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Lines as Continuous OpacityPowerPoint Presentation

Lines as Continuous Opacity

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### Lines as Continuous Opacity

Collaborators: D. J. Bord (Umich, Dearborn)

Glenn Wahlgren, (Lund)

Thanks to many others for advice.

1. Computational practicalities: ODF, OS, “individualized abundances.

2. Unclassified lines and their relation to photoionization “resonances.”

3. Relation to standard continuous opacity sources.

Relative importance of weak and strong lines.

4. Harmonic vs. straight means.

General Remark: There are no universal answers.

All questions depend on parameter space--

a. What is the wavelength interval?

b. What are the abundances?

c. What are the physical conditions (T, P, xt)?

d. How will integration through an atmosphere affect

answers to the above questions?

1. Computational Practicalities

Current procedure is an in vitro approach, the physical

conditions are fixed. Some modification for production

is surely in order (cf. Piskunov&Kupka ApJ, 547 (2001)

Calculations based primarily on Kurucz CDRoms 20, 21,

22. Therefore Ca-Ni. Some REE III to be noted later.

Pull off all lines of first through third spectra within

20A intervals at selected wavelengths. Reformat

data; use very nearly input to standard Michigan

synthesis codes.

Line lists are typically 20-40,000 lines.

Read into code that contains abundances, ionization potentials,

partition functions, so that for each line, the relevant number

density (cm-3) can be calculated.

Arrange filter so that in addition to using all lines, one may

exclude:

a. classified lines (levels found in laboratory).

b. unclassified lines

c. lines with upper levels below first ionization limit

(take only lines subject to autoionization)

Calculate the line opacity as if it were a synthesis. Main potentials,

difference in this and synthesis code is there is only one

set of physical conditions—no integration through atmosphere.

Arbitrary abundances are possible.

Get ODF’s. We use 1024 points at 0.02A spacings. Divide

into 8 bins of 128 points.

ODF’s are much like histograms, except that one first does

an intensity sort before binning.

The straight mean of the opacity for the 1024 points is by

definition the same as the straight mean of the opacity in

the 8 bins.

From the point of view of radiative transfer, the harmonic potentials,

mean is the more physical quantity, since the radiation

will escape through the transparent windows.

The harmonic mean for the 1024 points is not the same

as the harmonic mean of the 8 bins.

The harmonic mean of the bins is typically some five

per cent larger than the harmonic mean of the 1024

points.

2. Unclassified Lines and Relation to potentials,

Photoionization Resonances (TopBase).

Transitions to levels subject to autoionization will in

principle have counterparts in photoionization cross sections.

In practice, this is only approximately true because of

incompleteness in both sets of calculations.

At the moment, Kurucz has more realistic sets of

states than TopBase, but no specific treatment of

interaction with continuum states.

If one calculates ODF’s including lines subject to autoionization and later includes TopBase continuous opacities, some transitions

are going to be counted twice! This may be only a difficulty in principle, as the opacity from the transitions in question is typically a small fraction of the total.

T=6000, Log(Pg) = 5.0, Solar Abundances autoionization

Line Opacity: All CDRom 20, 21, 22

Lines: straight

Tot Continuous

Lines: harmonic

Contributions from individual metals all below here

What is the relative importance of weak and strong lines? autoionization

T = 6000K, Log(Pg) = 5.0, Solar Abundances 3800A

All 27627 lines

702 Classified Lines

Straight mean 1.94 E-06 1.92 E-06

Harmonic mean 1.94 E-08 1.07 E-08

Virtually all of the line opacity comes from the strong lines,

but the weaker lines are significant for the transparency

(Rosseland or harmonic mean).

Standard opacity sources:

(Mostly H-minus)

7.1E-08

4.6E-11

1.9E-10

Fe I (Atlas7)

MgI (Atlas7)

How is it for SMR Star? Again, T = 6000K, Log(Pg) = 5 autoionization

This time Z = 10 – 28 10 x Solar

Solar:

Using all 27627 lines

Straight mean of lines: 3.45E-5

Harmonic mean: 3.65E-7

Harmonic of 8 bins 3.84E-7

Total Continuous: 2.71E-7

1.94E-6

1.94E-8

2.04E-8

7.10E-8

Now, using 10 x Solar, but only unclassified lines (26925)

Straight mean of lines: 9.17E-7

Harmonic mean: 1.57E-7

Harmonic of 8 bins 1.62E-7

Note that the unclassified lines make a significant autoionization

contribution relative to the standard continuous opacity

sources.

-----------------------------------------------------------

Among the unclassified lines, some will be strong, and

recognized as lines in the stellar spectrum, but will not

be synthesized.

These lines will not be a part of the quasi-continuum, the

weak-line haze that cannot be distinguished from continuous

absorption.

Some fraction of the unclassified lines should be added

to the continuous absorption.

We don’t yet know what fraction of the line opacity autoionization

to add to the continuous opacity when doing spectral

synthesis.

In solar work, we have augmented standard opacity

sources until the calculated specific intensity matches

that observed.

In the UV, say 3600A, that can mean multiplying the

known continuous opacity by 1.6 or so!

If we don’t match the observed intensity, we aren’t

doing a calculation for the real sun!!

Next: We do a numerical experiment designed to see autoionization

the effect of line opacity on a cool Ap or CP star.

In particular, we are interested in knowing what the

effects of lines from the third spectra of the REE might

contribute.

We have calculated lines of Nd III and Sm III, and included

a few additional lines from the DREAM site.

What we found is that even with the REE overabundant

by a factor of 1000, the lines from the third spectra do

not seriously compete with standard opacity sources or

lines from the iron group.

T = 8000K Log(Pg) = 4.0, 3600A autoionization

10 x Z=22-28

1000 x Z> 57

Solar

10 x Z=22-28

5.71E-08

1.05E-09

1.10E-09

Straight Mean

Harmonic

Harmonic bins

5.70E-07

1.00E-08

1.05E-08

5.74E-07

1.06E-08

1.12E-08

Standard continuous opacity: 1.78E-07

Mostly b-f of neutral hydrogen

Finally, let’s look at an iron-peak poor case: autoionization

T = 8000 Log(Pg) = 4.0

Iron Group x 0.1, Lanthanides x 1000

Straight mean: 1.06 E-08

Harmonic mean: 1.80 E-10

Harmonic bins: 1.90 E-10

Standard Cont: 1.78 E-07

Conclusions: It does not seem likely that line opacity

from the third spectra of the REE competes significantly

with standard continuous opacity sources for most

Ap-Cp abundances.

Epilog: Opacity Sampling (OS) autoionization

For our 1024-point regions, we have not had much success

with opacity sampling. Perhaps it is just our limited

experience.

Random sampling 256 points can give a result in error by

a factor of two. Table gives ratio of sample to average of

all 1024 points. Since sample is random, 1024 points do

not give exact result.

Sample/No points Mrich Solar84

- 2.14 0.256
- 0.666 2.22
- 1.11 1.25
- 1024 1.20 0.965

Thank You Thank You Thank You autoionization

The End

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