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Peaks, Passes and Pits

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From Topography to Topology (via Quantum Mechanics) James Clerk Maxwell, 1831-1879 1861 ... On the Dynamical Theory of the Electromagnetic Field 1870 ... – PowerPoint PPT presentation

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Title: Peaks, Passes and Pits


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

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James Clerk Maxwell, 1831-1879
4
  • 1861 On Physical Lines of Force
  • 1864 On the Dynamical Theory of the
    Electromagnetic Field
  • 1870 On Hills and Dales
  • hilldale.pdf

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Scottish examples
7
Peak
Pass
Pit
8
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.

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Basic theorem
  • ( Peaks) ( Passes) ( Pits) Euler
    Characteristic (V-EF)
  • Euler Characteristic is a topological invariant
    2 for the sphere 0 for the torus.
  • Does not depend on which Morse function we choose!

11
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 Maxwells
    equations!
  • To see how PDE can relate to topology, think
    about vector fields and potentials

12
The physics connection
  • Ed Witten, Supersymmetry and Morse Theory, 1982

13
Wittens 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.

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Perturbation theory
  • Replace d by esh d 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!

16
  • In fact, it introduces a potential term, which
    forces our particles to congregate near the
    critical points of appropriate index.
  • The potential is
  • s2?h2 sXh
  • where Xh is a zero order vectorial term.

17
  • 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.

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  • 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.

20
James Clerk Maxwell, 1831-1879
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