8,663 research outputs found
Flavor stability analysis of dense supernova neutrinos with flavor-dependent angular distributions
Numerical simulations of the supernova (SN) neutrino self-induced flavor
conversions, associated with the neutrino-neutrino interactions in the deepest
stellar regions, have been typically carried out assuming the "bulb-model". In
this approximation, neutrinos are taken to be emitted half-isotropically by a
common neutrinosphere. In the recent Ref. \cite{Mirizzi:2011tu} we have removed
this assumption by introducing flavor-dependent angular distributions for SN
neutrinos, as suggested by core-collapse simulations. We have found that in
this case a novel multi-angle instability in the self-induced flavor
transitions can arise. In this work we perform an extensive study of this
effect, carrying out a linearized flavor stability analysis for different SN
neutrino energy fluxes and angular distributions, in both normal and inverted
neutrino mass hierarchy. We confirm that spectra of different nu species which
cross in angular space (where F_{\nu_e}=F_{\nu_x} and
F_{\bar\nu_e}=F_{\bar\nu_x}) present a significant enhancement of the flavor
instability, and a shift of the onset of the flavor conversions at smaller
radii with respect to the case of an isotropic neutrino emission. We also
illustrate how a qualitative (and sometimes quantitative) understanding of the
dynamics of these systems follows from a stability analysis.Comment: (v2: revised version. 10 pages, 10 eps figures. References updated.
Figures imrproved. Matches the version published in PRD.
Degeneracy lifting of Majorana bound states due to electron-phonon interactions
We study theoretically how electron-phonon interaction affects the energies
and level broadening (inverse lifetime) of Majorana bound states (MBSs) in a
clean topological nanowire at low temperatures. At zero temperature, the energy
splitting between the right and left MBSs remains exponentially small with
increasing nanowire length . At finite temperatures, however, the absorption
of thermal phonons leads to the broadening of energy levels of the MBSs that
does not decay with system length, and the coherent absorption/emission of
phonons at opposite ends of the nanowire results in MBSs energy splitting that
decays only as an inverse power-law in . Both effects remain exponential in
temperature. In the case of quantized transverse motion of phonons, the
presence of Van Hove singularities in the phonon density of states causes
additional resonant enhancement of both the energy splitting and the level
broadening of the MBSs. This is the most favorable case to observe the
phonon-induced energy splitting of MBSs as it becomes much larger than the
broadening even if the topological nanowire is much longer than the coherence
length. We also calculate the charge and spin associated with the energy
splitting of the MBSs induced by phonons. We consider both a spinless
low-energy continuum model, which we evaluate analytically, as well as a
spinful lattice model for a Rashba nanowire, which we evaluate numerically
Report drawn up on behalf of the Committee on Regional Policy and Regional Planning on the second periodic report on the social and economic situation and development of the regions of the Community. Working Documents 1986-87, Document A 2-6/86, 26 March 1986.
Report drawn up on behalf of the Committee on Regional Policy and Regional Planning on the proposals onthe European Regional Development Fund (ERDF) contained in the Commission's report on ways of increasing the effectiveness of the Community's structural funds (Doc. 1-646/83- COM(83) 501 final). Working Documents 1983-1984. Document 1-930/83. 28 October 1983.
Report drawn up on behalf of the Political Affairs Committee on the communication from the Commission of the European Communities to the Council and the European Parliament on the conciliation procedure (COM(81) 816 final). EP Working Documents 1983-84, Document 1-984/83, 8 November 1983
Entanglement negativity in quantum field theory
We develop a systematic method to extract the negativity in the ground state
of a 1+1 dimensional relativistic quantum field theory, using a path integral
formalism to construct the partial transpose rho_A^{T_2} of the reduced density
matrix of a subsystem A=A1 U A2, and introducing a replica approach to obtain
its trace norm which gives the logarithmic negativity E=ln||\rho_A^{T_2}||.
This is shown to reproduce standard results for a pure state. We then apply
this method to conformal field theories, deriving the result E\sim(c/4) ln(L1
L2/(L1+L2)) for the case of two adjacent intervals of lengths L1, L2 in an
infinite system, where c is the central charge. For two disjoint intervals it
depends only on the harmonic ratio of the four end points and so is manifestly
scale invariant. We check our findings against exact numerical results in the
harmonic chain.Comment: 4 pages, 5 figure
GRB Flares: UV/Optical Flaring (Paper I)
We present a new algorithm for the detection of flares in gamma-ray burst
(GRB) light curves and use this algorithm to detect flares in the UV/optical.
The algorithm makes use of the Bayesian Information Criterion (BIC) to analyze
the residuals of the fitted light curve, removing all major features, and to
determine the statistically best fit to the data by iteratively adding
additional `breaks' to the light curve. These additional breaks represent the
individual components of the detected flares: T_start, T_stop, and T_peak. We
present the detection of 119 unique flaring periods detected by applying this
algorithm to light curves taken from the Second Swift Ultraviolet/Optical
Telescope (UVOT) GRB Afterglow Catalog. We analyzed 201 UVOT GRB light curves
and found episodes of flaring in 68 of the light curves. For those light curves
with flares, we find an average number of ~2 flares per GRB. Flaring is
generally restricted to the first 1000 seconds of the afterglow, but can be
observed and detected beyond 10^5 seconds. More than 80% of the flares detected
are short in duration with Delta t/t of < 0.5. Flares were observed with flux
ratios relative to the underlying light curve of between 0.04 to 55.42. Many of
the strongest flares were also seen at greater than 1000 seconds after the
burst.Comment: Submitted to ApJ. 20 pages (including 8 figures and 1 table
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