Electromagnetismgraduate

Dirac Magnetic Monopole Quantization

Also known as: Dirac Quantization Condition · Magnetic Charge Quantization

Wrap an electron's quantum wavefunction around a monopole and its phase must come back to itself — single-valuedness. The phase picked up is set by the magnetic flux from the monopole; demanding it be a multiple of 2π forces the product of electric and magnetic charge to be quantized. Turn it around: even one monopole makes every electric charge a multiple of a basic unit.

eg=2πn=nh    g=nhee\,g = 2\pi n \hbar = n h \;\Rightarrow\; g = \frac{n h}{e}
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A magnetic monopole radiates field lines outward (a hedgehog) while electric charges orbit it, each winding accumulating a quantized phase; the slider steps the quantum number n.

Equivalent forms

eg2π=n, nZ\frac{e g}{2\pi\hbar} = n,\ n\in\mathbb{Z}
gD=he (n=1)g_D = \frac{h}{e}\ (n=1)
ge=12αn\frac{g}{e} = \frac{1}{2\alpha}n
One hypothetical particle, never yet seen, would explain a deep fact we observe everywhere — that charge comes in exact integer units. Few 'if' statements in physics buy so much.