Re: Dimensions
silus wrote:I was just wondering how many dimensions there are? Personally i only believe in the 4 but i read something recently that involved something with 248 dimensions. Can anyone shed any light on the subject?
Silus - what was the model with the 248 dimensions? If you're referring to E8 (Lie algebra) it doesn't really have 248 dimensions: the underlying dimensions never exceed 8 (eight) in any notional sense (the number 248 is just the number of roots to the equations involved, i.e. not real dimensions).
http://aimath.org/E8/e8.html
That's why it's called E8 to begin with
If you'd like something more advanced, these are 2 reasonably recent papers; not sure if they help with your question:
Quote:
1. On a Unified Theory of Generalized Branes Coupled to Gauge Fields, Including the Gravitational and Kalb-Ramond Fields.
By: Pavič, M.. Foundations of Physics, Aug2007, Vol. 37 Issue 8, p1197-1242, 46p; DOI: 10.1007/s10701-007-9147-3; (AN 26553650)
2. On the noncommutative and nonassociative geometry of octonionic space time, modified dispersion relations and grand unification.
By: Castro, Carlos. Journal of Mathematical Physics, Jul2007, Vol. 48 Issue 7, pN.PAG, 15p; DOI: 10.1063/1.2752013; (AN 25997800)
I'm posting abstracts of both papers as you may not be able to find them online:
1. We investigate a theory in which fundamental objects are branes described in terms of higher grade coordinates [.....] extend the notion of geometry from spacetime to that of an enlarged space, called Clifford space or C-space. If we start from four-dimensional spacetime, then the dimension of C-space is 16. The fact that C-space has more than four dimensions suggests that it could serve as a realization of Kaluza-Klein idea. The "extra dimensions" are not just the ordinary extra dimensions, they are related to the volume degrees of freedom, therefore they are physical, and need not be compactified. Gauge fields are due to the metric of Clifford space. It turns out that amongst the latter gauge fields there also exist higher grade, antisymmetric fields of the Kalb-Ramond type, and their non-Abelian generalization. All those fields are naturally coupled to the generalized branes, whose dynamics is given by a generalized Howe-Tucker action in curved C-space.
2. The octonionic geometry (gravity) ......... is extended to noncommutative and nonassociative space time coordinates associated with octonionic-valued coordinates and momenta. [.........] the energy-momentum dispersion relations without violating Lorentz invariance as it occurs with Hopf algebraic deformations of the Poincare algebra. The known octonionic realizations of the Clifford Cl(8), Cl(4) algebras should permit the construction of octonionic string actions that should have a correspondence with ordinary string actions for strings moving in a curved Clifford-space target background associated with a Cl(3, 1) algebra.