See The $p$-adics and Related Concepts for notation and basics on the $p$-adic numbers, Introduction to Boltzmann Statistics for notation and background on electrostatics, and Basics of Probability for notation and background on probability and… Read More »Background
As in Two-Dimensional Electrostatics, the joint density of particles and partition function in the canonical ensemble are then given by $$f(N,\beta; \mathbf x) = \frac{1}{Z(N,\beta,\lambda)} \prod_{m<n} |x_n – x_m |^{\beta}; \qquad Z(N, \beta, \lambda) =… Read More »The $p$-adic Canonical Ensemble
We have one recurrence for $\widetilde Z(N, \beta, \lambda)$ but it involves a complicated combinatorial sum and a product involving $p$ different terms $\widetilde Z(n_j, \beta, \lambda)$. Here we demonstrate a simpler quadratic recurrence. Theorem:… Read More »Quadratic Recurrences for the Canonical Partition Function
See The Grand Canonical Ensemble for details about the general setup, but the basic idea distinguishing the canonical ensemble and the grand canonical ensemble is that in the latter we allow the number of particles… Read More »The $p$-adic Grand Canonical Ensemble
We take a brief detour to talk about some operations on power series that arise in calculations of probabilities in the grand canonical ensemble. We already saw an example of this when we computed the… Read More »The $Q$-Transform on Formal Power Series
See Point Processes for the general set up of the cylinder $\sigma$-algebra, but it suffices to say here that we are interested in computing probabilities of events of the form $\{N_{B_1} = n_1, \ldots, N_{B_M}… Read More »Probabilities of Cylinder Sets