© ESO 2020

1. Introduction

Solar flares are characterized by fast plasma flows, e.g., by plasma outflows from the magnetic reconnection (Priest & Forbes 2000). If in such plasma flows there are sufficiently strong shears in flow velocities, then owing to the Kelvin–Helmholtz (shear flow) instability, magnetohydrodynamic turbulence is generated (Chiueh & Zweibel 1987). This turbulence plays an important role in particle acceleration (Miller et al. 1996; Petrosian 2016). Some estimations of the level of this turbulence were made based on the broadening of the observed spectral lines (Hassler et al. 1990; Harra et al. 2013; Polito et al. 2018). In the paper by Karlický (2014) the frequency variations of the zebra stripes were interpreted as being caused by the plasma turbulence. These frequency variations were analyzed by the Fourier method and the spectra with the power-law index close to the Kolmogorov index were found.

In the present paper we estimate the levels of the time and spatially varying turbulence in the density and magnetic field in the zebra radio sources observed during solar flares. In particular, the estimation of the levels of the magnetic field turbulence is new.

We use the zebra model based on the double-plasma resonance (DPR) instability (Zheleznyakov & Zlotnik 1975; Winglee & Dulk 1986; Kuznetsov & Tsap 2007; Tan 2010; Zlotnik 2013; Tan et al. 2014; Karlický & Yasnov 2015; Benáček & Karlický 2019). In this model, each zebra-stripe source is located at a different place. It enables us to estimate the turbulence level not only in each zebra-stripe source (time varying turbulence), but also the turbulence level in space between the zebra-stripe sources at a given time (spatially varying turbulence).

The spatially varying turbulence between zebra-stripe sources is a new aspect in the zebra-stripe analysis. Moreover, it removes some problems with the DPR zebra model recently discussed in the paper by Yasnov & Chernov (2020). The authors calculated a sequence of the gyro-harmonic numbers of zebra stripes in the whole zebra from the zebra-stripe frequencies at the high- and low-frequency parts of the zebras. They found that the sequence of the gyro-harmonic numbers derived from the high- and low-frequency zebra stripes differ in some zebras. Based on this, they concluded that these zebras cannot be explained by the DPR model. However, when we include the turbulence in the DPR model then the difference in calculated sequences of the gyro-harmonic numbers can be explained within the DPR model. In the DPR model the zebra-stripe sources are located at different positions, and thus the plasma turbulence modifies the zebra-stripe frequencies of different zebra stripes in a different way. This introduces a difference in the sequence of the gyro-harmonic numbers calculated from the high- and low-frequency parts of the zebras.

In this paper we also present a new method for determining the gyro-harmonic numbers of the zebra stripes. The results obtained by this new method are verified by our previous method, presented in the paper by Karlický & Yasnov (2015). We apply these methods for the 14 February 1999 zebra event and calculate not only the gyro-harmonic numbers of zebra stripes, but also the density and magnetic field. Then, knowing the gyro-harmonic numbers of zebra stripes in this zebra event, we estimate the level of the time varying and spatially varying turbulence in the density and magnetic field in the zebra-stripe sources. This enables us to compare these turbulence levels for the first time.

2. Method and its application

In our method we use the zebra model based on the double-plasma resonance (DPR) instability (Zheleznyakov & Zlotnik 1975; Winglee & Dulk 1986; Zlotnik 2013; Benáček & Karlický 2018). Our method consists of two steps. First, we determine the gyro-harmonic numbers of zebra stripes by a new method and by our previous methods (Karlický & Yasnov 2015). Second, knowing the gyro-harmonic numbers and the zebra-stripe frequencies, we calculate the density and magnetic field in the zebra-stripe sources, and also their temporal and spatial variations, and thus the levels of their turbulence. The new method for determining the gyro-harmonic numbers is highlighted by the example below where we use artificially generated zebra-stripe frequencies. Then this new method is applied to the observed zebra.

In the DPR model the ratio of the two different zebra-stripe frequencies can be expressed as (Karlický & Yasnov 2019)

(1)

where f_s and f_s + m are the zebra-stripe frequencies for the zebra stripe with the gyro-harmonic numbers s and s + m; R = L_b/L_n, where L_n and L_b is the density and magnetic field scale in the density n and magnetic field B profiles

(2)

assumed in the zebra source; n₀ and B₀ are the density and magnetic field at some reference level; and h means the distance along the axis of the source.

In order to highlight our new method for determining the gyro-harmonic numbers of zebra stripes, we employ model (artificial) zebra-stripe frequencies. We use relation (1) with R = 0.65, which corresponds to sequence A (Karlický & Yasnov 2018); i.e., the zebra-stripe frequency in the zebra increases with decreasing gyro-harmonic number. We take this sequence A because it agrees with all zebras analyzed so far. We define the gyro-harmonic number s_L for the lowest zebra-stripe frequency f_L. In our example, we take s_L = 30 for f_L = 1250 MHz. In the relation (1) we change m from −1 to −6, and calculate seven model zebra-stripe frequencies (F_model = 1250, 1270, 1292, 1315, 1339, 1365, and 1392 MHz).

Solving Eq. (1) for R we express R as R_1, 2 (i.e., in terms of the ratio of neighboring zebra-stripe frequencies and corresponding gyro-harmonic numbers). Thus, we obtain the relation as

(3)

Here R_1, 2 is computed between the zebra-stripe frequency 1 and higher neighboring zebra-stripe frequency 2, starting from the lowest frequency f_L. In the following we make a number of computations of R_1, 2 for all pairs of neighboring zebra-stripe frequencies using the s_L as free parameter. We calculated R_1, 2 for the F_model frequencies and for six values of s_L = 15, 20, 25, 30, 35, and 40.

In Fig. 1 we present the plots of these R_1, 2 values in dependance on the gyro-harmonic number s, including the regression lines. The red asterisks with the horizontal regression line in Fig. 1 correspond to the plot with s_L = 30. As expected in this case, in all computed pairs of frequencies R_1, 2 is equal to 0.65, as in the case when the model zebra-stripe frequencies were calculated from the relation (1) with s_L = 30 and R = 0.65. But, when we use a value of s_L lower than 30 to calculate R_1, 2, then the value of R_1, 2 increases with increasing s. On the other hand, when we use a value of s_L greater than 30 to calculate R_1, 2, then the value of R_1, 2 decreases with increasing s (see Fig. 1). It should be noted that we fitted all the plots of R_1, 2 by the straight line – regression line. Except the case with s_L = 30, where R_1, 2 lie on the regression line, the other plots of R_1, 2 subtly deviate from the regression lines and the deviations increase with increasing |s_L − 30|. In the following, we utilize the change in the slope of the R_1, 2 plots shown in Fig. 1 to calculate s_L and R in the observed zebra. The actual value of s_L is determined when the regression line in the R_1, 2 data, calculated from the observed zebra-stripe frequencies, has a minimum slope compared to the horizontal line. This solution also gives the value of R = constant.

Fig. 1. Ratio of R1, 2 in dependance on the gyro-harmonic number s for six values of sL = 15 (green asterisks), 20 (light blue), 25 (yellow), 30 (red), 35 (dark blue), and 40 (orange). Dashed lines mean the regression lines for all R1, 2.

For a calculation based on observations, we use the zebra recorded on 14 February 1999 by the Ondřejov radiospectrograph (Jiřička et al. 1993) (Fig. 2). As seen in this figure, the most distinct and continuous zebra stripes appear at approximately 12:08:57.0 UT. The zebra-stripe frequencies at this time are 1548, 1573, 1599, 1619, 1642, 1674, 1707, 1739, 1770, 1810, 1845, and 1880 MHz. We use these frequencies to determine the gyro-frequency numbers. We vary s_L in a reasonable interval from 10 to 70, and calculate plots of R_1, 2. For each R_1, 2 plot we compute the regression line in the same way as the variation in the slope of the R_1, 2 plots in Fig. 1, looking for such s_L that the regression line has a minimum slope (i.e., this regression line represents R = constant). In Fig. 3b we show R_1, 2 for the 14 February 1999 zebra versus s in the case when the regression line has the minimum slope. In this case s_L = 32 and the R corresponding to the regression (dashed) line is 0.625. For comparison, Figs. 3a and c show cases for s_L = 22 and s_L = 42; we see in this case that the slope of the regression lines change with s_L, exactly like those in Fig. 1.

Fig. 2. Radio spectrum showing the zebra observed at 14 February 1999.

Fig. 3. R1, 2 in dependance on s, derived from the 14 February 1999 zebra: (a) for sL = 22, (b) for sL = 32, and (c) for sL = 42. Dashed lines mean the regression lines. In case (b) the regression line has a minimum slope compared to the horizontal line. Thus, this case gives the resulting sL = 32 and R = 0.625.

We checked the resulting s_L and R using our previous method, which is described in Karlický & Yasnov (2015). The results from this previous method are the same (s_L = 32 and R = 0.625).

Now, knowing the gyro-harmonic numbers of the zebra stripes and using the relations

(4)

where f_s is in MHz, we calculated the density n and magnetic field B in the zebra-stripe sources at 12:08:57.0 UT. The results for each zebra-stripe source, designated by s, are in Table 1.

Now, let us estimate the level of turbulence in the zebra source. First, we estimate the level of the time varying turbulence. For this purpose we take the zebra-stripe frequencies at eight zebra stripes in the eight equal consecutive windows covering the interval 12:08:56.7–12:08:57.4 UT, i.e., at a time around 12:08:57.0 UT where the gyro-harmonic numbers were determined and where there are continuous zebra stripes. Using the relations in Eq. (4) we calculated the variations in density and magnetic field in the zebra-stripe sources in comparison to their mean values. The results are shown in Fig. 4. The level of the time varying turbulence in density and magnetic field, expressed as the standard deviation for each window, is |Δn/n|_t = 0.0112–0.0149 and |ΔB/B|_t = 0.0056–0.0074.

Fig. 4. Time variations of the density Δn/n and magnetic field ΔB/B in the time interval 12:08:56.7–12:08:57.4 UT for the 14 February 1999 zebra. Black line: s = 28; violet: s = 27; green: s = 26; light blue: s = 25; yellow: s = 24; red: s = 23; blue: s = 22; and orange: s = 21. The vertical dashed line shows the time 12:08:57 UT, when the calculation of the gyro-harmonic numbers was made.

Now, let us estimate the level of the spatially varying turbulence. Figure 3b shows that R_1, 2 varies, which means that the observed zebra-stripe frequencies differ from those in the model, where R = 0.625 (dashed line). Although the error in zebra-stripe frequency measurements, which is ∼2 MHz, can contribute to this variation, we assume that the variation is caused by the plasma turbulence in the zebra-stripe sources.

Using the lowest zebra-stripe frequency in the 14 February 1999 zebra (f_L = 1548 MHz) and computed values of s_L = 32 and R = 0.625 we generate the model frequencies according to relation (1). Thus, for all zebra stripes with s we know the observed and model frequencies. Using these frequencies and the relations in Eq. (4), we compute the frequency difference between the observed and modeled frequencies Δf and the variation in the density Δn/n and magnetic field ΔB/B in all zebra-stripe sources. The results are shown in Fig. 5. The corresponding levels of the spatially varying turbulence expressed as the standard deviations are |Δn/n|_s = 0.0047 and |ΔB/B|_s = 0.0024.

Fig. 5. Frequency difference between the observed and modeled zebra-stripe frequencies Δf, and variations in the density Δn/n and magnetic field ΔB/B in dependence on the gyro-harmonic number s at 12:08:57 UT for the 14 February 1999 zebra.

3. Discussion and conclusions

In this paper we presented not only a new method for estimating the plasma turbulence level in the zebra-stripe radio sources, but also a new method for determining the gyro-harmonic numbers s in zebras. The method used to determine s is equivalent to the method presented in Karlický & Yasnov (2015).

We estimated levels of the time and spatially varying turbulence in the zebra stripe sources. The estimated levels are |Δn/n|_t = 0.0112–0.0149 and |ΔB/B|_t = 0.0056–0.0074 for the time varying turbulence and |Δn/n|_s = 0.0047 and |ΔB/B|_s = 0.0024 for the spatially varying turbulence. These turbulence levels differ in that the level of the spatially varying turbulence is lower. It indicates some anisotropy of this turbulence, probably caused by the magnetic field structure around zebra-stripe sources.

As seen in Figs. 4 and 5, variations in the density and magnetic field are in phase, which indicates the fast magnetosonic wave turbulence. The estimated turbulence levels are partly corrupted by the errors on the observed zebra-stripe frequencies. The estimated error on this determination is about 2 MHz, to be compared with the maximum difference between the zebra-stripe frequency and the mean zebra-stripe frequency in the studied interval (12:08:56.7–12:08:57.4 UT) (∼20 MHz), and the maximum difference between model and observed zebra-stripe frequencies (∼10 MHz; Fig. 5).

Figure 6 shows the regions of the plasma beta parameter greater or smaller than 1 in dependance on the plasma temperature and the gyro-harmonic number s of zebra stripes. This plot is made using the plasma beta definition and the relations in Eq. (4). As seen in this figure, the plasma beta parameter in the zebra-stripe sources is lower than 1 if the temperature is at least 1 MK (coronal temperature) and the gyro-harmonic numbers is smaller than about 50. For higher gyro-harmonic numbers and β ≤ 1, the temperature in the zebra-stripe sources is lower than 1 MK. In our case of the 14 February 1999 zebra, the gyro-harmonic number s_L is 32; therefore, the temperature in the zebra source for the plasma beta parameter β <  1 can be up to 3 MK.

Fig. 6. Regions of the plasma beta parameter β > 1 and β < 1 in the diagram of the plasma temperature vs. the gyro-harmonic number s.

Acknowledgments

The authors thank the referee for constructive comments that improved the article. We acknowledge support from the project RVO-67985815 and GAČR grants 18-09072S, 19-09489S, 20-09922J, and 20-07908S. L. V. Yasnov acknowledges support from the Russian Foundation for Basic Research, Grants 18-29-21016-mk, and partly from Grant 18-02-00045, from Program RAN No.28, Project 1D and State Task No. AAAA-A17-117011810013-4.

References

All Tables

All Figures

	Fig. 1. Ratio of R1, 2 in dependance on the gyro-harmonic number s for six values of sL = 15 (green asterisks), 20 (light blue), 25 (yellow), 30 (red), 35 (dark blue), and 40 (orange). Dashed lines mean the regression lines for all R1, 2.
In the text

	Fig. 2. Radio spectrum showing the zebra observed at 14 February 1999.
In the text

	Fig. 3. R1, 2 in dependance on s, derived from the 14 February 1999 zebra: (a) for sL = 22, (b) for sL = 32, and (c) for sL = 42. Dashed lines mean the regression lines. In case (b) the regression line has a minimum slope compared to the horizontal line. Thus, this case gives the resulting sL = 32 and R = 0.625.
In the text

	Fig. 4. Time variations of the density Δn/n and magnetic field ΔB/B in the time interval 12:08:56.7–12:08:57.4 UT for the 14 February 1999 zebra. Black line: s = 28; violet: s = 27; green: s = 26; light blue: s = 25; yellow: s = 24; red: s = 23; blue: s = 22; and orange: s = 21. The vertical dashed line shows the time 12:08:57 UT, when the calculation of the gyro-harmonic numbers was made.
In the text

	Fig. 5. Frequency difference between the observed and modeled zebra-stripe frequencies Δf, and variations in the density Δn/n and magnetic field ΔB/B in dependence on the gyro-harmonic number s at 12:08:57 UT for the 14 February 1999 zebra.
In the text

	Fig. 6. Regions of the plasma beta parameter β > 1 and β < 1 in the diagram of the plasma temperature vs. the gyro-harmonic number s.
In the text