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factors. This is the continuous counterpart of the partition invariance prop-
erty of discrete Shannon entropy (see e.g. [62]).
Rényi's quadratic (differential) entropy of a partitioned PDF is expressed
as
ln
i
f i ( x ) dx ;
a i
H R 2 ( f )=
(C.4)
D i
that is, H R 2 ( f ) is not decomposable as Shannon's counterpart. Nevertheless,
as the minimization of H R 2 ( f ) is equivalent to the maximization of V R 2
=
exp(
H R 2 ), we may use the decomposition of the information potential V R 2
which is readily expressed as
V R 2 ( f )=
i
a i V R 2 ( f i ) .
(C.5)
The variance of f can also be decomposed as
V [ f ]=
i
a i V [ f i ]+
i
μ ) 2 ,
a i ( μ i
(C.6)
where μ ( μ i ) is the expected value of f ( f i ).
 
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