The invention relates to a method and also a device for the color correction of digital image data. In particular, the invention relates to a method and a device for the color correction of digital image data generated by spectral absorption of white light in color filters of a color film.
What is of crucial importance to the viewer of a film or television production, besides picture sharpness, is the subjective color impression. Therefore, in the course of producing the productions, it is endeavored to ensure that the colors, when reproduced at the cinema and/or on a television screen, as far as possible appear in the way that the director intended. This aim, inter alia, is striven for with the postprocessing of film or image material. A prerequisite for an efficient postprocessing is that, by way of example, the color representation on the monitors of a colorist corresponds as exactly as possible to the image projected in a cinema, for example. Nowadays, the starting point for postprocessing is generally digitized image data generated by film scanners or electronic cameras. Added to these are computer-generated images which are present as digital image data from the outset.
Devices which strive for such correspondence between color representations with different representation means are already commercially available as software and hardware solutions. These devices are based on the considerations described below.
Colors arise in different ways on different reproduction media. From the earliest times it has been known from painting that from just three different pigments, namely yellow, blue-green and purple-red, all intermediate hues can be produced by mixing the primary colors mentioned. Primary colors are understood to be those colors which cannot be mixed from other colors but from which all other colors can be mixed. In chromatics nowadays this type of color mixing is referred to as subtractive color mixing. The term subtractive color mixing is derived from the fact that a pigment layer absorbs certain spectral components of incident white light and reflects others, as a result of which the color impression arises for the viewer. Other types of color mixing were initially not known.
It was not until a long time later that Isaac Newton recognized that the spectral colors of the light, the so-called color stimuli, can also be mixed. With this type of color mixing the jargon uses the term additive mixing in contrast to subtractive color mixing explained above in the case of pigments. Additive color mixing is governed by relatively simple rules, known as Grassmann's laws, which also apply to self-luminous screens, such as, for example monitors based on cathode ray tubes.
A special case of subtractive color mixing is the combination or superposition of optical filters. The transmission of the filter combination is equal to the product of the respective transmissions of the individual filters, which is why the jargon also uses the term multiplicative color mixing in this case. This last-mentioned type of color mixing is also critical for color reproduction in the projection of color films which have three different color layers lying one above the other.
One important difference between additive and multiplicative color mixing is that Grassmann's laws cannot be applied to multiplicative color mixing. The reason for this is to be found in the fact that, by way of example, as the thickness of a cyan filter increases, there is a decrease not only in the transmission in the red spectral range but also to a considerable extent in the green spectral range. This fact and the resulting consequences are explained in detail further below. In known color correction systems, therefore, the absorption of test patterns (“test patches”) is measured with the aid of densitometers and the absorption in the secondary densities is corrected by a transformation of the color coordinates.
It has been shown in practice, however, that despite these measures, the correspondence of colors is not always achieved during reproduction with different representation means.
For this reason, there continues to be a need for a device and a method for color correction which, in comparison with the prior art, achieve an improved correspondence between the colors during reproduction with different representation means.
The method according to the invention serves for the color correction of digital image data generated by spectral absorption of white light in color filters of a first representation means. Firstly, the primary color values of the image data are detected, the primary color values being related to the first representation means. The primary color values are then corrected in order to generate secondary color values, which are related to a second representation means and which take account of the absorption of light in secondary densities of the color filters. According to the invention, a plurality of absorption spectra are generated for different densities of at least one color filter. Building on this, the spectral profile of the absorption spectra of the color filters influences the correction of the primary color values for generating the secondary color values.
One advantage of the method is that this achieves a better correspondence of the color reproduction between the first and second representation means.
In a development of the invention, intermediate spectra are calculated from the plurality of absorption spectra for different densities of the color filter. In this case, it may be expedient if a plurality of absorption spectra are generated for all the color filters.
In this case, intermediate spectra may be calculated for all the color filters. As a result, more data are available for the correction of the color values, which may, in principle, have a favorable effect on the correspondence of the color representations that is striven for.
Finally, provision may be made for convolving the spectra of the color filters with the spectral perception curve of a standard observer in order to generate the secondary color values. In this way, it is possible to take account of the physiological perception of colors by the human eye.
The drawing illustrates facts which serve to provide a better understanding of the invention. In the figures:
D=−log(T)
This means that at density zero, the relevant filter is completely transparent, and that the transmission decreases as the density increases. Density curves for filters with different transmissions are plotted for each of the primary colors red, green and blue. It can clearly be seen that, for the density curves for the red filter, by way of example, appreciable secondary maxima occur in the blue spectral range around 400 nm, and lead to a considerable absorption for the color impression. The same applies to a lesser extent to the density curves of the green filters. The density curves for the blue filters fall sharply in the wavelength range of between 440 nm and 380 nm in order to rise again below 380 nm. Furthermore, the density curves of the blue filters, with increasing density, exhibit a more and more highly pronounced plateau in the green spectral range around 550 nanometers, the plateau projecting right into the red spectral range. The absorption of a primary color filter in spectral ranges other than the spectral range assigned to the respective primary color is referred to as the “secondary density” of the density curve and results in color shifts during the projection of color films for example in the case of multiplicative color mixing. These effects are known in principle and are corrected for example by means of a linear transformation of the color coordinates. In order to better understand the extent to which the invention goes beyond the known methods, it is necessary firstly to discuss the conventional correction method in more detail.
Different film materials differ inter alia in the absorption properties of the colorants, which makes it necessary to adjust the color correction device 12 shown in
It has been shown in practice, however, that the correspondence between the color representation on the monitor 13 and the projection screen 18 that is striven for in this way still leaves something to be desired. The purpose of the invention is to improve said correspondence.
In order to realize this aim, the invention commences at determination of the correction values. From the more precise consideration of the spectral density curves of the color filters as shown in
In the case of conventional densitometer measurements, these changes are registered only as a change in the absorption in the respective measurement window. For this reason, it is not possible with densitometer measurements to determine the actual absorption at a specific wavelength. However, this is exactly what is important for as precise a correspondence as possible between the color representation on different representation means.
The invention therefore proposes measuring the test patches of the film materials using a spectrometer over the entire wavelength range and interpolating intermediate spectra from the spectra thus obtained. From the totality of the spectra, it is possible to derive, for the three primary colors, tables which put a color value that determines the representation on the colorist's monitor 13 into a relationship with a code value of the film exposer 14. A three-dimensional table is produced overall in this way.
The method according to the invention is described in greater detail below with reference to
In accordance with the flowchart in
Number | Date | Country | Kind |
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03300181.9 | Oct 2003 | EP | regional |