  We introduce a new paradigm for one-dimensional uniform electron gases
(UEGs). In this model, $n$ electrons are confined to a ring and interact via a
bare Coulomb operator. We use Rayleigh-Schr\"odinger perturbation theory to
show that, in the high-density regime, the ground-state reduced (i.e. per
electron) energy can be expanded as $\eps(r_s,n) = \eps_0(n) r_s^{-2} +
\eps_1(n) r_s^{-1} + \eps_2(n) +\eps_3(n) r_s + \ldots$, where $r_s$ is the
Seitz radius. We use strong-coupling perturbation theory and show that, in the
low-density regime, the reduced energy can be expanded as $\eps(r_s,n) =
\eta_0(n) r_s^{-1} + \eta_1(n) r_s^{-3/2} + \eta_2(n) r_s^{-2} + \ldots$. We
report explicit expressions for $\eps_0(n)$, $\eps_1(n)$, $\eps_2(n)$,
$\eps_3(n)$, $\eta_0(n)$ and $\eta_1(n)$ and derive the thermodynamic
(large-$n$) limits of each of these. Finally, we perform numerical studies of
UEGs with $n = 2, 3, \ldots, 10$, using Hylleraas-type and quantum Monte Carlo
methods, and combine these with the perturbative results to obtain a picture of
the behavior of the new model over the full range of $n$ and $r_s$ values.
