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一个物体颜色空间。

An object-color space.

作者信息

Logvinenko Alexander D

机构信息

Department of Vision Sciences, Glasgow Caledonian University, Glasgow, UK.

出版信息

J Vis. 2009 Oct 5;9(11):5.1-23. doi: 10.1167/9.11.5.

Abstract

Putting aside metaphorical meanings of the term, color space is understood as a vector space, where lights having the same color (i.e., subjectively indistinguishable) are represented as a point. The CIE 1931 color space, empirically based on trichromatic color measurements, is a classical example. Its derivatives, such as CIELAB and sRGB, have been successfully used in many applications (e.g., in color management). However, having been designed for presenting the color of self-luminous objects, these spaces are less suitable for presenting color of reflecting objects. Specifically, they can be used to represent color of objects only for a fixed illumination. Here I put forward a color space to represent the color of objects independently of illumination. It is based on an ideal color atlas comprising the reflectance spectra taking two values: k or 1 - k (0 < or = k < or = 1), with two transitions (at wavelengths lambda(1) and lambda(2)) across the spectrum. This color atlas is complete; that is, every reflecting object is metameric to some element of the atlas. When illumination alters, the classes of metameric reflectance spectra are reshuffled but in each class there is exactly one element of the atlas. Hence, the atlas can uniquely represent the metameric classes irrespective of illumination. Each element of the atlas (thus, object color) is specified by three numbers: (i) lambda = (lambda(1) + lambda(2))/2, which correlates well with hue of object color (as dominant wavelength correlates with hue of light color); (ii) delta =/lambda(1) - lambda/, which correlates with whiteness/blackness; and (iii) alpha =/1 - 2k/, which correlates with chroma of object color (as colorimetric purity correlates with saturation of light color). Using a geographical coordinate system, each element of the atlas (thus, each object color) is geometrically represented as a radius vector so that its length equals alpha, the latitude and longitude being proportional to delta and lambda, respectively.

摘要

撇开该术语的隐喻意义不谈,颜色空间被理解为一个向量空间,其中具有相同颜色(即主观上无法区分)的光被表示为一个点。基于三色颜色测量的CIE 1931颜色空间就是一个经典例子。它的衍生空间,如CIELAB和sRGB,已在许多应用中(如色彩管理)得到成功应用。然而,由于这些空间是为呈现自发光物体的颜色而设计的,所以不太适合呈现反射物体的颜色。具体而言,它们仅能用于在固定光照条件下表示物体的颜色。在此,我提出一种颜色空间,用于独立于光照来表示物体的颜色。它基于一个理想颜色图谱,该图谱包含取值为k或1 - k(0≤k≤1)的反射光谱,且在整个光谱范围内有两个转变点(波长分别为λ1和λ2)。这个颜色图谱是完备的;也就是说,每个反射物体都与图谱中的某个元素是同色异谱的。当光照改变时,同色异谱反射光谱的类别会重新排列,但每个类别中恰好有一个图谱元素。因此,无论光照如何,该图谱都能唯一地表示同色异谱类别。图谱的每个元素(即物体颜色)由三个数字指定:(i)λ = (λ1 + λ2)/2,它与物体颜色的色调相关性良好(如同主波长与光颜色的色调相关性一样);(ii)δ = |λ1 - λ|,它与白度/黑度相关;(iii)α = |1 - 2k|,它与物体颜色的色度相关(如同色度纯度与光颜色的饱和度相关性一样)。使用地理坐标系,图谱的每个元素(即每种物体颜色)在几何上被表示为一个半径向量,其长度等于α,纬度和经度分别与δ和λ成比例。

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