Define the discrete symmetry operator acting on second-kind boson basis vectors
Determine and formalize the discrete symmetry operator that acts on the second-kind even bosonic basis vectors A^{II}_{f} (the boson “basis vectors” that transform a given family member across families), and characterize its transformation properties and algebraic action on these basis vectors in the framework presented for even-dimensional spaces (e.g., d = 5 + 1 and d = 13 + 1).
References
The discrete symmetry operator (C P N N (d−1))b operating on the second kind of boson “basis vectors” needs further study and will be discussed in a separate paper.
— Can the "basis vectors", describing the internal spaces of fermion and boson fields with the Clifford odd (for fermion) and Clifford even (for boson) objects, explain interactions among fields, with gravitons included?
(2407.09482 - Borštnik, 10 May 2024) in Section 3.1, after Eq. (26)