CHANG-TSE HSIEHJIUNN-WEI CHEN2022-06-302022-06-30201103702693https://www.scopus.com/inward/record.uri?eid=2-s2.0-79960349293&doi=10.1016%2fj.physletb.2011.05.066&partnerID=40&md5=7b623d3dd2b6183050eec9c0126ce445https://scholars.lib.ntu.edu.tw/handle/123456789/614635The ratio η/s, shear viscosity (η) to entropy density (s), reaches its local minimum at the (second order) phase transition temperature in a wide class of systems. It was suspected that this behavior might be universal. However, a counterexample is found in a system of two weakly self-interacting real scalar fields with one of them condensing at low temperatures while the other remains in the symmetric phase. There is no interaction between the two fields. In our mean field analysis the resulting η/s is monotonically decreasing in temperature despite the second order phase transition. © 2011 Elsevier B.V.Finite temperature field theory; O(N) model; Transport coefficientsjournal article10.1016/j.physletb.2011.05.0662-s2.0-79960349293