7/15. Spin(11,1) string theory

Weak and color strings attach to Calabi-Yau five-fold embedded in 3+1 large spacetime dimensions Not a direct product of internal and spacetime manifolds.

Accomodates 10 internal and 3+1 large spacetime dimensions inside 11+1 dimensions.

The 4 weak vectors \(\hat{\boldsymbol{\gamma}}^\pm_k\), \(k = {\color{silver}{y}} , {\color{bronze}{z}} \), Lorentz transform like Dirac vector \(\boldsymbol{\gamma}_3\).
The 6 color vectors \(\hat{\boldsymbol{\gamma}}^\pm_k\), \(k = {\color{red}{r}} , {\color{dgreen}{g}} , {\color{blue}{b}} \), Lorentz transform like Dirac vector \(\boldsymbol{\gamma}_1\).

Fermat surface The 4 weak and 6 color vectors form a 10d compact complex manifold, a D10-brane, which carries the \(2^6\) spinors of \(\textrm{Spin}(11,1)\). The internal complex structure is generated by the color pseudoscalar \(I_{\color{red}{r}\color{dgreen}{g}\color{blue}{b}}\).

The weak and color gauge fields of the standard model are carried by bosonic open strings whose ends attach to D4 weak and D6 color subbranes of the fermionic D10-brane.

After symmetry breaking to the standard model (which is a subgroup of \(\textrm{SU}(5)\)), the compact internal fermionic D10-brane becomes a 10d Calabi-Yau five-fold. A Calabi-Yau \(n\)-fold is a complex manifold with \(\textrm{SU}(n)\) holonomy. A Calabi-Yau \(n\)-fold has the key property that it carries zero internal energy-momentum.

 -> 8/15. Compactification from 26 to 12 dimensions on 14 dimensional SU(8)×SU(8) torus
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