631 research outputs found

    Radio-wave propagation through a medium containing electron-density fluctuations described by an anisotropic Goldreich-Sridhar spectrum

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    We study the propagation of radio waves through a medium possessing density fluctuations that are elongated along the ambient magnetic field and described by an anisotropic Goldreich-Sridhar power spectrum. We derive general formulas for the wave phase structure function, visibility, angular broadening, diffraction-pattern length scales, and scintillation time scale for arbitrary distributions of turbulence along the line of sight, and specialize these formulas to idealized cases.Comment: 25 pages, 3 figures, submitted to Ap

    ΠœΠ°Ρ‚Π΅ΠΌΠ°Ρ‚ΠΈΡ‡Π΅ΡΠΊΠΈΠ΅ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈ ΠΏΡ€ΠΎΠ³Π½ΠΎΠ·Π° Π°Ρ„Ρ‚Π΅Ρ€ΡˆΠΎΠΊΠΎΠ² зСмлСтрясСний: Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒ смСны ΠΏΠ°Ρ€Π°Π΄ΠΈΠ³ΠΌΡ‹

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    Analysis and forecast of aftershocks of large earthquakes in the world practice is currently based exclusively on stochastic models of aftershock process. This makes it possible to use statistical methods of analysis, and also to apply the ”scenario” approach in forecasts by repeatedly generating random sequences of aftershocks and counting the frequency of repetition of the events of interest. Studies on the Russian Science Foundation project ”Development of information system for automatic seismic hazard assessment after large earthquakes based on geophysical monitoring” in 2016-2018 showed however that the effectiveness of such approaches has significant limitations. In this paper I give a critical review of statistical methods for the analysis and forecast of aftershocks, an interpretation of the effectiveness limits of forecasts using standard approaches, provide the rationale for the need to change the paradigm. As one of the search directions, the application of Discrete Mathematical Analysis (DMA) methods developed by Academician A.D. Gvishiani and his scientific school. An obvious advantage of this approach is demonstrated by the example of a simple algorithm for identification of aftershocks using fuzzy comparisons.Анализ ΠΈ ΠΏΡ€ΠΎΠ³Π½ΠΎΠ· Π°Ρ„Ρ‚Π΅Ρ€ΡˆΠΎΠΊΠΎΠ² ΡΠΈΠ»ΡŒΠ½Ρ‹Ρ… зСмлСтрясСний Π² ΠΌΠΈΡ€ΠΎΠ²ΠΎΠΉ ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠ΅ Π² настоящСС врСмя основан ΠΈΡΠΊΠ»ΡŽΡ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ Π½Π° стохастичСских модСлях развития Π°Ρ„Ρ‚Π΅Ρ€ΡˆΠΎΠΊΠΎΠ²ΠΎΠ³ΠΎ процСсса. Π­Ρ‚ΠΎ Π΄Π°Π΅Ρ‚ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ использования статистичСских ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² Π°Π½Π°Π»ΠΈΠ·Π°, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΡ€ΠΈΠΌΠ΅Π½ΡΡ‚ΡŒ Π² ΠΏΡ€ΠΎΠ³Π½ΠΎΠ·Π΅ ”сцСнарный” ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ ΠΏΡƒΡ‚Π΅ΠΌ ΠΌΠ½ΠΎΠ³ΠΎΠΊΡ€Π°Ρ‚Π½ΠΎΠ³ΠΎ гСнСрирования случайных ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚Π΅ΠΉ Π°Ρ„Ρ‚Π΅Ρ€ΡˆΠΎΠΊΠΎΠ² ΠΈ подсчСта частоты повторСния ΠΈΠ½Ρ‚Π΅Ρ€Π΅ΡΡƒΡŽΡ‰ΠΈΡ… событий. ИсслСдования ΠΏΠΎ ΠΏΡ€ΠΎΠ΅ΠΊΡ‚Ρƒ РНЀ ”БозданиС ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ систСмы автоматичСской ΠΎΡ†Π΅Π½ΠΊΠΈ сСйсмичСской опасности послС ΡΠΈΠ»ΡŒΠ½Ρ‹Ρ… зСмлСтрясСний ΠΏΠΎ Π΄Π°Π½Π½Ρ‹ΠΌ гСофизичСского мониторинга” Π² 2016-2018 Π³Π³. ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ ΠΎΠ΄Π½Π°ΠΊΠΎ, Ρ‡Ρ‚ΠΎ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ Ρ‚Π°ΠΊΠΈΡ… ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠ² ΠΈΠΌΠ΅Π΅Ρ‚ сущСствСнныС ограничСния. Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ даСтся критичСский ΠΎΠ±Π·ΠΎΡ€ статистичСских ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² Π°Π½Π°Π»ΠΈΠ·Π° ΠΈ ΠΏΡ€ΠΎΠ³Π½ΠΎΠ·Π° Π°Ρ„Ρ‚Π΅Ρ€ΡˆΠΎΠΊΠΎΠ², ΠΈΠ½Ρ‚Π΅Ρ€ΠΏΡ€Π΅Ρ‚ΠΈΡ€ΡƒΡŽΡ‚ΡΡ ΠΏΡ€Π΅Π΄Π΅Π»Ρ‹ эффСктивности ΠΏΡ€ΠΎΠ³Π½ΠΎΠ·ΠΎΠ² ΠΏΡ€ΠΈ использовании стандартных ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠ², приводится обоснованиС нСобходимости смСны ΠΏΠ°Ρ€Π°Π΄ΠΈΠ³ΠΌΡ‹. Π’ качСствС ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΈΠ· Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠΉ поиска прСдлагаСтся ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² ДискрСтного матСматичСского Π°Π½Π°Π»ΠΈΠ·Π° (Π”ΠœΠ), Ρ€Π°Π·Ρ€Π°Π±Π°Ρ‚Ρ‹Π²Π°Π΅ΠΌΡ‹Ρ… Π°ΠΊΠ°Π΄Π΅ΠΌΠΈΠΊΠΎΠΌ А.Π”. Π“Π²ΠΈΡˆΠΈΠ°Π½ΠΈ ΠΈ Π΅Π³ΠΎ Π½Π°ΡƒΡ‡Π½ΠΎΠΉ школой. ΠžΡ‡Π΅Π²ΠΈΠ΄Π½ΠΎΠ΅ прСимущСство Ρ‚Π°ΠΊΠΎΠ³ΠΎ ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Π° продСмонстрировано Π½Π° ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π΅ простого Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ Π°Ρ„Ρ‚Π΅Ρ€ΡˆΠΎΠΊΠΎΠ² с использованиСм Π°ΠΏΠΏΠ°Ρ€Π°Ρ‚Π° Π½Π΅Ρ‡Π΅Ρ‚ΠΊΠΈΡ… сравнСний

    Astrophysical Gyrokinetics: Basic Equations and Linear Theory

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    Magnetohydrodynamic (MHD) turbulence is encountered in a wide variety of astrophysical plasmas, including accretion disks, the solar wind, and the interstellar and intracluster medium. On small scales, this turbulence is often expected to consist of highly anisotropic fluctuations with frequencies small compared to the ion cyclotron frequency. For a number of applications, the small scales are also collisionless, so a kinetic treatment of the turbulence is necessary. We show that this anisotropic turbulence is well described by a low frequency expansion of the kinetic theory called gyrokinetics. This paper is the first in a series to examine turbulent astrophysical plasmas in the gyrokinetic limit. We derive and explain the nonlinear gyrokinetic equations and explore the linear properties of gyrokinetics as a prelude to nonlinear simulations. The linear dispersion relation for gyrokinetics is obtained and its solutions are compared to those of hot-plasma kinetic theory. These results are used to validate the performance of the gyrokinetic simulation code {\tt GS2} in the parameter regimes relevant for astrophysical plasmas. New results on global energy conservation in gyrokinetics are also derived. We briefly outline several of the problems to be addressed by future nonlinear simulations, including particle heating by turbulence in hot accretion flows and in the solar wind, the magnetic and electric field power spectra in the solar wind, and the origin of small-scale density fluctuations in the interstellar medium.Comment: emulateapj, 24 pages, 10 figures, revised submission to ApJ: references added, typos corrected, reorganized and streamline

    Spectral energy dynamics in magnetohydrodynamic turbulence

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    Spectral direct numerical simulations of incompressible MHD turbulence at a resolution of up to 102431024^3 collocation points are presented for a statistically isotropic system as well as for a setup with an imposed strong mean magnetic field. The spectra of residual energy, EkR=∣EkMβˆ’EkK∣E_k^\mathrm{R}=|E_k^\mathrm{M}-E_k^\mathrm{K}|, and total energy, Ek=EkK+EkME_k=E^\mathrm{K}_k+E^\mathrm{M}_k, are observed to scale self-similarly in the inertial range as EkR∼kβˆ’7/3E_k^\mathrm{R}\sim k^{-7/3}, Ek∼kβˆ’5/3E_k\sim k^{-5/3} (isotropic case) and EkβŠ₯R∼kβŠ₯βˆ’2E^\mathrm{R}_{k_\perp}\sim k_\perp^{-2}, EkβŠ₯∼kβŠ₯βˆ’3/2E_{k_\perp}\sim k_\perp^{-3/2} (anisotropic case, perpendicular to the mean field direction). A model of dynamic equilibrium between kinetic and magnetic energy, based on the corresponding evolution equations of the eddy-damped quasi-normal Markovian (EDQNM) closure approximation, explains the findings. The assumed interplay of turbulent dynamo and Alfv\'en effect yields EkR∼kEk2E_k^\mathrm{R}\sim k E^2_k which is confirmed by the simulations.Comment: accepted for publication by PR

    Dust Dynamics in Compressible MHD Turbulence

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    We calculate the relative grain-grain motions arising from interstellar magnetohydrodynamic (MHD) turbulence. The MHD turbulence includes both fluid motions and magnetic fluctuations. While the fluid motions accelerate grains through hydro-drag, the electromagnetic fluctuations accelerate grains through resonant interactions. We consider both incompressive (Alfv\'{e}n) and compressive (fast and slow) MHD modes and use descriptions of MHD turbulence obtained in Cho & Lazarian (2002). Calculations of grain relative motion are made for realistic grain charging and interstellar turbulence that is consistent with the velocity dispersions observed in diffuse gas, including cutoff of the turbulence from various damping processes. We show that fast modes dominate grain acceleration, and can drive grains to supersonic velocities. Grains are also scattered by gyroresonance interactions, but the scattering is less important than acceleration for grains moving with sub-Alfv\'{e}nic velocities. Since the grains are preferentially accelerated with large pitch angles, the supersonic grains will be aligned with long axes perpendicular to the magnetic field. We compare grain velocities arising from MHD turbulence with those arising from photoelectric emission, radiation pressure and H2_{2} thrust. We show that for typical interstellar conditions turbulence should prevent these mechanisms from segregating small and large grains. Finally, gyroresonant acceleration is bound to preaccelerate grains that are further accelerated in shocks. Grain-grain collisions in the shock may then contribute to the overabundance of refractory elements in the composition of galactic cosmic rays.Comment: 15 pages, 17 figure

    Measurement of the e+eβˆ’β†’K+Kβˆ’Ο€+Ο€βˆ’e^+e^- \to K^+K^-\pi^+\pi^- cross section with the CMD-3 detector at the VEPP-2000 collider

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    The process e+eβˆ’β†’K+Kβˆ’Ο€+Ο€βˆ’e^+e^- \to K^+K^-\pi^+\pi^- has been studied in the center-of-mass energy range from 1500 to 2000\,MeV using a data sample of 23 pbβˆ’1^{-1} collected with the CMD-3 detector at the VEPP-2000 e+eβˆ’e^+e^- collider. Using about 24000 selected events, the e+eβˆ’β†’K+Kβˆ’Ο€+Ο€βˆ’e^+e^- \to K^+K^-\pi^+\pi^- cross section has been measured with a systematic uncertainty decreasing from 11.7\% at 1500-1600\,MeV to 6.1\% above 1800\,MeV. A preliminary study of K+Kβˆ’Ο€+Ο€βˆ’K^+K^-\pi^+\pi^- production dynamics has been performed

    Study of the process e+eβˆ’β†’ppΛ‰e^+e^-\to p\bar{p} in the c.m. energy range from threshold to 2 GeV with the CMD-3 detector

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    Using a data sample of 6.8 pbβˆ’1^{-1} collected with the CMD-3 detector at the VEPP-2000 e+eβˆ’e^+e^- collider we select about 2700 events of the e+eβˆ’β†’ppΛ‰e^+e^- \to p\bar{p} process and measure its cross section at 12 energy ponts with about 6\% systematic uncertainty. From the angular distribution of produced nucleons we obtain the ratio ∣GE/GM∣=1.49Β±0.23Β±0.30|G_{E}/G_{M}| = 1.49 \pm 0.23 \pm 0.30

    Search for leptonic decays of D0 mesons

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    We search for the flavor-changing neutral current decays D0\to mu+mu- and D0\to e+e-, and for the lepton-flavor violating decays D0\to e\pm mu\mp using 660 fb^-1 of data collected with the Belle detector at the KEKB asymmetric-energy e+e- collider. We find no evidence for any of these decays. We obtain significantly improved upper limits on the branching fractions: B(D0\to mu+mu-)<1.4x10-7, B(D0\to e+e-)<7.9x10-8, and B(D0\to e+mu-)+B(D0\to mu+e-)<2.6x10-7 at 90% confidence level.Comment: 6 pages, 3 figure

    Quantifying shear-induced wave transformations in the solar wind

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    The possibility of velocity shear-induced linear transformations of different magnetohydrodynamic waves in the solar wind is studied both analytically and numerically. A quantitative analysis of the wave transformation processes for all possible plasma-Ξ²\beta regimes is performed. By applying the obtained criteria for effective wave coupling to the solar wind parameters, we show that velocity shear-induced linear transformations of Alfv\'en waves into magneto-acoustic waves could effectively take place for the relatively low-frequency Alfv\'en waves in the energy containing interval. The obtained results are in a good qualitative agreement with the observed features of density perturbations in the solar wind.Comment: Astrophysical Journal (accepted
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