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Fractional Fefferman–Stein inequalities on infinite rooted kk-ary trees

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Abstract

We study weighted endpoint estimates for the centered fractional maximal operator on the infinite rooted kk-ary tree, TT. Our first result is a Fefferman–Stein type estimate w({Mαf>λ})≲α,s1λ∑x∈T∣f(x)∣Mα,sw(x),s>1, w\bigl(\{M_αf>λ\}\bigr) \lesssim_{α,s} \frac1λ\sum_{x\in T}|f(x)|M_{α,s}w(x), \qquad s>1, with a constant independent of the branching parameter kk. Although the proof is inspired by the non-fractional argument of Ombrosi, Rivera-Ríos and Safe in \cite{ORRS}, the fractional normalization introduces a genuinely new scale interaction. At radius rr, one must renormalize the function by krαk^{rα} while keeping the dyadic cutoff at krk^r; this leads to a new summation mechanism involving simultaneously krαk^{rα} and kr(1−α)k^{r(1-α)}. We then study sharpness and the geometry of admissible weights. We construct counterexamples showing that the estimate cannot in general be reduced to s=1s=1 for any 0<α<10<α<1. In the subcritical range 0<α<1/20<α<1/2, we characterize power-type radial weights satisfying the natural fractional A1A_1 condition and prove that the failure persists after any fixed finite number of iterations of MαM_α. We also prove that Mαw≲wM_αw\lesssim w is necessary for the corresponding weighted weak type estimate but is not sufficient in the subcritical range. Finally, we identify a phase transition: for 1/2≤α<11/2\leα<1 no nonzero global weight can satisfy Mαw≲wM_αw\lesssim w.

Introduction and main results

Let k≥2k\geq2 be an integer. We consider TT the infinite rooted kk-ary tree, that is, a graph with an initial vertex x0x_0, called root, and each vertex has kk children.

Throughout the paper, we denote A≲θBA\lesssim_\theta B to mean that there exists a positive constant cθc_\theta depending only on θ\theta such that A≤cθBA\leq c_\theta B. We say that A≃θBA\simeq_\theta B when A≲θBA\lesssim_\theta B and B≲θAB\lesssim_\theta A.

It is possible to equip TT, with the graph distance dd and the counting measure μ\mu. The distance d(x,y)d(x,y) is the number of edges of the unique path between xx and yy and the measure μ\mu counts the number of vertices in the set. If A⊂TA\subset T, we denote ∣A∣=μ(A)|A|=\mu(A) and

f(A)=∫Af(x) dx=∑x∈Af(x).f(A)=\int_A f(x)\,dx=\sum_{x\in A}f(x).

All radii are nonnegative integers. By a weight we mean a function w:T→[0,∞)w:T\to[0,\infty) which is finite at every vertex; it may vanish on a subset of TT. We write w(E)=∑x∈Ew(x)w(E)=\sum_{x\in E}w(x).

Let S(x,r)S(x,r) denote the sphere of radius rr, S(x,r)={y∈T:d(x,y)=r}S(x,r)=\{y\in T:d(x,y)=r\}, observe that S(x,r)S(x,r) has exponential growth,

∣S(x,r)∣≃kr,|S(x,r)|\simeq k^r,

and μ\mu is not a doubling measure. This geometry makes TT a natural model in which classical covering arguments are unavailable but sharp maximal estimates can still be obtained by exploiting combinatorial expansion.

The study of classical operators in the context of kk-tree has recently received considerable attention, particularly through the works of Naor and Tao [7] and Ombrosi, Rivera-Ríos and Safe [9]. We also refer to the articles [12, 13] in which the authors studied connections between the geometrical properties of finite and infinite graphs and the boundedness of the Hardy-Littlewood maximal operator. For weighted estimates on trees, we refer to [4, 5, 8, 15].

In [7], Naor and Tao proved the unweighted weak type (1,1)(1,1) for the Hardy-Littlewood maximal operator in the kk-tree TT,

∣{x∈T:Mf(x)>λ}∣≤cλ∑x∈T∣f(x)∣\left|\{x \in T : Mf(x) > \lambda\}\right| \leq\frac{c}{\lambda}\sum_{x\in T}|f(x)|

where MM is defined by

Mf(x)=sup⁡r≥01∣B(x,r)∣∑y∈B(x,r)∣f(y)∣.Mf(x)=\sup_{r\geq0}\frac{1}{|B(x,r)|}\sum_{y\in B(x,r)}|f(y)|.

Recently, in [9] Ombrosi, Rivera-Ríos and Safe proved a weighted Fefferman–Stein inequality for the Hardy–Littlewood maximal operator on TT of the form

w({Mf>λ})≲1λ∑x∈T∣f(x)∣Msw(x),s>1,w(\{Mf>\lambda\})\lesssim\frac{1}{\lambda}\sum_{x\in T}|f(x)|M_sw(x), \qquad s>1,

where Ms(w)=M(w1/s)M_s(w)=M(w^{1/s}). The authors showed that not only it is not possible to choose s=1s=1 but also it is not even possible to choose any number of iterations of the maximal function for the inequality to hold. Their proof combines a weighted incidence estimate on spheres with a dyadic decomposition whose crucial gain is a positive power of 2n/kr2^n/k^r.

The Fefferman-Stein estimate was originally proved in [3], later these estimates and related variants have been studied in a variety of contexts [1, 6, 10, 11, 14]. In the fractional setting, the Fefferman-Stein for the fractional maximal operator is a consequence of classical covering lemmas [3]. In [2], the authors proved that the Fefferman-Stein estimate for the fractional integral holds with a fractional Llog⁡LL\log L-maximal operator and cannot be replaced with the fractional maximal operator.

The purpose of the present paper is to develop the corresponding theory for the fractional maximal operator with 0<α<10<\alpha<1,

Mαf(x)=sup⁡r≥01∣B(x,r)∣1−α∑y∈B(x,r)∣f(y)∣,M_\alpha f(x)=\sup_{r\geq0}\frac{1}{|B(x,r)|^{1-\alpha}}\sum_{y\in B(x,r)}|f(y)|,

and its spherical counterpart

Mα∘f(x)=sup⁡r≥01∣S(x,r)∣1−α∑y∈S(x,r)∣f(y)∣.M_\alpha^\circ f(x)=\sup_{r\geq0}\frac{1}{|S(x,r)|^{1-\alpha}}\sum_{y\in S(x,r)}|f(y)|.

Note that, in contrast to the standard Euclidean setting, here it makes sense to consider this kind of maximal function because S(x,r)S(x,r) are not sets of measure 0. For k≥2k\geq2, we have Mα≃αMα∘M_\alpha\simeq_\alpha M_\alpha^\circ as we will show in Proposition 2.1.

The fractional problem is not obtained by a formal substitution in the proof of [9]. The factor ∣S(x,r)∣α≃krα|S(x,r)|^\alpha\simeq k^{r\alpha} changes in a substantial form the distributional decomposition and the final summation.

We consider the fractional LsL^s maximal operator

Mα,sw(x)=sup⁡r≥0∣B(x,r)∣α(1∣B(x,r)∣∑y∈B(x,r)w(y)s)1/s.M_{\alpha,s}w(x)=\sup_{r\geq0}|B(x,r)|^\alpha\left(\frac{1}{|B(x,r)|}\sum_{y\in B(x,r)}w(y)^s\right)^{1/s}.

The first result gives a weighted endpoint estimate that survives fractional normalization in a space with exponential volume growth. The following theorem provides a Fefferman-Stein estimate with Mα,swM_{\alpha,s}w in the right-side.

Theorem 1.1. Let k>2k>2, 0<α<10<\alpha<1 and s>1s>1. Then, for every weight w≥0w\geq0 on TT,

w({x∈T:Mαf(x)>λ})≤Cα,s1λ∑x∈T∣f(x)∣Mα,sw(x),(1)w(\{x\in T:M_\alpha f(x)>\lambda\})\leq C_{\alpha,s}\frac{1}{\lambda}\sum_{x\in T}|f(x)|M_{\alpha,s}w(x), \tag*{(1)}

where Cα,sC_{\alpha,s} is independent of kk. The constant obtained in the proof deteriorates as s↓1s\downarrow1.

Theorem 1.1 is proved in § 2. The weighted sphere-incidence lemma, Lemma 2.3, is a fractional variant of the combinatorial estimate in [9], but its power of kk changes from the non-fractional one.

A central issue is whether the assumption s>1s>1 in Theorem 1.1 is genuinely necessary. The following counterexample therefore plays a decisive role: in the subcritical range 0<α<1/20<\alpha<1/2, it shows that the estimate fails not only for s=1s=1, but even when MαM_\alpha is replaced by any fixed finite iterate. This establishes the necessity of the modification introduced in Theorem 1.1 and identifies a fundamental obstruction in the fractional setting.

Theorem 1.2. For any n∈Nn\in\mathbb{N} and 0<α<1/20<\alpha<1/2, there exists a weight ww such that Mαw≲wM_\alpha w\lesssim w and a sequence of finitely supported functions {fj}\{f_j\} such that

w({Mαfj>1})∑x∈T∣fj(x)∣Mα(n)w(x)→j→∞∞.\frac{w(\{M_\alpha f_j>1\})}{\sum_{x\in T}|f_j(x)|M_\alpha^{(n)}w(x)}\xrightarrow[j\to\infty]{}\infty.

Consequently, no estimate of the form

w({Mαf>λ})≤Cλ∑x∈T∣f(x)∣Mα(n)w(x)w(\{M_\alpha f>\lambda\})\leq\frac{C}{\lambda}\sum_{x\in T}|f(x)|M_\alpha^{(n)}w(x)

can hold uniformly for all finitely supported ff and all λ>0\lambda>0.

Although Theorem 1.2 is the fractional counterpart of the result of [9], the construction of the counterexample requires a different approach. In their example, the weight is chosen to compensate the average of the ball. In the fractional setting, however, this normalization becomes ∣B(x,r)∣1−α|B(x,r)|^{1-\alpha}, and the natural adaptations of their weight no longer yield the balance needed to produce a counterexample. Thus, the non-fractional construction does not extend directly to our setting. Overcoming this difficulty requires a more delicate example, based on a suitably chosen subtree whose geometry compensates for the fractional normalization.

We next obtain a necessary condition for the weighted weak-type (1,1)(1,1) estimate. Testing this estimate on point masses recovers the condition Mαw≲wM_\alpha w\lesssim w. The preceding counterexample shows that this condition is not sufficient in the subcritical range.

Theorem 1.3. Let 0<α<10<\alpha<1 and let ww be a weight on TT. Assume that there exists Cw>0C_w>0 such that

w({x∈T:Mαf(x)>λ})≤Cwλ∑x∈T∣f(x)∣w(x)(2)w(\{x\in T:M_\alpha f(x)>\lambda\})\leq\frac{C_w}{\lambda}\sum_{x\in T}|f(x)|w(x) \tag*{(2)}

for every finitely supported ff and every λ>0\lambda>0. Then

Mαw(x)≲α,k,Cww(x),x∈T.M_\alpha w(x)\lesssim_{\alpha,k,C_w}w(x),\qquad x\in T.

Consequently, for 0<α<1/20<\alpha<1/2 this condition is necessary but not sufficient. If 1/2≤α<11/2\leq\alpha<1, no nonzero weight can satisfy Mαw≲wM_\alpha w\lesssim w, and hence no nontrivial weighted weak type estimate of the above form is possible; see Proposition 3.11.

At the critical value α=1/2\alpha=1/2, the exponential rates used in the supercritical argument coincide. The radial computation below nevertheless provides an additional factor depending on the generation, which rules out global weights also at the endpoint, without any radiality assumption.

We present the power-type radial weights of the form

wβ(x)=kβ∣x∣,w_\beta(x)=k^{\beta|x|},

where ∣x∣|x| is the generation of xx and β∈R\beta\in\mathbb{R}.

These weights allow us to compare the necessary condition with the sufficient condition involving Mα,sM_{\alpha,s}. Contributions from descendants and from paths passing through ancestors impose two restrictions on β\beta. Their balance determines the admissible interval and explains the threshold α=1/2\alpha=1/2.

Theorem 1.4. If 0<α<1/20<\alpha<1/2, then

Mαwβ≈wβ⟺β∈[α−1,−α].M_\alpha w_\beta\approx w_\beta\qquad\Longleftrightarrow\qquad\beta\in[\alpha-1,-\alpha].

If 1/2≤α<11/2 \le\alpha< 1, no power-type radial weight satisfies this estimate globally. Moreover, for s>1s > 1,

Mα,swβ≃wβM_{\alpha,s}w_\beta\simeq w_\beta

holds precisely in the range

References

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