Spontaneous symmetry breaking

Spontaneous symmetry breaking is a spontaneous process of symmetry breaking, by which a physical system in a symmetric state spontaneously ends up in an asymmetric state. In particular, it can describe systems where the equations of motion or the Lagrangian obey symmetries, but the lowest-energy vacuum solutions do not exhibit that same symmetry. When the system goes to one of those vacuum solutions, the symmetry is broken for perturbations around that vacuum even though the entire Lagrangian retains that symmetry. By definition, spontaneous symmetry breaking requires the existence of physical laws (e.g. quantum mechanics) which are invariant under a symmetry transformation (such as translation or rotation), so that any pair of outcomes differing only by that transformation have the same probability distribution. For example if measurements of an observable at any two different positions have the same probability distribution, the observable has translational symmetry. Spontaneous symmetry breaking occurs when this relation breaks down, while the underlying physical laws remain symmetrical. Conversely, in explicit symmetry breaking, if two outcomes are considered, the probability distributions of a pair of outcomes can be different. For example in an electric field, the forces on a charged particle are different in different directions, so the rotational symmetry is explicitly broken by the electric field which does not have this symmetry. Phases of matter, such as crystals, magnets, and conventional superconductors, as well as simple phase transitions can be described by spontaneous symmetry breaking. Notable exceptions include topological phases of matter like the fractional quantum Hall effect. Typically, when spontaneous symmetry breaking occurs, the observable properties of the system change in multiple ways. For example the density, compressibility, coefficient of thermal expansion, and specific heat will be expected to change when a liquid becomes a solid. Coleman–Weinberg potential Consider a symmetric upward dome with a trough circling the bottom.

Band Gap Renormalization at Different Symmetry Points in Perovskites

Primary and secondary order parameters in the fully frustrated transverse-field Ising model on the square lattice

Anomalous and Chern topological waves in hyperbolic networks

Primary and secondary order parameters in the fully frustrated transverse-field Ising model on the square lattice

Band Gap Renormalization at Different Symmetry Points in Perovskites

Anomalous and Chern topological waves in hyperbolic networks