Editing Dynamo theory (section)

=== Spontaneous breakdown of a topological supersymmetry ===
Kinematic dynamo can be also viewed as the phenomenon of the spontaneous breakdown of the topological supersymmetry of the associated stochastic differential equation related to the flow of the background matter.<ref>{{cite journal |author1=Ovchinnikov, I.V. |author2=Ensslin, T.A. |title=Kinematic dynamo, supersymmetry breaking, and chaos |journal=Physical Review D |volume=93 |issue=8 |pages=085023 |date=April 2016 |doi=10.1103/PhysRevD.93.085023 |arxiv=1512.01651 |bibcode=2016PhRvD..93h5023O |s2cid=59367815 }}</ref> Within [[Supersymmetric theory of stochastic dynamics|stochastic supersymmetric theory]], this supersymmetry is an intrinsic property of ''all'' [[stochastic differential equation]]s, its interpretation is that the model's phase space preserves continuity via continuous time flows. When the continuity of that flow spontaneously breaks down, the system is in the stochastic state of [[Chaos theory|''deterministic chaos'']].<ref>{{cite journal |author=Ovchinnikov, I.V. |date=March 2016 |title=Introduction to Supersymmetric Theory of Stochastics |journal=Entropy |volume=18 |issue=4 |pages=108 |doi=10.3390/e18040108 |arxiv=1511.03393 |bibcode=2016Entrp..18..108O |s2cid=2388285|doi-access=free }}</ref> In other words, kinematic dynamo arises because of chaotic flow in the underlying background matter.