# Ion friction at small values of the Coulomb logarithm

## TL;DR

This study investigates ion collision rates in strongly-coupled plasmas with small Coulomb logarithms using experiments on ultracold neutral plasmas and simulations, challenging traditional kinetic theories.

## Contribution

It provides the first experimental measurements and simulations of ion collisions in strongly-coupled plasmas at small Coulomb logarithms, using dual-species ultracold neutral plasmas.

## Key findings

- Strong collisional coupling observed between ion species.
- Good agreement between experiments and simulations.
- Potential for testing kinetic theory expressions for Coulomb logarithms.

## Abstract

Transport properties of high-energy-density plasmas are influenced by the ion collision rate. Traditionally, this rate involves the Coulomb logarithm, $\ln\Lambda$. Typical values of $\ln\Lambda$ are $\approx 10~\mbox{to}~20$ in kinetic theories where transport properties are dominated by weak-scattering events caused by long-range forces. The validity of these theories breaks down for strongly-coupled plasmas, when $\ln\Lambda$ is of order one. We present measurements and simulations of collision data in strongly-coupled plasmas when $\ln\Lambda$ is small. Experiments are carried out in the first dual-species ultracold neutral plasma (UNP), using Ca$^+$ and Yb$^+$ ions. We find strong collisional coupling between the different ion species in the bulk of the plasma. We simulate the plasma using a two-species fluid code that includes Coulomb logarithms derived from either a screened Coulomb potential or a the potential of mean force. We find generally good agreement between the experimental measurements and the simulations. With some improvements, the mixed Ca$^+$ and Yb$^+$ dual-species UNP will be a promising platform for testing theoretical expressions for $\ln\Lambda$ and collision cross-sections from kinetic theories through measurements of energy relaxation, stopping power, two-stream instabilities, and the evolution of sculpted distribution functions in an idealized environment in which the initial temperatures, densities, and charge states are accurately known.