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. 2023 Sep 9;33(11):359. doi: 10.1007/s12220-023-01360-4

Horizontally Affine Functions on Step-2 Carnot Algebras

Enrico Le Donne 1,2,, Daniele Morbidelli 3, Séverine Rigot 4
PMCID: PMC10492776  PMID: 37701677

Abstract

In this paper, we introduce the notion of horizontally affine, h-affine in short, function and give a complete description of such functions on step-2 Carnot algebras. We show that the vector space of h-affine functions on the free step-2 rank-n Carnot algebra is isomorphic to the exterior algebra of Rn. Using that every Carnot algebra can be written as a quotient of a free Carnot algebra, we shall deduce from the free case a description of h-affine functions on arbitrary step-2 Carnot algebras, together with several characterizations of those step-2 Carnot algebras where h-affine functions are affine in the usual sense of vector spaces. Our interest for h-affine functions stems from their relationship with a class of sets called precisely monotone, recently introduced in the literature, as well as from their relationship with minimal hypersurfaces.

Keywords: Step-2 Carnot groups, Step-2 Carnot algebras, Horizontally affine functions

Introduction

In this paper, we introduce the notion of horizontally affine function and give a complete description of such functions on step-2 Carnot algebras, or equivalently on step-2 Carnot groups. In the free step-2 rank-n case, we shall see that the vector space of horizontally affine functions is isomorphic to the exterior algebra of Rn. Using the known fact that every step-2 Carnot algebra can be written as a quotient of a free step-2 Carnot algebra, we shall next deduce from the free case a description of horizontally affine functions on arbitrary step-2 Carnot algebras, together with several characterizations of those step-2 Carnot algebras where h-affine functions are affine in the usual sense of vector spaces.

To introduce the discussion, let us recall some definitions. We refer to Sect. 2 for more details. Let g=g1g2 be a step-2 Carnot algebra, which means that g is a finite dimensional real1 nilpotent Lie algebra of step 2, g2:=[g,g] denotes the derived algebra, and g1 denotes a linear subspace of g that is in direct sum with g2. Such a Lie algebra is naturally endowed with the group law given by

x·y:=x+y+[x,y]

for x,yg that makes it a step-2 Carnot group. Actually every step-2 Carnot group can be realized in this way. We shall therefore view a step-2 Carnot algebra both as a Lie algebra and as a Lie group. We also adopt the notation yt:=ty for all tR and yg. A function f:gR is said to be horizontally affine, and for brevity, we say that f is h-affine and write fAffh(g), if for all xg and yg1 the function tRfx·yt is affine. Note that this definition is purely algebraic - it has in particular no connection with the choice of a subRiemannian metric structure on g – and can be equivalently restated in geometrical terms as follows. A function f:gR is h-affine if and only if its restriction to each integral curve of every left-invariant horizontal vector field is affine when seen as a function from R to R, where a left-invariant vector field is said to be horizontal whenever it belongs to g1.

Horizontally affine functions appear naturally in relation with monotone sets, an important class of sets introduced by Cheeger and Kleiner [5], see also [4, 8, 12, 14] and the discussion below. However, h-affine functions are studied systematically for the first time here. See also [1] for a further study of a related notion in more general settings.

Our purposes in the present paper are twofold. We first give a description of h-affine functions on step-2 Carnot algebras, starting with the free case from which the general case will follow. We shall next deduce from this description several characterizations of those step-2 Carnot algebras where h-affine functions are affine. We shall keep the standard terminology saying that a function f:gR is affine, writing fAff(g), to mean that f is affine in the usual sense considering the vector space structure on g. Note indeed that by elementary properties of step-2 Carnot algebras, each affine function fAff(g) is h-affine. In other words, in every step-2 Carnot algebra g, the vector space Aff(g) is a linear subspace of Affh(g), see the discussion in Sect. 2. This inclusion may, however, be strict, as we shall see.

More explicitly, h-affine functions can be described with the help of the Carnot dilations δt:gg given by δt(x1+x2):=tx1+t2x2 for x1g1, x2g2, and tR:=R\{0}. Given a non-negative integer i we define the vector space of i-homogeneous h-affine functions as

Affh(g)i:={fAffh(g):fδt=tiffor alltR}.

We shall prove that every fAffh(g) can be written in a unique way as a finite sum of i-homogeneous h-affine functions for some i’s in {0,,κ} where κ:=rankg if g is a free step-2 Carnot algebra and κ:=rankg-1 if g is a nonfree step-2 Carnot algebra. Recall that the rank of g is defined as rankg:=dimg1. Furthermore, denoting by ΛkRn the space of alternating k-multilinear forms over Rn (see Sect. 6 for our conventions about exterior algebra), we shall also prove that for every i{0,,κ} the vector space Affh(g)i is isomorphic to a linear subspace of Λκ-iRκ. See Theorems 1.1, 1.2, and 1.3 for detailed statements.

Let us first consider the free case. Throughout this paper, given an integer n2, we shall use the model for the free step-2 rank-n Carnot algebra fn given by

fn:=Λ1RnΛ2Rn

equipped with the Lie bracket where the only nontrivial relations are given by

[θ,θ]:=θθforθ,θΛ1Rn.

The induced group law takes the form

(θ+ω)·(θ+ω):=θ+θ+ω+ω+θθ

for θ,θΛ1Rn, ω,ωΛ2Rn. For notational convenience, we shall frequently identify fn with Λ1Rn×Λ2Rn writing elements in fn as (θ,ω) where θΛ1Rn, ωΛ2Rn.

Given integers n2, i{0,,n}, and ηΛn-iRn, we define φη:fnΛnRn as

φη(θ,ω):=ωkηifi=2kis evenθωkηifi=2k+1is odd. 1.1

The description of h-affine functions on fn can then be given in terms of the functions φη’s and reads as follows.

Theorem 1.1

For n2, we have

  • (i)

    Affh(fn)=i=0nAffh(fn)i.

Furthermore, given i{0,,n} and νΛnRn\{0}, we have

  • (ii)

    fAffh(fn)i if and only if there is ηΛn-iRn, which is unique, such that fν=φη.

Therefore, for i{0,,n}, the spaces Affh(fn)i and Λn-iRn are isomorphic as vector spaces, and hence, so are Affh(fn) and ΛRn. In particular, Affh(fn) is a finite dimensional vector space with dimension 2n.

Let us briefly explain our strategy to prove Theorem 1.1. Let νΛnRn\{0} be fixed. It is rather easy to verify that if a function f:fnR is such that fν=φη for some ηΛn-iRn with i{0,,n} then fAffh(fn)i, see Lemma 3.1. The injectivity of the map ηΛn-iRnφη is also not hard to verify and follows from general facts about exterior algebra, see Corollary 6.5. The main difficulties are thus to get the decomposition given in Theorem 1.1 (i), see Theorem 3.2 and Proposition 3.4 (i), as well as the fact that every function fAffh(fn)i can be written as fν=φν for some νΛn-iRn, see Proposition 3.5. This will occupy most of Sect. 3 to which we refer for more details. For the sake of completeness, let us mention the geometric interpretation behind the decomposition in Theorem 1.1 when passing from fn for n3 to any Lie subalgebra of fn that is isomorphic to fn-1. It can be proved that the zero level set of non-zero n-homogeneous h-affine functions on fn, namely, the set {(θ,ω)fn:ωn/2=0} if n is even, {(θ,ω)fn:θω(n-1)/2=0} if n is odd, coincides with the union of all Lie subalgebras of fn that are isomorphic to fn-1. Therefore, if f=f0++fnAffh(fn) with fiAffh(fn)i, one gets that its restriction to any Lie subalgebra isomorphic to fn-1 coincides with the restriction to this subalgebra of the sum of the i-homogeneous terms f0++fn-1 for i{0,,n-1} that show up in the decomposition of f.

Let us now turn to the general case of arbitrary step-2 Carnot algebras. Our starting point is the known fact that every step-2 Carnot algebra g can be written as a quotient of free step-2 Carnot algebras. Namely, by the universal property of free step-2 Carnot algebras, for every nrankg, there is a surjective Carnot morphism π:fng, see the discussion in Sect. 2. It turns out that there is a one-to-one correspondence between h-affine functions on g and h-affine functions on fn that factor through fn/Kerπ, see Lemma 2.3 and Corollary 2.4. The description of h-affine functions on g can therefore be deduced from the characterization of those functions φη that factor through fn/Kerπ. Namely, we shall verify that for ηΛiRn the function φη factors through fn/Kerπ if and only if η annihilates Kerπ, which means that ηAnhiKerπ where

AnhiKerπ:={ηΛiRn:ηζ=0for allζKerπ}

see Lemma 4.1. In the genuinely nonfree setting, such a characterization implies the following decomposition of Affh(g).

Theorem 1.2

Let g be a step-2 rank-r Carnot algebra. Assume that g is not isomorphic to fr. Then Affh(g)=i=0r-1Affh(g)i.

Note that, in contrast with the free case, one has Affh(g)r={0} when g is a step-2 rank-r Carnot algebra that is not isomorphic to fr. This follows from the fact that Kerπ{0}, and hence Anh0Kerπ={0}, whenever π:frg is a surjective Carnot morphism. A description of the summands Affh(g)i is provided by the following theorem that applies both in the free and in the nonfree cases (note that when g=fr and n=r, one recovers Theorem 1.1) and where the space of annihilators of Kerπ in ΛRn is defined by

AnhKerπ:={ηΛRn:ηζ=0for allζKerπ}.

Theorem 1.3

Let g be a step-2 rank-r Carnot algebra, nr, and π:fng be a surjective Carnot morphism. Then the following hold true. For i{0,,n}, νΛnRn\{0},

  • (i)

    for every ηAnhn-iKerπ, there is a unique fAffh(g)i such that (fπ)ν=φη;

  • (ii)

    for every fAffh(g)i, there is a unique ηAnhn-iKerπ such that (fπ)ν=φη;

  • (iii)

    via this correspondence, Affh(g)i and Anhn-iKerπ are isomorphic as vector spaces.

Consequently,

  • (iv)

    Affh(g) and AnhKerπ are isomorphic as vector spaces.

In particular, Affh(g) is a finite dimensional vector space.

As a consequence of Theorem 1.3, one gets that h-affine functions on step-2 Carnot algebras are polynomials and hence smooth. Let us stress here that there is no regularity assumption in our definition of h-affine functions. Such functions are indeed only assumed to be affine when restricted to horizontal lines and were not even assumed continuous, nor measurable, beforehand. As a further consequence of their smoothness (one actually only needs local integrability), one can characterize elements in Affh(g) as those locally integrable functions that are harmonic in the distributional sense with respect to every subLaplacian on g, see Remark 2.8. Let us mention that horizontally affine distributions have been recently studied in [1] in wider settings where they can be proved to be polynomials. Note, however, that this later notion may be different from a pointwise generalization of our present notion of h-affine functions to more general settings, as explained at the end of Remark 2.8.

Several characterizations of step-2 Carnot algebras g where Affh(g)=Aff(g) can easily be deduced from Theorem 1.3, see Theorem 1.4 below and Sect. 5. It turns out that one of these characterizations can be formulated using a class of Lie algebras known in literature as I-null, see [11]. We recall that a step-2 Carnot algebra g=g1g2 is I-null if every bilinear form b:g1×g2R satisfying b(x,[x,y])=0 for all x,yg1 vanishes identically on g1×g2, see Definition 2.6 and Proposition 2.7.

Theorem 1.4

Let g be a step-2 Carnot algebra. Then the following are equivalent:

  • (i)

    Affh(g)=Aff(g)

  • (ii)

    Affh(g)=i=02Affh(g)i

  • (iii)

    i3Affh(g)i={0}, equivalently, Affh(g)3={0}

  • (iv)

    g is I-null

  • (v)

    i=3nAnhn-iKerπ={0}, equivalently, Anhn-3Kerπ={0}, for some, equivalently all, nmax{3,rankg}, π:fng surjective Carnot morphism.

Note incidentally that it follows from Theorem 1.1 that Affh(fn)=Aff(fn) if and only if n=2. Therefore, the equivalent conditions given in Theorem 1.4 hold true on g=fn if and only if n=2. Theorem 1.4 can be efficiently applied in several concrete situations which will be discussed in Sect. 5.2 and to which we refer for more details.

Before closing this introduction, we briefly go back to the relationship between h-affine functions and precisely monotone sets, as defined in [5] in the Heisenberg setting. More generally, a subset of a Carnot algebra, identified with a Carnot group, is said to be precisely monotone if the restriction of its characteristic function to each integral curve of every left-invariant horizontal vector field is monotone when seen as a function from R to R. Equivalently, a precisely monotone set is a h-convex set with h-convex complement, see for instance [15] for more details about h-convex sets. Precisely monotone sets have been classified in the first Heisenberg algebra f2, in higher dimensional Heisenberg algebras, and in the direct product f2×R, see [5, 12, 14]. In the aforementioned step-2 settings, it turns out that the boundary of a nonempty precisely monotone strict subset is a hyperplane, while in step-3 Carnot algebras the same statement may be false, see [2, 3]. As a consequence of our results, we actually get plenty of examples of Carnot algebras already in the step-2 case where there are precisely monotone subsets whose boundary is not a hyperplane. Indeed, it can easily be seen that sublevel sets of h-affine functions are precisely monotone. Therefore if g is a step-2 Carnot algebra that is not I-null and if fAffh(g)\Aff(g) then every sublevel set of f is a precisely monotone set whose boundary is not a hyperplane. We refer to the recent paper [13] for a more detailed introduction to precisely monotone sets as well as for a classification of such sets in the step-2 rank-3 case in terms of sublevel sets of h-affine functions, and for further discussions about higher rank and higher step cases. To conclude these observations, let us mention that measurable precisely monotone sets, and therefore sublevel sets of h-affine functions on step-2 Carnot algebras, can be proved to be local minimizers for the intrinsic perimeter, see [18, Proposition 3.9] and [13, Proposition 2.9].

The rest of this paper is organized as follows. Section 2 contains our conventions and notations about step-2 Carnot algebras and h-affine functions. We also provide easy facts that will be useful for later arguments. In Sect. 3, we focus on the free case and prove Theorem 1.1. Theorems 1.2 and 1.3 are proved in Sect. 4. Section 5.1 is devoted to the proof of Theorem 1.4 and Sect. 5.2 to a discussion of several examples. In the final Sect. 6, we gather notations and facts in linear and exterior algebra.

Step-2 Carnot Algebras and Horizontally Affine Functions

We recall that a real2 and finite dimensional Lie algebra g is said to be nilpotent of step 2 if the derived algebra g2:=[g,g] is nontrivial, i.e., g2{0}, and central, i.e., [g,g2]={0}. Here, given U,Vg, we denote by [UV] the linear subspace of g generated by elements of the form [uv] with uU, vV. If g1 is a linear subspace of g that is in direct sum with g2 then [g1,g1]=g2 and the decomposition g=g1g2 is therefore a stratification of g. As a matter of fact, every stratification of a nilpotent Lie algebra of step 2 is of this form.

A step-2 Carnot algebra g is a Lie algebra nilpotent of step 2 equipped with a stratification g=g1g2. The rank of g is defined as rankg:=dimg1. Such a Lie algebra is naturally endowed with the group law3 given by

x·y:=x+y+[x,y]

for x,yg that makes it a step-2 Carnot group. It is actually well known that any step-2 Carnot group can be realized in this way. We shall therefore view a step-2 Carnot algebra both as a Lie algebra and group.

Throughout this paper, we shall always denote by g=g1g2 a step-2 Carnot algebra. Given tR, xg, we set xt:=tx.

Definition 2.1

Given Ag we say that f:gR is A-affine if for every xg, yA, the function tRf(x·yt) is affine.

When A=g, one recovers the notion of real-valued affine functions on g seen as a vector space. Indeed, since g is nilpotent of step 2, for x,yg, tR, we have x·yt=x+t(y+[x,y]) and x+ty=x·(y-[x,y])t. Therefore f:gR is g-affine if and only if for every x,yg, tR, the function tRf(x+ty) is affine, i.e., f is affine, see Proposition 6.1. In particular, real-valued affine functions are A-affine for every Ag.

In the present paper, we are interested in g1-affine functions, which we shall call horizontally affine, h-affine in short, namely:

Definition 2.2

(h-affine functions) We say that f:gR is horizontally affine, h-affine in short, if f is g1-affine. In other words, f is h-affine if for every xg, yg1, the function tRf(x·yt) is affine. We denote by Affh(g) the real vector space of h-affine functions on g.

We say that g is a horizontal line if there are xg, yg1\{0} such that ={x·yt:tR}. We already noticed that horizontal lines are 1-dimensional affine subspaces of g and therefore h-affine functions can equivalently be defined as functions whose restriction to every horizontal line is affine.

We recall that a Carnot morphism π:gg between step-2 Carnot algebras g=g1g2 and g=g1g2 is a homomorphism of graded Lie algebras, which means that π is a linear map such that π([x,y])=[π(x),π(y)] for all x,yg and π(gk)gk for k=1,2. Note that a Carnot morphism is both a homomorphism of graded Lie algebras and a group homomorphism.

Lemma 2.3

Let g,g be step-2 Carnot algebras and π:gg be a Carnot morphism. For fAffh(g), we have fπAffh(g). If π is surjective then fAffh(g) if and only if fπAffh(g).

Proof

Carnot morphisms map affinely horizontal lines to either horizontal lines or singletons therefore fπAffh(g) when fAffh(g). If the Carnot morphism π:gg is surjective then every horizontal line in g is the affine image through π of a horizontal line in g and therefore fAffh(g) when fπAffh(g).

For tR:=R\{0}, the Carnot dilation δt:gg is defined as the linear map such that δt(x)=tkx for xgk, k=1,2. The family (δt)tR is a one parameter group of Carnot automorphisms. Recall that, given a non-negative integer i, we denote by Affh(g)i:={fAffh(g):fδt=tiffor alltR}, the linear subspace of Affh(g) of i-homogeneous h-affine functions on g. Since dilations commute with Carnot morphisms, we get from Lemma 2.3 the following corollary.

Corollary 2.4

Let g,g be step-2 Carnot algebras, π:gg be a Carnot morphism, and i be a non-negative integer. For fAffh(g)i, we have fπAffh(g)i. If π is surjective then fAffh(g)i if and only if fπAffh(g)i.

We already noticed that the set Aff(g) of real-valued affine functions on g is a linear subspace of Affh(g). More precisely, we have the following inclusion.

Lemma 2.5

Aff(g) is a linear subspace of i=02Affh(g)i.

Proof

Let fAff(g). There are f0R and linear forms fk:gkR, k=1,2, such that f(x+z)=f0+f1(x)+f2(z) for all xg1, zg2. Clearly, constant functions belong to Affh(g)0 and the functions x+zg1g2f1(x) and x+zg1g2f2(z) belong to Affh(g)1 and Affh(g)2, respectively.

We say that step-2 Carnot algebras are isomorphic if there is a bijective Carnot morphism from one to the other. Note that being h-affine, respectively, affine, are intrinsic properties, in particular Affh(g)=Aff(g) if and only if Affh(g)=Aff(g) for isomorphic step-2 Carnot algebras g,g. This indeed more explicitly follows from Lemma 2.3 together with the fact that Carnot morphisms are linear maps.

Let us recall that by the universal property of free step-2 Carnot algebras, see Sect. 1 for our conventions about the free step-2 rank-n Carnot algebra fn, given a step-2 rank-r Carnot algebra g and given an integer nr, there is a surjective Carnot morphism π:fng, see for instance [17, p.45]. We also recall that for such a Carnot morphism, Kerπ is a graded ideal in fn, which means that Kerπ=i1i2 where ik are linear subspaces of ΛkRn, k=1,2, such that θθi2 for all θΛ1Rn, θi1.

We now recall the definition of I-null Lie algebras that will be used in one of our characterizations of those step-2 Carnot algebras where h-affine functions are affine, see Theorem 1.4.

Definition 2.6

[11] A Lie algebra m is said to be I-null if for every symmetric bilinear invariant form B:m×mR, we have B(m,[m,m])=0. Here B is said to be invariant if B(x,[y,z])=B([x,y],z) for all x,y,zm, or equivalently, if the trilinear form B(·,[·,·]) is alternating on m×m×m.

For step-2 Carnot algebras, the previous definition can be rephrased in the following way, of which we omit the elementary proof.

Proposition 2.7

A step-2 Carnot algebra g=g1g2 is I-null if and only if every bilinear form b:g1×g2R satisfying b(x,[x,y])=0 for all x,yg1 vanishes identically on g1×g2.

Remark 2.8

In the present article, we focus on step-2 Carnot algebras or, equivalently, step-2 Carnot groups. Let us mention that the notion of horizontally affine function makes sense in broader generality. One may for instance consider Carnot groups of arbitrary step (see [10, 16] for a primer on the subject) or, more generally, a connected nilpotent Lie group G equipped with a vector subspace Δ of its Lie algebra g that Lie generates g. Then we say that f:GR is Δ-affine if for every XΔ the restriction of f to each integral curve of X is affine when seen as a function from R to R. Here an element XΔ is seen as a left-invariant vector field on G. When G is a step-2 Carnot group with stratified Lie algebra g=g1g2 and Δ=g1 is the first, usually called horizontal, layer of the stratification of g, one recovers Definition 2.2, and this latter definition can hence be extended to Carnot groups of arbitrary step in the obvious way. Going back to the aforementioned more general setting and considering G equipped with a Haar measure, let us mention that we have the following characterizations of locally integrable Δ-affine functions. Namely, fLloc1(G) has a representative that is Δ-affine if and only if one of the following equivalent conditions holds true in the distributional sense:

  1. X2f=0 for every XΔ

  2. XYf+YXf=0 for every X,YΔ

  3. X12f++Xm2f=0 for every basis (X1,,Xm) of Δ.

Indeed, if a representative of fLloc1(G) is Δ-affine then (A.1) holds true as a consequence of the very definitions. Conversely, if fLloc1(G) satisfies (A.1) then f has a representative that is smooth by Hörmander’s hypoellipticity theorem and then it clearly follows from (A.1) that this representative is Δ-affine. The fact that (A.1) is equivalent to (A.2) is a consequence of Hörmander’s hypoellipticity theorem together with the identity (X+Y)2f=X2f+XYf+YXf+Y2f for smooth functions f. Condition (A.1) obviously implies (A.3). Conversely, if fLloc1(G) satisfies (A.3) and XΔ\{0}, one can complete X into a basis X,X2,,Xm of Δ. Then for every ε>0 one has X2f+εX22f++εXm2f=0 with the left-hand side converging to X2f as ε0 and therefore X2f=0. See also [1] for other generalizations of condition (A.1) for locally integrable functions.

To conclude this remark, note that in the specific setting considered in this paper, i.e., step-2 Carnot algebras g=g1g2, it follows from Theorem 1.3 that h-affine functions are smooth and hence locally integrable. Therefore each of the distributional sense conditions (A.1), (A.2), (A.3) with Δ=g1 makes sense for all h-affine functions and hence characterizes such a class of functions. In the more general setting considered in the present remark, it is, however, not clear to us whether Δ-affinity implies local integrability, and the class of locally integrable Δ-affine functions that can be characterized through each of the equivalent conditions (A.1), (A.2), and (A.3) could therefore be a strict subset of the class of Δ-affine functions.

Horizontally Affine Functions on Free Step-2 Carnot Algebras

This section is devoted to the proof of Theorem 1.1. The proof will proceed into 4 steps. We first verify in Lemma 3.1 that for ηΛn-iRn, we have φηAffh(fn,ΛnRn)i where φη is given by (1.1), together with the injectivity of the linear map ηΛn-iRnφηAffh(fn,ΛnRn)i. We shall next prove Theorem 1.1 for n=2, see Theorem 3.2, and deduce properties of h-affine functions on fn for n3 to be used in the next step, see Proposition 3.3. When n3, we first prove that Affh(fn)=i=0nAffh(fn)i together with preliminary information about elements in Affh(fn)i, see Proposition 3.4. We then upgrade these information in Proposition 3.5 to get the description stated in Theorem 1.1.

For notational convenience, we identify in this section fn with Λ1Rn×Λ2Rn and write elements in fn as x=(θ,ω) with θΛ1Rn, ωΛ2Rn. In the next lemma, we denote by Affh(fn,ΛnRn)i the analogue of Affh(fn)i for ΛnRn-valued functions. More explicitly, f:fnΛnRn belongs to Affh(fn,ΛnRn)i if and only if for every (θ,ω)fn, θΛ1Rn, the function tRf((θ,ω)·(tθ,0))ΛnRn is affine, and fδt=tif for all tR.

Lemma 3.1

For n2, i{0,,n}, and ηΛn-iRn, we have φηAffh(fn,ΛnRn)i where φη is given by (1.1). Furthermore, the linear map ηΛn-iRnφηAffh(fn,ΛnRn)i is injective.

Proof

Let ηΛn-iRn. Clearly φηδt=tiφη for all tR. If i=2k is even, we have

φη((θ,ω)·(tθ,0))=(ω+tθθ)kη=ωkη+tkωk-1θθη,

if i=2k+1 is odd,

φη((θ,ω)·(tθ,0))=(θ+tθ)(ω+tθθ)kη=θωkη+tθωkη,

for all (θ,ω)fn, θΛ1Rn. Therefore φηAffh(fn,ΛnRn)i. For the injectivity of the linear map ηΛn-iRnφηAffh(fn,ΛnRn)i, see Corollary 6.5.

Theorem 3.2

We have Affh(f2)=Aff(f2).

Proof

We recall that a set f2 is said to be a horizontal line if ={(θ,ω)·(tθ,0):tR} for some (θ,ω)f2, θΛ1R2\{0}. Define the h-affine hull of a set Af2 as the smallest set C containing A with the property that if a horizontal line meets C in more than one point then C. It follows from [5, Lemma 4.10] that there are 4 points in f2 whose h-affine hull is f2. Indeed, given linearly independent θ,θΛ1R2, the h-affine hull C of {(0,0),(θ,0),(θ,0),(θ+θ,θθ)} contains a pair of parallel lines with distinct projection in the sense of [5], namely, the horizontal line through (0, 0) and (θ,0) and the horizontal line through (θ,0) and (θ+θ,θθ), therefore C=f2 by [5, Lemma 4.10]. This implies that Affh(f2) is a vector space with dimension 4. Since Aff(f2) is a 4-dimensional linear subspace of Affh(f2), we get that Affh(f2)=Aff(f2), as claimed.

Note that Theorem 1.1 for n=2 follows from Lemma 2.5, Lemma 3.1 and Theorem 3.2. For n3, we set Σn:=θ,θΛ1RnLie(θ,θ) where Lie(θ,θ):=span{θ,θ}×span{θθ} denotes the Lie subalgebra of fn generated by θ,θΛ1Rn. We refer to Definition 2.1 for the definition of Σn-affine functions.

Proposition 3.3

For n3, fAffh(fn), the following hold true:

fisΣn-affine, 3.1
fωAff(Λ1Rn)for allωΛ2Rn, 3.2

where fω:Λ1RnR is given by fω(θ):=f(θ,ω) and Aff(Λ1Rn) denotes the space of real-valued affine functions on Λ1Rn.

Proof

Clearly, composing h-affine functions with left-translations yields h-affine functions. Therefore, to prove that every fAffh(fn) is Σn-affine, we only need to verify that for every fAffh(fn), θ1,θ2Λ1Rn, θ1θ20, (θ,ω)Lie(θ1,θ2), the function tRf(tθ,tω) is affine. Set h:=Lie(θ1,θ2) and denote by fh the restriction of f to h. On the one hand, the structure of step-2 Carnot algebra of fn induces on h a structure of step-2 Carnot algebra that makes it isomorphic to f2. Therefore Affh(h)=Aff(h) by Theorem 3.2. On the other hand, fhAffh(h). Thus fhAff(h), which implies that for all (θ,ω)h, the function tRf(tθ,tω) is affine and concludes the proof of (3.1). To prove (3.2), note that for ωΛ2Rn, θ,θΛ1Rn, tR, we have (θ+tθ,ω)=(θ,ω)·(tθ,tθθ). Since (θ,θθ)Σn, it follows from Proposition 6.1 that fωAff(Λ1Rn) for every Σn-affine function f, and hence, in particular for fAffh(fn) by (3.1).

In addition to the notations given in the appendix, see Sect. 6, we shall use the following ones in the rest of this section. Recall that (e1,,en) denotes a basis of Λ1Rn. For θ=j=1nθjejΛ1Rn, we set θJ:=θj1θjk for J=(j1,,jk)Jkn, see (6.4) for the definition of Jkn, with the convention θ:=1.

In the following, for α,βN, we write αβ to denote the multi-index with 2 indices. We set

I:=αβ:α,βN\{0},α<β,

and we equip I with the lexicographic order, i.e., we write αβ<αβ to mean either that α=α and β<β or that α<α. We set I¯0n:={},

I¯kn:=(α1β1,,αkβk)Ik:12α1β1<<αkβk(n-1)n

for k{1,,n(n-1)/2}, and I¯n:=0kn(n-1)/2I¯kn. We write im:= and imI:={α1β1,,αkβk}I for I=(α1β1,,αkβk)I¯kn. Given I,II¯n, we denote by I\II¯n the unique element in I¯n such that im(I\I)=imI\imI and we write II to mean that imIimI.

We recall from Sect. 6 that eJ:=ej1ejk for a multi-index J=(j1,,jk)Jkn. For ω=αβI¯1nJ2nωαβeαβΛ2Rn, we set ω:=1 and ωI:=ωα1β1ωαkβk for I=(α1β1,,αkβk)I¯kn.

We write N():= and N(I):={α1,β1,,αk,βk}N for I=(α1β1,,αkβk)I¯kn. We set I0n:={} and

Ikn:=(α1β1,,αkβk)I¯kn:N(αiβi)N(αjβj)=for allij.

for k{1,,n(n-1)/2}. Note that I¯0n=I0n, I¯1n=I1n. When n3, we have Ikn/I¯kn for 2kn(n-1)/2, and Ikn= for k>n/2.

Proposition 3.4

For n3, the following holds true:

  • (i)

    Affh(fn)=i=0nAffh(fn)i,

  • (ii)
    for k{0,,n/2}, every fAffh(fn)2k can be written as
    (θ,ω)IIknaIωI
    for constants aIR,
  • (iii)
    for k{0,,(n-1)/2}, every fAffh(fn)2k+1 can be written as
    (θ,ω)IIknbI(θ)ωI
    for linear forms bI:Λ1RnR.

Proof

For i{1,,n}, the Affh(fn)i are linear subspaces of Affh(fn) that are in direct sum. Therefore i=0nAffh(fn)iAffh(fn). Conversely, let fAffh(fn) be given.

We first prove that there are functions cI:Λ1RnR, II¯n, such that

f(θ,ω)=II¯ncI(θ)ωI. 3.3

Let θΛ1Rn be given. We know from (3.1) that, for every ωΛ2Rn, 1α<βn, the function tRf((θ,ω)·(0,teαβ)) is affine. Since f((θ,ω)·(0,teαβ))=f(θ,ω+teαβ), it follows from elementary properties of multiaffine maps, see Proposition 6.2 applied to ωΛ2Rnf(θ,ω), that there are cI(θ)R, II¯n, such that (3.3) holds true.

Next, we prove that

cIAff(Λ1Rn)for allII¯n. 3.4

We have I¯n=0kn(n-1)/2I¯kn and we prove by induction on k that cIAff(Λ1Rn) for all II¯kn. For k=0, we have I¯0n={} with c(θ)=f(θ,0) and we apply (3.2) with ω=0 to get that cAff(Λ1Rn). Given k{1,,n(n-1)/2}, assume that cIAff(Λ1Rn) for all I0ik-1I¯in. For I=(α1β1,,αkβk)I¯kn, we apply (3.2) with ω=j=1keαjβj to get that

cI+I0ik-1I¯inIIcIAff(Λ1Rn).

By induction hypothesis, we get that cIAff(Λ1Rn), which concludes the proof of (3.4).

It follows from (3.4) that there are constants aIR and linear forms bI:Λ1RnR, II¯n, such that cI(θ)=aI+bI(θ) for every θΛ1Rn. For k{0,,n(n-1)/2}, we set

f2k(θ,ω):=II¯knaIωIandf2k+1(θ,ω):=II¯knbI(θ)ωI,

so that f=i=0n(n-1)+1fi. We claim that fiAffh(fn)i for all i{0,,n(n-1)+1}. Indeed, let (θ,ω)fn, θΛ1Rn, sR be given. Since the dilations are Carnot automorphisms, we know from Lemma 2.3 that fδtAffh(fn) for all tR. Therefore

i=0n(n-1)+1tifi((θ,ω)·(sθ,0))=(fδt)((θ,ω)·(sθ,0))=(fδt)(θ,ω)+s((fδt)((θ,ω)·(θ,0))-(fδt)(θ,ω))=i=0n(n-1)+1ti(fi(θ,ω)+s(fi((θ,ω)·(θ,0))-fi(θ,ω)))

for all tR, which implies that fi((θ,ω)·(sθ,0))=fi(θ,ω)+s(fi((θ,ω)·(θ,0))-fi(θ,ω)) for all i{0,,n(n-1)+1}. Since this holds true for all (θ,ω)fn, θΛ1Rn, sR, we get that fiAffh(fn). Clearly, we also have fiδt=tifi for all tR. Therefore fiAffh(fn)i for all i{0,,n(n-1)+1}, as claimed.

For k{0,,n(n-1)/2}, we now claim that

aI=0for allII¯kn\Ikn. 3.5

For k{0,1}, we have I¯kn=Ikn and there is nothing to prove. Let k{2,,n(n-1)/2} be given. First, note that II¯kn\Ikn if and only if there are integers 1α<β<γn such that either (αβ,αγ)I, or (αγ,βγ)I, or (αβ,βγ)I. Now, let 1α<β<γn be given. On the one hand, since f2kAffh(fn), we know that, for every ωΛ2Rn, the function tRf2k((eα,ω)·(t(eβ+eγ),0)=f2k(0,ω+t(eαβ+eαγ)) is affine. On the other hand, this function is a polynomial for which the coefficient of t2, namely,

II¯kn(αβ,αγ)IaIωI\(αβ,αγ)

must therefore vanish. Since this holds true for every ωΛ2Rn, it follows that aI=0 for every II¯kn such that (αβ,αγ)I. Considering the function tRf2k(0,ω+t(eαγ+eβγ)), respectively, tRf2k(0,ω+t(eαβ+eβγ)), and arguing in a similar way, we get that aI=0 for every II¯kn such that (αγ,βγ)I, respectively, such that (αβ,βγ)I, which concludes the proof of (3.5).

For k{0,,n(n-1)/2}, we claim that

bI(θ)=0for allθΛ1Rn,II¯kn\Ikn. 3.6

Indeed, let k{0,,n(n-1)/2}, θΛ1Rn be given. Consider the function g:fnR given by g(τ,ω):=f2k+1(θ,ω) for (τ,ω)fn. We have g((τ,ω)·(tτ,0))=f2k+1((θ,ω)·(0,tττ)) for all (τ,ω)fn, τΛ1Rn. Since f2k+1Affh(fn), it follows from (3.1) that gAffh(fn). We then argue as for the proof of (3.5) to get that bI(θ)=0 for every II¯kn\Ikn, which concludes the proof of (3.6).

For k{n/2+1,,n(n-1)/2}, we have Ikn= and it follows from (3.5) and (3.6) that f2k=f2k+1=0.

We now prove that fn+1=0 whenever n is even. Assume that n=2p with p2. Let I=(α1β1,,αpβp)Ip2p be given. Note that N(I)={1,,2p}. Therefore, to show that bI=0, we need to verify that bI(eαj)=bI(eβj)=0 for every j{1,,p}. Let j{1,,p} be given. Set ωj:=1ip,ijeαiβi. On the one hand, since fn+1Affh(fn), the function tRfn+1((eαj,ωj)·(teβj,0)) is affine. On the other hand,

fn+1((eαj,ωj)·(teβj,0))=fn+1(eαj+teβj,teαjβj+ωj)=tbI(eαj+teβj)=tbI(eαj)+t2bI(eβj).

Therefore the coefficient of t2 vanishes, i.e., bI(eβj)=0. To prove that bI(eαj)=0, we argue in a similar way considering the function tRfn+1((-eβj,ωj)·(teαj,0)).

All together, we have shown that f=i=0nfi with fiAffh(fn)i that can be written as in (ii) when i=2k is even, respectively, as in (iii) when i=2k+1 is odd, which concludes the proof of the proposition.

Proposition 3.5

For n3, i{0,,n}, νΛnRn\{0}, every fAffh(fn)i can be written as fν=φη for some ηΛn-iRn.

Proof

Assume with no loss of generality that ν=e1en. We first prove the proposition when i=2k is even. Let fAffh(fn)2k and let aIR, IIkn, be given by Proposition 3.4 (ii) so that

f(θ,ω)=IIknaIωI.

For k=0 we get that f is constant and the required conclusion clearly holds true. Next, let us consider the case n=2p with p2 and k=p. For ωΛ2R2p, we have

ωp=p!IIp2pσ(I)ωIν

where, given I=(α1β1,,αpβp)Ip2p, σ(I) denotes the signature of the permutation of {1,,2p} given by (1,2,,2p)(α1,β1,,αp,βp). Therefore it suffices to prove that

σ(I)aI=σ(I)aIfor allI,IIp2p. 3.7

On the one hand, since fAffh(f2p), we know that for all (θ,ω)f2p, θΛ1R2p, the function

tRf((θ,ω)·(tθ,0))=IIp2paI(ω+tθθ)I

is affine. On the other hand, this function is a polynomial for which the coefficient of t2 is given by

IIp2paIH,KI12pH,KI,HKωI\(HK)(θθ)H(θθ)K=LIp-22pωLIIp2pILaI(θθ)I\L

and must therefore vanish. Since this holds true for all ωΛ2R2p, it follows that for all LIp-22p, θ,θΛ1R2p,

IIp2pILaI(θθ)I\L=0.

Now let LIp-22p be given and let 1α<β<δ<γ2p be such that {1,,2p}\N(L)={α,β,δ,γ}. Then the previous equality reads as

aL(αβ,δγ)(θθ)αβ(θθ)δγ+aL(αδ,βγ)(θθ)αδ(θθ)βγ+aL(αγ,βδ)(θθ)αγ(θθ)βδ=0

for all θ,θΛ1R2p. Looking at the coefficient of θαθβθδθγ we get that aL(αβ,δγ)=aL(αγ,βδ). Looking at the coefficient of θαθδθβθγ we get that aL(αδ,βγ)=-aL(αγ,βδ). Therefore, we have proved that σ(I)aI=σ(I)aI for all I,IIp2p such that I,IL for some LIp-22p. Since one can pass from any IIp2p to any IIp2p by a finite number of such steps, (3.7) follows.

Let us now consider the case n3 and i=2k is even with 2in-1. For JJ2kn set IkJ:={IIkn:N(I)=imJ} and define fJ:fnR by fJ(θ,ω):=IIkJaIωI so that

f=JJ2knfJ.

Set Λ1J:=span{ej:jimJ} and Λ2J:=span{ejj:j,jimJ}. We have fJ((θ,ω)·(tθ,0))=f((θ,ω)·(tθ,0)) for all θ,θΛ1J, ωΛ2J. Since fAffh(fn), it follows that the restriction of fJ to Λ1J×Λ2Jf2k belongs to Affh(f2k). Since (fJδt)(θ,ω)=t2kfJ(θ,ω) for all (θ,ω)Λ1J×Λ2J and all tR, we get that the restriction of fJ to Λ1J×Λ2J belongs to Affh(f2k)2k and it follows from the previous case that there is ηJR such that fJ(θ,ω)eJ=ηJωk for all (θ,ω)Λ1J×Λ2J. Since fJ does not depend on θ, this equality holds actually true for all θΛ1Rn, ωΛ2J. For (θ,ω)fn, we have fJ(θ,ω)=fJ(θ,ΠJ(ω)) where ΠJ:Λ2RnΛ2J denotes the projection map given by ΠJ(ω):=1j<jnj,jimJωjjejj. Therefore, for (θ,ω)fn, we have

f(θ,ω)ν=JJ2knfJ(θ,ΠJ(ω))ν=JJ2knσJηJΠJ(ω)keJc

where σJ{-1,1} is such that ν=σJeJeJc. Now, note that (ω-ΠJ(ω))eJc=0, therefore ΠJ(ω)keJc=ωkeJc, and the previous equality becomes

f(θ,ω)ν=JJ2knσJηJωkeJc=ωkη

where η:=JJ2knσJηJeJcΛn-2kRn, which concludes the proof of the proposition when i=2k is even.

We now consider the case where i=2k+1 is odd. Let fAffh(fn)2k+1 and let bI:Λ1RnR, IIkn, be linear forms given by Proposition 3.4 (iii) so that

f(θ,ω)=IIknbI(θ)ωI.

For k=0 we get that f(θ,ω)=b(θ) and the required conclusion clearly holds true. Thus assume that k{1,,(n-1)/2} and let θΛ1Rn be given. As in the proof of (3.6), consider the function g:fnR given by g(τ,ω):=f2k+1(θ,ω) for (τ,ω)fn. We have gAffh(fn), see the proof of (3.6), and since gδt=t2kg, it follows that gAffh(fn)2k. Then we know from the previous cases and Corollary 6.5 that there is a unique η¯(θ)Λn-2kRn such that f(θ,ω)ν=ωkη¯(θ) for all ωΛ2Rn. Next, it follows from the linearity of the bI that the map θΛ1Rnωkη¯(θ) is linear for every ωΛ2Rn. Since span{ωk:ωΛ2Rn}=Λ2kRn, see (6.1), we get that η¯:Λ1RnΛn-2kRn is linear. We now claim that θη¯(θ)=0 for all θΛ1Rn. Indeed, on the one hand, we know that the function tRf((θ,ω)·(tθ,0))=f(θ+tθ,ω+tθθ) is affine for all (θ,ω)fn, θΛ1Rn. On the other hand, we have

graphic file with name 12220_2023_1360_Equ55_HTML.gif

and hence the coefficient of t2 vanishes, i.e., ωk-1θθη¯(θ)=0 for every θ,θΛ1Rn, ωΛ2Rn. Since span{ωk-1θ:θΛ1Rn,ωΛ2Rn}=Λ2k-1Rn, see (6.2), we get that θη¯(θ)=0 for all θΛ1Rn, as claimed. Then the required conclusion follows from Proposition 6.6, and this concludes the proof of the proposition.

Horizontally Affine Functions on Arbitrary Step-2 Carnot Algebras

In this section, we prove Theorem 1.2, that will be deduced from Theorem 1.1 writing a step-2 rank-r Carnot algebra that is not isomorphic to fr as a proper quotient of fr, and Theorem 1.3. The main argument for proving both theorems is given in Lemma 4.1 where we characterize those functions in Affh(fn)j that factor through fn/i where i a graded ideal of fn. We refer to (6.5) and (6.6) for the notions of annihilators. For notational convenience, we shall again identify fn with Λ1Rn×Λ2Rn throughout this section.

Lemma 4.1

Let n2 and i be a graded ideal of fn. For j{0,,n}, ηΛn-jRn, the map φη given by (1.1) factors through fn/i if and only if ηAnhn-ji.

Proof

Write the graded ideal i of fnΛ1Rn×Λ2Rn as i=i1×i2 where i1, i2 are linear subspaces of Λ1Rn, Λ2Rn such that θθi2 for all θΛ1Rn, θi1. Recall that φ:fnΛnRn factors through fn/i if and only if φ(θ+τ,ω+ζ)=φ(θ,ω) for all (θ,ω)fn, (τ,ζ)i. If ηΛnRn then φη is constant and therefore clearly factors through fn/i. Since Anhni=ΛnRn, see (6.7), this proves the lemma for j=0. If ηΛn-1Rn then φη(θ,ω)=θη. Therefore φη factors through fn/i if and only if τη=0 for all τi1, i.e., ηAnhn-1i1=Anhn-1i, where the last equality comes from (6.8), which proves the lemma for j=1. Now let j{2,,n}. For ηAnhn-ji, it easily follows from (1.1) that φη factors through fn/i. Conversely, let ηΛn-jRn and assume that φη factors through fn/i. Then, for all (θ,ω)fn, ζi2, tR, we have φη(θ,ω+tζ)=φη(θ,ω), i.e.,

(ω+tζ)kη=ωkηifj=2kis evenθ(ω+tζ)kη=θωkηifj=2k+1is odd.

Identifying the coefficient of degree 1 in t, we get that for all θΛ1Rn, ωΛ2Rn, ζi2,

ωk-1ζη=0ifj=2kis evenθωk-1ζη=0ifj=2k+1is odd.

It then follows from (6.1) when j is even, (6.2) when j is odd, and Lemma 6.4 that ζηAnhn-j+2Λj-2Rn={0} for all ζi2, i.e., ηAnhn-ji2=Anhn-ji, where the last equality comes from (6.9), and this concludes the proof of the lemma.

We first prove Theorem 1.2.

Proof of Theorem 1.2

Let g be a step-2 rank-r Carnot algebra that is not isomorphic to fr. Clearly, i=0r-1Affh(g)iAffh(g). To prove the converse inclusion, let π:frg be a surjective Carnot morphism and νΛrRr\{0} be fixed. Recall for further use that Kerπ is a nontrivial graded ideal of fr. Let fAffh(g). Then fπAffh(fn) by Lemma 2.3 and it follows from Theorem 1.1 that there are ηiΛr-iRr, i{0,,r}, such that (fπ)ν=i=0rφηi. We claim that each φηi factors through fr/Kerπ. Indeed, since π commutes with dilations, we have for all (θ,ω)fr, (τ,ζ)Kerπ, tR,

i=0rtiφηi(θ+τ,ω+ζ)=i=0r(φηiδt)(θ+τ,ω+ζ)=(fπδt)(θ+τ,ω+ζ)ν=(fδtπ)(θ+τ,ω+ζ)ν=(fδtπ)(θ,ω)ν=(fπδt)(θ,ω)ν=i=0r(φηiδt)(θ,ω)=i=0rtiφηi(θ,ω).

This implies that for all i{0,,r}, φηi(θ+τ,ω+ζ)=φηi(θ,ω) for all (θ,ω)fr, (τ,ζ)Kerπ, i.e., φηi factors through fr/Kerπ, as claimed. Since π is surjective, it follows that for each i{0,,r} there is fi:gR such that (fiπ)ν=φηi. Since φηiAffh(fn,ΛnRn)i, we get from Corollary 2.4 that fiAffh(g)i (note indeed that the analogue of Corollary 2.4 holds true for ΛnRn-valued functions). Let us now verify that fr=0. Since φηr factors through fr/Kerπ, we know from Lemma 4.1 that ηrAnh0Kerπ. Since g is not isomorphic to fr, we have Kerπ{0} and hence Anh0Kerπ={0}. Therefore ηr=0 and hence fr=0. All together we get that f=i=0r-1fii=0r-1Affh(g)i and this concludes the proof of Theorem 1.2.

We now prove Theorem 1.3

Proof of Theorem 1.3

Let g be a step-2 rank-r Carnot algebra, nr, and π:fng be a surjective Carnot morphism. Let i{0,,n}, νΛnRn\{0}, ηAnhn-iKerπ. Since Kerπ is a graded ideal of fn, we know from Lemma 4.1 that φη factors through fn/Kerπ and since π is surjective we get the existence of a unique function f:gR such that (fπ)ν=φη. Furthermore, since φηAffh(fn,ΛnRn)i, we get from Corollary 2.4 that fAffh(g)i, which concludes the proof of Theorem 1.3 (i). Conversely, let fAffh(g)i. Then fπAffh(fn)i by Corollary 2.4 and it follows from Theorem 1.1 (ii) that there is a unique ηΛn-iRn such that (fπ)ν=φη. This equality shows in turn that φη factors through fn/Kerπ and hence ηAnhn-iKerπ by Lemma 4.1, which concludes the proof Theorem 1.3 (ii). By linearity of the map ηφη, we get that the bijective map ηAnhn-iKerπfAffh(g)i where f is given by Theorem 1.3 (i) is linear and therefore is an isomorphism of vector spaces, which concludes the proof of Theorem 1.3 (iii). By Theorem 1.1 (i) and Theorem 1.2, it follows that Affh(g) and i=0nAnhn-iKerπ are isomorphic as vector spaces. Finally, since Kerπ is a graded ideal of fn, we get from Corollary 6.9 that AnhKerπ=i=0nAnhn-iKerπ. Therefore Affh(g) and AnhKerπ are isomorphic as vector spaces, which concludes the proof of Theorem 1.3 (iv).

Remark 4.2

If g is a step-2 rank-r Carnot algebra that is not isomorphic to fr then dimAffh(g)2r-r+1. Indeed consider a surjective Carnot morphism π:frg. Then Kerπ is a nontrivial graded ideal of fr that is contained in Λ2Rr. Therefore AnhrKerπ=ΛrRr by (6.7), Anhr-1Kerπ=Anhr-1{0}=Λr-1Rr where the first equality follows from (6.8), and Anhr-iKerπ/Λr-iRr for i{2,,r-1}. This latter claim indeed follows from the inclusion KerπΛ2Rr together with the fact that Anh2Λr-iRr={0} for i{2,,r-1}, see Lemma 6.4. By Theorem 1.3 (iii) we get that Affh(g)i and Λr-iRr are isomorphic for i{0,1} and dimAffh(g)idimΛr-iRr-1 for i{2,,r-1}. Therefore dimAffh(g)2r-r+1 by Theorem 1.2.

Remark 4.3

It follows from Theorems 1.11.2,  1.3 (iii), and Lemma 6.11 that if g is a step-2 Carnot algebra then Affh(g)i={0} for some non-negative integer i if and only if jiAffh(g)j={0}.

Remark 4.4

Note that it follows from Theorems 1.1 and 1.3 (iii) that if n>r2 and π:fnfr is a surjective Carnot morphism then Anhn-iKerπ={0} for i{r+1,,n}. Similarly, it follows from Theorems 1.2 and 1.3 (iii) that if g is a step-2 rank-r Carnot algebra that is not isomorphic to fr, nr, and π:fng is a surjective Carnot morphism then Anhn-iKerπ={0} for i{r,,n}.

Step-2 Carnot Algebras Where Horizontally Affine Functions are Affine

Characterization

This section is devoted to the proof of Theorem 1.4 that characterizes step-2 Carnot algebras where h-affine functions are affine. We begin with an easy consequence of Theorem 1.3.

Lemma 5.1

Let g be a step-2 Carnot algebra. Then i=02Affh(g)i=Aff(g).

Proof

We already know from Lemma 2.5 that Aff(g)i=02Affh(g)i. Conversely, let fi=02Affh(g)i. Let r:=rankg, π:frg be a surjective Carnot morphism, and νΛrRr\{0}. By Theorem 1.3 (ii) there are ηiAnhn-iKerπ, i{0,1,2}, such that (fπ)ν=i=02φηi. Then it clearly follows from the form of φηi, see (1.1), together with the fact that π is a surjective Carnot morphism that fAff(g).

We now turn to the proof of Theorem 1.4.

Proof of Theorem 1.4

The equivalence between Theorem 1.4 (i) and (ii) follows from Lemmas 2.5 and 5.1. Next, Theorem 1.4 (ii) clearly implies Theorem 1.4 (iii) since Affh(g)i are linear subspaces of Affh(g) that are in direct sum, recalling also that i3Affh(g)i={0} if and only if Affh(g)3={0}, see Remark 4.3.

Now, assume that Affh(g)3={0}. Let b:g1×g2R be a bilinear form such that b(x,[x,x])=0 for all x,xg1. Identifying g with g1×g2, we have for x,xg1, zg2, tR,

b((x,z)·(tx,0))=b(x+tx,z+t[x,x])=b(x,z)+tb(x,z)+tb(x,[x,x])+tb(x,[x,x])=b(x,z)+tb(x,z)

and b(δt(x,z))=b(tx,t2z)=t3b(x,z). Therefore bAffh(g)3 and hence b=0, which proves that g is I-null.

Next, assume that g is I-null. Let nmax{3,rankg} and π:fng be a surjective Carnot morphism and let us verify that Anhn-3Kerπ={0}. Let νΛnRn\{0} be given. By Theorem 1.3 (i), for ηAnhn-3Kerπ there is fAffh(g)3 such that (fπ)ν=φη. Identifying fn with Λ1Rn×Λ2Rn, we have φη(θ,ω)=θωη. Therefore φη:Λ1Rn×Λ2RnΛnRn is bilinear. Since π is a surjective Carnot morphism, it follows that f:gg1×g2R is bilinear as well. Furthermore, for x,xg1, let θ,θΛ1Rn be such that x=π(θ), x=π(θ). Then [x,x]=π(θθ) and hence, identifying g with g1×g2, we have (x,[x,x])=π(θ,θθ). Therefore f(x,[x,x])ν=φη(θ,θθ)=0. Since g is I-null, it follows that f=0 and hence η=0 by Corollary 6.5. Therefore Anhn-3Kerπ={0}, as wanted. Recall that this is in turn equivalent to i=3nAnhn-iKerπ={0} by Lemma 6.11.

To conclude the proof of Theorem 1.4, assume that there are nmax{3,rankg} and a surjective Carnot morphism π:fng such that i=3nAnhn-iKerπ={0}. By Theorem 1.3 (iii) we get that i=3nAffh(g)i={0} and Theorems 1.1 (i) and 1.2 imply in turn Theorem 1.4 (ii).

Examples

In this section, we deduce from Theorem 1.4 sufficient conditions implying that h-affine functions are affine and necessary conditions that must be satisfied when this is the case. These conditions may be easier to verify on concrete examples than those given in the characterization obtained in Theorem 1.4. We, however, illustrate with explicit examples to what extent some of these easier conditions cannot be turned into characterizations of step-2 Carnot algebras where h-affine functions are affine. We shall also see from some of these examples that, unlike affine functions, a h-affine function defined on a Lie subalgebra of a step-2 Carnot algebra may not admit a h-affine extension to the whole algebra.

Proposition 5.2

Let g be a step-2 Carnot algebra and assume there is xg1 such that adx:yg1[x,y]g2 is surjective. Then Affh(g)=Aff(g).

Proof

If adx is surjective for some xg1 then so is adx for xU for some open neighborhood Ug1 of x. If b:g1×g2R is a bilinear form such that b(u,[u,v])=0 for all u,vg1 then, by bilinearity of b and surjectivity of adx, we get b(x,z)=0 for all xU, zg2, and finally b=0, using once again the bilinearity of b together with the fact that U is a nonempty open subset of g1. Therefore g is I-null and hence Affh(g)=Aff(g) by Theorem 1.4 (i)–(iv).

Proposition 5.2 applies in particular to step-2 Carnot algebras of Métivier’s type, i.e., step-2 Carnot algebras where adx is surjective for all xg1\{0}.

The condition given in Proposition 5.2 about the surjectivity of adx for some xg1 implying that g is I-null should not be confused with the surjectivity of the Lie bracket [·,·]:g1×g1g2. Indeed, step-2 Carnot algebras of Métivier’s type are examples of I-null Lie algebras where the Lie bracket is surjective, whereas Example 5.3 below gives an example of a I-null step-2 Carnot algebra where the Lie bracket is not surjective. On the other hand, free step-2 Carnot algebras of rank 3 or higher are not I-null whereas the Lie bracket (θ,θ)Λ1Rn×Λ1RnθθΛ2Rn is surjective if and only if n=3.

Example 5.3

Let i be the graded ideal of f4 given by i:=span{e12+e34} and let g:=f4/i. Elementary computations show that Anh1i={0}. Therefore Affh(g)=Aff(g) and g is I-null by Theorem 1.4 (i)–(iv)–(v). To see that the Lie bracket is not surjective we identify g with Λ1R4g2 where g2:={ωΛ2R4:ω34=0}. The only nontrivial bracket relations are given by

[θ,θ]=((θ1θ2-θ1θ2)-(θ3θ4-θ3θ4))e12+13ij24(θiθj-θiθj)eij

for θ,θΛ1R4 and we claim that

Im[·,·]{ωg2:ω14=ω23=0}{ωg2:ω122+4ω13ω240}.

Indeed, let ω=[θ,θ] with θ,θΛ1R4. Set ui:=(θi,θi)R2 for i=1,2,3,4. We have ωij=det(ui,uj) for 13ij24. If u2=(0,0) or u4=(0,0) then ω24=0 and we obviously have ω122+4ω13ω24=ω1220. Assume now that u2(0,0), u4(0,0), and ω14=ω23=0. Then u1 and u4, respectively, u2 and u3, are colinear. Therefore there are s,tR such that u1=su4 and u3=tu2. Since ω12=det(u1,u2)-det(u3,u4), we get that ω122+4ω13ω24=((s+t)2-4st)det(u2,u4)2=(s-t)2det(u2,u4)20, as claimed.

Given a step-2 Carnot algebra g, we say that g is a quotient of g if g is a step-2 Carnot algebra and there is a surjective Carnot morphism π:gg.

Proposition 5.4

Let g be a step-2 Carnot algebra such that Affh(g)=Aff(g). Then Affh(g)=Aff(g) for every quotient g of g.

Proof

By [11, Lemma 2.3] every quotient of a I-null Lie algebra is I-null and hence the proposition follows from Theorem 1.4 (i)–(iv).

Note that it may happen that Aff(g)/Affh(g) while Affh(g)=Aff(g) for every proper quotient g of g, i.e., for every quotient of g that is not isomorphic to g. A simple example is given by the free step-2 rank-3 Carnot algebra f3. Indeed, we know from Theorem 1.1 that Aff(f3)/Affh(f3), whereas every proper quotient g of f3 is either isomorphic to f2 or has rank 3 and is not isomorphic to f3, therefore Affh(g)=Aff(g) by Theorems 3.2, 1.2, and 1.4 (i)–(ii). See also Example 5.6 for another example that is not isomorphic to f3.

Note also that since Aff(f3)/Affh(f3), Proposition 5.4 has the following immediate corollary.

Corollary 5.5

Let g be a step-2 Carnot algebra that has f3 as one of its quotients. Then Aff(g)/Affh(g).

It may happen that Aff(g)/Affh(g) while g does not have f3 as one of its quotients, as shows Example 5.6 where g is a step-2 rank-5 Carnot algebra such that Aff(g)/Affh(g) and Affh(g)=Aff(g) for every proper quotient g of g.

Example 5.6

Let i be the graded ideal of f5 given by i:=Anh2{ζ} where ζ:=e12+e45 and let g:=f5/i so that g is in particular a step-2 rank-5 Carnot algebra and therefore is not isomorphic to f3. We have ζAnh2i and hence Aff(g)/Affh(g) by Theorem 1.4 (i)–(v). We now claim that Affh(g)=Aff(g) for every proper quotient g of g. Indeed, let g be a proper quotient of g and let π:gg be a surjective Carnot morphism. Let π¯:f5g denote the quotient map so that ππ¯:f5g is a surjective Carnot morphism and let us verify that Anh2Kerππ¯={0}. Let ηAnh2Kerππ¯. We have Anh1{ζ}Anh2{ζ}={0}Anh2{ζ}=Kerπ¯Kerππ¯Anh1{η}Anh2{η}. Since Anh2{ζ}=span{e12-e45,e14,e15,e24,e25}, we have (e12-e45)η=0, implying η34=η35=η45-η12=η13=η23=0, and eijη=0 for i=1,2, j=4,5, implying ηij=0 for i=1,2, j=4,5. Therefore ηspan{ζ}. If η0 then Anh1{η}Anh2{η}=Anh1{ζ}Anh2{ζ} which implies in turn Kerπ¯=Kerππ¯ and therefore Kerπ={0}. This contradicts the fact that g is a proper quotient of g and hence η=0. Therefore Anh2Kerππ¯={0} and it follows from Theorem 1.4 (i)–(v) that Affh(g)=Aff(g), as claimed.

We recall that the direct product g×Rd of a step-2 Carnot algebra with an abelian Lie algebra and the direct product g×g of step-2 Carnot algebras inherit naturally of a structure of step-2 Carnot algebra from those of g and g.

Proposition 5.7

Let g,g be a step-2 Carnot algebras and d1 be an integer. Then the following hold true:

  • (i)

    Affh(g×g)=Aff(g×g) if and only if Affh(g)=Aff(g) and Affh(g)=Aff(g)

  • (ii)

    Affh(g×Rd)=Aff(g×Rd) if and only if Affh(g)=Aff(g).

Proof

By [11, Lemma 2.3], any finite direct product of I-null Lie algebras is I-null. Therefore it follows from Theorem 1.4 (i)–(iv) that Affh(g×g)=Aff(g×g) whenever Affh(g)=Aff(g) and Affh(g)=Aff(g). Similarly, since abelian Lie algebras are I-null (see Definition 2.6), we have Affh(g×Rd)=Aff(g×Rd) whenever Affh(g)=Aff(g). The converse implications in (i) and (ii) follow from Proposition 5.4 noting that the projection maps from g×g onto either g or g and from g×Rd onto g are surjective Carnot morphisms.

The next proposition is another simple consequence of Theorem 1.4 that gives a sufficient condition ensuring that h-affine maps are affine.

Proposition 5.8

Let g be a step-2 Carnot algebra such that Aff(g)/Affh(g). Then there is a Lie subalgebra of g isomorphic to f3.

Proof

By Theorem 1.4 (i)–(iv) we know that g is not I-null. Then let b:g1×g2R be a non-zero bilinear form such that b(x,[x,x])=0 for all x,xg1. Since b0, there are xg1, zg2 such that b(x,z)0. By bilinearity together with the fact that [g1,g1]=g2, it follows that there are x1,x2,x3g1 such that b(x1,[x2,x3])=1. We claim that [x1,x2],[x1,x3],[x2,x3] are linearly independent and therefore the Lie subalgebra of g generated by x1,x2,x3 is isomorphic to f3. Indeed, note that since b(x,[x,x])=0 for all x,xg1, the trilinear form (x,x,x)g1×g1×g1b(x,[x,x]) is alternating and therefore b(x3,[x1,x2])=-b(x2,[x1,x3])=b(x1,[x2,x3])=1. Now let s1,s2,s3R be such that s3[x1,x2]+s2[x1,x3]+s1[x2,x3]=0. For i{1,2,3}, we have b(xi,s3[x1,x2]+s2[x1,x3]+s1[x2,x3])=sib(xi,[xk,xl])=0 where k<l and {k,l}={1,2,3}\{i}. Since b(xi,[xk,xl])0 for such indices ikl, it follows that s1=s2=s3=0, which concludes the proof of the lemma.

We stress that I-null step-2 Carnot algebras may have Lie subalgebras isomorphic to f3, as shown in the following two examples.

Example 5.9

[The quaternionic Heisenberg algebra.] Let ijk denote the quaternion units satisfying i2=j2=k2=ijk=-1 and denote by H:={q1+iq2+jq3+kq4:qiR} the set of quaternions. Given q=q1+iq2+jq3+kq4H, denote by Imq:=iq2+jq3+kq4 its imaginary part and q¯:=q1-iq2-jq3-kq4 its conjugate. Equip HImH with the Lie bracket for which the only nontrivial relations are given by [q,q]:=Im(q¯q) for q,qH which makes HImH a step-2 Carnot algebra that is well known to be of Heisenberg type, and therefore of Métivier’s type (see for instance [9]). Therefore, we have Affh(HImH)=Aff(HImH) and HImH is I-null by Proposition 5.2. We now claim that the Lie subalgebra of HImH generated by any three linearly independent elements in H is isomorphic to f3. Indeed, for q,qH, we have [q,q]=0 if and only if q and q are colinear. This indeed follows from the fact that for qH\{0}, the linear map adq:qH[q,q]ImH is surjective with qKeradq, together with the fact that dimH=4 and dimImH=3. Then let q1,q2,q3H be linearly independent and assume by contradiction that dimspan{[qi,qj]:i,j{1,2,3}}2. Exchanging the role of q1,q2,q3 if necessary, there are s,tR such that [q2,q3]=s[q1,q2]+t[q1,q3]. Then [q2-tq1,sq1+q3]=0 which implies that q2-tq1 and sq1+q3 are colinear and contradicts the fact that q1,q2,q3 are linearly independent. Therefore dimspan{[qi,qj]:i,j{1,2,3}}=3 and the Lie subalgebra generated by q1,q2,q3 is isomorphic to f3, as claimed.

Example 5.10

Let g:=f4/i where i:=span{e12+e34} be the I-null step-2 Carnot algebra given by Example 5.3. We claim that the Lie subalgebra of g generated by any three linearly independent elements in Λ1R4 is isomorphic to f3. Indeed let π:f4g denote the quotient map. Let θ1,θ2,θ3Λ1R4 be linearly independent and let a,b,cR be such that aπ(θ1θ2)+bπ(θ1θ3)+cπ(θ2θ3)=0, i.e., aθ1θ2+bθ1θ3+cθ2θ3Kerπ. We have (aθ1θ2+bθ1θ3+cθ2θ3)2=0 while Kerπ=span{e12+e34} with (e12+e34)20. It follows that aθ1θ2+bθ1θ3+cθ2θ3=0 and hence a=b=c=0. This proves that dimspan{π(θiθj):i,j{1,2,3}}=3 and therefore the Lie subalgebra of g generated by θ1,θ2,θ3 is isomorphic to f3, as claimed.

Theorem 1.4 (i)–(iv) together with Proposition 5.8 has the following immediate consequence.

Proposition 5.11

Let g be a step-2 Carnot algebra with dimg22. Then Affh(g)=Aff(g).

If rankg=dimg2=3 then g is isomorphic to f3 and therefore Aff(g)/Affh(g). This fact generalizes to higher rank step-2 Carnot algebras g with dimg2=3 in the following way.

Proposition 5.12

Let g be a step-2 Carnot algebra with dimg2=3. Then Affh(g)=Aff(g) if and only if g is not isomorphic to f3×Rd for some non-negative integer d.

Proof

If g is isomorphic to the direct product f3×Rd for some non-negative integer d then g has f3 as one of its quotients and we know by Corollary 5.5 that Aff(g)/Affh(g). Conversely, assume that Aff(g)/Affh(g). First, if rankg=3, since dimg2=3, then g is isomorphic to f3. Next, assume that r:=rankg4. By Proposition 5.8, there are x1,x2,x3g1 generating a Lie subalgebra of g isomorphic to f3 and there is a bilinear form b:g1×g2R such that b(x,[x,x])=0 for all x,xg1 and b(x1,[x2,x3])=1. Set V:=span{x1,x2,x3}. We claim that for every xg1\V, there is xV such that x+x lies in the center of g, i.e., [y,x+x]=0 for all yg1. To prove this claim, let xg1\V be given. Since dimg2=3=dimspan{[xi,xj]:1i<j3}, there are xijR, i,j{1,2,3}, such that [xj,x]=x3j[x1,x2]-x2j[x1,x3]+x1j[x2,x3] for j{1,2,3}. Set x:=x32x1+x13x2+x21x3 and let us verify that x+xCenter(g). We first verify that [xj,x+x]=0 for j{1,2,3}. Since b(x,[x,x])=0 for all x,xg1, the bilinear form (y,y)V×Vb(y,[y,x]) is skew-symmetric. For y=1i3αixiV and y=1j3βjxjV, we have b(y,[y,x])=1i,j3xijαiβj. By skew-symmetry, we get xij=-xji for i,j{1,2,3} and it follows that [xj,x+x]=0 for j{1,2,3}. Now let yg1 and write [y,x+x]=s3[x1,x2]-s2[x1,x3]+s1[x2,x3] with siR. Since the trilinear form b(·,[·,·]) is alternating, we have b(xi,[y,x+x])=si. On the other hand, b(xi,[y,x+x])=-b(y,[xi,x+x])=0. Hence si=0 for i{1,2,3} and therefore [y,x+x]=0, as wanted. It now clearly follows from this claim that one can complete (x1,x2,x3) into a basis (x1,,xr) of g1 in such a way that x4,,xrCenter(g), i.e., g is isomorphic to f3×Rr-3.

To conclude this section, let us remark that a h-affine function defined on a Lie subalgebra of a step-2 Carnot algebra may not admit a h-affine extension to the whole algebra. Indeed, let g be a step-2 Carnot algebra such that Affh(g)=Aff(g) and such that there is a Lie subalgebra f of g isomorphic to f3, see Examples 5.9 and 5.10. Then Aff(f)/Affh(f) and therefore there is hAffh(f)\Aff(f). Assume there is h¯Affh(g) whose restriction to f is h. By assumption on g, we have h¯Aff(g). Since f is a linear subspace of g, it follows that the restriction of h¯ to f is affine, i.e., hAff(f), which gives a contradiction. Recall that on the contrary an affine function defined on an affine subspace of a vector space can always be extended to an affine function on the whole space.

Appendix About Linear and Exterior Algebra

We gather in this appendix some basic facts about linear and exterior algebra not pertaining to h-affine functions that have been used in the previous sections.

We start with a characterization of affine maps between real vector spaces whose elementary proof is left to the reader.

Proposition 6.1

Let E, F be real vector spaces. A map f:EF is affine if and only if for every x,yE, the map tRf(x+ty) is affine.

For the sake of completeness, we state below an elementary property of multiaffine functions that has been used in the proof of Proposition 3.4. The proof can easily be done by induction on the dimension and is left to the reader.

Proposition 6.2

Let p1 be an integer and E be a p-dimensional real vector space. Let f:ER and assume that there is a basis (e1,,ep) of E such that the map tRf(v+tej) is affine for every vE and j{1,,p}. Then f is a linear combination of the uJ, where J ranges over the subsets of {1,,p} and uJ(v):=jJvj for v=j=1pvjej with the convention u(v):=1.

The rest of this appendix is devoted to (basic) facts about exterior algebra that have been used throughout this paper. Although some of them look quite elementary, we were, however, unable to find references in the literature and thus provide proofs for the reader’s convenience.

Given integers n1 and k1, we denote by ΛkRn the set of alternating k-multilinear forms over Rn. For k=0, we set Λ0Rn:=R. We denote by ΛRn:=k0ΛkRn the exterior algebra equipped with exterior product . We recall that ΛkRn={0} if k>n. For ζΛRn, we set ζ0:=1 and ζk:=ζζktimes for k1.

Lemma 6.3

For n1, we have in ΛRn

span{ωk:ωΛ2Rn}=Λ2kRn, 6.1
span{θωk:θΛ1Rn,ωΛ2Rn}=Λ2k+1Rn 6.2

for all k0.

Proof

We only need to consider the nontrivial cases where n2 and 1kn/2. Then (6.1) and (6.2) follow from the identity

(θ1θ2++θ2k-1θ2k)k=k!θ1θ2k 6.3

for all θ1,,θ2kΛ1Rn.

Given n1, we set J0n:={},

Jkn:={(j1,,jk)Nk:1j1<<jkn} 6.4

for k{1,,n}, and Jn:=0knJkn. We write im:= and imJ:={j1,,jk}N for J=(j1,,jk)Jkn. Given J,JJn, we denote by J\J the unique element in Jn such that im(J\J)=imJ\imJ and we set Jc:=(1,,n)\J. We fix a basis (e1,,en) of Rn and denote by (e1,,en) its dual basis. For J=(j1,,jk)Jkn, we set eJ:=ej1ejkΛkRn with the convention e:=1.

The space of exterior annihilators of an element in ΛiRn of some given order k has been introduced in [7], see also [6, Section 2.2]. More generally, given n1, k0, and AΛRn, we define the annihilator of A in ΛRn, respectively, ΛkRn, as

AnhA:={ηΛRn:ηζ=0for allζA}, 6.5
AnhkA:=ΛkRnAnhA. 6.6

We also set ΛkRn:=ikΛiRn.

Lemma 6.4

For n1, k{0,,n}, we have AnhΛkRn=Λn-k+1Rn.

Proof

For k=0, we clearly have AnhΛ0Rn={0}=Λn+1Rn. Let n1 and k{1,,n} be given. Clearly Λn-k+1RnAnhΛkRn. Since AnhΛkRn is graded, i.e., AnhΛkRn=i0AnhiΛkRn (see Lemma 6.8), if equality fails then AnhiΛkRn{0} for some i{0,,n-k}. Let ηAnhiΛkRn\{0} and J=(j1,,ji)Jin be such that η(ej1,,eji)0. Then ηeJc=η(ej1,,eji)eJeJc0. However, we can write eJc=eJ1eJ2 for some J1Jkn, J2Jn-i-kn, and since ηAnhΛkRn, we get ηeJc=0, which gives a contradiction.

Writing F(A,B) to denote the set of maps f:AB we deduce from Lemmas 6.3 and 6.4 the following corollary.

Corollary 6.5

For k{0,,n/2}, the linear map Λn-2kRnF(Λ2Rn,ΛnRn) given by η(ωωkη) is injective. For k{0,,(n-1)/2}, the linear map Λn-2k-1RnF(Λ1Rn×Λ2Rn,ΛnRn) given by η((θ,ω)θωkη) is injective.

Proof

By linearity we only need to verify that these maps have trivial kernel. Let k{0,,n/2} and ηΛn-2kRn be such that ωkη=0 for all ωΛ2Rn. On the one hand, by (6.1) we have ηAnhn-2kΛ2kRn. On the other hand, by Lemma 6.4, we have Anhn-2kΛ2kRn={0}. Therefore η=0. Similarly, for k{0,,(n-1)/2} and ηΛn-2k-1Rn such that θωkη=0 for all (θ,ω)Λ1Rn×Λ2Rn, we have by (6.2) and Lemma 6.4 that ηAnhn-2k-1Λ2k+1Rn={0}.

The next proposition played a key role at the end of the proof of Proposition 3.5.

Proposition 6.6

For n1 the following holds. Let k{1,,n} and η¯:Λ1RnΛkRn be linear. Assume that θη¯(θ)=0 for all θΛ1Rn. Then there is ηΛk-1Rn such that η¯(θ)=θη for all θΛ1Rn.

Proof

When k=n every map η¯:Λ1RnΛnRn satisfies the assumption θη¯(θ)=0 for all θΛ1Rn. If η¯:Λ1RnΛnRn is in addition assumed to be linear and ηjR is such that η¯(ej)=ηje(1,,n), then η¯(θ)=θη for all θΛ1Rn where η:=j=1nσjηje(1,,n)\(j) and σj{-1,1} is such that e(1,,n)=σjeje(1,,n)\(j).

Let us now argue by induction on n. First, if n=1, the conclusion follows from the previous remark. Next, let n2. By the previous remark, we only need to consider the case where k{1,,n-1}. By linearity of η¯, we only need to prove that there is ηΛk-1Rn such that η¯(ej)=ejη for j{1,,n}. Set Vj:={xRn:ej(x)=0} for j{1,,n}.

For j{1,,n-1}, since ejη¯(ej)=0, we can write η¯(ej)=ejηj for some ηjΛk-1Vj. Next, write ηj=τjen+ζj for some τjΛk-2Vn and ζjΛk-1Vn (when k=1, τj=0). Define τ¯:Λ1VnΛk-1Vn and ζ¯:Λ1VnΛkVn to be linear and such that τ¯(ej)=ejτj and ζ¯(ej)=ejζj for all j{1,,n-1}. For θΛ1Vn, we have η¯(θ)=τ¯(θ)en+ζ¯(θ). Thus θη¯(θ)=θτ¯(θ)en+θζ¯(θ)=0 for all θΛ1Vn and this implies in turn that θτ¯(θ)=0 and θζ¯(θ)=0 for all θΛ1Vn. By induction, there are τΛk-2Vn (again τ=0 when k=1) and ζΛk-1Vn such that τ¯(θ)=θτ and ζ¯(θ)=θζ for all θΛ1Vn. It follows that η¯(θ)=θ(τen+ζ) for all θΛ1Vn. We set η:=τen+ζΛk-1Rn. To conclude the proof of the proposition, it remains to verify that η¯(en)=enη. Since 1kn-1, this is equivalent to showing that ejη¯(en)=ejenη for all j{1,,n}, see Lemma 6.4. By assumption, we have θη¯(θ)=0 for all θΛ1Rn and therefore θη¯(θ)+θη¯(θ)=0 for all θ,θΛ1Rn. It follows that ejη¯(en)=-enη¯(ej)=-enejη=ejenη for j{1,,n-1}. Since enη¯(en)=0=enenη, we finally get η¯(en)=enη, and this concludes the proof of the proposition.

Recall that a graded ideal i of fn can be seen as a linear subspace of ΛRn of the form i=i1i2 where i1,i2 are linear subspaces of, respectively, Λ1Rn,Λ2Rn such that θθi2 for all θΛ1Rn, θi1. The structure of annihilators of such subsets of ΛRn, and in particular Corollary 6.9 and Lemma 6.10, played a major role in Sect. 4. Before proving Corollary 6.9 and Lemma 6.10, we first state two elementary lemmas. The easy proof of Lemma 6.7 is left to the reader.

Lemma 6.7

Let VW be linear subspaces of ΛRn that are in direct sum. Then Anh(VW)=AnhVAnhW and Anhk(VW)=AnhkVAnhkW for all k0.

Lemma 6.8

Let n1, j0, AΛjRn. Then AnhA=k0AnhkA.

Proof

Clearly, k0AnhkAAnhA. Conversely, let η=k=0nηkAnhA where ηkΛkRn. For aA, we have k=0nηka=0 with ηkaΛk+jRn therefore ηka=0 for all k{0,,n}. Since this holds true for all aA, we get that ηkAnhkA for all k{0,,n}, and therefore ηk0AnhkA.

Corollary 6.9

Let i1,i2 be linear subspaces of, respectively, Λ1Rn,Λ2Rn. Then Anh(i1i2)=k0Anhk(i1i2).

Proof

By Lemmas 6.7 and 6.8, we have

Anh(i1i2)=Anhi1Anhi2=(k0Anhki1)(k0Anhki2)=k0Anhki1Anhki2=k0Anhk(i1i2).

Lemma 6.10

Let n2, i1,i2 be linear subspaces of, respectively, Λ1Rn,Λ2Rn such that θθi2 for all θΛ1Rn, θi1. Then

Anhn(i1i2)=ΛnRn, 6.7
Anhn-1(i1i2)=Anhn-1i1, 6.8
Anhn-i(i1i2)=Anhn-ii2fori{2,,n}. 6.9

Proof

Clearly, AnhnA=ΛnRn for all AΛ1Rn and (6.7) follows. By Lemma 6.7, we have Anhn-1(i1i2)=Anhn-1i1Anhn-1i2. For AΛ2Rn, we have Anhn-1A=Λn-1Rn therefore Anhn-1i2=Λn-1Rn and (6.8) follows. For i{2,,n}, clearly Anhn-i(i1i2)Anhn-ii2. Conversely, let ηAnhn-ii2 and θi1. By assumption, θθi2 for all θΛ1Rn. Therefore ηθθ=0 for all θΛ1Rn, i.e., ηθAnhn-i+1Λ1Rn=Λn-i+1RnΛnRn, where the last equality follows from Lemma 6.4. Since i{2,,n}, we have n-i+1n-1, therefore Λn-i+1RnΛnRn={0} and hence ηθ=0. Since this holds true for all θi1, we get that ηAnhn-ii1Anhn-ii2=Anhn-i(i1i2), where the last equality comes from Lemma 6.7 and concludes the proof of (6.9).

We end this section with an observation that has been useful for our purposes in Remark 4.3 and Sect. 5.

Lemma 6.11

Let n1, k{0,,n}, AΛRn be such that AnhkA={0}. Then AnhjA={0} for all j{0,,k}.

Proof

Let j{0,,k}, ηAnhjA. For all ζΛk-jRn, aA, we have ζηa=0, i.e., ζηAnhkA. Since AnhkA={0}, it follows that ηAnhjΛk-jRn=ΛjRnΛn-k+j+1Rn, where the last equality follows from Lemma 6.4. Since n-k0, we have n-k+j+1j+1, therefore ΛjRnΛn-k+j+1Rn={0} and hence AnhjA={0}.

Acknowledgements

The authors are grateful to an anonymous reader of a previous version of this paper for valuable comments and remarks that helped them to improve and simplify the exposition.

Funding

Open Access funding provided by University of Jyväskylä (JYU).

Footnotes

1

It is worth to stress that our arguments and results can be verbatim extended to finite dimensional nilpotent Lie algebras of step 2 over an arbitrary field of characteristic zero.

2

As already mentioned in the introduction, our arguments and results can be verbatim extended to finite dimensional nilpotent Lie algebras of step 2 over an arbitrary field of characteristic zero.

3

Our convention for the group law is nothing but a technical convenience. Any other choice where [xy] is replaced by c[x,y] for some cR\{0} independent of x and y leads to the same results.

E.L.D. was partially supported by the Academy of Finland (Grant 288501 ‘Geometry of subRiemannian groups’ and by Grant 322898 ‘Sub-Riemannian Geometry via Metric-geometry and Lie- group Theory’) and by the European Research Council (ERC Starting Grant 713998 GeoMeG ‘Geometry of Metric Groups’). S.R. is partially supported by ANR Project SRGI (Sub-Riemannian Geometry and Interactions) ANR-15-CE40-0018.

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Contributor Information

Enrico Le Donne, Email: enrico.ledonne@unifr.ch.

Daniele Morbidelli, Email: daniele.morbidelli@unibo.it.

Séverine Rigot, Email: severine.rigot@univ-cotedazur.fr.

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