http://jipam.vu.edu.au/
Volume 4, Issue 4, Article 68, 2003
WEIGHTED GEOMETRIC MEAN INEQUALITIES OVER CONES IN RN
BABITA GUPTA, PANKAJ JAIN, LARS-ERIK PERSSON, AND ANNA WEDESTIG
DEPARTMENT OFMATHEMATICS, SHIVAJICOLLEGE(UNIVERSITY OFDELHI),
RAJAGARDEN, DELHI-110 027 INDIA. babita74@hotmail.com
DEPARTMENT OFMATHEMATICS,
DESHBANDHUCOLLEGE(UNIVERSITY OFDELHI), NEWDELHI-110019, INDIA.
pankajkrjain@hotmail.com
DEPARTMENT OFMATHEMATICS, LULEÅUNIVERSITY OFTECHNOLOGY,
SE-971 87 LULEÅ, SWEDEN. larserik@sm.luth.se
annaw@sm.luth.se
Received 7 November, 2002; accepted 20 March, 2003 Communicated by B. Opi´c
ABSTRACT. Let 0 < p ≤ q < ∞. Let A be a measurable subset of the unit sphere in RN, let E =x ∈ RN : x = sσ, 0 ≤ s < ∞, σ ∈ A be a cone in RN and let Sxbe the part of E with
’radius’ ≤ |x| . A characterization of the weights u and v on E is given such that the inequality
Z
E
exp
1
|Sx| Z
Sx
ln f (y)dy
q v(x)dx
1q
≤ C
Z
E
fp(x)u(x)dx
p1
holds for all f ≥ 0 and some positive and finite constant C. The inequality is obtained as a limiting case of a corresponding new Hardy type inequality. Also the corresponding companion inequalities are proved and the sharpness of the constant C is discussed.
Key words and phrases: Inequalities, Multidimensional inequalities, Geometric mean inequalities, Hardy type inequalities, Cones in RN, Sharp constant.
2000 Mathematics Subject Classification. 26D15, 26D07.
ISSN (electronic): 1443-5756
2003 Victoria University. All rights reserved.c
We thank Professor Alexandra ˇCižmešija for some valuable advice and the referee for pointing out an inaccuracy in our original manuscript (see Remark 4.6) and for several suggestions which have improved the final version of this paper.
118-02
1. INTRODUCTION
In their paper [2] J.A. Cochran and C.S. Lee proved the inequality (1.1)
Z ∞ 0
exp
εx−ε
Z x 0
yε−1ln f (y)dy
xadx ≤ ea+1ε Z ∞
0
xaf (x)dx,
where a, ε are real numbers with ε > 0, f is a positive function defined on (0, ∞) and the constant ea+1ε is the best possible. This inequality, in fact, is a generalization of what sometimes is referred to as Knopp’s inequality1 , which is obtained by taking ε = 1 and a = 0 in (1.1).
Inequalities of the type (1.1) and its analogues have further been investigated and generalized by many authors e.g. see [1], [5] – [11], [14] and [16] – [21].
In particular, very recently A. ˇCižmešija, J. Peˇcari´c and I. Peri´c [1, Th. 9, formula (23)]
proved an N − dimensional analogue of (1.1) by replacing the interval (0, ∞) by RN and the means are considered over the balls in RN centered at the origin. Their inequality reads:
(1.2) Z
RN
exp
ε |Bx|−ε Z
Bx
|By|ε−1ln f (y)dy
|Bx|adx ≤ ea+1ε Z
RN
f (x) |Bx|adx, where a ∈ R, ε > 0, f is a positive function on RN, Bxis a ball in RN with radius |x| , x ∈ RN, centered at the origin and |Bx| is its volume.
In this paper we prove a more general result, namely we characterize the weights u and v on RN such that for 0 < p ≤ q < ∞
Z
RN
exp
1
|Bx| Z
Bx
ln f (y)dy
q
v(x)dx
1q
≤ C
Z
RN
fp(x)u(x)dx
1p
holds for some finite positive constant C (See Corollary 3.3). In the case when v(x) = |Sx|a and u(x) = |Sx|b we obtain a genuine generalization of (1.2) (see Proposition 3.6 and Remark 3.7).
In this paper we also generalize the results in another direction, namely when the geometric averages over spheres in RN are replaced by such averages over spherical cones in RN (see notation below). This means in particular that our inequalities above and later on also hold when RN is replaced by RN+ or even more general cones in RN.
The paper is organized in the following way. In Section 2 we collect some preliminaries and prove a new Hardy inequality that averages functions over the cones in RN (see Theorem 2.1). In Section 3 we present and prove our main results concerning (the limiting) geometric mean operators (see Theorem 3.1 and Proposition 3.6). Finally, in Section 4 we present the corresponding companion inequalities (see Theorem 4.1, Corollary 4.2 and Proposition 4.4).
2. PRELIMINARIES
Let ΣN −1be the unit sphere in RN, that is, ΣN −1 = {x ∈ RN : |x| = 1}, where |x| denotes the Euclidean norm of the vector x ∈ RN. Let A be a measurable subset of ΣN −1, and let E ⊆ RN be a spherical cone, i.e.,
E =x ∈ RN : x =sσ, 0 ≤ s < ∞, σ ∈ A . Let Sx, x ∈ RN denote the part of E with ‘radius’ ≤ |x| , i.e.,
Sx =y ∈ RN : y =sσ, 0 ≤ s ≤ |x| , σ ∈ A .
1See e.g. [15, p. 143–144] and [12]. Note however that according to G.H. Hardy [ 4, p 156] this inequality was pointed out to him already in 1925 by G. Polya.
For 0 < p < ∞ and a non-negative measurable function w on E, by Lpw := Lpw(E) we denote the weighted Lebesgue space with the weight function w, consisting of all measurable functions f on E such that
kf kLp
w =
Z
E
|f (x)|pw(x)dx
1p
< ∞ , and make use of the abbreviations Lp and kf kLp when w(x) ≡ 1.
Let S = Sx, |x| = 1. The family of regions we shall average over is the collection of dilations of S. For x ∈ E \ {0} denote by |Sx| the Lebesgue measure of Sx. Using polar coordinates we obtain (dσ denotes the usual surface measure on ΣN −1)
|Sx| = Z |x|
0
Z
A
sN −1dσds = |x|N N |A|.
Moreover, we say that u is a weight function if it is a positive and measurable function on S.
Throughout the paper, for any p > 1 we denote p0 = p−1p .
For later purposes but also of independent interest we now state and prove our announced Hardy inequality.
Theorem 2.1. Let E be a cone in RN and Sx, A be defined as above. Suppose that 1 < p ≤ q < ∞ and that u, v are weight functions on E. Then, the inequality
(2.1)
Z
E
Z
Sx
f (y)dy
q
v(x)dx
1q
≤ C
Z
E
fp(x)u(x)dx
1p
holds for all f ≥ 0 if and only if (2.2) D := sup
t>0
Z
tS
u1−p0(x)dx
−1pZ
tS
v(x)
Z
Sx
u1−p0(y)dy
q
dx
1q
< ∞.
Moreover, the best constant C in (2.1) can be estimated as follows:
D ≤ C ≤ p0D.
Remark 2.2. Another weight characterization of (2.1) over balls in RN was proved by P.
Drábek, H.P. Heinig and A. Kufner [3] . This result may be regarded as a generalization of the usual (Muckenhaupt type) characterization in 1-dimension (see e.g. [13]) while our result may be seen as a higher dimensional version of another characterization by V.D. Stepanov and L.E. Persson (see [19] , [20]).
Proof. By the duality principle (see e.g. [13]), it can be shown that the inequality (2.1) is equivalent to that the inequality
(2.3)
Z
E
Z
E\Sx
g(y)dy
p0
u1−p0(x)dx
!p01
≤ C
Z
E
gq0(x)v1−q0(x)dx
q01
holds for all g ≥ 0 and with the same best constant C. First assume that (2.2) holds. Using polar coordinates and putting
(2.4) eg(t) =
Z
A
g(tσ)tN −1dσ, t ∈ (0, ∞) and
(2.5) u(t) =e
Z
A
u1−p0(tτ )tN −1dτ
1−p
, t ∈ (0, ∞)
we have Z
E
Z
E\Sx
g(y)dy
p0
u1−p0(x)dx
= Z ∞
0
Z
A
Z ∞ t
Z
A
g(sσ)sN −1dσds
p0
u1−p0(tτ )tN −1dτ dt
= Z ∞
0
Z ∞ t
eg(s)ds
p0
eu1−p0(t)dt.
Thus, using this, changing the order of integration and finally using Hölder’s inequality, we get
I :=
Z
E
Z
E\Sx
g(y)dy
p0
u1−p0(x)dx (2.6)
= Z ∞
0
Z ∞ t
eg(s)ds
p0
ue1−p0(t)dt
= Z ∞
0
Z ∞ z
−d dt
Z ∞ t
eg(s)ds
p0
dt
!
eu1−p0(z)dz
= p0 Z ∞
0
Z ∞ z
Z ∞
t eg(s)ds
p0−1
eg(t)dt
!
eu1−p0(z)dz
= p0 Z ∞
0
Z ∞ t
eg(s)ds
p0−1
eg(t)
Z t 0
ue1−p0(z)dz
dt
= p0 Z ∞
0
Z
A
Z ∞
t eg(s)ds
p0−1Z t
0 ue1−p0(s)ds
g(tτ )tN −1dτ dt
≤ p0
Z ∞ 0
Z
A
gq0(tτ )v1−q0(tτ )tN −1dτ dt
q01
× Z ∞
0
Z
A
Z ∞
t eg(s)ds
(p0−1)qZ t
0 ue1−p0(s)ds
q
v(tτ )tN −1dτ dt
!1q
= p0
Z
E
gq0(x)v1−q0(x)dx
q01 J1q,
where
J = Z ∞
0
Z ∞ t
eg(s)ds
(p0−1)qZ t 0
ue1−p0(s)ds
q ev(t)dt with
(2.7) ev(t) =
Z
A
v(tτ )tN −1dτ.
Using Fubini’s theorem, (2.2), (2.5) and (2.7), we get
J = Z ∞
0
Z ∞ t
d dz −
Z ∞ z
eg(s)ds
(p0−1)q! dz
Z t 0
ue1−p0(s)ds
q ev(t)dt
= Z ∞
0
"
d dz −
Z ∞
z eg(s)ds
(p0−1)q!#
Z z 0
Z t
0 eu1−p0(s)ds
q
ev(t)dtdz
= Z ∞
0
"
d dz −
Z ∞ z
eg(s)ds
(p0−1)q!#
×
Z z 0
Z
A
Z t 0
Z
A
u1−p0(sσ)sN −1dσds
q
v(tτ )tN −1dτ dt
dz
= Z ∞
0
"
d dz −
Z ∞ z
eg(s)ds
(p0−1)q!#
×
Z
zS
Z
Sx
u1−p0(y)dy
q
v(x)dx
dz
≤ Dq Z ∞
0
"
d dz −
Z ∞ z
eg(s)ds
(p0−1)q!#
Z
zS
u1−p0(x)dx
pq dz
= Dq Z ∞
0
"
d dz −
Z ∞
z eg(s)ds
(p0−1)q!#
Z z
0 ue1−p0(t)dt
qp dz.
Thus, using Minkowski’s integral inequality, (2.4) and (2.5) we have
J ≤ Dq
Z ∞
0
Z ∞ t
"
d dz −
Z ∞ z
eg(s)ds
(p0−1)q!#
dz
!pq
ue1−p0(t)dt
q p
= Dq Z ∞
0
Z ∞ t
eg(s)ds
p0
ue1−p0(t)dt
!qp
= Dq Z
E
Z
E\Sx
g(y)dy
p0
u1−p0(x)dx
!qp .
Assume first that in (2.6) I < ∞. Then
Z
E
Z
E\Sx
g(y)dy
p0
u1−p0(x)dx
!p01
≤ p0D
Z
E
gq0(x)v1−q0(x)dx
q01
i.e., (2.3) holds for all g ≥ 0 and also the constant C in (2.3) satisfies C ≤ p0D. For the case I = ∞ replace g(y) by an approximating sequence gn(y) ≤ g(y) (such that the corresponding In< ∞) and use the Monotone Convergence Theorem to obtain the result.
Conversely, suppose that (2.1) holds for all f ≥ 0. In this inequality, taking for any fixed t > 0 the function ft= χtSu1−p0, we find that
C ≥
Z
E
Z
Sx
ft(y)dy
q
v(x)dx
1q Z
E
ftp(x)u(x)dx
−1p
≥
Z
tS
Z
Sx
u1−p0(y)dy
q
v(x)dx
1q Z
tS
u1−p0(x)dx
−1p
.
By taking the supremum we find that (2.2) holds and, moreover, D ≤ C. The proof is complete.
3. GEOMETRICMEANINEQUALITIES
Here we prove our main geometric mean inequality by making a limit procedure in Theorem 2.1.
Theorem 3.1. Let 0 < p ≤ q < ∞ and suppose that all other assumptions of Theorem 2.1 are satisfied. Then the inequality
(3.1)
Z
E
exp
1
|Sx| Z
Sx
ln f (y)dy
q
v(x)dx
1q
≤ C
Z
E
fp(x)u(x)dx
1p
holds for all f > 0 if and only if D1 := sup
t>0
|tS|−1p
Z
tS
w(x)dx
1q
< ∞, where
(3.2) w(t) := v(x)
exp
1
|Sx| Z
Sx
ln 1 u(y)dy
qp
< ∞.
Moreover, the best constant C satisfies D1 ≤ C ≤ e1pD1. Proof. It is easy to see that (3.1) is equivalent to
Z
E
exp
1
|Sx| Z
Sx
ln f (y)dy
q
w(x)dx
1q
≤ C
Z
E
fp(x)dx
p1
with w(x) defined by (3.2). Let v(x) = w(x) |Sx|−q and u(x) =1 in Theorem 2.1 and choose an α such that 0 < α < p ≤ q < ∞. Then 1 < αp ≤ αq < ∞. Now, replacing f, p, q and v(x) by fα,pα,αq in Theorem 2.1, we find that the inequality
(3.3)
Z
E
1
|Sx| Z
Sx
fα(y)dy
αq
w(x)dx
!1q
≤ Cα
Z
E
fp(x)dx
1p
holds for all functions f > 0 if and only if D1 holds. Moreover, it is easy to see that (c.f. [20])
(3.4) D1 ≤ Cα ≤
p p − α
α1 D1.
By letting α → 0+in (3.3) and (3.4) we find that
p p−α
α1
→ e1p and
1
|Sx| Z
Sx
fα(y)dy
α1
→ exp
1
|Sx| Z
Sx
ln f (y)dy
,
i.e. the scale of power means converge to the geometric mean, and the proof follows. Remark 3.2. Our proof above shows that (3.1) in Theorem 3.1 may be regarded as a natural limiting case of Hardy’s inequality (2.1) as it is in the classical one-dimensional situation. This fact indicates that our formulation of Hardy’s inequality in Theorem 2.1 is very natural from this point of view.
As a special case, if we take E = RN and Sx = Bx the ball centered at the origin and with radius |x| , and |Bx| its volume, then we immediately obtain the following corollary to Theorem 3.1 that averages functions over balls in RN:
Corollary 3.3. Let 0 < p ≤ q < ∞ and u, v be weight functions in RN. Then the inequality
Z
RN
exp
1
|Bx| Z
Bx
ln f (y)dy
q
v(x)dx
1q
≤ C
Z
RN
fp(x)u(x)dx
1p
holds for all f > 0 if and only if
D2 := sup
z∈RN\{0}
|Bz|−p1 Z
Bz
v(x)
exp
1
|Bx| Z
Bx
ln 1 u(y)dy
qp dx
!1q
< ∞.
Moreover, the best constant C satisfies D2 ≤ C ≤ e1pD2.
Remark 3.4. Corollary 3.3 extends a result of P. Drábek, H.P. Heinig and A. Kufner [3, Theo- rem 4.1], who obtained it for the case p = q = 1 and with a completely different proof.
Remark 3.5. Setting E = RN+ = (x1, . . . , xN) ∈ RN, x1 ≥ 0, . . . , xN ≥ 0 in Theorem 3.1 we obtain that Corollary 3.3 holds also for RN+ instead of RN and Bx∩ RN+ instead of Bx.
We shall now consider the special weights discussed in our introduction and in [1].
Proposition 3.6. Let 0 < p ≤ q < ∞, a, b ∈ R, ε ∈ R+, and E, Sxbe defined as in Theorem 2.1. Then
(3.5)
Z
E
exp
ε |Sx|−ε Z
Sx
|Sy|ε−1ln f (y)dy
q
|Sx|adx
1q
≤ C
Z
E
fp(x) |Sx|bdx
1p
holds for all positive functions f for some finite constant C if and only if
(3.6) a + 1
q = b + 1 p and the least constant C in (3.5) satisfies
p q
1q
ε1p−1qeb+1εp −1p ≤ C ≤ p q
1q
ε1p−1qeb+1εp . Proof. By writing (3.5) in polar coordinates we find that
Z ∞ 0
Z
A
"
exp εNε tN ε|A|ε
Z t 0
Z
A
|A|
N
ε−1
sN ε−1ln f (sσ)dσds
#q
tN a+N −1 |A|
N
a
dτ dt
!1q
≤ Z ∞
0
Z
A
fp(tτ ) |A|
N
b
tN b+N −1dτ dt
!1p .
Exchanging variables, s = r1ε and t = z1ε we find that this inequality can be rewritten as
Z ∞ 0
Z
A
exp
N
|A| zN Z z
0
Z
A
ln f r1εσ
rN −1dσdr
q
× |A|
N
a
zN(a+1ε −1)zN −11 εdτ dz
1q
≤ C Z ∞
0
Z
A
fp
z1ετ
|A|
N
b
zN(b+1ε −1)zN −11 εdτ dz
!1p , that is,
(3.7)
Z
E
exp
1
|Sx| Z
Sx
ln f1(y)dy
q
|Sx|a+1ε −1dx
1q
≤ C |A|
N
(b+1p −a+1
q )(1−1ε) ε1q−1p
Z
E
f1p(x) |Sx|b+1ε −1dx
1p , where f1(rσ) = f (r1εσ). This means that (3.5) is equivalent to (3.7) i.e., (3.1) holds with the weights v(x) = |Sx|a+1ε −1and u(x) = |Sx|b+1ε −1. We note that for these weights we find after a direct calculation that the constant D1 from Theorem 3.1 is
D1 = sup
t>0
|tS|a+1εq −b+1εp e1p(b+1ε −1)
a+1
ε − qp b+1ε − 11q so we conclude that (3.6) must hold and then
D1 = e1p(b+1ε −1) p q
1q .
Thus, the proof follows from Theorem 3.1.
Remark 3.7. Setting p = q = 1, a = b, we have that (3.5) implies the estimate (1.2).
Remark 3.8 (Sharp Constant). In the above proposition, if we take p = q, then a = b. In this situation (3.5) holds with the constant C = e(b+1)/p. Indeed, this constant is sharp. In order to show this for δ > 0, we consider the function
fδ(x) =
e−b+1εp |S|−(b+1)|x|−Np(b+1−εδ), x ∈ S, e−b+1εp |S|−(b+1)|x|−Np(b+1+εδ), x ∈ E\S.
By using this function in (3.5), we find that 1 ≤ RHS
LHS ≤ epδ → 1 as δ → 0
and consequently the constant is sharp. Note that the sharpness of the constant for p = q, in Proposition 3.6 has been proved in the more general setting than that in [1].
4. THECOMPANIONINEQUALITIES
We present the following result which is a companion of Theorem 3.1:
Theorem 4.1. Let 0 < p ≤ q < ∞, ε > 0, and suppose that all other hypotheses of Theorem 3.1 are satisfied. Then the inequality
(4.1)
Z
E
exp
ε |Sx|ε
Z
E\Sx
|Sy|−ε−1ln f (y)dy
q
v(x)dx
1q
≤ C
Z
E
fp(x)u(x)dx
1p
holds for all f > 0 if and only if
D3 := sup
t>0
|tS|−1p Z
tS
v∗(x)
exp
1
|Sx| Z
Sx
ln 1 u∗(y)dy
qp dx
!1q
< ∞, where
u∗(y) := u(s−1εσ)1
εs−N(1+1ε), v∗(y) := v(s−1εσ)1
εs−N(1+1ε).
Moreover, the constant C satisfies D3 ≤ C ≤ ep1D3. Proof. Note that for x ∈ RN
|Sx| = Z |x|
0
Z
A
tN −1dτ dt = |x|N N |A|.
Now, using polar coordinates, (4.1) can be written as Z ∞
0
Z
A
expε |A|εtN ε N
Z ∞ t
Z
A
|A|
N
−ε−1
s−N ε−1ln f (sσ)dσds
!q
v(tτ )tN −1dτ dt
!1q
≤ C
Z ∞ 0
Z
A
fp(tτ )u(tτ )tN −1dτ dt
1p . Using the exchange of variables s = r−1/ε and t = z−1/ε we obtain
Z ∞ 0
Z
A
exp
N
|A| zN Z
A
Z z 0
ln f (r−1εσ)rN −1dσdr
q
v(z−1ετ )z−N (1+1ε)1
εzN −1dτ dz
1q
≤ C
Z ∞ 0
Z
A
fp(z−1ετ )u(z−1ετ )z−N (1+1ε)1
εzN −1dτ dz
1p
and put f∗(tτ ) = f (t−1ετ ). (4.1) can be equivalently rewritten as
Z
E
exp
1
|Sx| Z
Sx
ln f∗(y)dy
q
v∗(x)dx
1q
≤ C
Z
E
f∗p(x)u∗(x)dx
1p .
Now, the result is obtained by using Theorem 3.1.
Analogously to Corollary 3.3, we can immediately obtain a special case of Theorem 4.1 that averages functions over balls in RN centered at origin.
Corollary 4.2. Let 0 < p ≤ q < ∞, ε > 0, and u, v be weight functions in RN. Then the inequality
(4.2)
Z
RN
exp
ε |Bx|ε
Z
RN\Bx
|By|−ε−1ln f (y)dy
q
v(x)dx
1q
≤ C
Z
RN
fp(x)u(x)dx
1p
holds for all f > 0 if and only if
B := supe
z∈RN
|Bz|−1p Z
Bz
v0(x)
exp
1
|Bx| Z
Bx
ln 1 u0(y)dy
pq dx
!1q
< ∞, where
u0(x) := u(t−1ετ )1
εt−N (1+1ε), v0(x) := v(t−1ετ )1
εt−N (1+1ε). Moreover, the best constant C satisfies eB ≤ C ≤ e1pB.e
Remark 4.3. Note that by choosing E as in Remark 3.5 we see that Corollary 4.2 in fact holds also when RN is replaced by RN+ or more general cones in RN.
The corresponding result to Proposition 3.6 reads as follows and the proof is analogous.
Proposition 4.4. Let 0 < p ≤ q < ∞, ε > 0, and a, b ∈ R, and E, Sxbe defined as in Theorem 2.1. Then the inequality
(4.3)
Z
E
exp ε |Sx|ε Z
E\Sx
|Sy|−ε−1ln f (y)dy
q
|Sx|adx
1q
≤ C
Z
E
fp(x) |Sx|bdx
1p
holds for all f > 0 and some finite positive constant C if and only if a + 1
q = b + 1 p and the least constant C in (4.3) satisfies
p q
−1q
ε1p−1qe−(b+1εp +1p) ≤ C ≤ p q
−1q
εp1−1qe−b+1εp .
Remark 4.5 (Sharp Constant). Analogously to Proposition 3.6, in the above proposition we also find that if we take p = q, then a = b. In this situation (4.3) holds with the constant C = e−(b+1)/εp and the constant is sharp. This can be shown by considering, for δ > 0, the function
fδ(x) =
eb+1εp |S|−(b+1)|x|−Np(b+1−εδ), x ∈ S eb+1p |S|−(b+1)|x|−Np(b+1+εδ), x ∈ E\S.
Remark 4.6. It is tempting to think that the results in this paper hold also in general star-shaped regions in RN (c.f. [22]) but this is not true in general as was pointed out to us by the referee.
See also [22] and note that the results there also hold at least for cones in RN.
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