254 research outputs found
Leading Gravitational Corrections and a Unified Universe
Leading order gravitational corrections to the Einstein-Hilbert action can
lead to a consistent picture of the universe by unifying the epochs of
inflation and dark energy in a single framework. While the leading local
correction induces an inflationary phase in the early universe, the leading
non-local term leads to an accelerated expansion of the universe at the present
epoch. We argue that both the leading UV and IR terms can be obtained within
the framework of a covariant effective field theory of gravity. The
perturbative gravitational corrections therefore provide a fundamental basis
for understanding a possible connection between the two epochs.Comment: 5 pages, 2 figures. This essay received "Honorable Mention" in the
2016 Gravity Research Foundation Awards for Essays on Gravitation. arXiv
admin note: substantial text overlap with arXiv:1603.0002
Generation of scale invariant magnetic fields in bouncing universes
We consider the generation of primordial magnetic fields in a class of
bouncing models when the electromagnetic action is coupled non-minimally to a
scalar field that, say, drives the background evolution. For scale factors that
have the power law form at very early times and non-minimal couplings which are
simple powers of the scale factor, one can easily show that scale invariant
spectra for the magnetic field can arise before the bounce for certain values
of the indices involved. It will be interesting to examine if these power
spectra retain their shape after the bounce. However, analytical solutions for
the Fourier modes of the electromagnetic vector potential across the bounce are
difficult to obtain. In this work, with the help of a new time variable that we
introduce, which we refer to as the --fold, we investigate
these scenarios numerically. Imposing the initial conditions on the modes in
the contracting phase, we numerically evolve the modes across the bounce and
evaluate the spectra of the electric and magnetic fields at a suitable time
after the bounce. As one could have intuitively expected, though the complete
spectra depend on the details of the bounce, we find that, under the original
conditions, scale invariant spectra of the magnetic fields do arise for
wavenumbers much smaller than the scale associated with the bounce. We also
show that magnetic fields which correspond to observed strengths today can be
generated for specific values of the parameters. But, we find that, at the
bounce, the backreaction due to the electromagnetic modes that have been
generated can be significantly large calling into question the viability of the
model. We briefly discuss the implications of our results.Comment: v1: 19 pages, 5 figures; v2: 20 pages, 5 figures, minor revisions, to
appear in JCA
On the non-Gaussian correlation of the primordial curvature perturbation with vector fields
We compute the three-point cross-correlation function of the primordial
curvature perturbation generated during inflation with two powers of a vector
field in a model where conformal invariance is broken by a direct coupling of
the vector field with the inflaton. If the vector field is identified with the
electromagnetic field, this correlation would be a non-Gaussian signature of
primordial magnetic fields generated during inflation. We find that the signal
is maximized for the flattened configuration where the wave number of the
curvature perturbation is twice that of the vector field and in this limit, the
magnetic non-linear parameter becomes as large as |b_{NL}| ~ 10^3. In the
squeezed limit where the wave number of the curvature perturbation vanishes,
our results agree with the magnetic consistency relation derived in
arXiv:1207.4187.Comment: 18 pages. V3: some typos fixed, matches version published in JCA
Effective chemical potential in spontaneous baryogenesis
Models of spontaneous baryogenesis have an interaction term
in the Lagrangian, where is the baryonic
current and can be a pseudo-Nambu-Goldstone boson. Since the time
component of this term, , equals for a
spatially homogeneous current, it is usually argued that this term implies a
splitting in the energy of baryons and antibaryons thereby providing an
effective chemical potential for baryon number. In thermal equilibrium, one
{then obtains} . We however argue that a term of
this form in the Lagrangian does not contribute to the single particle energies
of baryons and antibaryons. We show this for both fermionic and scalar baryons.
But, similar to some recent work, we find that despite the above result the
baryon number density obtained from a Boltzmann equation analysis can be
proportional to . Our arguments are very different from that
in the standard literature on spontaneous baryogenesis.Comment: 16 pages, matches with the published versio
Radiative Corrections from Heavy Fast-Roll Fields during Inflation
We investigate radiative corrections to the inflaton potential from heavy
fields undergoing a fast-roll phase transition. We find that a logarithmic
one-loop correction to the inflaton potential involving this field can induce a
temporary running of the spectral index. The induced running can be a short
burst of strong running, which may be related to the observed anomalies on
large scales in the cosmic microwave spectrum, or extend over many e-folds,
sustaining an effectively constant running to be searched for in the future. We
implement this in a general class of models, where effects are mediated through
a heavy messenger field sitting in its minimum. Interestingly, within the
present framework it is a generic outcome that a large running implies a small
field model with a vanishing tensor-to-scalar ratio, circumventing the normal
expectation that small field models typically lead to an unobservable small
running of the spectral index. An observable level of tensor modes can also be
accommodated, but, surprisingly, this requires running to be induced by a
curvaton. If upcoming observations are consistent with a small tensor-to-scalar
ratio as predicted by small field models of inflation, then the present study
serves as an explicit example contrary to the general expectation that the
running will be unobservable.Comment: 35 pages, 4 figures, matches published versio
Cosmological Ohm's law and dynamics of non-minimal electromagnetism
The origin of large-scale magnetic fields in cosmic structures and the
intergalactic medium is still poorly understood. We explore the effects of
non-minimal couplings of electromagnetism on the cosmological evolution of
currents and magnetic fields. In this context, we revisit the mildly non-linear
plasma dynamics around recombination that are known to generate weak magnetic
fields. We use the covariant approach to obtain a fully general and non-linear
evolution equation for the plasma currents and derive a generalised Ohm law
valid on large scales as well as in the presence of non-minimal couplings to
cosmological (pseudo-)scalar fields. Due to the sizeable conductivity of the
plasma and the stringent observational bounds on such couplings, we conclude
that modifications of the standard (adiabatic) evolution of magnetic fields are
severely limited in these scenarios. Even at scales well beyond a Mpc, any
departure from flux freezing behaviour is inhibited.Comment: 24 pages, 2 figures; matches version published in JCA
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