Abstract
The discovery of connections between the distribution of energy levels of heavy nuclei and spacings between prime numbers has been one of the most surprising and fruitful observations in the twentieth century. The connection between the two areas was first observed through Montgomery’s work on the pair correlation of zeros of the Riemann zeta function. As its generalizations and consequences have motivated much of the following work, and to this day remains one of the most important outstanding conjectures in the field, it occupies a central role in our discussion below. We describe some of the many techniques and results from the past sixty years, especially the important roles played by numerical and experimental investigations, that led to the discovery of the connections and progress towards understanding the behaviors. In our survey of these two areas, we describe the common mathematics that explains the remarkable universality. We conclude with some thoughts on what might lie ahead in the pair correlation of zeros of the zeta function, and other similar quantities.
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- 1.
A total neutron cross section is defined as
$$\displaystyle\begin{array}{rcl} \frac{\mathrm{Number\ of\ events\ of\ all\ types\ per\ unit\ time\ per\ nucleus}} {\mathrm{Number\ of\ incident\ neutrons\ per\ unit\ time\ per\ unit\ area}},& & {}\\ \end{array}$$and has the dimensions of area (the standard unit is the barn, 10−24 cm2).
- 2.
The width, Γ, is related to the lifetime, τ, by the uncertainty relation Γ = h∕2π τ, where h is Planck’s constant. The finite width (lack of energy definition) is due to the fact that a resonant state can decay by emitting a particle, or radiation, whereas a state of definite energy must be a stationary state.
- 3.
If v is an eigenvector with eigenvalue \(\lambda\) of a Hermitian matrix A (so A = A ∗ with A ∗ the complex conjugate transpose of A, then v ∗(Av) = v ∗(A ∗ v) = (Av)∗ v); the first expression is \(\lambda \vert \vert v\vert \vert ^{2}\) while the last is \(\overline{\lambda }\vert \vert v\vert \vert ^{2}\), with \(\vert \vert v\vert \vert ^{2} = v^{{\ast}}v =\sum \vert v_{i}\vert ^{2}\) non-zero. Thus \(\lambda = \overline{\lambda }\), and the eigenvalues are real. This is one of the most important properties of Hermitian matrices, as it allows us to order the eigenvalues.
- 4.
In fact, one of the authors has used Weibull distributions to model run production in major league baseball, giving a theoretical justification for Bill James’ Pythagorean Won-Loss formula [103].
- 5.
Obviously this Weibull cannot be a normal distribution, as they have very different decay rates for large x, and this Weibull is a one-sided distribution! What we mean is that for 0 ≤ x ≤ 2 this Weibull is well approximated by a normal distribution which shares its mean and variance, which are (respectively) Γ(4∕3) ≈ 0. 893 and Γ(5∕3) −Γ(4∕3)2 ≈ 0. 105.
- 6.
In other words, while the above is enough to prove that the class number tends to infinity, we cannot use that argument to produce an explicit constant Q n for each n so that we could assert that the class number is at least n if q ≥ Q n . One of the best illustrations of the importance of effective constants is the following joke: There is a constant T 0 such that if all the non-trivial zeros of ζ(s) in the critical strip up to height T 0 are on the critical line, then they all are and the Riemann Hypothesis is true; in other words, it suffices to check up to a finite height! To see this, if the Riemann Hypothesis is true we may take T 0 to be 0, while if it is false we take T 0 to be 1 more than the height of the first exemption. We have therefore shown a constant exists, but such information is completely useless!
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Acknowledgements
The third named author was partially supported by NSF grant DMS1265673. We thank our colleagues and collaborators over the years for many helpful discussions on these and related topics. One of us (Miller) was fortunate to be a graduate student at Princeton, and had numerous opportunities then to converse with John Nash on a variety of mathematical topics. It was always a joy sitting next to him at seminars. We are grateful for his kind invitation to contribute to this work, and his comments on an earlier draft.
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Barrett, O., Firk, F.W.K., Miller, S.J., Turnage-Butterbaugh, C. (2016). From Quantum Systems to L-Functions: Pair Correlation Statistics and Beyond. In: Nash, Jr., J., Rassias, M. (eds) Open Problems in Mathematics. Springer, Cham. https://doi.org/10.1007/978-3-319-32162-2_2
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