A kinetic term contains derivatives of a field and determines its free propagation. Its quadratic differential operator becomes the inverse quantum field theory propagator.
A gauge-covariant kinetic term replaces ordinary derivatives by covariant derivatives. Expanding it generates interactions between the matter field and one or more gauge fields, including contact vertices with two gauge bosons.
Ancestors (7)
- Lagrangian density
- Lagrangian (field theory)
- Classical field theory
- Quantum field theory
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Incoming links (100)
- Adjoint triplet Higgs spectrum
- Canonical Abelian Higgs shift
- Chiral boost weights in two spacetime dimensions
- Continuous vacuum selection by an external source
- Critical dimension of a monomial scalar interaction
- Discrete symmetries of a two-component Dirac field in three dimensions
- Gauge-boson mass matrix
- Gauge contributions to the F-term supertrace
- Gauge singlet
- Goldstone directions in the scalar mass matrix
- Mixing of exactly massless neutrinos is removable
- Orthogonal completion of mixed neutral lepton kinetic terms
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- Radial and angular modes of an orthogonally invariant scalar potential
- Three-site Abelian Higgs chain
- Time-sliced configuration-space path integral
- Wilsonian rescaling of a scalar coupling
- Yang-Mills Lagrangian
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The kinetic term refers to the part of an equation or expression that represents the kinetic energy of a system. In physics, kinetic energy is the energy that an object possesses due to its motion.