Physics:Quantum Electroweak theory: Difference between revisions
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'''Electroweak theory''' is the unified quantum field theory that combines the electromagnetic and weak interactions into a single framework based on the gauge symmetry group <math>SU(2)_L \times U(1)_Y</math>.<ref name="weinberg">Weinberg, S. (1967). A model of leptons.</ref> It forms a central part of the Standard Model of particle physics. | '''Electroweak theory''' is the unified quantum field theory that combines the electromagnetic and weak interactions into a single framework based on the gauge symmetry group <math>SU(2)_L \times U(1)_Y</math>.<ref name="weinberg">Weinberg, S. (1967). A model of leptons.</ref> It forms a central part of the Standard Model of particle physics. | ||
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Revision as of 14:02, 17 May 2026
Electroweak theory is the unified quantum field theory that combines the electromagnetic and weak interactions into a single framework based on the gauge symmetry group .[1] It forms a central part of the Standard Model of particle physics.
Unification of forces
Electroweak theory shows that the electromagnetic force and weak nuclear force are different manifestations of a single interaction at high energies.
At low energies:
- electromagnetic interaction → long-range force
- weak interaction → short-range force
At high energies, they merge into a unified electroweak interaction.[2]
Gauge symmetry
The theory is based on the symmetry group:
where:
- acts on left-handed fermions
- corresponds to weak hypercharge
Gauge fields are introduced to preserve local symmetry, leading to four gauge bosons.[3]
Gauge bosons
The electroweak theory predicts four gauge bosons:
- (from )
- (from )
These combine to form the physical particles:
- and (charged weak bosons)
- (neutral weak boson)
- (photon)
This mixing explains how electromagnetic and weak forces are related.[1]
Spontaneous symmetry breaking
The electroweak symmetry is not directly observed because it is spontaneously broken.
This occurs through the Higgs mechanism, introducing a scalar field whose vacuum expectation value selects a specific ground state:
As a result:
- and acquire mass
- the photon remains massless
This explains the short range of the weak interaction.[4]
Electroweak Lagrangian
The electroweak Lagrangian includes:
- fermion kinetic terms
- gauge field terms
- Higgs field contributions
- interaction terms
These components together describe the full dynamics of the electroweak interaction.
Weak interactions
The weak interaction involves processes such as:
- beta decay
- neutrino interactions
- flavor-changing processes
These are mediated by the and bosons.
Experimental confirmation
Electroweak theory has been confirmed by numerous experiments, including:
- discovery of the and bosons
- precision measurements at particle accelerators
- observation of the Higgs boson
These results strongly support the validity of the theory.[3]
Role in the Standard Model
Electroweak theory, together with quantum chromodynamics, forms the core of the Standard Model.
It unifies two of the fundamental forces and provides a consistent framework for describing particle interactions.
Conceptual importance
Electroweak theory demonstrates how gauge symmetry and spontaneous symmetry breaking combine to produce realistic physical theories.
It is a cornerstone of modern particle physics and a key step toward deeper unification.
See also
Table of contents (198 articles)
Index
Full contents
References
Source attribution: Quantum field theory (QFT) core
















