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Direct measurement of the intra-pixel response function of the Kepler Space Telescope's CCDs

机译:开普勒太空望远镜CCD的像素内响应功能的直接测量

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Space missions designed for high precision photometric monitoring of stars often under-sample the point-spread function, with much of the light landing within a single pixel. Missions like MOST, Kepler, BRITE. and TESS, do this to avoid uncertainties due to pixel-to-pixel response nonuniformity. This approach has worked remarkably well. However, individual pixels also exhibit response nonuniformity. Typically, pixels are most sensitive near their centers and less sensitive near the edges, with a difference in response of as much as 50%. The exact shape of this fall-off, and its dependence on the wavelength of light, is the intra-pixel response function (IPRF). A direct measurement of the IPRF can be used to improve the photometric uncertainties, leading to improved photometry and astrometry of under-sampled systems. Using the spot-scan technique, we measured the IPRF of a flight spare e2v CCD90 imaging sensor, which is used in the Kepler focal plane. Our spot scanner generates spots with a full-width at half-maximum of approx<5 microns across the range of 400 mn - 900 mn. We find that Kepler's CCD shows similar IPRF behavior to other back-illuminated devices, with a decrease in responsivity near the edges of a pixel by ~50%. The IPRF also depends on wavelength, exhibiting a large amount of diffusion at shorter wavelengths and becoming much more defined by the gate structure in the near-IR. This method can also be used to measure the IPRF of the CCDs used for TESS. which borrows much from the Kepler mission.
机译:专为对恒星进行高精度光度监测而设计的太空任务经常对点扩展功能进行采样不足,大部分光都在单个像素内。像MOST,Kepler和BRITE这样的任务。和TESS,这样做是为了避免由于像素间响应不均匀而造成的不确定性。这种方法非常有效。但是,各个像素也表现出响应不均匀性。通常,像素在其中心附近最敏感,而在边缘附近则不那么敏感,响应差异高达50%。这种衰减的确切形状及其对光波长的依赖性是像素内响应函数(IPRF)。 IPRF的直接测量可用于改善光度不确定性,从而改善欠采样系统的光度和天体测量。使用点扫描技术,我们测量了开普勒焦平面中使用的备用e2v CCD90成像传感器的IPRF。我们的点扫描仪可在4亿至9亿个范围内产生最大半宽度约为<5微米的点。我们发现开普勒的CCD显示出与其他背照式设备类似的IPRF行为,像素边缘附近的响应度降低了约50%。 IPRF还取决于波长,在较短的波长下会显示出大量的扩散,并由近红外中的栅极结构所定义。该方法还可用于测量用于TESS的CCD的IPRF。这是从开普勒任务中借来的。

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