Influence of the Effective Potential on the Crossover Width in the Two Flavor Polyakov-Nambu-Jona-Lasinio Model

<table class="figure-group"><tr class="fig-image" id="a"><td><object data="https://static.hindawi.com/articles/ahep/volume-2020/6760547/figures/6760547.fig.002a.svgz" name="6760547.fig.002a" type="image/svg+xml"></object></td></tr><tr class="fig-caption"><td><b>(a) </b>Chiral condensate</td></tr><tr class="fig-image" id="b"><td><object data="https://static.hindawi.com/articles/ahep/volume-2020/6760547/figures/6760547.fig.002b.svgz" name="6760547.fig.002b" type="image/svg+xml"></object></td></tr><tr class="fig-caption"><td><b>(b) </b>Polyakov loop</td></tr><tr class="fig-image" id="c"><td><object data="https://static.hindawi.com/articles/ahep/volume-2020/6760547/figures/6760547.fig.002c.svgz" name="6760547.fig.002c" type="image/svg+xml"></object></td></tr><tr class="fig-caption"><td><b>(c) </b>Polyakov loop conjugate</td></tr></table>

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Advances in High Energy Physics

fig2

Figure 2

Figure 2: Influence of the Effective Potential on the Crossover Width in the Two Flavor Polyakov-Nambu-Jona-Lasinio Model 