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Weinberg–Salam Model

Electroweak Unification of Fundamental Forces

Introduction

The Weinberg–Salam model is a unified theory proposed independently by Sheldon Glashow, Abdus Salam, and Steven Weinberg. It unifies the electromagnetic and weak nuclear interactions into a single framework known as the Electroweak Theory.

At very high energies, electromagnetic and weak forces behave as a single force, called the electroweak force.

Why Electroweak Unification?

Gauge Symmetry of the Model

The model is a non-Abelian gauge theory based on:

\( SU(2)_L \times U(1)_Y \)

Gauge Bosons

Field Symbol Associated Force
Weak isospin fields \(W^1, W^2, W^3\) Weak interaction
Hypercharge field \(B\) Electroweak

After symmetry breaking, these combine to form physical particles.

Electroweak Symmetry Breaking

Initially all gauge bosons are massless. Mass generation occurs through the Higgs mechanism.

Higgs Field

Gauge invariance is preserved while weak bosons acquire mass.

Physical Gauge Bosons

Particle Symbol Mass Interaction
Photon \(\gamma\) 0 Electromagnetic
W bosons \(W^\pm\) Heavy Weak (charged)
Z boson \(Z^0\) Heavy Weak (neutral)

Weinberg Angle (Weak Mixing Angle)

The mixing between \(W^3\) and \(B\) fields is described by the Weinberg angle \( \theta_W \).

\[ \begin{aligned} A_\mu &= B_\mu \cos\theta_W + W^3_\mu \sin\theta_W \\ Z_\mu &= -B_\mu \sin\theta_W + W^3_\mu \cos\theta_W \end{aligned} \]

Electric Charge Relation

Electric charge is related to weak isospin and hypercharge:

\( Q = T_3 + \dfrac{Y}{2} \)

This explains charge quantization in the Standard Model.

Successes of the Model

Limitations

Summary

✔ Unifies electromagnetic and weak forces ✔ Based on \(SU(2)_L \times U(1)_Y\) symmetry ✔ Uses Higgs mechanism for mass generation ✔ Predicts W, Z bosons ✔ Cornerstone of the Standard Model