CARNOT GROUPS
YING-XIONG XIAO
Abstract. We prove some weighted Poincar´e inequalities on Carnot groups and obtain the sharp constants. These improve the corresponding results of Fausto Ferrari and Enrico Valdinoci.
1. Introduction
Let Ω be a domain inRn and Abe a smooth symmetric matrix function on Ω.
Assume that there exist Λ > 0 such that for every ξ ∈ Rn and all x∈ Ω, there hiolds
0≤ hA(x)ξ, ξi ≤Λ|ξ|2.
F. Ferrari and E. Valdinocihad [4] have showed that ifuis aC2stable week solution of the following PDE
div(A(x)∇u(x)) =f(u(x)), then the following general Poincar´e inequality holds:
(1.1)
Z
Ω
hA(x)∇φ,∇φi|∇u|2≥ Z
ΩT {∇u6=0}
W(x)φ2, where
W(x) = Xn
i=1
hA(x)∇ui,∇uii − hA(x)(D2u·N),(D2u·N)i − Xn
i=1
div(Ai(x)∇u)ui
and N = |∇u(x)|∇u(x). By the choice of suitable A(x) and stable solutions, F. Fer- rari and E. Valdinocihad [4] obtained some weighted Poincar´e inequalities for the Laplace operator in the Euclidean space Rn, Kohn’s sublaplace operator in the Heisenberg group Hn, the sublaplace operator in the Engel group, the Franchi- Grushin-Lanconelli operators and thep-laplacian in the Euclidean spaceRn.
The aim of this note is to prove analogous Poincar´e inequalities with weights on Carnot groups. We refer to [7, 11] for Hardy inequalities on this groups. Our proof shows if one considers the weighted Poincar´e inequalities on Carnot groups (not the general Poincar´e inequality (1.1)), one needs not use the stable solutions. In fact, we offer here an alternative elementary proof, in which some calculus is enough.
To state our results, we need some notations. Recall that a Carnot groupGis a stratified, simply connected nilpotent Lie group with the Lie algebra g=Lr
i=1Vi satisfying [V1, Vj] = Vj+1 for all 1 ≤ j ≤ r−1. The integer r is called the step of the group G. Set nj = dimVj (1 ≤ j ≤ r). Let {X1,· · · , Xn1} be a basis
2000Mathematics Subject Classification. Primary 26D10; 22E25.
Key words and phrases. weighted Poincar´e inequalities; Carnot group; best constant.
1
of V1 and denote by ∇G = (X1,· · · , Xn1). Set ξ(1) = ξ1X1+· · ·+ξn1Xn1 and
|ξ(1)|= q
ξ12+· · ·+ξn21. To this end, we have
Theorem 1.1. Let p >1 andα≥0. IfGis a Carnot group of step 2, then for all φ∈C0∞(G), there holds
(1.2)
µn1+α p
¶pZ
G
|φ|p|ξ(1)|α≤ Z
G
|∇Gφ|p|ξ(1)|α+p and the constant
³n1+α p
´p
in (1.2) is sharp.
LetHn be the Heisenberg group whose group structure is given by (x, t)◦(x0, t0) = (x+x0, t+t0+ 2
Xn
j=1
(x2jx02j−1−x2j−1x02j)).
The vector fieldsX2j−1= ∂x∂
2j−1 + 2x2j ∂
∂t, X2j = ∂x∂
2j −2x2j−1∂
∂t, (j= 1,· · · , n) are left invariant and generate the Lie algebra of Hn. It is easy to check thatHn is a Carnot group of step two. By Theorem 1.1, we have the following corollary which improves the Theorem 1.3 in [4].
Corollary 1.2. Let p >1 andα≥0. There holds, for allφ∈C0∞(Hn), (1.3)
µ2n+α p
¶pZ
Hn
|φ|p|x|α≤ Z
Hn
|∇Hφ|p|x|α+p, where∇H= (X1,· · ·, X2n), and the constant ³
2n+α p
´p
in (1.3) is sharp.
WhenGis a Carnot group of steprwithr >2, we have the following theorem.
Theorem 1.3. Let p >1and α≥0. IfGis a Carnot group of step rwith r >2, then forα≥0andφ∈C0∞(G), there holds,
(1.4)
µn1+α p
¶pZ
G
|φ|p|ξ(1)|α≤ Z
G
|∇Gφ|p|ξ(1)|α+p. Furthermore, ifp= 2, the constant ¡n
1+α 2
¢2
in (1.4) is sharp.
Denote byEthe Engel group. Let Z1= ∂
∂x1
+x2 ∂
∂x3
+x22 ∂
∂x4
and Z2= ∂
∂x2
.
It is known that Z1 and Z2 generate the Lie algebra of Engel group E and E is a Carnot group of step 3. By Theorem 4, we have the following corollary which generalizes the inequality (1.18) of [4].
Corollary 1.4. Let α≥0. There holds, for allφ∈C0∞(E), (1.5) (1 +α)2
Z
R4
|φ|2(x21+x22)α≤ Z
R4
|∇Eφ|2(x21+x22)α+1, where∇E= (Z1, Z2), and the constant (1 +α)2 in (1.5) is sharp.
We fail to show the constant
³n1+α p
´p
in (1.4) is sharp when p 6= 2. For the reasons, see Remark 3.1.
2. Proof of Theorem 1.1
Recall that ifGis a Carnot group of step two, then there existsm×mlinearly independent skew-symmetric matricesU(1),· · · , U(n), such thatGis isomorphic to (Rm+n,◦) with the following Lie group law (x∈Rm,t∈Rn) (see A.4, [2])
(x, t)◦(x0, t0) =
µ xi+x0i, i= 1,2,· · ·, m
tj+t0j+12 < x, U(j)x0 >, j= 1,2,· · · , n
¶ .
The vector fields in the Lie algebra gof G = (Rm+n,◦) that agree at the origin with ∂x∂
j(j= 1,· · ·, m) are given by Xj= ∂
∂xj +1 2
Xn
k=1
Ãm X
i=1
Ui,j(k)xi
!
∂
∂tk, and thatgis spanned by the left-invariant vector fields
X1,· · ·, Xm, T1= ∂
∂t1,· · ·, Tn= ∂
∂tn. The Kohn’s sub-Laplacian on the groupGis given by
∆G= Xm
j=1
Xj2= Xm
j=1
Ã
∂
∂xj +1 2
Xn
k=1
Ãm X
i=1
Uj,i(k)xi
!
∂
∂tk
!2
and the corresponding horizontal gradient is them-dimensional vector given by
∇G= (X1,· · · , Xm) =∇x−1
2U(1)x ∂
∂t1
− · · · − −1
2U(n)x ∂
∂tn
. (2.1)
To finish the proof of Theorem 1.1, it is enough to show that the following inequality is held for allφ∈C0∞(Rm+n)
(2.2)
µm+α p
¶pZ
Rm+n
|φ|p|x|α≤ Z
Rm+n
|∇Gφ|p|x|α+p and the corresponding constant is sharp.
For a functionφ∈C0∞(G), we denote by φ²:= [(|φ|2+²2)p/2−²p]1p with² >0.
Then 0 ≤φ² ∈ C0∞(Rn). In fact, φ² has the same support as φ. Notice that for
|x| 6= 0,
∆G|x|α+2= Xm
j=1
µ ∂
∂xj
¶2
|x|α+2= (α+ 2)(m+α)|x|α. Integrating by parts yields
(α+ 2)(m+α) Z
Rm+n
|φ²|p|x|α= Z
Rm+n
|φ²|p∆G|x|α+2
=− Z
Rm+n
h∇G|φ²|p,∇G|x|α+2i=−p Z
Rm+n
(|φ|2+²2)p−22 φh∇Gφ,∇G|x|α+2i
≤p Z
Rm+n
(|φ|2+²2)p−22 |φ| · |∇Gφ| · |∇G|x|α+2|
≤p(α+ 2) Z
Rm+n
(|φ|2+²2)p−12 |∇Gφ||x|α+1.
Letting²→0, we obtain (m+α)
Z
Rm+n
|φ|p|x|α≤p Z
Rm+n
|φ|p−1|∇Gφ||x|α+1. By H¨older’s inequality:
(m+α) Z
Rm+n
|φ|p|x|α≤p µZ
Rm+n
|φ|p|x|α
¶p−1
p µZ
Rm+n
|∇Gφ|p|x|α+2
¶1
p
. Canceling and raising both sides to the powerp, we get (2.2).
To see the constant
³m+α p
´p
in (2.2) is sharp, we follow [9], Lemma 2.5. Choosing f(x, t) =u(|x|)g(t), whereu(|x|)∈C0∞(Rm) andg(t) =Qn
j=1wj(tj) withwj(tj)∈ C0∞(R) for all 1≤j≤n. We have, by (2.1),
|∇Gf(x, t)|2=
¯¯
¯¯
¯¯g(t)∇xu(|x|)−1 2u(|x|)
Xn
j=1
U(j)x∂g
∂tj
¯¯
¯¯
¯¯
2
=g2|∇xu(|x|)|2+1 4u2(|x|)
¯¯
¯¯
¯¯ Xn
j=1
U(j)x∂g
∂tj
¯¯
¯¯
¯¯
2
−u(|x|)g· Xn
j=1
h∇xu(|x|), U(j)xi∂g
∂tj
.
SinceU(j)((1≤j ≤n)) is a skew-symmetric matric, h∇xu(|x|), U(j)xi=u0(|x|)
¿ x
|x|, U(j)x À
= 0.
Therefore,
(2.3) |∇Gf(x, t)|2=|∇xu|2g2+1 4u2
¯¯
¯¯
¯¯ Xn
j=1
U(j)x∂g
∂tj
¯¯
¯¯
¯¯
2
.
Using the inequality (cf. [9], inequality (4))
(2.4) (s21+s22)p/2≤(1−λ)1−psp1+λ1−psp2, s1, s2>0, 0< λ <1, we have, for 0< λ <1,
R
Rm+n|∇Gf|p|x|α+p R
Rm+n|f|p|x|α ≤(1−λ)1−p R
Rm|∇u|p|x|p+αdx R
Rm|u|p|x|αdx + λ1−p2−p
R
Rm+n|u|p
¯¯
¯Pn
j=1U(j)x∂t∂g
j
¯¯
¯p|x|p+α R
Rm+n|u(|x|)|p|g|p|x|α (2.5)
Notice that there exists a positive constantCn,p, depending only onnandp, such that ¯
¯¯
¯¯
¯ Xn
j=1
U(j)x∂g
∂tj
¯¯
¯¯
¯¯
p
≤Cn,p
Xn
j=1
¯¯
¯¯U(j)x∂g
∂tj
¯¯
¯¯
p
=Cn,p
Xn
j=1
¯¯
¯U(j)x
¯¯
¯p
¯¯
¯¯∂g
∂tj
¯¯
¯¯
p
.
We have, by using (2.5) andg(t) =Qn
j=1wj(tj), R
Rm+n|∇Gf|p|x|α+p R
Rm+n|f|p|x|α ≤(1−λ)1−p R
Rm|∇u|p|x|p+αdx R
Rm|u|p|x|αdx + 2−pλ1−pCn,p
R
Rm+n|u|p³Pn
j=1
¯¯U(j)x¯
¯p¯
¯¯∂t∂g
j
¯¯
¯p
´
|x|p+α R
Rm+n|u|p|g|p|x|α
=(1−λ)1−p R
Rm|∇u|p|x|p+αdx R
Rm|u|p|x|αdx + 2−pλ1−pCn,p
Xn
j=1
R
Rm|u|p|x|p+α|U(j)x|pdx R
Rm|u(|x|)|p|x|α · R
R|w0j(tj)|pdtj
R
R|wj(tj)|pdtj
. Since
w(t)∈Cinf0∞(R)\{0}
R
R|w0(t)|pdt R
R|w(t)|pdt = 0, we obtain, for 0< λ <1,
φ∈C0∞(Rinfm+n)\{0}
R
Rm+n|∇Gφ|p|x|α+p R
Rm+n|φ|p|x|α ≤(1−λ)1−p inf
u(|x|)∈C0∞(Rm)\{0}
R
Rm|∇u|p|x|p+αdx R
Rm|u|p|x|αdx
= (1−λ)1−p
µm+α p
¶p . Here we use the fact (see e.g. [9], Theorem 2.1)
µm+α p
¶p
= inf
u(|x|)∈C0∞(Rm)\{0}
R
Rm|∇u(|x|)|p|x|p+αdx R
Rm|u(|x|)|p|x|αdx . By lettingλ→0+, we can see the constant³
m+α p
´p
is sharp.
Remark 2.1. A simple calculation shows, if|x| 6= 0, then
|∇G|x|−α+mp |p=
µm+α p
¶p
|x|−α−m−p. It looks like that|x|−α+mp can realize the sharp constant
³m+α p
´p
. However, since Z
Rm+n
||x|−α+mp |p|x|αdxdt= +∞,
inequality (1.2) is strict for everyφ6= 0. It seems that one can anticipate improving this inequality by adding some nonnegative correction term to the left-hand side of the inequality (1.2) whenRm+n is replaced by a bounded domain. We refer to [3] and [10] for more information about this subject. Moreover, in their papers, it also shows that the sharp constant appeared in this type of inequality has some applications in PDE.
We can not directly use the the family of function found in [9], Lemma 2.3. In fact, if we set
u²(x, t) =
½ 1, |x| ≤1;
|x|−α+mp −², |x| ≥1,
then Z
Rm+n
|u²(x, t)|p|x|αdxdt= Z
Rn
dt· Z
Rm
|u²(x, t)|p|x|αdx= +∞.
3. Proof of Theorem 1.3
We begin by quoting some preliminary facts which will be needed in the sequel and refer to [1, 5, 6, 8] for more precise information about Carnot group. Let G be a Carnot group with the Lie algebrag=Lr
i=1Vi satisfying [V1, Vj] =Vj+1 for all 1 ≤j ≤ r−1. As a simply connected nilpotent group, G is differential with RN,N =Pr
i=1dimVi=Pr
i=1ni, via the exponential map exp :g→G. The Haar measure on Gis induced by the exponential mapping from the Lebesgue measure ong=RN and coincides the Lebesgue measure onRN.
Consider ξ = (ξ(1),· · ·, ξ(r)) ∈ RN with ξ(i) = (ξ1(i),· · ·, ξn(i)i) ∈ Rni. Forj = 1,· · · , n1, letXj be the unique vector field ingthat coincides with∂/∂ξj(1) at the origin. The second order differential operator
∆G =−
n1
X
j=1
Xj∗Xj =
n1
X
j=1
Xj2
is called a sub-Laplacian on G. We shall denote by the ∇G = (X1,· · · , Xn1) the related subelliptic gradient. By the Campbell-Hausdorff formula (see e.g. [5], page 2-4),Xj(1≤j≤n1) can be expressed as the following
(3.1) Xj= ∂
∂ξj(1) + Xr
k=2 nk
X
s=1
pjk,s(ξ(1),· · ·, ξ(k−1)) ∂
∂ξs(k)
, wherepjk,s(ξ(1),· · ·, ξ(k−1)) is a polynomial ofξ(1),· · ·, ξ(k−1).
Now we prove inequality (1.4). The proof is similar to that given in Section 2.
Following the proof of Theorem 1.1, we also denote byφ²:= [(|φ|2+²2)p/2−²p]1p with² >0 ifφ∈C0∞(G). Since, for|ξ(1)| 6= 0,
∆G|ξ(1)|α+2=
n1
X
j=1
à ∂
∂ξ(1)j
!2
|ξ(1)|α+2= (α+ 2)(n1+α)|ξ(1)|α, we have, through integrating by parts,
(α+ 2)(n1+α) Z
G
|φ²|p|ξ(1)|α= Z
G
|φ²|p∆G|ξ(1)|α+2
=− Z
G
h∇G|φ²|p,∇G|ξ(1)|α+2i=−p Z
G
(|φ|2+²2)p−22 φh∇Gφ,∇G|ξ(1)|α+2i
≤p Z
G
(|φ|2+²2)p−22 |φ| · |∇Gφ| · |∇G|ξ(1)|α+2|
≤p(α+ 2) Z
G
(|φ|2+²2)p−12 |∇Gφ||ξ(1)|α+1. Letting²→0 yields
(n1+α) Z
G
|φ|p|ξ(1)|α≤p Z
G
|φ|p−1|∇Gφ||ξ(1)|α+1. By H¨older’s inequality:
(n1+α) Z
G
|φ|p|ξ(1)|α≤p µZ
G
|φ|p|ξ(1)|α
¶p−1
p µZ
G
|∇Gφ|p|ξ(1)|α+2
¶1
p
. Canceling and raising both sides to the powerp, we get (1.4).
Next we shall show the constant¡n
1+α 2
¢2
in (1.4) is sharp whenp= 2. Choosing f(ξ) =u(ξ(1))g(ξ(2),· · ·, ξ(r)), whereu(·)∈C0∞(Rn1) andg=Qr
k=2
Qnk
s=1wk,s(ξs(k)) with wk,s(·)∈C0∞(R) for all 2≤k ≤r and 1 ≤s ≤nl. For convenience, we set wk,s≡1 for all 1≤s≤nk ifk= 1. By (3.1),
Z
G
|∇Gf|2|ξ(1)|α+2dξ=
n1
X
j=1
Z
RN
Ã
∂u
∂ξj(1)
!2
g2|ξ(1)|α+2dξ+
Z
RN
u2
¯¯
¯¯
¯ Xr
k=2 nk
X
s=1
pjk,s ∂g
∂ξ(k)s
¯¯
¯¯
¯
2
|ξ(1)|α+2dξ+ (∗)
,
where
(∗) =2 Z
RN
u2g Xr
k=2 nk
X
s=1
pjk,s ∂g
∂ξs(k)
|ξ(1)|α+2dξ
= Xr
k=2 nk
X
s=1
Z
RN
u2pjk,s(ξ(1),· · · , ξ(k−1)) ∂g2
∂ξ(k)s
|ξ(1)|α+2dξ.
Sincewk,s(·)∈C0∞(R) for all 2≤k≤rand 1≤s≤nk, Z
R
∂w2k,s(ξ(k)s )
∂ξs(k)
dξs(k)= 0 and hence
Z
R
∂g2
∂ξs(k)
dξs(k)= 0.
Thus (∗) = 0 and Z
G
|∇Gf|2|ξ(1)|α+2dξ=
n1
X
j=1
Z
RN
Ã
∂u
∂ξj(1)
!2
g2|ξ(1)|α+2dξ+
Z
RN
u2
¯¯
¯¯
¯ Xr
k=2 nk
X
s=1
pjk,s ∂g
∂ξs(k)
¯¯
¯¯
¯
2
|ξ(1)|α+2dξ
. (3.2)
Choose a positive constantC such that
¯¯
¯¯
¯ Xr
k=2 nk
X
s=1
pjk,s ∂g
∂ξs(k)
¯¯
¯¯
¯
2
≤C Xr
k=2 nk
X
s=1
¯¯
¯¯
¯pjk,s ∂g
∂ξs(k)
¯¯
¯¯
¯
2
. We have, by (3.2),
R
G|∇Gf|2|ξ(1)|α+2dξ R
Gf2|ξ(1)|αdξ
≤ R
Rn1
Pn1
j=1
µ
∂u
∂ξj(1)
¶2
|ξ(1)|α+2dξ(1) R
Rn1u2|ξ(1)|αdξ(1) +C Xr
k=2 nk
X
s=1
R
Gu2
¯¯
¯pjk,s ∂g
∂ξ(k)s
¯¯
¯2|ξ(1)|α+2dξ R
Gf2|ξ(1)|αdξ .
Since for all 2≤k≤rand 1≤s≤nl,
wk,s∈Cinf0∞(R)\{0}
R
R|w0k,s|2dξ(k)s
R
R|wk,s|2dξ(k)s
= 0, we have
wk,s∈Cinf0∞(R)\{0}
R
Gu2
¯¯
¯pjk,s ∂g
∂ξs(k)
¯¯
¯2|ξ(1)|α+2dξ R
Gf2|ξ(1)|αdξ
= R
Rn1+···+nk−1u2|pjk,s|2Qk−1
l=1
Qnl
i=1w2l,i|ξ(1)|α+2 R
Rn1+···+nk−1u2Qk−1
l=1
Qnl
i=1w2l,i|ξ(1)|α · inf
wk,s∈C0∞(R)\{0}
R
R|wk,s0 |2dξs(k)
R
R|wk,s|2dξs(k)
= 0.
Therefore,
φ∈C0∞inf(G)\{0}
R
G|∇Gφ|p|ξ(1)|α+2 R
G|φ|p|ξ(1)|α ≤ inf
u∈C∞0 (Rn1)\{0}
R
Rn1
Pn1
j=1
µ
∂u
∂ξ(1)j
¶2
|ξ(1)|α+2dξ(1) R
Rn1u2|ξ(1)|αdξ(1)
=
µn1+α 2
¶2 .
To get the last inequality above, we use the fact (see e.g. [9], Theorem 2.1) µn1+α
2
¶2
= inf
u(x)∈C∞0 (Rn1)\{0}
R
Rn1|∇u(x)|2|x|2+αdx R
Rn1|u(|x|)|2|x|αdx . The desired result follows.
Remark 3.1. We note that the equality (2.3) play an important role in the proof of sharpness of constant
³n1+α p
´p
in (1.2) when G is a Carnot group of step 2.
However, ifG is a Carnot group of stepr with r >2, we can only obtain similar equality forp= 2 (see (3.2)). This is the reason that we can not prove the sharpness of
³n1+α p
´p
in (1.4) whenp6= 2.
Acknowledgements
The authors thanks the referee for his/her careful reading and very useful com- ments which improved the final version of this paper.
References
[1] A. Bonfiglioli, E. Lanconelli and F. Uguzzoni, Stratified Lie Groups and Potential Theory for Their Sub-Laplacians, Springer Monographs in Mathematics, Springer, Berlin, 2007.
[2] A. Bonfiglioli, F. Uguzzoni, Nonlinear Liouville theorems for some critical problems on H-type groups, J. Func. Anal. 207 (2004), 161-215.
[3] H. Brezis, J.L. V´azquez, Blow-up solutions of some nonlinear elliptic problems, Rev. Mat.
Univ. Comp. Madrid, 10 (1997), 443-469.
[4] F. Ferrari and E. Valdinoci, Some weighted Poincar´e inequalities, Indiana Univ. Math. J.
58(4)(2009), 1619-1637.
[5] Folland G.B., Stein E.M., Hardy spaces on homogeneous groups, Princeton University Press, Princeton, NJ, 1982.
[6] Mitchell, J., On Carnot-Carath´eodory metrics, J. Diff. Geom. 21 (1)(1985), 35-45.
[7] Niu P., Zhang H., Wang Y., Hardy type and Rellich type inequalities on the Heisenberg group, Proc. Amer. Math. Soc., 129(12)(2001), 3623-3630.
[8] Pansu, P.P., M´etriques de Carnot-Carath´eodory et quasiisom´etries des espaces sym´etriques de rang un, Ann. Math. 129(1989), 1-60.
[9] S. Secchi, D. Smets and M. Willem, Remarks on a Hardy-Sobolev inequality, C. R. Acad.
Sci. Paris, Ser. I, 336(2003), 811-815.
[10] J. L. Vazquez, E. Zuazua, The Hardy inequality and the asymptotic behaviour of the heat equation with an inverse-square potential, J. Funct. Anal. 173 (2000), 103-153.
[11] Wang J., Niu P., Sharp weighted Hardy type inequalities and Hardy-Sobolev type inequalities on polarizable Carnot groups, C. R. Acad. Sci. Paris, Ser. I, 346(23-24)(2008), 1231-1234.
School of Mathematics and Statistics, Xiaogan University ,Xiaogan, Hubei, 432000, People’s Republic of China
E-mail address:[email protected]