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R. S. Stankovi´ c et al.
The Gibbs dyadic derivative of a bent function is the set of eigenvalues of
this operator with the signs corresponding to that in the function values, and it
consists of first 2 n non-negative integers. In this way, the Gibbs dyadic derivative
associates with each bent function an easily determined Gibbs permutation matrix.
These matrices are not the same as matrices converting a bent function into another
in either Boolean or Walsh spectral domain, since they relate these functions in
the Gibbs dyadic derivative domain. They however still can be used to establish
relationships among bent functions and to generate them from the subsets of bent
functions.
We show that Gibbs permutation matrices have a particular block structure which
can be expressed in terms of four precisely defined submatrices.
References
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