FEYNMAN DIAGRAMS

The straight and wavy lines in a diagram are not paths a particle traces through space; they are bookkeeping symbols for computing probability amplitudes. A line joining two vertices is a virtual particle: off-shell, and never directly observed. Every vertex carries a coupling constant — √α in quantum electrodynamics, where α ≈ 1/137 — so the more vertices, the smaller the contribution. Those few rules alone are enough to build Møller and Compton scattering, annihilation, pair production and beta decay through a W⁻.

▸ Drawing notation: fermion (arrow) · photon (wave) · gluon (coil)…
▸ Building interaction vertices — conserving charge & momentum
▸ Loading processes: Møller · Compton · pair annihilation/production · β decay…
▸ Note: a diagram = a CALCULATION TOOL, not a real trajectory
▸ Calibrating the light pulse along the lines — Online. ✅
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⌂ Particles & Quantum

Simulation room Feynman Diagrams

Feynman Diagrams
Online
QED · QCD · Weak force
Now showing
✏️ Ký hiệu giản đồ
Process—
Force / carrier—
Vertices (order)—
External lines—
Coupling—
Scenario—
How to read it
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Click 1 line/vertex in the diagram (or in the right column) = open its detail card · switch the Scenario to view each scattering/decay process
Light-pulse rhythm along the lines (the feel of particles moving) fermionphoton
About Feynman Diagrams

The straight and wavy lines in a diagram are not paths a particle traces through space; they are bookkeeping symbols for computing probability amplitudes. A line joining two vertices is a virtual particle: off-shell, and never directly observed. Every vertex carries a coupling constant — √α in quantum electrodynamics, where α ≈ 1/137 — so the more vertices, the smaller the contribution. Those few rules alone are enough to build Møller and Compton scattering, annihilation, pair production and beta decay through a W⁻.

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