15.7: References and Supplemental Reading
- Page ID
- 141709
\( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)
\( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)
\( \newcommand{\dsum}{\displaystyle\sum\limits} \)
\( \newcommand{\dint}{\displaystyle\int\limits} \)
\( \newcommand{\dlim}{\displaystyle\lim\limits} \)
\( \newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\)
( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\)
\( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)
\( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\)
\( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)
\( \newcommand{\Span}{\mathrm{span}}\)
\( \newcommand{\id}{\mathrm{id}}\)
\( \newcommand{\Span}{\mathrm{span}}\)
\( \newcommand{\kernel}{\mathrm{null}\,}\)
\( \newcommand{\range}{\mathrm{range}\,}\)
\( \newcommand{\RealPart}{\mathrm{Re}}\)
\( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)
\( \newcommand{\Argument}{\mathrm{Arg}}\)
\( \newcommand{\norm}[1]{\| #1 \|}\)
\( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)
\( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\AA}{\unicode[.8,0]{x212B}}\)
\( \newcommand{\vectorA}[1]{\vec{#1}} % arrow\)
\( \newcommand{\vectorAt}[1]{\vec{\text{#1}}} % arrow\)
\( \newcommand{\vectorB}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)
\( \newcommand{\vectorC}[1]{\textbf{#1}} \)
\( \newcommand{\vectorD}[1]{\overrightarrow{#1}} \)
\( \newcommand{\vectorDt}[1]{\overrightarrow{\text{#1}}} \)
\( \newcommand{\vectE}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{\mathbf {#1}}}} \)
\( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)
\(\newcommand{\longvect}{\overrightarrow}\)
\( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)
\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)- Woolley, R.v.d.R., and Stibbs, D.W.N. The Outer Layers of a Star, Oxford University Press, London, 1953, p. 152.
- Böhm, K.-H. "Basic Theory of Line Formation", Stellar Atmospheres, (Ed.: J. Greenstein), Stars and Stellar Systems: Compendium of Astronomy and Astrophysics, Vol.6, University of Chicago Press, 1960, pp. 88 - 155.
- Mihalas, D. Stellar Atmospheres, W.H. Freeman, San Francisco, 1970, pp. 337 - 378.
- Mihalas, D. Stellar Atmospheres, 2d ed., W.H. Freeman, San Francisco, 1978, pp. 138.
- Henyey, L. Near Thermodynamic Radiative Equilibrium, Ap.J. 103, 1946, pp. 332 - 350.
- Hummer, D.G. Non-Coherent Scattering, Mon. Not. R. astr. Soc. 125, 1962, pp. 21 - 37.
- Omont, A., Smith, E.R., and Cooper, J. Redistribution of Resonance Radiation I. The Effect of Collisions, Ap.J. 175, 1972, pp. 185 - 199.
- McKenna,S. A Reinvestigation of Redistribution Functions RIII and RIV, Ap. J. 175, 1980, pp. 283 - 293.
- McKenna, S. The Transfer of Polarized Radiation in Spectral Lines:Formalism and Solutions in Simple Cases, Astrophy. & Sp. Sci., 108, 1985, pp. 31 - 66.
- Hummer, D.G., and Mihalas, D. Line Formation with Non-Coherent Electron Scattering in O and B Stars, Ap.J. Lett. 150, 1967, pp. 57 - 59.
- McKenna, S. A Method of Computing the Complex Probability Functionand Other Related Functions over the Whole Complex Plane, Astrophy. & Sp. Sci. 107, 1984, pp. 71 - 83.
- McKenna, S. The Transfer of Polarized Radiation in Spectral Lines: Solar-Type Stellar Atmospheres, Astrophy. & Sp. Sci., 106, 1984, pp. 283 - 297.
- Chandrasekhar,S. The Radiative Equilibrium of the Outer Layers of a Star with Special Reference to the Blanketing Effect of the Reversing Layer, Mon. Not. R. astr. Soc. 96, 1936, pp. 21 - 42.
- Sneden, C., Johnson, H.R., and Krupp, B.M. A Statistical Method for Treating Molecular Line Opacities, Ap. J. 204, 1976, pp. 281 - 289.
- Carpenter,K.G. A Study of Magnetic, Line-Blanketed Model Atmospheres, doctoral dissertation: The Ohio State University, Columbus, 1983.
- Kurucz, R., and Peytremann, E. A Table of Semiemperical gf Values Part 3, SAO Special Report #362, 1975.
Although they have been cited frequently, the serious student of departures from LTE should read both these:
Mihalas, D.: Stellar Atmospheres, W.H.Freeman, San Francisco, 1970, chaps. 7-10, 12, 13.
and
Mihalas, D.: Stellar Atmospheres, 2d ed., W.H.Freeman, San Francisco, 1978, chaps. 11-13.
A somewhat different perspective on the two-level and multilevel atom can be found in:
Jefferies, J.T.: Spectral Line Formation, Blaisdell, New York, 1968, chaps. 7, 8.
Although the reference is somewhat old, the physical content is such that I would still recommend reading the entire chapter:
Böhm, K.-H.: "Basic Theory of Line Formation", Stellar Atmospheres, (Ed.: J.Greenstein), Stars and Stellar Systems: Compendium of Astronomy and Astrophysics, Vol.6, University of Chicago Press, Chicago, 1960, chap. 3.


