Abstract
Some key points out of my recent study of the characteristic features of the small ( x ⪡ 1), intermediate ( x ⋍ 1) and large ( x ⪢ 1) Leutwyler-Smilga regimes for QCD-type theories in a finite volume ( x = VΣ m) are presented, and a few immediate consequences for full QCD simulations are discussed.
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