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Philip G. Steen

Publications and source records attributed to Philip G. Steen.

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High-Precision Photometry with a scientific CMOS Camera: II On-Sky Testing of the Marana camera at the NGTS facility

Modern scientific CMOS cameras offer very fast readout speeds and low read noise. In this study, we evaluate the performance of the Andor Marana CMOS camera through on-sky testing carried out at the NGTS facility at the ESO Paranal Observatory in Chile. We mount the Marana camera to an NGTS telescope, and conduct photometric observations of bright stars. In particular, we target transit events around eight known bright exoplanet host stars. Simultaneous observations are carried out using an existing Andor iKon-L CCD camera on a neighbouring NGTS telescope. This allows for a direct comparison of the photometric precision between the CMOS and CCD cameras. We find that the Marana CMOS exhibits a similar level of photometric performance to the CCD camera, achieving 500\,ppm at a 30-minute timescale for a T $=10$\,mag star. Although the CCD has a slightly better quantum efficiency over the NGTS filter range (520-890\,nm), we find that the faster readout speed of the CMOS compared to the CCD means that the CMOS camera detects 20\,\% more photons per unit time for a solar-type star in our standard 10\,s exposure time operation mode. This results in the CMOS performing slightly better photometry in the photon-limited regime. We conclude that modern CMOS cameras, such as the Marana, are very well-suited for astronomical time-series photometry applications.

astro-ph.IM

High-Precision Photometry with a scientific CMOS Camera: I Lab Testing of the Marana camera

Scientific CMOS cameras are becoming increasingly prevalent in modern observational astronomy. We assess the ability of CMOS image sensors technology to perform high-precision photometry with a detailed laboratory characterization of the Marana 4.2BV-11 CMOS camera. We characterise the camera in the Fastest Frame Rate (FFR) and High Dynamic Range (HDR) modes. Our evaluation includes read noise, dark current, photo response and dark signal non-uniformities, quantum efficiency and window transmittance. The read noise is found to be 1.577\,e$^-$ for the FFR mode. For the HDR mode the read noise floor is measured to be 1.571\,e$^-$ for signal levels below approximately 1800\,e$^-$. The bias level shows dark signal non-uniformities with values of 0.318\,e$^-$ and 0.232\,e$^-$ for FFR and HDR mode, respectively. Pixel well capacity reached 2366 e$^-$pix$^{-1}$ for the FFR mode and 69026 e$^-$pix$^{-1}$ with a dynamic range of 93\,dB for the HDR mode. The camera demonstrates good linearity, yielding linearity errors of 0.099\,\% for FFR mode and 0.122\,\% for HDR mode. The uniformity across the image arrays show a photo response non-uniformity of 0.294\,\% for the FFR mode and 0.131\,\% for the HDR mode. The dark current displays a noticeable glow pattern, resulting in mean dark current levels of $1.674\pm0.011$\, \eps\, for the FFR mode and $1.617\pm0.008$\,\eps\, for the HDR mode at a constant temperature of -25\,$^\circ$C. We measured the quantum efficiency across the visible spectrum, with a peak of of >95\,\% at 560\,nm. Our tests indicate that the Marana CMOS camera is potentially capable of performing precise photometry.

astro-ph.IM