Higher-order field theories: $\phi^6$, $\phi^8$ and beyond
Avadh Saxena, Ivan C. Christov, Avinash Khare

TL;DR
This paper explores advanced higher-order scalar field theories like $^6$ and $^8$, analyzing their properties, phase transition roles, and connections to high-energy physics, highlighting new models with complex equilibria and long-range interactions.
Contribution
It introduces recent developments in higher-order field theories, including detailed analysis of $^6$ potentials, their phase transition relevance, and connections to high-energy physics models.
Findings
Analysis of symmetric triple well $^6$ potential.
Existence of kink solutions with power-law tails.
Connections between field theories and high-energy physics models.
Abstract
The 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 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 , 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 …
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