8,479 research outputs found
Inflationary paradigm after Planck 2013
Models of cosmic inflation posit an early phase of accelerated expansion of
the universe, driven by the dynamics of one or more scalar fields in curved
spacetime. Though detailed assumptions about fields and couplings vary across
models, inflation makes specific, quantitative predictions for several
observable quantities, such as the flatness parameter ()
and the spectral tilt of primordial curvature perturbations (), among others---predictions that match the latest
observations from the {\it Planck} satellite to very good precision. In the
light of data from {\it Planck} as well as recent theoretical developments in
the study of eternal inflation and the multiverse, we address recent criticisms
of inflation by Ijjas, Steinhardt, and Loeb. We argue that their conclusions
rest on several problematic assumptions, and we conclude that cosmic inflation
is on a stronger footing than ever before.Comment: 11 pages, no figures; added references, and brief additions to
Footnote 1, Section VI, and the Acknowledgment
Relativistic Corrections to Nonrelativistic Effective Field Theories
In this paper we develop a formalism for studying the nonrelativistic limit
of relativistic field theories in a systematic way. By introducing a simple,
nonlocal field redefinition, we transform a given relativistic theory,
describing a real, self-interacting scalar field, into an equivalent theory,
describing a complex scalar field that encodes at each time both the original
field and its conjugate momentum. Our low-energy effective theory incorporates
relativistic corrections to the kinetic energy as well as the backreaction of
fast-oscillating terms on the behavior of the dominant, slowly varying
component of the field. Possible applications of our new approach include axion
dark matter, though the methods developed here should be applicable to the
low-energy limits of other field theories as well.Comment: 31pp. References added, and 3 appendices added, showing (a) how to
implement the field redefinition as a canonical transformation, (b) how to
develop the effective field theory using a local field redefinition, and (c)
how to use a further field redefinition to compare our results with those of
Mukaida, Takimoto, and Yamad
Inflationary Cosmology: Exploring the Universe from the Smallest to the Largest Scales
Understanding the behavior of the universe at large depends critically on
insights about the smallest units of matter and their fundamental interactions.
Inflationary cosmology is a highly successful framework for exploring these
interconnections between particle physics and gravitation. Inflation makes
several predictions about the present state of the universe -- such as its
overall shape, large-scale smoothness, and smaller-scale structure -- which are
being tested to unprecedented accuracy by a new generation of astronomical
measurements. The agreement between these predictions and the latest
observations is extremely promising. Meanwhile, physicists are busy trying to
understand inflation's ultimate implications for the nature of matter, energy,
and spacetime.Comment: 16 pages, 4 figures, written for "Einstein's Legacy" issue of Science
magazin
Wavelet Methods in the Relativistic Three-Body Problem
In this paper we discuss the use of wavelet bases to solve the relativistic
three-body problem. Wavelet bases can be used to transform momentum-space
scattering integral equations into an approximate system of linear equations
with a sparse matrix. This has the potential to reduce the size of realistic
three-body calculations with minimal loss of accuracy. The wavelet method leads
to a clean, interaction independent treatment of the scattering singularities
which does not require any subtractions.Comment: 14 pages, 3 figures, corrected referenc
Electromagnetic vortex lines riding atop null solutions of the Maxwell equations
New method of introducing vortex lines of the electromagnetic field is
outlined. The vortex lines arise when a complex Riemann-Silberstein vector
is multiplied by a complex scalar function
. Such a multiplication may lead to new solutions of the Maxwell
equations only when the electromagnetic field is null, i.e. when both
relativistic invariants vanish. In general, zeroes of the function give
rise to electromagnetic vortices. The description of these vortices benefits
from the ideas of Penrose, Robinson and Trautman developed in general
relativity.Comment: NATO Workshop on Singular Optics 2003 To appear in Journal of Optics
Electromagnetic inertia, reactive energy, and energy flow velocity
In a recent paper titled "Coherent electromagnetic wavelets and their
twisting null congruences," I defined the local inertia density (I), reactive
energy density (R), and energy flow velocity (v) of an electromagnetic field.
These are the field equivalents of the mass, rest energy, and velocity of a
relativistic particle. Thus R and I are Lorentz-invariant and |v|<=c, with
equality if and only if R=0. The exceptional fields with |v|=c were called
"coherent" because their energy moves in complete harmony with the field,
leaving no inertia or reactive energy behind. Generic electromagnetic fields
become coherent only in the far zone. Elsewhere, their energy flows at speeds
|v|<c. The purpose of this paper is to confirm and clarify this statement by
studying the local energy flow in several common systems: a time-harmonic
electric dipole field, a time-dependent electric dipole field, and a standing
plane wave. For these fields, the energy current (Poynting vector) is too weak
to carry away all of the energy, thus leaving reactive energy in its wake. For
the time-dependent dipole field, we find that the energy can flow both
transversally and inwards, back to the source. Neither of these phenomena show
up in the usual computation of the energy transport velocity which considers
only averages over one period in the time-harmonic case.Comment: 20 pages, 7 figure
Maxwell Fields and Shear-Free Null Geodesic Congruences
We study and report on the class of vacuum Maxwell fields in Minkowski space
that possess a non-degenerate, diverging, principle null vector field (null
eigenvector field of the Maxwell tensor) that is tangent to a shear-free null
geodesics congruence. These congruences can be either surface forming (the
tangent vectors proportional to gradients) or not, i.e., the twisting
congruences. In the non-twisting case, the associated Maxwell fields are
precisely the Lienard-Wiechert fields, i.e., those Maxwell fields arising from
an electric monopole moving on an arbitrary worldline. The null geodesic
congruence is given by the generators of the light-cones with apex on the
world-line. The twisting case is much richer, more interesting and far more
complicated. In a twisting subcase, where our main interests lie, it can be
given the following strange interpretation. If we allow the real Minkowski
space to be complexified so that the real Minkowski coordinates x^a take
complex values, i.e., x^a => z^a=x^a+iy^a with complex metric g=eta_abdz^adz^b,
the real vacuum Maxwell equations can be extended into the complex and
rewritten as curlW =iWdot, divW with W =E+iB. This subcase of Maxwell fields
can then be extended into the complex so as to have as source, a complex
analytic world-line, i.e., to now become complex Lienard-Wiechart fields. When
viewed as real fields on the real Minkowski space, z^a=x^a, they possess a real
principle null vector that is shear-free but twisting and diverging. The twist
is a measure of how far the complex world-line is from the real 'slice'. Most
Maxwell fields in this subcase are asymptotically flat with a time-varying set
of electric and magnetic moments, all depending on the complex displacements
and the complex velocities.Comment: 3
Interplay between disorder, quantum and thermal fluctuations in ferromagnetic alloys: The case of UCu2Si(2-x)Ge(x)
We consider, theoretically and experimentally, the effects of structural
disorder, quantum and thermal fluctuations in the magnetic and transport
properties of certain ferromagnetic alloys.We study the particular case of
UCu2Si(2-x)Ge(x). The low temperature resistivity, rho(T,x), exhibits Fermi
liquid (FL) behavior as a function of temperature T for all values of x, which
can be interpreted as a result of the magnetic scattering of the conduction
electrons from the localized U spins. The residual resistivity, rho(0,x),
follows the behavior of a disordered binary alloy. The observed non-monotonic
dependence of the Curie temperature, Tc(x), with x can be explained within a
model of localized spins interacting with an electronic bath whose transport
properties cross-over from ballistic to diffusive regimes. Our results clearly
show that the Curie temperature of certain alloys can be enhanced due to the
interplay between quantum and thermal fluctuations with disorder.Comment: 4 pages, 3 figures, to appear in Phys. Rev. Let
One-dimensional transport in polymer nanofibers
We report our transport studies in quasi one-dimensional (1D) conductors -
helical polyacetylene fibers doped with iodine and the data analysis for other
polymer single fibers and tubes. We found that at 30 K < T < 300 K the
conductance and the current-voltage characteristics follow the power law: G(T)
~ T^alpha with alpha ~ 2.2-7.2 and I(V) ~ V^betta with betta ~ 2-5.7. Both G(T)
and I(V) show the features characteristic of 1D systems such as Luttinger
liquid or Wigner crystal. The relationship between our results and theories for
tunneling in 1D systems is discussed.Comment: 11 pages, 3 figures, accepted for publication in Phys. Rev. Letter
Integrated Diamond Optics for Single Photon Detection
Optical detection of single defect centers in the solid state is a key
element of novel quantum technologies. This includes the generation of single
photons and quantum information processing. Unfortunately the brightness of
such atomic emitters is limited. Therefore we experimentally demonstrate a
novel and simple approach that uses off-the-shelf optical elements. The key
component is a solid immersion lens made of diamond, the host material for
single color centers. We improve the excitation and detection of single
emitters by one order of magnitude, as predicted by theory.Comment: 10 pages, 3 figure
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