Physics:Quantum field theory (QFT) basics

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Quantum field theory basics: particles as excitations of fields, spacetime, Feynman diagrams, and gauge symmetries.
Quantum field theory describes particles as excitations of underlying fields, combining quantum mechanics with special relativity to explain particle interactions and fundamental forces.[1]

Overview of key concepts in quantum field theory

Creation/annihilation operators

In quantum field theory, particles are described as excitations of underlying fields. The creation and annihilation operators provide a mathematical framework for adding or removing particles from a system.[2]

Definition

The annihilation operator a^k removes a particle from a mode with momentum k, while the creation operator a^k adds a particle:

a^k|nk=nk|nk1,

a^k|nk=nk+1|nk+1.

Commutation relations

For bosons, the operators satisfy

[a^k,a^k]=δkk.

For fermions, they satisfy anticommutation relations:

{a^k,a^k}=δkk.

Field expansion

A quantum field can be written as a sum over modes:

ϕ(x)=k(a^kuk(x)+a^kuk*(x)).

This expresses the field as a superposition of particle creation and annihilation processes.

Physical significance

Creation and annihilation operators:

  • describe particle number changes,
  • allow treatment of multi-particle systems,
  • form the basis of quantum field quantization.

Fock space

Fock space is the Hilbert space used in quantum field theory to describe systems with a variable number of particles. It is constructed as a direct sum of multi-particle spaces built from single-particle states.[3]

Definition

Fock space is defined as

=(),

where is the single-particle Hilbert space.

Each term represents states with:

  • 0 particles (vacuum),
  • 1 particle,
  • 2 particles,
  • and so on.

Vacuum state

The vacuum state |0 contains no particles and satisfies

a^k|0=0.

All other states are built by applying creation operators to the vacuum.

Multi-particle states

A general multi-particle state is constructed as

|n1,n2,=k(a^k)nknk!|0.

This describes a configuration with nk particles in each mode.

Bosons and fermions

The structure of Fock space depends on particle statistics:

  • Bosons — symmetric states (no restriction on occupation number)
  • Fermions — antisymmetric states (Pauli exclusion principle: nk=0 or 1)

Physical significance

Fock space:

  • allows description of systems with changing particle number,
  • provides the natural setting for quantum fields,
  • is essential in particle physics and quantum many-body theory.

Propagators

In quantum field theory, a propagator describes the probability amplitude for a particle to travel from one spacetime point to another. It plays a central role in calculations of particle interactions and quantum processes.[4]

Definition

For a scalar field, the propagator is given by the time-ordered product

D(xy)=0|T{ϕ(x)ϕ(y)}|0,

where T denotes time ordering.

This quantity represents the amplitude for a particle created at point y to be annihilated at point x.

Momentum-space form

In momentum space, the propagator for a free scalar field has the form

D~(p)=1p2m2+iϵ.

The small imaginary term iϵ ensures proper boundary conditions and causality.

Interpretation

Propagators encode how disturbances in a field propagate through spacetime. They are not classical trajectories, but quantum amplitudes that contribute to observable processes.

Role in interactions

In interacting theories, propagators appear as internal lines in Feynman diagrams. They connect interaction vertices and represent virtual particles.

Physical significance

Propagators:

  • describe the propagation of particles and fields,
  • are fundamental building blocks of quantum field theory,
  • enable calculation of scattering amplitudes and correlation functions.

Feynman diagrams

Feynman diagrams are graphical representations of interactions between particles in quantum field theory. They provide an intuitive and systematic way to calculate probability amplitudes for physical processes.[5]

Basic elements

A Feynman diagram consists of:

  • External lines — incoming and outgoing particles
  • Internal lines — propagators (virtual particles)
  • Vertices — interaction points

Each element corresponds to a mathematical expression in perturbation theory.

Example

Example of a Feynman diagram: electron–photon scattering. Straight lines represent fermions, wavy lines represent photons, and vertices represent interactions.

A simple interaction, such as electron–photon scattering, can be represented by a diagram where:

  • straight lines represent fermions,
  • wavy lines represent photons,
  • vertices represent electromagnetic interactions.

Perturbation theory

Feynman diagrams arise from expanding the evolution operator in powers of the interaction strength. Each diagram corresponds to a term in this expansion.

The total amplitude is obtained by summing over all relevant diagrams.

Feynman rules

Each quantum field theory has a set of Feynman rules that translate diagrams into mathematical expressions:

  • propagators correspond to internal lines,
  • interaction terms determine vertex factors,
  • external lines correspond to particle states.

These rules allow systematic computation of scattering amplitudes.

Virtual particles

Internal lines represent virtual particles, which do not satisfy the usual energy–momentum relation:

p2m2.

They are not directly observable but contribute to measurable quantities.

Physical significance

Feynman diagrams:

  • provide a visual representation of particle interactions,
  • simplify complex calculations in quantum field theory,
  • are essential in particle physics and high-energy experiments.

They are one of the most powerful tools for connecting theory with experimental predictions.

Further reading

General readers

Introductory texts

Advanced texts

See also

Table of contents (185 articles)

Index

Full contents

9. Quantum optics and experiments (5) ↑ Back to index
14. Plasma and fusion physics (8) ↑ Back to index
Conceptual illustration of plasma physics in a fusion context, showing magnetically confined ionized gas in a tokamak and the collective behavior governed by electromagnetic fields and transport processes.
Conceptual illustration of plasma physics in a fusion context, showing magnetically confined ionized gas in a tokamak and the collective behavior governed by electromagnetic fields and transport processes.

References

  1. Peskin, Michael E. (1995). 
  2. Peskin, Michael E.; Schroeder, Daniel V. (1995). An Introduction to Quantum Field Theory. Westview Press. 
  3. Peskin, Michael E.; Schroeder, Daniel V. (1995). An Introduction to Quantum Field Theory. Westview Press. 
  4. Peskin, Michael E.; Schroeder, Daniel V. (1995). An Introduction to Quantum Field Theory. Westview Press. 
  5. Peskin, Michael E.; Schroeder, Daniel V. (1995). An Introduction to Quantum Field Theory. Westview Press. 
Author: Harold Foppele

Source attribution: Quantum field theory (QFT) basics