Asymptotic freedom was believed to be an important characteristic of strong interactions.

In the course of asymptotic freedom, the strong interaction becomes weaker at higher temperatures.

Later it was used to understand asymptotic freedom.

This is an ultraviolet fixed point, associated with the phenomenon known as 'asymptotic freedom'.

At the same time the radiation is damped moderately due to asymptotic freedom.

One of the most important results obtained for Yang-Mills theory is asymptotic freedom.

The other side of asymptotic freedom is confinement.

In addition, current quarks possess one asymptotic freedom within the perturbation theory described limits.

The general idea, with small logarithmic modifications, is explained in quantum chromodynamics by "asymptotic freedom".

Asymptotic freedom, independently discovered by Politzer, was important for the development of quantum chromodynamics.

The gluon field strength has extra terms which lead to self-interactions between the gluons and asymptotic freedom.

If the fixed point is trivial (aka Gaussian), the theory is said to have asymptotic freedom.

As mentioned, asymptotic freedom means that at large energy - this corresponds also to short distances - there is practically no interaction between the particles.

This approach is based on asymptotic freedom, which allows perturbation theory to be used accurately in experiments performed at very high energies.

This causes asymptotic freedom: as quarks come closer to each other, the chromodynamic binding force between them weakens.

Gauge theories with quarks became a viable contender for the strong interaction in 1973 when the concept of asymptotic freedom was identified.

However, there is another property of the strong nuclear force, called asymptotic freedom, that makes the concept of quarks and gluons well defined.

A pair of properties that are unique to QCD help provide solutions to these problems: asymptotic freedom and confinement.

Because the quarks are treated as free quarks inside the bag, the radius-independence in a sense validates the idea of asymptotic freedom.

Asymptotic freedom, which means that in very high-energy reactions, quarks and gluons interact very weakly.

If n 16, the ensuing beta function dictates that the coupling decreases with increasing energy scale, a phenomenon known as asymptotic freedom.

Asymptotic freedom can be derived by calculating the beta-function describing the variation of the theory's coupling constant under the renormalization group.

Here, no Asymptotic freedom exists, but the interactions between valence quarks and sea quarks gain strongly on significance.

Another aspect of confinement is asymptotic freedom which makes it conceivable that quantum Yang-Mills theory exists without restriction to low energy scales.

Gauge theories became even more attractive when it was realized that non-abelian gauge theories reproduced a feature called asymptotic freedom.