// Workers AI · traducción al español
Función poligámica equilibrada
En matemáticas, la función de poligamia generalizada o función negapolygamma equilibrada es una función introducida por Olivier Espinosa Aldunate y Victor Hugo Moll.
Traducción generada por IA. El artículo original en inglés continúa abajo.
Balanced polygamma function
From Wikipedia, the free encyclopedia
In mathematics, the generalized polygamma function or balanced negapolygamma function is a function introduced by Olivier Espinosa Aldunate and Victor Hugo Moll .[ 1]
It generalizes the polygamma function to negative and fractional order, but remains equal to it for integer positive orders.
The generalized polygamma function is defined as follows:
ψ
(
z
,
q
)
=
ζ
′
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z
+
1
,
q
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+
(
ψ
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−
z
)
+
γ
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ζ
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z
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1
,
q
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Γ
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−
z
)
{\displaystyle \psi (z,q)={\frac {\zeta '(z+1,q)+{\bigl (}\psi (-z)+\gamma {\bigr )}\zeta (z+1,q)}{\Gamma (-z)}}}
or alternatively,
ψ
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z
,
q
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=
e
−
γ
z
∂
∂
z
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e
γ
z
ζ
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1
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Γ
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−
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,
{\displaystyle \psi (z,q)=e^{-\gamma z}{\frac {\partial }{\partial z}}\left(e^{\gamma z}{\frac {\zeta (z+1,q)}{\Gamma (-z)}}\right),}
where ψ (z ) is the polygamma function and ζ (z ,q ) , is the Hurwitz zeta function .
The function is balanced, in that it satisfies the conditions
f
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0
)
=
f
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1
)
and
∫
0
1
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d
x
=
0
{\displaystyle f(0)=f(1)\quad {\text{and}}\quad \int _{0}^{1}f(x)\,dx=0}
.
Several special functions can be expressed in terms of generalized polygamma function.
ψ
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ψ
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0
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ψ
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n
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=
ψ
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n
∈
N
Γ
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=
exp
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ψ
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−
1
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x
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+
1
2
ln
2
π
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ζ
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=
(
−
1
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z
Γ
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ψ
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z
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1
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ζ
′
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=
ψ
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2
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2
2
−
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2
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1
12
{\displaystyle {\begin{aligned}\psi (x)&=\psi (0,x)\\\psi ^{(n)}(x)&=\psi (n,x)\qquad n\in \mathbb {N} \\\Gamma (x)&=\exp \left(\psi (-1,x)+{\tfrac {1}{2}}\ln 2\pi \right)\\\zeta (z,q)&={\frac {(-1)^{z}}{\Gamma (z)}}\psi (z-1,q)\\\zeta '(-1,x)&=\psi (-2,x)+{\frac {x^{2}}{2}}-{\frac {x}{2}}+{\frac {1}{12}}\\\end{aligned}}}
K
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z
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=
A
exp
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ψ
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−
2
,
z
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+
z
2
−
z
2
)
{\displaystyle K(z)=A\exp \left(\psi (-2,z)+{\frac {z^{2}-z}{2}}\right)}
where K (z ) is the K -function and A is the Glaisher constant .
The balanced polygamma function can be expressed in a closed form at certain points (where A is the Glaisher constant and G is the Catalan constant ):
ψ
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−
2
,
1
4
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=
1
8
ln
A
+
G
4
π
ψ
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−
2
,
1
2
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=
1
2
ln
A
−
1
24
ln
2
ψ
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−
3
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1
2
)
=
3
ζ
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3
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32
π
2
ψ
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−
2
,
1
)
=
−
ln
A
ψ
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−
3
,
1
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=
−
ζ
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3
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8
π
2
ψ
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−
2
,
2
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=
−
ln
A
−
1
ψ
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−
3
,
2
)
=
−
ζ
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3
)
8
π
2
−
3
4
{\displaystyle {\begin{aligned}\psi \left(-2,{\tfrac {1}{4}}\right)&={\tfrac {1}{8}}\ln A+{\frac {G}{4\pi }}&&\\\psi \left(-2,{\tfrac {1}{2}}\right)&={\tfrac {1}{2}}\ln A-{\tfrac {1}{24}}\ln 2&\\\psi \left(-3,{\tfrac {1}{2}}\right)&={\frac {3\zeta (3)}{32\pi ^{2}}}\\\psi (-2,1)&=-\ln A&\\\psi (-3,1)&={\frac {-\zeta (3)}{8\pi ^{2}}}\\\psi (-2,2)&=-\ln A-1&\\\psi (-3,2)&={\frac {-\zeta (3)}{8\pi ^{2}}}-{\tfrac {3}{4}}\\\end{aligned}}}