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Primon gas

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In mathematical physics, the primon gas or free Riemann gas is a toy model illustrating in a simple way some correspondences between number theory and ideas in quantum field theory and dynamical systems. The idea of the primon gas is attributed to Bernard Julia [1]

The model

Consider a simple quantum Hamiltonian H having eigenstates labelled by the prime numbers p, and having energies <ath>\log p</math>. That is,

with

The second-quantized version of this Hamiltonian converts states into particles, the primons. A multi-partcile state is denotedby a natural number n as

The labelling by the integer n is unique, since every prime number has a unique factorization into primes. The energy of such a multi-particle state is clearly .

The statistical mechanics partition function is given by the [[Riemann zeta function]]:

after identifying where is Boltzmann's constant and T is the temperature.

The supersymmetric model

The above second-quantized model takes the particles to be bosons. If the particles are taken to be fermions, then the [[Pauli exclusion principle]] prohibits multi-particle states which include squares of primes. By the spin-statistics theorem, field states with an even number of particles are bosons, while those with an odd number of particles are fermions. The fermion operator (−1)F has a very concrete realization in this model as the Mobius function , in that the Mobius function is positive for bosons, negative for fermions, and zero on exclusion-principle-prohibited states.

More complex models

The analogy can be somewhat further extended in topological field theory and K-theory, where prime ideals take the role of the prime numbers, the group representations take the role of integers, group characters taking the place the [[Dirichlet character]]s, and so on.

References

  1. ^ Bernard L. Julia, Statistical theory of numbers, in Number Theory and Physics, eds. J. M. Luck, P. Moussa, and M. Waldschmidt, Springer Proceedings in Physics, Vol. 47, Springer-Verlag, Berlin, 1990, pp. 276-293.