A new approach to analyzing solar coronal spectra and updated collisional ionization equilibrium calculations. ii. updated ionization rate coefficients
Summary (5 min read)
1. INTRODUCTION
- Investigating the dynamics of the solar corona is crucial if one is to understand fundamental solar and heliospheric physics.
- Gaps remain in their understanding of some of the most fundamental processes taking place in the corona.
- Analyzing the spectral emission of the corona can give the temperature and density of the plasma, as well as information on the complex plasma structures common in this region of the Sun’s atmosphere.
- The authors also investigate here the observed relative elemental abundances and the first ionization potential (FIP) effect.
- Section 8 discusses the consequences of these results, in particular highlighting discrepancies between the results of this paper and those of Landi et al. (2002).
2. OBSERVATIONS
- The spectrum analyzed by Landi et al. (2002), and revisited here, was detected using the Solar Ultraviolet Measurement of Emitted Radiation Spectrometer (SUMER; Wilhelm et al. 1995) onboard the Solar and Heliospheric Observatory (SOHO).
- Known typos in the line assignment labels of Landi et al. (2002) have been corrected; these do not affect their reported results.
- The remaining spectral lines are split into three distinct groups, labeled in the first column of Table 1 as I.
- Transitions between the ground and the first excited configuration: IIa.
- The subdivision of transition Group II is to allow us to investigate a longstanding discrepancy between EMs derived using Li- and Na-like ions and those derived using other isoelectronic sequences (e.g., Dupree 1972; Feldman et al. 1998; Landi et al. 2002).
3. METHOD OF CALCULATING TEMPERATURE AND
- Only those emission lines that have a strong density sensitivity in this range will be affected by the density gradient (Lang et al. 1990).
- (5) This has the same value for all transitions if the constant temperature and density assumption is correct, which the authors label EMc.
- Thus, from the observed line intensities, Iji, and using accurate data for Gji(Te, ne), one can calculate the EM and Te of the emitting region.
- For ease of reading, the authors typically drop these units below.
4. IMPROVED CIE CALCULATIONS
- The plasma conditions of the solar upper atmosphere are often described as being optically thin, low density, dust free, and in steady state or quasi-steady state.
- This is commonly called CIE or coronal equilibrium.
- These conditions are not always the case in the solar upper atmosphere in the event of impulsive heating events but, given the inactivity and low density of the plasma analyzed here, they sufficiently describe the observed conditions.
- At the temperature of peak formation in CIE, DR dominates over RR for most ions.
- Considering all the ions and levels that need to be taken into account, it is clear that vast quantities of data are needed.
4.1. Recombination Rate Coefficients
- The DR and RR rate coefficients used to determine the CIE fractional abundances utilized by Landi et al. (2002) were those recommended by Mazzotta et al. (1998).
- There has been a significant improvement in the recombination rate coefficients since then.
- The RR rate coefficients are in even better agreement, typically within 10% over this temperature range.
- For both DR and RR outside this temperature range, agreement between these two state-of-the-art theories can become significantly worse.
- The DR calculations have also been compared to experimental measurements, where they exist, and found to be in agreement to within 35% in the temperature range where the ion forms in CIE.
4.2. EII Rate Coefficients
- There have also been recent attempts to improve the state of the EII rate coefficients used in CIE calculations.
- The most complete of these studies is that of Dere (2007), who produced recommended rate coefficients for all ionization stages of the elements H through Zn.
- For the ions important to the present work, differences between recent recommended rate coefficients of up to 50% are seen.
- In short, the authors do not see (An extended version of this figure set is available in the online journal.) the uniform agreement between recommended sets of EII data as they do for the state-of-the-art DR and RR calculations.
- Given the large differences between the Dere (2007) and Mattioli et al. (2007) results, the authors believe that further analysis of the EII database is required to resolve these differences.
4.3. Updated CIE Calculations
- Their results show large differences from the Mazzotta et al. (1998) data for certain elements.
- Here the authors revise the work of Bryans et al. (2006) to include these newly recommended EII rate coefficients for all elements from H through Zn and some further updates to the DR and RR rate coefficients for selected ions.
- The authors also include some corrections for Ca-like ions (K. P. Dere 2007, private communication).
- The DR and RR rate coefficients used here are those of Bryans et al. (2006) but updated to include recent corrections to the fitting of some of the rate coefficients (Badnell 2006b).
- Here the authors provide an electronic table of the CIE fractional abundances for all elements from H through Zn calculated using these data (Table 2; Fe shown only to illustrate the format and content).
5. A NEW APPROACH TO DERIVE AVERAGE EMS AND TEMPERATURES
- Using the method described in Section 3, the assumption of constant temperature and density, and their updated CIE results, the authors can calculate the EM curve for each of the observed spectral lines listed in Table 1.
- The authors calculate the EM curves using a constant electron density of 1.8 × 108 cm−3 as was reported by Feldman et al. (1999) for the same source region.
- Step 1 of their approach is to take the mean of all crossing points of the EM curves for a given group of lines.
- This can be seen in the left panel of Figure 3.
- Also, because of the shape of the curves, any outlying crossings are far more likely to occur at a higher EM than at a lower EM.
6. CORONAL ABUNDANCE ENHANCEMENT FACTORS
- There they used only a single line, whereas here the authors use two.
- The authors have repeated the analysis using the Mazzotta et al. (1998) CIE fractional abundances.
7. ANALYSIS BY GROUPS
- Using their derived coronal abundances the authors calculate the EM and Te of each of the line categorizations given in Section 2.
- Figures 7–15 show the GEM approach as applied to each of these groups.
- For the Group I and II categorizations, the authors show their individual subcategorizations as well as the groups as a whole.
- In the case of Group IIb, the emission lines have been further subdivided by separating out the N v and O vi lines.
- The authors elaborate on the possible reasons for this in Section 8.
8.1. Updated CIE Fractional Abundances
- One of the aims of this paper is to investigate the effect of their new CIE fractional abundances on the EM analysis.
- The authors also compare with the recently recommended CIE fractional abundances of Bryans et al. (2006) in Figure 2.
- Differences between the current CIE results and those of Mazzotta et al. (1998) are large for all elements other than H, He, and Li. Factors of typically at least 2 difference in abundance are found for at least one ionization stage of each of these elements.
- The authors attribute all these differences primarily to the EII rate coefficients.
- In Sections 8.2 and 8.4 the authors discuss the impact of these updated CIE calculations on the analysis of the present SUMER observation.
8.2. Comparison With FIP Factor Observations
- For this same SUMER observation, FIP factors were also determined by Feldman et al. (1998).
- First, their reference EM value is taken from the crossing of two Ar EM curves whereas Feldman et al. (1998) use the emission from a single Li-like O vi line as their reference value.
- Furthermore, in determining the FIP factor for each element the authors generally use more emission lines than Feldman et al. (1998).
- They estimate log10 Te = 6.13 (the same value at which the authors ultimately arrive) but only calculate these FIP factor versus.
- The error bars on their results for Na and Ca are also relatively large and the Feldman et al. (1998) results lie within these errors.
8.3. Comparison with the FIP Factor Model
- The FIP effect model of Laming (2004, 2009) allows an opportunity to quantitatively compare their derived coronal elemental abundances with those of theory.
- The Laming model builds on that of Schwadron et al. (1999) by explaining the FIP effect in terms of Alfvén waves in the chromosphere.
- The authors results suggest that upward wave energy fluxes in this range best describe the solar conditions at the time of this particular SUMER observation.
- The authors data generally fit the model well, with the exception of K.
- It should also be noted that the low-FIP results of the present work were calculated relative to a high-FIP enhancement of 1, while in the Laming model the high-FIP elements do show a slight abundance variation dependent on their FIP value.
8.4. Groups
- The authors have used the same group splitting as that used by Landi et al. (2002) and thus can compare directly with their results.
- Figure 10 shows the EM curves for the lines in Group IIa.
- Given the disagreement with the other lines in Group IIa, and the lower formation temperature of N v and O vi compared to the other ions in the group, it is possible that the emission lines from these two ions originate from a different region of plasma.
- In addition to the comparison of EM within Group II, the authors also compare the EM from the Li- and Na-like ions (Group IIa∗) with the EM derived from every other ion in the observation (i.e., those from Groups I, IIb, and III).
- The authors results have larger errors, which the authors believe to be more realistic due to their more rigorous method of calculating the mean and standard deviation of EM and Te.
8.5. Other Issues
- There are a number of indications that the observed emission does not come from an isothermal plasma.
- It is also possible that the relatively large errors in EM and Te are suggestive of a non-isothermal plasma.
- This issue has been raised by Feldman & Laming (2000) in reference to Fe8+ emission.
- These authors found that the contribution function of emission from Li-like lines only becomes significantly affected on reaching densities 1011 cm−3, orders of magnitude higher than the density of 1.8 × 108 cm−3 inferred by Feldman et al. (1999) for the observation analyzed here.
- Again, such a study is beyond the scope of this paper.
9. PROPOSALS FOR FUTURE OBSERVATIONS
- The authors work shows that SUMER observations can go a long way toward constraining FIP models such as those of Laming (2004, 2009).
- Even better constraints can be achieved through the simultaneous observation of lines from a number of additional charge states.
- More lines from high-FIP elements such as N, O, Ne, and Ar are required to better determine the EM for these high-FIP elements, which can then be used to normalize the low-FIP elements.
- For N, O, and Ne, emission lines from H- and He-like stages need to be observed to avoid using Li-like ions.
- This may require simultaneous observations using separate, crosscalibrated spectrometers.
10. SUMMARY
- This work has re-analyzed data from a SUMER coronal observation in an attempt to improve upon previous methods of analysis.
- Their results differ from those of Landi et al. (2002) in certain respects.
- Also, the previously reported discrepancy between the EM derived from Li- and Na-like lines and the EM from all other lines (Groups I, IIb, and III) is not supported by their results, rather the two agree at the 1σ level.
- CHIANTI is a collaborative project involving the NRL (USA), RAL (UK), MSSL (UK), the Universities of Florence and Cambridge (UK), and George Mason University (USA).
- P.B. and D.W.S. were supported in part by the NASA Solar and Heliospheric Physics Supporting Research and Technology program and the NASA Astronomy and Physics Research and Analysis Program.
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Citations
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Cites background or methods or result from "A new approach to analyzing solar c..."
...In their papers Bryans et al. (2006, 2009) compare the electron-impact ionization (EII) and recombination data with earlier data sets and with experimental measurements....
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...Bryans et al. (2009) use the Dere (2007) data due to its broader scope, but the authors note (and we agree) that this discrepancy should be revisited and if possible resolved in the future....
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...Detailed information can be found in the papers of Bryans et al. (2006, 2009)....
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...Bryans et al. (2006, 2009) have produced a new compilation for elements from hydrogen (Z = 1) to zinc (Z=30), which we have included in AtomDB v2....
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References
2,116 citations
"A new approach to analyzing solar c..." refers methods in this paper
...For example, Landi et al. (2002) compared off-disk spectral observations of the solar corona with predictions from the CHIANTI version 3 atomic database (Dere et al. 1997, 2001)....
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1,041 citations
"A new approach to analyzing solar c..." refers background or methods or result in this paper
...As expected, differences between the present results and those of Bryans et al. (2006) are not as large as those found between the present results and those of Mazzotta et al. (1998)....
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...Same as Table 3 but for silicon and using the DR and RR rate coefficients of Mazzotta et al. (1998) for ions not calculated by Badnell (2006b,c)....
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...We label our results as “New” and those of Mazzotta et al. (1998) as “Old”....
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...The DR and RR data for all other ions are those of Mazzotta et al. (1998)....
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...Such variation between the current results and those of Mazzotta et al. (1998) is a result of the new recombination and ionization rate coefficients being used here....
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903 citations
"A new approach to analyzing solar c..." refers background in this paper
...For example, the so-called coronal heating problem remains unsolved (Gudiksen & Norlund 2005; Klimchuk 2006) and we are still unable to explain the onset processes that cause solar flares and coronal mass ejections (Forbes 2000; Priest & Forbes 2002)....
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873 citations
"A new approach to analyzing solar c..." refers background in this paper
...For example, the so-called coronal heating problem remains unsolved (Gudiksen & Norlund 2005; Klimchuk 2006) and we are still unable to explain the onset processes that cause solar flares and coronal mass ejections (Forbes 2000; Priest & Forbes 2002)....
[...]
751 citations
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Frequently Asked Questions (7)
Q2. What is the effect of the Alfvén waves on the chromosphere?
These Alfvén waves drive a pondermotive force on their reflection or transmission at the chromosphere–corona boundary which results in the elemental fractionation.
Q3. What is the powerful tool for understanding the properties of the solar corona?
One of the most powerful tools for understanding the properties of the solar corona is spectroscopy (Tandberg-Hanssen & Emslie 1988; Foukal 2004).
Q4. What is the contribution function of emission from Li-like lines?
These authors found that the contribution function of emission from Li-like lines only becomes significantly affected on reaching densities 1011 cm−3, orders of magnitude higher than the density of 1.8 × 108 cm−3 inferred by Feldman et al. (1999) for the observation analyzed here.
Q5. Why is there no common intersection of all EM curves at a single?
Due to oversimplifications of the plasma model, uncertainties in the observations, and errors in the atomic data, there is no common intersection of all EM curves at a single [Tc, EMc].
Q6. What does the fieldman et al. (1998) use to determine the FIP factors?
Feldman et al. (1998), however, use only one or two emission lines to determine the FIP factors for each of the elements they consider.
Q7. What is the EM curve for each of the observed spectral lines?
Using the method described in Section 3, the assumption of constant temperature and density, and their updated CIE results, the authors can calculate the EM curve for each of the observed spectral lines listed in Table 1.