Invariance

The Mathematics of Emmy Noether: symmetry and conservation in physics, and finiteness in algebra.

In 1918 Emmy Noether proved that every continuous symmetry of a Lagrangian comes with a conserved quantity. Because the laws of motion are the same from one moment to the next, energy is conserved; because they are the same from place to place, momentum is. A few years later she rebuilt commutative algebra around a single finiteness condition on ideals.

The series has three acts. Act I builds the tools: group actions, invariants, Lagrangians and the first theorem. Act II runs the theorem on energy, momentum, angular momentum, the Kepler problem and electric charge, and ends with her second theorem. Act III follows her algebra through ideals, Noetherian rings, Hilbert's basis theorem and Noether normalization.

Act I, The Principle of Invariance
From group actions to Lagrangians to Noether's first theorem.
01

What Is an Invariant?

Group actions, orbits and stabilizers, the D4 Cayley table, a Burnside count of colourings, and symmetric polynomials reduced step by step.

02

Invariants of a Binary Form

How the discriminant and the quartic invariants I and J scale by a power of the determinant under substitution, the question Noether's 1907 dissertation studied, checked in exact arithmetic.

03

Least Action and Lagrangians

A bead race to the cycloid, a knotted path relaxing onto the true motion, and the Euler-Lagrange equation that follows; least action is sometimes only a saddle.

04

Symmetries of a Lagrangian

Continuous symmetries, infinitesimal generators, and the change δL that the theorem is built on.

05

Noether's First Theorem, in Pictures

Five lines of calculus that turn a continuous symmetry into a conserved quantity, checked numerically.

Act II, Conservation Laws from Symmetry
The first theorem in action: energy, momentum, angular momentum, charge.
06

Energy, Momentum and Angular Momentum

Time shifts, space shifts and rotations; a kicked pendulum, a driven oscillator and a spinning hoop, and how to tell integrator drift from physics.

07

Kepler's Hidden Symmetry

The Laplace-Runge-Lenz vector, its precession under a perturbation, the SO(4) bracket algebra of bound orbits, and the degeneracies of hydrogen.

08

Phase and Electric Charge

Phase rotation of a Schrödinger field gives conserved charge, checked as current through the walls of a box; making the phase local forces a gauge field on the lattice.

09

Noether's Second Theorem

Local symmetries give identities instead of conservation laws: gauge on a lattice, Maxwell's identity on a grid, underdetermined motion, and why energy in GR is subtle.

Act III, The Algebraic Revolution
Ideals, chain conditions, and the abstract method that became modern algebra.
10

Ideals as the New Numbers

Unique factorization fails in ℤ[√−5]; Dedekind restores it by factoring ideals.

11

Noetherian Rings

Rings where every ascending chain of ideals stabilizes: chains in ℤ and k[x], a monomial staircase that must close, and a ring of all algebraic integers where the chain never stops.

12

Hilbert's Basis Theorem

If R is Noetherian, so is R[x]. Gordan's "theology" complaint, and Buchberger's algorithm, a later constructive tool for ideals that halts by the same chain condition.

13

Noether Normalization

Every affine variety is a finite cover of affine space; fiber counts over sampled base points, a substitution that stops roots escaping, and dimension read from Hilbert-function growth.