Statistical properties of flares are a powerful tool for addressing the upper solar atmosphere heating problem.We simulate time series of synthetic flares by means of a dynamic model of the atmospheric magnetic field in which magnetic loop footpoints are controlled by photospheric flows computed through a n-body algorithm. The n-body simulation reproduces the behavior of a system where large spatial organization scales (i.e., mesogranulation) occur from the interaction of small-scale advection flows (i.e., granulation). The frequency function of the emitted magnetic energies obtained from the simulation is well approximated by a power law with index 2:4, while the frequency function of the waiting times between emissions shows a P...
We estimated photospheric velocities by separately applying the Fourier Local Correlation Tracking a...
© ESO 2019. Context. The Sun features on its surface typical flow patterns called the granulation, m...
Context. The quiet Sun presents magnetized plasma whose field strengths vary from zero to about 2 kG...
Statistical properties of flares are a powerful tool for addressing the upper solar atmosphere heati...
We present a dynamic model of the atmospheric magnetic field in which magnetic loop footpoints are c...
Abstract. We present a dynamic model of atmospheric magnetic field in which magnetic loop footpoints...
The quiet Sun may be the biggest laboratory to study physical elementary processes of fundamental im...
Small-scale magnetic reconnection processes in the form of nanoflares have become increasingly hypot...
Context. We interpret solar flares as events originating in active regions that have reached the sel...
A model of the Lu–Hamilton kind is applied to the study of critical behavior of the magnetized solar...
A model describing physical processes of solar flares and their homologous behavior is presented bas...
A two-dimensional probabilistic Cellular Automaton is used to model the appearance of active regions...
Context. Nanoflares are small impulsive bursts of energy that blend with and possibly make up much o...
To describe the distributionof the total number of flares per time unit p(E), we bring forward a new...
Solar flares stem from the reconnection of twisted magnetic field lines in the solar photo-sphere. T...
We estimated photospheric velocities by separately applying the Fourier Local Correlation Tracking a...
© ESO 2019. Context. The Sun features on its surface typical flow patterns called the granulation, m...
Context. The quiet Sun presents magnetized plasma whose field strengths vary from zero to about 2 kG...
Statistical properties of flares are a powerful tool for addressing the upper solar atmosphere heati...
We present a dynamic model of the atmospheric magnetic field in which magnetic loop footpoints are c...
Abstract. We present a dynamic model of atmospheric magnetic field in which magnetic loop footpoints...
The quiet Sun may be the biggest laboratory to study physical elementary processes of fundamental im...
Small-scale magnetic reconnection processes in the form of nanoflares have become increasingly hypot...
Context. We interpret solar flares as events originating in active regions that have reached the sel...
A model of the Lu–Hamilton kind is applied to the study of critical behavior of the magnetized solar...
A model describing physical processes of solar flares and their homologous behavior is presented bas...
A two-dimensional probabilistic Cellular Automaton is used to model the appearance of active regions...
Context. Nanoflares are small impulsive bursts of energy that blend with and possibly make up much o...
To describe the distributionof the total number of flares per time unit p(E), we bring forward a new...
Solar flares stem from the reconnection of twisted magnetic field lines in the solar photo-sphere. T...
We estimated photospheric velocities by separately applying the Fourier Local Correlation Tracking a...
© ESO 2019. Context. The Sun features on its surface typical flow patterns called the granulation, m...
Context. The quiet Sun presents magnetized plasma whose field strengths vary from zero to about 2 kG...