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Light Field Duality: Concept and Applications: Difference between revisions
Light Field Duality: Concept and Applications (view source)
Revision as of 20:22, 23 December 2020
, 23 December 2020→Dual Representation
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</math> | </math> | ||
Given a point, this constraint defines the hyperline in the 4D light field space. | Given a point, this constraint defines the hyperline in the 4D light field space. | ||
Henceforth, a hyperline will be represented as <math>(a, b, c, d)</math> where hyperpoints on said line satisfy: | |||
<math> | |||
\begin{bmatrix} | |||
a & 0 & b & 0\\ | |||
0 & a & 0 & b | |||
\end{bmatrix} | |||
\begin{bmatrix} | |||
s \\ t \\ u \\ v | |||
\end{bmatrix} | |||
= | |||
\begin{bmatrix} | |||
c \\ d | |||
\end{bmatrix} | |||
</math> | |||
The paper has the following remarks: | The paper has the following remarks: | ||