On Symmetry and Emmy Noether

Today is my birthday, and also the 100th International Women’s Day. In honor of the latter, I want to highlight a mathematician who is famous among physicists but not well known among the general public: Emmy Noether.

Noether (1882-1935) has two major accomplishments to her name: she was a leader in the development of what is known today as abstract algebra (one of the major branches of mathematics), and she proved a theorem that bears her name that connects symmetries of nature to physical conservation laws. Algebra isn’t something I can talk intelligently about, so I’ll let others eulogize her for her contributions to that area. Her other major contribution is one that not only shows up in my research, but one I think can be understood by non-scientists.

Noether’s theorem, which she proved in 1915, says that there is a direct correspondence between a symmetry of nature and the conservation of a quantity. The most famous conservation law in physics is probably conservation of energy: you cannot create or destroy energy, simply transform it from one type to another. Noether’s theorem shows that the conservation of energy is related to time: if you run the clock backwards on an experiment and everything still looks “normal”, then energy is conserved. Here’s a simple experiment: take a ball and roll it up a ramp. It will roll up a certain distance, stop, then roll back down. If you run the clock in reverse, the motion of the ball looks the same! Noether’s theorem says this is no accident, but a statement about a symmetry in time. (Nitpickers will point out that this is a gross oversimplification, and they’re right. I hope this captures the spirit of the theorem well enough to satisfy most of you, though.) However, not all types of energy are “useful”: some are known as dissipative. The prime example of dissipative energy is friction—you can’t use energy converted into friction to (for example) lift an object. It’s lost to any useful purpose. Friction breaks the symmetry of time: you lose the same amount of energy to friction whether the clock is running forward or backwards, so a system with friction will not look “right” if you run the clock in reverse.

Other types of symmetry are more familiar: a sphere spinning around an axis has rotational symmetry, and if the sphere is featureless like a pool cue ball, you can pick any axis for it to rotate around. In ordinary classical physics, symmetry of this type leads to conservation of angular momentum, which figure skaters exploit by pulling in their arms to spin faster; in particle physics, symmetry of the same type (known as SU(2) symmetry for those physicists or mathematicians reading along at home) is associated with the nuclear forces. If you restrict the rotation to one axis (known as U(1) symmetry), the associated force is the electromagnetic force. (Supersymmetry goes a few steps further, and predicts a whole zoo of as-yet undiscovered particles—but it’s all still closely tied in to Noether’s theorem.) There’s also reflection symmetry of various sorts, rotations by fixed angles (think of a starfish with its five arms), and fairly abstract symmetries that are hard to describe in everyday language; each of these are associated with conservation laws if they are exhibited within a physical model. Even physicists who don’t know specifically what the theorem says and don’t know how to use it in a formal way still apply it, whether they know it or not.

Obviously a physical and mathematical principle this powerful is extremely noteworthy. I find it fitting to honor Emmy Noether today on International Women’s Day, not least because there are still significant gender imbalances in the world of science and math. Noether had to teach without official recognition on several occasions in her life; as a woman in Germany in the early 20th century, she needed to get special permission even to study her subject. Thankfully, we’ve gotten past that blindness in many countries, but there are still nations where women are denied basic educational opportunities. How many Emmy Noethers might there be, who are lacking the opportunity to excel in a field to which they are denied access by restrictive cultural norms?

Here and there a cygnet is reared uneasily among the ducklings in the brown pond, and never finds the living stream in fellowship with its own oary-footed kind. Here and there is born a Saint Theresa, foundress of nothing, whose loving heart-beats and sobs after an unattained goodness tremble off and are dispersed among hindrances, instead of centring in some long-recognizable deed. — George Eliot, “Middlemarch”


6 responses to “On Symmetry and Emmy Noether”

  1. […] relativity led to innovations in particle physics—specifically the Yang-Mills theory, which underlies our understanding of the nuclear forces. Even though he was slow to come around on cosmology and the expansion of the universe, […]

  2. […] I honor scientists on their birthdays (or in one case, on my birthday), but today I want to honor Harry Houdini (1874-1936). Known best as a magician and escapologist, […]

  3. […] than he is — even when writing on the same topics — but he gets it right with a lot less windiness. Click on the panel to the right to see the whole […]

  4. […] are reasonable. Curie was an outstanding scientist by any standard, as was Lise Meitner, as was Emmy Noether. But here’s the deal: each one of those women stood head and shoulders above the vast […]

  5. […] Emmy Noether and her theorem: if there is a symmetry in energy between two states, there must be a symmetry in time too. […]

  6. […] Although I’ve done a lot of computer programming, I’m not a computer scientist, so I’ll leave others to talk about Ada and her colleagues. As a theoretical physicist with a highly mathematical focus, I will instead highlight a mathematician who is famous among physicists but not well known among the general public: Emmy Noether. (This post ran in a slightly different version on March 8 of this year.) […]

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