"An effective two dimensionality" cases bring a new hope to the Kaluza-Klein[like] theories
arXiv:1001.4679 · doi:10.1088/1367-2630/13/10/103027
Abstract
One step towards realistic Kaluza-Klein[like] theories and a loop hole through the Witten's "no-go theorem" is presented for cases which we call an effective two dimensionality cases: In the equations of motion following from the action with the linear curvature leave spin connections and zweibeins undetermined. We present the case of a spinor in compactified on a formally infinite disc with the zweibein which makes a disc curved on an almost and with the spin connection field which allows on such a sphere only one massless normalizable spinor state of a particular charge, which couples the spinor chirally to the corresponding Kaluza-Klein gauge field. We assume no external gauge fields. The masslessness of a spinor is achieved by the choice of a spin connection field (which breaks parity), the zweibein and the normalizability condition for spinor states, which guarantee a discrete spectrum forming the complete basis. We discuss the meaning of the hole, which manifests the noncompactness of the space.
26 pages, 1 figure, an addition which helps to clarify the assumptions and their consequences (the discreteness of spectrum, the massless solution of one handedness,..)
References in corpus (6)
- On the origin of families of fermions and their mass matrices
- On the origin of families of quarks and leptons - predictions for four families
- Fermions with no fundamental charges call for extra dimensions
- An example of Kaluza-Klein-like theory with boundary conditions, which lead to massless and mass protected spinors chirally coupled to gauge fields
- Particular boundary condition ensures that a fermion in d=1+5, compactified on a finite disk, manifests in d=1+3 as massless spinor with a charge 1/2, mass protected and chirally coupled to the gauge field
- A new understanding of fermion masses from the unified theory of spins and charges
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