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Spin representations, Spin representation periodicity

Bott Periodicity Models the Assembly of Mental Contexts

Abstract

The Folk Dance

The mechanism of Bott periodicity.

Given {$N$} dancers (or perspectives or dimensions or agents)

  • Pair up the dancers into couples. There may be one dancer left over.
  • Line up the couples from left to right: {$c_1, \dots, c_m$}
  • Have adjacent couples swap positions {$c_jc_k\rightarrow c_kc_j$}. where {$j<k$}, until the line is inverted: {$c_m, \dots, c_1$}.

If the number of swaps is even, then we say the dance matches the music, and the dance is a success, but if the number of swaps is odd, then it does not, and the dance is a failure.

We can think of swaps as taking place one after the other. Alternatively, we can think of pairs of swaps occurring together. For this to happen, we need four couples.

Understand

  • Why is the bilinear form {$\beta(s,t)$} important in the case when the irreducible representation is even {$S^+$} or odd {$S^-$} and the overall {$S$} is generated from an odd-dimensional {$W$}?
  • What does it mean when {$\beta(s,t)=0$} for all {$s,t$}?
  • Why are spin representations irreducible (when {$n$} is odd) or reducible (when {$n$} is even)?
  • When matrices satisfy a symmetric bilinear form, why are they orthogonal?
  • When matrices satisfy a skew-symmetric bilinear form, why are they symplectic?
  • Why are these matrices all special linear?

Metaphysical interpretation

Insights from various manifestations of Bott periodicity

Spinor representations

Clifford algebra representations

Mutually anticommuting linear complex structures

Lie group embeddings

Dimensions of Lie groups

Quantum symmetries

Hamiltonians

Super division algebras

Symmetric spaces

Homotopy groups of compact Lie groups

Octonions

{$(\phi, \chi)$}-representations of {$CT$}-groups

Random matrices

Homotopy groups of spheres

References