Envelope

A. Caruso
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Extensive results are given for the Anders-Grevesse (1989) metal abundances which allow accurate interpolation in temperature, density, hydrogen mass fraction, and metal mass fraction. The range of T and R cover typical stellar conditions from the Beat Cepheids are classical Cepheids which pulsate simultaneously in the fundamental and first overtone. The two periods can be accurately disentangled and extracted from observations. In attempting to analyze such stars, use is made of the Petersen diagram where the ratio of the first overtone to fundamental period, Pl/P0,is plotted against the fundamental period P0. One approach in modelling such stars is to use linear non-adiabatic theory, with masses and luminosities mandated by stellar evolutionary calculations, to compute the fundamental and first overtone modes. The spectra of highly charged ions of NEON, ARGON, KRYPTON and XENON with few valence electrons have been studied in the 300-2100 A range using a pulsed discharge tube. For Ne spectra we found lines up to the sixth degree of ionization, We have developed a powerful technique for compacting and assessing atomic data for electron impact excitation of positive ions. Rate coefficients for such processes are derived from thermally average collision strengths T(T) which usually vary smoothly with temperature. The present method begins by scaling T in order to produce a reduced form T r . This is then plotted as a function of the scaled temperature T r which maps the entire range of T onto the interval (0,1). Y r can be accurately fitted by a 5-point cubic spline, so economising on storage while at the same time providing a convenient means for interpolating and extrapolating data. Straightforward tabulation normally requires more data points than this to cover a limited temperature range. With increasing amounts of atomic data becoming available, the problem of storage needs careful consideration. The present method is a possible solution. It forms the basis of an interactive computer program called OMEUPS which uses graphical display and is designed to be convenient for use by astrophysicists as well of those working in atomic collision theory. Some graphic examples will be presented to illustrate the method. The precision and accuracy of modern high resolution spectroscopic observations of cosmic bodies continues to drive the need for improved laboratory data and theories of atoms and molecules. Inparticular, recent measurements of asymmetric molecular hydrogen quadrupole lines in the absorption spectrum of Uranus and observations of high / rotational transitions in the infrared emission spectrum of molecular hydrogen in the Orion nebulae point to the need for high resolution and high accuracy data. We have recently completed the measurement of pressure shifts, line strengths and shapes, broadening coefficients and line positions for the S(0) and S(l) lines of molecular hydrogen in the 4-0 vibration-rotation band. We have also detected for the first time in the laboratory the 5-0 S(l) line and confirm its detection in Uranus. With these and other high quality measurements of the overtone spectrum of molecular hydrogen in the infrared and visible, a consistent set of parameters has emerged which should be useful to astrophysicists and may challenge theorists to improve their ab-initio calculations. Approximations in Brueckner's theory of spectral broadening by collisions with neutral hydrogen atoms relevant to a solar-type atmosphere have been discussed, and a modified theory for s-p transitions has been presented. The theory utilises explicit expressions for the interatomic interaction energy between a hydrogen atom in its ground state and general m = 0, ± 1 p-states, derived from second-order perturbation theory without exchange, allowing for removal of the Lindholm-Foley average over m-states in the original Brueckner model. Approximate upper and lower bounds for the linewidth of the sodium D-lines are derived, and these values are contrasted with available theoretical, experimental and solar empirical results. The removal of the Lindholm-Foley average is shown to reduce the D-state linewidths by about 30%, and an analysis of the interatomic separations important in the line-broadening cross-section for the D-lines has shown that there is little atomic overlap at the separations that are important.","PeriodicalId":342376,"journal":{"name":"9 x 9 – A Method of Design","volume":"6 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-07-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"9","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"9 x 9 – A Method of Design","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1515/9783035610994-009","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 9

Abstract

We present radiative Rosseland mean opacity tables calculated with the OPAL code (Iglesias and Rogers 1991) which removes several approximations present in previous calculations. In particular, improvements in the atomic physics have been incorporated which yield reasonably accurate photon absorption data (accuracy comparable to single-configuration, self-consistent field calculations with relativistic corrections) and include the configuration term splitting in the LS-coupling scheme. In some cases, the latter can increase the number of spectral lines by orders of magnitude compared to previous opacity codes. OPAL also employs an equation of state method which avoids the usual ad hoc cut offs introduced in free energy minimizaton schemes. The opacity tables are given in terms of temperature and R, where R = p/T^ with p the density and T the temperature. Extensive results are given for the Anders-Grevesse (1989) metal abundances which allow accurate interpolation in temperature, density, hydrogen mass fraction, and metal mass fraction. The range of T and R cover typical stellar conditions from the Beat Cepheids are classical Cepheids which pulsate simultaneously in the fundamental and first overtone. The two periods can be accurately disentangled and extracted from observations. In attempting to analyze such stars, use is made of the Petersen diagram where the ratio of the first overtone to fundamental period, Pl/P0,is plotted against the fundamental period P0. One approach in modelling such stars is to use linear non-adiabatic theory, with masses and luminosities mandated by stellar evolutionary calculations, to compute the fundamental and first overtone modes. The spectra of highly charged ions of NEON, ARGON, KRYPTON and XENON with few valence electrons have been studied in the 300-2100 A range using a pulsed discharge tube. For Ne spectra we found lines up to the sixth degree of ionization, We have developed a powerful technique for compacting and assessing atomic data for electron impact excitation of positive ions. Rate coefficients for such processes are derived from thermally average collision strengths T(T) which usually vary smoothly with temperature. The present method begins by scaling T in order to produce a reduced form T r . This is then plotted as a function of the scaled temperature T r which maps the entire range of T onto the interval (0,1). Y r can be accurately fitted by a 5-point cubic spline, so economising on storage while at the same time providing a convenient means for interpolating and extrapolating data. Straightforward tabulation normally requires more data points than this to cover a limited temperature range. With increasing amounts of atomic data becoming available, the problem of storage needs careful consideration. The present method is a possible solution. It forms the basis of an interactive computer program called OMEUPS which uses graphical display and is designed to be convenient for use by astrophysicists as well of those working in atomic collision theory. Some graphic examples will be presented to illustrate the method. The precision and accuracy of modern high resolution spectroscopic observations of cosmic bodies continues to drive the need for improved laboratory data and theories of atoms and molecules. Inparticular, recent measurements of asymmetric molecular hydrogen quadrupole lines in the absorption spectrum of Uranus and observations of high / rotational transitions in the infrared emission spectrum of molecular hydrogen in the Orion nebulae point to the need for high resolution and high accuracy data. We have recently completed the measurement of pressure shifts, line strengths and shapes, broadening coefficients and line positions for the S(0) and S(l) lines of molecular hydrogen in the 4-0 vibration-rotation band. We have also detected for the first time in the laboratory the 5-0 S(l) line and confirm its detection in Uranus. With these and other high quality measurements of the overtone spectrum of molecular hydrogen in the infrared and visible, a consistent set of parameters has emerged which should be useful to astrophysicists and may challenge theorists to improve their ab-initio calculations. Approximations in Brueckner's theory of spectral broadening by collisions with neutral hydrogen atoms relevant to a solar-type atmosphere have been discussed, and a modified theory for s-p transitions has been presented. The theory utilises explicit expressions for the interatomic interaction energy between a hydrogen atom in its ground state and general m = 0, ± 1 p-states, derived from second-order perturbation theory without exchange, allowing for removal of the Lindholm-Foley average over m-states in the original Brueckner model. Approximate upper and lower bounds for the linewidth of the sodium D-lines are derived, and these values are contrasted with available theoretical, experimental and solar empirical results. The removal of the Lindholm-Foley average is shown to reduce the D-state linewidths by about 30%, and an analysis of the interatomic separations important in the line-broadening cross-section for the D-lines has shown that there is little atomic overlap at the separations that are important.
信封
我们提出了用OPAL代码(Iglesias and Rogers 1991)计算的辐射Rosseland平均不透明度表,它消除了以前计算中存在的几个近似值。特别是,原子物理学的改进被纳入其中,产生了相当精确的光子吸收数据(精度可与单配置相媲美,自一致的场计算与相对论修正),并在ls耦合方案中包含了配置项分裂。在某些情况下,与以前的不透明编码相比,后者可以将光谱线的数量增加几个数量级。OPAL还采用状态方程方法,避免了自由能最小化方案中通常引入的临时截止。不透明度表以温度和R表示,其中R = p/T^, p为密度,T为温度。广泛的结果给出了Anders-Grevesse(1989)金属丰度,它允许在温度、密度、氢质量分数和金属质量分数中进行精确的插值。T和R的范围涵盖了典型的造父变星的恒星条件,它们是经典的造父变星,同时在基本音和第一泛音中脉动。这两个周期可以精确地从观测中分离和提取出来。在试图分析这类恒星时,使用了彼得森图,其中第一泛音与基本周期的比值Pl/P0与基本周期P0对应。建模这类恒星的一种方法是使用线性非绝热理论,用恒星演化计算规定的质量和光度来计算基本模式和第一泛音模式。用脉冲放电管研究了氖、氩、氪和氙等价电子少的高电荷离子在300-2100 A范围内的光谱。我们已经开发了一种强大的技术来压缩和评估正离子的电子冲击激发的原子数据。这种过程的速率系数由热平均碰撞强度T(T)推导而来,它通常随温度平滑变化。目前的方法从缩放T开始,以产生一个简化形式tr。然后将其绘制为缩放温度T r的函数,该函数将整个T范围映射到区间(0,1)上。Y r可以通过5点三次样条精确拟合,因此节省了存储,同时为插值和外推数据提供了方便的手段。简单的制表通常需要比这更多的数据点来覆盖有限的温度范围。随着可用的原子数据量的增加,需要仔细考虑存储问题。目前的方法是一种可能的解决办法。它构成了一个名为OMEUPS的交互式计算机程序的基础,该程序使用图形显示,旨在方便天体物理学家以及从事原子碰撞理论研究的人使用。本文将给出一些图解的例子来说明这种方法。现代宇宙天体的高分辨率光谱观测的精确性和准确性继续推动对改进实验室数据和原子和分子理论的需求。特别是,最近对天王星吸收光谱中不对称分子氢四极线的测量和对猎户座星云中分子氢红外发射光谱中高/旋转跃迁的观测表明,需要高分辨率和高精度的数据。我们最近完成了4-0振动-旋转带中氢分子S(0)和S(l)谱线的压力位移、谱线强度和形状、拓宽系数和谱线位置的测量。我们还首次在实验室中探测到5-0 S(l)线,并确认它在天王星上被探测到。通过这些和其他高质量的红外和可见光氢分子泛音光谱的测量,一组一致的参数已经出现,这对天体物理学家来说应该是有用的,并且可能挑战理论家改进他们的从头计算。讨论了与太阳型大气有关的中性氢原子碰撞引起的光谱展宽理论中的近似,并提出了一个修正的s-p跃迁理论。该理论利用了氢原子在基态和一般m = 0,±1 p态之间的原子间相互作用能的显式表达式,推导自二阶微扰理论,没有交换,允许去除原始Brueckner模型中m态的Lindholm-Foley平均值。推导了钠d线宽度的近似上界和下界,并将这些值与现有的理论、实验和太阳经验结果进行了对比。
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