1,014 research outputs found
Internal Security and Economic Cost of Violence: An Analysis
South Asia is one of the most unstable and volatile regions of the world and stands second least peaceful region out of nine regions that were evaluated by the Institute for Economics and Peace (IEP). The ranking of the peacefulness of most of the South Asian countries is also rather low. In a developing country like India, the economic cost of violence at 5 percent of its GDP is too high. The causes of internal conflicts can be attributed to factors like ineffectiveness of the governance systems, sub-nationalism, deprivations, discrimination, social injustice, ethnic, sectarian, and religious polarisation, socio-economic exclusion, identity crisis, and competition for fast depleting crucial resources. These conflicts manifest in the form of insurgencies, terrorism, low-intensity armed conflicts, civil wars, and related political violence. There is a definite relationship between terrorism and internal armed conflicts, as both generally follow near similar contours. The terrorists have tried to destroy the very idea of India - democratic, secular, growth-oriented economy, excellence in IT and industry. Almost all elements of national power have a role - direct or indirect - on matters of national security, to suppress internal armed conflicts, and finally to resolve them. The legitimate aspirations and grievances of the people must be identified region-wise and addressed with a sense of urgency. The Government needs to formulate a comprehensive National Security Strategy (CNSS), to give a definite direction to the role of each element of national power in the short and long term, and minimize its economic cost of violence
Neutrino oscillations with disentanglement of a neutrino from its partners
We bring attention to the fact that in order to understand existing data on
neutrino oscillations, and to design future experiments, it is imperative to
appreciate the role of quantum entanglement. Once this is accounted for, the
resulting energy-momentum conserving phenomenology requires a single new
parameter related to disentanglement of a neutrino from its partners. This
parameter may not be CP symmetric. We illustrate the new ideas, with
potentially measurable effects, in the context of a novel experiment recently
proposed by Gavrin, Gorbachev, Veretenkin, and Cleveland. The strongest impact
of our ideas is on the resolution of various anomalies in neutrino oscillations
and on neutrino propagation in astrophysical environments.Comment: 6 page
Comparative experimental and Density Functional Theory (DFT) study of the physical properties of MgB2 and AlB2
In present study, we report an inter-comparison of various physical and
electronic properties of MgB2 and AlB2. Interestingly, the sign of S(T) is +ve
for MgB2 the same is -ve for AlB2. This is consistent our band structure plots.
We fitted the experimental specific heat of MgB2 to Debye Einstein model and
estimated the value of Debye temperature (theta) and Sommerfeld constant
(gamma) for electronic specific heat. Further, from gamma the electronic
density of states (DOS) at Fermi level N(EF) is calculated. From the ratio of
experimental N (EF) and the one being calculated from DFT, we obtained value of
Lembda to be 1.84, thus placing MgB2 in the strong coupling BCS category. The
electronic specific heat of MgB2 is also fitted below Tc using pi-model and
found that it is a two gap superconductor. The calculated values of two gaps
are in good agreement with earlier reports. Our results clearly demonstrate
that the superconductivity of MgB2 is due to very large phonon contribution
from its stretched lattice. The same two effects are obviously missing in AlB2
and hence it is not superconducting. DFT calculations demonstrated that for
MgB2 the majority of states come from Sigma and Pi 2p states of boron on the
other hand Sigma band at Fermi level for AlB2 is absent. This leads to a weak
electron phonon coupling and also to hole deficiency as Pi bands are known to
be of electron type and hence obviously the AlB2 is not superconducting. The
DFT calculations are consistent with the measured physical properties of the
studied borides, i.e., MgB2 and AlB2Comment: 16 pages Text + Figs: comments/suggestions welcome
([email protected])/www.freewebs.com/vpsawana
Interplay of gravitation and linear superposition of different mass eigenstates
The interplay of gravitation and the quantum-mechanical principle of linear
superposition induces a new set of neutrino oscillation phases. These ensure
that the flavor-oscillation clocks, inherent in the phenomenon of neutrino
oscillations, redshift precisely as required by Einstein's theory of
gravitation. The physical observability of these phases in the context of the
solar neutrino anomaly, type-II supernovae, and certain atomic systems is
briefly discussed
Extra Dirac Equations
This paper has rather a pedagogical meaning. Surprising symmetries in the
Lorentz group representation space are analyzed. The aim is
to draw reader's attention to the possibility of describing the particle world
on the ground of the Dirac "doubles". Several tune points of the variational
principle for this kind of equations are briefly discussed.Comment: REVTeX 3.0, 14p
Anomalous Thermoelectric power of over-doped Bi2Sr2CaCu2O8 superconductor
Temperature dependence of thermoelectric power S(T) of three differently
processed Bi2Sr2CaCu2O8 (Bi2212) samples, viz. as-processed melt quenched
(Bi2212-MQ), 6000C N2-annealed (Bi2212-N2) and 6000C O2-annealed (Bi2212-O2) is
reported here. All the samples possess single-phase character and their
superconducting transition temperatures (TcR=0) are 85 K, 90 K and 72 K
respectively for Bi2212-MQ, Bi2212-N2 and Bi2212-O2. While Bi2212-MQ and
Bi2212-N2 samples are in near optimum doping regime, Bi2212-O2 is an over-doped
sample. TcS=0 values obtained through S(T) data are also in line with those
deduced from the temperature dependence of resistance and DC magnetization.
Interestingly, S(T) behaviour of the optimally-doped Bi2212-MQ and Bi2212-N2
samples is seen to be positive in whole temperature range, it is found negative
for the over-doped Bi2212-O2 sample above TcS=0. These results have been seen
in the light of the recent band structure calculations and the ensuing split
Fermi surface as determined by angle-resolved photoelectron spectroscopy
(ARPES).Comment: 11 Pages Text + Figs: comments welcome ([email protected]
Phantom energy from graded algebras
We construct a model of phantom energy using the graded Lie algebra SU(2/1).
The negative kinetic energy of the phantom field emerges naturally from the
graded Lie algebra, resulting in an equation of state with w<-1. The model also
contains ordinary scalar fields and anti-commuting (Grassmann) vector fields
which can be taken as two component dark matter. A potential term is generated
for both the phantom fields and the ordinary scalar fields via a postulated
condensate of the Grassmann vector fields. Since the phantom energy and dark
matter arise from the same Lagrangian the phantom energy and dark matter of
this model are coupled via the Grassman vector fields. In the model presented
here phantom energy and dark matter come from a gauge principle rather than
being introduced in an ad hoc manner.Comment: 8 pages no figures; references added and discussion on condensate of
vector grassman fields added. To be published MPL
Hypothesis of path integral duality: Applications to QED
We use the modified propagator for quantum field based on a ``principle of
path integral duality" proposed earlier in a paper by Padmanabhan to
investigate several results in QED. This procedure modifies the Feynman
propagator by the introduction of a fundamental length scale. We use this
modified propagator for the Dirac particles to evaluate the first order
radiative corrections in QED. We find that the extra factor of the modified
propagator acts like a regulator at the Planck scales thereby removing the
divergences that otherwise appear in the conventional radiative correction
calculations of QED. We find that:(i) all the three renormalisation factors
, , and pick up finite corrections and (ii) the modified
propagator breaks the gauge invariance at a very small level of
. The implications of this result to generation of the
primordial seed magnetic fields are discussed.Comment: 15 pages, LaTeX2e (uses ijmpd.sty); To appear in IJMP-D; References
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