Topology, symmetry, and phase transitions in lattice gauge ... - tuprints
Topology, symmetry, and phase transitions in lattice gauge ... - tuprints
Topology, symmetry, and phase transitions in lattice gauge ... - tuprints
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
50 universal aspects of conf<strong>in</strong>ement <strong>in</strong> 2 + 1 dimensions<br />
Figure 3.19: Critical coupl<strong>in</strong>gs for 2 + 1 d SU(2) (N t = 4) from self-duality compared to<br />
those of Table 3.1, with N s up to 96 <strong>and</strong> the <strong>in</strong>f<strong>in</strong>ite-volume extrapolated result<br />
β c = 6.53658(16) shown as the narrow gray b<strong>and</strong> here.<br />
N s β c (F k = F e ) β c (F k = f I (0))<br />
12 6.53474(42) 6.51333(33)<br />
16 6.53627(36) 6.52508(13)<br />
24 6.53645(17) 6.5324(14)<br />
32 6.53672(24) 6.5346(23)<br />
w. av. N S = 24, 32 exp. (full set N s ≤ 96)<br />
6.53654(14) 6.53658(16)<br />
Table 3.3: Comparison of N t = 4 pseudo-critical critical coupl<strong>in</strong>gs β c (N t , N s ) for SU(2) <strong>in</strong><br />
2 + 1 d obta<strong>in</strong>ed us<strong>in</strong>g self-duality (with weighted mean) versus the <strong>in</strong>tersection<br />
of F k with its known universal value (with <strong>in</strong>f<strong>in</strong>ite volume extrapolation from the<br />
full set of N s <strong>lattice</strong>s). The <strong>in</strong>tersections F k = F e were obta<strong>in</strong>ed us<strong>in</strong>g a simultaneous<br />
l<strong>in</strong>ear fit.