Abstract:In high-energy astronomical phenomena, the stochastic particle acceleration by turbulences is one of the promising processes to generate non-thermal particles. In this paper, we investigate the energydiffusion efficiency of relativistic particles in a temporally evolving wave ensemble that consists of a single mode (Alfvén, fast or slow) of linear magnetohydrodynamic waves. In addition to the gyroresonance with waves, the transit-time damping (TTD) also contributes to the energy-diffusion for fast and slow-mod… Show more
“…In this case, most of the previous works have used test particle simulations, where turbulence was represented by prescribed fields (e.g. Micha lek & Ostrowsky 1996;Arzner et al 2006;Fraschetti & Melia 2008;O'Sullivan et al 2009;Teraki & Asano 2019) or it was provided by turbulent fields obtained from MHD simulations (e.g. Ambrosiano et al 1988;Dmitruk et al 2004;Kowal et al 2012;Dalena et al 2014;Lynn et al 2014;Kimura et al 2016;Beresnyak & Li 2016;Isliker et al 2017;González et al 2017;Kimura et al 2019).…”
Magnetized turbulence and magnetic reconnection are often invoked to explain the nonthermal emission observed from a wide variety of astrophysical sources. By means of fully-kinetic 2D and 3D particle-in-cell simulations, we investigate the interplay between turbulence and reconnection in generating nonthermal particles in magnetically-dominated (or, equivalently, "relativistic") pair plasmas. A generic by-product of the turbulence evolution is the generation of a nonthermal particle spectrum with a power-law energy range. The power-law slope p is harder for larger magnetizations and stronger turbulence fluctuations, and it can be as hard as p 2. The Larmor radius of particles at the high-energy cutoff is comparable to the size l of the largest turbulent eddies. Plasmoid-mediated reconnection, which self-consistently occurs in the turbulent plasma, controls the physics of particle injection. Then, particles are further accelerated by stochastic scattering off turbulent fluctuations. The work done by parallel electric fields -naturally expected in reconnection layers -is responsible for most of the initial energy increase, and is proportional to the magnetization σ of the system, while the subsequent energy gain, which dominates the overall energization of high-energy particles, is powered by the perpendicular electric fields of turbulent fluctuations. The two-stage acceleration process leaves an imprint in the particle pitch-angle distribution: low-energy particles are aligned with the field, while the highest energy particles move preferentially orthogonal to it. The energy diffusion coefficient of stochastic acceleration scales as D γ ∼ 0.1σ(c/l)γ 2 , where γ is the particle Lorentz factor. This results in fast acceleration timescales t acc ∼ (3/σ) l/c. Our findings have important implications for understanding the generation of nonthermal particles in high-energy astrophysical sources.
“…In this case, most of the previous works have used test particle simulations, where turbulence was represented by prescribed fields (e.g. Micha lek & Ostrowsky 1996;Arzner et al 2006;Fraschetti & Melia 2008;O'Sullivan et al 2009;Teraki & Asano 2019) or it was provided by turbulent fields obtained from MHD simulations (e.g. Ambrosiano et al 1988;Dmitruk et al 2004;Kowal et al 2012;Dalena et al 2014;Lynn et al 2014;Kimura et al 2016;Beresnyak & Li 2016;Isliker et al 2017;González et al 2017;Kimura et al 2019).…”
Magnetized turbulence and magnetic reconnection are often invoked to explain the nonthermal emission observed from a wide variety of astrophysical sources. By means of fully-kinetic 2D and 3D particle-in-cell simulations, we investigate the interplay between turbulence and reconnection in generating nonthermal particles in magnetically-dominated (or, equivalently, "relativistic") pair plasmas. A generic by-product of the turbulence evolution is the generation of a nonthermal particle spectrum with a power-law energy range. The power-law slope p is harder for larger magnetizations and stronger turbulence fluctuations, and it can be as hard as p 2. The Larmor radius of particles at the high-energy cutoff is comparable to the size l of the largest turbulent eddies. Plasmoid-mediated reconnection, which self-consistently occurs in the turbulent plasma, controls the physics of particle injection. Then, particles are further accelerated by stochastic scattering off turbulent fluctuations. The work done by parallel electric fields -naturally expected in reconnection layers -is responsible for most of the initial energy increase, and is proportional to the magnetization σ of the system, while the subsequent energy gain, which dominates the overall energization of high-energy particles, is powered by the perpendicular electric fields of turbulent fluctuations. The two-stage acceleration process leaves an imprint in the particle pitch-angle distribution: low-energy particles are aligned with the field, while the highest energy particles move preferentially orthogonal to it. The energy diffusion coefficient of stochastic acceleration scales as D γ ∼ 0.1σ(c/l)γ 2 , where γ is the particle Lorentz factor. This results in fast acceleration timescales t acc ∼ (3/σ) l/c. Our findings have important implications for understanding the generation of nonthermal particles in high-energy astrophysical sources.
“…Since the properties of the turbulences are highly uncertain (see Teraki & Asano 2019;Demidem et al 2020, and references therein). In this study, we use = 2 to simulate hard sphere scattering between the MHD waves and the electrons.…”
Using a time-dependent one-zone leptonic model that incorporates both shock acceleration and stochastic acceleration processes, we investigate the formation of the narrow spectral feature at ∼ 3 TeV of Mrk 501 which was observed during the X-ray and TeV flaring activity in July 2014. It is found that the broadband spectral energy distribution (SED) can be well interpreted as the synchrotron and synchrotron-self-Compton emission from the electron energy distribution (EED) that is composed by a power-law (PL) branch and a pileup branch. The PL branch produces synchrotron photons which are scattered by the electrons of the pileup branch via inverse-Compton scattering and form the narrow spectral feature observed at the TeV energies. The EED is produced by two injection episodes, and the pileup branch in EED is caused by shock acceleration rather than stochastic acceleration.
“…Recently some research has been devoted to combine the fluid and the PIC approaches (Bai et al 2015) to study the DSA (Mignone et al 2018). The final numerical method uses a Monte Carlo technique to study particle acceleration by shock waves (Achterberg & Krulls 1992;Baring et al 1994;Marcowith & Kirk 1999;Wolff & Tautz 2015) and turbulence (Giacalone & Jokipii 1999;Teraki & Asano 2019). Among all of the numerical techniques available, the PIC method has an advantage (Ostrowski 1988;Ellison et al 1990;Ellison & Double 2002;Lemoine & Pelletier 2003;Baring 2004;Niemiec & Ostrowski 2006) over all other techniques because PIC not only can model the particle acceleration process, it can also determine the self-generated magnetic turbulence, and treat them self-consistently with the cosmic ray particles.…”
Particle acceleration is a ubiquitous phenomenon in astrophysical and space plasma. Diffusive shock acceleration (DSA) and stochastic turbulent acceleration (STA) are known to be the possible mechanisms for producing very highly energetic particles, particularly in weakly magnetized regions. An interplay of different acceleration processes along with various radiation losses is typically observed in astrophysical sources. While DSA is a systematic acceleration process that energizes particles in the vicinity of shocks, STA is a random energizing process, where the interaction between cosmic ray particles and electromagnetic fluctuations results in particle acceleration. This process is usually interpreted as a biased random walk in energy space, modeled through a Fokker-Planck equation. In the present work, we describe a novel Eulerian algorithm, adopted to incorporate turbulent acceleration in the presence of DSA and radiative processes like synchrotron and inverse Compton emission. The developed framework extends the hybrid Eulerian−Lagrangian module in a full-fledged relativistic Magneto-hydrodynamic (RMHD) code PLUTO. From our validation tests and case studies, we showcase the competing and complementary nature of both acceleration processes. Axisymmetric simulations of an RMHD jet with this extended hybrid framework clearly demonstrate that emission due to shocks is localized, while that due to turbulent acceleration originates in the backflow and is more diffuse, particularly in the high-energy X-ray band.
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