It is a remarkable result of differential geometry that certain global features of a
spacetime manifold are determined by some local invariant densities. These topological invariants
have an important property in common. They are total divergences and in any local theory,
these invariants, when treated as Lagrangian densities, contribute nothing to the
Euler-Lagrange equations.
Hence in a local theory only a few parts, not the whole part, of these invariants can
be kept in a Lagrangian density. A gravitational Lagrangian was proposed in this
direction sometime ago (Mahato, 2002), where a Lorentz invariant part of the de Sitter
Pontryagin density, i.e., having broken de Sitter symmetry, was treated as the Einstein-Hilbert
Lagrangian. In this way the role of torsion in the underlying spacetime manifold has become
multiplicative rather than additive one and the Lagrangian looks like torsion curvature. In other
words—the additive torsion is decoupled from the theory but not the multiplicative one. This
indicates that torsion is uniformly nonzero everywhere. In the geometrical sense, this implies
that micro local spacetime is such that, at every point there is a direction vector (vortex
line) attached to it. This effectively corresponds to the noncommutative geometry having
the manifold M4 x Z2, where the discrete space Z2 is just not the two point space (Connes,
1994) but appears as an attached direction vector. This has direct relevance in the quantization
of a fermion where the discrete space appears as the internal space of a particle (Ghosh
and Bandyopadhyay, 2000).
Considering torsion and torsion-less connections as independent
fields (Mahato, 2004), it has been found that K of Einstein-Hilbert Lagrangian appears as an
integration constant in such a way that it has been found to be linked with the topological
Nieh-Yan density of U4 space. If we consider axial vector torsion, together with a scalar field connected to a local scale factor (Mahato, 2005 and 2007a), then the Euler-Lagrange equations not
only give the constancy of the gravitational constant, but they also the link, in laboratory
scale, the mass of the scalar field with the Nieh-Yan density and, in cosmic scale of
FRW-cosmology, they predict only three kinds of the phenomenological energy density representing
mass, radiation and cosmological constant. Recently, it has been shown that (Mahato, 2007b)
using field equations of all fields except the frame field, the starting Lagrangian reduces to
a generic f (R) gravity Lagrangian which, for FRW metric, gives standard FRW cosmology. |