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Total Galaxy Magnitudes and Effective Radii from Petrosian Magnitudes and Radii

机译:岩石星等的总星等和有效半径

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摘要

> Petrosian magnitudes were designed to help with the difficult task of determining a galaxy's total light. Although these magnitudes (taken here as the flux within 2R_Pet, with the inverted Petrosian index 1/eta(R_Pet)=0.2) can represent most of an object's flux, they do of course miss the light outside of the Petrosian aperture. Under the assumption of similar surface brightness distributions, this missing flux is simply a constant value and therefore easily corrected for. The size of the flux deficit, however, varies monotonically with the shape of a galaxy's light-profile, i.e., its concentration. In the case of a de Vaucouleurs R^{1/4} profile, the deficit is 0.20 mag; for an R^{1/8} profile this figure rises to 0.50 mag. Here we provide a simple method for recovering total magnitudes from Petrosian magnitudes using only the galaxy concentration within the Petrosian aperture. We also show how this concentration can be used to convert Petrosian radii into effective half-light radii, enabling a robust measure of the mean effective surface brightness. Our technique is applied to the SDSS DR2 Petrosian parameters, yielding excellent agreement with the total magnitudes, effective radii, and mean effective surface brightnesses obtained from the NYU-VAGC Sersic fits by Blanton et al. (2005). Although the method described here is specifically applicable to the SDSS DR2 and DR3, it is generally applicable to all imaging data where any Petrosian index and concentration can be constructed.
机译:> Petrosian量级旨在帮助确定银河系总光的艰巨任务。尽管这些大小(此处取为2R_Pet内的通量,而反向Petrosian指数为1 / eta(R_Pet)= 0.2)可以表示大多数对象的通量,但它们的确会错过Petrosian孔径之外的光。在类似的表面亮度分布的假设下,这种漏磁通量只是一个恒定值,因此很容易校正。但是,通量不足的大小随银河系的光线轮廓形状即浓度而单调变化。在de Vaucouleurs R ^ {1/4}剖面的情况下,赤字为0.20 mag。对于R ^ {1/8}剖面,该数字上升到0.50磁。在这里,我们提供了一种简单的方法,仅使用Petrosian孔径内的星系浓度从Petrosian量级中恢复总量级。我们还展示了如何使用该浓度将Petrosian半径转换为有效的半光半径,从而能够可靠地测量平均有效表面亮度。我们的技术应用于SDSS DR2 Petrosian参数,与Blanton等从NYU-VAGC Sersic拟合获得的总幅度,有效半径和平均有效表面亮度产生了极佳的一致性。 (2005)。尽管此处描述的方法特别适用于SDSS DR2和DR3,但通常适用于可以构建任何Petrosian指数和浓度的所有成像数据。

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