Self-duality and local chirality as a function of temperature

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Plan

We will generate a set of ensembles with lattices of size $$20^3\times N_t$$, where $$N_t=4, 6, 7, 8, 9, 10, 12, 20$$ and lattice spacing $$a=0.085\,{\rm fm}$$. These will correspond to temperatures of $$579$$, $$386$$, $$331$$, $$290$$, $$258$$, $$232$$, $$193$$, and $$116\,{\rm MeV}$$. We will then scan the temperature going from the confined to the de-confined phase, the transition for pure-glue theory being expected at $$T_c\approx 277\,{\rm MeV}$$ (to get this result we used $$T_c/\sqrt{\sigma}=0.631(2)$$, from hep-lat/9706006 where $$\sigma=(440\,{\rm MeV})^2$$ is the string tension).

Ensemble Size T[MeV] $$N_\text{config}$$ $$\Lambda_\text{low}^\text{ave}$$ for $$p=1$$ $$\Lambda_\text{high}^\text{ave}$$ for $$p=1$$ $$\Lambda_\text{low}^\text{ave}$$ for $$p=2$$ $$\Lambda_\text{high}^\text{ave}$$ for $$p=2$$
AZ1 $$16^4$$ 145 101 87 1889 137 1887
AZ2 $$20^4$$ 116 101 37 1423 58 1421
AZ3 $$24^4$$ 97 101 17 1100 28 1097
AZ4 $$32^4$$ 72 101 8 673 11 670
AT1 $$20^3\times 12$$ 193 201 58 1680 91 1678
AT2 $$20^3\times 10$$ 232 201 68 1778 109 1776
AT3 $$20^3\times 9$$ 258 201 71 1836 116 1834
AT4 $$20^3\times 8$$ 290 401 94 1903 151 1901
AT5 $$20^3\times 7$$ 331 401 518 2002 630 2000
AT6 $$20^3\times 6$$ 386 101 904 2143 956 2141
AT7 $$20^3\times 4$$ 579 101 1800 2697 1838 2694


To generate these lattices we use Wilson gauge action with $$\beta=6.054$$. We determined this coupling using a non-perturbative parametrization for lattice spacing (see Lattice spacing). We used heat-bath with over-relaxation; at each step we did 5 heat-bath hits and 9 over-relaxation updates. We thermalized the configuration for 2000 steps and save a lattice every 200 steps. We generated 100 configs for each ensemble.

Update: The temperature scale used above, based on the string tension, is not very accurate. In our paper we used $$r_0 T_c= 0.7498(50)$$ value determined by Silvia Necco to set the scale. A more recent determination of the critical coupling $$\beta_c$$ as a function of the temporal lattice size was carried out by Mikko Laine and collaborators. For $$N_t=8$$ the determine $$\beta_c=6.06239(38)$$.