“…However, the Potts model has a much richer phase structure, which makes it an important testing ground for new theories and algorithms in the study of critical phenomena. The scope of research for the q-state Potts Model extend to its critical manifolds (Scullard & Jacobsen, 2016), its topological phases in the antiferromagnetic configuration (Zhao et al, 2018), its static critical behavior in high resolution (Caparica et al, 2015), fraction of uninfected walkers in its one-dimensional model (O'Donoghue & Bray, 2002), its ferromagnetic states with multisite interaction (Schreiber et al, 2018), its disordered states without a ferromagnetic phase (Marinari et al (1999), Carlucci (1999), approximate theories of first-order phase transitions on its twodimensional model (Dasgupta & Pandit, 1987) [which has Critical exponents of domain walls (Dubail et al, 2010), critical polynomials Jacobsen & Scullard (2013), entanglement entropy measurable using wavelet analysis Tomita (2018)], periodic p-adic Gibbs Measures Ahmad et al (2018), local scale invariance in ageing (Lorenz & Janke, 2007), Potts glass models (Yamaguchi, 2015), percolation models on bowtie lattices (Ding et al, 2012), Roughness exponent in two-dimensional percolation, and clock model (Redinz & Martins, 2001), interfacial adsorption in two-dimensional pure and random-bond Potts models (Fytas et al, 2017), exact valence bond entanglement entropy and probability distribution in the XXX Spin Chain (Jacobsen & Saleur, 2008), lung cancer pathological image analysis using a hidden Potts model (Li et al, 2017), the cellular Potts model (He et al (2009), Durand & Guesnet (2016), Albert & Schwarz (2014), Albert & Schwarz (2014), Voss-Böhme (2012), R. Noppe et al (2015), Scianna & Preziosi (2014), Harrison & Vasiev (2008)), the two (2)-Dimensional Wetting transition (Lopes & Mombach, 2017), the random resistor network and its...…”