Dirac, 1931
The particle implied by symmetry
Amagnetic monopole is the elegant missing half of a familiar story: an isolated north or south magnetic pole, unpaired and standing alone. Ordinary magnets always arrive as dipoles. Cut one in two and each fragment politely grows a new opposite pole. The monopole asks whether nature might also permit a single magnetic charge, as fundamental as the electron is to electricity.1
Paul Dirac noticed that even one such particle anywhere in the universe would explain why electric charge appears in tidy units. The argument feels less like an engineering proof than a poem written in equations: topology placing integers where continuous values might have been.
One unseen pole could make every observed charge count in whole numbers.