Issue |
A&A
Volume 511, February 2010
|
|
---|---|---|
Article Number | A60 | |
Number of page(s) | 13 | |
Section | Atomic, molecular, and nuclear data | |
DOI | https://doi.org/10.1051/0004-6361/200912392 | |
Published online | 10 March 2010 |
Recommended data on proton-ion collision rate coefficients for Fe X-Fe XXIII ions
I. Skobelev1,2 - I. Murakami1 - T. Kato1
1 - National Institute for Fusion Science, Oroshi-cho, Toki, Gifu, 509-5292, Japan
2 -
Joint Institute for High Temperatures of RAS, Izhorskaya 13/19, 125412 Russia
Received 27 April 2009 / Accepted 4 December 2009
Abstract
Aims. Proton-ion collisions are important for excitation or
de-excitation of certain excited states in a high-temperature low
density astrophysical plasma.
Methods. In the present work an evaluation of data obtained for
proton-induced transitions in Fe X-Fe XXIII ions is carried out with
the help of different theoretical methods.
Results. A simple analytical formula with seven parameters is
suggested. This formula allows us to describe the dependence of the
proton rate coefficient on the proton temperature in a wide temperature
range. The values of the free parameters have been determined by
fitting the approximation formula to numerical data and are presented
for recommended data together with fitting accuracies. By comparing
proton collision rates with electron rates it is shown that proton
impact excitation processes may be important for Fe X, XI,
XIII-XV, XVII-XXIII ions. The results obtained can be used for plasma
kinetics calculations and for the development of spectroscopic methods
of astrophysical plasma diagnostics.
Key words: atomic processes - atomic data - plasmas
1 Introduction
The importance of proton-ion collisions for ion kinetic calculations
was first demonstrated by Seaton (1964) for the case of the Fe XIV ion.
It has been shown that proton excitation rates can become comparable
to (or even larger than) the electron excitation rates for transitions
for which the excitation energy
E is much smaller than the proton temperature
.
It should be noted that often proton-ion collisions are not important
for populating ion levels even in the case
,
i.e. this condition is necessary but is not sufficient.
For example, such a situation occurs in dense plasma where closely
spaced ionic levels are as a rule statistically populated.
In low density plasma the importance of proton-ion collisions may be
very high especially for transitions within the ground configuration of an ion.
The number of such transitions is not very large and so, compared to
the electron processes, relatively little data are required to account
for proton processes in a particular ion.
In principle, proton collision can influence the population kinetics by increasing either excitation rates for some levels or their collision decay rates.
An increase of excitation rates can be important only for levels i
near the ground ion state (or close to a strongly metastable state).
In this case proton collision will be important for a plasma
with an electron density
which satisfies the condition
![]() |
(1) |
(where Ai and

Increase of collision decay rates can be important for excited
levels i if the proton density satisfies the reverse condition
![]() |
(2) |
If radiative decay of level i is allowed, the last condition can be valid only in a dense plasma (laser-produced plasma, Z-pinches, exploding wires), while for metastable levels it can be satisfied even in low density astrophysical or laboratory plasmas.
Thus, proton excitation/de-excitation of fine-structure transitions involving ground or low-lying ion metastable states are of primary interest.
At present there are a lot of papers where proton-ion
collision rates Cij have been calculated for different Fe ions.
In these papers proton collision rate coefficients were published
in a table form. Because positive ions repel protons, the rate coefficients
fall sharply to zero at the threshold energy, and tabulated values of
rate coefficients typically change by several orders of magnitude
over a small temperature range. For many applications tabular data
presentation is not very convenient, and some analytical representation
would be preferable. Therefore the purpose of
the present work was not only an evaluation of proton rates calculated
for Fe X-Fe XXIII ions with the help of different methods, but also
the choice of a simple function allowing us to describe dependencies
for all transitions considered.
2 Methods used for calculations of proton rate coefficients
Several different methods, both semiclassical and quantal, can be employed in deriving proton rate coefficients (see for example reviews by Dalgarno 1983; Reid 1988; Copeland et al. 1997; Young et al. 2003).
The most basic is the semiclassical (or impact-parameter) approach in which the position of the proton relative to the ion is treated classically. This approach was originally applied to Coulomb excitation of nuclei by Alder et al. (1956) and first extended to the proton excitation of ions by Seaton (1964). In the case of semiclassical calculations, either first-order approximations or close-coupling approximations have been used.
At low proton energies the semiclassical first-order approximation is valid at all impact parameters because the interactions between the proton and electrons of an ion are weak due to Coulomb repulsion of proton and ion. At intermediate energies and low impact parameter values the first-order approximation fails, and it is necessary to adopt a different approximation or solve numerically the coupled differential equations describing the interaction. In the semiclassical close-coupling approximation, the transition probabilities are determined by means of the numerical solution of coupled differential equations, thereby removing the need for first-order approximations and hence the uncertainty in the intermediate energy range.
Generally speaking, the most accurate method is to treat the proton's trajectory quantum mechanically and solve the complete set of close-coupling equations. Such an approach is commonly used in R-matrix calculations of electron-ion collisions; however, it is computationally much more demanding for proton collisions, and only a few results were obtained for Fe ions by this method. Within the semiclassical approach, it has been shown that symmetrizing the problem with respect to the initial and final velocities (Alder et al. 1956), and including polarization effects (Heil et al. 1982, 1983), can improve the accuracy of the proton rates. In the paper of Faucher & Landman (1977) it has been shown that for highly charged ions both a quantum and a semiclassical close-coupling approach can give very close results.
It should be noted that an estimation of the accuracy of the computations is very difficult. In the best cases we can expect a data accuracy of about 10-25% (see also Copeland et al. 1997).
3 Analytical function for an approximation of the dependencies of proton collision rates on proton temperature
In the present work we have used a simple function to approximate
calculated temperature dependencies
:
![]() |
(3) |
In Eq. (3)

It should be mentioned that Eq. (3) is not based on the known properties of the rate coefficients. It has a qualitatively correct behavior at low temperatures and absolutely incorrect behavior at high temperature. But in the temperature range that is most important for plasma applications, Eq. (3) allows us to describe numerical data with an accuracy better than 5% for all transitions in all ions considered. The values of the seven free parameters and the temperature ranges over which the fit is valid are presented in the present paper together with approximation accuracies. Note that functions with five to nine free parameters are now often used in different databases to store data on electron-ions collisions.
The values of the free parameters pi were determined by the following two-stage procedure. In the first stage we chose manually initial values pi(0) which gave the correct qualitative temperature-dependence of the rate coefficient. In the second stage we constructed a seven-dimensional grid around the point pi(0) with steps of about 0.01pi(0). The differences between the theoretically-calculated rate coefficients and the approximation Eq. (3) were then calculated at all given temparatures for all points of the grid. If for some grid point this difference was less than 5% for all temperatures, the calculation was stopped, and the coordinates of this grid point were taken as the required pi values. The values of pi determined in this way do not give the best fit of Eq. (3) to the theoretically-calculated values (which was not our purpose), but they provide approximations to the theoretically-calculated results with an accuracy better than the intrinsic accuracy of those theoretical results. Such simple approximations are currently employed to include detailed radiation-collisional ion kinetics in two- and three-dimensional plasma gas-dynamical calculations.
4 Results
4.1 Chlorine-like Fe X (3s23p5 2P)
For the Fe X ion proton collision excitation is important for only
one transition
-
.
Bely & Faucher (1970) used a symmetrized first-order semiclassical
approximation to calculate the proton cross section and rate coefficient
for the
transition in Fe X.
In the intermediate energy range, where a first-order theory breaks down,
an approximation referred to as Coulomb-Bethe II was employed, borrowed
from the theory of electron excitation of positive ions, to determine
the cross section. Bely & Faucher (1970) estimate their rate coefficients
to be accurate to within 50% for the first ions in the chlorine isoelectronic
sequence. The estimated error is smaller for the more highly charged ions.
Kastner (1977) and Kastner & Bhatia (1979) also used the first-order semiclassical approximation for low energies, while for intermediate energies a form for the cross section due to Bahcall & Wolff (1968) was used. From the comparison presented in Fig. 1 one can see that the results of Kastner (1977) and Kastner & Bhatia (1979) are on the whole lower than the earlier values of Bely & Faucher (1970). All results agree within 50% throughout the temperature range of 50-350 eV, while for temperatures <100 eV the agreement is very good. Because the first-order semiclassical approximation systematically overestimates the rates in the high energy region, we recommend to use the data of Kastner & Bhatia (1979), but we present in Table 1 the results of the approximation for both the data of Kastner & Bhatia (1979) and of Bely & Faucher (1970).
Table 1: The values of fitting parameters, defined in Eq. (3), for proton excitation rate coefficients of transitions in ions Fe X-Fe XV.
Bhatia & Doschek (1995) calculated the rate of this transition for a single temperature value of 106 K. As we see from Fig. 1 this result agrees with both Bely & Faucher (1970) and Kastner & Bhatia (1979) as well as with our fitting.
In Fig. 1 the electron collision rate coefficient calculated by
Aggarwal & Keenan (2005b) is also presented. It can be seen that proton
collisions will influence the population of the
level in plasmas with temperature higher than 100 eV.
![]() |
Figure 1:
Proton collision rate coefficient for transition
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4.2 Sulfur-like Fe XI (3s23p4 3P)
For the Fe XI ion proton collisions must be taken into account for
three transitions between the fine structure components of the ground
term. The corresponding rate coefficients
have been calculated by Landman (1980) with the help of a symmetrized,
semiclassical close-coupling method. This method retains the classical
treatment for the proton trajectory, but the transition probabilities
are determined by numerically solving the close-coupling equations,
removing the uncertainties at intermediate energies of the first-order
approximation. For the transitions
at a temperature
of
K the proton rates were calculated
by Bhatia & Doschek (1996)
with the help of the first-order semiclassical approach.
It can be seen from Fig. 2 that the first-order approach significantly
overestimates the collision rates.
We fitted the data of Landman (1980) by Eq. (3), and the results for pi are presented in Table 1, while dependencies of the rate coefficients on the proton temperature are shown in Fig. 2.
In Fig. 2 the electron collision rate coefficients calculated
by Gupta & Tayal (1999) are also presented. It can be seen that
proton collisions will influence the population of the
levels in plasma with a temperature higher
than 100 eV.
![]() |
Figure 2:
Proton collision rate coefficients for the transitions
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4.3 Phosphorus-like Fe XII (3s23p3 4S, 2D, 2P)
For the Fe XII ion proton collisions must be taken into account for
ten transitions between fine structure components of the ground
configuration. The corresponding rate coefficients have been calculated
by Landman (1978) with the help of a symmetrized, semiclassical
close-coupling method.
We fitted the data of Landman (1978)
by Eq. (3). The obtained values of pi are presented in Table 1
and the dependencies of rate coefficients on proton temperature are
shown in Figs. 3-5.
In Figs. 3-5 the electron collision rate coefficients calculated by Binello et al. (1998) are also presented. It can be seen that proton collisions are not important for the kinetics of the Fe XII ion in the plasma with any reasonable temperature.
![]() |
Figure 3:
Proton collision rate coefficients for transitions
in P-like Fe XII: thick solid, dashed and dot lines - formula (3),
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![]() |
Figure 4:
Proton collision rate coefficients for transitions in
P-like Fe XII: solid, dashed and doted lines - Eq. (3),
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![]() |
Figure 5:
Proton collision rate coefficients for transitions in
P-like Fe XII: solid, dashed and doted lines - Eq. (3),
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4.4 Silicon-like Fe XIII (3s23p2 3P, 1D, 1S)
For the Fe XIII ion it is necessary to consider ten transitions
among the levels of the ground configuration
.
Cross sections and
rate coefficients for these transitions have been obtained by using the
semiclassical close-coupling theory (Masnou-Seeuws & McCarroll 1972;
Landman 1975), a first-order semiclassical method (Sahal-Breshot 1974;
Kastner 1977; Kastner & Bhatia 1979) and a quantal approach to
the close-coupling method (Faucher 1977; Faucher & Landman 1977).
The quantal approach is based on the work of Faucher (1975)
which adapts the electron-ion quantum collision theory (Bely et al. 1963)
to the proton-ion case. While such quantal calculations can model
the short-range interaction more accurately, it is possible to expect
that the accuracy of the data of Faucher (1977) and Faucher & Landman (1977)
is higher than others (Masnou-Seeuws & McCarroll 1972; Landman 1975;
Sahal-Brechot 1974; Kastner 1977).
In Fig. 6 the proton excitation cross-sections between the fine
structure levels of
are shown as a function of
the incident proton energy. In this figure quantum results of
Faucher (1975, 1977) and Faucher & Landman (1977) (square) are compared
with semi-classical results of Landman (1975) (solid line) and of
Masnou-Seeuws & McCarroll (1972) (dotted line). It can be seen from
this figure that the semi-classical cross-sections obtained in
Landman (1975) by directly solving Schrodinger's equation are very similar
to those obtained by Faucher (1975) with a quantum method in the low and
intermediate energy range.
![]() |
Figure 6:
Proton excitation cross sections for transitions in
Si-like Fe XIII: squares - quantum results of Faucher (1977),
solid line - semi-classical results of Landman (1975),
dotted line - semi-classical results of Masnou-Seeuws & McCarroll (1972);
for (1) the
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Among the two available calculations of
Masnou-Seeuws & McCarroll (1972) and Landman (1975) we choose the data of
Landman (1975) because these data agree better with the
quantum calculations of Faucher (1977) and Faucher & Landman (1977) and
are presented for a wider range of transitions. In Landman (1975) data are
given for all transitions between the individual magnetic sublevels of
the
and
levels of
the ground configuration.
These rates have been summed over the magnetic sublevels and fitted
to Eq. (3).
Results obtained are presented in Table 1 and Figs. 7-9.
In Figs. 7-9 the electron collision rate coefficients calculated by
Aggarwal & Keenan (2005a) are also presented. It can be seen that
proton collisions will significantly influence the population of the
and
levels in plasma with a
temperature higher than 200 eV and will not influence the population of the
level.
![]() |
Figure 7:
Proton collision rate coefficients for transitions in
Si-like Fe XIII: thick solid, thin solid, dashed and doted lines - Eq. (3),
diamonds - data of Landman (1975) for the
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![]() |
Figure 8:
Proton collision rate coefficients for transitions in
Si-like Fe XIII: solid, dashed and doted lines - Eq. (3),
diamonds - data of Landman (1975) for the
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![]() |
Figure 9:
Proton collision rate coefficients for transitions in
Si-like Fe XIII: solid, dashed and doted lines - Eq. (3),
diamonds - data of Landman (1975) for the
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4.5 Aluminium-like Fe XIV (3s23p 2P)
For the Fe XIV ion the proton collision rates are important only for one
transition
.
For this transition
data calculated with the help of all methods considered above are available.
In the papers of Bely & Faucher (1970), Kastner & Bhatia (1979), and Burgess & Tully (2005) a first-order semiclassical theory has been used with different methods of a limitation of the transition probabilities for small values of the impact parameter. In the work of Landman (1975) the rate coefficient was calculated using a semi-classical close-coupling treatment analogous to Masnou-Seeuws & McCarroll (1972). Close-coupling quantal calculations have been carried out by Heil et al. (1983). The cross sections calculated in this paper are probably the most accurate for Fe XIV to date because of the approach (Heil et al. 1983) to model the interaction accurately not only by expressing the short-range term accurately, but also by including the polarization term for the long-range interaction as well as the quadrupole term. The results obtained in these papers are shown in Fig. 10. It can be seen that as usual the first-order semiclassical method overestimates the rate coefficient in medium and high energy regions, and the semiclassical close-coupling results are close enough to the quantal calculations. It should be noted that the results in Landman (1975) at higher temperatures are higher than the data in Heil et al. (1983). This is likely caused by the following reason. In Heil et al. (1983) the cross sections were calculated only for a proton energy of up to 900 eV, which is not large enough to obtain reliable rate coefficients at high temperatures. In Landman (1975) a wider energy range (up to 2900 eV) was considered. Therefore we have chosen the data of Landman (1975) as our recommended data and fit them in Eq. (3). The results obtained are presented in Table 1.
In Fig. 10 the electron collision rate coefficient calculated by
Storey et al. (1996) is also presented. It can be seen that proton
collisions will strongly influence the population of the
level in the plasma with a temperature higher than 200 eV.
![]() |
Figure 10:
Proton collision rate coefficients for the transition
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4.6 Magnesium-like Fe XV (3s3p 3P)
Two calculations (Kastner 1977; Landman & Brown 1979) have been
carried out for the fine-structure transitions
in magnesium-like Fe XV. In Kastner (1977) a first-order
semiclassical theory was used, while the calculations of Landman & Brown (1979)
were based on the semiclassical close-coupling treatment. We recommend
to use the results of Landman & Brown (1979) and corresponding fitting
parameters are presented in Table 1. The dependencies of the proton rate
coefficients on proton temperature are shown in Fig. 11.
In Fig. 11 the electron collision rate coefficients calculated by
Aggarwal et al. (2003a,b) are also presented. It can be seen that proton
collisions will significantly influence the population of the
levels in plasma with a temperature higher than 400 eV.
![]() |
Figure 11:
Proton collision rate coefficients for the transitions in
Mg-like Fe XV: solid, dashed and doted lines - Eq. (3),
diamonds - data of Landman & Brown (1979) for the
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It should be noted that in the CHIANTI database (Young et al. 2003) for proton impact excitation of transitions in Fe XI, XII, XIII, and Fe XV ions, the data presented in the papers by Landman (1980, 1978, 1975), and Landman & Brown (1979) are used. These data are the same as we recommend in the present paper. For Fe X they use the data in Bely & Faucher (1970), while we recommend the data in Kastner & Bhatia (1979), and for Fe XIV they use unpublished calculations by Tully J. (2002, unpublished), while we recommend data in Landman (1975).
4.7 Ne-like Fe XVII ion (2s22p53s 3,1P)
For Ne-like Fe XVII we know only one paper of Landman (1985) where
proton collisional excitation rate coefficients have been calculated for
transitions among the
levels.
The calculations have been performed according to a symmetrized semiclassical
impact parameter theory in which the truncated Schrodinger equation for
quadrupole excitation is directly integrated. Intermediate coupling wave
functions for the J = 1 levels were determined
using the observed
energy levels; otherwise, the Slater and spin-orbit interaction integrals
obtained with Froese Fischer's MCHF77 program (Froese Fischer 1978) were
used. The LS-coupled quadrupole interaction matrix was then converted to
intermediate coupling according to the derived transformation coefficients.
The results of Landman's calculations (Landman 1985) are presented in Figs. 12 and 13. Note that at present no other theoretical or
experimental results are available for a comparison of the proton rate
coefficients. It is possible to compare proton collision excitation with
electron excitation. In Figs. 12 and 13 the electron rate coefficients
calculated by extrapolation of the data of Aggarwal et al. (2003a,b) in the low
energy region are presented. It should be noted that designations of
energy levels used in the paper of Aggarwal et al. (2003a,b) (namely,
,
and
)
differ from the designations
used in paper of Landman (1985)
(namely,
,
and
).
Our presentation of the proton rate coefficients in Figs. 12 and 13 and
in Table 2 corresponds to the designations of Aggarwal et al. (2003a,b).
One can see from Figs. 12 and 13 that in the region
K
proton collisions are important for all levels considered.
Table 2: The values of fitting parameters, defined in Eq. (3), for proton excitation rate coefficients of transitions in ions Fe XVII-Fe XXIII.
![]() |
Figure 12:
Collision rate coefficient for transition
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Figure 13:
Collision rate coefficient for the transition
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We fitted the data of Landman (1985) by Eq. (3) and the values of pi obtained are presented in Table 2.
It should be noted that proton collisions can not effectively
excite
levels from the ground level. However,
the
and
levels are metastable and can have
substantial population densities in relatively low density plasma.
Therefore, proton collisions can play a significant role at densities
where the collision depopulation of these levels competes with their
radiative decay. Under these conditions, for example, the relative
intensities of the
M1 and
M2 lines relative to
the
line may provide
useful density diagnostics (Landman 1985). Because of the radiative
probabilities
,
,
(see, for example, Landman 1985) it follows from the data presented in Figs. 12 and 13
and condition (2) that proton collision decay will be
important for the
level at
and for the
level at
.
Note that the CHIANTI database (Young et al. 2003) does not use proton impact
de-excitation data.
4.8 F-like Fe XVIII ion (2s22p5 2P3/2-2P1/2)
Several semiclassical calculations, both first-order and close-coupling, have been performed for the Fe XVIII ion. The first-order semiclassical calculations have been done by Kastner & Bhatia (1979) and some later by Feldman et al. (1980).
The close-coupling semiclassical method of Reid & Schwarz (1969)
has been used by several authors to calculate both proton collision
excitation cross sections and rate coefficients for the
transition in Fe XVIII
(Keenan & Reid 1987, 1989; Foster et al. 1994). In the earlier paper of
Keenan & Reid (1987) aspects like the polarization effects,
symmetrization of coupled equations, or departures from LS-coupling
were not considered. Later Keenan & Reid (1989) have developed
this method to incorporate symmetrization with respect to channel
velocities, and in a further development, Foster et al. (1994) have
improved the accuracy of the calculations by considering both
symmetrization and polarization effects, whereby they have included
the
level by means of a polarization potential.
The inclusion of these factors has resulted in a difference of 60%
in the cross sections compared with those of Keenan & Reid (1989, see Fig. 14).
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Figure 14:
Proton collision cross section for the transition
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The importance of including polarization effects in
intramultiplet excitation collisions was noted in the papers of
Heil et al. (1982, 1983) where a quantal molecular approach was used to
describe the proton-ion interaction. In the calculations of Foster et al. (1994),
the polarization was taken into account by the inclusion of the
state alone. For Fe XVIII ion the major component
of the polarization can be really incorporated by a single state,
because the next states that contribute to the polarization (i.e., states
with configuration
)
have about six times larger excitation
energies than
.
This is a feature of highly charged F-like
systems and, generally speaking, one would not expect that a single state
could give a good representation of the polarization in a general case.
The excitation rate coefficients obtained in
Kastner & Bhatia (1979), Feldman et al. (1980), Keenan & Reid (1989),
and Foster et al. (1994) are presented in Fig. 15. It should be noted
that results from Foster et al. (1994) are more than a factor of two smaller
than the semiempirical results of Kastner & Bhatia (1979) and
Feldman et al. (1980) over the narrow temperature range for which
they present results, and are 30-36% lower than the results of Keenan & Reid (1989), where the effects of the
state were not included.
We recommend using the data of Foster et al. (1994), and present the corresponding
values of fitting parameters in Table 2.
![]() |
Figure 15:
Proton collision rate coefficient for the transition
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The extrapolation of the results obtained in Hummer et al. (1993) for the
excitation of the transition
by
electron impact shows that in the temperature region
K
the electron rate coefficient is about
.
It means that in a plasma with
the excitation by proton impact
can increase the population of the
level only by
10%. Of course, at
the influence of the proton excitation
may be more important.
Note also that the critical density in Eq. (1) for the transition
considered is about
(see, for example,
Foster et al. 1994). It follows from this that the proton excitation process
may be important for Fe XVIII ion only in the low density plasma with
,
and it is not necessary to take this process into
account for simulations of more dense plasma kinetics.
Foster et al. (1994) used their proton excitation rates to
calculate the intensity ratio R for the spectral lines
and
at plasma parameters
determined independently in the experiment on the JIPP T-II-U tokamak
(Nagoya, Japan) and showed that the modeling results agree
very well with results observed by Sato et al. (1986).
The CHIANTI database uses data of Foster et al. (1994).
4.9 O-like Fe XIX ion (2s22p4 3PJ)
There is only one paper of Feldman et al. (1980) where data on
the proton excitation of the
and
transitions in O-like Fe XIX ion were calculated by a first-order
semiclassical method and are presented for one temperature value.
There are unpublished data calculated by Ryans et al. by using the semiclassical close-coupling approach of Reid & Schwarz (1969). These data are now used in the CHIANTI database (Young et al. 2003) and only these data have been fitted to Eq. (3) in the present work.
In Figs. 16-18 we present: 1) the result of our fit of the proton
excitation rates; 2) the proton excitation rates calculated in Feldman et al. (1980); 3)
the proton excitation rates calculated in
Ryans, Keenan, & Reid (unpublished);
and 4) the electron excitation
rate coefficients obtained by Butler & Zeippen (2001b). It can be seen
from Figs. 16 and 17 that proton-ion collisions will strongly influence
the population of the
and
levels at practically all
reasonable values of temperature. It is interesting that the electron
rate coefficient for the
transition (not presented in Fig. 18)
is higher than the proton one by about two orders of magnitude. This means that
collision mixing of the
and
levels will occur only by
electron-ion collisions. The probabilities of radiative decay for
the levels
and
are (Cheng et al. 1979):
,
and
.
Because for temperatures about 107 K the electron collision rate coefficient
for the
transition is about
(Butler & Zeippen 2001b), it is possible to conclude that in a plasma
with
electrons will cause a Boltzmann
equilibrium among the fine-structure levels, and proton collision will not
be important for ion kinetics.
![]() |
Figure 16:
Collision rate coefficients for the transition
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Figure 17:
Collision rate coefficients for the transition
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Figure 18:
Collision rate coefficient for the transition
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4.10 N-like Fe XX ion (2s22p3 4S3/2, 2D 3/2,5/2, 2P 1/2,3/2)
At present there is only one paper where Bhatia & Mason (1980)
have used the semiclassical first-order method of Bely & Faucher (1970)
to calculate proton impact excitation of fine-structure transitions
in Fe XX ions. We have fitted these data to Eq. (3) and the results
obtained are presented in Table 2. In Figs. 19, 21 the temperature
dependencies of the proton excitation rates are shown together with
the electron excitation rates calculated by Butler & Zeippen (2001a).
It can be seen that for practically all transitions (except for
)
the proton rate coefficients are
comparable or larger than the electron ones at all reasonable temperatures.
The density region where proton collisions are important for the population
kinetics of the fine-structure levels can be estimated from Eq. (2)
by using the radiative probabilities calculated in the paper of Bhatia & Mason (1980).
Because the total radiative decay probabilities are
,
,
,
and
,
we find that it is
necessary to take into account the proton collisions in the kinetic calculations
for a plasma with an electron density of
.
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Figure 19:
Collision rate coefficients for the transitions
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Figure 20:
Collision rate coefficients for the transitions
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Figure 21:
Collision rate coefficients for the transitions
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The CHIANTI database uses the data of Bhatia & Mason (1980).
4.11 C-like Fe XXI ion (2s22p2 3P)
Several calculations, both semiclassical and quantal have been performed for the ground configuration of the Fe XXI ion.
Close-coupling semiclassical calculations have been done by
Ryans et al. (1999a,b). They consider the
,
and
transitions among the fine-structure levels
of carbon-like Fe XXI and have calculated
the proton rates using the symmetrized close-coupling semi-classical
approach in which the interaction matrix elements were modified to give
them the correct short-range forms, and the effects of dipole coupling
to nearby terms were included by means of a polarization potential.
A set of excited terms was selected which are coupled to the ground state
by the E1 interaction. In the present case of the
ground state,
the terms that can contribute to the polarization have the symmetry
,
,
or
.
Therefore the calculations in the paper of
Ryans et al. (1999a) were made in two approximations: 1) when only the
three excited terms
,
,
and
were
included in the calculation via the polarization potential and 2) when
the terms
and
were also
included to test the convergence of the results. It has been shown that
for the Fe XXI ion and for protons as perturbers the inclusion of the
further excited terms had a small effect on the cross sections.
For Fe XXI as well as for other heavy ions the polarization affects
the cross sections significantly at all impact energies. However,
for the heavy ions the polarization potential is dominated by the
terms, because the excitation energies of the
,
and higher configurations are much higher than the
excitation energies of
.
This means that the representation of the
polarization by the
terms is adequate to calculate the
transitions in the Fe XXI ions.
Note that additionally including
terms does not allow us to
increase the accuracy of the calculation, because in this case the includion of
some other configurations (for example,
)
is also needed.
The results of the calculations of Ryans et al. (1999b) where only the
configuration was taken into account for the polarization potential are
shown in Figs. 22-24. Note also that in the low energy tail of
the cross sections, where the close-coupling calculations are difficult,
the first-order cross sections modified to allow for polarization were
used in the calculations of the proton rate coefficients by Ryans et al. (1999b).
These rate coefficients were fitted to Eq. (3) and the results
obtained are presented in Table 2. Note that the CHIANTI database uses the
data of Ryans et al. (1999b).
![]() |
Figure 22:
Collision rate coefficients for the transition
|
Open with DEXTER |
![]() |
Figure 23:
Collision rate coefficients for the transition
|
Open with DEXTER |
![]() |
Figure 24:
Collision rate coefficients for the transition
|
Open with DEXTER |
Earlier Faucher (1977) have considered a proton-impact excitation
of C-like Fe XXI using a quantal formulation. For Fe XXI the differences
between the results of Faucher (1977) and Ryans et al. (1999b) are significant,
especially for the
transition (see Figs. 22-24).
In Faucher's calculations the electrostatic interaction potential was
approximated by its long-range quadrupole part and no polarization effects
were taken into account. Ryans et al. (1999a) have made a special calculation
with the polarization omitted and with the same atomic data as Faucher (1977).
This calculation differs from Faucher (1977) only in two respects:
1) in the collision treatment - semiclassical versus quantal, and
2) in the interaction between matrix elements - short-range modified
forms versus purely asymptotic forms.
For the
and
transitions these
results are close to Faucher (1977) in the energy region of
KeV,
and for higher energies the progressive divergence in the two calculations
is due to the difference in the short-range part of the interaction potential.
For the
transition the discrepancy is more pronounced because
this strictly second-order process is more sensitive to the short-range
forms of the matrix elements (Ryans et al. 1999a). Thus, in the calculations of
Faucher (1977) two important effects (the modification of the interaction potential
at short distances and polarization) were not taken into account,
and we recommend to use the data of Ryans et al. (1999b).
Comparisons of proton and electron excitation rates are also shown
in Figs. 22-24. It is clearly seen that only for the transition
proton collisions are insignificant, while for the
transitions
and
the proton rates
dominate. According to the paper of Cheng et al. (1979) the total probabilities
of the radiative decay of the
and
levels are:
and
.
This means (see Eq. (2)) that only
in a plasma with
electrons will cause a
Boltzmann equilibrium among the fine-structure levels and the proton collision
will be unimportant for ion kinetics.
4.12 B-like Fe XXII ion (2s22p 2P, 2s2p2 4P)
At present for B-like Fe XXII there are only the calculations
made by Foster et al. (1996, 1997a,b). In these papers cross sections and
excitation rate coefficients for the fine-structure transitions within both
the ground
and the metastable
terms
have been obtained by the same method as in Foster et al. (1994).
In the former case (Foster et al. 1996), the
,
and
terms were included, while in the latter (Foster et al. 1997a,b),
the
term was also included. Additionally, in these
calculations the interaction matrix elements were modified to give them
the correct short-range forms. The values of the magnitudes of the required
matrix elements have been derived from the best available oscillator
strengths, while the signs of the matrix elements were taken to be those which
would arise from LS-coupled hydrogenic orbitals. This means that errors
might arise if the ion departs too far from LS-coupling. Therefore
Foster et al. (1997b) estimated the accuracy of their data for Fe XXII to be 30%
in the high temperature region. We have fitted the data of Foster et al. (1997b)
to Eq. (3) and the values of the fitting parameters are presented in
Table 2. The CHIANTI database uses the data of Foster et al. (1997b).
In Figs. 25 and 26 the temperature dependencies of proton excitation
rates are shown together with the data of Zhang & Pradhan (1997) for the
electron excitation rates. It is seen that for the transitions
,
and
the proton collisions dominate
at practically all reasonable temperatures, and for the
transition the proton collisions are
important at T > 107 K.
![]() |
Figure 25:
Collision rate coefficients for the transition
|
Open with DEXTER |
![]() |
Figure 26:
Collision rate coefficients for the transition
|
Open with DEXTER |
According to Cheng et al. (1979) the total probabilities
of a radiative decay of the levels considered are:
,
,
,
and
.
This means that proton collisions will be able to populate the
level at plasma densities of
(see Eq. (1)), and significantly influence the populations of the
levels at
(see Eq. (2)). So in this case it is necessary to take the proton excitation
processes into account in both low and high density plasma.
4.13 Be-like Fe XXIII ion (2s2p 3P0,1,2)
![]() |
Figure 27:
Collision rate coefficients for the transition
|
Open with DEXTER |
The excitation of Fe XXIII levels from the ground state by proton
impact is not important because the first excited configuration lies too
far from the ground configuration .
However, the first excited
configuration contains the closely spaced metastable levels
,
for which proton-induced transitions can be important. The are several
papers concerned with the calculation of the proton rates for these transitions.
Feldman et al. (1980) used a first-order semiclassical approach (see above) and presented the proton rate only at one temperature value.
More sophisticated calculations based on the semiclassical close-coupling method were carried out by Doyle (1987). The calculations were split into two energy ranges: a low-energy and an intermediate-energy range. For both energy ranges, the perturbing proton follows a classical Coulomb trajectory, but for the first range the first-order theory was used and close-coupling equations were solved only for the second region. Calculations were carried out with different short-range forms of interaction matrix elements, but no polarization effects have been taken into account.
The importance of including the effects of higher-lying states
in the calculation of proton rates via a polarization potential technique
was demonstrated by Foster et al. (1994) and Ryans et al. (1999a,b) for
the ground term fine-structure transitions in F-like and B-like ions.
Ryans et al. (1998) have extended this approach to Be-like ions and
calculated proton excitation cross sections and rate coefficients for the
transitions among the
fine-structure levels of Fe XXIII.
The cross sections for the transitions
were calculated by the same symmetrized close-coupled semiclassical
treatment that we have described above (F-like and B-like Fe ions):
the interaction matrix elements are modified to have the correct
short-range forms, and the effects of dipole coupling to nearby terms are
included by means of a polarization potential. In the case of the Fe XIII ion
dipole coupling to the
,
and
D terms
were included in the polarization potential. Ryans et al. (1998) estimated
the accuracy of their data for Fe XXII to be 20%. We have fitted the data of
Ryans et al. (1998) to Eq. (3) and the values of fitting parameters
are presented in Table 2. The CHIANTI database uses the data of Ryans et al. (1998).
In Fig. 27 the temperature dependencies of the proton excitation rates
calculated in the papers of Feldman et al. (1980), Doyle (1987), and Ryans et al. (1998)
are shown together with the data of Chidichimo et al. (2005) for electron
excitation rates. It is seen that proton collisions are very important
for the transitions
,
at T > 107 K and are insignificant for the transition
at practically all reasonable temperatures.
Among the components of the
term,
level
has the largest probability of radiative decay:
(Cheng et al. 1979). This means that in plasma with
the electron collisions alone can cause
a Boltzmann population distribution among the states of the
term.
In a lower density
plasma it is necessary to take the proton excitation processes into account
in collisional-radiative kinetic calculations.
5 Conclusions
In the present work the comparison of data obtained for proton-induced excitation transitions in Fe X-Fe XXIII ions by different theoretical methods is carried out. A simple analytical equation with seven parameters is proposed; this allows us to describe the proton temperature dependence of the proton rate coefficients in a wide temperature range. The values of the free parameters have been determined by fitting the equation with numerical data. The recommended data are presented together with the fitting accuracies. A comparison of the proton collision rates with the electron ones shows that the proton impact excitation processes may be important for the Fe X, XI, XIII-XV, and XVII-XXIII ions. The results obtained can be used for plasma kinetics calculations and for the development of spectroscopic methods of astrophysical plasma diagnostics.
AcknowledgementsPart of the present work was carried out when I.S. was a visiting professor at the National Institute for Fusion Science. The authors are grateful to Prof. R.M. More for a careful reading of the manuscript. Work of I.S. was partly supported by ISTC grant 3504.
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All Tables
Table 1: The values of fitting parameters, defined in Eq. (3), for proton excitation rate coefficients of transitions in ions Fe X-Fe XV.
Table 2: The values of fitting parameters, defined in Eq. (3), for proton excitation rate coefficients of transitions in ions Fe XVII-Fe XXIII.
All Figures
![]() |
Figure 1:
Proton collision rate coefficient for transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 2:
Proton collision rate coefficients for the transitions
|
Open with DEXTER | |
In the text |
![]() |
Figure 3:
Proton collision rate coefficients for transitions
in P-like Fe XII: thick solid, dashed and dot lines - formula (3),
|
Open with DEXTER | |
In the text |
![]() |
Figure 4:
Proton collision rate coefficients for transitions in
P-like Fe XII: solid, dashed and doted lines - Eq. (3),
|
Open with DEXTER | |
In the text |
![]() |
Figure 5:
Proton collision rate coefficients for transitions in
P-like Fe XII: solid, dashed and doted lines - Eq. (3),
|
Open with DEXTER | |
In the text |
![]() |
Figure 6:
Proton excitation cross sections for transitions in
Si-like Fe XIII: squares - quantum results of Faucher (1977),
solid line - semi-classical results of Landman (1975),
dotted line - semi-classical results of Masnou-Seeuws & McCarroll (1972);
for (1) the
|
Open with DEXTER | |
In the text |
![]() |
Figure 7:
Proton collision rate coefficients for transitions in
Si-like Fe XIII: thick solid, thin solid, dashed and doted lines - Eq. (3),
diamonds - data of Landman (1975) for the
|
Open with DEXTER | |
In the text |
![]() |
Figure 8:
Proton collision rate coefficients for transitions in
Si-like Fe XIII: solid, dashed and doted lines - Eq. (3),
diamonds - data of Landman (1975) for the
|
Open with DEXTER | |
In the text |
![]() |
Figure 9:
Proton collision rate coefficients for transitions in
Si-like Fe XIII: solid, dashed and doted lines - Eq. (3),
diamonds - data of Landman (1975) for the
|
Open with DEXTER | |
In the text |
![]() |
Figure 10:
Proton collision rate coefficients for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 11:
Proton collision rate coefficients for the transitions in
Mg-like Fe XV: solid, dashed and doted lines - Eq. (3),
diamonds - data of Landman & Brown (1979) for the
|
Open with DEXTER | |
In the text |
![]() |
Figure 12:
Collision rate coefficient for transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 13:
Collision rate coefficient for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 14:
Proton collision cross section for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 15:
Proton collision rate coefficient for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 16:
Collision rate coefficients for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 17:
Collision rate coefficients for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 18:
Collision rate coefficient for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 19:
Collision rate coefficients for the transitions
|
Open with DEXTER | |
In the text |
![]() |
Figure 20:
Collision rate coefficients for the transitions
|
Open with DEXTER | |
In the text |
![]() |
Figure 21:
Collision rate coefficients for the transitions
|
Open with DEXTER | |
In the text |
![]() |
Figure 22:
Collision rate coefficients for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 23:
Collision rate coefficients for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 24:
Collision rate coefficients for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 25:
Collision rate coefficients for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 26:
Collision rate coefficients for the transition
|
Open with DEXTER | |
In the text |
![]() |
Figure 27:
Collision rate coefficients for the transition
|
Open with DEXTER | |
In the text |
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