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. 2022 Jul 18;32(9):239. doi: 10.1007/s12220-022-00971-7

On Rectifiable Measures in Carnot Groups: Existence of Density

Gioacchino Antonelli 1,, Andrea Merlo 2
PMCID: PMC9293879  PMID: 35874859

Abstract

In this paper, we start a detailed study of a new notion of rectifiability in Carnot groups: we say that a Radon measure is Ph-rectifiable, for hN, if it has positive h-lower density and finite h-upper density almost everywhere, and, at almost every point, it admits a unique tangent measure up to multiples. First, we compare Ph-rectifiability with other notions of rectifiability previously known in the literature in the setting of Carnot groups, and we prove that it is strictly weaker than them. Second, we prove several structure properties of Ph-rectifiable measures. Namely, we prove that the support of a Ph-rectifiable measure is almost everywhere covered by sets satisfying a cone-like property, and in the particular case of Ph-rectifiable measures with complemented tangents, we show that they are supported on the union of intrinsically Lipschitz and differentiable graphs. Such a covering property is used to prove the main result of this paper: we show that a Ph-rectifiable measure has almost everywhere positive and finite h-density whenever the tangents admit at least one complementary subgroup.

Keywords: Carnot groups, Rectifiability, Rectifiable measure, Density, Intrinsic Lipschitz graph, Intrinsic differentiable graph

Introduction

In Euclidean spaces, a Radon measure ϕ is said to be k-rectifiable if it is absolutely continuous with respect to the k-dimensional Hausdorff measure Hk and it is supported on a countable union of k-dimensional Lipschitz surfaces, for a reference see [13, §3.2.14]. This notion of regularity for a measure is an established, thoroughly studied, and well-understood concept and its versatility is twofold. On the one hand, it can be effortlessly extended to general metric spaces. On the other hand, it can be shown, at least in Euclidean spaces, that the global regularity properties arise as a consequence of the local structure of the measure, as it is clear from the following classical proposition, see, e.g., [36, Theorem 16.7].

Proposition 1.1

Assume ϕ is a Radon measure on Rn and k is a natural number such that 1kn. Then, ϕ is a k-rectifiable measure if and only if for ϕ-almost every xRn we have

  • (i)

    0<Θk(ϕ,x)Θk,(ϕ,x)<+,

  • (ii)

    Tank(ϕ,x){λHkV:λ>0,andVis ak-dimensional vector subspace},

where Θk(ϕ,x) and Θk,(ϕ,x) are, respectively, the lower and the upper k-density of ϕ at x, see Definition 2.8, and Tank(ϕ,x) is the set of k-tangent measures to ϕ at x, see Definition 2.7, while Hk is the Hausdorff measure.

As mentioned above, one can define rectifiable measures in arbitrary metric spaces: however, one quickly understands that there are some limitations to what the classical rectifiability can achieve.

The first example of this is the curve in L1([0,1]) that at each t[0,1] assigns the indicator function of the interval [0, t]. This curve is Lipschitz continuous; however, it fails to be Fréchet differentiable at every point of [0, 1], thus not admitting a tangent. This shows that we cannot expect anything like Proposition 1.1 to hold in infinite dimension.

For the second example, we need to briefly introduce Carnot groups, see Sect. 2 for details. A Carnot group G is a simply connected nilpotent Lie group, whose Lie algebra is stratified and generated by its first layer. Carnot groups are a generalization of Euclidean spaces, and we remark that (quotients of) Carnot groups arise as the infinitesimal models of sub-Riemannian manifolds and their geometry, even at an infinitesimal scale, might be very different from the Euclidean one. We endow G with an arbitrary left-invariant homogeneous distance d, and we recall that any two of them are bi-Lipschitz equivalent. These groups have finite Hausdorff dimension, that is commonly denoted by Q, and any Lipschitz map f:RQ-1(G,d) has HQ-1-null image, unless G is an Euclidean space, see for instance [2] and [35, Theorem 1.1]. This from an Euclidean perspective means that there are no Lipschitz-regular parametrized one-codimensional surfaces inside (G,d), unless G is an Euclidean space. However, as shown in the foundational papers [19, 20], in Carnot groups there is a well-defined notion of finite perimeter set and in Carnot groups of step 2 their reduced boundary can be covered up to HQ-1-negligible sets by countably many intrinsic C1-regular hypersurfaces, CH1 hypersurfaces from now on, see [20, Definition 6.4]. The success of the approach attempted in [20] has started an effort to study Geometric Measure Theory in sub-Riemannian Carnot groups, and in particular to study various notion(s) of rectifiability, see, e.g., [10, 11, 14, 1719, 21, 22, 2426, 31, 32, 3941]. The big effort represented by the aforementioned papers in trying to understand rectifiability in Carnot groups has given rise to a multiplication of definitions, each one suiting some particular cases.

As we shall see in the subsequent paragraphs, not only one could consider our approach reversed with respect to the ones known in the literature but it also has a twofold advantage. On the one hand, the definition of P-rectifiable measure is natural and intrinsic with respect to the (homogeneous) structure of Carnot groups and it is equivalent to the usual one in the Euclidean setting; on the other hand, we do not have to handle the problem of distinguishing, in the definition, between the low-dimensional and the low-codimensional rectifiability.

Nevertheless, for arbitrary Carnot groups, we prove non-trivial structure results for rectifiable measures, see Sect. 1.2. These structure results will be used to prove the main Theorem of this paper, see Theorem 1.3. Moreover, the study of the structure properties proved in Sect. 1.2 is completed in the subsequent paper [6].

In a companion paper [5], which roughly corresponds to an elaboration of Sect. 5 of the second version in the arXiv submission of the Preprint [7], we shall prove a Marstrand–Mattila type rectifiability criterion for P-rectifiable measures that in turn will lead to the proof of the one-dimensional Preiss’s theorem for the first Heisenberg group H1 endowed with the Koranyi distance.

Additional remark. The present work consists of an elaboration of Sects. 2, 3, 4, and 6 of the second version in the arXiv submission of the Preprint [7]. This is the first of two companion papers derived from [7]. The second one is an elaboration of Sects. 2, and 5 of [7]. We stress that the results in Sects. 2, 3, 4, and 6 of [7] do not use the results in Sect. 5 of [7]. As a result this paper can be read fully and independently from its companion paper.

P-Rectifiable Measures

In this paper, we study structure results in the class of P-rectifiable measures, which have been introduced in [41, Definition 3.1 & Definition 3.2]. Let G be a Carnot group of Hausdorff dimension Q.

Definition 1.1

(P-rectifiable measures) Let 1hQ be a natural number. A Radon measure ϕ on G is said to be Ph-rectifiable if for ϕ-almost every xG we have

  • (i)

    0<Θh(ϕ,x)Θh,(ϕ,x)<+,

  • (ii)

    Tanh(ϕ,x){λShV(x):λ0}, where V(x) is a homogeneous subgroup of G of Hausdorff dimension h,

where Θh(ϕ,x) and Θh,(ϕ,x) are, respectively, the lower and the upper h-density of ϕ at x, see Definition 2.8, Tanh(ϕ,x) is the set of h-tangent measures to ϕ at x, see Definition 2.7, and Sh is the spherical Hausdorff measure of dimension h, see Definition 2.4. Furthermore, we say that ϕ is Ph-rectifiable if (ii) is replaced with the weaker

(ii)Tanh(ϕ,x){λShV:λ0,Vis a homogeneous subgroup ofGof Hausdorff dimension h}.

If we impose more regularity on the tangents, we can define different subclasses of P-rectifiable or P-rectifiable measures, see Definition 2.19 for details. We notice that, a posteriori, in the aforementioned definitions, we can and will restrict to λ>0, see Remark 2.5.

The definition of P-rectifiable measure is natural in the setting of Carnot groups. Indeed, we have on G a family of dilations {δλ}λ>0, see Sect. 2, that we can use to give a good definition of blow-up of a measure. Hence we ask, for a measure to be rectifiable, that the tangents are flat. The natural class of flat spaces, i.e., the analogous of vector subspaces of the Euclidean space, seems to be the class of homogeneous subgroups of G. This latter assertion is suggested also from the result in [37, Theorem 3.2] according to which on every locally compact group G endowed with dilations and isometric left translations, if a Radon measure μ has a unique (up to multiplicative constants) tangent μ-almost everywhere then this tangent is μ-almost everywhere (up to multiplicative constants), the left Haar measure on a closed dilation-invariant subgroup of G. As a consequence, in the definition of Ph-rectifiable measure, we can equivalently substitute item (ii) of Definition 1.1 with the weaker requirement

(ii)Tanh(ϕ,x){λνx:λ>0},whereνxis a Radon measure onG.

Moreover, we stress that if a metric group is locally compact, isometrically homogeneous and admits one dilation, as it is for the class of metric group studied in [37], and moreover the distance is geodesic, then it is a sub-Finsler Carnot group, see [28, Theorem 1.1].

As already mentioned, according to one of the approaches to rectifiability in Carnot groups, the good parametrizing objects for the notion of rectifiability are CH1-regular surfaces with complemented tangents in G, i.e., sets that are locally the zero-level sets of CH1 functions f - see Definition 5.1 - with surjective Pansu differential df, and such that Ker(df) admits a complementary subgroup in G. This approach has been taken to its utmost level of generality through the works [25, 32, 34]. In particular, in [25, Definition 2.18], the authors give the most general, and available up to now, definition of (G,G)-rectifiable sets, see Definition 5.2 and Definition 5.3, and they prove area and coarea formulae within this class of rectifiable sets. We stress that an improvement of the area formula in [25] is obtained by the two authors of this work in [6, Theorem 1.3]. Related results are in [8].

We remark that our definition of rectifiability is strictly weaker than the one in [25], see Proposition 5.2 and Remark 5.2. Moreover for discussions on the converse of the following Proposition 1.2 we refer the reader to Remark 5.3. We stress that, as a result of the subsequent work [6, Corollary 5.3], at least in the co-horizontal setting, the notion of P-rectifiable measure and the notion of rectifiability given in terms of (G,G)-rectifiable sets coincide.

Proposition 1.2

Let us fix G and G two arbitrary Carnot groups of homogeneous dimensions Q and Q, respectively. Let us take ΣG a (G,G)-rectifiable set. Then SQ-QΣ is a PQ-Q-rectifiable measure with complemented tangents. Moreover, there exists G a Carnot group, ΣG, and 1hQ such that ShΣ is a Ph-rectifiable measure and, for every Carnot group G, Σ is not (G,G)-rectifiable.

Let us stress that the second part of Proposition 1.2 is not surprising. Indeed, the approach to rectifiability described above and used in [25] is selecting rectifiable sets whose tangents are complemented normal subgroups of G, see [25, Sect. 2.5] for a more detailed discussion. This can be easily understood if one thinks that, according to this approach to rectifiability, the parametrizing class of objects is given by CH1-regular surfaces Σ with complemented tangents Ker(dfp) at pΣ, which are complemented (and normal) subgroups.

In some sense, we could say that the approach of [25] is covering, in the utmost generality known up to now, the case of low-codimensional rectifiable sets in a Carnot group G. It has been clear since the works [22, 39] that, already in the Heisenberg groups Hn, one should approach the low-dimensional rectifiability in a different way with respect to the low-codimensional one. Indeed, in the low-dimensional case in Hn, the authors in [22, 39] choose as a parametrizing class of objects the images of CH1-regular (or Lipschitz-regular) functions from subsets of Rd to Hn, with 1dn, see [22, Definition 3.1 & Definition 3.2], and [39, Definition 2.10 and Definition 3.13].

The bridge between the definition of P-rectifiability and the ones discussed above is done in [39] in the setting of Heisenberg groups and in [24] in arbitrary homogeneous groups but in the case of horizontal tangents. Let us stress that the result in [39, (i)(iv) of Theorem 3.15] shows that in the Heisenberg groups the P-rectifiability with tangents that are vertical subgroups is equivalent to the rectifiability given in terms of CH1-regular surfaces. Moreover [39, (i)(iv) of Theorem 3.14] shows that in the Heisenberg groups, the P-rectifiability with tangents that are horizontal subgroups is equivalent to the rectifiability given in terms of Lipschitz-regular images.

Moreover, very recently, in [24, Theorem 1.1], the authors prove a generalization of [39, Theorem 3.14] in arbitrary homogeneous groups. Namely they prove that in a homogeneous group the k-rectifiability of a set in the sense of Federer can be characterized with the fact that the tangent measures to the set are horizontal subgroups, or equivalently with the fact that there exists an approximate tangent plane that is a horizontal subgroup almost everywhere. In our setting this implies that the P-rectifiability with tangents that are horizontal subgroups is equivalent to the rectifiability given in terms of Lipschitz-regular images, which is Federer’s one. We observe that in the subsequent paper [6] we shall exploit the results proved in this paper and we shall further develop the theory of P-rectifiable measures thus obtaining generalizations of [39, Theorem 3.14 and 3.15] in arbitrary Carnot groups and in all dimensions. See the introduction of [6], and [6, Theorem 1.1]. For results similar to the ones of [6, 24, 39] but in the different setting of the parabolic Rn and in all the codimensions, we point out the recent [38].

We stress that the previous results leave open the challenging question of understanding what is the precise structure of a measure ϕ on H1 such that the tangents are ϕ-almost everywhere the vertical line.

Results

The main contribution of this paper is the proof of the fact that a Ph-rectifiable measure with complemented tangents has density, see Corollary 4.14, and Proposition 2.20 for the last part of the following statement. We recall that when we say that a homogeneous subgroup V of a Carnot group G admits a complementary subgroup, we mean that there exists a homogeneous subgroup L such that G=V·L and VL={0}.

Theorem 1.3

(Existence of the density) Let ϕ be a Ph-rectifiable measure with complemented tangents on G, and assume d is a homogeneous left-invariant metric on G. Let B(xr) be the closed metric ball relative to d of center x and radius r. Then, for ϕ-almost every xG we have

0<lim infr0ϕ(B(x,r))rh=lim supr0ϕ(B(x,r))rh<+.

Moreover, for ϕ-almost every xG we have

r-hTx,rϕΘh(ϕ,x)ChV(x),asrgoes to0,

where the map Tx,r is defined in Definition 2.7, the convergence is understood in the duality with the continuous functions with compact support on G, Θh(ϕ,x) is the h-density with respect to the distance d, and ChV(x) is the h-dimensional centered Hausdorff measure, with respect to the distance d, restricted to V(x), see Definition 2.4.

A way of reading the previous theorem is the following: we prove that whenever a Radon measure on a Carnot group has strictly positive h-lower density and finite h-upper density, and at almost every point, all the blow-up measures are supported on the same (depending on the point) h-dimensional homogeneous complemented subgroup, then the measure has h-density.

We observe here that, as a non-trivial consequence of the results that will be developed in [6], see [6, Theorem 1.1], we have that whenever ΓG is a Borel set such that 0<Sh(Γ)<+, and ChΓ is Ph-rectifiable with complemented tangents, then Θh(ChΓ,x)=1 for Ch-almost every xΓ. See Remark 4.1. We remark that the fact that ChΓ has density one is not a straightforward consequence of Corollary 1.3, and it requires additional work, cf. [6, Proposition 3.9].

Let us remark that the previous Theorem 1.3 solves the implication (ii)(i) of the density problem formulated in [41, page 50] in the setting of Ph-rectifiable measures with complemented tangents. In Euclidean spaces, the proof of Theorem 1.3 is an almost immediate consequence of the fact that projections on linear spaces are 1-Lipschitz in conjunction with the area formula. In our context, we do not have at our disposal the Lipschitz property of projections and an area formula for Ph-rectifiable measures with complemented tangents is obtained in [6, Theorem 1.2] as a consequence of a more refined study of such measures. So the proof requires new ideas. In order to obtain Theorem 1.3, first of all one reduces to the case of the surface measure on an intrinsically Lipschitz graph with very small Lipschitz constant thanks to the structure result Theorem 1.5 below. Secondly, one needs to show that the surface measures of the tangents and their push-forward on the graph are mutually absolutely continuous. For this, last point to hold it will be crucial, on the one hand, that a Ph-rectifiable measure with complemented tangents can be covered almost everywhere with intrinsic graphs, see the forthcoming Theorem 1.5, and, on the other hand, that intrinsic Lipschitz graphs have big projections on their bases, see Proposition 4.6. Third, one exploits the fact that the density exists for the surface measures on the tangents to infer its existence for the original measure.

We remark that with the tools developed in the subsequent paper [6] and pushing forward the study started in this paper, we shall show an area formula for Ph-rectifiable measures with complemented tangents, see [6, Theorem 1.2 and Theorem 1.3].

Other contributions of this paper are structure results for P-rectifiable measures. Since they will be given in terms of sets that satisfy a cone property, let us clarify which cones we are choosing. For any α>0 and any homogeneous subgroup V of G, the cone CV(α) is the set of points wG such that dist(w,V)αw, where · is the homogeneous norm relative to the fixed distance d on G. Moreover a set EG is a CV(α)-set if EpCV(α) for every pE. We refer the reader to Sect. 2.4 for such definitions and some properties of them. We stress that the cones CV(α) are used to give the definition of intrinsically Lispchitz graphs and functions, see [15, Definition 11 and Proposition 3.1]. The first result reads as follows, see Theorem 3.5.

Theorem 1.4

Let G be a Carnot group endowed with an arbitrary left-invariant homogeneous distance. Let ϕ be a Ph-rectifiable measure on G. Then G can be covered ϕ-almost everywhere with countably many compact sets with the cone property with arbitrarily small opening. In other words for every α>0, we have

ϕ(G\i=1+Γi)=0,

where Γi are compact CVi(α)-sets, where Vi are homogeneous subgroups of G of Hausdorff dimension h.

If we ask that the tangents are complemented subgroups, we can improve the previous result. In particular we can take the Γi’s to be intrinsic Lipschitz graphs, see Theorem 3.4 and Proposition 2.17. For the definition of intrinsically Lipschitz function, we refer the reader to Definition 2.16. Let us remark that the fact that the Γi’s can be taken to be graphs will be crucial for the proof of the existence of the density in Theorem 1.3. Actually, by pushing a little bit further the information about the fact that the tangent measures at ϕ-almost every x are constant multiples of ShV(x), we can give a structure result within the class of intrinsically differentiable graphs. Roughly speaking we say that the graph of a function between complementary subgroups φ:UVL is intrinsically differentiable at a0·φ(a0) if graph(φ) admits a homogeneous subgroup as Hausdorff tangent at a0·φ(a0), see Definition 5.5 for details. For the forthcoming theorem, see Corollary 5.5.

Theorem 1.5

Let G be a Carnot group of homogeneous dimension Q endowed with an arbitrary left-invariant homogeneous distance. Let h{1,,Q}, and let ϕ be a Phc-rectifiable, i.e., a Ph-rectifiable measure with tangents that are complemented almost everywhere.

Then G can be covered ϕ-almost everywhere with countably many compact graphs that are simultaneously intrinsically Lipschitz with arbitrarily small constant, and intrinsically differentiable almost everywhere. In other words, for every α>0, we can write

ϕ(G\i=1+Γi)=0,

where Γi=graph(φi) are compact sets, with φi:AiViLi being a function between a compact subset Ai of Vi, which is a homogeneous subgroup of G of homogeneous dimension h, and Li, which is a subgroup complementary to Vi; in addition graph(φi) is a CVi(α)-set, and it is an intrinsically differentiable graph at a·φi(a) for ShAi-almost every aVi, see Definition 5.5.

Let us briefly remark that when a Rademacher-type theorem holds, i.e., if an intrinsically Lipschitz function is intrinsically differentiable almost everywhere, the full result in Theorem 1.5 would simply be deduced by the analogous result but only requiring a covering with intrinsic Lipschitz graphs. We remark that a Rademacher-type theorem at such level of generality, i.e., between arbitrary complementary subgroups of a Carnot group, is now known to be false, see the counterexample in [27]. On the other hand, some positive results in particular cases have been provided in [4, 14, 17] for intrinsically Lipschitz functions with one-dimensional target in groups in which De Giorgi CH1-rectifiability for finite perimeter sets holds, and for functions with normal targets in arbitrary Carnot groups. We stress that very recently in [44], the author proves the Rademacher theorem at any codimension in the Heisenberg groups Hn.

We stress that, as a consequence of the result [6, Theorem 1.1], we get that the Ph-rectifiability of measures of the type ShΓ is equivalent to the fact that Sh-almost every Γ is covered by countably many intrinsic differentiable graphs. Thus, the negative result of [27] gives as a consequence that we cannot substitute intrinsic differentiable with intrinsic Lipschitz in the latter sentence. Ultimately, the general notion of rectifiability by means of coverings with countably many intrinsic Lipschitz graphs is not equivalent to the infinitesimal notion of rectifiability (namely, the P-rectifiability) that one can give by asking that the tangents are almost everywhere unique (and then, as a consequence, homogeneous subgroups).

Let us briefly comment on the results listed above. Theorem 1.3 extends the implication in [39, (iv)(ii) of Theorem 3.15] to the setting of Ph-rectifiable measures whose tangents are complemented in arbitrary Carnot groups. Indeed, in [39, (iv)(ii) of Theorem 3.15], the authors prove that if n+1h2n, and ShΓ is a Ph-rectifiable measure with tangents that are vertical subgroups in the Heisenberg group Hn, then the h-density of ShΓ exists almost everywhere and the tangent is unique almost everywhere. The analogous property in Hn, but with Ph-rectifiable measures with tangents that are horizontal subgroups, is obtained in [39, (iv)(ii) of Theorem 3.14], and in arbitrary homogeneous groups in the recent [24, (iii)(ii) of Theorem 1.1]. However, in this special horizontal case treated in [39, Theorem 3.14] and [24, Theorem 1.1], the authors do not assume Θh(ShΓ,x)>0 since it comes from the existence of an approximate tangent, see [39, Theorem 3.10], while the authors in [24] are able to overcome this issue by adapting [13, Lemma 3.3.6] in [24, Theorem 4.4]. We do not address in this paper the question of obtaining the same general results as in Theorem 1.4, Theorem 1.3, and Theorem 1.5 removing the hypothesis on the strictly positive lower density in item (i) of Definition 1.1 when the tangent is unique (up to a multiplicative constant). Nevertheless, we stress that the results obtained in [24, 39] are for sets, while our results hold for arbitrary Radon measures.

We finally mention that, as a consequence of the machinery developed in the subsequent paper [6], the covering property with intrinsically differentiable graphs proved in Theorem 1.5 actually characterizes the Ph-rectifiability with complemented tangents, see [6, 3. 1. of Theorem 1.1]. The previous characterization is in fact obtained through a delicate rectifiability results for intrinsically differentiable graphs, see [6, Theorem 1.3], and more precisely [6, Lemma 3.9 and Lemma 3.10]. Moreover, as a consequence of [6, Theorem 1.1], the Ph-rectifiability with complemented tangents is equivalent to asking that Preiss’s tangents are complemented homogeneous subgroups without any requirement on the h-lower and upper densities. We refer the reader to [6] for details.

Preliminaries

Carnot Groups

In this subsection, we briefly introduce some notations on Carnot groups that we will extensively use throughout the paper. For a detailed account on Carnot groups, we refer to [29].

A Carnot group G of step κ is a simply connected Lie group whose Lie algebra g admits a stratification g=V1V2Vκ. We say that V1V2Vκ is a stratification of g if g=V1V2Vκ,

[V1,Vi]=Vi+1,for anyi=1,,κ-1,[V1,Vκ]={0},andVκ{0},

where [A,B]:=span{[a,b]:aA,bB}. We call V1 the horizontal layer of G. We denote by n the topological dimension of g, by nj the dimension of Vj for every j=1,,κ. Furthermore, we define πi:GVi to be the projection maps on the i-th strata. We will often shorten the notation to vi:=πiv.

For a Carnot group G, the exponential map exp:gG is a global diffeomorphism from g to G. Hence, if we choose a basis {X1,,Xn} of g, any pG can be written in a unique way as p=exp(p1X1++pnXn). This means that we can identify pG with the n-tuple (p1,,pn)Rn and the group G itself with Rn endowed with the group operation · determined by the Baker–Campbell–Hausdorff formula. From now on, we will always assume that G=(Rn,·) and, as a consequence, that the exponential map exp acts as the identity.

For any pG, we define the left translation τp:GG as

qτpq:=p·q.

As already remarked above, the group operation · is determined by the Campbell–Hausdorff formula, and it has the form (see [19, Proposition 2.1])

p·q=p+q+Q(p,q),forallp,qRn,

where Q=(Q1,,Qκ):Rn×RnV1Vκ, and the Qi’s have the following properties. For any i=1,κ and any p,qG we have

  • (i)

    Qi(δλp,δλq)=λiQi(p,q),

  • (ii)

    Qi(p,q)=-Qi(-q,-p),

  • (iii)

    Q1=0 and Qi(p,q)=Qi(p1,,pi-1,q1,,qi-1).

Thus, we can represent the product · as

p·q=(p1+q1,p2+q2+Q2(p1,q1),,pκ+qκ+Qκ(p1,,pκ-1,q1,,qκ-1)). 1

The stratification of g carries with it a natural family of dilations δλ:gg, that are Lie algebra automorphisms of g and are defined by

δλ(v1,,vκ):=(λv1,λ2v2,,λκvκ),for anyλ>0,

where viVi. The stratification of the Lie algebra g naturally induces a gradation on each of its homogeneous Lie sub-algebras h, i.e., sub-algebras that are δλ-invariant for any λ>0, that is

h=V1hVκh. 2

We say that h=W1Wκ is a gradation of h if [Wi,Wj]Wi+j for every 1i,jκ, where we mean that W:={0} for every >κ. Since the exponential map acts as the identity, the Lie algebra automorphisms δλ can be read also as group automorphisms of G.

Definition 2.1

(Homogeneous subgroups) A subgroup V of G is said to be homogeneous if it is a Lie subgroup of G that is invariant under the dilations δλ.

We recall the following basic terminology: a horizontal subgroup of a Carnot group G is a homogeneous subgroup of it that is contained in exp(V1); a Carnot subgroup W=exp(h) of a Carnot group G is a homogeneous subgroup of it such that the first layer V1h of the grading of h inherited from the stratification of g is the first layer of a stratification of h.

Homogeneous Lie subgroups of G are in bijective correspondence through exp with the Lie sub-algebras of g that are invariant under the dilations δλ. For any Lie algebra h with gradation h=W1Wκ, we define its homogeneous dimension as

dimhom(h):=i=1κi·dim(Wi).

Thanks to (2) we infer that, if h is a homogeneous Lie sub-algebra of g, we have dimhom(h):=i=1κi·dim(hVi). We introduce now the class of homogeneous and left-invariant distances.

Definition 2.2

(Homogeneous left-invariant distance) A metric d:G×GR is said to be homogeneous and left invariant if for any x,yG, we have

  • (i)

    d(δλx,δλy)=λd(x,y) for any λ>0,

  • (ii)

    d(τzx,τzy)=d(x,y) for any zG.

We remark that two homogeneous left-invariant distances on a Carnot group are always bi-Lipschitz equivalent. It is well known that the Hausdorff dimension (for a definition of Hausdorff dimension see for instance [36, Definition 4.8]) of a graded Lie group G with respect to an arbitrary left-invariant homogeneous distance coincides with the homogeneous dimension of its Lie algebra. For a reference for the latter statement, see [30, Theorem 4.4]. From now on, if not otherwise stated, G will be a fixed Carnot group. We recall that a homogeneous norm · on G is a function ·:G[0,+) such that δλx=λx for every λ>0 and xG; x·yx+y for every x,yG; and x=0 if and only if x=0. We introduce now a distinguished homogeneous norm on G.

Definition 2.3

(Smooth-box metric) For any gG, we let

g:=max{ε1|g1|,ε2|g2|1/2,,εκ|gκ|1/κ},

where ε1=1 and ε2,εκ are suitably small parameters depending only on the group G. For the proof of the fact that we can choose the εi’s in such a way that · is a homogeneous norm on G that induces a left-invariant homogeneous distance, we refer to [19, Sect. 5].

Given an arbitrary homogeneous norm · on G, the distance d induced by · is defined as follows:

d(x,y):=x-1·y.

Vice-versa, given a homogeneous left-invariant distance d, it induces a homogeneous norm through the equality x:=d(x,e) for every xG, where e is the identity element of G.

Given a homogeneous left-invariant distance d, we let U(x,r):={zG:d(x,z)<r} be the open metric ball relative to the distance d centered at x and with radius r>0. The closed ball will be denoted with B(x,r):={zG:d(x,z)r}. Moreover, for a subset EG and r>0, we denote with B(E,r):={zG:dist(z,E)r} the closed r-tubular neighborhood of E and with U(E,r):={zG:dist(z,E)<r} the open r -tubular neighborhood of E.

The following estimate on the norm of the conjugate will be useful later on. It appears in [34, Lemma 3.6].

Lemma 2.1

For any homogeneous norm · and any >0, there exists a constant C1()>1 such that for every x,yB(0,), we have

y-1·x·yC1x1/κ.

Definition 2.4

(Hausdorff Measures) Throughout the paper, we define the h- dimensional spherical Hausdorff measure relative to a left-invariant homogeneous metric d as

Sh(A):=supδ>0inf{j=1rjh:Aj=1B(xj,rj),rjδ},

for every AG. We define the h-dimensional Hausdorff measure relative to d as

Hh(A):=supδ>0infj=12-h(diamEj)h:Aj=1Ej,diamEjδ,

for every AG. We define the h-dimensional centered Hausdorff measure relative to d as

Ch(A):=supEAC0h(E),

for every AG, where

C0h(E):=supδ>0inf{j=1rjh:Ej=1B(xj,rj),xjE,rjδ},

for every EG. We stress that Ch is an outer measure, and thus, it defines a Borel regular measure, see [12, Proposition 4.1], and that the measures Sh,Hh,Ch are all equivalent measures, see [13, Sect. 2.10.2] and [12, Proposition 4.2].

Definition 2.5

(Hausdorff distance) Given a left-invariant homogeneous distance d on G, for any couple of sets A,BG, we define the Hausdorff distance of A from B as

dH,G(A,B):=max{supxAdist(x,B),supyBdist(A,y)},

where

dist(x,A):=infyAd(x,y),

for every xG and AG.

Densities and Tangents of Radon Measures

Throughout the rest of the paper, we will always assume that G is a fixed Carnot group endowed with an arbitrary left-invariant homogeneous distance d. Some of the forthcoming results will be proved in the particular case in which d is the distance induced by the distinguished homogeneous norm defined in Definition 2.3, and we will stress this when it will be the case.

The homogeneous, and thus Hausdorff, dimension with respect to d will be denoted with Q. Furthermore, as discussed in the previous subsection, we will assume without loss of generality that G coincides with Rn endowed with the product induced by the Baker–Campbell–Hausdorff formula relative to Lie(G).

Definition 2.6

(Weak convergence of measures) Given a family {ϕi}iN of Radon measures on G, we say that ϕi weakly converges to a Radon measure ϕ, and we write ϕiϕ, if

fdϕifdϕ,for anyfCc(G).

Definition 2.7

(Tangent measures) Let ϕ be a Radon measure on G. For any xG and any r>0 we define the measure

Tx,rϕ(E):=ϕ(x·δr(E)),for any Borel setE.

Furthermore, we define Tanh(ϕ,x), the h-dimensional tangents to ϕ at x, to be the collection of the Radon measures ν for which there is an infinitesimal sequence {ri}iN such that

ri-hTx,riϕν.

Remark 2.1

(Zero as a tangent measure) We remark that our definition potentially admits the zero measure as a tangent measure, as in [9], while the definitions in [42] and [39] do not.

Definition 2.8

(Lower and upper densities) If ϕ is a Radon measure on G, and h>0, we define

Θh(ϕ,x):=lim infr0ϕ(B(x,r))rh,andΘh,(ϕ,x):=lim supr0ϕ(B(x,r))rh,

and we say that Θh(ϕ,x) and Θh,(ϕ,x) are the lower and upper h-density of ϕ at the point xG, respectively. Furthermore, we say that measure ϕ has h-density if

0<Θh(ϕ,x)=Θh,(ϕ,x)<,forϕ-almost anyxG.

Lebesgue theorem holds for measures with positive lower density and finite upper density, and thus, local properties are stable under restriction to Borel subsets.

Proposition 2.2

Suppose ϕ is a Radon measure on G with 0<Θh(ϕ,x)Θh,(ϕ,x)< for ϕ-almost every xG. Then, for any Borel set BG and for ϕ-almost every xB, we have

Θh(ϕB,x)=Θh(ϕ,x),andΘh,(ϕB,x)=Θh,(ϕ,x).

Proof

This is a direct consequence of Lebesgue differentiation Theorem of [23, page 77] that can be applied since (G,d,ϕ) is a Vitali metric measure space due to [23, Theorem 3.4.3].

We stress that whenever the h-lower density of ϕ is strictly positive and the h-upper density of ϕ is finite ϕ-almost everywhere, the set Tanh(ϕ,x) is nonempty for ϕ-almost every xG, see [41, Proposition 1.12]. The following proposition has been proved in [41, Proposition 1.13].

Proposition 2.3

(Locality of tangents) Let h>0, and let ϕ be a Radon measure such that for ϕ-almost every xG we have

0<Θh(ϕ,x)Θh,(ϕ,x)<.

Then for every ρL1(ϕ) that is nonnegative ϕ-almost everywhere we have Tanh(ρϕ,x)=ρ(x)Tanh(ϕ,x) for ϕ-almost every xG. More precisely, the following holds: for ϕ-almost every xG, then

ifri0is such thatri-hTx,riϕνthenri-hTx,ri(ρϕ)ρ(x)ν. 3

Let us introduce a useful split of the support of a Radon measure ϕ on G.

Definition 2.9

Let ϕ be a Radon measure on G that is supported on the compact set K. For any ϑ,γN we define

E(ϑ,γ):={xK:ϑ-1rhϕ(B(x,r))ϑrhfor any0<r<1/γ}. 4

Let us stress that Definition 2.9 does not only depend on ϑ,γ but obviously also on h. Anyway throughout the proofs of this paper, we always assume h to be fixed, and hence, we will not stress this dependence in the notation E(ϑ,γ).

Proposition 2.4

For any ϑ,γN, the set E(ϑ,γ) defined in Definition 2.9 is compact.

Proof

This is [41, Proposition 1.14].

Proposition 2.5

Assume ϕ is a Radon measure supported on the compact set K such that 0<Θh(ϕ,x)Θh,(ϕ,x)< for ϕ-almost every xG. Then ϕ(G\ϑ,γNE(ϑ,γ))=0.

Proof

Let wK\ϑ,γE(ϑ,γ) and note that this implies that either Θh(ϕ,x)=0 or Θh,(ϕ,x)=. Since 0<Θh(ϕ,x)Θh,(ϕ,x)< for ϕ-almost every xG, this concludes the proof.

We recall here a useful proposition about the structure of Radon measures.

Proposition 2.6

( [41, Proposition 1.17 and Corollary 1.18]) Let ϕ be a Radon measure supported on a compact set on G such that 0<Θh(ϕ,x)Θh,(ϕ,x)< for ϕ-almost every xG. For every ϑ,γN, we have that ϕE(ϑ,γ) is mutually absolutely continuous with respect to ShE(ϑ,γ).

Intrinsic Grassmannian in Carnot Groups

Let us recall the definition of the Euclidean Grassmannian, along with some of its properties.

Definition 2.10

(Euclidean Grassmannian) Given kn we let Gr(n,k) to be the set of the k-vector subspaces of Rn. We endow Gr(n,k) with the following distance

deu(V1,V2):=dH,euV1Beu(0,1),V2Beu(0,1),

where Beu(0,1) is the (closed) Euclidean unit ball, and dH,eu is the Hausdorff distance between sets induced by the Euclidean distance on Rn.

Remark 2.2

(Euclidean Grassmannian and convergence) It is well known that the metric space (Gr(n,k),dH,eu) is compact. Moreover, the following hold

  • (i)

    if VnV, then for every vV there exist vnVn such that vnv;

  • (ii)

    if VnV and there is a sequence vnVn such that vnv, then vV.

The proof of the two items above is left to the reader as an exercise.

We now give the definition of the intrinsic Grassmannian on Carnot groups and introduce the class of complemented homogeneous subgroups.

Definition 2.11

(Intrinsic Grassmannian on Carnot groups) For any 1hQ, we define Gr(h) to be the family of homogeneous subgroups V of G that have Hausdorff dimension h.

Let us recall that if V is a homogeneous subgroup of G, any other homogeneous subgroup L such that

V·L=GandVL={0}.

is said to be a complement of G. We let Grc(h) to be the subfamily of those VGr(h) that have a complement and we will refer to Grc(h) as the h-dimensional complemented Grassmannian.

Let us introduce the stratification vector of a homogeneous subgroup.

Definition 2.12

(Stratification vector) Let h{1,,Q} and for any VGr(h) we denote with s(V) the vector

s(V):=(dim(V1V),,dim(VκV)),

that with abuse of language we call the stratification, or the stratification vector, of V. Furthermore, we define

S(h):={s(V)Nκ:VGr(h)}.

We remark that the cardinality of S(h) is bounded by i=1κ(dimVi+1) for any h{1,,Q}.

We now collect in the following result some topological properties of the Grassmannians introduced above.

Proposition 2.7

(Compactness of the Grassmannian) For any 1hQ the function

dG(W1,W2):=dH,G(W1B(0,1),W2B(0,1)),

with W1,W2Gr(h), is a distance on Gr(h). Moreover (Gr(h),dG) is a compact metric space.

Proof

The fact that dG is a distance comes from well-known properties of the Hausdorff distance. Let us consider a sequence {Wj}jNGr(h), with Wj=Wj,1Wj,κ, where Wj,i:=ViWj for any jN and 1iκ. By extracting a (non-re-labeled) subsequence, we can suppose that there exist {ki}i=1,,κ natural numbers such that the topological dimension is dimWj,i=ki for all jN, and for all 1iκ. In particular, the topological dimension of Wj is constant. Exploiting the compactness of the Euclidean Grassmannian, see Remark 2.2, we get that up to a (non-re-labeled) subsequence,

Wj,iWi,i.e.deu(Wj,i,Wi)0for any1iκ, 5

where the convergence is meant in the Euclidean Grassmannian Gr(ki,Vi). As a consequence

Wj=Wj,1Wj,κW=W1Wκ,i.e.,dH,eu(Wj,W)0, 6

where the convergence is meant in the Euclidean Grassmannian Gr(i=1κki,n). The previous equality is a consequence of (5) and the following observation: if V and W are two orthogonal linear subspaces such that Rn=VW, and AB are vector subspaces of V, and CD are vector subspaces of W, then

deu(AC,BD)deu(A,B)+deu(C,D),

where the direct sums above are orthogonal too. Let us notice that, from (6) it follows that

dH,eu(WjB(0,1),WB(0,1))0, 7

where we stress that B(0, 1) is the closed unit ball in the homogeneous left-invariant metric d. The proof of (7) can be reached by contradiction exploiting (6) and the fact that B(0, 1) is compact. We leave the routine details to the reader.

In order to conclude the proof, we need to show that

dG(WjB(0,1),WB(0,1))0. 8

Indeed, on the compact set B(0, 1), one has dCdeu1/κ for some constant C>0, see for instance [43, Proposition 2.15]. This means that for subsets contained in B(0, 1) one has dHCdH,eu1/s. This last inequality with (7) gives (8). Finally from (8) we get, by the very definition of dG,

dG(Wj,W)0.

If we show that W is a homogeneous subgroup of homogeneous dimension h we are done. The homogeneity comes from the fact that W admits a stratification (6), while the homogeneous dimension is fixed because it depends on the dimensions of Wi that are all equal to ki. Let us prove W is a subgroup. First of all W is inverse-closed, because W=expW, and W is a vector space. Now take a,bW. By the first point of Remark 2.2 we find an,bnWn such that ana, and bnb. Then, by continuity of the operation, an·bna·b, and an·bnWn. Then from the second point of Remark 2.2 we get that a·bW.

Proposition 2.8

There exists a constant ħG>0, depending only on G, such that if W,VGr(h) and dG(V,W)ħG, then s(V)=s(W).

Proof

Let us fix 1hQ. Let us suppose by contradiction that there exist Vi and Wi in Gr(h) such that, for every iN, the stratification of Vi is different from Wi and such that dG(Vi,Wi)0. Up to extract two (non-re-labeled) subsequences we can assume that the Vi’s have the same stratification for every iN, as well as the Wi’s. Then, by compactness, see the proof of Proposition 2.7, we can assume up to passing to a (non re-labeled) subsequence that WiW where W has the same stratification of the Wi’s, and ViV where V has the same stratification of the Vi’s. Since dG(Vi,Wi)0, we get that dG(V,W)=0 and then V=W but this is a contradiction since they have different stratifications. This proves the existence of a constant ħ that depends both on G and h. However, taking the minimum over h of such ħ’s, the dependence on h is eliminated.

Proposition 2.9

Suppose VGr(h) is a homogeneous subgroup of topological dimension d. Then ShV, HhV, ChV and HeudV are Haar measures of V. Furthermore, any Haar measure λ of V is h-homogeneous in the sense that

λ(δr(E))=rhλ(E),for any Borel setEV.

Proof

This follows from the fact that the Hausdorff, the spherical Hasudorff, and the centered Hausdorff measures introduced in Definition 2.5 are invariant under left translations and thus on the one hand, they are Haar measures of V. Furthermore, one can show by an explicit computation that the Lebesgue measure Ld restricted to the vector space exp-1(V) is a Haar measure. Indeed, this last assertion comes from the fact that for every vV the map pv·p has unitary Jacobian determinant when seen as a map from V to V, see [15, Lemma 2.20]. Thus since when seen V as immersed in Rn we have that the Lebesgue measure of V coincides with HeudV, we conclude that HeudV is a Haar measure of V as well. The last part of the proposition comes from the fact that the property is obvious by definition for the spherical Hausdorff measure, and the fact that all the Haar measures are the same up to a constant.

We now introduce the projections related to a splitting G=V·L of the group.

Definition 2.13

(Projections related to a splitting) For any VGrc(h) with a homogeneous complement L, we can find two unique elements gV:=PVgV and gL:=PLgL such that

g=PV(g)·PL(g)=gV·gL.

We will refer to PV(g) and PL(g) as the splitting projections, or simply projections, of g onto V and L, respectively.

We recall here below a very useful fact on splitting projections.

Proposition 2.10

Let us fix VGrc(h) and L two complementary homogeneous subgroups of a Carnot group G. Then, for any xG, the map Ψ:VV defined as Ψ(z):=PV(xz) is invertible and it has unitary Jacobian. As a consequence Sh(PV(E))=Sh(PV(xPV(E)))=Sh(PV(xE)) for every xG and EG Borel.

Proof

The first part is a direct consequence of [15, Proof of Lemma 2.20]. For the second part it is sufficient to use the first part and the fact that for every x,yG we have PV(xy)=PV(xPVy).

The following proposition holds for the distance d induced by the norm introduced in Definition 2.3.

Proposition 2.11

Let G be a Carnot group endowed with the homogeneous norm · introduced in Definition 2.3. Let WGr(h) be a homogeneous subgroup of Hausdorff dimension h and of topological dimension d. Then

  • (i)
    there exists a constant C2:=C2(s(W)) such that for any pW and any r>0 we have
    HeudB(p,r)W=C2rh, 9
  • (ii)

    there exists a constant β(W) such that ChW=β(W)HeudW,

  • (iii)

    β(W)=HeudW(B(0,1))-1 and in particular β(W)=β(s(W)).

Proof

Thanks to Proposition 2.9, we have

Heud(B(p,r)W)=Heud(B(0,r)W)=Heud(δr(B(0,1)W))=rhHeud(B(0,1)W).

Furthermore, if V is another homogeneous subgroup such that s(W)=s(V), we can find a linear map T that acts as an orthogonal transformation on each of the Vi’s and that maps W to V. Since we are endowing G with the box metric Definition 2.3, we get that T(B(0,1)W)=B(0,1)V. Since T is an orthogonal transformation itself, it is an isometry of Rn and this implies that

Heud(B(0,1)W)=Heud(T(B(0,1)W))=Heud(B(0,1)V).

Concerning (ii) thanks to Proposition 2.9, we have that both ChW and HeudW are Haar measures of W. This implies that there must exist a constant β(W) such that β(W)HeudW=ChW.

Finally, in order to prove (iii), we prove the following. For every left-invariant homogeneous distance d on G and every homogeneous subgroup WG of Hausdorff dimension h, we have that

Ch(WB(0,1))=1, 10

where Ch is the centered Hausdorff measure relative to the distance d and B(0, 1) is the closed ball relative to the distance d.

Indeed, let us fix an ε>0, let us take AWB(0,1) such that C0h(A)Ch(WB(0,1))-ε, δ>0 and a covering of A with closed balls Bi:={B(xi,ri)}iN centered on AW and with radii riδ such that

iNrihC0h(A)+ε.

This implies that

Ch(B(0,1)W)(Ch(B(0,1)W)+ε)Ch(B(0,1)W)(C0h(A)+ε)iNCh(B(0,1)W)rih=iNCh(B(xi,ri)W)Ch(A)C0h(A)Ch(WB(0,1))-ε,

where the first inequality is true since Ch(B(0,1)W)Ch(A)C0h(A), and the third equality is true since xiW and ChW is a Haar measure on W. Thanks to the arbitrariness of ε, we finally infer that Ch(WB(0,1))1.

On the other hand, thanks to [16, item (ii) of Theorem 2.13 and Remark 2.14], we have that, calling Bt:={xWB(0,1):Θ,h(ChW,x)>t} for every t>0, we infer that Ch(Bt)tCh(Bt) for every t>0. Thus, for every t>1 we conclude Ch(Bt)=0 and hence for ChW-almost every xWB(0,1) we have that Θ,h(ChW,x)1. For one of such xWB(0,1) we can write

Ch(B(0,1)W)=lim supr0Ch(B(x,r)W)rh=Θ,h(ChW,x)1,

where the first equality comes from Proposition 2.9. Thus Ch(WB(0,1))=1 and this concludes the proof of the first part of (iii) thanks to item (ii). The fact that β(W) depends only on s(W) follows from item (i)

Remark 2.3

The above proposition can be proved whenever the distance is a multiradial distance, see [33, Definition 8.5].

Remark 2.4

We stress here for future references that in the proof of item (iii) of Proposition 2.11 we proved that whenever G is endowed with an arbitrary left-invariant homogeneous distance d, then for every homogeneous subgroup WG of Hausdorff dimension h, we have that

Ch(WB(0,1))=1. 11

We conclude this subsection with two Propositions.

Proposition 2.12

(Corollary 2.15 of [15]) Let · be a homogeneous norm on G and let V and L be two complementary subgroups. Then there exists a constant C3(V,L) such that for any gG we have

C3(V,L)PL(g)dist(g,V)PL(g),for anygG. 12

In the following, whenever we write C3(V,L), we are choosing the supremum of all the constants such that inequality (12) is satisfied.

Proposition 2.13

For any VGrc(h) with complement L, there is a constant C4(V,L)>0 such that for any pG and any r>0 we have

ShV(PV(B(p,r)))=C4(V,L)rh.

Furthermore, for any Borel set AG for which Sh(A)<, we have

ShV(PV(A))2C4(V,L)Sh(A). 13

Proof

The existence of such C4(V,L) is yielded by [15, Lemma 2.20]. Suppose {B(xi,ri)}iN is a countable covering of A with closed balls for which iNrih2Sh(A). Then

Sh(PV(A))Sh(PV(iNB(xi,ri)))C4(V,L)iNrih2C4(V,L)Sh(A).

Cones Over Homogeneous Subgroups

In this subsection, we introduce the intrinsic cone CW(α) and the notion of CW(α)-set, and prove some of their properties. In this subsection, G will be a fixed Carnot group endowed with an arbitrary homogeneous norm · that induces a left-invariant homogeneous distance d.

Definition 2.14

(Intrinsic cone) For any α>0 and WGr(h), we define the cone CW(α) as

CW(α):={wG:dist(w,W)αw}.

Definition 2.15

(CW(α)-set) Given WGr(h), and α>0, we say that a set EG is a CW(α)-set if

Ep·CW(α),for anypE.

Lemma 2.14

For any W1,W2Gr(h), ε>0 and α>0 if dG(W1,W2)<ε/4, then

CW1(α)CW2(α+ε).

Proof

We prove that any zCW1(α) is contained in the cone CW2(α+ε). Thanks to the triangle inequality, we infer

dist(z,W2)d(z,b)+infwW2d(b,w),for anybW1.

Thus, choosing bW1 in such a way that d(z,b)=dist(z,W1), and evaluating the previous inequality at b, we get

dist(z,W2)dist(z,W1)+dist(b,W2)αz+dist(b,W2), 14

where in the second inequality, we used zCW1(α).

Let us notice that, given W an arbitrary homogeneous subgroup of G, pG an arbitrary point such that pW is one of the points at minimum distance from W to p, then the following inequality holds

p2p. 15

Indeed,

p-p(p)-1·p=d(p,W)pp2p.

Now, by homogeneity, since bW1 is the point at minimum distance from W1 of z, we get that D1/z(b) is the point at minimum distance from W1 of D1/z(z). Thus, since D1/z(z)=1, from (15), we get that D1/z(b)2. Finally we obtain

dist(b,W2)=zdist(D1/z(b),W2)=zdist(D1/z(b),W2B(0,4))zdH(W1B(0,4),W2B(0,4))=4zdH(W1B(0,1),W2B(0,1))<εz, 16

where the first equality follows from the homogeneity of the distance; the second is a consequence of the fact that D1/z(b)2, and thus, from (15), the point at minimum distance of D1/z(b) from W2 has norm bounded above by 4; the third inequality comes from the definition of Hausdorff distance; the fourth equality is true by homogeneity; and the last inequality comes from the hypothesis dG(W1,W2)<ε/4. Joining (14), and (16), we get zCW2(α+ε), that was what we wanted.

Lemma 2.15

Let VGrc(h), and let L be a complementary subgroup of V. There exists ε1:=ε1(V,L)>0 such that

LCV(ε1)={0}.

Moreover, we can, and will, choose ε1(V,L):=C3(V,L)/2.

Proof

We prove that it suffices to take ε1(V,L):=C3(V,L)/2. Let us suppose the statement is false. Thus there exists 0vLCV(ε1). From Proposition 2.12 and from the very definition of the cone CV(ε1) we have

C3(V,L)vdist(v,V)ε1v=C3(V,L)v/2,

which is a contradiction with the fact that v0.

We will not use the following proposition in the paper, but it is worth mentioning it.

Proposition 2.16

The family of the complemented subgroups Grc(h) is an open subset of Gr(h).

Proof

Fix a WGrc(h) and let L be one complementary subgroup of W and set ε<min{ε1(V,L),ħG}. Then, if WGr(h) is such that dG(W,W)<ε/4, Lemma 2.14 implies that WCW(ε) and in particular

LWLCW(ε)={0}.

Moreover, since ε<ħG from Proposition 2.8, we get that W has the same stratification of W and thus the same topological dimension. This, jointly with the previous equality and the Grassmann formula, means that (WVi)+(LVi)=Vi for every i=1,,κ. This, jointly with the fact that LW={0}, implies that L and W are complementary subgroups in G due to the triangular structure of the product · on G, see (1). For an alternative proof of the fact that L and W are complementary subgroups, see also [25, Lemma 2.7].

The following definition of intrinsically Lipschitz functions is equivalent to the classical one in [15, Definition 11] because the cones in [15, Definition 11] and the cones CV(α) are equivalent whenever V admits a complementary subgroup, see [15, Proposition 3.1].

Definition 2.16

(Intrinsically Lipschitz functions) Let WGrc(h) and assume L is a complement of W and let EW be a subset of V. Let α>0. A function f:EL is said to be an α-intrinsically Lipschitz function if graph(f):={v·f(v):vE} is a CW(α)-set. A function f:EL is said to be an intrinsically Lipschitz function if there exists α>0 such that f is an α-intrinsically Lipschitz function.

Proposition 2.17

Let us fix WGrc(h) with complement L. If ΓG is a CW(α)-set for some αε1(W,L), then the map PW:ΓW is injective. As a consequence, Γ is the intrinsic graph of an intrinsically Lipschitz map defined on PW(Γ).

Proof

Suppose by contradiction that PW:ΓW is not injective. Then, there exist pq with p,qΓ such that PW(p)=PW(q). Thus p-1·qL. Moreover, since Γ is a CW(α)-set, we have that p-1·qCW(α). Eventually we get

p-1·qLCW(α)LCW(ε1(W,L)),

where the last inclusion follows since αε1(W,L). The above inclusion, jointly with Lemma 2.15, gives that p-1·q=0 and this is a contradiction. Concerning the last part of the statement, let us notice that the map PL((PW)|Γ)-1 is well defined from PW(Γ) to L and its intrinsic graph is Γ by definition. Moreover, since Γ is a CW(α)-set, the latter map is intrinsically Lipschitz by Definition 2.16.

The following two lemmata will play a fundamental role in the proof that Phc-rectifiable measures have h-density.

Lemma 2.18

Let VGrc(h) and L be one of its complementary subgroups. For any 0<α<C3(V,L)/2, let

c(α):=α/(C3(V,L)-α). 17

Then we have

B(0,1)VPV(B(0,1)CV(α))B(0,1/(1-c(α)))V. 18

Proof

The first inclusion comes directly from the definition of projections and cones. Concerning the second, if vB(0,1)CV(α), thanks to Proposition 2.12, we have

C3(V,L)PL(v)dist(v,V)αvα(PL(v)+PV(v)). 19

This implies in particular that PL(v)c(α)PV(v) and thus

1PV(v)PL(v)PV(v)-PL(v)(1-c(α))PV(v).

This concludes the proof of the lemma.

Lemma 2.19

Let VGrc(h) and L be one of its complementary subgroups. Suppose Γ is a CV(α)-set with α<C3(V,L)/2, and let

C(α):=1-c(α)1+c(α), 20

where c(α) is defined in (17). Then

Sh(PV(B(x,r)Γ))Sh(PV(B(x,C(α)r)xCV(α))PV(Γ)),for anyxΓ.

The same inequality above holds if we substitute Sh with any other Haar measure on V, see Proposition 2.9, because all of them are equal up to a constant.

Proof

First of all, let us note that we have

Sh(PV(B(x,r)Γ))=Sh(PV(B(0,r)x-1Γ)), 21

where the last equality is true since Sh(PV(E))=Sh(PV(x-1E)) for any Borel EG, see Proposition 2.10. We wish now to prove the following inclusion

PV(B(0,C(α)r)CV(α))PV(x-1Γ)PV(B(0,r)x-1Γ). 22

Indeed, fix an element y of PV(B(0,C(α)r)CV(α))PV(x-1Γ). Thanks to our choice of y, there are a w1x-1Γ and a w2B(0,C(α)r)CV(α) such that

PV(w1)=y=PV(w2).

Furthermore, since Γ is a CV(α)-set, we infer that w1CV(α) and thus with the same computations as in (19), we obtain that PL(w1)c(α)PV(w1) and thus

w1(1+c(α))PVw1(1+c(α))y. 23

Furthermore, since by assumption w2B(0,C(α)r)CV(α), Lemma 2.18 yields

y=PV(w2)C(α)r/(1-c(α))=r/(1+c(α)). 24

The bounds (23) and (24) together imply that w1r, and thus w1B(0,r)x-1Γ and this concludes the proof of the inclusion (22). Finally (21), (22) imply

Sh(PV(B(x,r)Γ))Sh(PV(B(0,C(α)r)CV(α))PV(x-1Γ)). 25

Furthermore, for any Borel subset E of G, we have PV(xE)=PV(xPV(E)), since for every gE we have the following simple equality PV(xg)=PV(xPVg). Therefore, by using the latter observation and Proposition 2.10, we get, denoting with Ψ the map Ψ(v)=PV(x-1v) for every vV, that

Sh(PV(B(0,C(α)r)CV(α))PV(x-1Γ))=Sh(PV(x-1PV(B(x,C(α)r)xCV(α)))PV(x-1PV(Γ)))=Sh(Ψ(PV(B(x,C(α)r)xCV(α)))Ψ(PV(Γ)))=Sh(PV(B(x,C(α)r)xCV(α))PV(Γ)). 26

Joining together (25) and (26) gives the sought conclusion.

Rectifiable Measures in Carnot Groups

In what follows we are going to define the class of h-flat measures on a Carnot group and then we will give proper definitions of rectifiable measures on Carnot groups. Again we recall that throughout this subsection G will be a fixed Carnot group endowed with an arbitrary left-invariant homogeneous distance.

Definition 2.17

(Flat measures) For any h{1,,Q} we let M(h) to be the family of flat h-dimensional measures in G, i.e.,

M(h):={λShW:for someλ>0andWGr(h)}.

Furthermore, if G is a subset of the h-dimensional Grassmannian Gr(h), we let M(h,G) to be the set

M(h,G):={λShW:for someλ>0andWG}. 27

We stress that in the previous definitions we can use any of the Haar measures on W, see Proposition 2.9, since they are the same up to a constant.

Definition 2.18

(Ph andPh-rectifiable measures) Let h{1,,Q}. A Radon measure ϕ on G is said to be a Ph-rectifiable measure if for ϕ-almost every xG we have

  • (i)

    0<Θh(ϕ,x)Θh,(ϕ,x)<+,

  • (ii)

    there exists a V(x)Gr(h) such that Tanh(ϕ,x){λShV(x):λ0}.

Furthermore, we say that ϕ is Ph-rectifiable if (ii) is replaced with the weaker

(ii)

Tanh(ϕ,x){λShV:λ0andVGr(h)}.

Remark 2.5

(About λ=0 in Definition 2.18) It is readily noticed that, since in Definition 2.18 we are asking Θh(ϕ,x)>0 for ϕ-almost every x, we can not have the zero measure as a tangent measure. As a consequence, a posteriori, we have that in item (ii) and item (ii)* above, we can restrict to λ>0. We will tacitly work in this restriction from now on.

On the contrary, if we only know that for ϕ-almost every xG we have

Θh,(ϕ,x)<+,andTanh(ϕ,x){λShV(x):λ>0}, 28

for some V(x)Gr(h), hence Θh(ϕ,x)>0 for ϕ-almost every xG, and the same property holds with the item (ii)* above. Indeed, if at some x for which (28) holds we have Θh(ϕ,x)=0, then there exists ri0 such that ri-hϕ(B(x,ri))=0. Since Θh,(ϕ,x)<+, up to subsequences (see [1, Theorem 1.60]), we have ri-hTx,riϕλShV(x), for some λ>0. Hence, by applying [1, Proposition 1.62(b)] we conclude that ri-hTx,riϕ(B(0,1))λShV(x)(B(0,1))>0, that is a contradiction.

Throughout the paper, it will be often convenient to restrict our attention to the subclass of Ph- and Ph-rectifiable measures, given by the measures that have complemented tangents. More precisely, we give the following definition.

Definition 2.19

(Phc-rectifiable measures) Let h{1,,Q}. In the following we denote by Phc the family of those Ph-rectifiable measures such that for ϕ-almost every xG we have

Tanh(ϕ,x)M(h,Grc(h)).

Remark 2.6

As explained in the introduction, the bridge between the notion of Phc-rectifiable measures and the other notions of rectifiability in the Heisenberg groups Hn is nowadays very well understood after the results in [39, Theorem 3.14 and Theorem 3.15] and [44]. Let us now discuss some examples of flat rectifiable measures in a different setting, i.e., in the Engel group, which we denote by E.

The Engel group E is the Carnot group whose Lie algebra e admits a basis {X1,X2,X3,X4} such that [X1,X2]=X3, and [X1,X3]=X4. Hence it is a step-3 Carnot group of topological dimension 4 and homogeneous dimension 7 where V1=span{X1,X2}, V2=span{X3}, and V3=span{X4). In exponential coordinates associated with the basis (X1,X2,X3,X4), the law product can be explicitly written as in [15, Example 2.6]. As explicitly computed in [15, Example 2.6], in E we have two families of homogeneous complementary subgroups. The first family is given by Mα,β·Nγ,δ where α,β,γ,δR satisfy αδ-βγ0, and

Mα,β:={(αt,βt,0,0):tR},Nγ,δ:={(γt,δt,x3,x4):t,x3,x4R}.

In this case notice that, by homogeneity, S1Mα,β and S6Nγ,δ are both Phc-rectifiable measures. Notice, moreover, that Nγ,δ is normal and it is also a CH1-hypersurface, thus being rectifiable in the sense of Definition 5.3. The same does not hold for Mα,β since it is not normal, compare with Remark 5.2.

The second family of homogeneous subgroups is given by K·Hα,β, where α,βR satisfy α+β0, and

K:={(x1,-x1,x3,0):x1,x3R},Hα,β:={(αt,βt,0,x4):t,x4R}.

Notice that S3K and S4Hα,β are both Phc-rectifiable measures. Nevertheless, since both K and Hα,β are not normal, none of them can be a CH1(E;G) for any Carnot group G because otherwise the tangent, which coincides everywhere with the same subgroup by homogeneity, would be normal, compare with Remark 5.2.

Proposition 2.20

Let h{1,,Q} and assume ϕ is a Radon measure on G. If {ri}iN is an infinitesimal sequence such that ri-hTx,riϕλChV for some λ>0 and VGr(h) then

limiϕ(B(x,ri))/rih=λ.

Proof

Since ChV(x)(B(0,1))=0, see e.g., [25, Lemma 3.5], thanks to Remark 2.4 and to [1, Proposition 1.62(b)] we have

λ=λChV(x)(B(0,1))=limiTx,riϕ(B(0,1))rih=limiϕ(B(x,ri))rih,

and this concludes the proof.

The above proposition has the following immediate consequence.

Corollary 2.21

Let h{1,,Q} and assume ϕ is a Ph-rectifiable. Then for ϕ-almost every xG, we have

Tanh(ϕ,x){λChW:λ[Θh(ϕ,x),Θh,(ϕ,x)]andWGr(h)}.

We introduce now a way to estimate how far two measures are.

Definition 2.20

Given ϕ and ψ two Radon measures on G, and given KG a compact set, we define

FK(ϕ,ψ):=supfdϕ-fdψ:fLip1+(K). 29

We also write Fx,r for FB(x,r).

Remark 2.7

With few computations that we omit, it is easy to see that Fx,r(ϕ,ψ)=rF0,1(Tx,rϕ,Tx,rψ). Furthermore, FK enjoys the triangle inequality, indeed if ϕ1,ϕ2,ϕ3 are Radon measures and fLip1+(K), then

|fdϕ1-fdϕ2||fdϕ1-fdϕ3|+|fdϕ3-fdϕ2|FK(ϕ1,ϕ2)+FK(ϕ2,ϕ3).

The arbitrariness of f concludes that FK(ϕ1,ϕ2)FK(ϕ1,ϕ3)+FK(ϕ3,ϕ2).

The proof of the following criterion is contained in [41, Proposition 1.10] and we omit the proof.

Proposition 2.22

Let {μi} be a sequence of Radon measures on G. Let μ be a Radon measure on G. The following are equivalent

  1. μiμ;

  2. FK(μi,μ)0, for every KG compact.

Now, we are going to define a functional that in some sense tells how far is a measure from being flat around a point xG and at a certain scale r>0.

Definition 2.21

For any xG, any h{1,,Q}, and any r>0, we define the functional:

dx,r(ϕ,M(h)):=infΘ>0,VGr(h)Fx,r(ϕ,ΘShxV)rh+1. 30

Furthermore, if G is a subset of the h-dimensional Grassmannian Gr(h), we also define

dx,r(ϕ,M(h,G)):=infΘ>0,VGFx,r(ϕ,ΘShxV)rh+1.

Remark 2.8

It is a routine computation to prove that, whenever hN and r>0 are fixed, the function xdx,r(ϕ,M(h,G)) is a continuous function. The proof can be reached as in [41, Item (ii) of Proposition 2.2]. Moreover, from the invariance property in Remark 2.7 and Proposition 2.9, if in (30) we use the measure ChxV, we obtain the same functional.

Proposition 2.23

Let ϕ be a Radon measure on G satisfying item (i) in Definition 2.18. Further, let G be a subfamily of Gr(h) and let M(h,G) be the set defined in (27). If, for ϕ-almost every xG, we have Tanh(ϕ,x)M(h,G), then, for ϕ-almost every xG, we have

limr0dx,r(ϕ,M(h,G))=0.

Proof

Let us fix xG a point for which Tanh(ϕ,x)M(h,G) and let us assume by contradiction that there exist ri0 such that, for some ε>0 we have

dx,ri(ϕ,M(h,G))>ε. 31

Since ϕ satisfies item (i) in Definition 2.18, we can use [1, Proposition 1.62(b)] and then, up to subsequences, there are Θ>0 and VG such that

ri-hTx,riϕΘShV. 32

Thus,

dx,ri(ϕ,M(h,G))=d0,1(ri-hTx,riϕ,M(h,G))F0,1(ri-hTx,riϕ,ΘShV)0,

where the first equality follows from the first part of Remark 2.7, and the last convergence follows from (32), and Proposition 2.22. This is in contradiction with (31).

Structure of Ph-Rectifiable Measures

In what follows we let G be a Carnot group of homogeneous dimension Q and we fix 1hQ. We endow G with a fixed homogeneous left-invariant distance. We also assume that ϕ is a fixed Radon measure on G and we suppose that it is supported on a compact set K . Moreover we fix ϑ,γN and we freely use the notation E(ϑ,γ) introduced in Definition2.9.

In this section, we prove Theorem 1.4 and an important step toward the proof of Corollary 1.5, see the statements in Theorem 3.4 and Theorem 3.5, respectively.

The first step in order to prove Theorem 1.4 is to observe the following general property that can be made quantitative at arbitrary points xE(ϑ,γ): if the measure ShxV, with VGr(h), is sufficiently near to ϕ in a precise Measure Theoretic sense at the scale r around x, then in some ball of center x and with radius comparable with r, the points in the set E(ϑ,γ) are not too distant from xV. Roughly speaking, if we denote with Fx,r the functional that measures the distance between measures on the ball B(xr), see Definition 2.20, we prove that the following implication holds

if there exist aΘ,δ>0such thatFx,r(ϕ,ΘShxV)δrh+1,thenE(ϑ,γ)B(x,r)B(xV,ω(δ)r)whereωis continuous andω(0)=0. 33

For the precise statement of (33), see Proposition 3.1. Let us remark that when ϕ is a Ph-rectifiable measure, then for ϕ-almost every xG the bound on Fx,r in the premise of (33) is satisfied with V(x)Gr(h), for arbitrarily small δ>0 whenever r<r0(x,δ). Thus, for Ph-rectifiable measures, we deduce that the estimate in the conclusion of (33) holds for arbitrarily small δ, and with r<r0(x,δ). This latter estimate easily implies, by a very general geometric argument, that E(ϑ,γ)B(x,r)xCV(x)(α) for arbitrarily small α and for all r<r0(x,α). For the latter assertion, we refer the reader to Proposition 3.2. The proof of Theorem 1.4 is thus concluded by joining together the previous observations and by the general cone-rectifiability criterion in Proposition 3.3.

There is a difference between the Euclidean case and the Carnot case that we discuss now. In the Euclidean case, it is easy to see that whenever we are given a vector subspace V, an arbitrary CV(α)-set, with α sufficiently small, is actually the graph of a (Lipschitz) map f:AVV. The main reason behind this latter statement is the following: we have a canonical choice of a complementary subgroup V of V, and moreover VCV(α)={0} for α small enough. Already in the first Heisenberg group H1 if we take the vertical line VH1, we notice that there is no choice of a complementary subgroup of VH1 in H1. One could try to bypass this problem by defining properly some coset projections that would play the role of the projection over a splitting, see Definition 2.13. This will be the topic of further investigations.

Nevertheless, if we work in an arbitrary Carnot group G and one of its homogeneous subgroups V admits a complementary subgroup L, we already proved that there exists a constant ε1:=ε1(V,L) such that every CV(ε1)-set is the intrinsic graph of a function f:AVL. This last statement is precisely the analogous of the Euclidean property that we discussed above, see Proposition 2.17. As a consequence, in order to start to prove Theorem 1.5 we follow the path of the proof of Theorem 1.4, which we discussed above, but we have to pay attention to one technical detail. We have to split the subset of the Grassmannian Gr(h) made by the homogeneous subgroups V that admit at least one complementary subgroup L into countable subsets according to the value of ε1(V,L). Then we have to write the proof of Theorem 1.4 by paying attention to the fact that we want to control the opening of the final CVi(αi)-sets with αi<ε1(Vi,Li). This is what we do in Theorem 3.4: we prove a refinement of Theorem 3.5 in which we further ask that the opening of the cones is controlled above also by some a priori defined function F(V,L).

Definition 3.1

Let us fix xG, r>0 and ϕ a Radon measure on G. We define Πδ(x,r) to be the subset of planes VGr(h) for which there exists Θ>0 such that

Fx,r(ϕ,ΘShxV)2δrh+1. 34

Definition 3.2

For any ϑN, we define δG=δG(h,ϑ):=ϑ-12-(4h+5).

In the following proposition, we prove that if ϕ is sufficiently dx,r-near to M(h), see Definition 2.21 for the definition of dx,r, then E(ϑ,γ) is at a controlled distance from a plane V.

Proposition 3.1

Let xE(ϑ,γ), fix δ<δG, where δG is defined in Definition 3.2, and set 0<r<1/γ. Then for every VΠδ(x,r), see Definition 3.1, we have

supwE(ϑ,γ)B(x,r/4)dist(w,xV)r21+1/(h+1)ϑ1/(h+1)δ1/(h+1)=:C4(ϑ,h)δ1/(h+1). 35

Proof

Let V be any element of Πδ(x,r) and suppose Θ>0 is such that

|fdϕ-ΘfdShxV|2δrh+1,for anyfLip1+(B(x,r)).

Since the function g(w):=min{dist(w,U(x,r)c),dist(w,xV)} belongs to

Lip1+(B(x,r)), we deduce that

2δrh+1g(w)dϕ(w)-Θg(w)dShxV=g(w)dϕ(w)B(x,r/2)min{r/2,dist(w,xV)}dϕ(w).

Suppose that y is a point in B(x,r/4)E(ϑ,γ) furthest from xV and let D:=dist(y,xV). If Dr/8, this would imply that

2δrh+1B(x,r/2)min{r/2,dist(w,xV)}dϕ(w)B(y,r/16)min{r/2,dist(w,xV)}dϕ(w)r16ϕ(B(y,r/16))rh+1ϑ16h+1,

where the last inequality follows from the definition of E(ϑ,γ) and the fact that 0<r<1/γ. The previous inequality would imply δϑ-12-(4h+5), which is not possible since δ<δG=ϑ-12-(4h+5), see Definition 3.2. This implies that Dr/8 and as a consequence, we have

2δrh+1B(x,r/2)min{r/2,dist(w,xV)}dϕ(w)B(y,D/2)min{r/2,dist(w,xV)}dϕ(w)Dϕ(B(y,D/2))2ϑ-1D2h+1, 36

where the second inequality comes from the fact that B(y,D/2)B(x,r/2). This implies thanks to (36), that

supwE(ϑ,γ)B(x,r/4)dist(w,xV)rDr21+1/(h+1)ϑ1/(h+1)δ1/(h+1)=C5(ϑ,h)δ1/(h+1).

Remark 3.1

Notice that a priori Πδ(x,r) in the statement of Proposition 3.1 may be empty. Nevertheless, it is easy to notice, by using the definitions, that if dx,r(ϕ,M)δ then Πδ(x,r) is nonempty.

In the following proposition, we show that if we are at a point xE(ϑ,γ) for which the h-tangents are flat, then locally around x the set E(ϑ,γ) enjoys an appropriate cone property with arbitrarily small opening.

Proposition 3.2

For any α>0 and any xE(ϑ,γ) for which Tanh(ϕ,x){λShV(x):λ>0} for some V(x)Gr(h), there exists a ρ(α,x)>0 such that whenever 0<r<ρ we have

E(ϑ,γ)B(x,r)xCV(x)(α).

Proof

By using Proposition 2.23, we conclude that

limr0infΘ>0Fx,r(ϕ,ΘShxV(x))rh+1=0.

From the previous equality, it follows that for every ε>0 there exists 1/γ>r0(ε)>0 such that

infΘ>0Fx,r(ϕ,ΘShxV(x))εrh+1,whenever0<rr0(ε). 37

Now we aim at proving that, for ε>0 small enough, E(ϑ,γ)B(x,r0(ε)/4)xCV(x)(α). In order to prove this, we notice that (37) and Proposition 3.1 imply that, for ε>0 sufficiently small, the following inequality holds

suppE(ϑ,γ)B(x,r/4)dist(p,xV(x))C5(h,ϑ)ε1/(h+1)r,whenever0<rr0(ε). 38

Indeed, from (37), it follows that V(x)Πε(x,r) for every 0<rr0, see Definition 3.1; so that it suffices to choose ε<δG=ϑ-12-(4h+5), see Definition 3.2, in order to apply Proposition 3.1 and conclude (38).

Now let us take ε<δG so small that the inequality 8C5(h,ϑ)ε1/(h+1)<α holds. We finally prove E(ϑ,γ)B(x,r0(ε)/4)xCV(x)(α). Indeed, let pE(ϑ,γ)B(x,r0(ε)/4), and k3 be such that r02-k<x-1·pr02-k+1. Since pE(ϑ,γ)B(x,(r02-k+3)/4), from (38), we get

d(p,xV(x))C5(h,ϑ)ε1/(h+1)r02-k+38C5(h,ϑ)ε1/(h+1)x-1·pαx-1·p,

thus showing the claim.

We now prove a cone-type rectifiability criterion that will be useful in combination with the previous results in order to split the support of a Ph or a Phc-rectifiable measures with sets that have the cone property.

Proposition 3.3

(Cone-rectifiability criterion) Suppose that E is a closed subset of G for which there exists a countable family FGr(h) and a function α:F(0,1) such that for every xE, there exist ρ(x)>0, and V(x)F for which

B(x,r)ExCV(x)(α(V(x))), 39

whenever 0<r<ρ(x). Then, there are countably many compact CVi(3βi)-sets Γi such that ViF, and α(Vi)<βi<2α(Vi) for which

E=iNΓi. 40

Proof

Let us split E in the following way. Let G(ijk) be the subset of those xEB(0,k) for which

B(x,r)ExCVi(α(Vi)),

for any 0<r<1/j. Then, from the hypothesis, it follows E=i,j,kNG(i,j,k). Since E is closed, it is not difficult to see that G(ijk) is closed too. Let us fix i,j,kN, some βi<1 with α(Vi)<βi<2α(Vi), and let us prove that G(ijk) can be covered with countably many compact CVi(3βi)-sets. Since i,j,kN are fixed from now on, we assume without loss of generality that G(i,j,k)=E so that we can drop the indexes.

Let us take {q} a dense subset of E, and let us define the closed tubular neighborhood of qV

S():=B(qV,2-κj-κC1(14k)-κβκ), 41

where we recall that κ is the step of the group, and where C1 is defined in (2.1). We will now prove that S()E is a CV(3β)-set, or equivalently that for any pS()E we have

S()Ep·CV(3β). 42

If qS()EB(p,1/(2j)), the inclusion (42) holds thanks to our assumptions on E. If on the other hand qS()E\B(p,1/(3j)), let p,qV be such that d(p,qV)=(p)-1q-1p, and d(q,qV)=(q)-1q-1q. Let us prove that q4k and p4k. This is due to the fact that

q-q-q(q)-1q-1q=d(q,qV)1,

where the last inequality follows from the definition of S(), see (41). From the previous inequality, it follows that q2k+1, since q,qB(0,k). A similar computation proves the bound for p and this implies that

p-1·q·p+(p)-1·qp-1+q+2p+q14k.

The application of Lemma 2.1 and the fact that (q)-1p and p-1qp are in B(0, 14k), due to the previous inequality, imply that

d(p-1q,V)(q)-1p·p-1q=(q)-1p·p-1·qp(p)-1q(q)-1q-1·q(q)-1p·p-1qp·(p)-1q+(q)-1q-1qC1(14k)p-1qp1/κ+d(q,qV)=C1(14k)d(p,qV)1/κ+d(q,qV). 43

Finally, thanks to (41) and (43) we infer

d(p-1q,V)C1(14k)+12jC1(14k)ββj-13βp-1q,

thus showing (42) in the remaining case. In conclusion, we have proved that for any i,j,k,N, the sets G(i,j,k)S() are CVi(3βi)-sets. This concludes the proof since

Ei,j,k,NG(i,j,k)S(),

and on the other hand, every G(i,j,k)S() is a bounded and closed, thus compact, CVi(3βi)-set. The fact that the sets G(i,j,k)S() are contained in E follows by definition, thus concluding the proof of the equality.

In the following, with the symbol Sub(h), we denote the subset of Grc(h)×Grc(Q-h) defined by

{(V,L):VGrc(h)andLis a homogeneous subgroup complementary toV}, 44

we fix a function F:Sub(h)(0,1), and for every N with 2 let us define

GrcF(h,):={VGrc(h):Lcomplement ofVs.t.1/<F(V,L)1/(-1)}.

Observe that Proposition 2.7 implies that GrcF(h,) is separable for any N, since GrcF(h,)Gr(h) and (Gr(h),dG) is a compact metric space, see Proposition 2.7. Let

D:={Vi,}iN, 45

be a countable dense subset of GrcF(h,) and

for alliN,choose a complementLi,ofVi,s.t.1/<F(Vi,,Li,)1/(-1). 46

Let us now prove the following theorem which will be of fundamental importance to prove Corollary 1.5.

Theorem 3.4

Let F:Sub(h)(0,1) be a function, where Sub(h) is defined in (44), and for every N define D as in (45), set F:={Vi,}i,N, and choose Li, as in (46). Furthermore, let β:N(0,1) and define β(Vi,):=β() for every i,N. For the ease of notation we rename F:={Vk}kN. Then the following holds.

Let ϕ be a Phc-rectifiable measure. There are countably many compact sets Γk that are CVk(min{F(Vk,Lk),β(Vk)})-sets for some VkF, and such that

ϕ(G\k=1+Γk)=0.

Proof

Let us notice that without loss of generality, by restricting the measure on balls with integer radius, we can suppose that ϕ has a compact support. Fix ϑ,γN and let E(ϑ,γ) be the set introduced in Definition 2.9 with respect to ϕ. Furthermore, for any ,i,jN, we let

F(i,j):={xE(ϑ,γ):B(x,r)E(ϑ,γ)xCVi,(6-1min{F(Vi,,Li,),β(Vi,)for any0<r<1/j}. 47

It is not hard to prove, since E(ϑ,γ) is compact, see Proposition 2.4, that for every ,i,j, the sets F(i,j) are compact. We claim that

ϕ(E(ϑ,γ)\,i,jNF(i,j))=0. 48

Indeed, let wE(ϑ,γ) be such that Tanh(ϕ,w){λShV(w):λ>0} for some V(w)Grc(h); this can be done for ϕ-almost every point w in E(ϑ,γ) since ϕ is Phc-rectifiable. Let (w)N be the smallest natural number for which there exists L complementary to V(w) with 1/(w)<F(V(w),L)1/((w)-1). Then by definition, we have V(w)GrcF(h,(w)). By density of the family D(w) in GrcF(h,(w)), there exists a plane Vi,(w)D(w) such that

dG(Vi,(w),V(w))<30-1min{1/(w),β(Vi,(w))};

for this last observation to hold it is important that β only depends on (w), as it is by construction. The previous inequality, jointly with Lemma 2.14, imply that

CV(w)(30-1min{1/(w),β(Vi,(w))})CVi,(w)(6-1min{1/(w),β(Vi,(w))})CVi,(w)(6-1min{F(Vi,(w),Li,(w)),β(Vi,(w))}), 49

where the last inclusion follows from the fact that by definition of the family D(w) it holds F(Vi,(w),Li,(w))>1/(w). Thanks to Proposition 3.2, we can find a ρ(w)>0 such that for any 0<r<ρ(w), we have

B(w,r)E(ϑ,γ)wCV(w)(30-1min{1/(w),β(Vi,(w))}). 50

In particular, putting together (49) and (50), we infer that for ϕ-almost every wE(ϑ,γ), there are an i=i(w)>0, an (w)N, and a ρ(w)>0 such that whenever 0<r<ρ(w), we have

B(w,r)E(ϑ,γ)wCVi,(w)(6-1min{F(Vi,(w),Li,(w)),β(Vi,(w))}).

This concludes the proof of (48).

Now, if we fix ,i,jN, we can apply Proposition 3.3 to the set F(i,j). It suffices to take the family F in the statement of Proposition 3.3 to be the singleton {Vi,} and the function α in the statement of Proposition 3.3 to be α(Vi,):=6-1min{F(Vi,,Li,),β(Vi,)}. As a consequence we can write each F(i,j) as the union of countably many compact CVi,(min{F(Vi,,Li,),β(Vi,)})-sets. Thus, the same holds ϕ-almost everywhere for E(ϑ,γ), allowing i, to vary in N, since (48) holds. Finally, we have

ϕ(G\ϑ,γNE(ϑ,γ))=0,

due to Proposition 2.5.

Thus, we can cover ϕ-almost all of G with compact CVi,(min{F(Vi,,Li,),β(Vi,)})-sets for i, that vary in N, concluding the proof of the proposition.

The following theorem is a more detailed version of Theorem 1.4.

Theorem 3.5

There exists a countable subfamily F:={Vk}kN of Gr(h) such that the following holds. Let ϕ be a Ph-rectifiable measure. For any 0<β<1, there are countably many compact sets Γk that are CVk(β)-sets for some VkF, and such that

ϕ(G\k=1+Γk)=0.

Proof

The proof is similar to the one of Theorem 3.4. It suffices to choose, as a family F, an arbitrary countable dense subset of Gr(h) and then one can argue as in the proof of Theorem 3.4 without the technical effort of introducing the parameter . We skip the details.

Bounds for the Densities of Sh on CV(α)-Sets

Throughout this subsection, we assume that VGrc(h) and that V·L=G. In this chapter whenever we deal with CV(α)-sets we are always assuming that α<ε1(V,L), where ε1 is defined in Lemma 2.15.

This section is devoted to the proof of Theorem 1.3, that is obtained through three different steps. Let Γ be a compact CV(ε1(V,L)) set, and recall that by Proposition 2.17 we can write Γ=graph(φ) with φ:PV(Γ)L. Let us denote Φ(v):=v·φ(v) for every vPV(Γ).

We first show that if we assume that Θh(ShΓ,x)>0 at ShΓ-almost every point x, then the push-forward measure (Φ)(ShV) is mutually absolutely continuous with respect to ShΓ, see Proposition 4.7. In other words we are proving that whenever an intrinsically Lipschitz graph over a subset of an h-dimensional subgroup has strictly positive lower density almost everywhere, then the push-forward of the measure Sh on the subgroup by means of the graph map is mutually absolutely continuous with respect to the measure Sh on the graph. We stress that we do not address the issue of removing the hypothesis on the strict positivity of the lower density in Proposition 4.7 as it is out of the aims of this paper. We remark that in the Euclidean case the analogous statement holds true without this assumption: this is true because in the Euclidean case every Lipschitz graph over a subset of a vector subspace of dimension h has strictly positive lower h-density almost everywhere. We also stress that every intrinsically Lipschitz graph over a open subset of a h-dimensional homogeneous subgroups has strictly positive lower h-density almost everywhere, see [15, Theorem 3.9].

As a second step in order to obtain the proof of Theorem 1.3, we prove the following statement that can be made quantitative: if VGrc(h), Γ is a compact CV(α)-set with α sufficiently small, and ShΓ is a Ph-rectifiable measure with complemented tangents, which we called Phc-rectifiable, then we can give an explicit lower bound of the ratio of the lower and upper h-densities of ShΓ. We refer the reader to Proposition 4.11 for a more precise statement and the proof of the following proposition.

Proposition 4.1

(Bounds on the ratio of the densities) Let V be in Grc(h). There exists C:=C(V) such that the following holds. Suppose Γ is a compact CV(α)-set with α<C(V) and such that ShΓ is a Phc-rectifiable measure. Then there exists a continuous function ω:=ω(V) of α, with ω(0)=0, such that for Sh-almost every xΓ we have

1-ω(α)Θh(ShΓ,x)Θh,(ShΓ,x)1. 51

The previous result is obtained through a blow-up analysis and a careful use of the mutually absolute continuity property that we discussed above, and which is contained in Proposition 4.7. We stress that in order to differentiate in the proof of Proposition 4.1, we need to use proper ShPV(Γ) and ShV-Vitali relations, see Proposition 4.9, and Proposition 4.10, respectively.

As a last step of the proof of Theorem 1.3, we first use the result in Proposition 4.1 in order to prove that Theorem1.3 holds true for measures of the type ShΓ, see Theorem 4.13. Then, we conclude the proof for arbitrary measures by reducing ourselves to the sets E(ϑ,γ), see Corollary 4.14. The last part about the convergence in Theorem1.3 readily comes from the first part and Proposition 2.20.

We start this chapter with some lemmata.

Lemma 4.2

There exists an A:=A(V,L)>1 such that for any wB(0,1/5A), any yB(0,1)CV(ε1(V,L)) and any zB(y,1/5A), we have w-1zL.

Proof

By contradiction let us assume that we can find sequences {wn}, {yn}B(0,1)CV(ε1) and znB(yn,1/n) such that wn converges to 0 and wn-1znL. By compactness without loss of generality we can assume that the sequence yn converges to some yB(0,1)CV(ε1). Furthermore, by construction we also have that zn must converge to y. This implies that wn-1zn converges to y and since by hypothesis wn-1znL, thanks to the fact that L is closed we infer that yL. This, however, is a contradiction since y has unit norm and at the same time we should have yCV(ε1)L={0} by Lemma 2.15.

Proposition 4.3

Let α<ε1(V,L) and suppose Γ is a compact CV(α)-set. For any xΓ let ρ(x) to be the biggest number satisfying the following condition. For any yB(x,ρ(x))Γ we have

PV(B(x,r))PV(B(y,s))=for anyr,s<d(x,y)/5A,

where A=A(V,L) is the constant yielded by Lemma 4.2. Then, the function xρ(x) is positive everywhere on Γ and upper semicontinuous.

Proof

Let xΓ and suppose by contradiction that there is a sequence of points {yi}iNΓ converging to x and

PV(B(x,ri))PV(B(yi,si)), 52

for some ri,si<d(x,yi)/5A. We note that (52) is equivalent to assuming that there are ziB(x,ri) and wiB(yi,si) such that

PV(wi)=PV(zi). 53

Identity (53) implies in particular that for any iN, we have wi-1ziL and let us denote ρi:=d(x,yi). Thanks to the assumptions on yi,zi and wi, we have that

  1. d(0,δ1/ρi(x-1yi))=1 and thus we can assume without loss of generality that there exists a yB(0,1) such that
    limiδ1/ρi(x-1yi)=y,
  2. d(0,δ1/ρi(x-1zi))1/5A and thus up to passing to a non-re-labeled subsequence, we can assume that there exists a zB(0,1/5A) such that
    limiδ1/ρi(x-1zi)=z,
  3. d(δ1/ρi(x-1yi),δ1/ρi(x-1wi))1/5A and thus, up to passing to a non-re-labeled subsequence, we can suppose that there exists a wB(y,1/5A) such that
    limiδ1/ρi(x-1wi)=w.

Since Γ is supposed to be a CV(α)-set, we have that for any iN the point x-1yi is contained in the cone CV(α) and, since CV(α) is closed, we infer that yCV(α). Since we assumed α<ε1(V,L), we have yB(0,1)CV(ε1(V,L)). Since δ1/ρi(x-1zi) and δ1/ρi(x-1wi) converge to z and w, respectively, we have

limiδ1/ρi(wi-1zi)=limiδ1/ρi(wi-1x)δ1/ρi(x-1zi)=w-1z.

Furthermore since wi-1ziL for any iN, we infer that w-1zL since L is closed. Applying Lemma 4.2 to yzw, we see that the fact that w-1zL, zB(0,1/5A) and wB(y,1/5A) results in a contradiction. This concludes the proof of the first part of the proposition.

In order to show that ρ is upper semicontinuous, we fix an xΓ and we assume by contradiction that there exists a sequence {xi}iNΓ converging to x such that

lim supiρ(xi)>(1+τ)ρ(x), 54

for some τ>0. Fix an yB(x,(1+τ/2)ρ(x))Γ and assume s,r<d(x,y)/5A. Thus, thanks to (54) and the fact that the xi converge to x, we infer that there exists a i0N such that, up to non-re-labeled subsequences, for any ii0, we have ρ(xi)>(1+τ)ρ(x), d(xi,x)<τρ(x)/4 and s,r+d(xi,x)<d(xi,y)/5A. Therefore, for any ii0, we have

yB(xi,(1+3τ/4)ρ(x))B(xi,ρ(xi)),ands,r+d(xi,x)<d(xi,y)/5A.

This, however, thanks to the definition of ρ(xi), implies that

PV(B(x,r))PV(B(y,s))PV(B(xi,r+d(xi,x)))PV(B(y,s))=.

Summing up, we have proved that for any yB(x,(1+τ/2)ρ(x))Γ whenever r,s<d(x,y)/5A we have

PV(B(x,r))PV(B(y,s))=,

and this contradicts the maximality of ρ(x). This concludes the proof.

Corollary 4.4

Let us fix α<ε1(V,L) and suppose that Γ is a compact CV(α)-set. Let us fix xΓ and choose ρ(x)>0 as in the statement of Proposition 4.3. Then there is a 0<r(x)<1/2 such that the following holds

if0<r<r(x)andyΓare such thatPV(B(x,2r))PV(B(y,10r)),thenyB(x,ρ(x))andd(x,y)50Ar, 55

where A=A(V,L) is the constant yielded by Lemma 4.2.

Proof

Let us first prove that there exists α~:=α~(α,x) such that whenever yΓ is such that d(x,y)ρ(x) then d(PV(x),PV(y))α~. Indeed if it is not the case, we have a sequence {yi}iNΓ such that d(x,yi)ρ(x) for every iN and d(PV(x),PV(yi))0 as i+. Since Γ is compact, we can suppose, up to passing to a non-re-labeled subsequence, that yiyΓ. Moreover, since d(x,yi)ρ(x) and d(PV(x),PV(yi))0, we conclude that d(x,y)ρ(x), and hence xy, and moreover PV(x)=PV(y). Then y-1·xLCV(α) that is a contradiction with Lemma 2.15 because yx and α<ε1.

Since PV is uniformly continuous on the closed tubular neighborhood B(Γ,1), there exists a r(x)>0 depending on α~=α~(α,x) such that for any yΓ and any r<r(x), we have

PV(B(y,10r))B(PV(y),α~/10). 56

Let us show the first part of the statement. It is sufficient to prove that if r<r(x) and yΓ is such that d(x,y)ρ(x), then PV(B(x,2r))PV(B(y,10r))=. Indeed if d(x,y)ρ(x) then d(PV(x),PV(y))α~. Moreover, from (56), we deduce that PV(B(x,10r))B(PV(x),α~/10) and PV(B(y,10r))B(PV(y),α~/10). Since d(PV(x),PV(y))α~, we conclude that B(PV(x),α~/10)B(PV(y),α~/10)= and then also PV(B(x,10r))PV(B(y,10r))=, from which the sought conclusion follows. In order to prove d(x,y)50Ar, once we have yB(x,ρ(x)), the conclusion follows thanks to Proposition 4.3.

Lemma 4.5

Fix some NN and assume that F is a family of closed balls of G with uniformly bounded radii. Then we can find a countable disjoint subfamily G of F such that

  • (i)

    if B,BG then 5NB and 5NB are disjoint,

  • (ii)

    BFBBG5N+1B.

Proof

If N=0, there is nothing to prove, since it is the classical 5-Vitali’s covering Lemma.

Let us assume by inductive hypothesis that the claim holds for N=k and let us prove that it holds for k+1. Let Gk be the family of balls satisfying (i) and (ii) for N=k, and apply the 5-Vitali’s covering Lemma to the family of balls F~:={5k+1B:BGk}. We obtain a countable subfamily G~ of F~ such that if 5k+1B,5k+1BG~ then 5k+1B and 5k+1B are disjoint and that satisfies BF~BBG~5B. Therefore, if we define

Gk+1:={BGk:5k+1BG~},

point (i) directly follows and thanks to the inductive hypothesis we have

BFBBGk5k+1BBGk+15k+2B,

proving the second point of the statement.

Proposition 4.6

Let α<ε1(V,L) and suppose Γ is a compact CV(α)-set of finite Sh-measure such that

Θh(ShΓ,x)>0,

for Sh-almost every xΓ. Then, there exists a constant C6>0 depending on V, L, and the left-invariant homogeneous distance on G, such that for Sh-almost every xΓ there exists an R:=R(x)>0 such that for any 0<R we have

Sh(PV(ΓB(x,)))C6Θh(ShΓ,x)2h. 57

Proof

First of all, let us recall that two homogeneous left-invariant distances are always bi-Lipschitz equivalent on G. Therefore if dc is a Carnot-Carathéodory distance on G, which is in particular geodesic, see [29, Sect. 3.3] there exists a constant L(d,dc)1 such that

L(d,dc)-1dc(x,y)d(x,y)L(d,dc)dc(x,y)for anyx,yG.

We claim that if for any ϑ,γN for which Sh(E(ϑ,γ))>0 we have that for Sh-almost any wE(ϑ,γ) there exists a R(w)>0 such that

Sh(PV(ΓB(w,)))C4(V,L)h8·53hAhL(d,dc)2hϑ2, 58

whenever 0<<R(w), then the proposition is proved. This is due to the following reasoning. First of all, thanks to [13, Proposition 2.10.19(5)], we know that Θh,(ShΓ,x)1. Secondly, if we set, for any kN, Γk:={wΓ:1/(k+1)<Θh(ShΓ,x)1/k}, we have that

Sh(Γ\kNΓk)=0. 59

We observe now that if Sh(Γk)>0, then Sh-almost every wΓk belongs to some E(k+1,γ) provided γ is big enough, or in other words

Sh(Γk\γNE(k+1,γ))=0. 60

If our claim (58) holds true, whenever Sh(E(k+1,γ))>0, we have that for ShE(k+1,γ)-almost every w there exists R(w) such that whenever 0<<R(w) the following chain of inequalities holds

Sh(PV(ΓB(w,)))C4(V,L)h8·53hAhL(d,dc)2h(k+1)2C4(V,L)h25·53hAhL(d,dc)2hk2C4(V,L)Θh(ShΓ,x)2h25·53hAhL(d,dc)2h=C6Θh(ShΓ,x)2h. 61

Identities (59) and (60) together with (61) imply that our claim suffices to prove the proposition. Therefore, in the following we will assume that ϑ,γN are fixed and such that Sh(E(ϑ,γ))>0, and we want to prove (58).

Let NN be the unique natural number for which 5N-2AL(d,dc)2<5N-1 and for any kN and 0<δ<1/2 we define the following sets, where ρ(x) is defined in Proposition 4.3,

Aϑ,γ(k):={xE(ϑ,γ):ρ(x)>1/k},Dϑ,γ(k):={xAϑ,γ(k):limr0Sh(B(x,r)Aϑ,γ(k))Sh(B(x,r)E(ϑ,γ))=1},Fδ(k):={B(x,r):xDϑ,γ(k)andrmin{ϑ-1,γ-1,k-1,δ}1000AL(d,dc)2}.

For any ϑ,γN the sets Aϑ,γ(k) are Borel since thanks to Proposition 4.3, the function ρ is upper semicontinuous. Before going on, we observe that ShE(ϑ,γ)(Aϑ,γ(k)\Dϑ,γ(k))=0. This comes from the fact that the points of Dϑ,γ(k) are exactly the points of density one of Aϑ,γ(k) with respect to the measure ShE(ϑ,γ), that is asymptotically doubling at ShE(ϑ,γ)-almost every point because it has positive lower density and finite upper density at ShE(ϑ,γ)-almost every point, see Proposition 2.2. Moreover observe that from Proposition 4.3Sh(E(ϑ,γ)\k=1+Aϑ,γ(k))=0. Let us apply Lemma 4.5 to N and Fδ(k), and thus we infer that there exists a subfamily Gδ(k) such that

(α)

for any B,BGδ(k) we have that 5NB5NB=,

(β)

BFδ(k)BBGδ(k)5N+1B.

The point (α) above implies in particular that whenever B(x,r),B(y,s)Gδ(k), we have d(x,y)>L(d,dc)-25N(r+s), since d is L(d,dc)-Lipschitz equivalent to the geodesic distance dc, and thanks to the choice of N, we deduce that

r+s<d(x,y)5A.

Throughout the rest of the proof, we fix a wDϑ,γ(k) and a

0<R(w)<min{ϑ-1,γ-1,k-1}/8,

such that

ShΓ(B(w,))h12ϑ,andShDϑ,γ(k)(B(w,))ShΓ(B(w,))12,for any0<R(w). 62

For the ease of notation, we continue the proof fixing the radius =R(w)=R. We stress that the forthcoming estimates are verified, mutatis mutandis, also for any 0<<R. The first inequality above comes from the definition of E(ϑ,γ), see Definition 2.9, while the second is true, up to choose a sufficiently small R(w), because ShΓ-almost every point of Dϑ,γ(k) has density one with respect to the asymptotically doubling measure ShΓ. Let us stress that if we prove our initial claim for such w and R(w) we are done since ShΓ-every point of Dϑ,γ(k) satisfies (62), ShE(ϑ,γ)(Aϑ,γ(k)\Dϑ,γ(k))=0, and Sh(E(ϑ,γ)\k=1+Aϑ,γ(k))=0.

Let us notice that the definition of Fδ(k) implies that there must exist a ball BGδ(k) such that w5N+1B. We now prove that for any couple of closed balls B(x,r),B(y,s)Gδ(k) such that B(wR) intersects both B(x,5N+1r) and B(y,5N+1s), we have

PV(B(x,r))PV(B(y,s))=. 63

Indeed, Suppose that pB(x,5N+1r)B(w,R) and note that

d(x,w)d(x,p)+d(p,w)R+5N+1r(18+5N+11000AL(d,dc)2)min{ϑ-1,γ-1,k-1}min{ϑ-1,γ-1,k-1}4, 64

where the last inequality comes from the choice of N. The bound (64) shows in particular that

d(x,y)d(x,w)+d(w,y)min{ϑ-1,γ-1,k-1}2<ρ(x),

where the last inequality comes from the fact that by construction x is supposed to be in Dϑ,γ(k). Thanks to the fact that r+s<d(x,y)/5A and yB(x,ρ(x))E(ϑ,γ), we have that Proposition 4.3 implies that (63) holds.

In order to proceed with the conclusion of the proof, let us define

Fδ(w,R):={BFδ(k):5N+1BB(w,R)Dϑ,γ(k)},Gδ(w,R):={BGδ(k):5N+1BB(w,R)Dϑ,γ(k)},

Thanks to our choice of R, see (62), and the definition of Gδ(w,R) we have

Rh2ϑShΓ(B(w,R))2ShDϑ,γ(k)(B(w,R))2ShDϑ,γ(k)(BGδ(w,R)5N+1B).

Let Gδ(w,R)={B(xi,ri)}iN and recall that xiDϑ,γ(k) and that 5N+1ri1/γ. This implies, thanks to Proposition 2.13, that

ShDϑ,γ(k)(BGδ(w,R)5N+1B)2ϑ5h(N+1)iNrih=2ϑ5h(N+1)C4(V,L)-1iNSh(PV(B(xi,ri)))=2ϑ5h(N+1)C4(V,L)-1Sh(PV(iNB(xi,ri)))2ϑ5h(N+1)C4(V,L)-1Sh(PV(BFδ(w,R)B)),

where the first inequality comes from the subadditivity and the upper estimate that we have in the definition of E(ϑ,γ), see Definition 2.9, while identity in the third line above comes from (63). Summing up, for any δ>0 we have

C4(V,L)Rh8·5h(N+1)ϑ2Sh(PV(BFδ(w,R)B)).

We now prove that the projection under PV of the closure of BFδ(w,R)B converges in the Hausdorff sense to PV(Dϑ,γ(k)B(w,R)¯) as δ goes to 0. Since the set BFδ(w,R)B is a covering of Dϑ,γ(k)B(w,R) we have that

Dϑ,γ(k)B(w,R)BFδ(w,R)B. 65

On the other hand, since by definition the balls of Fδ(w,R) have radii smaller than δ/4 and center in Dϑ,γ(k), we also have

BFδ(w,R)BB(Dϑ,γ(k)B(w,R),5N+2δ). 66

Putting together (65) and (66), we infer that the closure of BFδ(w,R)B converges in the Hausdorff metric to the closure of B(w,R)Dϑ,γ(k). Furthermore, since PV restricted to the ball B(w,R+1) is uniformly continuous, we infer that

PV(BFδ(w,R)B¯)HPV(Dϑ,γ(k)B(w,R)¯).

Thanks to the upper semicontinuity of the Lebesgue measure with respect to the Hausdorff convergence we eventually infer that

C4(V,L)Rh8·5h(N+1)ϑ2lim supδ0Sh(PV(BFδ(w,R)B¯))Sh(PV(Dϑ,γ(k)B(w,R)¯))Sh(PV(E(ϑ,γ)B(w,R))),

where the last inequality above comes from the fact that by construction Dϑ,γ(k)E(ϑ,γ) and the compactness of E(ϑ,γ). Finally, since C6=2-55-3hA-hL(d,dc)-2hC4(V,L), we infer

Sh(PV(E(ϑ,γ)B(w,R)))C4(V,L)Rh8·5h(N+1)ϑ24C6Rhϑ2,

thus showing the claim (58) and then the proof.

Proposition 4.7

Let us fix α<ε1(V,L) and suppose Γ is a compact CV(α)-set of finite Sh-measure such that

Θh(ShΓ,x)>0,

for Sh-almost every xΓ. Let us set φ:PV(Γ)L the map whose graph is Γ, see Proposition 2.17, and set Φ:PV(Γ)G to be the graph map of φ. Let us define ΦShV to be the measure on Γ such that for every measurable AΓ we have ΦShV(A):=ShV(Φ-1(A))=ShV(PV(A)). Then ΦShV is mutually absolutely continuous with respect to ShΓ.

Proof

The fact that ΦShV is absolutely continuous with respect to ShΓ is an immediate consequence of Proposition 2.13. Vice-versa, suppose by contradiction that there exists a compact subset C of Γ of positive Sh-measure such that

0=ΦShV(C)=Sh(PV(C)). 67

Since by assumption Θh(ShC,x)>0 for Sh-almost every xC, by Proposition 2.2 and the fact that C has positive and finite Sh-measure, we infer thanks to Proposition 4.6 that it must have a projection of positive Sh-measure. This, however, comes in contradiction with (67).

In the following propositions, we are going to introduce two fine coverings of PV(Γ) and V, respectively, that will be used in the proof of Proposition 4.1 to differentiate with respect to the measure ShPV(Γ).

Definition 4.1

(ϕ-Vitali relation) Let (Xd) be a metric space with a Borel measure ϕ on it and let B(X) be the family of Borel sets of X. We say that SX×B(X) is a covering relation if

S={(x,B):xBX}.

Furthermore for any ZX we let

S(Z):={B:(x,B)Sfor somexZ}. 68

Finally a covering S is said to be fine at xX if and only if

inf{diam(B):(x,B)S}=0.

By a ϕ-Vitali relation, we mean a covering relation that is fine at every point of X and the following condition holds

  • If C is a subset of S and Z is a subset of X such that C is fine at each point of Z, then C(Z) has a countable disjoint subfamily covering ϕ-almost all of Z.

If δ is a nonnegative function on S(X), for any BS(X) we define its δ-enlargement as

B^:={B:BS(X),BBandδ(B)5δ(B)}. 69

In the remaining part of this section, we use the following general result due to Federer: it contains a criterion to show that a fine covering relation is a ϕ-Vitali relation, and a Lebesgue theorem for ϕ-Vitali relations.

Proposition 4.8

( [13, Theorem 2.8.17, Corollary 2.9.9 and Theorem 2.9.11]) Let X be a metric space, and let ϕ be a Borel regular measure on X that is finite on bounded sets. Let S be a covering relation such that S(X) is a family of bounded closed sets, S is fine at each point of X, and let δ be a nonnegative function on S(X) such that

limε0+supδ(B)+ϕ(B^)ϕ(B):(x,B)S,diamB<ε<+,

for ϕ-almost every xX. Then S is a ϕ-Vitali relation.

Moreover, if S is a ϕ-Vitali relation on X, and f is a ϕ-measurable real-valued function with K|f|dϕ<+ on every bounded ϕ-measurable K, we have

limε0+supB|f(z)-f(x)|dϕ(z)ϕ(B):(x,B)S,diamB<ε=0,

for ϕ-almost every xX. In addition, given AX, if we define

P:=xX:limε0+infϕ(BA)ϕ(B):(x,B)S,diamB<ε=1,

then P is ϕ-measurable and ϕ(A\P)=0.

Proposition 4.9

Let α<ε1(V,L) and suppose that Γ is a compact CV(α)-set of finite Sh-measure such that

Θh(ShΓ,x)>0,

for Sh-almost every xΓ. As in the statement of Proposition 4.7, let us denote with Φ:PV(Γ)G the graph map of φ:PV(Γ)L whose intrinsic graph is Γ. Then the covering relation

S1:={(z,PV(B(Φ(z),r)Γ)):zPV(Γ)and0<r<min{1,R(Φ(z))}},

is a ShPV(Γ)-Vitali relation, where R(Φ(z)) is defined as in Proposition 4.6 for ShPV(Γ)-almost every zV and it is + on the remaining null set where Proposition 4.6 eventually does not hold.

Proof

First of all, it is readily noticed that S1 is a fine covering of PV(Γ) sine PV is continuous. Let us prove that S1 is a ShPV(Γ)-Vitali relation in (PV(Γ),d) with the distance d induced form G. For xPV(Γ) and r>0, define G(x,r):=PV(B(Φ(x),r)Γ). Notice that an arbitrary element of S1(PV(Γ)), see (68), is of the form G(xr) for some xPV(Γ) and some 0<r<min{1,R(Φ(x))}. Let δ(G(x,r)):=r and note that the δ-enlargement, see (69), of G(xr) is

G^(x,r):={G(y,s):yPV(Γ),0<s<min{1,R(Φ(y))},G(y,s)G(x,r)andδ(G(y,s))5δ(G(x,r))}={G(y,s):yPV(Γ),0<s<min{1,R(Φ(y))},G(y,s)G(x,r)ands5r}. 70

Whenever G(x,r)G(y,s) we have that d(Φ(x),Φ(y))r+s: indeed, since PV is injective on Γ, see Proposition 2.17, we have PV(B(Φ(x),r)Γ)PV(B(Φ(y),s)Γ) if and only if B(Φ(x),r)B(Φ(y),s)Γ. In particular, since s5r we have B(Φ(y),s)B(Φ(x),12r), and thus G^(x,r)G(x,12r) for every xPV(Γ) and 0<r<min{1,R(Φ(x))}.

Finally, thanks to Proposition 4.6 and Proposition 4.7, for Sh-almost every xPV(Γ), we have

limξ0supδ(G(x,r))+Sh(G^(x,r))Sh(G(x,r)):0<r<min{1,R(Φ(x))},diam(G(x,r))ξ1+limξ0supSh(G(x,12r))Sh(G(x,r))1+limξ0supSh(PV(B(Φ(x),12r)))Sh(PV(B(Φ(x),r)Γ))1+(12r)hSh(PV(B(0,1)))C6Θh(ShΓ,Φ(x))2rh=1+12hSh(PV(B(0,1)))C6Θh(ShΓ,Φ(x))2, 71

where we explicitly mentioned the set over which we take the supremum only in the first line for the ease of notation, and where the first inequality in the third line follows from the fact that Sh(PV(E))=Sh(PV(xE)) for any xG and any Borel set EG, see Proposition 2.10. Thanks to (71), we can apply the first part of Proposition 4.8 and thus we infer that S1 is a ShPV(Γ)-Vitali relation.

Proposition 4.10

Let α<ε1(V,L) and let Γ be a compact CV(α)-set of finite Sh-measure. As in the statement of Proposition 4.7, let us denote with Φ:PV(Γ)G the graph map of φ:PV(Γ)L whose intrinsic graph is Γ. Then for Sh-almost every wPV(Γ), we have

limr0Sh(PV(B(Φ(w),r)Φ(w)CV(α))PV(Γ))Sh(PV(B(Φ(w),r)Φ(w)CV(α)))=1. 72

Proof

For any wV\PV(Γ), we let

ρ(w):=inf{r0:B(w,r)PV(B(Γ,r1/κ))}.

It is immediate to see that ρ(w)dist(w,PV(Γ)) and that ρ(w)=0 if and only if wPV(Γ). Throughout the rest of the proof we let S be the fine covering of V given by the couples (wG(wr)) for which

(α)

if wV\PV(Γ) then r(0,min{ρ(w)/2,1}) and G(w,r):=B(w,r)V,

(β)

if wPV(Γ) then r(0,1) and G(w,r):=PV(B(Φ(w),r)Φ(w)CV(α)).

Furthermore, for any wV, we define the function δ on S(V), see (68), as

δ(G(w,r)):=r. 73

If we prove that S is a ShV-Vitali relation, the second part of Proposition 4.8 directly implies that (72) holds. If for Sh-almost every wV, we prove that

limξ0sup(w,G(w,r))S,diam(G(w,r))ξδ(G(w,r))+Sh(G^(w,r))Sh(G(w,r))1+limξ0supSh(G^(w,r))Sh(G(w,r))<, 74

where we explicitly mentioned the set over which we take the supremum only the first time for the ease of notation, and where G^(w,r) is the δ-enlargement of G(wr), see (69); thus, thanks to the first part of Proposition 4.8 we would immediately infer that S is a ShV-Vitali relation. In order to prove that (74) holds, we need to get a better understanding of the geometric structure of the δ-enlargement of G(wr).

If wV\PV(Γ), we note that there must exist an 0<r(w)<min{ρ(w)/2,1} such that for any 0<r<r(w) we have

B(w,r)PV(B(Γ,5r))=.

Indeed, if this is not the case there would exist a sequence ri0 and a sequence {zi}iN such that

ziB(w,ri)PV(B(Γ,5ri)).

Since PV(Γ) is compact and PV is continuous on the closed tubular neighborhood B(Γ,1), up to passing to a non-re-labeled subsequence we have that the zi’s converge to some zPV(Γ) and, on the other hand, by construction the zi’s converge to w which is not contained in PV(Γ), and this is a contradiction. This implies that if 0<r<r(w), we have

G^(w,r)={G(y,s):yV,s>0,(y,G(y,s))S,G(y,s)G(w,r),ands5r}{B(y,s)V:B(y,s)B(w,r)Vands5r}B(w,11r)V, 75

where in the inclusion we are using the fact that if y were in PV(Γ), and s5r, then G(y,s)PV(B(Γ,s))PV(B(Γ,5r)) which would be in contradiction with G(y,s)G(w,r), since we chose 0<r<r(w). Summing up, if wV\PV(Γ) the bound (74) immediately follows thanks to (75) and the homogeneity of Sh.

If on the other hand wPV(Γ), the situation is more complicated. If yV\PV(Γ) and s5r are such that

G(y,s)PV(B(Φ(w),r))=B(y,s)PV(B(Φ(w),r)), 76

since by construction of the covering S we also assumed that 0<s<ρ(y)/2, we infer that we must have rs1/κ for (76) to be satisfied. This allows us to infer that, for every wPV(Γ) and 0<r<1, we have

G^(w,r)={G(y,s):yV,s>0,(y,G(y,s))S,G(y,s)G(w,r),ands5r}{PV(B(Φ(y),s)):yPV(Γ),PV(B(Φ(y),s))PV(B(Φ(w),r)),ands5r}{B(y,s)V:yV\PV(Γ),B(y,s)PV(B(Φ(w),r)),andsmin{5r,ρ(y)/2}}{PV(B(Φ(y),s)):yPV(Γ),PV(B(Φ(y),s))PV(B(Φ(w),r)),ands5r}B(PV(B(Φ(w),r)),3rκ)V, 77

where in the last inclusion we are using the observation right after (76) according to which srκ. We now study independently each of the two terms of the union of the last two lines above. Let us first note that if w,yPV(Γ), s5r and

PV(B(Φ(y),s))PV(B(Φ(w),r)),

then PV(B(Φ(y),10r))PV(B(Φ(w),2r)). This observation and Corollary 4.4 imply that if 0<r<r(w) is sufficiently small we have d(Φ(w),Φ(y))50Ar, where the constant A=A(V,L) is yielded by Lemma 4.2. In particular we deduce that for every 0<r<r(w) sufficiently small

{PV(B(Φ(y),s)):yPV(Γ),PV(B(Φ(y),s))PV(B(Φ(w),r)),ands5r}PV(B(Φ(w),50(A+1)r)).

In order to study the term in the last line of (77), we prove the following claim: for every 0<r<1, every zPV(B(Φ(w),r)), and every ΔB(0,3rκ)V we have zΔPV(B(Φ(w),C(Γ)r)), where C(Γ) is a constant depending only on Γ. Indeed, since Γ is compact and PL is continuous, there exists a constant K:=K(Γ) such that whenever 0<r<1, and zPV(B(Φ(w),r)), there exists an L such that zB(Φ(w),r) and K. Thus there exists a constant K:=K(Γ)>0 such that whenever 0<r<1, zPV(B(Φ(w),r)), and ΔB(0,3rκ)V, there exists L with zB(Φ(w),r) and Δ+K. Thus, we can estimate

d(Φ(w),zΔ)d(Φ(w),z)+d(z,zΔ)r+C1(K)Δ1/κC(Γ)r,

where the second inequality in the last equation comes from Lemma 2.1. Thus, zΔPV(B(Φ(w),C(Γ)r)), and the claim is proved. Summing up, we have proved that whenever wPV(Γ) and 0<r<r(w) is sufficiently small we have

G^(w,r)PV(B(Φ(w),50(A+1)r))PV(B(Φ(w),C(Γ)r)),

and thus (74) immediately follows by the homogeneity of ShV and the fact that Sh(PV(xE))=Sh(PV(E)) for every xG and E a Borel subset of G, see Proposition 2.10. This concludes the proof of the proposition.

We prove below a more precise version of Proposition 4.1.

Proposition 4.11

Let us fix α<ε1(V,L). Suppose Γ is a compact CV(α)-set such that ShΓ is Phc-rectifiable. For Sh-almost every xΓ we have

(1-c(α))2h(1+c(α))-hΘh(ShΓ,x)Θh,(ShΓ,x)1, 78

where c(α) is defined in Lemma 2.18.

Proof

Let us preliminarily observe that since ShV and ChV are both Haar measures on V, they coincide up to a constant. Since for Sh-almost every xΓ we have Θh,(ShΓ,x)>0, the upper bound is trivial. Let us proceed with the lower bound. Thanks to Proposition 4.7 and the Radon–Nikodym Theorem, see [23, page 82], there exists ρL1(ΦChV) such that

  • (i)

    ρ(x)>0 for ΦChV-almost every xΓ,

  • (ii)

    ShΓ=ρΦChV.

We stress that the following reasoning holds for ShΓ-almost every xΓ. Let {ri}iN be an infinitesimal sequence such that ri-hTx,riShΓλChV(x) for some λ>0. First of all, we immediately see that Corollary 2.21 implies that λ[Θh(ShΓ,x),Θh,(ShΓ,x)] and that

1=limiShΓ(B(x,ri))ShΓ(B(x,ri))=limiPV(B(x,ri)Γ)ρ(Φ(y))dChV(y)ShΓ(B(x,ri))=ρ(x)λlimiChV(PV(B(x,ri)Γ))rih,

where the last identity comes from Proposition 4.9 that allows us to differentiate by using the second part of Proposition 4.8, and Proposition 2.20. Thanks to Lemma 2.18, Remark 2.4, and the fact that Γ is a CV(α)-set, we have

λρ(x)limiChV(PV(B(x,ri)xCV(α)))rih=Ch(PV(B(0,1)CV(α)))ChV(B(0,1))(1-c(α))h=(1-c(α))-h, 79

where in the second equality we are using the homogeneity of Ch and the fact that Ch(PV(xE))=Ch(PV(E)) for every xG and E a Borel subset of G, see Proposition 2.10. On the other hand, thanks to Lemma 2.19 we have

λρ(x)=limiChV(PV(B(x,ri)Γ))rihlimiCh(PV(B(x,C(α)ri)xCV(α))PV(Γ))Ch(PV(B(x,C(α)ri)xCV(α)))Ch(PV(B(x,C(α)ri)xCV(α)))rih=C(α)hCh(PV(B(0,1)CV(α)))C(α)h, 80

where the first identity in the last line comes from Proposition 4.10 and the last inequality from Lemma 2.18, Remark 2.4, and C(α) is defined in (20). Putting together (79) and (80), we have

(1-c(α))h(1+c(α))hλρ(x)1(1-c(α))h. 81

Thanks to the definition of Θh(ShΓ,x) and Θh,(ShΓ,x) we can find two sequences {ri}iN and {si}iN such that

Θh(ShΓ,x)=limiShΓ(B(x,ri))rih,andΘh,(ShΓ,x)=limiShΓ(B(x,si))sih,

and without loss of generality, taking Proposition 2.20 into account, we can assume that

ri-hTx,riShΓΘh(ShΓ,x)ChV(x),,si-hTx,siShΓΘh,(ShΓ,x)ChV(x).

The bounds (81) imply therefore that

(1-c(α))h(1+c(α))hΘh(ShΓ,x)ρ(x)1(1-c(α))h,(1-c(α))h(1+c(α))hΘh,(ShΓ,x)ρ(x)1(1-c(α))h. 82

Finally the bounds in (82) yield

(1-c(α))2h(1+c(α))-hΘh(ShΓ,x)Θh,(ShΓ,x)1,

and this concludes the proof.

We prove now the existence of density of Phc-rectifiable measures, see Corollary 1.3. We first prove an algebraic lemma, then we prove the existence of the density for measures of the type ShΓ, and then we conclude with the proof of the existence of the density for arbitrary Phc-rectifiable measures.

Lemma 4.12

Let us fix 0<ε<1 a real number, ,hN, and let f be the function defined as follows

f:{(α,C)(0,+)2:α<C}(0,+),f(α,C):=αC-α.

Then, there exists α~:=α~(ε,,h)>0 such that the following implication holds

if0<αα~andC>1/,thenα<Cand(1-f(α,C))2h(1+f(α,C))-h1-ε.

Proof

Let us choose 0<ε~:=ε~(ε,h)<1 such that

(1-x)2h(1+x)-h1-ε,for all0xε~.

Let us show that the sought constant α~(ε,,h) is α~:=ε~/((1+ε~)). Indeed, if αα~ and C>1/ we infer that α<C and

αε~(1+ε~)Cε~1+ε~,and thenf(α,C)=αC-αε~.

This implies that if αα~ and C>1/, then

(1-f(α,C))2h(1+f(α,C))-h1-ε,

where the last inequality above comes from the choice of ε~. This concludes the proof.

Theorem 4.13

Let Γ be a compact subset of G such that ShΓ is a Phc-rectifiable measure. Then

0<Θh(ShΓ,x)=Θ,h(ShΓ,x)<+,forShΓ-almost everyxG.

Proof

In the following, for any ε>0, we will construct a measurable set AεΓ such that Sh(Γ\Aε)=0 and

1-εΘ,h(ShΓ,x)Θh(ShΓ,x)1,for everyxAε. 83

If (83) holds then we are free to choose ε=1/n for every nN and then the density of ShΓ exists on the set n=1+A1/n, that has full ShΓ-measure. So we are left to construct Aε as in (83). Let us define the function

F(V,L):=ε1(V,L),for allVGrc(h)with complementL.

Let us take the family F:={Vi}i=1+Grc(h) and let us choose Li complementary subgroups to Vi as in the statement of Theorem 3.4. We remark that the choices of the family F and of the complementary subgroups depend on the function F previously defined, see the discussion before Theorem 3.4. Let us define

β:N(0,1),β():=α~(ε,,h),

where α~(ε,,h) is the constant in Lemma 4.12, and with an abuse of notation let us lift β to a function on F as we did in the statement of Theorem 3.4. From Theorem 3.4 we conclude that there exist countably many Γi’s that are compact CVi(min{ε1(Vi,Li),β(Vi)})-sets contained in Γ such that

ShΓ\i=1+Γi=0. 84

Let us write, for the ease of notation, αi:=min{ε1(Vi,Li),β(Vi)} for every iN. Since ΓiΓ and ShΓ is Phc-rectifiable, we conclude, by exploiting the locality of tangents, see Proposition 2.3, and the Lebesgue differentiation theorem in Proposition 2.2, that the measures ShΓi are Phc-rectifiable as well for every iN. Thus, since αiε1(Vi,Li), we can apply Proposition 4.11 and conclude that, for every iN, we have

(1-c(αi))2h(1+c(αi))-hΘ,h(ShΓi,x)Θh(ShΓi,x)1,forShΓi-almost everyxG,

where c(αi):=αi/(C3(Vi,Li)-αi). Since Θ,h(ShΓi,x)=Θ,h(ShΓ,x) and Θh(ShΓi,x)=Θh(ShΓ,x) for ShΓi-almost every xG, see Proposition 2.2, for every iN we conclude that

(1-c(αi))2h(1+c(αi))-hΘ,h(ShΓ,x)Θh(ShΓ,x)1,forShΓi-almost everyxG. 85

Let us now fix iN and note there exists a unique (i)N such that

1/(i)<ε1(Vi,Li)1/((i)-1).

Moreover, from the definition of β and F we see that β(Vi)=β(ε,(i),h). This allows us to infer that

  1. αiβ(Vi)=β(ε,(i),h), since αi:=min{ε1(Vi,Li),β(Vi)},

  2. C3(Vi,Li)>1/(i), since 1/(i)<ε1(Vi,Li)=C3(Vi,Li)/2, see Lemma 2.15.

Thus we can apply Lemma 4.12 and conclude that

(1-c(αi))2h(1+c(αi))-h1-ε.

This shows, thanks to (85), that for any iN, we have

1-εΘ,h(ShΓ,x)Θh(ShΓ,x)1,forShΓi-almost everyxG.

Thus by taking into account (84) and the previous equation we conclude (83), that is the sought claim.

Remark 4.1

It is a classical result that if ERn is a h-rectifiable set, with 1hn, then Θh(ShE,x)=1 for Sh-almost every point xE, see [13, Theorem 3.2.19]. This is true also in the setting of Heisenberg groups for arbitrary Phc-rectifiable measures, and it is a direct consequence of [39, (iv)(ii) of Theorem 3.14 & Theorem 3.15].

We point out that as a consequence of the non-trivial results developed in the subsequent paper [6], see [6, Theorem 1.1], we have that whenever ΓG is a Borel set such that 0<Sh(Γ)<+, and ChΓ is Phc-rectifiable, then Θh(ChΓ,x)=1 for Ch-almost every xΓ.

Corollary 4.14

Let ϕ be a Phc-rectifiable measure on a Carnot group G. Then

0<Θh(ϕ,x)=Θ,h(ϕ,x)<+,forϕ-almost everyxG.

Proof

We stress that by restricting ourselves on balls of integer radii, by using Proposition 2.2 and Proposition 2.3, we can assume that ϕ has compact support. Let us first recall that, by Proposition 2.5, we have

ϕG\ϑ,γNE(ϑ,γ)=0. 86

Let us fix ϑ,γN. From Lebesgue’s differentiation theorem, see Proposition 2.2, and the locality of tangents, see Proposition 2.3, we deduce that ϕ being Phc-rectifiable implies that ϕE(ϑ,γ) is Phc-rectifiable. From Proposition 2.6 we deduce that ϕE(ϑ,γ) is mutually absolutely continuous with respect to ShE(ϑ,γ), and thus, by Radon–Nikodym theorem, see [23, page 82], there exists a positive function ρL1(ShE(ϑ,γ)) such that ϕE(ϑ,γ)=ρShE(ϑ,γ). We stress that we can apply Lebesgue–Radon–Nikodym theorem since ϕE(ϑ,γ) is asymptotically doubling because it has positive h-lower density and finite h-upper density almost everywhere. By Lebesgue–Radon–Nikodym theorem, see [23, page 82], and the locality of tangents again, we deduce that ShE(ϑ,γ) is a Phc-rectifiable measure, since ϕE(ϑ,γ) is a Phc-rectifiable measure. Thus, we can apply Theorem 4.13 to ShE(ϑ,γ) and obtain that for every ϑ,γN, we have that

0<Θh(ShE(ϑ,γ),x)=Θ,h(ShE(ϑ,γ),x)<+,forShE(ϑ,γ)-a.e.xG.

Since ϕE(ϑ,γ)=ρShE(ϑ,γ) we thus conclude from the previous equality and by Lebesgue-Radon-Nikodym theorem that for every ϑ,γN we have that

0<Θh(ϕE(ϑ,γ),x)=Θ,h(ϕE(ϑ,γ),x)<+,forϕE(ϑ,γ)-a.e.xG.

The previous equality, jointly with Proposition 2.2 and together with (86) allows us to conclude the proof.

Comparison with Other Notions of Rectifiability

In this section, we provide the proof of Proposition 1.2 and Corollary 1.5. The key step for proving the rectifiability with intrinsically differentiable graphs is the following proposition.

Proposition 5.1

(Hausdorff convergence to tangents) Let ϕ be a Ph-rectifiable measure. Let K be a compact set such that ϕ(K)>0. Then for ϕ-almost every point xK there exists V(x)Gr(h) such that

δ1/r(x-1·K)V(x),as r goes to0,

in the sense of Hausdorff convergence on closed balls {B(0,k)}k>0.

First of all, by reducing the measure ϕ to have compact support, e.g., considering the restriction on the balls with integer radii, and then by using Proposition 2.5, we can assume without loss of generality that KE(ϑ,γ) for some ϑ,γN. In order to prove the Hausdorff convergence to the plane V(x), we need to prove two different things: first, around almost every point x of K, the point of the set K at decreasingly small scales lies ever closer to the points of xV(x), and this is exactly what comes from the implication (33), see Proposition 3.1. Secondly, we have to prove the converse assertion with respect to the previous one, i.e., that the points of xV(x) around x at decreasingly small scales are ever closer to the points of K. For this latter assumption to hold we also need to add to the condition in (33) the additional control Fx,r(ϕK,ΘShxV)δrh+1, see Proposition 5.3. As a consequence of Proposition 5.1, we can prove Corollary 1.5 for measures of the form ShΓ. Finally by the usual reduction to E(ϑ,γ), we can give the proof of Corollary 1.5 for arbitrary measures.

CH1(G,G)-Rectifiability

This subsection is devoted to the proof of Proposition 1.2, i.e., the fact that the spherical Hausdorff measure restricted to a (G,G)-rectifiable set is P-rectifiable. In [25] the authors give the following definitions of CH1-submanifold of a Carnot group and rectifiable sets. We first recall the definition of CH1-function.

Definition 5.1

(CH1-function) Let G and G be two Carnot groups endowed with left-invariant homogeneous distances d and d, respectively. Let ΩG be open and let f:ΩG be a function. We say that f is Pansu differentiable at xΩ if there exists a homogeneous homomorphism dfx:GG such that

limyxd(f(x)-1·f(y),dfx(x-1·y))d(x,y)=0.

Moreover, we say that f is of class CH1 in Ω if the map xdfx is continuous from Ω to the space of homogeneous homomorphisms from G to G.

Definition 5.2

(CH1-submanifold) Given an arbitrary Carnot group G, we say that ΣG is a CH1-submanifold of G if there exists a Carnot group G such that for every pΣ, there exists an open neighborhood Ω of p and a function fCH1(Ω;G) such that

ΣΩ={gΩ:f(g)=0}, 87

and dfp:GG is surjective with Ker(dfp) complemented. In this case we say that Σ is a CH1(G,G)-submanifold.

Definition 5.3

((G,G)-rectifiable set) Given two arbitrary Carnot groups G and G of homogeneous dimension Q and Q, respectively, we say that ΣG is a (G,G) -rectifiable set if there exist countably many subsets Σi of G that are CH1(G,G)-submanifolds, such that

HQ-QΣ\i=1+Σi=0.

Using the results of [25], we prove the following.

Proposition 5.2

Let us fix G and G two arbitrary Carnot groups of homogeneous dimensions Q and Q, respectively, and suppose ΣG is a (G,G)-rectifiable set. Then the measure SQ-QΣ is PQ-Qc-rectifiable.

Proof

By [25, Corollary 3.6] a (G,G)-rectifiable set Σ has SQ-QΣ-almost everywhere positive and finite density. Thus, by the locality of tangents, see Proposition 2.3, by Lebesgue differentiation theorem in Proposition 2.2, and by the very definitions of (G,G)-rectifiable set and CH1(G,G)-submanifold, it suffices to prove the statement when Σ is the zero-level set of a function fCH1(Ω,G), with ΩG open, and such that for every p{gΩ:f(g)=0}=:Σ the differential dfp:GG is surjective with Ker(dfp) complemented.

Fix pΣ and note that the homogeneous subgroup Ker(dfp), where f is a representation as in (87), is independent of the choice of f. This follows for instance from [25, Lemma 2.14, (iii)]. We denote this homogeneous subgroup with W(p) and we call it the tangent subgroup at p to Σ. We first prove that

TanQ-Q(SQ-QΣ,p){λSQ-QW(p):λ>0},foreverypΣ. 88

Indeed, from [25, Lemma 3.4], denoting by Σp,r the set δ1/r(p-1·Σ), we have

SQ-QΣp,rSQ-QW(p),foreverypΣandforr0. 89

We claim that this last equality implies that

ri-(Q-Q)Tp,ri(SQ-QΣ)SQ-QW(p),foreveryinfinitesimalsequenceri,

thus showing (88). Indeed, for every measurable set AG, we have

Tp,ri(SQ-QΣ)(A)=SQ-QΣ(p·δri(A))=SQ-Q(p-1·Σ)(δri(A))=riQ-QSQ-QΣp,ri(A), 90

and thus the claim follows from (89). In order to conclude the proof, we have to prove that item (i) of Definition 2.18 holds. This follows from [25, Corollary 3.6]. Indeed, it is there proved that every (G,G)-rectifiable set has density SQ-Q-almost everywhere, that is stronger than item (i) of Definition 2.18.

Remark 5.1

We remark that the proof above is heavily based on [25, Lemma 3.4 & Corollary 3.6]. The two latter results in the reference are consequences of the area formula [25, Theorem 1.1]. As a consequence the approach in [25] is, in some sense, reversed with respect to our approach. The authors in [25] deal with the category of CH1(G,G)-regular submanifolds and prove the area formula relying upon [25, Proposition 2.2], that ultimately tells that a Borel regular measure μ with positive and finite Federer’s density θ with respect to the spherical Hausdorff measure Sh admits a representation μ=θSh. Then with this area formula, they are able to prove the results that led to the proof of the above Proposition 5.2.

We stress that in the subsequent paper [6], we push forward the study of P-rectifiable measures started here, and we prove an area formula for intrinsically differentiable graphs, see [6, Theorem 1.3], that extends the result of [25, Theorem 1.1].

Remark 5.2

(P-rectifiability and (G,G)-rectifiable sets) From Definition 5.2 and Definition 5.3 it follows that the tangent subgroup W at a point of a (G,G)-rectifiable set is always normal and complemented. Moreover, from [25, Lemma 2.14, (iv)], every complementary subgroup to W must be a Carnot subgroup of G that in addition is isomorphic to G. This results in a lack of generality of this approach to rectifiability. Let us give here an example where the previous phenomenon becomes clear. If we take L a horizontal subgroup in the first Heisenberg group H1, on the one hand, S1L is P1-rectifiable, on the other hand, L is not (H1,G)-rectifiable for any Carnot group G since L is not normal.

Rectifiability with Intrinsically Differentiable Graphs

This subsection is devoted to the proof of Proposition 5.1 and Corollary 1.5. Throughout this subsection, we let G to be a Carnot group of homogeneous dimension Q and h an arbitrary natural number with 1hQ. Whenever ϕ is a Radon measure supported on a compact set we freely use the notation E(ϑ,γ) introduced in Definition 2.9, for ϑ,γN. We start with some useful definitions and facts.

Definition 5.4

For 1hQ and ϑN, let us set

η(h):=1/(h+1),

and then let us define the constant

C7=C7(h,ϑ):=η(1-η)h32ϑh+2.

Proposition 5.3

Let ϕ be a Radon measure supported on a compact subset of G and let K be a Borel subset of suppϕ. Let ϑ,γ and 1hQ be natural numbers. Let xE(ϑ,γ), 0<r<1/γ, and 0<δ<C7. Assume further that there exist Θ>0 and VGr(h) such that

Fx,r(ϕK,ΘChxV)+Fx,r(ϕ,ΘChxV)2δrh+1. 91

Then for any wB(x,r/2)xV we have ϕ(KB(w,δ1h+2r))>0, and thus in particular KB(w,δ1h+2r).

Proof

From the hypothesis, we have that Fx,r(ϕ,ΘChxV)2δrh+1. Define g(x):=min{dist(x,U(0,1)c),η}, where η is defined in Definition 5.4. From the very definition of the function g and the choice of Θ above, we deduce that

ϑ-1(1-η)hηrh+1-Θηrh+1ηrϕ(B(x,(1-η)r))-ηrΘChxV(B(x,r))rg(δ1/r(x-1z))dϕ(z)-Θrg(δ1/r(x-1z))dChxV(z)2δrh+1,

where in the first inequality we are using that xE(ϑ,γ) and Remark 2.4, and in the last inequality, we are using that rg(δ1/r(x-1·))Lip1+(B(x,r)). Simplifying and rearranging the above chain of inequalities, we infer that

Θϑ-1(1-η)h-2δ/η(A)(2ϑ)-1(1-η)h=(B)(2ϑ)-1(1-1/(h+1))h,

where (A) comes from the fact that δ<C7<((1-η)hη)/(4ϑ), see Definition 5.4, and (B) comes from the definition of η, see Definition 5.4. Since the function h(1-1/(h+1))h is decreasing and bounded below by e-1, we deduce, from the previous inequality, that Θ1/(2ϑe).

We now claim that for every λ with δ1/(h+2)λ<1/2 and every wxVB(x,r/2) we have ϕ(B(w,λr)K)>0. This will finish the proof. By contradiction assume there is wxVB(x,r/2) such that ϕ(B(w,λr)K)=0. This would imply that

Θη(1-η)hλh+1rh+1=ΘηλrChxV(B(w,(1-η)λr))Θλrg(δ1/(λr)(w-1z))dChxV(z)=Θλrg(δ1/(λr)(w-1z))dChxV(z)-λrg(δ1/(λr)(w-1z))dϕK(z)2δrh+1, 92

where the first equality comes from Remark 2.4, and the last inequality comes from the choice of Θ as in the statement, and the fact that

λrg(δ1/(λr)(w-1·))Lip1+(B(w,λr))Lip1+(B(x,r)) because λ<1/2 and wB(x,r/2). Thanks to (92), the choice of λ, and the fact, proved some line above, that 1/(4eϑ)<Θ, we have that

δh+1h+24eϑη(1-η)h<Θλh+1η(1-η)h2δ,and thenδ1/(h+2)η(1-η)h8eϑ,

which is a contradiction since δ<C7=((η(1-η)h)/(32ϑ))h+2, see Definition 5.4.

Proof of Proposition 5.1

First of all, by reducing the measure ϕ to have compact support, e.g., considering the restriction on the balls with integer radii, and then by using Proposition 2.5, we can assume without loss of generality that KE(ϑ,γ) for some ϑ,γN

Since ϕ is a Ph-rectifiable measure, by using the locality of tangents with the density ρχK, see Proposition 2.3, for ϕ-almost every xK we have that the following three conditions hold

  • (i)

    Tanh(ϕ,x){λShV(x):λ>0}, where V(x)Gr(h),

  • (ii)

    0<Θh(ϕ,x)Θh,(ϕ,x)<+.

  • (iii)

    if ri0 is such that there exists Θ>0 with ri-hTx,riϕΘChV(x), then ri-hTx,ri(ϕK)ΘChV(x).

From now on let us fix a point xK for which the three conditions above hold. If we are able to prove the convergence in the statement for such a point then the proof of the proposition is concluded.

Thus, we have to show that for every k>0 the following holds

limr0dH,G(δ1/r(x-1·K)B(0,k),V(x)B(0,k))=0, 93

where dH,G is the Hausdorff distance between closed subsets in G. For some compatibility with the statements that we already proved, we are going to prove (93) for k=1/4. The proof of (93) for an arbitrary k>0 can be achieved by changing accordingly the constants in the statements of Proposition 3.1 and Proposition 5.3, that we are going to crucially use in this proof. We leave this generalization to the reader, as it will be clear from this proof.

Let us fix ε<min{δG,C7}, where δG is defined in Definition 3.2 and C7 in Definition 5.4, and let us show that there exist an r0=r0(ε) and a real function f1 such that

dH,Gδ1/r(x-1·K)B(0,1/4),V(x)B(0,1/4)f1(ε),for all0<r<r0(ε), 94

where

f1(ε):=max{C5ε1/(h+1)+f2(ε),3ε1/(h+2)+f3(ε)}, 95

and where the constant C5 is defined in Proposition 3.1, and the functions f2, f3 are introduced in (101) and (103), respectively. By the definition of f1,f2,f3, it follows that f1(ε)0 as ε0 and thus, if we prove (94), we are done.

In order to reach the proof of (94) let us add an intermediate step. We claim that there exists an r0:=r0(ε)<1/γ such that the following holds

for every0<r<r0there exists aΘ:=Θ(r)for whichFx,r(ϕK,ΘChxV)+Fx,r(ϕ,ΘChxV)2εrh+1. 96

The conclusion in (96) follows if we prove that

limr0infΘ>0Fx,r(ϕK,ΘChxV)+Fx,r(ϕ,ΘChxV)rh+10. 97

We prove (97) by contradiction. If (97) was not true, there would exist an ε~ and an infinitesimal sequence {ri}iN such that

infΘ>0Fx,ri(ϕK,ΘChxV)+Fx,ri(ϕ,ΘChxV)>ε~rih+1,for everyiN. 98

Thus, from items (i) and (ii) above, and from [1, Corollary 1.60], we conclude that, up to a non-re-labeled subsequence of ri, there exists a Θ>0 such that we have ri-hTx,riϕΘChV(x) as ri0. Then by exploiting the item (iii) above we get also that ri-hTx,ri(ϕK)ΘChV(x) as ri0. These two conclusions immediately imply, by exploiting Remark 2.7 and (2.22), that

limi+ri-(h+1)Fx,ri(ϕK,ΘChxV)+Fx,ri(ϕ,ΘChxV)0,

which is a contradiction with (98). Thus, the conclusion in (96) holds. Let us continue the proof of (94).

Taking into account the bound on ε and (96) we can apply Proposition 3.1, since V(x)Πε(x,r) for all 0<r<r0, and Proposition 5.3 to obtain, respectively, that for all 0<r<r0

suppKB(x,r/4)dist(p,xV(x))suppE(ϑ,γ)B(x,r/4)dist(p,xV(x))C5rε1/(h+1),for everypB(x,r/2)xV(x)we haveB(p,ε1/(h+2)r)K. 99

Let us proceed with the proof of (94). Fix 0<r<r0 and note that for any wδ1/r(x-1·K)B(0,1/4) there exists a point pKB(x,r/4) such that w=:δ1/r(x-1·p). From the first line of (99), we get that dist(x-1·p,V(x))C5rε1/(h+1) and thus there exists a vV(x) such that d(x-1·p,v)C5rε1/(h+1). This in particular means that d(w,δ1/rv)C5ε1/(h+1) and then, since wB(0,1/4), we get also that δ1/rvV(x)B(0,1/4+C5ε1/(h+1)). Thus, we conclude that

dist(w,V(x)B(0,1/4+C5ε1/(h+1)))C5ε1/(h+1), 100

for all wδ1/r(x-1·K)B(0,1/4). Define the following function

f2(ε):=supuV(x)(B(0,1/4+C5ε1/(h+1))\U(0,1/4))d(u,δ4-1u-1u), 101

and notice that by compactness it is easy to see that f2(ε)0 as ε0. With the previous definition of f2 in hands, we can exploit (100) and conclude that

supwδ1/r(x-1·K)B(0,1/4)dist(w,V(x)B(0,1/4))C5ε1/(h+1)+f2(ε). 102

The latter estimate is the first piece of information we need to prove (94). Let us now estimate dist(δ1/r(x-1·K)B(0,1/4),v) for any vV(x)B(0,1/4). If uV(x)(B(0,1/4)\U(0,1/4-ε1/(h+2))), then there exists a unique μ=μ(u)>0 such that δμ(u)uV(x)B(0,1/4-ε1/(h+2)). Let us define

f3(ε):=supuV(x)(B(0,1/4)\U(0,1/4-ε1/(h+2)))d(u,δμ(u)u), 103

and by compactness it is easy to see that f3(ε)0 as ε0. Let us now fix vV(x)B(0,1/4). Then x·δrvB(x,r/4)xV(x)B(x,r/2)xV(x). We can use the second line of (99) to conclude that there exists wB(x·δrv,ε1/(h+2)r)K. Thus w~:=δ1/r(x-1·w)B(v,ε1/(h+2))δ1/r(x-1·K). Now we have two cases

  • if v was in B(0,1/4-ε1/(h+2)) we would get w~B(0,1/4) and then
    dist(δ1/r(x1·K)B(0,1/4),v)ε1/(h+2); 104
  • if instead vV(x)(B(0,1/4)\U(0,1/4-ε1/(h+2))), we denote v:=δμ(v)v the point that we have defined above and then we still have x·δrvB(x,r/2)xV(x). Thus we can again apply the second line of (99) to deduce the existence of wB(x·δrv,ε1/(h+2)r)K. Then we conclude w~:=δ1/r(x-1·w)B(v,ε1/(h+2))δ1/r(x-1·K). Now we can estimate
    d(w~,w~)=1rd(w,w)1r(d(w,x·δrv)+d(x·δrv,x·δrv)+d(x·δrv,w))2ε1/(h+2)+f3(ε). 105
    Moreover, since vB(0,1/4-ε1/(h+2)) and w~B(v,ε1/(h+2)) we get that w~B(0,1/4)δ1/r(x-1·K). Then by the triangle inequality and (105) we conclude that, in this second case,
    d(w~,v)3ε1/(h+2)+f3(ε), 106
    and then
    dist(δ1/r(x1·K)B(0,1/4),v)3ε1/(h+2)+f3(ε). 107

By joining together the conclusion of the two cases, see (104) and (107), we conclude that

supvV(x)B(0,1/4)dist(δ1/r(x1·K)B(0,1/4),v)3ε1/(h+2)+f3(ε). 108

The equations (102) and (108) imply (94) by the very definition of Hausdorff distance. Thus the proof is concluded.

Let us now give the definition of intrinsically differentiable graph.

Definition 5.5

(Intrinsically differentiable graph) Let V and L be two complementary subgroups of a Carnot group G. Let φ:KVL be a continuous function with K compact in V. Let a0K. We say that graph(φ) is an intrinsically differentiable graph at a0·φ(a0) if there exists a homogeneous subgroup V(a0) such that for all k>0

limλdH,Gδλ((a0·φ(a0))-1·graph(φ))B(0,k),V(a0)B(0,k)=0, 109

where dH,G is the Hausdorff distance between closed subsets of G.

We prove now that the support of a Phc-rectifiable measure ShΓ, where Γ is compact, can be written as the countable union of almost everywhere intrinsically differentiable graphs.

Theorem 5.4

For any 1hQ, there exist a countable subfamily F:={Vk}k=1+ of Grc(h), and Lk complementary subgroups of Vk such that the following holds.

Let Γ be a compact subset of G such that 0<Sh(Γ)<+, and ShΓ is a Phc-rectifiable measure. Then for every α>0, there are countably many compact Γi’s that are intrinsic graphs of functions φi:PVi(Γi)Li, and that satisfy the following three conditions: Γi are CVi(α)-sets, Γi are intrinsically differentiable graphs at a·φi(a) for ShPVi(Γi)-almost every aPVi(Γi), and

Sh(Γ\i=1+Γi)=0.

Proof

First of all, let

F(V,L):=ε1(V,L),for all(V,L)Sub(h),

where Sub(h) is defined in (44). Given the above-defined function F, we construct the family F:={Vk}k=1+ and choose Lk complementary subgroups of Vk as in the statement of Theorem 3.4. Notice that this choice is dependent on the function F that we chose above. We claim that the family for which the statement holds is F.

Applying Theorem 3.4 with βmin{1/2,α} to the measure ShΓ we get countably many compact sets ΓiΓ that are CVi(min{F(Vi,Li),α})-sets and such that

Sh(Γ\i=1+Γi)=0.

Since F(Vi,Li)=ε1(Vi,Li), we conclude that each Γi is also the intrinsic graph of a function φi:PVi(Γi)Li, see Proposition 2.17. It is left to show that, for every iN, graph(φi) is an intrinsically differentiable graph at a·φi(a) for ShPV(Γi)-almost every aPVi(Γi).

Indeed, since ShΓ is Phc-rectifiable, we can apply Proposition 5.1 and, for every iN, we conclude that

δ1/r(x-1·Γi)V(x),as r goes to0,forShΓi-almost everyxG,whereV(x)Gr(h), 110

in the sense of Hausdorff convergence on closed balls {B(0,k)}k>0. Moreover, thanks to Proposition 4.7 and to Lebesgue differentiation theorem in Proposition 2.2, we infer that (Φi)ShVi is mutually absolutely continuous with respect to ShΓi, where Φi is the graph map of φi. Furthermore, since every point xΓi can be written as x=a·φi(a), with aPVi(Γi), we conclude, from (110) and latter absolute continuity, that Γi=graph(φi) is an intrinsically differentiable graph at a·φi(a) for ShPV(Γi)-almost every aPVi(Γi), and this concludes the proof.

In the following corollary we provide the proof of Corollary 1.5.

Corollary 5.5

For any 1hQ, there exist a countable subfamily F:={Vk}k=1+ of Grc(h), and Lk complementary subgroups of Vk such that the following holds.

For any Phc-rectifiable measure ϕ and for any α>0, there exist countably many compact sets Γi’s that are CVi(α)-sets, that are intrinsic graphs of functions φi:PVi(Γi)Li, and that satisfy the following conditions: Γi are intrinsically differentiable graphs at a·φi(a) for ShPVi(Γi)-almost every aPVi(Γi), and

ϕ(G\i=1+Γi)=0.

Proof

By restricting on closed balls of integer radii we can assume without loss of generality that ϕ has compact support. Let us fix ϑ,γN. We can infer this corollary by working on ϕE(ϑ,γ), that is mutually absolutely continuous with respect to ShE(ϑ,γ), see Proposition 2.6, and by using the previous Corollary 5.4 together with Proposition 2.5. The resulting strategy is identical to the one in Corollary 4.14 so we omit the details.

Remark 5.3

(Uniformly intrinsically differentiable graphs and CH1(G,G)-surfaces) By the recent work of the second named author, see [41, Theorem 3], one can show that in an arbitrary Carnot group of homogeneous dimension Q, the support of a PQ-1-rectifiable measure can be covered by countably many CH1-regular hypersurfaces. Moreover, it is known that a CH1-regular hypersurface is characterized, locally, by being the graph of a uniformly intrinsically differentiable function, see [3, Theorem 1.6]. This means that, in some particular cases, as it is the codimension-one case, we can strengthen the conclusion in Corollary 5.5 by obtaining that the maps are uniformly intrinsically differentiable.

This latter observation gives raise to two questions, that in the co-horizontal case are the same thanks to [3, Theorem 1.6], but in general could be different: is it always possible to improve the intrinsic differentiability in Corollary 5.5 to some kind of uniform intrinsic differentiability? Is it possible to prove that when a Ph-rectifiable measure, or even a Ph-rectifiable measure, on G admits only complemented normal subgroups that have only complementary subgroups that are Carnot subgroups, then we can write its support as the countable union of CH1(G,G)-surfaces, see Definition 5.2? Let us stress that if one answers positively to the second question, this would mean, taking into account Proposition 5.2, that whenever they can agree, see Remark 5.2, the two notions of P-rectifiable measure and (G,G)-rectifiable set agree.

We do not address these questions in this paper, but we stress that with the results proved in [6], we show that, at least in the co-horizontal case, the notion of P-rectifiable measure and the notion of rectifiability given in terms of (G,G)-rectifiable sets coincide, see [6, Corollary 5.3].

In the final part of this section, we briefly discuss how the notion of intrinsically differentiable graph in Definition 5.5 is related to the already available notion of intrinsic differentiability, see [14, Definition 3.2.1] and [4, Definition 2.5]. Throughout the rest of this section V and L are two fixed complementary subgroups in a Carnot group G.

Definition 5.6

(Intrinsic translation of a function) Given a function φ:UVL, we define, for every qG,

Uq:={aV:PV(q-1·a)U},

and φq:UqVL by setting

φq(a):=(PL(q-1·a))-1·φ(PV(q-1·a)). 111

Definition 5.7

(Intrinsically linear function) The map :VL is said to be intrinsically linear if graph() is a homogeneous subgroup of G.

Definition 5.8

(Intrinsically differentiable function) Let φ:UVL be a function with U Borel in V. Fix a density point a0D(U) of U, let p0:=φ(a0)-1·a0-1 and denote with φp0:Up0VL the shifted function introduced in Definition 5.6. We say that φ is intrinsically differentiable at a0 if there is an intrinsically linear map dφφa0:VL such that

limbe,bUp0dφφa0[b]-1·φp0(b)b=0. 112

The function dφφa0 is called the intrinsic differential of φ at a0.

Let us fix φ:UVL with U open. Whenever the intrinsic differential introduced in Definition 5.8 exists, it is unique: see [14, Theorem 3.2.8]. In [14] the authors prove the following result: a function φ:UVL, with U open, is intrinsically differentiable at a0 if and only if graph(φ) is an intrinsically differentiable graph at a0·φ(a0) with the tangent V(a0) complemented by L, see Definition 5.5, and moreover V(a0)=graph(dφφa0). In the setting we are dealing with, i.e., with maps φ:UVL with U compact, the above equivalence still holds at density points of U. We do not give a proof of this last assertion since it follows by routine modifications of the argument in [14], and moreover, we do not need it in this paper.

Acknowledgements

The first author is partially supported by the European Research Council (ERC Starting Grant 713998 GeoMeG ‘Geometry of Metric Groups’). The second author is supported by the Simons Foundation Wave Project, Grant 601941, GD. The authors wish tho express their gratitude to the anonymous referee for the careful reading of the paper.

Funding

Open access funding provided by Scuola Normale Superiore within the CRUI-CARE Agreement.

Footnotes

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