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Topology Through Peaks, Passes, and Pits: Exploring Quantum Mechanics and Mathematical Connections

Explore the fascinating world of topology through peaks, passes, and pits in the context of quantum mechanics. Discover how the Euler characteristic, Hodge equations, and Morse theory tie together in a seamless web of mathematical relationships. From Maxwell's equations to perturbation theory, delve into the intricate interplay between critical points and topological properties.

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Topology Through Peaks, Passes, and Pits: Exploring Quantum Mechanics and Mathematical Connections

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  1. Peaks, Passes and Pits From Topography to Topology (via Quantum Mechanics)

  2. James Clerk Maxwell, 1831-1879

  3. 1861 – “On Physical Lines of Force” • 1864 – “On the Dynamical Theory of the Electromagnetic Field” • 1870 – “On Hills and Dales” • hilldale.pdf

  4. Scottish examples

  5. Peak Pass Pit

  6. Critical points of a function on a surface • Peaks (local maxima) • Passes (saddle points) • Pits (local minima) • Can identify by looking at 2nd derivative • “Topology only changes when we pass through a critical point”.

  7. Basic theorem • (# Peaks) – (# Passes) + (# Pits) = Euler Characteristic (V-E+F) • Euler Characteristic is a topological invariant; 2 for the sphere; 0 for the torus. • Does not depend on which Morse function we choose!

  8. The Hodge equations • The Euler characteristic can also be obtained by counting solutions to certain partial differential equations – the “Hodge equations”. • They are geometrical analogs of Maxwell’s equations! • To see how PDE can relate to topology, think about vector fields and potentials…

  9. The physics connection Ed Witten, Supersymmetry and Morse Theory, 1982

  10. Witten’s method • Consider the Hodge equation as a quantum mechanical Hamiltonian. • Different types of ‘particle’ according to the Morse index (‘peakons, passons and pitons’). • Euler characteristic given by counting the low energy states of these particles.

  11. Perturbation theory • Replace d by eshd e-sh, where h is the Morse function and s is a real parameter. • This perturbation does not change the number of low energy states. • But it does change the Hodge equations!

  12. In fact, it introduces a potential term, which forces our particles to congregate near the critical points of appropriate index. • The potential is s2|h|2 + sXh where Xh is a zero order vectorial term.

  13. The term Xh has a ‘zero point energy’ effect which forces each type of particle to congregate near the critical points of the appropriate index; ‘peakons’ near peaks, ‘passons’ near passes and so on.

  14. Thus the number of low energy n-on modes approaches the number of critical points of index n, as the parameter s becomes large. • Appropriately formulated, this proves the fundamental result of Morse theory; peaks – passes + pits = Euler characteristic.

  15. James Clerk Maxwell, 1831-1879

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