Discussion on exact null boundary controllability of nonlinear fractional stochastic evolution equations in Hilbert spaces

Dedicated to the memory of Professor Ireneo Peral, with high feelings of admiration for his notable contributions in Mathematics and great affection

1.   Introduction

In recent years, geometric analysis and partial differential equations on the Heisenberg group have attracted great attention. In this article, we investigate some concentration–compactness results related to the Hardy–Sobolev embedding on the classical and fractional Folland–Stein spaces in the Heisenberg group. Before stating the main results, let us recall some relevant contributions in the topic.

The Heisenberg group $\mathbb H^n$ is the Lie group which has $\mathbb R^{2n+1}$ as a background manifold and whose group structure is given by the non–Abelian law

for all $\xi$, $\xi'\in \mathbb H^n$, with

We denote by $r$ the Korányi norm, defined as

with $\xi = (z, t)$, $z = (x, y) \in \mathbb R^n \times \mathbb R^n$, $t \in \mathbb R$, and $|z|$ the Euclidean norm in $\mathbb R^{2n}$.

A key result, whose importance is also due to its connection with the CR Yamabe problem, is the subelliptic Sobolev embedding theorem in $\mathbb H^n$, which is due to Folland and Stein ^[14]. This result is valid in the more general context of Carnot groups, but we state it in the set up of the Heisenberg group. If $1 < p < Q$, where $Q = 2n+2$ is the homogeneous dimension of the Heisenberg group $\mathbb{H}^n$, we know by ^[14] that there exists a positive constant $C = C(p, Q)$ such that

and $p^*$ is the critical exponent related to $p$. Moreover, the vector

is the horizontal gradient of a regular function $u$, where $\{X_j, Y_j\}_{j = 1}^n$ is the basis of horizontal left invariant vector fields on $\mathbb H^n$, that is

Unlike the Euclidean case, cf. ^[34] and ^[2], the value of the best constant in (1.1) is unknown. In the particular case $p = 2$, the problem of the determination of the best constant in (1.1) is related to the CR Yamabe problem and it has been solved by the works of Jerison and Lee ^{[21,22,23,24]}. In the general case, existence of extremal functions of (1.1) was proved by Vassilev in ^[35] via the concentration–compactness method of Lions, see also ^[20]. This method does not allow an explicit determination of the best constant $C_{ p^*}$ of (1.1). However, we know from ^[35] that $C_{ p^*}$ is achieved in the Folland–Stein space $S^{1, p}(\mathbb H^n)$, which is defined, for $1 < p < Q$, as the completion of $C_c^\infty(\mathbb H^n)$ with respect to the norm

Thus, we can write the best constant $C_{ p^*}$ of the Folland–Stein inequality (1.1) as

Note that the Euler–Lagrange equation of the nonnegative extremals of (1.1) leads to the critical equation

where the operator $\Delta_{H, p}$ is the well known $p$ Kohn–Spencer Laplacian, which is defined as

for all $\varphi \in C^2(\mathbb H^n)$.

The study of critical equations is deeply connected to the concentration phenomena, which occur when considering sequences of approximated solutions. Indeed, given a weakly convergent sequence $(u_k)_k$ in $S^{1, p}(\mathbb{H}^n)$, we can infer that $(u_k)_k$ is bounded in $L^{ p^*}(\mathbb H^n)$, but we do not have compactness properties in general. On the other hand, we know that the sequences $\mu_k = |D_H u|_H^{ p}d\xi$ and $\nu_k = |u_k|^{ p^*} d\xi$ weak$^*$ converge to some measures $\mu$ and $\nu$ in the dual space $\mathcal M(\mathbb H^n)$ of all real valued, finite, signed Radon measures on $\mathbb H^n$. An essential step in the concentration–compactness method is the study of the exact behavior of the limit measures in the space $\mathcal M(\mathbb H^n)$ and in the spirit of Lions. In particular, following ^[25,26], Ivanov and Vassilev in ^[20] proved the following result.

Theorem A (Lemma 1.4.5, Ivanov and Vassilev ^[20]). Let $(u_k)_k$ be a sequence in $S^{1, p}(\mathbb{H}^n)$ such that $u_k \rightharpoonup u$ in $S^{1, p}(\mathbb{H}^n)$ and $|u_k|^{ p^*} d\xi \overset{\ast}{\rightharpoonup} \nu$, $|D_H u_k|_H^{ p}d\xi \overset{\ast}{\rightharpoonup} \mu$ in $\mathcal M(\mathbb{H}^n)$, for some appropriate $u\in S^{1, p}(\mathbb{H}^n)$, and finite nonnegative Radon measures $\mu$, $\nu$ on $\mathbb H^n$.

Then, there exist an at most countable set $J$, a family of points $\{\xi_j\}_{j\in J}\subset\mathbb H^n$ and two families of nonnegative numbers $\{\mu_j\}_{j\in J}$ and $\{\nu_j\}_{j\in J}$ such that

where $\delta_{\xi_j}$ are the Dirac functions at the points $\xi_j$ of $\mathbb H^n$.

The aim of this paper is to extend Theorem A in two different ways. First, we want to prove a version of Theorem A suitable to deal with a combined Hardy and Sobolev embedding. Indeed, following ^[16], we set

Assume from now on that $1 < p < Q$ and let $\varphi\in C_c^\infty(\mathbb{H}^n \setminus \{O\})$. Then, the Hardy inequality in the Heisenberg group states as follows

Inequality (1.4) was obtained by Garofalo and Lanconelli in ^[16] when $p = 2$ and then extended to all $p > 1$ in ^[7,29]. When $p = 2$, the optimality of the constant $\left(2/(Q-2)\right)^2$ is shown in ^[18]. Let us also mention that a sharp inequality of type (1.4) has been derived in general Carnot–Carathéodory spaces by Danielli, Garofalo and Phuc in ^[8].

Obviously, inequality (1.4) remains valid in $S^{1, p}(\mathbb H^n)$. Moreover, inequalities (1.1) and (1.4) imply that for any $\sigma \in(-\infty, \mathcal H_{ p})$ the following best constant is well defined

where

Note that, when $\sigma = 0$, we recover the Sobolev embedding, that is $\mathcal I_0 = C_{ p^*}$. However, the Hardy embedding $S^{1, p}(\mathbb H^n)\hookrightarrow L^p(\mathbb H^n, \psi^p r^{-p}d\xi)$ is continuous, but not compact, even locally in any neighborhood of $O$, where $O = (0, 0)$ denotes the origin of $\mathbb H^n$. A challenging problem is then to provide sufficient conditions for the existence of a nontrivial solution to critical equations with Hardy terms in the whole space $\mathbb H^n$, when a triple loss of compactness takes place. To overcome this difficulty, we prove in Theorem 1.1 and Theorem 1.2 some versions of the concentration–compactness principle for related to the embedding (1.5).

Theorem 1.1. Let $\sigma \in(-\infty, \mathcal H_{ p})$ and let $(u_k)_k$ be a sequence in $S^{1, p}(\mathbb{H}^n)$ such that $u_k \rightharpoonup u$ in $S^{1, p}(\mathbb{H}^n)$, and$|u_k|^{ p^*} d\xi \overset{\ast}{\rightharpoonup} \nu$, $|D_H u_k|_H^{ p}d\xi \overset{\ast}{\rightharpoonup} \mu$, $|u_k|^{ p}\psi^ p\dfrac{d\xi}{r(\xi)^{ p}}\overset{\ast}{\rightharpoonup} \omega$ in $\mathcal M(\mathbb{H}^n)$, for some appropriate$u\in S^{1, p}(\mathbb{H}^n)$, and finite nonnegative Radon measures $\mu$, $\nu$, $\omega$ on $\mathbb H^n$.

Then, there exist an at most countable set $J$, a family of points $\{\xi_j\}_{j\in J}\subset\mathbb H^n$, two families of nonnegative numbers $\{\mu_j\}_{j\in J}$ and $\{\nu_j\}_{j\in J}$ and three nonnegative numbers $\nu_0, \mu_0, \omega_0$, such that

where$C_{ p^*} = \mathcal{I}_{0}$ and $\mathcal{I}_{\sigma}$ are defined in $(1.3)$ and $(1.5)$, while $\delta_O, \delta_{\xi_j}$ are the Dirac functions at the points $O$ and $\xi_j$ of $\mathbb H^n$, respectively.

Theorem 1.1 extends Theorem A and also Theorem 1.2 of ^[5] to the case of unbounded domains, see also ^[20,31,32]. The strategy is the same as the one in the seminal papers of Lions ^[25,26], but there are some complications due to the non Euclidean context.

The whole Heisenberg group is endowed with noncompact families of dilations and translations, which could provide a loss of compactness due to the drifting towards infinity of the mass, or – in other words – the concentration at infinity. In order to deal with this type of phenomena, we prove a variant of the concentration–compactness principle of Lions, that is the concentration–compactness principle at infinity. This variant was introduced by Bianchi, Chabrowski and Szulkin in ^[3,6] and we prove an extension of their results suitable to deal with critical Hardy equations in the Heisenberg group.

Denote by $B_R(\xi)$ the Korányi open ball of radius $R$ centered at $\xi$. For simplicity $B_R$ is the ball of radius $R$ centered at $\xi = O$.

Theorem 1.2. Let $(u_k)_k$ be a sequence in $S^{1, p}(\mathbb{H}^n)$ as in Theorem $1.1$ and define

Then,

where $\mu, \nu, \omega$ are the measures introduced in Theorem $1.1$.

In the second part of the paper, we want to extend the previous results to the fractional case. Let $0 < s < 1$ and $1 < p < \infty$. We define the fractional Sobolev space $HW^{s, p}(\mathbb H^n)$ as the completion of $C_c^\infty(\mathbb H^n)$ with respect to the norm

where

The fractional Sobolev embedding in the Heinseberg group was obtained in ^[1] following the lines of ^[9] and states as follows. If $s p < Q$, then there exists a constant $C_{ p^*_s}$ depending on $p, \, Q$ and $s$ such that

The proof of the above inequality is obtained directly, by extending the method of ^[9] to the Heisenberg context.

For notational simplicity, the fractional $(s, p)$ horizontal gradient of any function $u\in HW^{s, p}(\mathbb H^n)$ is denoted by

Note that the $(s, p)$ horizontal gradient of a function $u\in HW^{s, p}(\mathbb H^n)$ is well defined a.e. in $\mathbb H^n$ and $|D_H^{s} u|^ p\in L^1(\mathbb H^n)$ thanks to Tonelli's theorem.

From now on we fix $0 < s < 1$, $1 < p < \infty$ with $s p < Q$. Then, the following result holds true.

Theorem 1.3. Let $(u_k)_k$ be a sequence in $HW^{s, p}(\mathbb{H}^n)$ such that $u_k \rightharpoonup u$ in $HW^{s, p}(\mathbb{H}^n)$, and furthermore$|u_k|^{ p^*_s} d\xi \overset{\ast}{\rightharpoonup} \nu$, $|D_H^s u_k|^{ p}d\xi \overset{\ast}{\rightharpoonup} \mu$, in $\mathcal M(\mathbb{H}^n)$, for some appropriate$u\in HW^{1, p}(\mathbb{H}^n)$, and finite nonnegative Radon measures $\mu$, $\nu$ on $\mathbb H^n$.

Then, there exist an at most countable set $J$, a family of points $\{\xi_j\}_{j\in J}\subset\mathbb H^n$, two families of nonnegative numbers $\{\mu_j\}_{j\in J}$ and $\{\nu_j\}_{j\in J}$such that

where the constant $C_{ p^*_s}$ is defined in $(1.16)$.

In the Euclidean setting, the first extension of the $CC$ method in the fractional Sobolev spaces was obtained in ^[30] for $p = 2$ and then in ^[28] for any $p$, with $1 < p < N /s$. We also refer to ^[4,10,12] for similar results in this context and to ^[33] for the vectorial fractional Sobolev spaces.

In Theorem 1.3 we extend the previous results from the Euclidean setting to the Heisenberg environment and we also widen Theorem A from the local case to the fractional setup. To the best of our knowledge Theorem 1.3 is the first extension of the method in the fractional Sobolev space in Heisenberg group.

Actually, the strategy is the same as the one in the seminal papers of Lions ^[25,26], but there are several complications due to both the nonlocal and the subelliptic context. In order to overcome these difficulties, we employ the crucial Lemmas 4.4 and 4.5, proved using the key Lemma 4.2 and Corollary 4.3. To enter into details, the latter results give precise decay estimates and scaling properties for the fractional $(s, p)$ horizontal gradients of functions of class $C_c^\infty(\mathbb H^n)$, with respect to the intrinsic family of dilations $\delta_R$.

The paper is organized as follows. In Section 2, we recall some fundamental definitions and properties related to the Heisenberg group $\mathbb{H}^n$. Section 3 is devoted to the proof of Theorems 1.1 and 1.2, while the final Section 4 deals with the proof of Theorem 1.3, based on some preliminary lemmas.

2.   Preliminaries

2.1.   The Heisenberg group

In this section we present the basic properties of $\mathbb{H}^n$ as a Lie group. For a complete treatment, we refer to ^{[13,16,17,20,35]}. Let $\mathbb H^n$ be the Heisenberg group of topological dimension $2n+1$, that is the Lie group which has $\mathbb R^{2n+1}$ as a background manifold and whose group structure is given by the non–Abelian law

for all $\xi$, $\xi'\in \mathbb H^n$, with

The inverse is given by $\xi^{-1} = -\xi$ and so $(\xi\circ \xi')^{-1} = (\xi')^{-1}\circ \xi^{-1}$.

The real Lie algebra of $\mathbb H^n$ is generated by the left–invariant vector fields on $\mathbb H^n$

for $j = 1, \dots, n$. This basis satisfies the Heisenberg canonical commutation relations

Moreover, all the commutators of length greater than two vanish, and so $\mathbb H^n$ is a nilpotent graded stratified group of step two. A left invariant vector field $X$, which is in the span of $\{X_j, Y_j\}_{j = 1}^n$, is called horizontal.

For each real positive number $R$, the dilation $\delta_R:\mathbb{H}^n\rightarrow \mathbb{H}^n$, naturally associated with the Heisenberg group structure, is defined by

It is easy to verify that the Jacobian determinant of the dilatation $\delta_R$ is constant and equal to $R^{2n+2}$, where the natural number $Q = 2n+2$ is the homogeneous dimension of $\mathbb H^n$.

The anisotropic dilation structure on $\mathbb H^n$ introduces the Korányi norm, which is given by

Consequently, the Korányi norm is homogeneous of degree 1, with respect to the dilations $\delta _R$, $R > 0$, that is

Clearly, $\delta_R(\eta\circ \xi) = \delta_R(\eta)\circ \delta_R(\xi)$. The corresponding distance, the so called Korányi distance, is

Let $B_R(\xi_0) = \{\xi\in \mathbb H^n\, :\, d_K(\xi, \xi_0) < R\}$ be the Korányi open ball of radius $R$ centered at $\xi_0$. For simplicity we put $B_R = B_R(O)$, where $O = (0, 0)$ is the natural origin of $\mathbb{H}^n$.

The Lebesgue measure on $\mathbb R^{2n+1}$ is invariant under the left translations of the Heisenberg group. Thus, since the Haar measures on Lie groups are unique up to constant multipliers, we denote by $d\xi$ the Haar measure on $\mathbb H^n$ that coincides with the $(2n+ 1)$–Lebesgue measure and by $|U|$ the $(2n+ 1)$–dimensional Lebesgue measure of any measurable set $U \subseteq \mathbb H^n$. Furthermore, the Haar measure on $\mathbb H^n$ is $Q$–homogeneous with respect to dilations $\delta_R$. Consequently,

In particular, $|B_R(\xi_0)| = |B_1|R^Q$ for all $\xi_0\in \mathbb H^n$.

We define the horizontal gradient of a $C^1$ function $u:\mathbb{H}^n\rightarrow \mathbb{R}$ by

Clearly, $D_{H}u \in \mbox{span}\{X_j, Y_j\}_{j = 1}^n$. In $\mbox{span}\{X_j, Y_j\}_{j = 1}^n\simeq \mathbb{R}^{2n}$ we consider the natural inner product given by

for $X = \{ x^jX_j + \widetilde x^jY_j\}_{j = 1}^n$ and $Y = \{y^jX_j + \widetilde y^jY_j\}_{j = 1}^n$. The inner product $\big(\cdot, \cdot \big)_{H}$ produces the Hilbertian norm

for the horizontal vector field $X$.

For any horizontal vector field function $X = X(\xi)$, $X = \{ x^jX_j + \widetilde x^jY_j\}_{j = 1}^n$, of class $C^1(\mathbb H^n, \mathbb R^{2n})$, we define the horizontal divergence of $X$ by

Similarly, if $u\in C^2(\mathbb H^n)$, then the Kohn–Spencer Laplacian in $\mathbb H^n$, or equivalently the horizontal Laplacian, or the sub–Laplacian, of $u$ is

According to the celebrated Theorem 1.1 due to Hörmander in ^[19], the operator $\Delta_{H}$ is hypoelliptic. In particular, $\Delta_{H}u = {\rm{div}}_{H}D_{H}u$ for each $u\in C^2(\mathbb H^n)$. A well known generalization of the Kohn–Spencer Laplacian is the horizontal $p$–Laplacian on the Heisenberg group, $p\in (1, \infty)$, defined by

2.2.   Classical Sobolev spaces in the Heisenberg group

Let us now review some useful facts about the classical Sobolev spaces on the Heisenberg group $\mathbb H^n$. We just consider the special case in which $1\leq p < Q$ and $\Omega$ is an open set in $\mathbb{H}^n$. Denote by $HW^{1, p}(\Omega)$ the horizontal Sobolev space consisting of the functions $u \in L^ p(\Omega)$ such that $D_{H}u$ exists in the sense of distributions and $|D_{H}u|_{H} \in L^ p(\Omega)$, endowed with the natural norm

By ^[14] we know that if $1\leq p < Q$, then the embedding

is continuous.

Let us also briefly recall a version of the Rellich theorem in the Heisenberg group. This topic is largely treated in ^{[13,16,17,20]} for vector fields satisfying the Hörmander condition. The general Hörmander vector fields have been introduced in ^[19] and include, as a special case, the horizontal vector fields (1.2) on the Heisenberg group. For our purposes it is sufficient to recall that for any $p$, with $1\le p < Q$, and for any Korányi ball $B_R(\xi_0)$, the embedding

is compact, provided that $1\le q < p^*$. This result holds, more in general, for bounded Poincaré–Sobolev domains $\Omega$ of $\mathbb H^n$ and was first established in ^[27], even for general Hörmander vector fields. For a complete treatment on this topic we mention, e.g., ^[16,20,25].

2.3.   Fractional Sobolev spaces in the Heisenberg group

Let $s\in (0, 1)$ and $1 < p < \infty$. We endow $HW^{s, p}(\mathbb{H}^n)$, defined in the Introduction, with the norm

Our aim is to prove the compactness of the immersion $HW^{s, p}(\mathbb{H}^n) \hookrightarrow L^{p}(B_R(\xi_0))$ for all $\xi_0\in\mathbb{H}^n$ and $R > 0$. The proof relies on a Lie group version of the celebrated Frèchet–Kolmogorov Compactness Theorem, cf. Theorem A.4.1 of ^[11]. First, we need the following lemma.

Lemma 2.1. Let $0 < s < 1$, $1 < p < \infty$.Then, there exists a constant $C = C(s, p, n) > 0$ such that for any $h\in\mathbb{H}^n$, with $0 < r(h) < 1/2$,

where $\tau_h u(\xi) = u(h\circ \xi)$ for $\xi\in\mathbb H^n$.

Proof. Fix $u\in HW^{s, p}(\mathbb{H}^n)$, $h\in\mathbb{H}^n$, with $0 < r(h) < 1/2$, and $\xi\in\mathbb H^n$. Take any $\eta\in B(\xi, r(h))$. Let us first observe that $r(\eta^{-1}\circ \xi)\leq r(h)$, so that $r(\eta^{-1}\circ h \circ \xi)\leq r(\eta^{-1}\circ \xi)+ r(h)\leq 2 r(h)$ by the triangle inequality. Then,

Now, averaging in $\eta$ over $B(\xi, r(h))$, we get

with $c = c(s, p, n)$. Thus, integrating in $\xi$ over $\mathbb H^n$, we obtain

with $C = 4c$.

Theorem 2.2. Let $0 < s < 1$ and $1 < p < \infty$. Then, for every sequence $(u_k)_k$ bounded in $HW^{s, p}(\mathbb{H}^n)$ there exists $u\in HW^{s, p}(\mathbb{H}^n)$ and a subsequence $(u_{k_j})_j\subset(u_k)_k$ such thatfor all $\xi_0\in\mathbb{H}^n$ and $R > 0$

Proof. Let $M = \sup_{k\in\mathbb N} \|u_k\|_{HW^{s, p}(\mathbb{H}^n)}.$ Clearly, if $(u_k)_k$ is bounded in $HW^{s, p}(\mathbb{H}^n)$, then is also bounded in $L^p(\mathbb{H}^n)$. Moreover, by Lemma 2.1, we know that

Consequently,

Therefore, a Lie group version of the Fréchet–Kolmogorov theorem, cf. Theorem A.4.1 of ^[11], yields the existence of a function $u\in L^p(\mathbb{H}^n)$ and a subsequence of $(u_k)_k$, still denoted $(u_k)_k$, such that $u_k\to u$ a.e. in $\mathbb H^n$ and $u_k \to u$ in $L^p(B_R(\xi_0))$ for all $\xi_0\in\mathbb{H}^n$ and $R > 0$.

It remains to prove that $u\in HW^{s, p}(\mathbb{H}^n)$. This follows straightly from an application of Fatou's Lemma. Indeed,

Consequently, Fatou's Lemma, together with the lower semicontinuity of $[\, \cdot\, ]_{H, s, p}$, gives

This concludes the proof.

3.   Proof of Theorems 1.1 and 1.2

This section is devoted to the proof of Theorems 1.1 and 1.2.

Proof of Theorem $1.1$. Let $(u_k)_k$ be a sequence in $S^{1, p} (\mathbb H^n)$ as in the statement of the theorem. Obviously, (1.7), (1.8) and the first part of (1.10) follow from Theorem A, see ^[20]. Thus, there is no reason to repeat the proof here. Let us then focus on the proof of (1.9). We proceed diving the argument into two cases.

Case 1. $u = 0$. Fix $\varphi\in C_c^{\infty}(\mathbb H^n)$. Then, since clearly $\varphi u_k\in S^{1, p} (\mathbb H^n)$ for all $k$, we get by (1.6)

Now, by the subelliptic Rellich Theorem, see (2.1), we know that $u_k \to 0$ in $L^ p(B_R)$ for all $R > 0$. Therefore,

Consequently, by the weak$^*$ convergence and (3.2), letting $k\to\infty$, we obtain

Thus, by Lemma 1.4.6 of ^[20], we conclude that there exist an at most countable set $J$, a family of points $\{\xi_j\}_{j\in J}\subset\mathbb H^n$ and a family of nonnegative numbers $\{\omega_j\}_{j\in J\cup \{0\}}$, such that

Clearly, the set $J$ determined in (3.3) is not necessary the same of the one obtained in the representation of $\nu$. However, since the coefficients $\nu_j, \mu_j, \omega_j$ are allowed to be 0, we can replace these two sets with their union (which is still at most countable). For this reason we keep the same notation $J$ for the index set.

In order to conclude the proof of (1.9) on Case 1, it remains to show that $\omega$ is concentrated at $O$, namely that $\omega_j = 0$ for any $j\in J$. But this is obvious. Indeed, fix $\varphi \in C_c^\infty(\mathbb H^n)$, with $O \notin \mbox{supp}\;\varphi$, so that $\xi \mapsto |\varphi(\xi)|^{ p}\psi^ p r(\xi)^{- p}$ is in $L^\infty(\mbox{supp}\;\varphi)$. Then, since obviously $u_k \to 0$ in $L^{ p}(\mbox{supp}\;\varphi)$, we get

as $k \to \infty$. This, combined with the weak$^*$ convergence, gives $\int_{\mathbb H^n} |\varphi|^{ p}d \omega = 0$, that is $\omega$ is a measure concentrated in $O$. Hence $\omega = \omega_0 \delta_O$, and so (1.9) in proved in Case 1.

Case 2. $u\neq 0$. Set $\widetilde{u}_k = u_k-u$. Clearly, $\widetilde{u}_k\rightharpoonup 0$ in $S^{1, p} (\mathbb H^n)$ and (3.1) still holds for $\varphi\widetilde{u}_k$ for any $\varphi\in C_c^{\infty}(\mathbb H^n)$. Moreover, thanks to Case 1, there exists a finite nonnegative Radon measure $\widetilde{\omega}$ on $\mathbb H^n$, such that, up to a subsequence still labelled $(\widetilde{u}_k)_k$, we have as $k\to\infty$

where

and $\omega_0$ is an appropriate nonnegative number as shown in Case 1. Now, by (2.1), up to a subsequence,

for some $g_R\in L^ p(B_R)$ and all $R > 0$. Thus, for all $\varphi\in C_c^{\infty}(\mathbb H^n)$ an application of Brézis–Lieb lemma yields

A combination of the above formulas gives for all $\varphi\in C_c^{\infty}(\mathbb H^n)$

where $o(1)\overset{\ast}{\rightharpoonup} 0$ in $\mathcal M(\mathbb H^n).$ Then, computing the limit in (3.6), by the weak$^*$ convergence and (3.4), we get $\widetilde{\omega} = \omega - |{u}_k-u|^{ p}\psi^ p\dfrac{d\xi}{r(\xi)^ p}$. Consequently, taking into account (3.5), we obtain (1.9).

It remains to prove that $\nu_0^{ p/ p^*}\le (\mu_0-\sigma \omega_0)/ \mathcal I_{\sigma}$. Fix $\varphi\in C^\infty_c(\mathbb H^n)$ such that $0\le\varphi\le1$, $\varphi(O) = 1$ and supp $\varphi = \overline{B_1}$. Take $\varepsilon > 0$ and put $\varphi_{\varepsilon}(\xi) = \varphi(\delta_{1/\varepsilon}(\xi))$, $\xi\in\mathbb H^n$. Then,

arguing as before. Now, we know that

and

Finally, from (1.9) and the fact that $\omega \geq\omega_0\delta_O$ we get

Hence, passing to the limit as $k\to\infty$ and $\varepsilon\to0^+$ in (3.7), by (3.8)–(3.10) we obtain that

This concludes the proof.

In Theorem 1.1 we examine the behavior of weakly convergent sequences in the Folland–Stein space in situations in which the lack of compactness occurs. However, this method does not exclude a possible loss of compactness due to the drifting towards infinity of the mass, or – in other words – the concentration at infinity. Let us then turn to the proof of the concentration–compactness principle at infinity, which extend the method introduced in the Euclidean setting in ^[3,6].

Proof of Theorem $1.2$. Fix a sequence $(u_k)_k$ in $S^{1, p} (\mathbb H^n)$, as in the statement of the Theorem 1.1.

Let $\Psi\in C^\infty(\mathbb H^n)$ be such that $0\leq \Psi \leq 1$, $\Psi = 0$ in $B_1$ and $\Psi = 1$ in $B_2^c$. Take $R > 0$ and put $\Psi_{R}(\xi) = \Psi(\delta_{1/R}(\xi))$, $\xi\in\mathbb H^n$. Write

We first observe that

and so by (1.11)

On the other hand, since $\mu$ is finite, $1 - |\Psi_R|^ p$ has compact support and $\Psi_R\to0$ a.e. in $\mathbb H^n$, we have by the definition of $\mu$ and the dominated convergence theorem that

Using (3.12) and (3.13) in (3.11) we obtain the second part of (1.13). Arguing similarly for $\nu$ and $\omega$, we see that

and

Thus, (1.13)–(1.14) are proved in the same way.

In order to show the last part of (1.14), let us consider again the regular function $\Psi_R$. Then, since $0\leq \Psi_R\leq 1$, by (1.5) applied to $\Psi_R u_k \in S^{1, p} (\mathbb H^n)$, we get for all $k$

Finally, from the fact that $\lim_{R\to\infty}\limsup_{k\to\infty}\|D_H\Psi_R u_k \|_{ p}^ p = 0$, using (3.12) and (3.14) in (3.15) we obtain the desired conclusion.

4.   Proof of Theorem 1.3

This section is devoted to the proof of Theorem 1.3. Before getting there, we need some preliminary results.

Lemma 4.1. Let $\varphi\in C_c^\infty(\mathbb H^n)$, $\varepsilon > 0$ and $\xi_0\in\mathbb H^n$. Define $\mathbb H^n\ni\xi\mapsto\varphi_{\varepsilon}(\xi) = \varphi(\delta_{1/\varepsilon}(\xi_0^{-1}\circ \xi))$. Then,

Proof. Fix $\varphi\in C_c^\infty(\mathbb H^n)$, $\varepsilon > 0$ and $\xi_0\in\mathbb H^n$. The proof is a simple consequence of the change of variables formula. Indeed, if we put $\eta = \delta_{1/\varepsilon}(h)$, $d\eta = \varepsilon^{-Q} dh$, then

as required thanks to (1.17).

Note that, in general, the nonlocal $(s, p)$ horizontal gradient of a compactly supported function does not need to have compact support. For this, we use the following lemma, which gives valuable decay estimates of the fractional $(s, p)$ horizontal gradient of a $C_c^\infty(\mathbb H^n)$ function as $r(\xi)\to\infty$. The next lemma is an extension of Lemma 2.2 of ^[4] to the Heisenberg setting.

Lemma 4.2. Let $\varphi\in C_c^\infty(\mathbb H^n)$ be such that $0\leq \varphi\leq1$, ${\rm{supp}}\; \varphi\subset B_R$ for some $R > 0$.Then, there exists a constant $C = C(s, p, n)$ such that for any $\xi\in\mathbb H^n$

In particular, $|D^s_H \varphi|^ p\in L^{\infty}(\mathbb H^n)$.

Proof. Let us first prove the global $L^\infty$ bound. Consider for any $\xi\in\mathbb H^n$

and compute separately the last two integrals. By the mean value theorem and ^[14]

since $Q +s p- p < Q$. On the other hand,

being obviously $Q +s p > Q$. Now, consider $\xi \in \mathbb H^n$ with $r(\xi)\geq 2R$. Clearly, $\varphi(\xi) = 0$ and so

Now, if $r(\xi\circ h) < R$ and $r(\xi) > 2R$, then $r(\xi)-r(h)\leq r(\xi\circ h)$ so that $r(h)\geq r(\xi)-R \geq r(\xi)/2$. Therefore,

This concludes the proof of the lemma.

Combining Lemma 4.1 and Lemma 4.2, we obtain the following.

Corollary 4.3. Let $\varphi\in C_c^\infty(\mathbb H^n)$ be such that $0\leq \varphi\leq1$ and ${\rm{supp}}\; \varphi\subset B_1$. Let $\xi_0\in\mathbb H^n$ and define $\mathbb H^n\ni\xi\mapsto\varphi_{\varepsilon}(\xi) = \varphi(\delta_{1/\varepsilon}(\xi_0^{-1}\circ \xi))$. Then, there exists a constant $C = C(s, p, n)$ such that for any $\xi\in\mathbb H^n$

Using the previous estimates, we are able to prove the next result, which is an extension of Lemma 2.4 of ^[4] to the Heisenberg context.

Lemma 4.4. Let $\varphi\in C_c^\infty(\mathbb H^n)$.Then, the following embedding is compact

Proof. Let $(u_k)_k$ be a bounded sequence in $HW^{s, p }(\mathbb H^n)$, say $\sup_k\|u_k\|_{HW^{s, p }(\mathbb H^n)}\le M$, with $M > 0$. From the reflexivity of $HW^{s, p }(\mathbb H^n)$ and Theorem 2.2, there exist $u\in HW^{s, p }(\mathbb H^n)$ and a subsequence, still denoted by $(u_k)_k$, such that

Fix $R > 0$ so large that ${\rm{supp}}\; \varphi\subset B_R$. Certainly,

Now, from Lemma 4.2 and (4.1)

as $k\to\infty$. On the other hand, using (1.16) and the Hölder inequality with $q = p ^*_{s}/ p = Q/(Q-s p)$ and $q' = Q/s p$, we get by Lemma 4.2

where ${C} = 2^{ p^2}\|\varphi\|_\infty^{ p^2}M^p$. Now, for any $\tau > 0$ we can choose $R > 0$ ever larger, if necessary, so that

Finally, by (4.2) and (4.3), we obtain

for all $\tau > 0$. Sending $\tau\to0^+$ we get the desired conclusion.

The proof of the next lemma is based on the precise decay rate of $|D_H^{s} \varphi_\varepsilon|^ p$, cf. Corollary 4.3. The main difficulty here, as we already pointed out in the Introduction, is based essentially on the fact that the nonlocal $(s, p)$ horizontal gradient $|D_H^{s} \varphi_\varepsilon|^p$ does not need to have compact support. The proof uses the same strategy of Lemma 4.4, which is effective thanks to the decay estimates given in Lemma 4.1 and Corollary 4.3.

Lemma 4.5. Let $(u_k)_k$ be a bounded sequence in $HW^{s, p}(\mathbb H^n)$ and let $\varphi\in C^\infty_c(\mathbb H^n)$ besuch that $0\le\varphi\le1$, $\varphi(O) = 1$ andsupp $\varphi\subset B_1$. Take $\varepsilon > 0$, fix $\xi_0\in\mathbb H^n$ and put$\mathbb H^n\ni\xi\mapsto\varphi_{\varepsilon}(\xi) = \varphi(\delta_{1/\varepsilon}(\xi_0^{-1}\circ \xi))$. Then

Proof. Let $(u_k)_k$ be a bounded sequence in $HW^{s, p }(\mathbb H^n)$, say $\sup_k\|u_k\|_{HW^{s, p }(\mathbb H^n)} = M$. From the reflexivity of $HW^{s, p}(\mathbb H^n)$ and Theorem 2.2, there exist $u \in HW^{s, p}(\mathbb H^n)$ and a subsequence, still denoted by $(u_k)_k$, such that

for any $R > 0$ and $\xi_0\in \mathbb H^n$. Clearly,

Let us first estimate the integral over $B_\varepsilon(\xi_0)$. By Corollary 4.3 there exists $C = C(s, p, n) > 0$ such that

thanks to (4.4) and the Lebesgue theorem, being $sp < Q$.

Now we turn to the integral over $B_\varepsilon^c(\xi_0)$. Using the Hölder inequality with $q = p ^*_{s}/ p = Q/(Q-s p)$ and $q' = Q/s p$, and again Corollary 4.3, we get

Therefore, it follows that

Finally, using (4.5) and (4.6), we conclude

as required.

Lemma 4.5 extends to the Heisenberg case a remark given in the proof of Theorem 1.1 of ^[4], stated in the Euclidean framework.

Proof of Theorem $1.3$. Let $(u_k)_k$ be a sequence in $HW^{s, p}(\mathbb H^n)$, as in the statement of the theorem, and let us divide the proof into two cases.

Case 1. $u = 0$. Fix $\varphi\in C_c^{\infty}(\mathbb H^n)$. Then, an application of Lemma 4.4 immediately yields

as $k\to \infty$. Consequently, since $\varphi u_k \in HW^{s, p}(\mathbb H^n)$ for all $k$, we get

as $k\to\infty$. Therefore, passing to the limit in (4.7), by the weak$^*$ convergence we have the following reverse Hölder inequality

Thus, by Lemma 1.4.6 of ^[20], we conclude that there exist an at most countable set $J$, a family of points $\{\xi_j\}_{j\in J}\subset\mathbb H^n$ and a family of nonnegative numbers $\{\nu_j\}_{j\in J}$ such that

Case 2. $u \neq 0$. Set $\widetilde{u}_k = u_k-u$. Clearly, $\widetilde{u}_k\rightharpoonup 0$ in $HW^{s, p}(\mathbb H^n)$ and (4.7) still holds for $\varphi\widetilde{u}_k$ for any $\varphi\in C_c^{\infty}(\mathbb H^n)$. Moreover, $k\mapsto |\widetilde{u}_k|^{ p^*_s} d\xi$ and $k\mapsto|D^s_H \widetilde{u}_k|^{ p}d\xi$ are still bounded sequences of measures and so by Proposition 1.202 of ^[15], we can conclude that there exist two bounded nonnegative Radon measure $\widetilde{\nu}$ and $\widetilde{\mu}$ on $\mathbb H^n$, such that, up to a subsequence, we have

Thus, from Case 1 there exist an at most countable set $J$, a family of points $\{\xi_j\}_{j\in J}\subset\mathbb H^n$ and a family of nonnegative numbers $\{\nu_j\}_{j\in J}$ such that $\widetilde{\nu} = \sum_{j\in J} \nu_j\delta_{\xi_j}.$ Consequently, the claimed representation (1.7) of $\nu$ follows exactly as in Theorem 1.1.

Let us now prove the first part of (1.10). Fix a test function $\varphi\in C^\infty_c(\mathbb H^n)$, such that $0\le\varphi\le1$, $\varphi(O) = 1$ and supp $\varphi\subset B_1$. Take $\varepsilon > 0$ and put $\varphi_{\varepsilon, j}(\xi) = \varphi(\delta_{1/\varepsilon}(\xi_j^{-1}\circ \xi))$, $\xi\in\mathbb H^n$, for any fixed $j\in J$, where $\{\xi_j\}_j$ is introduced in (1.7). Fix $j\in J$ and $\tau > 0$. Then, there exists $C_\tau > 0$ such that, by (1.16) applied to $\varphi_{\varepsilon, j}u_k$, we have

We aim to pass to the limit in (4.10) as $k\to\infty$ and $\varepsilon\to0^+$. To do this, let us observe first that from the weak$^*$ convergence and (1.7) we get

since

as $\varepsilon\to 0^+$, being $0\leq\varphi\leq 1$. On the other hand, the weak$^*$ convergence gives

while Lemma 4.5 yields

Then, combining (4.11)–(4.13) and letting $\varepsilon\to 0^+$ in (4.10), we find that

where $\mu_j = \lim_{\varepsilon\to 0^+}\mu(B_\varepsilon(\xi_j))$. Since $\tau > 0$ is arbitrary, sending $\tau\to0^+$, we finally obtain

Obviously,

Denote by $\mathcal B_\varepsilon(\xi_0)$ the Euclidean ball of $\mathbb{R}^{2n+1}$ of center $\xi_0\in\mathbb H^n$ and radius $\varepsilon$. By Lebesgue's differentiation theorem for measures (see for example ^[15]), in order to prove that $\mu\ge |D_H^s u|^ p d\xi$ it suffices to show that

where $|\mathcal B_\varepsilon(\xi_0)|$ is the Lebesgue measure of the Euclidean ball $\mathcal B_\varepsilon(\xi_0)$.

Clearly, since $|D_H^s u|^ p d\xi \in L^{1}_{\rm{loc}}(\mathbb H^n)$, we know that for a.e. $\xi_0\in\mathbb H^n$

Fix $\varepsilon > 0$ and $\xi_0\in\mathbb H^n$ such that (4.15) holds. Now, the functional $\Phi: HW^{s, p}(\mathbb H^n)\rightarrow \mathbb{R}$, defined as

is convex and strongly continuous on $HW^{s, p}(\mathbb H^n)$. Thus, since $u_k\rightharpoonup u$ in $HW^{s, p}(\mathbb H^n)$, we have

Therefore, an application of Proposition 1.203 – Part $(ii)$ of ^[15] gives

Now, passing to the liminf as $\varepsilon \to0^+$ and using (4.15), we obtain (4.14).

Finally, since $|D^s_H u|^ p d\xi$ is orthogonal to $\sum_{j\in J}\mu_j\delta_{\xi_j}$, we get the desired conclusion. This concludes the proof.

Acknowledgments

The authors are members of the Gruppo Nazionale per l'Analisi Matematica, la Probabilità e le loro Applicazioni (GNAMPA) of the Istituto Nazionale di Alta Matematica (INdAM). P. Pucci was partly supported by the INdAM – GNAMPA Project Equazioni alle derivate parziali: problemi e modelli (Prot_U-UFMBAZ-2020-000761) and also by the Fondo Ricerca di Base di Ateneo – Esercizio 2017–2019 of the University of Perugia, named PDEs and Nonlinear Analysis.

Conflict of interest

All authors declare no conflicts of interest in this paper.