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On the sun's absolute disk-center and mean disk intensities, its limb darkening, and its `limb temperature' (λλ330 to 1099 nm)

机译:在太阳的绝对圆盘中心和平均圆盘强度下,其四肢变黑,并且其“肢体温度”(λλ330至1099 nm)

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摘要

The coefficients A 0 of the limb-darkening functions I(μ)/I center=P 5(μ)=ΣA iμi (i=0,...5, μ=cos θ), published by Neckel and Labs (1994), and the corresponding disk-center intensities I center=I(μ=1), which were taken from the absolutely calibrated Kitt Peak FTS Atlas of the disk center (Brault et al., see Neckel and Labs, 1984, and Neckel 1999), are used to derive `limb intensities' I limb=I(μ=0)=A 0 I center. The corresponding `limb temperatures' T limb vary only slightly with wavelength; the mean value (≃4750 K) and the wavelength of maximum intensity (≃605 nm) conform to Wien's law (λmax T=0.288 cm K). Further, T limb agrees closely with that temperature, which follows from Avrett's (2000) model of the photosphere for τ500≃0.006; for this layer the optical thickness along the line of sight is close to 1 (`the limb'; compare Unsöld, 1968). The slight variation of T limb with wavelength is presumably due to systematic errors in the Neckel and Labs intensity data: it corresponds almost precisely to the differences between their data and the more recent ones provided by, e.g., Burlov-Vasiljev, Gurtovenko, and Matvejev (1995), and Burlov-Vasiljev, Matvejev, and Vasiljeva (1998). Two simple correction functions (for λ≦550 nm and λ≧550 nm) are proposed, which apply to all Neckel and Labs intensity data (disk center and full disk, line spectrum and (quasi) continuum), and to the absolutely calibrated Kitt-Peak FTS Atlas (spectra of disk center and full disk) as well.
机译:肢体变暗函数I(μ)/ I center = P 5 (μ)=ΣAi μi的系数A 0 (i = 0,... 5,μ= cosθ)(由Neckel和Labs(1994)出版)以及相应的磁盘中心强度I center = I(μ= 1),它们是从绝对校准后获得的磁盘中心的Kitt Peak FTS Atlas(Brault等人,请参阅Neckel和Labs,1984和Neckel 1999)用于得出“肢体强度” I肢 = I(μ= 0)= A 0 我居中。相应的“肢体温度” T肢仅随波长而略有变化;平均值(≃4750K)和最大强度波长(≃605nm)符合维恩定律(λmax T = 0.288 cm K)。此外,T limb 与该温度非常吻合,该温度遵循Avrett(2000)的光球模型,其τ500≃0.006;对于这一层,沿视线的光学厚度接近1(“肢体”;比较Unsöld,1968年)。 T limb 随波长的轻微变化可能是由于Neckel和Labs强度数据中的系统误差所致:它几乎精确地对应于其数据与Burlov-Vasiljev等提供的最新数据之间的差异, Gurtovenko和Matvejev(1995),以及Burlov-Vasiljev,Matvejev和Vasiljeva(1998)。提出了两个简单的校正函数(针对λ≦550 nm和λ≧550 nm),它们适用于所有Neckel和Labs强度数据(磁盘中心和全磁盘,线谱和(准)连续体),以及绝对校准的Kitt -峰值FTS Atlas(磁盘中心和完整磁盘的频谱)。

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  • 来源
    《Solar Physics》 |2003年第2期|239-250|共12页
  • 作者

    Heinz Neckel;

  • 作者单位

    Hamburger Sternwarte;

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  • 原文格式 PDF
  • 正文语种 eng
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  • 入库时间 2022-08-18 00:03:38

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