739 research outputs found
A non-geodesic motion in the R^-1 theory of gravity tuned with observations
In the general picture of high order theories of gravity, recently, the R^-1
theory has been analyzed in two different frameworks. In this letter a third
context is added, considering an explicit coupling between the R^-1 function of
the Ricci scalar and the matter Lagrangian. The result is a non-geodesic motion
of test particles which, in principle, could be connected with Dark Matter and
Pioneer anomaly problems.Comment: Accepted for Modern Physics Letters
f(R) Gravity, relic coherent gravitons and optical chaos
We discuss the production of massive relic coherent gravitons in a particular
class of f(R) gravity which arises from string theory and their possible
imprint in Cosmic Microwave Background. In fact, in the very early universe
these relic gravitons could have acted as slow gravity waves. They may have
then acted to focus the geodesics of radiation and matter. Therefore, their
imprint on the later evolution of the universe could appear as filaments and
domain wall in the Universe today. In that case, the effect on Cosmic Microwave
Background should be analogous to the effect of water waves, which, in focusing
light, create optical caustics which are commonly seen on the bottom of
swimming pools. We analyze this important issue by showing how relic massive
GWs perturb the trajectories of Cosmic Microwave Background photons
(gravitational lensing by relic GWs). The consequence of the type of physics
discussed is outlined by illustrating an amplification of what might be called
optical chaos.Comment: 32 pages, 1 figure, invited paper to appear in "Beyond Standard
Gravity and Cosmology", special issue of "Galaxies" edited by Antonaldo
Diaferi
Interferometer Response to Scalar Gravitational Waves
It was recently suggested that the magnetic component of Gravitational Waves
(GWs) is relevant in the evaluation of frequency response functions of
gravitational interferometers. In this paper we extend the analysis to the
magnetic component of the scalar mode of GWs which arise from scalar-tensor
gravity theory. In the low-frequency approximation, the response function of
ground-based interferometers is calculated. The angular dependence of the
electric and magnetic contributions to the response function is discussed.
Finally, for an arbitrary frequency range, the proper distance between two test
masses is calculated and its usefulness in the high-frequency limit for
space-based interferometers is briefly considered.Comment: Accepted for publication by Int. Journ. Mod. Phys. D. Final versio
A precise response function for the magnetic component of Gravitational Waves in Scalar-Tensor Gravity
The important issue of the magnetic component of gravitational waves (GWs)
has been considered in various papers in the literature. From such analyses, it
resulted that such a magnetic component becomes particularly important in the
high frequency portion of the frequency range of ground based interferometers
for GWs which arises from standard General Theory of Relativity (GTR).
Recently, such a magnetic component has been extended to GWs arising from
Scalar-Tensor Gravity (STG) too. After a review of some important issues on GWs
in STG, in this paper we re-analyse the magnetic component in the framework of
STG from a different point of view, by correcting an error in a previous paper
and by releasing a more precise response function. In this way, we also show
that if one neglects the magnetic contribution considering only the
low-frequency approximation of the electric contribution, an important part of
the signal could be, in principle, lost. The determination of a more precise
response function for the magnetic contribution is important also in the
framework of the possibility to distinguish other gravitational theories from
GTR. At the end of the paper an expansion of the main results is also shown in
order to recall the presence of the magnetic component in GRT too.Comment: Accepted for publication in Physical Review D, to be published during
2011. 36 pages, in this second version typos have been corrected and
references have been update
Some exact solutions of F(R) gravity with charged (a)dS black hole interpretation
In this paper we obtain topological static solutions of some kind of pure
gravity. The present solutions are two kind: first type is uncharged
solution which corresponds with the topological (a)dS Schwarzschild solution
and second type has electric charge and is equivalent to the
Einstein--conformally invariant Maxwell solution. In other word,
starting from pure gravity leads to (charged) Einstein- solutions
which we interpreted them as (charged) (a)dS black hole solutions of pure
gravity. Calculating the Ricci and Kreschmann scalars show that there is
a curvature singularity at . We should note that the Kreschmann scalar of
charged solutions goes to infinity as , but with a rate slower
than that of uncharged solutions.Comment: 21 pages, 4 figures, generalization to higher dimensions, references
adde
The Friedmann-Lemaitre-Robertson-Walker Big Bang singularities are well behaved
We show that the Big Bang singularity of the
Friedmann-Lemaitre-Robertson-Walker model does not raise major problems to
General Relativity. We prove a theorem showing that the Einstein equation can
be written in a non-singular form, which allows the extension of the spacetime
before the Big Bang. The physical interpretation of the fields used is
discussed. These results follow from our research on singular semi-Riemannian
geometry and singular General Relativity.Comment: 10 pages, 5 figure
Tyrosinase Inhibitor Activity of Coumarin-Resveratrol Hybrids
In the present work we report on the contribution of the coumarin moiety to
tyrosinase inhibition. Coumarin-resveratrol hybrids 1-8 have been resynthesized to
investigate the structure-activity relationships and the IC50 values of these compounds
were measured. The results showed that these compounds exhibited tyrosinase inhibitory
activity. Compound 3-(3’,4’,5’-trihydroxyphenyl)-6,8-dihydroxycoumarin (8) is the most
potent compound (0.27 mM), more so than umbelliferone (0.42 mM), used as reference
compound. The kinetic studies revealed that compound 8 caused non-competitive
tyrosinase inhibition
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