FIELD THEORY AND QUANTUM MECHANICS

Quantum field theory is the theoretical framework used to describe elementary particles and predict their behaviour. Developed starting in the 1920s, quantum field theory combines the principles of quantum mechanics and special relativity in a coherent framework. This is one of the most beautiful and profound triumphs of modern physics, thanks to which we understand the laws that govern the elementary components of matter.
In this theory, particles are described as excitations of fields that extend across all spacetime. The fields are governed by a Lagrangian, a function that determines both the behaviour of non-interacting fields and their interactions.
Quantum field theory successfully describes three of the four fundamental interactions of nature: electromagnetism, the strong nuclear force, and the weak nuclear force.

For each of these interactions, there is a quantum field theory that explains its properties and behaviour. Quantum electrodynamics (QED) describes the interaction between photons, the quantums of the electromagnetic field, and charged particles, for example electrons. Quantum chromodynamics (QCD) describes the interaction between gluons, the mediator particles of the strong interaction, and quarks, the constituents of protons and neutrons. The electroweak theory provides a single description of the electromagnetic interaction and weak interaction, mediated by the bosons W and Z, responsible for radioactive decay of nuclei.
All these theories belong to a particularly important class of quantum field theories that takes the name of “gauge” theories. Under the spell of the “gauge” principle, to quote the Nobel Prize winner Gerard ‘t Hooft, the fundamental interactions are obtained by imposing suitable (“gauge”) symmetries on the Lagrangian that describes the non-interacting fields. “Gauge” symmetries and fundamental interactions, with the related mediator particles, are,thus, intimately connected.

Illustration of quark-gluon plasma (© CERN)