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To avoid the ambiguity of the term pixel – does it constitute one component or three? I suggest that you call a sensor element a photosite.

In a “one-chip” camera, hardware or firmware performs spatial interpolation to reconstruct R, G, and B at each photosite. In a “three-chip” camera, dichroic filters are mounted on one or two glass blocks. In optical engineering, a glass block is called a prism, but it is not the prism that separates the wavelengths, it is the dichroic filters.

Kuniba, Hideyasu and Roy S. Berns,

(2009), “Spectral sensitivity optimization of color image sensors considering photon shot noise,” in Journal of Electronic Imaging 18 (2):

023002-1–023002-14.

Figure 26.3, on page 300

Figure 26.4, on page 301

Figure 26.5, on page 302

Figure 26.6, on page 303

Figure 26.7, on page 304

Figure 26.8, on page 305

Every colour video camera or digital still camera needs to sense the image through three different spectral characteristics. Digital still cameras and consumer camcorders typically have a single area array CCD sensor (“one chip”); each 2× 2 tile of the array has sensor elements covered by three different types of filter. Typically, filters appearing red, green, and blue are used; the green filter is duplicated onto two of the photosites in the 2× 2 tile. This approach loses light, and therefore sensitivity. Conventional studio video cameras separate incoming light using dichroic filters operating as beam splitters; each component has a dedicated CCD sensor (“3 CCD,” or “3 CMOS”). Such an optical system separates different wavelength bands without absorbing any light, achieving about a factor of two higher sensitivity than a mosaic sensor.

Figure 26.7 shows the set of spectral sensitivity functions implemented by the beam splitter and filter (“prism”) assembly of an actual HD camera. The functions are positive everywhere across the spectrum, so the filters are physically realizable. However, rather poor colour reproduction will result if these signals are used directly to drive a display having BT.709 primaries. Figure 26.8 shows the same set of camera analysis functions processed through a 3× 3 matrix transform. The transformed components will reproduce colour more accurately – the more closely these curves resemble the ideal BT.709 CMFs of Figure 26.5, the more accurate the camera’s colour reproduction will be.

In theory, and in practice, using a linear matrix to process the camera signals can capture all colours correctly. However, capturing all colours is seldom necessary in practice, as I will explain in the Gamut section below. Also, capturing the entire range of colours would incur a noise penalty, as I will describe in

Noise due to matrixing, on page 308.

Normalization and scaling

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The y(λ) CMF is standardized by the CIE such that its

maximum value lies at unity. For the 10 nm CIE CMFs

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commonly used in image science, the y curve integrates

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to about 10.68. The x(λ) and z(λ) CMFs are scaled such that they integrate to the same value. The CIE derived its 10 nm CMFs by interpolation from its 1 nm curves;

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Figure 26.3 CMFs for CIE XYZ primaries. To acquire all colours in a scene requires filters having

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the CIE x(λ), y(λ), and z(λ) spectral sensitivities. The functions are nonnegative, and therefore could be realized in practice. However, these functions are seldom used in actual cameras or scanners, for various engineering reasons.

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SPD of red primary

SPD of green primary

SPD of blue primary

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Figure 26.4 SPDs for CIE XYZ primaries. To directly reproduce a scene that has been analyzed using the CIE XYZ colour-matching functions requires nonphysical primaries having negative excursions, which cannot be realized in practice. Many different sets are possible. In this hypothetical example, the power in each primary is concentrated at the same three discrete wavelengths, 470, 550, and 600 nm.

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Figure 26.5 CMFs for BT.709 primaries. These analysis functions are theoretically correct to acquire RGB components for display using BT.709 primaries. The functions are not directly realizable in a camera or a scanner, due to their negative lobes; however, they can be realized by a 3× 3 matrix transformation of the CIE XYZ colour-matching functions of Figure 26.3.

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Figure 26.6 SPDs for BT.709 display primaries. This set of SPDs has chromaticity coordinates that conform to SMPTE RP 145, similar to BT.709. Many SPDs could produce the same chromaticity coordinates; this particular set is produced by a Sony Trinitron CRT display. The red primary uses rare earth phosphors that produce very narrow spectral distributions, different in character from the phosphors used for green or blue.

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RSR of red sensor

RSR of green sensor

RSR of blue sensor

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Figure 26.7 Relative spectral responses (RSRs) for a real camera. This set of spectral response functions is produced by the dichroic colour separation filters (prism) of a 2000-vintage beamsplitter CCD studio HD camera. I call these relative spectral response (RSR) functions.

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Matrixed sensitivity of green Matrixed sensitivity of red

Matrixed sensitivity of blue

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Figure 26.8 Effective response after matrixing for BT.709 primaries. These curves result from the analysis functions of Figure 26.7, opposite, being processed through a suitable 3× 3 matrix. Colours as “seen” by this camera will be accurate to the extent that these curves match the ideal CMFs for BT.709 primaries shown in Figure 26.5.

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