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The effective field theory below the electroweak scale after integrating out the , , Higgs, and top quark. It contains QCD and QED for light fields plus higher-dimension weak and possible beyond-Standard-Model operators.
wp-physics-effective_field_theoryjhep-leftpenco-eftEach relation below ends at this concept.
This is an authored directed relation from the source endpoint to the target endpoint.
Fermi four-fermion interactions are leading weak-operator components within the broader low-energy effective field theory.
The source supplies a substantive formal ingredient, dynamical sector, law, field content, or mechanism of the target theoretical framework.
jhep-lefttong-standard-modelThis is an authored directed relation from the source endpoint to the target endpoint.
QCD for the light quarks and gluons is a renormalizable gauge-sector component of LEFT.
The source supplies a substantive formal ingredient, dynamical sector, law, field content, or mechanism of the target theoretical framework.
jhep-leftpdg-qcdThis is an authored directed relation from the source endpoint to the target endpoint.
QED for the light charged fields is a renormalizable gauge-sector component of LEFT.
The source supplies a substantive formal ingredient, dynamical sector, law, field content, or mechanism of the target theoretical framework.
jhep-lefttong-qftThis is an authored directed relation from the source endpoint to the target endpoint.
Below the electroweak scale, integrating out , , Higgs, and top degrees of freedom yields LEFT with QCD, QED, and local higher-dimension operators.
The target retains the degrees of freedom and interactions relevant below a stated scale or within a stated regime, while higher-energy or unresolved degrees of freedom from the source are integrated out, coarse-grained, or encoded in effective couplings.
jhep-lefttong-standard-modelThis is an authored directed relation from the source endpoint to the target endpoint.
SMEFT matches onto LEFT after electroweak symmetry breaking and integration of heavy Standard Model fields; LEFT Wilson coefficients retain the effects of SMEFT operators.
The target retains the degrees of freedom and interactions relevant below a stated scale or within a stated regime, while higher-energy or unresolved degrees of freedom from the source are integrated out, coarse-grained, or encoded in effective couplings.
jhep-leftpenco-eftEach relation below starts at this concept.
No direct relations are authored in this direction.