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
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3.6 exploit<strong>in</strong>g self-duality 51<br />
N t ω from F k = F e offset red. χ 2 ω from β c (N t , N s ) extrap. red. χ 2<br />
2 1.61(9) 0.78 1.34(12) 0.83<br />
3 1.53(25) 0.36 1.16(50) 0.21<br />
4 1.54(7) 1.52 1.47(6) 0.98<br />
Table 3.4: SU(2) correction to scal<strong>in</strong>g exponents obta<strong>in</strong>ed from the offset of F k = F e from<br />
the universal value f I (0) (left) <strong>and</strong> from the extrapolations of pseudo-critical<br />
coupl<strong>in</strong>gs <strong>in</strong> Section 3.4.3, together with the reduced χ 2 of the fits that they were<br />
extracted from.<br />
comparison with the values for ω obta<strong>in</strong>ed as a fit parameter <strong>in</strong> our extrapolations<br />
of pseudo-critical coupl<strong>in</strong>gs β c (N t , N s ) <strong>in</strong> Section 3.4.3 from universality alone. Exploitation<br />
of self-duality to s<strong>in</strong>gle out the scal<strong>in</strong>g correction yields a more consistent<br />
estimate for ω between various values of N t , <strong>and</strong> is therefore the preferred method.