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Reprocessing in Luminous Disks

机译:在发光磁盘中进行重新处理

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We develop and investigate a procedure that accounts for disk reprocessing of photons that originate in the disk itself. Surface temperatures and simple, blackbody spectral energy distributions (SEDs) of protostellar disks are calculated. In disks that flare with radius, reprocessing of stellar photons results in temperature profiles that are not power-law at all radii but are consistently shallower than r-3/4. Including the disk as a radiation source (as in the case of active accretion) along with the stellar source further flattens the temperature profile. Disks that flare strongly near the star and then smoothly curve over and become shadowed at some distance ("decreasing curvature" disks) exhibit nearly power-law temperature profiles that result in power-law infrared SEDs with slopes in agreement with typical observations of young stellar objects. Disk models in which the photospheric thickness is controlled by the local opacity and in which the temperature decreases with radius naturally have this shape. Uniformly flaring models do not match observations as well; progressively stronger reprocessing at larger radii leads to SEDs that flatten toward the infrared or even have a second peak at the wavelength corresponding (through the Wien law) to the temperature of the outer edge of the disk. In FU Orionis outbursting systems, the dominant source of energy is the inner disk. Reprocessing throughout the disk depends sensitively on the inner disk shape and emitted temperature profile. We show that the thermal instability outburst models of Bell & Lin reproduce trends in the observed SEDs of FU Ori systems with T ∝ r-3/4 in the inner disk (r 0.25 AU corresponding to λ 10 μm) and T ∝ r-1/2 in the outer disk. Surface irradiation during outburst and quiescence is compared in the region of planet formation (1-10 AU). The contrast between the two phases is diminished by the importance of the reprocessing of photons from the relatively high mass flux, outer disk ( = 10-5 M☉ yr-1), which is present during both outburst and quiescence.
机译:我们开发并研究了一种程序,该程序负责对源自磁盘本身的光子进行磁盘再处理。计算了原恒星盘的表面温度和简单的黑体光谱能量分布(SED)。在具有半径耀斑的圆盘中,对恒星光子的后处理会导致温度曲线在所有半径上都不是幂律,而是始终比r-3 / 4浅。包括磁盘作为辐射源(在主动积聚的情况下)以及恒星源一起,进一步使温度分布曲线变得平坦。在恒星附近强烈耀斑,然后平滑弯曲并在一定距离处被遮盖的圆盘(“曲率减小”的圆盘)显示出近乎幂律的温度分布,这导致幂律红外SED的斜率与年轻恒星的典型观测结果一致对象。圆盘模型具有这种形状,其中光球厚度由局部不透明度控制,并且温度随半径降低而降低。均匀张开的模型也与观测值不匹配;在较大半径处逐渐增强的后处理会导致SED向红外方向展平,或者甚至在(通过维恩定律)与磁盘外边缘温度相对应的波长处具有第二个峰值。在FU Orionis爆发系统中,能量的主要来源是内盘。整个磁盘的后处理敏感地取决于内部磁盘的形状和发出的温度曲线。我们显示,Bell&Lin的热不稳定性爆发模型再现了观测到的FU Ori系统SED的趋势,内圆盘中的T ∝ r-3 / 4(r 0.25 AU对应于λ10μm)和T ∝ r-1 / 2在外盘中。比较了行星形成区域(1-10 AU)爆发和静止期间的表面辐射。相对高的质量通量外盘(= 10-5M☉yr-1)对光子进行后处理的重要性降低了这两个阶段之间的对比,该通量在爆发和静止过程中都存在。

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