"Specifically, the observable sector is N=1 supersymmetric with gauge group SU(3)_C x SU(2)_L x U(1)_Y x U(1)_{B-L}, three families of quarks and leptons, each family with a right-handed neutrino, and one Higgs-Higgs conjugate pair."
@Slereah I think there's a weird tendency where string theorists are often not actually interested in "realistic models"? It's weird and I often don't quite understand why they study the models they do
I knew there was a 10 second derivation of a general lorentz transform somewhere, finally... $\Lambda x = [\cosh(\theta) t + \sinh(\theta) \mathbf{n} \cdot \mathbf{x} \ , \ \mathbf{x} + (\cosh(\theta) - 1) \mathbf{n} (\mathbf{n} \cdot \mathbf{x}) + \sinh(\theta) \mathbf{n} t ]^T$
Incredibly terrifying when you see it just stated in Jackson
'a phenomenological string theory was proposed based on qualitative topology and hypercomplex numbers. The current presentation takes this further by delving into the ancient Chinese origin of phenomenological string theory'