A three-CCD (3CCD) camera is a camera whose imaging system uses three separate charge-coupled devices (CCDs), each one receiving filtered red, green, or blue color ranges. Light coming in from the lens is split by a complex prism into three beams, which are then filtered to produce colored light in three color ranges or "bands". The system is employed by high quality still cameras, telecine systems, professional video cameras and some prosumer video cameras.
Compared to cameras with only one CCD, three-CCD cameras generally provide superior image quality by using full-frame dichroic filters to better separate the red, green and blue color bands, and better low-light performance. By separating red, green, and blue color ranges with a 1:1 pixel ratio (known as "4:4:4"), three-CCD cameras achieve much better precision than single-CCD cameras.
In contrast, almost all single-CCD cameras use a Bayer filter, using less accurate dye filters in front of each pixel to separate the colors. Because each pixel on a single CCD sensor is covered with its own tiny color filter, a frame is necessary to keep the dye filters from leaking into adjacent pixels. The result is less light absorbed compared to a CCD without a Bayer filter. Typically there is a 2:1 ratio of green and red/blue pixels, producing less color detail.
Three-CCD cameras are more expensive than single-CCD cameras because they use three sensors rather than one, and because they use a beam splitter to drive each of the three CCD chips. Additionally most 3CCD cameras use higher quality but more expensive dichroic filters to separate the color bands.
The practice of cameras using three separate colors for color reproduction dates back to the advent of color photography, when three glass plates covered with photographic emulsion were used beginning in the late nineteenth century.
Now that (C)MOS (MOS = "metal oxide semiconductor") sensors are sufficiently advanced to compete with CCD technology, the catch-all term "three-chip" has arisen to cover all cameras that use beam splitters and three sensors for color reproduction. Previously, CCD sensors were superior to MOS in areas like image noise and sensitivity, and the ability to operate with global shutter.
Prior to CCD technology, color cameras used vacuum tube sensors for both color and monochrome. Because of mechanical tolerances and electrical changes as electronic components aged, 3-tube cameras had to be adjusted for image registration before each use. Each pixel in a CCD imager is fixed, so each of the three CCD elements on a 3CCD camera are registered in the factory, and permanently glued onto the optical block, thus eliminating any need for manual alignment (registration) by the end user.
Those with an elementary understanding of optics often wrongly assume that the prism assembly in the optical block bends light by refraction into the different colors, as a dispersive prism does. In fact the type of prism used for 3-chip cameras is used only as a beam splitter. Each of the three resulting beams still contain all visible colors, just as complex prisms in binoculars and single-lens reflex cameras also pass the entire visible spectrum. Optical filters are what separate the full spectrum into three sub-spectra (not just primary colors) for color reproduction.
The notion that a larger single sensor is as good as a 3-chip system is less-than-true due to two main factors: The first is that current Bayer filter designs use absorptive dye filters, which are inferior to dichroic filters in terms of color purity. The second is that current Bayer filter designs collect significantly less red and blue information than green, resulting in 1/4 the color resolution of 3-chip sensors. These limitations could possibly be overcome by using many tiny dichroic filters, and by designing Bayer filter matrices with equal numbers of red, green and blue pixels. However none currently exist.
- "3CCD colour advantages -AT". www.adept.net.au. Retrieved 11 April 2018.
- Cliff Wootton (2005). A Practical Guide to Video and Audio Compression: From Sprockets and Rasters to Macroblocks. Elsevier. p. 137. ISBN 978-0-240-80630-3.