<br />

··· ⎟<br />

··· ⎟<br />

··· ⎠<br />

. ..<br />

.<br />

There are many interesting features of this P matrix (see [Higham 1996, p.<br />

520]), but for this exercise we concentrate on its fractal structure modulo<br />

primes.<br />

Define the matrix Qn = P mod n, where the mod operation is taken<br />

elementwise. Now imagine a geometrical object created by coloring each zero

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