27 research outputs found
EGMF Constraints from Simultaneous GeV-TeV Observations of Blazars
Attenuation of the TeV gamma-ray flux from distant blazars through pair
production with extragalactic background light leads to the development of
electromagnetic cascades and subsequent, lower energy, GeV secondary gamma-ray
emission. Due to the deflection of VHE cascade electrons by extragalactic
magnetic fields (EGMF), the spectral shape of this arriving cascade gamma-ray
emission is dependent on the strength of the EGMF. Thus, the spectral shape of
the GeV-TeV emission from blazars has the potential to probe the EGMF strength
along the line of sight to the object. We investigate constraints on the EGMF
derived from observations of blazars for which TeV observations simultaneous
with those by the Fermi telescope were reported. We study the dependence of the
EGMF bound on the hidden assumptions it rests upon. We select blazar objects
for which simultaneous Fermi/LAT GeV and Veritas, MAGIC or HESS TeV emission
have been published. We model the development of electromagnetic cascades along
the gamma-ray beams from these sources using Monte Carlo simulations, including
the calculation of the temporal delay incurred by cascade photons, relative to
the light propagation time of direct gamma-rays from the source. Constraints on
EGMF could be derived from the simultaneous GeV-TeV data on the blazars RGB
J0710+591, 1ES 0229+200, and 1ES 1218+304. The measured source flux level in
the GeV band is lower than the expected cascade component calculated under the
assumption of zero EGMF. Assuming that the reason for the suppression of the
cascade component is the extended nature of the cascade emission, we find that
B>10^{-15} G (assuming EGMF correlation length of ~1 Mpc) is consistent with
the data. Alternatively, the assumption that the suppression of the cascade
emission is caused by the time delay of the cascade photons the data are
consistent with B>10^{-17} G for the same correlation length.Comment: 9 pages, 9 figure
Chemical Descriptors of Yttria-Stabilized Zirconia at Low Defect Concentration: An <i>ab Initio</i> Study
Yttria-stabilized zirconia (YSZ)
is an important oxide ion conductor with applications in solid oxide
fuel cells (SOFCs) and oxygen sensing devices. Doping the cubic phase
of zirconia (c-ZrO<sub>2</sub>) with yttria (Y<sub>2</sub>O<sub>3</sub>) is isoelectronic, as two Zr<sup>4+</sup> ions are replaced by two
Y<sup>3+</sup> ions, plus a charge compensating oxygen vacancy (O<sub>vac</sub>). Typical doping concentrations include 3, 8, 10, and 12
mol %. For these concentrations, and all below 40 mol %, no phase
with long-range order has been observed in either X-ray or neutron
diffraction experiments. The prediction of local defect structure
and the interaction between defects is therefore of great interest.
This has not been possible to date as the number of possible defect
topologies is very large and to perform reliable total energy calculations
for all of them would be prohibitively expensive. Previous theoretical
studies have only considered a selection of representative structures.
In this study, a comprehensive search for low-energy defect structures
using a combined classical modeling and density functional theory
approach is used to identify the low-energy isolated defect structures
at the dilute limit, 3.2 mol %. Through analysis of energetics computed
using the best available Born–Mayer–Huggins empirical
potential model, a point charge model, DFT, and a local strain energy
estimated in the harmonic approximation, the main chemical and physical
descriptors that correlate to the low-energy DFT structures are discussed.
It is found that the empirical potential model reproduces a general
trend of increasing DFT energetics across a series of locally strain
relaxed structures but is unreliable both in predicting some incorrect
low-energy structures and in finding some metastable structures to
be unstable. A better predictor of low-energy defect structures is
found to be the total electrostatic energy of a simple point charge
model calculated at the unrelaxed geometries of the defects. In addition,
the strain relaxation energy is estimated effectively in the harmonic
approximation to the imaginary phonon modes of undoped c-ZrO<sub>2</sub> but is found to be unimportant in determining the low-energy defect
structures. These results allow us to propose a set of easily computed
descriptors that can be used to identify the low-energy YSZ defect
structures, negating the combinatorial complexity and number of defect
structures that need to be considered