Characterizations of intrinsic rectifiability in Heisenberg groups
PERTTIMATTILA, RAULSERAPIONI AND FRANCESCOSERRACASSANO
Abstract. We define rectifiable sets in the Heisenberg groups as countable unions of Lipschitz images of subsets of a Euclidean space, in the case of low- dimensional sets, or as countable unions of subsets of intrinsicC1surfaces, in the case of low-codimensional sets. We characterize both low-dimensional rectifiable sets and low codimensional rectifiable sets with positive lower density, in terms of almost everywhere existence of approximate tangent subgroups or of tangent measures.
Mathematics Subject Classification (2010): 28A75 (primary); 28C10 (sec- ondary).
1.
Introduction
Rectifiable sets are basic concepts of geometric measure theory. They were intro- duced in the 1920’s in the plane by Besicovitch and in 1947 in general dimensions in Euclidean spaces by Federer. A systematic study of rectifiable sets in general metric spaces was made by Ambrosio and Kirchheim in [2] in 2000. However, the definitions they used are not always appropriate in Heisenberg groups, and many other Lie groups, when equipped with their natural Carnot-Carath´eodory metric;
indeed, often there are only trivial rectifiable sets of measure zero.
A different definition, in Heisenberg groups
H
n and more general Carnot groups, has been given in [14], for sets of codimension 1, and in general dimen- sions in [17, 18]. Let us sketch the inspiring ideas.According to Federer’s original definition, k-dimensional rectifiable sets are contained, up to a negligible set, in countable unions of Lipschitz images of subsets of
R
k. In Euclidean spaces, it is equivalent to use coverings with countable unions ofk-dimensionalC1sub-manifolds (see [12, 31]).The authors are supported by GALA project of the 6t h framework programme of the E.U. P.
Mattila is supported by the Academy of Finland, R. Serapioni and F. Serra Cassano are supported by University of Trento and MIUR, Italy.
Received March 2, 2009; accepted in revised form November 2, 2009.
Also in groups it is possible to follow the pattern of both definitions, provided we have good intrinsic notions of Lipschitz maps and ofC1sub-manifolds. Respec- tively we will define the classes of(k,
H
L)-rectifiable sets and of(k,H
)-rectifiable sets.Let us begin with the notion of intrinsicC1sub-manifold (see Definition 2.10).
If k is an integer, 1 ≤ k ≤ 2n, intrinsic k-dimensionalC1 sub-manifolds of
H
n (also calledH
-regular surfaces) are locally defined, if 1 ≤ k ≤ n, as images of continuously differentiable mapsR
k →H
nand, ifn+1≤k ≤2n, as non critical level sets of continuously differentiable functionsH
n→R
2n+1−k.Notice that differentiable means always Pansu differentiable (see Definition 2.5). We recall that, ifdis the distance, defined in (2.1), equivalent with the Carnot- Carath´eodory metric, and if
S
k is thek-dimensional spherical Hausdorff measure inH
n, built using the distanced, then the Hausdorff dimension ofH
n is 2n+2 and a (typical)k-dimensionalH
-regular sub-manifold has Hausdorff dimensionkm, wherekm=k, if 1≤k≤n, andkm =k+1, ifn+1≤k≤2n.Then we say that E ⊂
H
n is (k,H
)-rectifiable if there is a sequence of k- dimensionalH
-regular surfacesSi such thatS
kmE\
i
Si
=0.
We introduce also the following analogue of Federer’s Lipschitz definition. Ifkis an integer with 1≤k≤2n, we say thatE ⊂
H
nis(k,H
L)-rectifiable if there is a sequence of Lipschitz functions fi : Ai ⊂R
k →H
nsuch thatS
kmE\
i
fi(Ai)
=0.
This last definition is non trivial only if 1 ≤ k ≤ n, because, forn+1 ≤ k and f Lipschitz, always Skm(f(A)) = 0 (see [2]), hence we will consider (k,
H
L)- rectifiable sets only for 1≤k≤n.Given that the above mentioned generalization of Federer’s Lipschitz definition is not a good one for high dimensional rectifiable sets in Carnot groups, different re- lated approaches have been proposed in the literature. As an example, Pauls in [28]
considered images in
H
nof Lipschitz maps defined not onR
k but on subgroups ofH
n; in [18] a different notion of intrinsic Lipschitz sub-manifold is considered.We explicitly observe that we do not know if(k,
H
L)-rectifiability and(k,H
)- rectifiability are equivalent if 1≤k ≤n. Clearly they are not ifn+1≤k≤2n.In this paper we approach the problem of characterizing intrinsick-rectifiable sets in
H
nthrough almost everywhere existence and uniqueness of generalized tan- gent subgroups or tangent measures.We prove two main theorems. Suppose that E ⊂
H
n has locally finiteS
km measure.• The first one, Theorem 3.14, deals with the case 1≤ k ≤nand with(k,
H
L)- rectifiability. We prove that E is (k,H
L)-rectifiable if and only if it has an approximate tangent subgroup,S
kalmost everywhere. The latter means that, forS
k almost all p ∈ E, there exists a homogeneous subgroupT
p, of topological and Hausdorff dimensionk, such thatlim
r→0r−k
S
kE∩B(p,r)∩ {q :d(p−1·q,T
p) >sd(p,q)}=0 for alls>0, where the distancedis defined in (2.1) and is comparable with the Carnot-Carath´eodory distance inH
n.• The second main theorem, Theorem 3.15, deals withn+1≤k≤2nand(k,
H
)- rectifiability. We prove that E is (k,H
)-rectifiable if and only if it has,S
km almost everywhere, an approximate tangent subgroup and, additionally, positive lower density. These two conditions mean that, forS
km almost all p∈ E, there exists a homogeneous subgroupT
p, of topological dimensionkand Hausdorff dimensionkm=k+1, such thatlim
r→0r−km
S
kmE∩B(p,r)∩ {q :d(p−1·q,T
p) >sd(p,q)}=0 for alls >0, andlim inf
r→0 r−km
S
km(E∩B(p,r)) >0.We do not know if the assumption of positive lower density is necessary.
In both cases, we shall also give other equivalent conditions in terms of weak con- vergence of blow-ups and existence of tangent measures. One of these, condi- tion (v) of Theorem 3.15, says that E, with positive density as above, is (k,
H
)- rectifiable if and only if forS
km-a.e. p∈ Ethere is a non-trivial Radon measureλpsuch that every tangent measure at pof the restriction
S
km Eis a constant multi- ple ofλp. More informally, this means that, at all sufficiently small scales around p,S
km E looks, suitably magnified, likeλp. Note that this condition does not refer to any particular kind of subgroups, parametrizations or concepts of differen- tiability, whence its equivalence to rectifiability in a way indicates that the concept of intrinsic rectifiability we are using is a natural one.Notice that Ambrosio and Kirchheim’s definition in general metric spaces, when specialized to Heisenberg groups, coincides with(k,
H
L)-rectifiability. They also have a characterization of rectifiability, under the assumption of positive lower density, in terms of approximate tangent planes. Their approach to the notion of (approximate) tangent space is different from ours. Indeed they imbed their metric space into a Banach space and use the linear structure there. However, eventually, the two notions coincide.Notice that we use the spherical Hausdorff measure
S
m instead of the usual Hausdorff measureH
mbecause the blow-up Theorem 3.4 is only known for it andhence we can get the conditions (ii) and (iv), of both main theorems, only for the spherical Hausdorff measure. As
S
m andH
m have the same null-sets, and evenH
m(A) ≤S
m(A) ≤ 2mH
m(A)for all A ⊂H
n, the rectifiable sets are the same for both measures and the equivalence of the conditions (i), (iii) and (v) in Theo- rem 3.14 and 3.15 holds also forH
m.In [14,15],(2n,
H
)-rectifiable sets were used to establish De Giorgi’s structure theory for sets of finite perimeter in step 2 Carnot groups, see also [3] for more gen- eral Carnot groups. In Euclidean spaces, rectifiable sets have been fundamental in many aspects of geometric calculus of variations, in particular for minimal surfaces of general dimensions. Problems of existence and regularity of minimal surfaces in Heisenberg groups have recently been considered by many people and it could be expected that rectifiable sets would play a significant role also here. See also, for a different application, the recent [10].Finally we thank the referee for his careful reading of this paper.
2.
Heisenberg groups
2.1. Algebraic and metric structure of
H
nFor a general review on Carnot groups, and in particular on Heisenberg groups, we refer to [8, 9, 19, 32] and to [33]. We limit ourselves to fix some notations.
H
nis the n-dimensional Heisenberg group, identified withR
2n+1through ex- ponential coordinates. A point p ∈H
n is denoted p = (p1, . . . ,p2n,p2n+1) = (p,p2n+1), with p ∈R
2nand p2n+1∈R
. If pandq ∈H
n, the group operation is defined asp·q:=
p+q,p2n+1+q2n+1−2 n i=1
(piqi+n− pi+nqi)
. The inverse of pis p−1:=(−p,−p2n+1)ande=0 is the identity of
H
n.The centre of
H
nis the subgroupT
:= {p=(0, . . . ,0,p2n+1)}.For anyq ∈
H
n andr > 0, we denote asτq :H
n →H
n the left translation p→q· p=τq(p)and asδr :H
n→H
nthe dilationp→(r p,r2p2n+1)=δrp. Notice that dilations are also automorphisms of
H
n.We denote, for all p,q∈
H
n,p :=d(p,e):=max{(p1,· · · ,p2n)R2n,|p2n+1|1/2} and
d(p,q)=d(q−1· p,e)= q−1· p. (2.1)
Then, for all p,q,z∈
H
n and for allr >0,d(z· p,z·q)=d(p,q) and d(δrp, δrq)=r d(p,q).
Finally,U(p,r)andB(p,r)are the open and the closed ball associated withd.
The standard basis of the Lie algebra
h
ofH
nis given byXi :=∂i +2xi+n∂2n+1, Yi :=∂i+n−2xi∂2n+1, T :=∂2n+1,
for i = 1, . . . ,n. The horizontal subspace
h
1 is the subspace ofh
spanned by X1, . . . ,Xn andY1, . . . ,Yn. Denoting byh
2the linear span ofT, the 2-step strati- fication ofh
is expressed ash
=h
1⊕h
2.The Lie algebra
h
is endowed with the scalar product·,·, that makesX1, ...,Yn,T orthonormal, and by the induced norm · .The vector fieldsX1, . . . ,Xn,Y1, . . . ,Yndefine a vector subbundle of the tan- gent vector bundle T
H
n, the so called horizontal vector bundle HH
n– according to the notation of Gromov, (see [19] and [26]). We identify sections φof HH
n, us- ing coordinates with respect to the moving frame X1, . . . ,Yn, with functionsφ = (φ1, . . . , φ2n):H
n →R
2n. We will also identify sectionsφ : ⊂H
n → HH
n with the mapφ:→h
1defined asφ(p)=n
j=1
φj(p)Xj +φn+j(p)Yj.
We denote byπ :
H
n →h
1the map defined as π(p):=n j=1
pjXj +pn+jYj
. (2.2)
Remark 2.1. Because the topologies defined byd and by the Euclidean distance coincide, the topological dimension of
H
n is 2n +1. Moreover d is bilipschitz equivalent to the Carnot-Carath´eodory metricdc induced by the horizontal sub- bundle HH
n(see [19, 26]).The (2n+1)-dimensional Lebesgue measure
L
2n+1 onH
n ≡R
2n+1 is left (and right) invariant and it is a Haar measure of the group.Form≥0, we denote by
S
mthem-dimensional spherical Hausdorff measure, obtained from the distanced following Carath´edory’s construction as in [12, Sec- tion 2.10.2].ForA⊂
H
nandδ >0,S
m(A)=limδ→0S
δm(A), whereS
δm(A)=infi
αmrim : A⊂
i
B(pi,ri),ri ≤δ
.
We have to be precise about the constants αm appearing in this definition. We will define αm only form integer, 0 ≤ m ≤ 2n +2 and m = n+1. Indeed explicit computations will be carried out only in these cases, because, as observed in the introduction, k-dimensional C1 (or Lipschitz) submanifolds have intrinsic Hausdorff dimensionkif 1≤k ≤nand Hausdorff dimensionk+1 ifn+1≤k ≤ 2n+1.
Hence, ifωm is the
L
m measure of the unit Euclidean ball Bm,eucinR
m, we defineαm:= ωm if 1≤m≤n,
2ωm−2 ifn+2≤m ≤2n+2. (2.3) With this choice, the
S
mmeasure restricted to homogeneous subgroups ofG
(H
n) (see Definition 2.16) coincides with the appropriate Lebesgue measure. The precise statement is in Proposition 2.20.Translation invariance and homogeneity under dilations of Hausdorff measures follow as usual. For allA⊆
H
n, for all p∈H
n,r ∈(0,∞)and 1≤m≤2n+2S
m(τpA)=S
m(A),S
m(δr(A))=rmS
m(A). (2.4) Finally we denote byH
eucm the m-dimensional Hausdorff measure related to the Euclidean distance inR
2n+1.2.2. Function spaces
Ifis an open subset of
H
n ≡R
2n+1andk ≥0 is a non negative integer,Ck() indicates the usual space of real valued functions which arek times continuously differentiable in the Euclidean sense. We denote by Ck(,HH
n) the set of all Ck-sections of HH
n where theCk regularity is understood as regularity between smooth manifolds.Definition 2.2. Ifis an open subset of
H
n and f ∈ C1()we define thehori- zontal gradientof f as∇Hf :=(X1f, . . . ,Xnf,Y1f, . . . ,Ynf) . (2.5) Alternatively∇Hf can be defined as the section of H
H
n∇Hf :=
n j=1
(Xjf)Xj +(Yj f)Yj
whose canonical coordinates are(X1f, . . . ,Xnf,Y1f, . . . ,Ynf).
Definition 2.3. We say that f :
H
n →R
isdifferentiable along Xj(or along Yj)at p0if the mapr → f(p0·δrej)(respectively:r → f(p0·δrej+n)) is differentiable atr =0. Hereek is thek-th vector of the canonical basis ofR
2n+1.Clearly, if f ∈ C1() then f is differentiable along Xj and Yj, for j = 1, . . . ,n, at all points ofand
df
dr(p0·δrej)
r=0= Xjf(p0) , df
dr (p0·δrej+n)
r=0=Yj f(p0) for all p0∈. Hence, if f is differentiable alongXj’s andYj’s atp0and we define the horizontal gradient to be
∇Hf(p0):=
n j=1
Xj f(p0)Xj + n
j=1
Yj f(p0)Yj (2.6) then this definition naturally extends the one given in (2.5).
Definition 2.4. If
U
⊂H
n, we denote byC1H(U
)the set of continuous real valued functions inU
such that∇Hf exists and is continuous inU
;[C1H(U
)]k is the set of k-tuples f =(f1,· · ·, fk)such that each fi ∈C1H(U
)for 1≤i ≤k.Notice thatC1()⊂C1H(), and the inclusion is strict (see [14, Remark 5.9]).
The following definition of differentiability, for functions acting between Carnot groups, was given by Pansu in [27].
Definition 2.5. Let(
G
1,d1)and(G
2,d2)be Carnot groups andA
⊂G
1. A func- tion f :A
→G
2 is Pansu differentiable in g ∈A
if there is a homogeneous homomorphism Lg:G
1→G
2such thatd2
f(g)−1· f(g),Lg(g−1·g)
d1(g,g) →0, asd1(g,g)→0,g∈
A
. The homogeneous homomorphism Lg is denoted dHfg and is called the Pansu differentialof f ing.Pansu obtained, in [27], a Rademacher type theorem for Lipschitz functions acting between Carnot groups proving that they are almost everywhere differen- tiable, in the sense of Definition 2.5. We shall use the following case of Pansu’s theorem, (see [21, Theorem 3.4.11]).
Theorem 2.6. Let A ⊂
R
m be anL
m measurable set and f :A
→H
n be a Lipschitz map. Then f is Pansu differentiableL
m-a.e. inA
.The functions ofC1H()are differentiable in Pansu’s sense (see [27] and [14]) and the Pansu differentialdHf is represented by the horizontal gradient∇Hf. Proposition 2.7. With the notations of Definition 2.3, f ∈C1H()if and only if its distributional derivatives Xi f , Yif (i =1, . . . ,n) are continuous in.
Moreover, if f ∈C1H(), then for all p,p0∈
f(p)= f(p0)+dHfp0(p−01· p)+o(d(p,p0)), as p→ p0. (2.7)
We mention also the following ‘converse’ result to Theorem 2.6.
Proposition 2.8. Let1≤d ≤n. If f :
A
⊂R
d →H
nis Pansu differentiable in x0then f is also Euclidean differentiable in x0andf(x0)·dHfx0(
R
d)= f(x0)+d fx0(R
d).Proof. By the contact property of H-linear maps (see [21] or [17]) we know that L :=dH fx0 is a classical linear map from
R
d toR
2n+1andL(v)=(Av,0)where Ais a suitable 2n×dmatrix. Then, for the first 2ncomponents f1, . . . , f2nof f, Pansu differentiability coincides with Euclidean differentiability so thatA=
∇f1(x0)
∇f2n...(x0)
while a not difficult computation yields
∇f2n+1(x0)=2 n
j=1
fj+n(x0)∇fj(x0)− fj(x0)∇fj+n(x0) .
It follows that, for allv∈
R
d,f(x0)·dHfx0(v)= f(x0)+d fx0(v) and the proof is completed.
We conclude this section mentioning the following Whitney’s extension theo- rem (see [14]).
Theorem 2.9. Let F ⊂
H
n be a closed set, f : F →R
, k : F → HH
n be continuous functions. DefineR(p,p):= f(p)− f(p)− k(p), π(p−1·p) d(p,p) , and, if K ⊂ F is a compact set,
ρK(δ):=sup{|R(p,p)| : p,p∈K, 0<d(p,p) < δ}.
IfρK(δ)→0asδ→0for every compact set K ⊂ F , then there exists f˜:
H
n →R
, f˜∈C1H(H
n), such thatf˜|F = f and ∇Hf˜|F =k. 2.3.
H
-regular surfacesH
-regular surfaces are the intrinsicC1embedded submanifolds inH
n. A systematic study ofH
-regular surfaces has been recently carried out in [4, 5, 11, 17]. Let us begin with the definition.Definition 2.10. S⊂
H
nis ad-dimensionalH
-regular surfacewhen the following is true(i) for 1≤d≤n
for any p∈Sthere are open sets
U
⊂H
n,V
⊂R
d and a functionϕ:V
→U
such that p ∈U
, ϕ is injective, and continuously Pansu differentiable with dHϕpinjective, andS∩
U
=ϕ(V
);(ii) forn+1≤d≤2n
for any p∈Sthere are an open set
U
⊂H
nand a function f :U
→R
2n+1−d such that p ∈U
, f ∈ [C1H(U
)]2n+1−d, withdH fq surjective for everyq ∈U
andS∩
U
= {q∈U
: f(q)=0}.In this second case, sometimes we speak of(2n+1−d)-codimensional
H
-regular surfaces.These notions of
H
-regular submanifolds are different from the corresponding Euclidean ones and from each other. Indeed d-dimensionalH
-regular submani- folds, 1 ≤ d ≤ n, are a subclass ofd-dimensional Euclidean C1 submanifolds ofR
2n+1 (see [17]). On the contrary, k-codimensional H-regular submanifolds, 1≤k≤n, can be very irregular objects from a Euclidean point of view. An exam- ple of a 1-codimensional H-regular surface inH
1≡R
3, with fractional Euclidean dimension equal to 2.5, is provided in [20]. On the other side, the horizontal plane {p: p2n+1=0} =exph
1is Euclidean regular but not intrinsic regular at the origin.Nevertheless,
H
-regular surfaces share several properties with the Euclidean regu- lar ones. To see this let us first introduce the notion ofintrinsic tangent subgroupto anH
-regular surface.Definition 2.11. LetSbe ad-dimensional
H
-regular surface inH
nandϕand f as in Definition 2.10. Thetangent grouptoSin p0 ∈ S, denoted asTHS(p0), is the homogeneous subgroup ofH
n defined,(i) for 1≤d≤n, as
THS(p0):= {dHϕx0(x):x∈
R
d}, whereϕ(x0)= p0. (ii) forn+1≤d≤2n, asTHS(p0):= {p∈
H
n:dHfp0(p)=0}.Remark 2.12. If 1≤d ≤nand ifSis a
H
-regulard-dimensional surface, then, for all p ∈ S,THS(p)is ad-dimensional subgroup contained in HH
n. Moreover the Euclidean tangent plane toSinpcoincides withTHS(p)(see [17, Theorem 3.5]). If n+1≤d≤2nand ifSis anH
-regulard-surface, thenTHS(p)is ad-dimensional subgroup containing the centreT
ofH
n(see [17]). Finally, it follows, from the very Definition 2.10, that Sis ak-codimensionalH
-regular surface, 1≤ k < n, if and only ifSis, locally, the intersection ofk1-codimensionalH
-regular hypersurfaces, with linearly independent normal vectors.2.4. The intrinsic Grassmannian
A subgroup
G
ofH
nis ahomogeneous subgroupif δrg∈G
,for all g∈
G
and for allr > 0. Notice that, through the identification ofH
n withR
2n+1, homogeneous subgroups ofH
n are vector subspaces ofR
2n+1. Homoge- neous subgroups either are contained in the horizontal plane exph
1, and are then calledhorizontal, or they contain the centreT
ofH
n, and are calledvertical. Hor- izontal subgroups are commutative while vertical subgroups are non-commutative normal subgroups ofH
n.We use the symbol dim
G
to indicate the ‘linear’ dimension of the subgroupG
,i.e. the dimension of its Lie algebra, and the symbol dimHG
for its Hausdorff dimension, with respect to the metric d, defined in (2.1). It follows from a gen- eral result of Mitchell (see [25]), and also from direct verification in this case, that dimHV
=dimV
, ifV
is a horizontal subgroup, and that dimHW
=dimW
+1, ifW
is a vertical subgroup.In the following we will refer to homogeneous subgroups
G
of linear dimen- siondasd-subgroups and we will denote asdmthe metric dimension ofG
. Definition 2.13. Two homogeneous subgroupsV
andW
ofH
narecomplementary subgroupsinH
n, ifW
∩V
= {e}and if, for all p ∈H
n, there arew ∈W
and v∈V
such that p=w·v. IfW
andV
are complementary subgroups, we say thatH
nis the product ofW
andV
and we writeH
n =W
·V
,Remark 2.14. In
H
n one of two complementary subgroups, is always a normal subgroup and the other one a horizontal subgroup. Hence the productH
n=W
·V
in Definition 2.13, is always asemidirect product(see Proposition 2.17). We will use the symbolW
for normal subgroups and the symbolV
for the horizontal ones.Proposition 2.15. If
H
n =W
·V
is as above, withV
horizontal andW
vertical, each p∈H
nhas uniquecomponents pW ∈W
, pV ∈V
, such thatp= pW· pV.
For all p,q∈
H
nandλ >0, pW and pVdepend continuously on p and,(p−1)W =(pV)−1·(pW)−1· pV, (p−1)V=(pV)−1 (2.8) (δλp)W =δλpW, (p·q)W = pW· pV·qW· p−V1
(δλp)V =δλpV, (p·q)V = pV·qV, (2.9) hence, in particular, the map p →pV, from
H
ntoV
, is a homogeneous homomor- phism.There is a constant c=c(
W
,V
) >0such that, for all p∈H
n, c(pW + pV)≤ p ≤ pW + pV, cp−V1· pW· pV + pV
≤ p ≤ p−V1·pW· pV + pV. (2.10) and consequently
cpV ≤d(p,
W
)≤ pV,cp−V1·pW· pV ≤d(p,
V
)≤ pV−1· pW· pV. (2.11) Proof. Uniqueness, continuity, (2.8) and (2.9) are trivial. Then (2.10) follows from triangular inequality and by a compactness argument, observing also that p= pW·pV = pV·(pV)−1· pW·pV. Because
d(p,
W
)=inf{d(p, w):w∈W
} =inf{w−1·p :w∈W
}, we get, from (2.10),d(p,
W
)=inf{w−1· pW ·pV :w∈W
} ≤ pV and, on the other side,w−1· pW· pV ≥c(w−1·pW + pV)≥cpV that gives the first one of (2.11).
Once more from (2.10),
d(p,
V
)=inf{p−1·v :v∈V
}=inf{(pV)−1·(pW)−1·pV·(pV)−1·v :v∈
V
}≥cinf{(pV)−1·(pW)−1·pV + (pV)−1·v :v∈
V
}=cpV−1·(pW)−1·pV
=cpV−1· pW· pV.
The estimate from above is obtained in the same way.
Definition 2.16. Letd be a non negative integer. We denote by
H
(H
n,d,dm)the set of alld-subgroups ofH
nwith metric dimensiondmand byH
(H
n)the family of all homogeneous subgroups. Ad-subgroupG
belongs to the intrinsic Grassman- nian of the d-subgroupsG
(H
n,d), if there is a(2n+1−d)-subgroupH
such thatH
n =G
·H
, that isG
(H
n,d):=
G
:G
is a d-subgroup andH
n=G
·H
for a(2n+1−d)-subgroupH
.
Theintrinsic Grassmannianis defined as
G
(H
n)=2n+1 d=0
G
(H
n,d).Proposition 2.17. The trivial subgroups {e}and
H
n are the unique elements of, respectively,G
(H
n,0)andG
(H
n,2n+1). Moreover,(i) for 1 ≤ d ≤ n,
G
(H
n,d) =H
(H
n,d,d), the set of all horizontal homoge- neous d-subgroups;(ii) for n+1≤d ≤2n,
G
(H
n,d)=H
(H
n,d,d+1)coincides with the set of all vertical homogeneous d-subgroups.On the contrary, a vertical subgroup
W
with1≤ dimW
≤n is not inG
(H
n). In particular, the1-subgroupT
is not inG
(H
n).Proof. In all the possible splittings of
H
nas semidirect product of two subgroups,H
n =W
·V
, one of the two subgroups, sayV
, is horizontal and the other one,W
, containsT
. In terms of Lie algebras, settingv
andw
the Lie algebras ofV
andW
, we have thath
=v
⊕w
,v
andw
are subalgebras ofh
and,V
being horizontal,v
is commutative.Hence 0 ≤dim
V
≤nbecause inh
there are at mostnlinearly independent, commuting horizontal vector fields. Consequently,n<dimW
=2n+1−dimV
<2n+1. This shows that vertical subgroups of linear dimension not exceedingncan never be a factor of a splitting of
H
n.If L is any vector subspace of
h
1 then span{L,T} is a subalgebra ofh
and exp{span{L,T}}is a vertical subgroup ofH
n. It follows that all the horizontal subgroups are inG
(H
n). Indeed, given a horizontal subgroupV
, its Lie algebrav
is a vector subspace ofh
1. LetLbe any complementary vector subspace ofv
inh
1and define
W
:=exp{span{L,T}}. ThenH
nis the semidirect product ofV
andW
, so thatV
∈G
(H
n).On the other side, if
W
is a vertical subgroup of dimension larger thannit is proved in Lemma 3.26 of [17] that a complementary horizontal subgroupV
exists such thatH
nis the direct product ofW
andV
.Remark 2.18.
G
(H
n)andH
(H
n)are, in a natural way, subsets of the Euclidean GrassmannianG
(R
2n+1)and are endowed with the same topology. Moreover no- tice thatG
(H
n,d)andH
(H
n,d,dm)are compact metric spaces with respect to the distanceρ(
G
1,G
2):=dH ausG
1∩B(e,1),G
2∩B(e,1), (2.12) wheredH ausis the Hausdorff distance induced by the distanced.Remark 2.19. If Sis ad-dimensional
H
-regular surface and p∈Sthen THS(p)∈G
(H
n,d).Proposition 2.20. Let
G
∈H
(H
n,d,dm). ThenH
deucG
, is a left Haar measure ofG
andH
deucG
=S
dmG
, wheredm=d if
G
is a horizontal subgroup, dm=d+1 ifG
is a vertical subgroup.In particular, if
G
∈G
(H
n,d)then dimHG
=dm, where dm =d if1≤d ≤n,(2.13) dm =d+1 if n+1≤d≤2n.
Proof. It is known, and can be checked by direct computation (seee.g.[13]), that the Lebesgue measure
L
d is a, left and right invariant, Haar measure onG
. More- over, for all Borel setsA
⊂G
andr >0,L
d(δrA
)=rdmL
d(A
) andL
dG
=H
eucdG
. Notice also that, ifG
is horizontal, thenB(e,1)∩
G
= Bdm,eucand, if
G
is vertical, thenB(e,1)∩
G
=(B2n,euc× [−1,1])∩G
= Bdm−2,euc× [−1,1].In the preceding lines we have identified
G
, respectively, withR
d or withR
d ×R
whileBm,eucdenotes the unit closed ball inR
m. Now, letA
be a fixed Borel set and let p∈A
∩G
. Then, taking into account (2.3),H
deucB(p,r)∩
G
=L
dB(p,r)∩G
=rdmL
dB(e,1)∩G
=rdm
H
deucB(e,1)∩
G
=αdmrdm. Then by [12, 2.10.17(2) and 2.10.19(3)]H
deucG
∩A
=S
dmG
∩A
and the thesis follows.
We say that two homogeneous subgroups are orthogonal if their subalgebras are orthogonal vector subspaces in
h
.Remark 2.21. If 1 ≤ d ≤ n and
V
∈G
(H
n,d), there is a unique subgroupV
⊥ ∈G
(H
n,2n+1−d)that is orthogonal toV
. ThenV
,V
⊥are complementary subgroups and we define the projectionsPV :
H
n →V
andPV⊥ :H
n →V
⊥,where, for all p∈
H
n,PV(p)is theV
-component ofpin the decompositionV
,V
⊥ ofH
nand analogously forPV⊥(p).As observed in Proposition 2.15, the functionPVis a homogeneous homomor- phism and we can also state differently Proposition 2.15.
Proposition 2.22. Let
V
∈G
(H
n,d), with1≤d≤n. Then there is c1=c1(d) >0such that (2.10)holds with c = c1 and pV = PV(p), pW = PV⊥(p). Conse- quently,(2.11)becomes
c1PV(p) ≤d(p,
V
⊥)≤ PV(p)c1PV(p)−1·PV⊥(p)·PV(p) ≤d(p,
V
)≤ PV(p)−1· PV⊥(p)·PV(p), (2.14) for all p ∈H
n.Proof. We have to check only that, if
W
isV
⊥, the constant in (2.10) depends only ond. Indeed, by rotation, we can assume thatV
= {(v1, . . . , vd,0, . . . ,0)}hence
W
=V
⊥ = {(0, . . . ,0, wd+1, . . . , w2n+1)}and the compactness argument gives a constant depending only ond. Finally, (2.14) follows by the same proof giving (2.11) from (2.10).
Lemma 2.23. Let
V
∈G
(H
n,d), with 1 ≤ d ≤ n. Then there are s = s(d) ∈ (0,1)andη=η(s) >0such that the following holds:d(p−1·q,
V
) <s d(p,q) =⇒ dPV(p),PV(q)> ηd(p,q) (2.15) whenever p,q∈
H
n.Proof. Without loss of generality, we can assumep=e. Indeed, from (2.9), PV(p−1·q)= PV(p)−1·PV(q).
Hence (2.15) is equivalent to
d(q,