Geometry of Spin(10) Symmetry Breaking

Abstract

We provide a new characterisation of the Standard Model gauge group GSM as a subgroup of Spin(10). The new description of GSM relies on the geometry of pure spinors. We show that GSM is the subgroup that stabilises a pure spinor Psi1 and projectively stabilises another pure spinor Psi2, with Psi1, Psi2 orthogonal and such that their arbitrary linear combination is still a pure spinor. Our characterisation of GSM relies on the facts that projective pure spinors describe complex structures on R10, and the product of two commuting complex structures is a what is known as a product structure. For the pure spinors Psi1, Psi2 satisfying the stated conditions the complex structures determined by Psi1, Psi2 commute and the arising product structure is R10 = R6 + R4, giving rise to a copy of Pati-Salam gauge group inside Spin(10). Our main statement then follows from the fact that GSM is the intersection of the Georgi-Glashow SU(5) that stabilises Psi1, and the Pati-Salam Spin(6) x Spin(4) arising from the product structure determined by Psi1, Psi2. We have tried to make the paper self-contained and provided a detailed description of the creation/annihilation operator construction of the Clifford algebras Cl(2n) and the geometry of pure spinors in dimensions up to and including ten.

0

Turn this paper into a lesson

ArcXiv compiles a structured reading guide from this paper's metadata: plain-English importance, contributions, prerequisite concepts, which sections to read first, flashcards, and a quiz. Grounded in the abstract, never invented.

Discussion (0)

Sign in to join the discussion.

Loading comments…