John Carlos Baez on Nostr: I've been talking about how a classical particle in an inverse square force law, like ...
I've been talking about how a classical particle in an inverse square force law, like the Earth orbiting the Sun, can secretly be seen as a particle moving at the speed of light on a sphere in 4-dimensional space.
That's already cool. But the same story also works in quantum mechanics, like for an electron orbiting a proton in a hydrogen atom!
There are various ways to show this is true. I'll take a brutally efficient approach. I’ll start with wavefunctions on a sphere in 4d space and describe operators on these arising from rotational symmetries. Combining these with standard facts about the hydrogen atom, we can set up a correspondence between such wavefunctions and bound states of a hydrogen atom — that is, states where the electron orbits the proton, instead of flying off.
Here’s how. Chemists use a basis of bound states of the hydrogen atom called |𝑛,ℓ,𝑚〉where
• n tells us the energy of the state,
• ℓ tells us its total angular momentum, and
• m tells us its angular momentum around the z axis.
(For now we’re ignoring the electron’s spin: I'll bring that in later.) In this blog article, I'll show that wavefunctions on the sphere in 4-dimensional space *also* have a nice basis of states called |𝑛,ℓ,𝑚〉. This will let us match up hydrogen atom bound states and wavefunctions on a sphere in 4d space.
So the most basic element turns out to be 4-dimensional, in a sense.
https://johncarlosbaez.wordpress.com/2025/07/23/the-kepler-problem-part-5/Published at
2025-07-23 09:13:36 UTCEvent JSON
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"content": "I've been talking about how a classical particle in an inverse square force law, like the Earth orbiting the Sun, can secretly be seen as a particle moving at the speed of light on a sphere in 4-dimensional space. \n\nThat's already cool. But the same story also works in quantum mechanics, like for an electron orbiting a proton in a hydrogen atom! \n\nThere are various ways to show this is true. I'll take a brutally efficient approach. I’ll start with wavefunctions on a sphere in 4d space and describe operators on these arising from rotational symmetries. Combining these with standard facts about the hydrogen atom, we can set up a correspondence between such wavefunctions and bound states of a hydrogen atom — that is, states where the electron orbits the proton, instead of flying off.\n\nHere’s how. Chemists use a basis of bound states of the hydrogen atom called |𝑛,ℓ,𝑚〉where\n\n• n tells us the energy of the state,\n• ℓ tells us its total angular momentum, and\n• m tells us its angular momentum around the z axis.\n\n(For now we’re ignoring the electron’s spin: I'll bring that in later.) In this blog article, I'll show that wavefunctions on the sphere in 4-dimensional space *also* have a nice basis of states called |𝑛,ℓ,𝑚〉. This will let us match up hydrogen atom bound states and wavefunctions on a sphere in 4d space.\n\nSo the most basic element turns out to be 4-dimensional, in a sense.\n\nhttps://johncarlosbaez.wordpress.com/2025/07/23/the-kepler-problem-part-5/",
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