Difference between revisions of "LSST Camera"

From Camera-wiki.org
Jump to: navigation, search
m (two plausible cats)
m (math, d'oh)
Line 28: Line 28:
 
The telescope's design calls for a folded light path to allow for a shorter and more maneuverable telescope structure. The primary mirror is 8.4 meters in diameter (over 27 feet), however the central 5 meters are figured to a deeper curvature to serve as the system's tertiary mirror (M3), and do not contribute to its light-gathering area. (An unobstructed 6.7m telescope would have equivalent light-gathering power.<ref name="OptDes"/>)
 
The telescope's design calls for a folded light path to allow for a shorter and more maneuverable telescope structure. The primary mirror is 8.4 meters in diameter (over 27 feet), however the central 5 meters are figured to a deeper curvature to serve as the system's tertiary mirror (M3), and do not contribute to its light-gathering area. (An unobstructed 6.7m telescope would have equivalent light-gathering power.<ref name="OptDes"/>)
  
In addition to the three-bounce mirror elements, the telescope also includes corrector lenses to provide a flat field at the sensor plane. The largest of these is 1.55 m or ~6 feet in diameter<ref name="OptDes" />.
+
In addition to the three-bounce mirror elements, the telescope also includes corrector lenses to provide a flat field at the sensor plane. The largest of these is 1.55 m or ~5 feet in diameter<ref name="OptDes" />.
  
  

Revision as of 02:42, 31 January 2015

The LSST Camera is the digital-imaging package planned for the Large Synoptic Survey Telescope under construction at Cerro Pachon in Chile.

According to its design team, this will be the largest "digital camera" ever constructed—albeit one highly specialized for astrophotography. The design as planned "will be the size of a small car and weigh more than 3 tons[1]" (excluding the optics of the telescope), with a sensor array boasting 3,200 megapixels.

It is not possible to fabricate a monolithic silicon image sensor of the required size. Current plans call for an array of roughly 200 individual 42x42 mm square CCD chips, each encompassing 16 megapixels. These are to be butted edge to edge with a minimal loss of imaging area.

To maximize sensitivity to faint light, each CCD pixel is about 10x10 µm square (about 40% more area than the pixels of the Sony a7S, perhaps today's most low-light-capable consumer model). Furthermore the sensor will be cooled to -100°C within a vacuum chamber to minimize spurious thermal noise.

There is no color filter array over the sensor. Instead the camera has a system of five 75 cm-wide filters, each of which passes a different spectral band, which can be swapped into place over the entire sensor for sequential exposures.[2]

In January, 2015 the camera design team at SLAC received “Critical Decision 2” approval from the US Department of Energy, which continues funding to develop the instrument.[1]


Telescope optics

The LSST itself is an unusual telescope, optimized for rapid, repeated wide-field imaging of the entire sky in order to capture transient phenomena. It essentially represents a massive f/1.2 telephoto lens with an effective focal length of 10,310 mm.[3]

The telescope's design calls for a folded light path to allow for a shorter and more maneuverable telescope structure. The primary mirror is 8.4 meters in diameter (over 27 feet), however the central 5 meters are figured to a deeper curvature to serve as the system's tertiary mirror (M3), and do not contribute to its light-gathering area. (An unobstructed 6.7m telescope would have equivalent light-gathering power.[2])

In addition to the three-bounce mirror elements, the telescope also includes corrector lenses to provide a flat field at the sensor plane. The largest of these is 1.55 m or ~5 feet in diameter[2].




Notes

  1. 1.0 1.1 "World’s Most Powerful Camera Receives Funding Approval" from SLAC National Accelerator Laboratory of Stanford University
  2. 2.0 2.1 2.2 "Optical Design" from lsst.org
  3. " The effective focal length of the optical system is 10.31-m making the final f-number 1.2345," according to an LSST presentation poster.


Links