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and L$_{t}$ is sufficiently large. The corresponding effective paramet ers are tabulated in Tabs. II, III and IV. The fits always give reasonable χ $^{2}$/DOF , which are shown in the last four columns, one for each observable. We note that as β becomes smaller, µ (0) c becomes larger while µ (1) c − µ (0) c becomes smaller. This is the reason it becomes difficult to ma tch the data to an effective quantum mechanics description at small β without going to very large L$_{t}$ . Note also that the value of µ (0) c has approximately reached the thermodynamic limit at β = 0 . 2 for L = 8 . We plot our four observables near µ (0) c at L = 16 and β = 0 . 43 in Fig. 6 and at L = 6 and β = 0 . 2 in Fig. 7 along with the fits. 

