In image analysis, the generalized structure tensor (GST) is an extension of the Cartesian structure tensor to curvilinear coordinates. It is mainly used to detect and to represent the "direction" parameters of curves, just as the Cartesian structure tensor detects and represents the direction in Cartesian coordinates. Curve families generated by pairs of locally orthogonal functions have been the best studied. It is a widely known method in applications of image and video processing including computer vision, such as biometric identification by fingerprints, and studies of human tissue sections.
GST in 2D and locally orthogonal bases Let the term image represent a function f ( ξ ( x , y ) , η ( x , y ) ) {\displaystyle f(\xi (x,y),\eta (x,y))} where x , y {\displaystyle x,y} are real variables and ξ , η {\displaystyle \xi ,\eta } , and f {\displaystyle f} , are real valued functions. GST represents the direction along which the image f {\displaystyle f} can undergo an infinitesimal translation with minimal (total least squares) error, along the "lines" fulfilling the following conditions: 1. The "lines" are ordinary lines in the curvilinear coordinate basis ξ , η {\displaystyle \xi ,\eta }
cos ( θ ) ξ ( x , y ) + sin ( θ ) η ( x , y ) = constant {\displaystyle \cos(\theta )\xi (x,y)+\sin(\theta )\eta (x,y)={\text{constant}}}
which are curves in Cartesian coordinates as depicted by the equation above. The error is measured in the L 2 {\displaystyle L^{2}} sense and the minimality of the error refers thereby to L2 norm. 2. The functions ξ ( x , y ) , η ( x , y ) {\displaystyle \xi (x,y),\eta (x,y)} constitute a harmonic pair, i.e. they fulfill Cauchy–Riemann equations,
∂ ξ ∂ x = − ∂ η ∂ y , ∂ ξ ∂ y = ∂ η ∂ x . {\displaystyle {\begin{aligned}&{\frac {\partial \xi }{\partial x}}=-{\frac {\partial \eta }{\partial y}},\\[4pt]&{\frac {\partial \xi }{\partial y}}={\frac {\partial \eta }{\partial x}}.\end{aligned}}}
Accordingly, such curvilinear coordinates ξ , η {\displaystyle \xi ,\eta } are locally orthogonal. Then GST consists in
G S T = ( λ m a x − λ m i n ) ∫ w ( ξ , η ) [ ∂ f ∂ ξ ∂ f ∂ η ] [ ∂ f ∂ ξ , ∂ f ∂ η ] d ξ d η + λ m i n I {\displaystyle GST=(\lambda _{max}-\lambda _{min})\int w(\xi ,\eta )\left[{\begin{array}{c}{\frac {\partial f}{\partial \xi }}\\{\frac {\partial f}{\partial \eta }}\\\end{array}}\right][{\frac {\partial f}{\partial \xi }},{\frac {\partial f}{\partial \eta }}]d\xi d\eta +\lambda _{min}I}
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