SOL2017-09-04 (M5.5) 2017 as a Source of Relativistic Electrons and Protons
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|1st Author:||Alexei Struminsky|
|2nd Author:||(see Acknowledgments)|
|Published:||16 March 2020|
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As related in many of these Nuggets, particle acceleration figures prominently in the physics of solar flares and coronal mass ejections. We can observe these particles in the flare regions via their secondary X-ray and γ-ray emissions, and also in space more directly via the solar energetic particles (SEPs; "solar cosmic rays").
The relation between the number of accelerated protons and electrons is an important characteristic of these processes. The RHESSI observations are consistent with two (possibly concurrent) acceleration processes: one that accelerates electrons above 50 keV but not above 0.3 MeV (the first phase), and a second that accelerates both ions and electrons proportionally to high energies (the second phase) (Ref. ). In order to choose a specific acceleration mechanism suggested for solar flares (see the Table) we need to track electrons of ~10 MeV and protons of ~100 MeV. From the table it is clear that any acceleration mechanism may operate during the first phase, but we have only two possibilities for the second phase.
To get information on 10 MeV electrons is possible via modeling the results of radio, X-ray and γ-ray observations, but this problem has not been solved unambiguously yet. It is impossible in principle to get information on protons with energies between 30 and 300 MeV (between protons generating nuclear γ-ray lines and π0-mesons). Therefore let's consider both solar and interplanetary observations, as described in Ref. . As a proxy of solar > 100 MeV proton flux we use the count rate of the anticoincidence shield of the spectrometer on the INTEGRAL spacecraft. Information on relativistic solar electrons is available from the Earth via SOHO.
In studying a solar event, we must be clear about timing. Since the acceleration phases differ by either the presence or the absence of relativistic electrons, we assume a time "zero" at the onset time of the 15.4 GHz radio emission, generated by relativistic electrons via the gyrosynchrotron mechanism. The chosen time zero can be considered as the time at which relativistic electrons first appear in the solar atmosphere, and the boundary between the first and the second phases.
Observations of SOL2017-09-04 (M5.5)
This flare is a brilliant example of two-phase acceleration. It had distinct first and second phases separated by about ten minutes. The M5.5 flare in the SXR radiation (GOES) began at 20:28 UT (- 15 min with respect to our zero time). However, RHESSI recorded the beginning of a gradual signal increase in its 25-50 keV channel substantially earlier, approximately from 20:17 UT (-26 min). The RHESSI data also revealed two separate episodes of HXR radiation ("spikes") as clearly seen in Figure 1. The first spike started at time -13 min. It was characterized by a relatively soft spectrum (HXR below 100 keV, radio waves at frequencies <8.8 GHz) and coincided with the maximum of the SXR flare according to the GOES data. The small delay time of the emission-measure maximum relative to the maximum of the temperature characterizes the impulsive character of the flare at this time. The preflare and impulsive stages of this event lasted more than 20 min and were accompanied by the acceleration of electrons with energies of less than 100 keV. The second spike was observed during the decay phase decay of the SXR radiation. It started simultaneously with the emission of radio waves at 15.4 GHz and was characterized by a harder spectrum (up to 100 keV), along with a gradual temporal profile. Note that both HXR spikes correspond to the post-eruption phase, because they were detected after the inferred time of the CME position at a distance of one solar radius, as judged from the LASCO data shown in Figure 1.
Comparing Figures 1 and 2 reveals that the second HXR spike was the source of the gradual electron and proton event. These show energetic electrons in the 0.27-0.7 MeV channel (v/c 0.78-0.91) to be increasing at approximately +2.5 min; i.e., if the electrons were injected at time zero, they had propagated the distance of 1.2 AU. Hence, electrons in the 0.67-3.0-MeV channel (v/c = 0.91-0.99) arrived at +7.5 min, they were injected at time +5.8 min, and those in the 2.64-10.4 MeV channel (v/c = 0.99) that arrived at +12.5 min were injected at time +10.8 min. These data are indicative of a prolonged and gradual acceleration of electrons.
The delay time relative to electromagnetic radiation for protons with energies of 100 and 500 MeV (v/c 0.43 and 0.76) is ~14 and 5 min, respectively. The arrival time of the first protons varied between +15 (possibly) and +25 min (Fig.2, ACS SPI). Hence, the 100-MeV protons appeared in interplanetary space between 0 and 10 min, while the 500-MeV protons appeared between 10 and 20 min (Fig. 2), which coincides with the second HXR spike at the decay stage of the M5.5 flare. Therefore, we identify the first HXR spike with the first phase of the flare acceleration, while identifying the second spike with the second phase of the flare acceleration. Apparently, electrons exhibiting a softer spectrum that were accelerated in the first HXR spike did not reach the threshold energies for their detection by SOHO and/or their intensity was below the background (Fig. 2).
The similarity of the time profiles of the fluxes of electrons and protons (Figure 2) suggests that the mechanisms of their acceleration and propagation are the same. To explain the time profiles of proton fluxes in interplanetary space, it is necessary to assume their prolonged injection, which can take place either due to prolonged acceleration or trapping. The time profiles of the proton fluxes are similar to those of the electrons, for which prolonged trapping is precluded by synchrotron losses. Accordingly, the hypothesis of prolonged acceleration is strongly preferred. A prolonged acceleration of protons would be possible either at the post-eruptive phase of the flare or at the CME shock front. Since relativistic electrons of the second phase could not be accelerated at the shock wave, only one possibility remains, namely, stochastic acceleration at the post-eruptive phase.
The flare itself can consist of a number of elementary actions of acceleration stochastically distributed in the chromosphere and corona, both in the first and the second phases (Ref. ). Elementary acts can differ from one to another by their duration and energy. The physical mechanisms of acceleration in these elementary actions can be different and are unimportant in the proposed scenario. The energy of accelerated electrons in a flare at the first phase does not reach the maximum possible value, and the proton energy is too low to allow their detection by nuclear γ-ray lines (the so-called "silent protons"). Later the radiation losses and continued acceleration smooth out the spectra of electrons accelerated in different elementary actions.
There is no role for CME/SEPs in this scenario of particle acceleration in long duration flares, as explained in Figure 3.
- The observational data do not contradict the scenario of stochastic acceleration in which protons and electrons simultaneously gain energy in elementary actions, whose duration is much shorter than the duration of the flare itself.
- The proposed scenario combines two, at first sight irreconcilable, approaches, namely, acceleration both in the flares and in the CME shock waves as well.
- The acceleration rate at the flare site should be greater than that at the shock front. Flare-accelerated protons, rather than shock-accelerated SEPS (Ref. ) would produce the sustained γ-ray -emission.
Irina Grigorieva, Yuri Logachov and Andrei Sadovskii are co-authors of this Nugget.