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    Quantum Field Theory

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    • Introduction to Quantum Mechanics
      • 1.1Historical Background
      • 1.2Introduction to Quantum Concepts
      • 1.3Quantum States and Observables
    • Wave-Particle Duality
      • 2.1The Double Slit Experiment
      • 2.2Heisenberg's Uncertainty Principle
      • 2.3Quantum Superposition and Entanglement
    • The Schrödinger Equation
      • 3.1Time-Dependent Equation
      • 3.2Stationary States
      • 3.3Square Well Potential
    • Quantum Operators and Measurement
      • 4.1Quantum Operators
      • 4.2The Measurement Postulate
      • 4.3Complex Probability Amplitudes
    • Quantum Mechanics of Systems
      • 5.1Quantum Harmonic Oscillator
      • 5.2Quantum Angular Momentum
      • 5.3Particle in a Box
    • The Dirac Equation
      • 6.1Wave Equations
      • 6.2The Dirac Sea
      • 6.3Hole Theory
    • Introduction to Quantum Electrodynamics (QED)
      • 7.1Electromagnetic Field
      • 7.2Feynman Diagrams
      • 7.3QED Interactions
    • Path Integrals and Quantum Mechanics
      • 8.1Feynman’s Approach
      • 8.2Action Principle
      • 8.3Quantum Oscillator Problem
    • Symmetries in Quantum Field Theory
      • 9.1Gauge Symmetry
      • 9.2Poincaré Symmetry
      • 9.3Global and Local Symmetries
    • Quantum Chromodynamics
      • 10.1Color Charge
      • 10.2Quark Model
      • 10.3Confinement and Asymptotic Freedom
    • The Higgs Mechanism
      • 11.1Electroweak Symmetry Breaking
      • 11.2The Higgs Boson
      • 11.3Implication for Mass of Known Particles
    • Quantum Field Theory in Curved Space-Time
      • 12.1The Concept of Spacetime
      • 12.2Quantum Effects in Curved Spaces
      • 12.3Hawking Radiation
    • Quantum Cosmology and Conclusion
      • 13.1Big Bang Theory
      • 13.2Cosmic Inflation
      • 13.3Looking Ahead: Frontiers in Quantum Mechanics

    Introduction to Quantum Electrodynamics (QED)

    Understanding Feynman Diagrams in Quantum Electrodynamics

    pictorial representations of the behavior of subatomic particles

    Pictorial representations of the behavior of subatomic particles.

    Feynman diagrams are a powerful tool in quantum field theory and particularly in Quantum Electrodynamics (QED). Named after the American physicist Richard Feynman, these diagrams provide a pictorial representation of the mathematical expressions describing the behavior of subatomic particles.

    Introduction to Feynman Diagrams

    Feynman diagrams are used to represent interactions between particles in quantum field theory. They are a type of space-time diagram, with time typically represented on the vertical axis and space on the horizontal axis. Each line in the diagram represents a particle, and each vertex where lines meet represents an interaction between particles.

    Rules for Drawing Feynman Diagrams

    There are specific rules for drawing Feynman diagrams. Each type of particle is represented by a specific type of line: solid lines for fermions (like electrons and quarks), wavy lines for bosons (like photons), and dashed lines for scalar particles (like the Higgs boson).

    Particles moving forward in time are represented by lines pointing upwards, while antiparticles moving forward in time are represented by lines pointing downwards. Each vertex must conserve charge, momentum, and other quantum numbers.

    Interpreting Feynman Diagrams

    Feynman diagrams are not just pictures; they represent mathematical expressions. Each line corresponds to a factor in the expression, and each vertex corresponds to a term in the interaction Hamiltonian, the part of the quantum mechanical total energy operator that describes the energy due to interactions.

    The probability of an interaction occurring is proportional to the square of the absolute value of the sum of the expressions for all possible diagrams representing that interaction.

    Using Feynman Diagrams to Calculate Probabilities

    Feynman diagrams can be used to calculate the probabilities of different outcomes in a quantum interaction. This is done by translating each diagram into a mathematical expression using the rules of quantum field theory, and then adding up these expressions for all possible diagrams.

    The resulting expression can then be squared and integrated over all possible final states to give the total probability for the interaction.

    In conclusion, Feynman diagrams are a crucial tool in understanding and calculating quantum interactions. They provide a visual way to represent and calculate complex quantum phenomena, making them an invaluable tool in the field of Quantum Electrodynamics.

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