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I study finite-temperature $\mathcal N=1$ super Yang-Mills for any gaugegroup $G=A_N, B_N, C_N, D_N, E_{6,7,8},F_4,G_2$, compactified from fourdimensions on a torus, $\mathbb R^2\times S^1_L\times S^1_{\beta}$. I examinein particular the low temperature regime $L\ll\beta=1/T$, where $L$ is thelength of the spatial circle with periodic boundary conditions and withanti-periodic boundary conditions for the adjoint gauginos along the thermalcycle $S^1_{\beta}$. For small such $L$ we are in a regime were semiclassicalcalculations can be performed and a transition occurs at $T_c$ much smallerthan $1/NL$. The transition is mediated by the competition betweennon-perturbative objects including 'exotic' topological molecules: neutral andmagnetic bions composed of BPS and KK monopole constituents, with $r=rank(G)$different charges in the co-root lattice of the gauge group $G$, and theperturbative electrically charged W-bosons (along with their winosuperpartners). I determine a duality to a double Coulomb gas of neutral andmagnetic bions of different charges of their constituent monopole-instantons,and W-bosons of both scalar and electric charges. Aharanov-Bohm interactionsexist between magnetic bions and W-bosons, and scalar charges of W-bosons andneutral bions attract like charges, as opposed to the magnetic and electriccharges where like charges repel. It is hoped in the future that latticestudies of this Coulomb gas can be done as in [1] for all gauge groups. It ishoped that a dual lattice 'affine' XY model with symmetry breakingperturbations can also be found in future studies of general gauge group asdone in [1] for $SU(2)$.

Deconfinement on $\mathbb R^2\times S^1_L\times S^1_{\beta}$ for all gauge groups and duality to double Coulomb Gas