A sphaleron is a static solution to the electroweak field equations of the Standard Model of particle physics,
and is involved in certain hypothetical processes that violate baryon and lepton numbers.
Such processes cannot be represented by perturbative methods such as Feynman diagrams,
and are therefore called non-perturbative. Geometrically,
a sphaleron is a saddle point of the electroweak potential.
This saddle point rests at the top of a barrier between two different low-energy equilibria of a given system,
the two equilibria are labeled with two different baryon numbers.
One of the equilibria might consist of three baryons, the other, alternative,
equilibrium for the same system might consist of three antileptons.
In order to cross this barrier and change the baryon number,
a system must either tunnel through the barrier or must for a reasonable period of time be brought up to a high enough energy that it can classically cross over the barrier.
In both the instanton and sphaleron cases,
the process can only convert groups of three baryons into three antileptons and vice versa.
This violates conservation of baryon number and lepton number,
but the difference B−L is conserved.
The minimum energy required to trigger the sphaleron process is believed to be around 10 TeV, however,
sphalerons cannot be produced in existing LHC collisions,
because while the LHC can create collisions of energy 10 TeV and greater,
the generated energy cannot be concentrated in a manner that would create sphalerons.A sphaleron is similar to the midpoint of the instanton,
so it is non-perturbative.
This means that under normal conditions sphalerons are unobservably rare. However,
they would have been more common at the higher temperatures of the early universe. 
