Telescopes and Instruments
Explore below to learn more about the SDSS telescopes, the SDSS spectrographs, and the SDSS imager.
The Sloan Foundation 2.5m Telescope at Apache Point Observatory
The SDSS uses a dedicated 2.5-m f/5 modified Ritchey-Chrétien altitude-azimuth telescope located at Apache Point Observatory, in south east New Mexico (Latitude 32° 46′ 49.30″ N, Longitude 105° 49′ 13.50″ W, Elevation 2788m). A 1.08 m secondary mirror and two corrector lenses result in a 3° distortion-free field of view. The telescope is described in detail in a paper by Gunn et al. (2006).
The Irénée du Pont Telescope at Las Campanas Observatory
The new fourth phase of the SDSS will include observations from the Southern Hemisphere for the first time. The southern observations will be taken from the Irénée du Pont Telescope at Las Campanas Observatory in northern Chile (Latitude 29° 0′ 52.56″ S, Longitude 70° 41′ 33.36″ W, Elevation 2380m). The du Pont telescope is a Ritchey-Chrétien 2.5-m f/7.5 telescope with a Gascoigne corrector lens. The telescope is described in detail in a paper by Bowen & Vaughan (1973).
eBOSS / BOSS
The eBOSS spectroscopic survey will continue to use the spectrographs built for BOSS. These two identical spectrographs are rebuilt from the original SDSS spectrographs, which were used for the SDSS Legacy and SEGUE surveys. Each spectrograph has two cameras, one red and one blue, with a dichroic splitting the light at roughly 6000 Å and a full wavelength range from 3600 to 10,400 Å. Additional Information can be found on the BOSS spectrograph page.
APOGEE-2 / APOGEE
The APOGEE-2 survey will continue to use the high-resolution near-infrared spectrograph used for the APOGEE survey. The APOGEE spectrograph is a custom-built multi-object spectrograph which records the spectrum of 300 targets simultaneously across 1.51 to 1.70 micron within the H-band with a nominal resolution of 22,500. Additional Information can be found on the APOGEE spectrograph page.
MaNGA is a galaxy survey which aims to make detailed integral field unit (IFU) resolved spectroscopy measurements of 10,000 nearby galaxies. MaNGA uses the eBOSS / BOSS spectrograph, but instead of placing a single fiber on each galaxy, it uses specially-designed hexagonal ferrules to close-pack the circular fibers into hexagonal bundles. Each MaNGA cartridge contains 17 bundles ranging in size from 19 to 127 fibers, each enabling detailed observations of 17 galaxies simultaneously. Additional Information can be found on the Instrumentation section of the MaNGA surveys page.
MARVELS used a specially-built interferometric spectrograph to obtain high-precision radial velocity measurements of stars looking for exoplanet candidates. In contrast to the more traditional high-resolution echelle spectrographs, MARVELS used a new approach to measuring radial velocities. The spectrograph is a fiber-fed dispersed fixed-delay interferometer (DFDI), a combination of Michelson interferometer and a medium resolution (R~6,000-10,000) spectrograph, which overlays interferometer fringes on a long-slit stellar spectrum. Additional Information can be found on the MARVELS spectrograph page.
The SDSS’s imaging camera is now at the Smithsonian, but all the images it collected are available online. The imaging camera collected photometric imaging data using an array of 30 SITe/Tektronix 2048 by 2048 pixel CCDs arranged in six columns of five CCDs each, aligned with the pixel columns of the CCDs themselves. SDSS r, i, u, z, and g filters cover the respective rows of the array, in that order. The survey operated the instrument in a drift scan mode: the camera slowly reads the CCDs while the telescope moves along great circles on the sky so that images of objects move along the columns of the CCDs at the same rate the CCDs are being read. As an image of an object moves along the column of the CCDs, a CCD in each row collects data on that object. Therefore, the camera produces five images of a given object, all from the same column of CCDs, one from each CCD in that column. It takes an object 54 seconds to move from the beginning of a CCD to the end, so the effective exposure time in each filter is 54 seconds. Because there is some space between the rows of CCDs, it takes an image 71.7 seconds to move from the beginning of one row to the next. Each row corresponds to a different filter, so each object has one image in each filter, taken at 71.7 second intervals. A detailed description of the imager can be found in Gunn et al. (1998) and in the SDSS-I project book. Additional Information can be found on the Camera page.
A time-lapse video of one night of operations at the SDSS telescope
During the night, an observer changes the cartridge to observe a new set of stars or galaxies roughly every hour. Each cartridge contains hundreds of fiber-optic cables plugged into holes in a large aluminum plate. Each fiber observes a single star or galaxy.
The “bright time” observing is during full moon, the “dark time” is before moonrise, with the moon (not the sun!) rising shortly before the end of the video. Credit: John Parejko (Yale University) and the SDSS collaboration.