Am 21.01.2015 um 06:42 schrieb Dale:
>
> okay, LMS is still the response of the cones and photopic vision?
LMS is not XYZ. LMS space is defined by the sensitivity curves of the
cones. Rod vision is (for this purpose) irrelevant.
> XYZ is "thought" up to be a tri-stimulus space similiar to LMS
> with Y being as close to luminousity as possible, and X,Z carrying
> the color load?
No, once again, XYZ space is not LMS space. The X, Y and Z curves are
"somewhat" arbitrary and not (directly) related to the cone response
curves. Y is lumiance (approximately), X and Z add color information,
but XYZ is not an opponent colorspace (like YCbCr)
> Xbar,ybar,zbar are the color matching functions used with spectral
> power distributions of colors, in color matching experiments, to
> get XYZ, and ybar is defined as V the luminousity efficency function
> which is close to M in LMS?
Well, not really. Y is "observed luminance", and to that, all cones
contribute, more or less. Mostly M, yes, but not only.
> XYZ is the "standard observer" (1931,1964?,199sum?) not xbar,ybar,zbar?
XYZ coordinates are defined by the response curves x,y,z, these define
the "standard observer".
>
> the same process in put in place for the CIE RGB space, note your
> comment that RGB is more of a implementation, but I think it is
> the closest hues that can be associated with LMS
There is no "CIE RGB color space". There are multiple RGB color spaces
(sRGB, ITU 601, ITU 709,...).
> since CIECAM02 defines LMS as the connection space for appearance
> matching, from XYZ, why not get rid of XYZ and use LMS for device
> matching too?
Why would it make any difference? XYZ is standardized, so there are
tables you can use. LMS is not. Depending on the researcher, the
experiment, the observers... LMS space is a little different. But even
if one would standardize LMS space, what difference would it make? LMS
to XYZ is a linear matrix multiplication, thus there isn't much to do,
and there are no advantages.
Besides, XYZ has been defined for various targets in mind, for example
to have always positive coordinates for all physically possible light
sensations.
Greetings,
Thomas