Volume 2009, Article ID 901397,8pages doi:10.1155/2009/901397
Research Article
An Inequality for the Beta Function with
Application to Pluripotential Theory
Per ˚
Ahag
1and Rafał Czy ˙z
21Department of Natural Sciences, Engineering and Mathematics, Mid Sweden University,
871 88 H¨arn¨osand, Sweden
2Institute of Mathematics, Jagiellonian University,Łojasiewicza 6, 30-348 Krak´ow, Poland
Correspondence should be addressed to Per ˚Ahag,[email protected]
Received 4 June 2009; Accepted 22 July 2009
Recommended by Paolo Ricci
We prove in this paper an inequality for the beta function, and we give an application in pluripotential theory.
Copyrightq2009 P. ˚Ahag and R. Czy ˙z. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
1. Introduction
A correspondence that started in 1729 between Leonhard Euler and Christian Goldbach was the dawn of the gamma function that is given by
Γx
∞
0
e−ttx−1dt 1.1
see, e.g.,1,2. One of the gamma function’s relatives is the beta function, which is defined by
Ba, b
1
0
ta−11−tb−1dt . 1.2
The connection between these two Eulerian integrals is
Ba, b ΓaΓb
Since Euler’s days the research of these special functions and their generalizations have had great impact on, for example, analysis, mathematical physics, and statistics. In this paper we prove the following inequality for the beta function.
Inequality A. For all n∈N and allp≥0p /0,p /1there exists a numberk >0 such that
knpnp/np Bp1, kn> Bp1, n. 1.4
If p0,then we have equality in1.4, and ifp1,then we have the opposite inequality for alln∈N,k >0.
In Section 3 we will give an application of Inequality A within the pluripotential theory.
2. Proof of Inequality A
A crucial tool inLemma 2.2is the following theorem.
Theorem 2.1. Letψx Γx/Γxbe the digamma function. Then forx >0it holds that
ψx> 1 x
1
2x2, ψx>−
1
x2 −
1
x3 −
1
2x4. 2.1
Proof. This follows from3, Theorem 8 see also4,5.
Lemma 2.2. Letα:N×0,∞ → Rbe a function defined by
αn, p 1 n
p
npψn−ψ
np1, 2.2
where ψx Γx/Γxis the digamma function. Thenαn, p/0for alln ∈ Nand allp > 0
(p /1). Furthermore,αn,1 0for alln∈N.
Proof. Sinceψx1 ψx 1/x,we have thatαn,1 0, and
αn, p 1 n
p−1
np ψn−ψ
np. 2.3
From the construction ofαwe also have thatαn,0 0. By using2.3we get that
∂α ∂p
n1
np2 −ψ
np .
2.4
FromTheorem 2.1it follows that
∂α ∂p <
n1
np2 −
1
np −
1 2np2
1−2p
Thus,
∂α
∂p <0 forp∈
1 2,∞
. 2.6
Furthermore,
∂2α
∂p2
−2n1
np3 −ψ
np, 2.7
and sinceψx>−1/x2−1/x3−1/2x4Theorem 2.1, we get that
∂2α
∂p2 <
−2n1
np3
1
np2
1
np3
1 2np4
−2n2−2n−2p2p21
2np4 ,
2.8
which means that
∂2α
∂p2 <0 forp∈0,1. 2.9
From2.6,2.9, and the fact thatαn,1 αn,0 0, we conclude thatαn, p/0 for all
n∈Nand allp >0p /1.
Proof of Inequality A.
Case 1p0. The definition
Ba, b
1
0
ta−11−tb−1dt 2.10
yields thatBa,1 B1, a 1/a. Thus,
kB1, kn 1
n B1, n, 2.11
which is precisely the desired equality.
Case 2p1. We will now prove that for allk >0 it holds that
Inequality2.12is equivalent to
k2n1/n1 1 kn1
1
kn ≤
1
nn1. 2.13
Hence, to complete this case we need to prove that for allk >0 we have that
kn/n1 1 kn1 ≤
1
n1. 2.14
Leth:0,∞ → Rbe defined by
hk kn1−kn/n1n−kn/n1. 2.15
To obtain2.14it is sufficient to prove thath≥0. The definition ofhyields that
h0 1, lim
k→ ∞hk ∞, h
k n1−k−1/n1. 2.16
Thus,
ahhas a minimum point ink1;
bhis decreasing on0,1;
chis increasing on1,∞;
dh1 0.
Thus,hk≥0 fork≥0.
Case 3p >0, p /1. Fixn∈N. LetF:0,∞ → Rbe the function defined by
Fk knpnp/npBp1, kn−Bp1, n. 2.17
This construction implies thatF is continuously differentiable, andF1 0. To prove this case it is enough to show thatF1/0. By rewritingBp1, knwith1.3the functionFcan be written as
Fk knpnp/npΓ
p1Γkn
Γknp1 −B
and therefore we get that
Fk Γp1 npnp
np k
np/np Γkn
Γknp1
nknpnp/npΓ
knΓknp1−ΓknΓknp1
Γ2knp1
nknp/npBkn, p11
n p npk
ψkn−ψknp1.
2.19
Thus
F1 nBn, p11
n p
npψn−ψ
np1, 2.20
whereψx Γx/Γxis the digamma function. This proof is then completed by using
Lemma 2.2.
3. The Application
We start this section by recalling some definitions and needed facts. Adomainis an open and connected set, and a bounded domainΩ⊆Cnishyperconvexif there exists a plurisubharmonic
functionϕ :Ω → −∞,0such that the closure of the set{z ∈ Ω :ϕz < c}is compact in
Ω, for everyc∈−∞,0; that is, for everyc < 0 the level set{z ∈Ω:ϕz < c}is relatively compact inΩ. The geometric condition that our underlying domain should be hyperconvex is to ensure that we have a satisfying quantity of plurisubharmonic functions. ByE0Ωwe denote the family of all bounded plurisubharmonic functionsϕdefined onΩsuch that
lim
z→ξϕz 0 for everyξ∈∂Ω,
Ω
ddcϕn<∞, 3.1
where ddc·n
is the complex Monge-Amp`ere operator. Next letEpΩ,p > 0, denote the
family of plurisubharmonic functions u defined on Ω such that there exists a decreasing sequence{uj},uj∈ E0, that converges pointwise touonΩ, asjtends to∞, and
sup
j≥1
Ω
−uj p
ddcuj n
sup
j≥1
ep
uj
<∞. 3.2
If u ∈ EpΩ, then epu < ∞ 6, 7. It should be noted that it follows from6 that
the complex Monge-Amp`ere operator is well defined onEp. For further information about
pluripotential theory and the complex Monge-Amp`ere operator we refer to8,9.
Theorem 3.1. Letp >0, andn≥1. Then there exists a constantDn, p≥1, depending only onn
andp, such that for anyu0, u1, . . . , un∈ Epit holds that
Ω−u0 p
ddcu1∧ · · · ∧ddcun≤D
n, pepu0p/pnepu11/pn. . . epun1/pn. 3.3
Moreover,
Dn, p≤
⎧ ⎪ ⎨ ⎪ ⎩
1
p
n/n−p
, if0< p <1,
ppan,p/p−1, if p>1,
3.4
Dn,1 1and an, p p2p1/pn−1 −p1. If n 1, then one follows [12] and interprets3.3as
Ω−u
pΔ
v≤D1, p Ω−u
pΔ
u
p/p1
Ω−v
pΔ
v
1/p1
. 3.5
IfDn, p 1 for all functions inEp, then the methods in15 would immediately
imply that the vector spaceEp−Ep, with certain norm, is a Banach space. Furthermore, proofs
in15 see also6could be simplified, and some would even be superfluous. Therefore, it is important to know for whichn, pthe constantDn, pis equal or strictly greater than one. With the help of Inequality A we settle this question. InExample 3.2, we show that there are functions such that, for alln∈Nand allp >0p /1, the constantDn, p, in3.3, is strictly greater than 1.
Example 3.2. LetB0,1⊂Cnbe the unit ball, and forα >0 set
uαz |z|2α−1. 3.6
Hence,
wheredλnis the Lebesgue measure onCn. Forβ >0 we then have that
B0,1 −uαp
ddcu β
n
n!4nβn1
B0,1
1− |z|2αp|z|2nβ−1dλn
n!4nβn1
∂B0,1dσn 1
0
1−t2αpt2nβ−1t2n−1dt
n!4nβn1σn∂B0,1 1
0
1−t2αpt2nβ−1dt
n!4nβn12 π
n
n−1! 1 2α
1
0
1−spsnβ/α−1ds
n4πnβ
n1
α B
p1,β αn
,
3.8
wheredσnis the Lebesgue measure on∂B0,1. Ifα β, then
B0,1
−uαpddcuαnn4πnαn B
p1, n. 3.9
If we assume thatDn, p 1 inTheorem 3.1, then it holds that
n4πnβ
n1
α B
p1,β αn
≤n4πnαnBp1, np/npn4πnβnBp1, nn/np.
3.10
Hence,
β α
npnp/np
B
p1,β αn
≤Bp1, n ∀α, β >0. 3.11
In particular, ifβ/αk, then we get that
knpnp/npBp1, kn≤Bp1, n. 3.12
This contradicts Inequality A. Thus, there are functions such thatDn, p>1 for alln∈Nand allp >0p /1.
Acknowledgments
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