Gluon condensate

Template:Short description In quantum chromodynamics (QCD), the gluon condensate is a non-perturbative property of the QCD vacuum which could be partly responsible for giving masses to light mesons.

If the gluon field tensor is represented as G_μν, then the gluon condensate is the vacuum expectation value $⟨G_{\mu \nu }{G}^{\mu \nu }⟩$. It is not clear yet whether this condensate is related to any of the known phase changes in quark matter. There have been scattered studies of other types of gluon condensates, involving a different number of gluon fields.

For more on the context in which this quantity occurs, see the article on the QCD vacuum.

See also

• Quantum chromodynamics
• QCD vacuum and chiral condensates
• Vacuum in quantum field theory
• Quark–gluon plasma
• QCD matter

References

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