Radon Measures and Lipschitz Graphs

RADON MEASURES AND LIPSCHITZ GRAPHS

MATTHEW BADGER AND LISA NAPLES

Abstract. For all 1 ≤ m ≤ n − 1, we investigate the interaction of locally finite measures in Rn with the family of m-dimensional Lipschitz graphs. For instance, we characterize Radon measures µ, which are carried by Lipschitz graphs in the sense that n S∞ there exist graphs Γ1, Γ2,... such that µ(R \ 1 Γi) = 0, using only countably many evaluations of the measure. This problem in geometric measure theory was classically studied within smaller classes of measures, e.g. for the restrictions of m-dimensional Hausdorff measure Hm to E ⊆ Rn with 0 < Hm(E) < ∞. However, an example of Csörnyei, Käenmäki,Rajala, and Suomala shows that classical methods are insufficient to detect when a general measure charges a Lipschitz graph. To develop a characterization of Lipschitz graph rectifiability for arbitrary Radon measures, we look at the behavior of coarse doubling ratios of the measure on dyadic cubes that intersect conical annuli. This extends a characterization of graph rectifiability for pointwise doubling measures by Naples by mimicking the approach used in the characterization of Radon measures carried by rectifiable curves by Badger and Schul.

Contents 1. Introduction 1 2. Suﬃcient Conditions 7 3. Necessary Conditions 11 4. Proof of the Main Theorem 13 5. Variations 14 References 15

1. Introduction A general goal in geometric measure theory that has not yet been fully achieved is to understand in a systematic way how generic measures on a metric space interact with a prescribed family of sets in the space, e.g. rectiﬁable curves, smooth submanifolds, etc. For instance, we could ask: Is a measure positive on some set in the family? Do there exist countably many sets in the family whose union captures all of the mass of the measure? For Hausdorﬀ measures and measures with a priori bounds on the asymptotic densities

Date: December 16, 2020. 2010 Mathematics Subject Classification. Primary 28A75. Key words and phrases. Radon measure, Lipschitz graph, rectifiability, doubling, cone approximation. The authors were partially supported by NSF DMS grant 1650546. 1 2 MATTHEW BADGER AND LISA NAPLES of the measure, much progress has been made. A description of this work as it stood at the end of the last century can be found can be found in [Mat95]. Newer developments in the theory of rectifiability of absolutely continuous measures include [AT15, Tol15, TT15, ENV17, Ghi20, Goe19, Dab19, Dab20b]. An alternative regularity condition that is usually a priori weaker than upper and lower density bounds is asymptotic control on how much the measure grows when the radius of a ball is doubled. Recent investigations on the rectifiability of doubling measures include [ADT16, ADT17, ATT20, Nap20]. For Radon measures, which in general do not possess good bounds on density or doubling, the situation is far less understood and examples show that classical geometric measure theory methods are not strong enough to detect when measures charge Lipschitz images of Euclidean subspaces or graphs of Lipschitz functions [MM88], [CKRS10], [GKS10], [MO18], [Tol19]. On the positive side, we now possess a complete description of the interaction of an arbitrary Radon measure in Euclidean space with rectifiable curves [BS17]. This advance required a thorough understanding of the geometry of subsets of rectifiable curves in Hilbert spaces [Jon90, Oki92, Sch07] and further blending geometric measure theory with techniques from modern harmonic analysis. For a longer overview of these and other related developments on generalized rectifiability of measures, including fractional and higher-order rectifiability, see the survey [Bad19]. In this paper, we obtain a complete description of the interaction of Radon measures in Rn with graphs of Lipschitz functions over m-dimensional subspaces for all 1 ≤ m ≤ n−1. Moreover, the characterization of Lipschitz graph rectifiability that we identify depends only on the value of the measure on dyadic cubes below a fixed generation. The key insight is that to construct Lipschitz graphs that charge a measure, one must be able to equitably distribute mass which appears in bad cones. For a detailed statement, see Theorem 1.5 and the definition of cone defect. The connection between Lipschitz graphs and the geometry of measures have been studied for over ninety years, appearing in foundational work on the structure of Hausdorff measures in the plane [Bes28, Bes38, MR44] and higher- dimensional Euclidean space [Fed47]. Radon measures on smooth Lipschitz graphs supply a model for generalized surfaces in connection with Plateau’s problem [Alm69, Dav14]. Beyond the domain of geometric measure theory, understanding rectifiability of measures with respect to Lipschitz graphs is crucial in the study of boundedness of singular integral operators [CMM82, DS91, DS93, NTV14] and absolute continuity of harmonic measure on rough domains [DJ90, Bad12, AHM+16, AAM19].

Cones and Lipschitz Graph Rectiﬁability. Throughout the paper, we ﬁx integer dimensions 1 ≤ m ≤ n − 1, where n denotes the dimension of ambient space and m denotes the dimension of a Lipschitz graph. A bad cone X = X(V, α) is a set of the form

n ⊥ X = {x ∈ R : dist(x, V ) > α dist(x, V )}, where V ∈ G(n, m) is any m-dimensional subspace of Rn, V ⊥ ∈ G(n, n − m) denotes its orthogonal complement, and α ∈ (0, ∞). In other words, X is the set of points which are relatively closer to V ⊥ than V . We exclude the degenerate case α = 0, which corresponds RADON MEASURES AND LIPSCHITZ GRAPHS 3

n n to X = R \ V . For every x ∈ R and bad cone X, we let Xx = x + X = {x + y : y ∈ X} denote the translate of X with center x. The importance of this family of cones is that they yield a perfect test to determine when a set is contained in a Lipschitz graph.

Lemma 1.1 (Geometric Lemma). Let V ∈ G(n, m), α ∈ (0, ∞), X = X(V, α), and E ⊆ Rn be nonempty. There exists a Lipschitz function f : V → V ⊥ with Lipschitz constant at most α such that E is contained in

⊥ n Graph(f) = {(x, f(x)) : x ∈ V } ⊆ V × V = R if and only if E ∩ Xx = ∅ for all x ∈ E. The conclusion also holds when α = 0.

Proof. Unwind the definitions or see e.g. the proof in [DL08, Lemma 4.7]. We adopt the convention that a Radon measure µ on Rn is a Borel regular outer measure that is finite on compact sets. At one extreme, given a nonempty family F of Borel sets, n S∞ we say that µ is carried by F if there exist F1,F2, · · · ∈ F such that µ(R \ 1 Fi) = 0. At the other extreme, we say that µ is singular to F provided µ(F ) = 0 for every F ∈ F. For any Radon measure µ and Borel set E ⊆ Rn, the restriction µ E defined by the rule µ E(A) = µ(E ∩ A) for all sets A ⊆ Rn is again a Radon measure. The support spt µ of a Radon measure is the smallest closed set such that µ(Rn \ spt µ) = 0. A Radon measure µ on Rn is Lipschitz graph rectifiable of dimension m if µ is carried by m-dimensional Lipschitz graphs, i.e. graphs of Lipschitz functions f : V → V ⊥ over subspaces V ∈ G(n, m). For example, let Γ1, Γ2,... be a sequence of Lipschitz graphs in n m R with uniformly bounded Lipschitz constants, let µi = H Γi denote the restriction of m the m-dimensional Hausdorff measure H to Γi, and let c1, c2, · · · ∈ (0, ∞) be a sequence P∞ P∞ of weights with 1 ci < ∞. Then µ = 1 ciµi is an m-dimensional Lipschitz graph n S∞ rectifiable Radon measure on R with support equal to 1 Γi. In particular, there exist Lipschitz graph rectifiable measures with spt µ = Rn. The following classical criterion for Lipschitz graph rectifiability is due to Federer [Fed47, Theorem 4.7]. The theorem only applies to Radon measures satisfying the upper −m density bounds 0 < lim supr↓0 r µ(B(x, r)) < ∞ µ-a.e. Such measures are strongly m-dimensional in the sense that µ is carried by sets of finite Hausdorff measure Hm and singular to sets of zero Hm measure; e.g. this can be shown using [Mat95, Theorem 6.9].

Theorem 1.2 (Federer). Let µ be a Radon measure on Rn. If for µ-a.e. x ∈ Rn, there exists a bad cone X = X(Vx, αx) such that m µ(Xx ∩ B(x, r)) αx µ(B(x, r)) (1.1) lim sup m < m lim sup m < ∞, r↓0 r 2 · 100 r↓0 r then µ is carried by m-dimensional Lipschitz graphs.

For general locally ﬁnite measures, there is no uniform comparison between the measure of a ball and the radius of the ball. Thus, it is natural to try to replace the normalizing factor rm in Federer’s condition (1.1) with µ(B(x, r)). In this direction, Naples obtained 4 MATTHEW BADGER AND LISA NAPLES a characterization of Lipschitz graph rectiﬁability for measures in Hilbert space with pointwise bounded asymptotic doubling. See [Nap20, Theorem D].

Theorem 1.3 (Naples). Let µ be a Radon measure on Rn or a locally finite Borel regular outer measure on the Hilbert space `2. Assume that µ is pointwise doubling, i.e. µ(B(x, 2r)) lim sup < ∞ at µ-a.e. x. r↓0 µ(B(x, r)) Then µ is carried by m-dimensional Lipschitz graphs if and only if for µ-a.e. x there exists a bad cone X = X(Vx, αx) such that µ(X ∩ B(x, r)) (1.2) lim x = 0. r↓0 µ(B(x, r)) The restriction to pointwise doubling measures in Theorem 1.3 is crucial. For general Radon measures in Euclidean space, which may be non-doubling, it is impossible to characterize Lipschitz graph rectifiability using condition (1.2) by an example of Csörnyei, Käenmäki,Rajala, and Suomala. See [CKRS10, Example 5.5].

Theorem 1.4 (Cs¨ornyei et al.). There exists a non-zero Radon measure µ on R2 and V ∈ G(2, 1) such that for all α > 0, condition (1.2) holds for µ and X = X(V, α) at µ-a.e. x ∈ R2, and µ is singular to 1-dimensional Lipschitz graphs. In a recent preprint [Dab20a], Dabrowski independently announced a characterization of m-dimensional Lipschitz graph rectiﬁable measures, which are absolutely continuous with respect to Hm. The characterization is in terms of a Dini condition on conical densities of the form r−mµ(X ∩B(x, r)) and requires certain a priori bounds on the lower and upper m-dimensional density on µ; for related examples, see [Dab20c]. In [DNOI19], Del Nin and Obinna Idu supply an extension of Theorem 1.2 to C1,α graphs.

Conical Defect. Our goal is to promote the characterization of subsets of Lipschitz graphs given by the geometric lemma to a characterization of Radon measures carried by Lipschitz graphs. Motivated by the characterization of Radon measures carried by rectiﬁable curves [BS17], we follow [Bad19, Remark 2.10] and design an anisotropic version n S of the geometric lemma for measures. For any nonempty set Q ⊆ R , let XQ = x∈Q Xx denote the union of bad cones centered on Q. In particular, suppose that Q is a (half-open) dyadic cube, i.e. a set of the form j j + 1 j j + 1 Q = 1 , 1 × · · · × n , n , k, j , . . . , j ∈ . 2k 2k 2k 2k 1 n Z

−k We denote the side length 2 of Q by side Q. Let xQ denote the geometric center of Q. For each X = X(V, α) with α ∈ (0, ∞), let rQ,X > 0 be suﬃciently large such that if R is a dyadic cube of the same generation as Q and R intersects the conical annulus AQ,X ,

AQ,X = XQ ∩ B(xQ, rQ,X ) \ U(xQ, rQ,X /3), RADON MEASURES AND LIPSCHITZ GRAPHS 5

Figure 1. A conical annulus AQ,X(V,α) (on the left) and its discretization ∗ ◦ ◦ ∆Q,X(V,α) (on the right), where V = span~v, ~v = (cos(150 ), sin(150 )), and α = 1.

c then R∩B(xQ, rQ,X /4) = ∅ and gap(R,Xx(V, α/2) ) ≥ diam Q for all x ∈ Q. Here B(x, r) and U(x, r) denote the closed and open balls centered at x with radius r, respectively, diam Q denotes the diameter of Q, Sc = Rn \ S for every set S ⊆ Rn, and gap(S,T ) = inf{|s − t| : s ∈ S, t ∈ T } for all nonempty sets S,T ⊆ Rn. (In harmonic analysis, gap(S,T ) is often denoted by dist(S,T ), but because the gap between sets fails the triangle inequality, we believe it should not be called a distance; our terminology comes from variational analysis, see e.g. [Bee93].) By Lemma 2.1 below, we may choose √ rQ,X = 81 n max(α, 1/α) side Q. ∗ ∗ Define the discretized conical annulus ∆Q,X to be the set of all such R, i.e. R ∈ ∆Q,X if and only if R is a dyadic cube, side R = side Q, and R has nonempty intersection with AQ,X . S ∗ Of course, the discretized conical annulus covers the conical annulus, i.e. AQ,X ⊆ ∆Q,X . ∗ In addition, define the dual discretized conical annulus ∇R,X by setting ∗ ∗ Q ∈ ∇R,X if and only if R ∈ ∆Q,X . ∗ ∗ 1 ∗ (In fact, it can be shown that ∇R,X and ∆R,X are the same set of dyadic cubes , but ∇R,X ∗ and ∆R,X play different logical roles in the proofs below, so we use separate notation.) ∗ ∗ Note that each discretized region ∆Q,X and ∇R,X is a finite family of cubes with cardinality controlled by n and α. For every Radon measure µ on Rn, dyadic cube Q with µ(Q) > 0, and bad cone X = X(V, α) with α ∈ (0, ∞), we define the conical defect to be the quantity X µ(R) Defect(µ, Q, X) = ∈ [0, ∞). ∗ µ(Q) R∈∆Q,X We also set Defect(µ, Q, X) = 0 if µ(Q) = 0. The conical defect is a weighted measurement S ∗ of the mass of µ in the annular region ∆Q,X ⊇ AQ,X . It is anisotropic insofar as the

1We thank an anonymous referee for this observation. 6 MATTHEW BADGER AND LISA NAPLES normalization of each term µ(R) that appears in the defect depends on the value of the ∗ measure in cubes Q ∈ ∇R,X emanating in different directions from the cube R. Conical Dini Functions. For every Radon measure µ on Rn and bad cone X = X(V, α) n with α ∈ (0, ∞), we define the conical Dini function Gµ,X : R → [0, ∞], X n Gµ,X (x) = Defect(µ, Q, X) χQ(x) for all x ∈ R , side Q≤1 where the sum ranges over all dyadic cubes Q of side length at most 1 that contain x. The definition of Gµ,X (x) is similar in spirit to the definition of the density-normalized square functions in [BS15, BS16, BS17]. The magnitude of the conical Dini function determines the interaction of µ with m-dimensional Lipschitz graphs. There are several possible ways to formulate this. Perhaps the most important is the following. Theorem 1.5 (Main Theorem). Let 1 ≤ m ≤ n − 1 be integers. Every Radon measure n ⊥ µ on R decomposes uniquely as µ = µG + µG, where µG is a Radon measure carried by ⊥ m-dimensional Lipschitz graphs and µG is a Radon measure singular to m-dimensional Lipschitz graphs. The component measures are identified by n µG = µ {x ∈ R : Gµ,X (x) < ∞ for some bad cone X}, ⊥ n µG = µ {x ∈ R : Gµ,X (x) = ∞ for every bad cone X}.

That is, there exists a sequence Γ1, Γ2,... of m-dimensional Lipschitz graphs such that n S∞ ⊥ µG(R \ 1 Γi) = 0 and µG(Γ) = 0 for every m-dimensional Lipschitz graph Γ. The main theorem implies that to determine whether or not a measure charges some Lipschitz graph or is carried by Lipschitz graphs it is enough to evaluate the measure on only countably many sets, e.g. on dyadic cubes of side length at most 1. Consequences. The ﬁrst two corollaries are immediate applications of the main theorem. For variations on Corollary 1.6 and 1.7, which account for the direction V and Lipschitz constant α of the underlying Lipschitz graphs, see §§ 2 and 3.

Corollary 1.6. A Radon measure µ on Rn is carried by m-dimensional Lipschitz graphs n if and only if Gµ,X (x) < ∞ for some bad cone X = X(Vx, αx) for µ-a.e. x ∈ R . Corollary 1.7. A Radon measure µ on Rn charges some m-dimensional Lipschitz graph, i.e. µ(Γ) > 0 for some Lipschitz graph Γ, if and only if there exists E ⊆ Rn with µ(E) > 0 such that Gµ,X (x) < ∞ for some bad cone X = X(Vx, αx) for each x ∈ E. A basic geometric measure-theoretic fact is that every m-dimensional Lipschitz graph in Rn has locally ﬁnite m-dimensional packing measure. Further, typical points of sets of ﬁnite s-dimensional packing measure have positive lower s-dimensional density. Hence we discover the following relationship between the conical Dini functions for µ and the lower m-dimensional density for µ. For details, see e.g. [BS15, Lemma 2.7, 2.8].

Corollary 1.8. Let µ be a Radon measure on Rn. RADON MEASURES AND LIPSCHITZ GRAPHS 7

n (1) At µ-a.e. x ∈ R such that Gµ,X (x) < ∞ for some bad cone X, we have µ(B(x, r)) Dm(µ, x) = lim inf > 0. r↓0 rm n m (2) At µ-a.e. x ∈ R such that D (µ, x) = 0, we have Gµ,X (x) = ∞ for every bad cone X. It is a difficult, open problem to obtain similar theorems for Radon measures and Lipschitz images of Rm in Rn when 2 ≤ m ≤ n − 1. (However, the case when µ vanishes on sets of zero m-dimensional Hausdorff measure is well understood, see e.g. [Mat95].) The obstacle is back at the beginning of the paper: there is no known substitute for Lemma 1.1 that characterizes subsets of Lipschitz images. Even the case m = 2, n = 3 is wide open. For related work on subsets of alternative classes of higher-dimensional curves and surfaces, see [AS18, BNV19, ENV19, Hyd20] and the references therein. Organization. We establish sufficient conditions for Lipschitz graph rectifiability in §2, followed by necessary conditions in §3. Using these results, we prove Theorem 1.5 in §4. Finally, we discuss variations on the main theorem in §5.

2. Sufficient Conditions We adopt the following standard notation. We write C = C(p, q, . . . ) to denote that 0 < C < ∞ is a constant depending on at most the parameters p, q, . . . . The value of C may change from line to line. The notation a .p,q,... b is short hand for a ≤ C(p, q, . . . ) b. Lemma 2.1. Let X = X(V, α) be a bad cone over V ∈ G(n, m) with opening α ∈ (0, ∞). In the definition of the conical defect, we may choose the radius √ rQ,X = 81 n max(α, 1/α) side Q. For every dyadic cube Q and for every x ∈ Q, √ 1 Xx ∩ B(x, sQ,X ) \ U x, 2 sQ,X ⊆ AQ,X , where sQ,X = rQ,X − n side Q. ∗ There exists a constant C1 = C1(n, α) such that for every dyadic cube Q and R ∈ ∆Q,X , the Hausdorff distance between Q and R is at most C1 side Q. Moreover, there exists a ∗ ∗ constant C2 = C2(n, α) < ∞ such that ∆Q,X and ∇R,X have cardinality at most C2 for every dyadic cube Q and R in Rn. n 1 1 1 1 Proof. For ease of computation, pick coordinates on R so that Q = [− 2 , 2 )×· · ·×[− 2 , 2 ) is a “dyadic cube” of side length 1 with center at the origin. We return to the conventional definition of dyadic cubes at the conclusion of the proof. Suppose that R is another dyadic cube of side length 1 such that R ∩ XQ \ U(0, r/3) 6= ∅. We first want to determine how large r must be to ensure that R∩U(0, r/4) = ∅. Choose any point z ∈ R∩X \U(0, r/3). √ √ Q For any x ∈ R, |x| ≥ |z| − diam R ≥ r/3 − n. Hence |x| > r/4 if r > 12 n. Impose this lower bound on r. c Next we find how large r must be to guarantee that gap(R,Xb(V, α/2) ) ≥ diam Q for every b ∈ Q. Continuing to work with z, pick a ∈ Q such that z ∈ Xa, which 8 MATTHEW BADGER AND LISA NAPLES

c exists because z ∈ XQ. Fix b ∈ Q. To show that gap(R,Xb(V, α/2) ) ≥ diam Q, it suﬃces to prove B(z, 2 diam R) ⊆ X (V, α/2). Fix w ∈ B(z, 2 diam R) and recall that √ b diam Q = diam R = n. By repeated use of the triangle inequality and deﬁnition of Xa,

√ ⊥ √ ⊥ √ dist(w, Vb) ≥ dist(z, Va) − 3 n > α dist(z, Va ) − 3 n ≥ α dist(w, Vb ) − 3(1 + α) n α α √ = dist(w, V ⊥) + dist(w, V ⊥) − 3(1 + α) n. 2 b 2 b

We now split into cases. From the displayed inequality, we see that w ∈ Xb(V, α/2) if ⊥ √ ⊥ √ (α/2) dist(w, Vb ) ≥ 3(1 + α) n. Suppose otherwise that dist(w, Vb ) < 6 n(1 + α)/α. By the Pythagorean theorem, we have

2 2 ⊥ 2 2 ⊥ 2 dist(w, Vb) = |w − b| − dist(w, Vb ) ≥ (|z| − |w − z| − |b|) − dist(w, Vb ) √ 2 ⊥ 2 ≥ (r/3 − 3 n) − dist(w, Vb ) .

⊥ We want dist(w, Vb) > (α/2) dist(w, Vb ). Thus, we want r to be large enough so that r √ 2 α2 − 3 n ≥ + 1 dist(w, V ⊥)2. 3 2 b

√ ⊥ √ 1 2 2 Set ρ = r/3 − 3 n. Because dist(w, Vb ) < 6 n(1 + α)/α and ( 4 α + 1) < (1 + α) , it suffices to choose ρ large enough so that ρ2 ≥ 36n(1 + α)4/α2. Taking square roots and using the crude estimate (1 + α)2/α ≤ 4 max(α, 1/α), we see that it suffices to assume √ that r ≥ 81 n max(α, 1/α). The computations above were for a dyadic cube Q of side length 1 centered at the origin. By scale and translation invariance, we conclude that if we define √ rQ,X = 81 n max(α, 1/α) side Q for all Q, then R∩B(x , r /4) = ∅ and gap(R,X (V, α/2)c) ≥ diam Q for all R ∈ ∆∗ and x ∈ Q. Q Q,X √ x Q Now, put sQ,X = rQ,X − n side Q for each dyadic cube Q. Fix a dyadic cube Q and 1 a ∈ Q. Suppose that y ∈ Xa ∩ B(a, sQ,X ) \ U(a, 2 sQ,X ). On the one hand, √ |y − xQ| ≤ |y − a| + |a − xQ| ≤ sQ,X + n side Q = rQ,X .

On the other hand, s √ |y − x | ≥ |y − a| − |a − x | ≥ Q,X − n side Q Q Q 2 r 3√ √ r ≥ Q,X − n side Q ≥ 39 n max(α, 1/α) side Q > Q,X . 2 2 3 Thus, y ∈ X ∩ B(x , r ) \ U(x , r /3) ⊆ A . a Q Q,X Q Q,X Q,X √ For every dyadic cube Q and R ∈ ∆∗ , we have Q ⊆ B(x , n side Q) and R ⊆ √ Q,X Q √ B(xQ, rQ,X + n side Q), because R intersects AQ,X and diam Q = n side Q. Therefore, the Hausdorﬀ distance between Q and R is at most C1(n, α) side Q. By volume doubling, ∗ ∗ it follows that ∆Q,X and ∇R,X have cardinality at most C2(n, α). RADON MEASURES AND LIPSCHITZ GRAPHS 9

We say that T is a tree of dyadic cubes if T is a set of dyadic cubes ordered by inclusion such that T has a unique maximal element, denoted by Top(T ), and if Q ∈ T , then P ∈ T S∞ for all dyadic cubes Q ⊆ P ⊆ Top(T ). We may partition T = 0 Ti, where −i side Q = 2 side Top(T ) for all Q ∈ Ti.

An infinite branch is a decreasing sequence Q0 ⊇ Q1 ⊇ Q2 ⊇ · · · of cubes in T with each Qi ∈ Ti. We define the set of leaves of T , denoted by Leaves(T ), to be ( ∞ ) [ \ Leaves(T ) = Qi : Q0 ⊇ Q1 ⊇ Q2 ⊇ · · · is an infinite branch of T . i=0 Although the set of leaves is facially a union over uncountably many infinite branches, T∞ S because #Ti < ∞ for all i ≥ 0, one may prove that Leaves(T ) = i=0 Ti; e.g., see the argument at the top of [Rog98, p. 48]. Hence Leaves(T ) is an Fσδ Borel set.

Lemma 2.2. Let T be a tree of dyadic cubes in Rn, let µ be a Radon measure on Rn, ∗ and let X = X(V, α) be a bad cone. If µ(R) = 0 for every Q ∈ T and R ∈ T ∩ ∆Q,X , then there is a Lipschitz function f : V → V ⊥ with Lipschitz constant at most α such that µ(Leaves(T ) \ Graph(f)) = 0. Proof. We may assume that Leaves(T ) 6= ∅, since otherwise the conclusion is trivial. Let S S A = Leaves(T ) \ ∗ R. Then Q∈T R∈T ∩∆Q,X X X µ(Leaves(T ) \ A) ≤ µ(R) = 0. ∗ Q∈T R∈T ∩∆Q,X We will use Lemma 1.1 to show that A is contained in the graph of a Lipschitz function over V with Lipschitz constant at most α. Let x ∈ A and pick an inﬁnite branch Q0 ⊇ Q ⊇ Q ⊇ · · · such that {x} = T∞ Q . We must show that A ∩ X = ∅. For each dyadic 1 2 √ 0 i x cube Q, write sQ,X = rQ,X − n side Q and note that sQ,X = C(n, α) side Q diam Q. By Lemma 2.1, for each cube Qi in the inﬁnite branch containing x, [ A ∩ X ∩ B(x, s ) \ U x, 1 s ⊆ A ∩ A ⊆ T ∩ ∆∗ ⊆ n \ A. x Qi,X 2 Qi,X Qi,X Qi,X R 1 Because sQi+1,X = 2 sQi,X for each i ≥ 0, it follows that A ∩ Xx ∩ B(x, sQ0,X ) = ∅. Also, since A ⊆ Q0 and sQ0,X diam Q0, we have A ∩ Xx \ B(x, sQ0,X ) = ∅, as well. Thus, ⊥ A∩Xx = ∅ for all x ∈ A. By Lemma 1.1, there exists f : V → V with Lipschitz constant at most α such that A ⊆ Graph(f). Finally,

µ(Leaves(T ) \ Graph(f)) ≤ µ(Leaves(T ) \ A) = 0. We have reached the main technical result of the paper. The proof of Proposition 2.3 dictates the deﬁnition of the conical defect; see especially the computation in (2.1). Proposition 2.3 (Drawing Lipschitz Graphs through Leaves of a Tree). Let T be a tree of dyadic cubes in Rn and let µ be a Radon measure on Rn. If there exists a bad cone P X = X(V, α) such that Q∈T Defect(µ, Q, X) µ(Q) < ∞, then µ Leaves(T ) is carried by graphs of Lipschitz functions f : V → V ⊥ with Lipschitz constant at most α. 10 MATTHEW BADGER AND LISA NAPLES

S∞ −i Proof. Suppose that T = 0 Ti, where Ti denotes the cubes of side length 2 side Top(T ). Without loss of generality, we may assume that side Top(T ) = 1 and µ(Q) > 0 for every cube Q ∈ T , because deleting cubes in the tree with µ measure zero has no effect on the graph rectifiability of µ Leaves(T ). As every µ null set is trivially graph rectifiable, we may further assume that µ(Leaves(T )) > 0. The general scheme of the proof is to identify countably many subtrees of T whose sets of leaves are each contained in a Lipschitz graph and collectively cover µ almost all of the set of leaves of T . ∗ We will say that a dyadic cube R ∈ T is bad if there exists Q ∈ T such that R ∈ ∆Q,X . Bad cubes are the obstacles to invoking Lemma 2.2. Let us compute the total measure of bad cubes in level i of the tree. There are no bad cubes in T0, because the first level only contains one cube. Fix i ≥ 1 and let Bi denote the set of Q ∈ Ti such that there exists ∗ R ∈ ∆Q,X ∩ T , i.e. the discretized conical annulus for Q contains a bad cube. Then X X X µ(R)µ(Q) X X µ(R)µ(Q) µ(R) = S ∗ = S ∗ ∗ µ( ∇R,X ∩ T ) ∗ µ( ∇R,X ∩ T ) bad R∈Ti bad R∈Ti Q∈∇ ∩T Q∈Bi R∈∆ ∩T (2.1) R,X Q,X X X µ(R)µ(Q) X ≤ ≤ Defect(µ, Q, X) µ(Q), ∗ µ(Q) Q∈Bi R∈∆Q,X Q∈Ti

S ∗ where in the penultimate inequality 0 < µ(Q) ≤ µ( ∇R,X ∩ T ) because Q ∈ Bi and ∗ ∗ Q ∈ ∇R,X for all R ∈ ∆Q,X . The ﬁrst equality in (2.1) may be interpreted as equitably ∗ distributing the mass of a bad cube R to the cubes Q ∈ ∇R,X ∩ T which “see” R. Let 0 < δ < 1 be given. Because the weighted sum of the conical defect over T converges, there exists i0 = i0(δ) ≥ 1 suﬃciently large such that the tail

∞ ∞ X X X X (2.2) µ(R) ≤ Defect(µ, Q, X) µ(Q) < δ µ(Leaves(T )).

i=i0 bad R∈Ti i=i0 Q∈Ti

δ δ δ Let Q1,...,Qk be an enumeration of the cubes in Ti0 such that each cube Qj is not bad. δ δ δ δ Then let U1 ,..., Uk denote the maximal subtrees of T with Top(Uj ) = Qj that contain δ Sk δ no bad cubes. By (2.2), the trees exist, and the set A = j=1 Leaves(Uj ) satisﬁes µ(Aδ) ≥ (1 − δ)µ(Leaves(T )).

δ δ Moreover, by k applications of Lemma 2.2 (each Uj contains no bad cubes), A is contained in the union of k = k(δ) Lipschitz graphs over V of Lipschitz constant at most α. To complete the proof, repeat the construction in the previous paragraph over any countable choice of parameters δ = δj with limj→∞ δj = 0. Let T be a tree of dyadic cubes, let b : T → [0, ∞) be any function, and let µ be a Radon measure on Rn. Following [BS17, §5], we deﬁne the µ-normalized sum function

X χQ(x) S (µ, x) = b(Q) for all x ∈ n, T ,b µ(Q) R Q∈T RADON MEASURES AND LIPSCHITZ GRAPHS 11 with the convention that 0/0 = 0 and 1/0 = ∞. For example, for every dyadic cube Q0 of side length 1, the conical Dini function Gµ,X (x) = ST ,b(µ, x) for all x ∈ Q0, where T is the tree of dyadic cubes contained in Q0 and b(Q) = Defect(µ, Q, X) µ(Q). Lemma 2.4 (Localization Lemma, [BS17, Lemma 5.6]). Let T be a tree of dyadic cubes, let b : T → [0, ∞), and let µ be a Radon measure on Rn. For all N < ∞ and ε > 0, there exists a partition of T into a set G of good cubes and a set B of bad cubes with the following properties. (1) Either G = ∅ or G is a tree of dyadic cubes with Top(G) = Top(T ). (2) Every child of a bad cube is a bad cube: if P,Q ∈ T , P ∈ B, and Q ⊆ P , then Q ∈ B.

(3) The set A = {x ∈ Top(T ): ST ,b(x) ≤ N} is Borel and µ(A ∩ Leaves(G)) ≥ (1 − εµ(Top(T ))) µ(A). P (4) The sum of b over G is finite: Q∈G b(Q) < N/ε. Countably many applications of Proposition 2.3 and Lemma 2.4 yield the following sufficient condition in terms of the conical Dini function for Lipschitz graph rectifiability of a measure with prescribed direction V and Lipschitz constant α. Being similar to the proof of [BS17, Theorem 5.1], we omit the details.

Theorem 2.5. Let µ be a Radon measure on Rn and let X = X(V, α) be a bad cone for n some V ∈ G(n, m) and α ∈ (0, ∞). Then µ {x ∈ R : Gµ,X (x) < ∞} is carried by graphs of Lipschitz functions f : V → V ⊥ of Lipschitz constant at most α.

3. Necessary Conditions

Recall that gap(S,T ) = inf{|s − t| : s ∈ S, t ∈ T } for all nonempty sets S,T ⊆ Rn. We define the quantity excess(S,T ) = sups∈S inft∈T |s − t| ∈ [0, ∞] for all nonempty sets S,T ⊆ Rn. By convention, we also set excess(∅,S) = 0, but leave excess(S, ∅) undefined. The Hausdorff distance between nonempty sets S and T is defined to be the maximum of excess(S,T ) and excess(T,S). To establish necessary conditions for Lipschitz graph rectifiability in terms of the conical Dini functions, we follow the strategy used in [BS15, §3] and [BS17, §4] to prove necessary conditions for a Radon measure to be carried by rectifiable curves. The argument must be modified to incorporate the geometry of Lipschitz graphs.

Proposition 3.1. Let µ be a Radon measure on Rn and let X = X(V, α) be a bad cone for some V ∈ G(n, m) and α ∈ (0, ∞). Suppose that Γ = Graph(f) for some Lipschitz function f : V → V ⊥ with Lipschitz constant at most α/2. There exists a constant

C = C(n, α) > 1 such that for every x0 ∈ Γ and r0 > 0, Z (3.1) Gµ,X (x) dµ(x) .n,α µ(B(x0, r0 + C) \ Γ) < ∞. Γ∩B(x0,r0)

In particular, Gµ,X (x) < ∞ at µ-a.e. x ∈ Γ. 12 MATTHEW BADGER AND LISA NAPLES

Proof. Let µ, V , α, f, Γ, x0, and r0 be ﬁxed as in the statement of the lemma. Abbreviate Γ0 = Γ ∩ B(x0, r0). By Tonelli’s theorem, Z X Z Gµ,X (x) dµ(x) = Defect(µ, Q, X) χQ(x) dµ(x) Γ0 side Q≤1 Γ0 X X = Defect(µ, Q, X) µ(Γ0 ∩ Q) ≤ Defect(µ, Q, X) µ(Q). side Q≤1 side Q≤1 µ(Γ0∩Q)>0

For any dyadic cube Q such that side Q ≤ 1 and µ(Γ0 ∩ Q) > 0,

X µ(R) [ ∗ Defect(µ, Q, X) µ(Q) = µ(Q) = µ ∆Q,X , ∗ µ(Q) R∈∆Q,X S ∗ ∗ where ∆Q,X denotes the union of all cubes in ∆Q,X Thus, Z X [ ∗ Gµ,X (x) dµ(x) ≤ µ ∆Q,X . Γ0 side Q≤1 µ(Γ0∩Q)>0 S ∗ We now aim to prove that the non-tangential regions TQ,X = ∆Q,X associated to dyadic n cubes with side Q ≤ 1 and µ(Γ0∩Q) > 0 are contained in R \Γ and have bounded overlap. This requires that we use the geometry of the Lipschitz graph Γ.

Let Q be a dyadic cube of side length at most 1 such that µ(Γ0∩Q) > 0. Pick a ∈ Γ0∩Q. Because Γ is the graph of a Lipschitz function over V with Lipschitz constant at most c α/2, Lemma 1.1 tells us that the graph Γ is contained in Xa(V, α/2) . By deﬁnition of c ∗ rQ,X or proof of Lemma 2.1, gap(R,Xa(V, α/2) ) ≥ diam Q for all R ∈ ∆Q,X . Hence c (3.2) gap(TQ,X , Γ) ≥ gap(TQ,X ,Xa(V, α/2) ) ≥ diam Q. ∗ If R ∈ ∆Q,X , then there exists z ∈ R such that |z − xQ| ≤ rQ,X = 81 max(α, 1/α) diam Q. For an arbitrary point y ∈ R, |y − a| ≤ |y − z| + |z − xQ| + |xQ − a|. Thus,

(3.3) excess(TQ,X , Γ) ≤ excess(TQ,X , {a}) ≤ 83 max(α, 1/α) diam Q. √ 0 It follows that TQ,X ⊆ B(x0, r0 + 83 n max(α, 1/α)) \ Γ. Furthermore, suppose that Q is −N 0 a dyadic cube of side length 2 side Q such that µ(Γ0 ∩Q ) > 0. By (3.2) and (3.3), TQ,X −N and TQ0,X are disjoint if 2 83 max(α, 1/α) < 1. Thus, if TQ,X ∩ TQ0,X 6= ∅, where TQ,X 0 and TQ0,X are non-tangential regions associated to dyadic cubes Q and Q intersecting Γ0 of side lengths 2−λ and 2−λ0 at most 1, then |λ − λ0| ≤ C(n, α). Another consequence of (3.3) is that diam TQ,X ≤ 166 max(α, 1/α) diam Q. It follows that we have bounded overlap of the non-tangential regions: TQ,X intersects TQ0,X for at most C(n, α) other 0 0 0 cubes Q with side Q ≤ 1 and µ(Γ0 ∩ Q ) > 0. Therefore, Z X √ Gµ,X (x) dµ(x) ≤ µ (TQ,X ) .n,α µ(B(x0, r0 + 83 n max(α, 1/α)) \ Γ). Γ0 side Q≤1 µ(Γ0∩Q)>0 The last displayed quantity is ﬁnite, because µ is a Radon measure. This veriﬁes that

(3.1) holds for all x0 ∈ Γ and r0 > 0. Hence the conical Dini function Gµ,X (x) < ∞ at RADON MEASURES AND LIPSCHITZ GRAPHS 13 S∞ µ-a.e. x ∈ Γ0 = Γ ∩ B(x0, r0). Because r0 > 0 was arbitrary and Γ ⊆ k=1 B(x0, k), we conclude that Gµ,X (x) < ∞ at µ-a.e. x ∈ Γ. Theorem 3.2. Let µ be a Radon measure on Rn. Suppose V ∈ G(n, m) and α ∈ (0, ∞). If µ is carried by graphs of Lipschitz functions f : V → V ⊥ of Lipschitz constant at most n α and β ≥ 2α, then Gµ,X(V,β)(x) < ∞ at µ-a.e. x ∈ R . ⊥ Proof. The hypothesis asserts that there exist Lipschitz functions f1, f2, ··· : V → V n S∞ with Lipschitz constant at most α such that µ(R \ 1 Γi) = 0, where each Γi = Graph(fi). Let β ≥ 2α, so that each function fi has Lipschitz constant at most β/2. By Proposition 3.1, for each i ≥ 1, there exists a set Ni ⊆ Γi such that µ(Ni) = 0 and Gµ,X(V,β)(x) < ∞ S∞ at every x ∈ Γi \ Ni. Set E = 1 Γi \ Ni. Then Gµ,X(V,β)(x) < ∞ for every x ∈ E and ∞ ! ∞ n n [ X µ(R \ E) ≤ µ R \ Γi + µ(Ni) = 0. 1 1 4. Proof of the Main Theorem

Let 1 ≤ m ≤ n − 1 and let µ be a Radon measure on Rn. Existence and uniqueness of the decomposition is standard.

⊥ Lemma 4.1. There exists a unique decomposition µ = µG + µG, where µG is a Radon ⊥ measure that is carried by m-dimensional Lipschitz graphs and µG is a Radon measure that is singular to m-dimensional Lipschitz graphs. Proof. The decomposition follows from a simple modiﬁcation of the usual proof of the Lebesgue decomposition theorem. For each integer r ≥ 2, use the approximation property of the supremum to choose a set Γr, which is a ﬁnite union of m-dimensional Lipschitz graphs, such that

µ(Γr) ≥ (1 − 1/r) sup µ(Γ ∩ B(0, r)) < ∞, Γ where the supremum ranges over all sets Γ, which are ﬁnite unions of m-dimensional n S∞ ⊥ Lipschitz graphs in R . Then µG = µ r=2 Γr and µG = µ − µG. Uniqueness of the decomposition can be proved by contradiction. For full details, see e.g. the appendix of [BV19]. The content of Theorem 1.5 over Lemma 4.1 and our task in the remainder of the proof ⊥ is to identify the component measures µG and µG using the conical Dini functions.

Lemma 4.2. For every bad cone X, the conical Dini function Gµ,X is Borel measurable.

Proof. By deﬁnition, each conical Dini function Gµ,X is a countable linear combination of characteristic functions of Borel sets. Lemma 4.3. There exists a countable family X (n, m) of bad cones (independent of µ) n such that Gµ,X (x) < ∞ at some x ∈ R for some bad cone X if and only if Gµ,X0 (x) < ∞ for some X0 ∈ X (n, m). 14 MATTHEW BADGER AND LISA NAPLES

Proof. The value of a conical Dini function Gµ,X (x) is determined by the value of the ∗ measure on dyadic cubes Q and R ∈ ∆Q,X , where Q ranges over all dyadic cubse of side ∗ length at most 1 that contains x. The cubes belonging to ∆Q,X for any particular Q ∗ are completely determined by xQ, side Q, and the arrangement of cubes in ∆Q0,X , where ∗ Q0 = [0, 1) × · · · × [0, 1). By Lemma 2.1, the cubes in ∆Q0,X are dyadic cubes of side length 1 contained in B(xQ0 ,C(n, α)), where for each integer N ≥ 1, the constant C(n, α) is uniformly bounded for all α ∈ (1/N, N). Therefore, there are only countably many ∗ possible configurations of ∆Q,X . Define X (n, m) by including exactly one bad cone X for each possible configuration of ∆∗ . Q0,X

We are ready to complete the proof of Theorem 1.5. Let µ1 and µ2 be the measures deﬁned by n µ1 = µ {x ∈ R : Gµ,X (x) < ∞ for some bad cone X}, n µ2 = µ {x ∈ R : Gµ,X (x) = ∞ for every bad cone X}. By Lemma 4.3, we may alternatively express n µ1 = µ {x ∈ R : Gµ,X (x) < ∞ for some X ∈ X (n, m)}, n µ2 = µ {x ∈ R : Gµ,X (x) = ∞ for every X ∈ X (n, m)}.

In view of Lemma 4.2, we conclude that µ1 and µ2 are restrictions of a Radon measure to a Borel set. Hence µ1 and µ2 are Radon. n On the one hand, for each bad cone X, µG,X = µ {x ∈ R : Gµ,X (x) < ∞} is carried by m-dimensional Lipschitz graphs by Theorem 2.5. Because X (n, m) is countable, P µ+ = X∈X (n,m) µG,X is also carried by Lipschitz graphs. By Lemma 4.3, µ1 ≤ µ+. Thus, µ1 is carried by m-dimensional Lipschitz graphs, because the dominant measure µ+ is carried by Lipschitz graphs. On the other hand, let Γ be an arbitrary m-dimensional Lipschitz graph, say that Γ = Graph(f) where f is a Lipschitz function f : V → V ⊥ with Lipschitz constant at most α. By Proposition 3.1, Gµ,X(V,2α)(x) < ∞ at µ-a.e. x ∈ Γ. Because µ2 ≤ µ, we have Gµ,X(V,2α)(x) < ∞ at µ2-a.e. x ∈ Γ, as well. By deﬁnition, the measure µ2 vanishes on n {x ∈ R : Gµ,X(V,2α)(x) < ∞}. Therefore, µ2(Γ) = 0. Since Γ was arbitrary, we conclude that µ2 is singular to m-dimensional Lipschitz graphs. It is immediate from the deﬁnition of µ1 and µ2 that µ = µ1 + µ2. Since µ1 and µ2 are Radon measures, µ1 is carried by m-dimensional Lipschitz graphs, and µ2 is singular to ⊥ m-dimensional Lipschitz graphs, we know that µ1 = µG and µ2 = µG by uniqueness of the decomposition in Lemma 4.1. This completes the proof of Theorem 1.5.

5. Variations We conclude with some remarks on ﬂexibility in the deﬁnition of the conical defect and variations on the main theorem. The restriction to half-open dyadic cubes is hidden in the proof of the localization lemma for the µ-normalized sum function (see Lemma 2.4). The lemma remains valid for any system of sets A with the property that if T is a tree of RADON MEASURES AND LIPSCHITZ GRAPHS 15 sets in A and B is a subset of T such that A, B ∈ B and A ⊆ B implies A = B, then B has bounded overlap with constants independent of B and T . Of course, half-open dyadic cubes, half-open triadic cubes, etc. enjoy this property with bounded overlap 1. One could probably design a version of the conical defect and main theorem with Euclidean balls by using the Besicovitch covering theorem instead of the localization lemma. The main theorem remains valid if one replaces the conical defect by the larger quantity

X µ(SR) , ∗ µ(Q) R∈∆Q,X where SR is any Borel set containing R with diameter at most C diam R for some constant 1 ≤ C < ∞ independent of R. This change requires increasing the size of the radius rQ,X c depending on the constant C to ensure that gap(SR,X(V, γ) ) & diam Q for some γ < α. Because the sets SR may overlap, this is a slight strengthening of the necessary condition for Lipschitz graph rectiﬁability.

If one prefers a construction where the radius rQ,X of the conical annulus is independent ∗ of the cone opening α, this can be achieved at the cost of taking the cubes R ∈ ∆Q,X to have side length smaller than Q. In particular, there existsr ˜Q,X depending only on n and a jump parameter J ∈ N depending on n and α with the following property. If R is a −J dyadic cube of side length 2 side Q that intersects XQ∩B(xQ, r˜Q,X )\B(xQ, r˜Q,X /3), then c R∩B(xQ, r˜Q,X /4) = ∅ and gap(R,X(V, α/2) ) ≥ diam R. The proofs of the suﬃcient and necessary conditions with this modiﬁcation are essentially the same as above, although there is more bookkeeping involving J.

Every m-dimensional plane x0 + V is a Lipschitz graph over V with constant at most α n for every α > 0. It follows that µ {x ∈ R : ∀V ∈G(n,m)∃α>0 Gµ,X(V,α) = ∞} is singular to aﬃne m-dimensional planes. However, this cannot be directly used to characterize Radon measures that are carried by or singular to planes. We leave ﬁnding such a characterization as an open problem for future research.

References [AAM19] Murat Akman, Jonas Azzam, and Mihalis Mourgoglou, Absolute continuity of harmonic measure for domains with lower regular boundaries, Adv. Math. 345 (2019), 1206–1252. MR 3903916 [ADT16] Jonas Azzam, Guy David, and Tatiana Toro, Wasserstein distance and the rectifiability of doubling measures: part I, Math. Ann. 364 (2016), no. 1-2, 151–224. MR 3451384 [ADT17] Jonas Azzam, Guy David, and Tatiana Toro, Wasserstein distance and the rectifiability of doubling measures: part II, Math. Z. 286 (2017), no. 3-4, 861–891. MR 3671564 [AHM+16] Jonas Azzam, Steve Hofmann, JoséMar´ıaMartell, Svitlana Mayboroda, Mihalis Mourgoglou, Xavier Tolsa, and Alexander Volberg, Rectifiability of harmonic measure, Geom. Funct. Anal. 26 (2016), no. 3, 703–728. MR 3540451 [Alm69] F. J. Almgren, Jr., Measure theoretic geometry and elliptic variational problems, Bull. Amer. Math. Soc. 75 (1969), 285–304. MR 240689 [AS18] Jonas Azzam and Raanan Schul, An analyst’s traveling salesman theorem for sets of dimension larger than one, Math. Ann. 370 (2018), no. 3-4, 1389–1476. MR 3770170 16 MATTHEW BADGER AND LISA NAPLES

[AT15] Jonas Azzam and Xavier Tolsa, Characterization of n-rectifiability in terms of Jones’ square function: Part II, Geom. Funct. Anal. 25 (2015), no. 5, 1371–1412. MR 3426057 [ATT20] Jonas Azzam, Xavier Tolsa, and Tatiana Toro, Characterization of rectifiable measures in terms of α-numbers, Trans. Amer. Math. Soc. 373 (2020), no. 11, 7991–8037. MR 4169680 [Bad12] Matthew Badger, Null sets of harmonic measure on NTA domains: Lipschitz approximation revisited, Math. Z. 270 (2012), no. 1-2, 241–262. MR 2875832 [Bad19] Matthew Badger, Generalized rectifiability of measures and the identification problem, Com- plex Anal. Synerg. 5 (2019), no. 1, Paper No. 2, 17. MR 3941625 [Bee93] Gerald Beer, Topologies on closed and closed convex sets, Mathematics and its Applications, vol. 268, Kluwer Academic Publishers Group, Dordrecht, 1993. MR 1269778 [Bes28] A. S. Besicovitch, On the fundamental geometrical properties of linearly measurable plane sets of points, Math. Ann. 98 (1928), no. 1, 422–464. MR 1512414 [Bes38] A. S. Besicovitch, On the fundamental geometrical properties of linearly measurable plane sets of points (II), Math. Ann. 115 (1938), no. 1, 296–329. MR 1513189 [BNV19] Matthew Badger, Lisa Naples, and Vyron Vellis, Höldercurves and parameterizations in the Analyst’s Traveling Salesman theorem, Adv. Math. 349 (2019), 564–647. MR 3941391 [BS15] Matthew Badger and Raanan Schul, Multiscale analysis of 1-rectifiable measures: necessary conditions, Math. Ann. 361 (2015), no. 3-4, 1055–1072. MR 3319560 [BS16] Matthew Badger and Raanan Schul, Two sufficient conditions for rectifiable measures, Proc. Amer. Math. Soc. 144 (2016), no. 6, 2445–2454. MR 3477060 [BS17] Matthew Badger and Raanan Schul, Multiscale Analysis of 1-rectifiable Measures II: Charac- terizations, Anal. Geom. Metr. Spaces 5 (2017), 1–39. MR 3627148 [BV19] Matthew Badger and Vyron Vellis, Geometry of measures in real dimensions via Hölder parameterizations, J. Geom. Anal. 29 (2019), no. 2, 1153–1192. MR 3935254 [CKRS10] Marianna Csörnyei, Antti Käenmäki,Tapio Rajala, and Ville Suomala, Upper conical density results for general measures on Rn, Proc. Edinb. Math. Soc. (2) 53 (2010), no. 2, 311–331. MR 2653235 [CMM82] R. R. Coifman, A. McIntosh, and Y. Meyer, L’intégrale de Cauchy définitun opérateur bornésur L2 pour les courbes lipschitziennes, Ann. of Math. (2) 116 (1982), no. 2, 361–387. MR 672839

[Dab19] Damian Dabrowski, Necessary condition for rectiﬁability involving Wasserstein distance W2, preprint, arXiv:1904.11000v2, 2019. [Dab20a] Damian Dabrowski, Cones, rectiﬁability, and singular integral operators, preprint, arXiv:2006.14432, 2020.

[Dab20b] Damian Dabrowski, Sufficient condition for rectifiability involving Wasserstein distance W2, preprint, arXiv:1904.11004v2, 2020. [Dab20c] Damian Dabrowski, Two examples related to conical energies, preprint, arXiv:2011.12717, 2020. [Dav14] Guy David, Should we solve Plateau’s problem again?, Advances in analysis: the legacy of Elias M. Stein, Princeton Math. Ser., vol. 50, Princeton Univ. Press, Princeton, NJ, 2014, pp. 108–145. MR 3329849 [DJ90] G. David and D. Jerison, Lipschitz approximation to hypersurfaces, harmonic measure, and singular integrals, Indiana Univ. Math. J. 39 (1990), no. 3, 831–845. MR 1078740 [DL08] Camillo De Lellis, Rectifiable sets, densities and tangent measures, Zurich Lectures in Ad- vanced Mathematics, European Mathematical Society (EMS), Zürich, 2008. MR 2388959 [DNOI19] Giacomo Del Nin and Kennedy Obinna Idu, Geometric criteria for C1,α rectifiability, preprint, arXiv:1909.10625v2, 2019. RADON MEASURES AND LIPSCHITZ GRAPHS 17

[DS91] G. David and S. Semmes, Singular integrals and rectifiable sets in Rn: Beyond Lipschitz graphs, Astérisque(1991), no. 193, 152. MR 1113517 (92j:42016) [DS93] Guy David and Stephen Semmes, Analysis of and on uniformly rectifiable sets, Mathematical Surveys and Monographs, vol. 38, American Mathematical Society, Providence, RI, 1993. MR 1251061 (94i:28003) [ENV17] Nick Edelen, Aaron Naber, and Daniele Valtorta, Quantitative Reifenberg theorem for measures, preprint, arXiv:1612.08052v2, 2017. [ENV19] Nick Edelen, Aaron Naber, and Daniele Valtorta, Effective Reifenberg theorems in Hilbert and Banach spaces, Math. Ann. 374 (2019), no. 3-4, 1139–1218. MR 3985109 [Fed47] Herbert Federer, The (ϕ, k) rectifiable subsets of n-space, Trans. Amer. Soc. 62 (1947), 114– 192. MR 0022594 [Ghi20] Silvia Ghinassi, Sufficient conditions for C1,α parametrization and rectifiability, Ann. Acad. Sci. Fenn. Math. 45 (2020), 1065–1094. [GKS10] John Garnett, Rowan Killip, and Raanan Schul, A doubling measure on Rd can charge a rectifiable curve, Proc. Amer. Math. Soc. 138 (2010), no. 5, 1673–1679. MR 2587452 (2011a:28018) [Goe19] Max Goering, Characterizations of countably n-rectifiable Radon measures by higher- dimensional Menger curvatures, preprint, arXiv:1804.02497v4, 2019. [Hyd20] Matthew Hyde, An Analyst’s Travelling Salesman Theorem for general sets in Rn, preprint, arXiv:2006.16677v2, 2020. [Jon90] Peter W. Jones, Rectifiable sets and the traveling salesman problem, Invent. Math. 102 (1990), no. 1, 1–15. MR 1069238 (91i:26016) [Mat95] Pertti Mattila, Geometry of sets and measures in Euclidean spaces, Cambridge Studies in Advanced Mathematics, vol. 44, Cambridge University Press, Cambridge, 1995, Fractals and rectifiability. MR 1333890 (96h:28006) [MM88] Miguel Angel´ Mart´ınand Pertti Mattila, k-dimensional regularity classifications for s-fractals, Trans. Amer. Math. Soc. 305 (1988), no. 1, 293–315. MR 920160 [MO18] Henri Martikainen and Tuomas Orponen, Boundedness of the density normalised Jones’ square function does not imply 1-rectifiability, J. Math. Pures Appl. (9) 110 (2018), 71–92. MR 3744920 [MR44] A. P. Morse and John F. Randolph, The φ rectifiable subsets of the plane, Trans. Amer. Math. Soc. 55 (1944), 236–305. MR 0009975 [Nap20] Lisa Naples, Rectifiability of pointwise doubling measures in Hilbert space, preprint, arXiv:2002.07570, 2020. [NTV14] Fedor Nazarov, Xavier Tolsa, and Alexander Volberg, On the uniform rectifiability of AD- regular measures with bounded Riesz transform operator: the case of codimension 1, Acta Math. 213 (2014), no. 2, 237–321. MR 3286036 [Oki92] Kate Okikiolu, Characterization of subsets of rectifiable curves in Rn, J. London Math. Soc. (2) 46 (1992), no. 2, 336–348. MR 1182488 (93m:28008) [Rog98] C. A. Rogers, Hausdorff measures, Cambridge Mathematical Library, Cambridge University Press, Cambridge, 1998, Reprint of the 1970 original, With a foreword by K. J. Falconer. MR 1692618 [Sch07] Raanan Schul, Subsets of rectifiable curves in Hilbert space—the analyst’s TSP, J. Anal. Math. 103 (2007), 331–375. MR 2373273 (2008m:49205) [Tol15] Xavier Tolsa, Characterization of n-rectifiability in terms of Jones’ square function: part I, Calc. Var. Partial Differential Equations 54 (2015), no. 4, 3643–3665. MR 3426090

[Tol19] Xavier Tolsa, Rectiﬁability of measures and the βp coeﬃcients, Publ. Mat. 63 (2019), no. 2, 491–519. MR 3980933 18 MATTHEW BADGER AND LISA NAPLES

[TT15] Xavier Tolsa and Tatiana Toro, Rectiﬁability via a square function and Preiss’ theorem, Int. Math. Res. Not. IMRN (2015), no. 13, 4638–4662. MR 3439088

Department of Mathematics, University of Connecticut, Storrs, CT 06269-1009 E-mail address: [email protected]

Department of Mathematics, University of Connecticut, Storrs, CT 06269-1009 Current address: Department of Mathematics, Statistics, and Computer Science, Macalester College, St. Paul, MN 55105 E-mail address: [email protected]