Watch a finite cell rearrange until its short-range order matches the ideal random alloy.
α(shell) → 0 — i.e. it forces the small cell's
pair statistics to match a truly random alloy. This is a teaching analog; the paper's production SQS used
ICET, a 3-D FCC cell, 256 atoms, then was cut to a 4×4×6 (111) slab (96 atoms) with a pure-Pt skin.
Take the converged random arrangement as the bulk, cut a (111) slab, then replace the outermost layer with pure Pt.
A truly random alloy is infinite — we can't put it in DFT. An SQS is a small periodic cell chosen so its correlation functions match the random alloy for the most important short-range clusters.
The Warren–Cowley parameter αij = 1 − P(j|i)/cj measures deviation from random neighbours. Clustering gives α>0; ordering gives α<0. The search minimizes Σ α² over the nearest shells.
Metropolis Monte Carlo swaps two atoms and accepts good moves (and occasionally bad ones while "hot"). Cooling the temperature locks in the best-mixed, lowest-α configuration — the SQS.