Feynman diagram
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A Feynman diagram is a bookkeeping device for performing calculations in quantum field theory, invented by American physicist Richard Feynman.
The problem of calculating scattering cross sections in particle physics reduces to summing over the amplitudes of all possible intermediate states, in what is known as a perturbation expansion. These states can be represented by Feynman diagrams, which are much easier to keep track of than frequently torturous calculations. Feynman showed how to calculate diagram amplitudes using so-called Feynman rules, which can be derived from the system's underlying Lagrangian. Each internal line corresponds to a factor of the corresponding virtual particle's propagator; each vertex where lines meet gives a factor derived from an interaction term in the Lagrangian, and incoming and outgoing lines provide constraints on energy, momentum and spin.
In addition to their value as a mathematical technology, Feynman diagrams provide deep physical insight to the nature of particle interactions. Particles interact in every way available; in fact, intermediate "virtual" particles are allowed to propagate faster than light. (This does not violate relativity for deep reasons; in fact, it helps preserve causality in a relativistic spacetime.) The probability of each outcome is then obtained by summing over all such possibilities. This is closely tied to the functional integral formulation of quantum mechanics, also invented by Feynman - see path integral formulation.
The naive application of such calculations often produces diagrams whose amplitudes are infinite, which is undesirable in a physical theory. The problem is that particle self-interactions are erroneously ignored. The technique of renormalization, pioneered by Feynman, Schwinger, and Tomonaga, compensates for this effect and eliminates the troublesome infinite terms. After renormalization has been carried out, Feynman diagram calculations often match experimental results with very good accuracy.
Feynman diagram and path integral methods are also used in statistical mechanics.
Murray Gell-Mann always referred to Feynman diagrams as Stückelberg diagrams, after a Swiss physicist, Ernst Stückelberg, who devised a similar notation[1].
Example
To the right is the Feynman diagram for beta decay. The straight lines in the diagrams represent fermions, while the wavy line represents virtual bosons. As time runs along the y-coordinate of the diagram, the neutrino looks as if it is moving against or backwards in time. But using such notation only means that that fermion is not the particle travelling backwards in time but its antiparticle travelling forwards in time. Hence the particle labelled neutrino is, in fact, an antineutrino. This method works very well for all particles and antiparticles.
de:Feynmandiagramm sl:Feynmanov diagram
External Links
WikiTeX supports editing Feynman diagrams directly in Wiki articles.
