a singular charge / theoretical / unobserved

monopole.tech

— on the elegance of a particle that should exist —
lat 37°14′ / lon -115°48′ field strength: indeterminate fig. 1.0
ii.

the theory

Dirac, 1931 — a string of singularities
fig. 2.1 — radial field g

A point source from which lines of magnetic flux radiate in every direction — not the familiar dipole, but a true singularity of charge.

eq. 2.1 — quantization
eg = nℏc2 — n ∈ ℤ

If a single monopole exists anywhere in the universe, all electric charge must be quantized. The mere possibility forces the discreteness we observe.

“The mere existence of one pole would suffice to explain why charge is granular.”

— P. A. M. Dirac, 1931
fig. 2.2 — the dirac string +g -g

The string is unobservable — an artifact of the gauge, a thread of coordinate fiction connecting the pole to infinity. Move the string anywhere; the physics is unchanged.

note. 2.3

In the symmetric Maxwell equations, electricity and magnetism stand as mirror twins. Yet only one twin has ever knocked at the door.

∇·E = ρe ∇·B = ρm ρm ≡ ?
marginalia

— if charge is quantized because a single monopole exists somewhere, then the universe’s arithmetic was decided by a particle no one has held.

iv.

the edge

where the diagrams begin to fade

absence is not the same as non-existence. the desert is full of things that have not yet arrived.

coda

A century of theory. Half a century of search. The monopole remains a mathematical certainty in a universe that has not yet agreed.

fig. 4.1 — the listening