Higher-order field theories: $Ï^6$, $Ï^8$ and beyond
arXiv:1806.06693 · doi:10.1007/978-3-030-11839-6_12
Abstract
The $Ï^4$ model has been the "workhorse" of the classical Ginzburg--Landau phenomenological theory of phase transitions and, furthermore, the foundation for a large amount of the now-classical developments in nonlinear science. However, the $Ï^4$ model, in its usual variant (symmetric double-well potential), can only possess two equilibria. Many complex physical systems possess more than two equilibria and, furthermore, the number of equilibria can change as a system parameter (e.g., the temperature in condensed matter physics) is varied. Thus, "higher-order field theories" come into play. This chapter discusses recent developments of higher-order field theories, specifically the $Ï^6$, $Ï^8$ models and beyond. We first establish their context in the Ginzburg--Landau theory of successive phase transitions, including a detailed discussion of the symmetric triple well $Ï^6$ potential and its properties. We also note connections between field theories in high-energy physics (e.g., "bag models" of quarks within hadrons) and parametric (deformed) $Ï^6$ models. We briefly mention a few salient points about even-higher-order field theories of the $Ï^8$, $Ï^{10}$, etc.\ varieties, including the existence of kinks with power-law tail asymptotics that give rise to long-range interactions. Finally, we conclude with a set of open problems in the context of higher-order scalar fields theories.
24 pages, 7 figures, Springer book class, invited contribution to the upcoming book "A dynamical perspective on the $Ï^4$ model: Past, present and future", eds. P.G. Kevrekidis and J. Cuevas-Maraver; v2: revisions as a result of feedback from book editor; v3: corrects some typos