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There is no known closed form of the entropy, which can be written as H =
I ( r, k ) /F ( r, k )+ln a +ln F ( r, k ) ( I ( r, k ) is defined in D.2.2). Therefore, in
terms of a , H ( V ) is clearly USF. Setting k =1, numerical computation leads
to the conclusion that H ( V ) is also USF in terms of r (and therefore of m ,
the parameter controlling the tails).
Student's t -distribution is the special symmetrical case ( k =0)of this
family. It is easy to check that the entropy of the Student's t distribution is
aUSFof V .
Type V: Δ =0.
Corresponds
to
the
Inverse
Gamma
family
f ( x )
=
1
β α
β/x ) ( α ),with x> 0 (shape), β (scale) > 0.The
variance and the entropy are given in Sect. D.2.2. Note that in order for
f ( x ) to have variance α must be larger than 2. For fixed α ,theentropyis
x α +1 exp(
ln( V ) plus a constant, which is an obvious USF. For fixed β ,numerical
computation shows that the entropy is also a USF of V .
Type VI: Δ> 0 and x
a 2 , the larger root.
Corresponds to f ( x )= Kx −q 1 ( x
a ) q 2 ,with q 1 < 1 ,q 2 >
1 ,q 1 >q 2
1,
and x
]. There is no known entropy formula for the general solution.
A particular subtype is the Beta distribution of the second kind (also known
as Beta prime distribution), with f ( x )= x α− 1 (1+ x ) −α−β /B ( α, β ) for x
] a,
0.
The variance is given in Sect. D.2.2; there is no known formula of the entropy.
Numerical computation shows that H ( V ) is a USF function both in terms of
α and β .
Another special subtype is the F distribution family, whose variance and
entropy are given in Sect. D.2.2. Numerical computation shows that the en-
tropy is a USF of V , in relation to either of the two parameters (degrees of
freedom) of this family.
Type VII: Δ> 0 ,b =0 ,c> 0 .
Corresponds to f ( x )= K (1+ x 2 /a 2 ) −m ,with a
=0 ,m> 1 / 2. A particular
case is the Student's t -density already analyzed in type IV. The entropy of
Type VII distributions is a USF of the variance for fixed a or m .
Type VIII: Δ> 0 and a 1 = a 2 =
m .
Corresponds to f ( x )= K (1 + x/a ) −m ,with m> 1 and x ∈ ] − a, 0].
These are asymmetric distributions, with hyperbolic shape sharply peaked
for high m . Setting w.l.o.g. a =1( a simply controls where the peak occurs)
and x
]0 , 1[ (the area is infinite for =0), one
obtains a family of distributions with variance defined for m> 2.Numerical
computation shows that the entropy of the family is then an up-saturating
function of the variance.
[
1+ , 0],with
Type IX: Δ> 0 and a 1 = a 2 = m .
A version of Type VIII, with f ( x )= K (1 + x/a ) m ,m>
1 and x
]
a, 0]. The area is finite for m
0, which affords simpler formulas for
 
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