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DOI 10.1007/s00526-016-1004-9

Calculus of Variations

On a generalization of L

p

-differentiability

Daniel Spector1

Received: 12 October 2015 / Accepted: 11 April 2016 / Published online: 20 May 2016

© Springer-Verlag Berlin Heidelberg 2016

Abstract In this paper we connect Calderón and Zygmund’s notion ofLp-differentiability (Calderón and Zygmund, Proc Natl Acad Sci USA 46:1385–1389,1960) with some recent characterizations of Sobolev spaces via the asymptotics of non-local functionals due to Bourgain, Brezis, and Mironescu (Optimal Control and Partial Differential Equations, pp.

439–455,2001). We show how the results of the former can be generalized to the setting of the latter, while the latter results can be strengthened in the spirit of the former. As a consequence of these results we give several new characterizations of Sobolev spaces, a novel condition for whether a function of bounded variation is in the Sobolev spaceW1,1, and complete the proof of a characterization of the Sobolev spaces recently claimed in (Leoni and Spector, J Funct Anal 261:2926–2958,2011; Leoni and Spector, J Funct Anal 266:1106–1114,2014).

Mathematics Subject Classification 46E35 1 Introduction

1.1Lp-differentiability andLp-Taylor approximations

Lp-differentiability was introduced by Calderón and Zygmund in their study of the local properties of solutions of elliptic differential equations [5,6]. It is a natural extension of classical differentiability in that it relaxes the requirement of the existence of a locally linear map in a uniform sense to its existence in an averaged sense. As the Sobolev spaces arise readily in the study of partial differential equations, it is not surprising that Sobolev functions possess anLp-derivative. The following theorem asserting this fact was proven by Calderón and Zygmund [6, Theorem 12] (for a modern reference, see the monograph of Evans and Gariepy [8]).

Communicated by H. Brezis.

B

Daniel Spector

[email protected]

1 Department of Applied Mathematics, National Chiao Tung University, Hsinchu, Taiwan

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Theorem 1.1 (Calderón and Zygmund)Suppose1≤ p<and fW1,p(RN). Then 1

pq

B(0,)|f(x+h)f(x)− ∇f(x)·h|pq dh 1

pq →0 (1.1)

forLN almost every x ∈RN, where1≤qNNp if1≤ p< N ,1≤q <if p= N , and1 ≤ q ≤ ∞if p > N (When q = ∞the left side of (1.1)is understood to be the L(B(0, ))norm applied to the integrand).

While Lp-differentiability is a necessary condition for the inclusion of a function in W1,p, the fact that it does not characterize the space is readily seen by the improvement of exponent in Theorem1.1. A natural question is then whether one can characterize the Sobolev spaces in the spirit of the condition (1.1). Several results have been given in this direction, for instance, a sort of converse to Theorem1.1due to Bagby and Ziemer [2], as well as some characterizations due to Swanson [12,13] that are based on the Calderón–Zygmund classes (see, for example, [16, Chapter 3, p. 132]). In fact, the ideas in [12] were virtually simultaneously introduced by Bourgain, Brezis, and Mironescu [3], who had shown that for

fLp(RN)the simple condition lim sup

→0

RN

B(0,)

|f(x+h)f(x)|p

|h|p dhd x<+∞

characterizesW1,p(RN)for 1 < p < +∞(which actually holds in the context of more general mollifiers, see Section1.2). The main idea in both [3,12] is that instead of considering the infinitesimal behavior of averaged difference quotients one should consider the integrated infinitesimal behavior—that is, one should utilize two integrals instead of one. Notice that the case p = 1 is excluded, since here one obtains a characterization not of W1,1(RN) but B V(RN), the space of functions of bounded variation. To unify the approach for all 1≤p<+∞, let us introduce the following definition.

Definition 1.2 A functionf :RN →Ris said to have a first orderLp-Taylor approximation if fLp(RN)and there exists a functionvLp(RN;RN)such that

→0lim

RN

B(0,)

|f(x+h)f(x)v(x)·h|p

|h|p dhd x=0. (1.2)

The first result of this paper is the following theorem which asserts that functions in the Sobolev spaceW1,p(RN)possess a first orderLp-Taylor approximation.

Theorem 1.3 Let1 ≤ p <and fW1,p(RN). Then f has a first order Lp-Taylor approximation, and moreover, one has the stronger convergence

→0lim

RN

B(0,)

|f(x+h)f(x)− ∇f(x)·h|pq

|h|pq dh

1

q

d x=0, (1.3) where1≤qNNp if1≤p<N ,1≤q<if p=N , and1≤q≤ ∞if p>N .

What is quite surprising is that this property—the existence of a Taylor approximation in thisLpsense—in fact characterizes Sobolev functions. Precisely, we have the following theorem characterizing the Sobolev spaceW1,p(RN)in terms of theLp(RN)convergence (1.2).

Theorem 1.4 Let1 ≤ p <+∞. Then f ∈ W1,p(RN)if and only if f has a first order Lp-Taylor approximation.

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The existence of anL1-Taylor approximation is of a similar character to the assumption of Swanson in [13], since it allows one to gain some equi-integrability in an approximating sequence. If one does not make such a strong assumption, say that the limit (1.3) is finite but not zero, one obtains the following characterization of the space of functions of bounded variation.

Theorem 1.5 Suppose fL1(RN). Then fB V(RN)if and only if there exists a function vL1(RN;RN)such that

lim sup

0

RN

B(0,)

|f(x+h)f(x)v(x)·h|q

|h|q dh 1

q

d x<+∞ (1.4) for any1≤qNN1.

In general, the limit (1.4) is bounded by a constant times|Dsf|(RN), the total variation of the singular portion of the measureD f. However, whenq=1 one can explicitly compute the limit, which is given by

Theorem 1.6 Suppose fB V(RN). Then writing D f=vLN+Dsf wherevL1(RN;RN) and DsfLN, one has

lim0

RN

B(0,)

|f(x+h)f(x)v(x)·h|

|h| dhd x=K1,N|Dsf|(RN).

HereK1,N is as below in Sect.1.2. These results have been announced in [11] (with the exception of Theorem1.6) with proofs of several implications, and it is our intention here to provide the complete proofs of all of the claims. However, another major point we wish to address is the fact that both Theorem1.1and Theorem1.3hold in the context of a larger framework—the use of more general approximations of the identity as seen in the work of Bourgain, Brezis, and Mironescu [3]. We now develop the necessary background for these results and several later in the paper.

1.2 Connections to the work of Bourgain, Brezis, and Mironescu

Let us suppose that⊂RN is open, bounded, and smooth (or all ofRN), and that{ρ} ⊂ L1(RN)are radial mollifiers that satisfy

ρ≥0,

RNρ(x)d x=1, (1.5)

lim0

|x|>δρ(x)d x=0 for allδ >0. (1.6) Takingρ(x) = |B(0,)|1 χB(0,)(x), we revert to the assumptions of the previous section.

However, one has the possibility of new interesting examples, such as that of the “Gagliardo semi-norms”:

ρ(x)=c χB(0,R)

|x|N+(−1)r, forc→0 as→0, or more generally (cf. Brezis [4])

ρ(x)=

⎧⎨

0 if 0<|x| ≤, aψ(|x|) if <|x| ≤1, 0 if 1<|x|,

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whereψL1loc(0,1)satisfies 1

0 ψ(r)rN−1dr= +∞

and

a:=

1

ψ(r)rN1dr −1

→0 as→0.

Then the work1of Bourgain, Brezis, and Mironescu [3] showed two results of particular relevance here. Firstly, if 1≤p<+∞and fC2()then one has

lim0

|f(x)f(y)|p

|xy|p ρ(xy)d y=Kp,N|∇f(x)|p (1.7) for everyx(see [3], p. 444) for

Kp,N :=

SN−1|e1·σ|pdHN−1(σ ).

Secondly, they showed that if 1< p<+∞and fLp(), one has fW1,p()if and only if

lim sup

→0

|f(x)f(y)|p

|x−y|p ρ(xy)d yd x <+∞, and in that case

→0lim

|f(x)f(y)|p

|x−y|p ρ(xy)d yd x =Kp,N

|∇f(x)|p d x. (1.8) In fact, whenρ(x)= |B(0,)|1 χB(0,)(x)one can deduce the convergence (1.7) (even for W1,pfunctions, compare with Corollary1.8below) as a consequence ofLp-differentiability (in an improved form allowing for|h1|p in place of1p, cf. Ambrosio, Fusco, and Pallara [1]), since the estimate

|ApBp| ≤ |A−B|C(1+Ap1+Bp1), (1.9) and Hölder’s inequality imply

lim0

B(x,)

|f(y)f(x)|p

|xy|p d yKp,N|∇f(x)|p

= lim

0

B(x,)

|f(y)f(x)|p

|xy|p d y

B(x,)

f(x)· yx

|yx| p d y

≤lim

0

B(x,)

|f(y)f(x)− ∇f(x)·(yx)|p

|xy|p d y 1

p

×

B(x,)C(1+|f(y)f(x)|p

|xy|p + |∇f(x)|p)d y 1

p

,

1We follow the convention of the subsequent paper of Ponce [14] in taking mollifiers indexed byinstead ofn.

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while the difference quotient appearing in the second quantity can be bounded by observing that

B(x,)

|f(y)f(x)|p

|xy|p d y 1

p

B(x,)

|f(y)f(x)− ∇f(x)·(yx)|p

|xy|p d y 1

p

+

B(x,)

f(x)· yx

|y−x|

p d y 1

p.

The same computation follows for general mollifiers, and in this spirit, one might ask whether the stronger pointwise convergence result of Theorem1.1holds in this setting. Indeed, we have the following theorem to this effect.

Theorem 1.7 Let1≤ p <and fWloc1,p(RN). Supposeρare radial non-increasing and satisfy(1.5)and(1.6). Then for anyη >0one has

→0lim

B(0,η)

|f(x+h)f(x)− ∇f(x)·h|pq

|h|pq ρ(h)dh=0

forLNalmost every x ∈RN, where1≤qNNp if1≤p<N and1≤q<if pN . Combined with the analysis preceding the theorem, one has the following corollary, a version of the pointwise convergence (1.7) for functions inW1,p.

Corollary 1.8 Let1≤ p<and fW1,p(). Supposeρ are radial non-increasing and satisfy(1.5)and(1.6). Then forLNalmost every x ∈RN one has

→0lim

B(0,η)

|f(x+h)f(x)|p

|h|p ρ(h)dh=Kp,N|∇f(x)|p for everyη >0such that B(x, η).

This observation prompts us to return to the energy convergence (1.8) and perform a similar estimate. In this setting, one observes that using Minkowski’s inequality for integrals implies

lim0

|f(y)f(x)|pq

|xy|pq ρ(xy)d y 1

qK

1 q

pq,N|∇f(x)|p

d x

≤ lim

→0

|f(y)f(x)|p

|xy|p

f(x)· yx

|xy| pq

ρ(xy)d y 1q

d x,

which using again the inequality (1.9) and Hölder’s inequality yields

→0lim

|f(y)f(x)|pq

|x−y|pq ρ(xy)d y 1

qK

1

pq,Nq |∇f(x)|p

d x

≤lim

→0

|f(y)f(x)− ∇f(x)·(yx)|pq

|x−y|pq ρ(xy)d y 1

q

d x 1p

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×

C(1+|f(y)f(x)|pq

|x−y|pq + |∇f(x)|pq) ρ(xy)d y 1

q

d x p1

. The same estimate as before shows that the quantities in question are finite, provided one can establish a generalization of the estimate (1.3) to other families of mollifiers. The following theorem shows that for p >1 and pq< p, the Sobolev critical exponent (see Sect.2), one has such a generalization.

Theorem 1.9 Let1< p<and fWloc1,p(RN). Supposeρare radial non-increasing and satisfy(1.5)and(1.6). Then for anyη >0one has

→0lim

K

B(0,η)

|f(x+h)f(x)− ∇f(x)·h|pq

|h|pq ρ(h)dh 1q

d x=0 (1.10) for all K ⊂RN compact, and where1≤q< N−Np if1<p<N .

The degeneracy when p = 1 is more than an issue withW1,1 versus B V, the space of functions of bounded variation. Whereas previously in the paper [10], the author and G.

Leoni had given an example of a function fB V(0,1)showing one could not expect such a convergence for fB V, we present a counterexample to theW1,1case in Sect.5(which is an adaptation a counterexample of Ponce presented by Nguyen in [15]) of a family of radial non-increasing mollifiersρand a function fW1,1(0,1)for which

lim0

1

0

1

0

|f(x)f(y)|q

|xy|q ρ(xy)d y 1q

d x= +∞

for anyq>1. In particular, this shows the restrictionp>1 in Theorem1.9is necessary. It would be interesting to understand whether for 1< p<Nthe assumption thatpq< pis also necessary or an artifact of the proof.

The plan of the paper is as follows. In Sect.2we review our notation and recall some lemmata regarding weakly differentiable functions. In Sect.3we restrict our attention to mollification by the characteristic function, completing the proofs of Theorems1.3,1.4, and 1.5announced in [11]. We also prove Theorem1.6. In Sect.4we treat the case of general radial non-increasing mollifiers and prove the main results from Sect.1.2. Finally, in Sect.5we treat the case of non-smooth domains in relation to the works [9,10]. Here we substantiate a claim in the paper [9], provided one is willing restrict oneself to radial non-increasing mollifiers (or mollifiers that admit a family of radial non-increasing majorants—see Sect.5).

2 Preliminaries

In what follows for 1≤ p<N we denote by p= N p

Np

the Sobolev critical exponent and formally takep= +∞ifp>N. We use the notation

B(x,r)f(y)d y:= 1

|B(x,r)|

B(x,r) f(y)d y

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to denote the average value of the function f over the open ball centered atxand of radius r, which we sometimes will shorten to

f, when the set of integration is implied by the context.

We utilizeSN−1for the unit sphere inRNandHN−1for the(N−1)-dimensional Hausdorff measure.

For fWloc1,p(RN)we write∇f for the distributional gradient of f, while for fB Vloc(RN)we writeD f. Let us recall thatD f admits a decompositionD f = ∇fLN+Dsf, where we utilize with an abuse of notation ∇fL1loc(RN;RN) to denote the Radon–

Nikodym derivative of D f with respect to the Lebesgue measure and Dsf its singular measure (DsfLN).

We utilize the notation

M(g)(x):=sup

t>0

B(x,t)|g(y)|d y,

to denote the Hardy–Littlewood maximal function.

We denote byC a constant which may depend on the dimension N and the parameters p,q, though whose precise value may change from line to line.

Let us here record some inequalities that will be useful in the sequel. The first lemma is a Sobolev–Poincaré inequality for Sobolev functions on balls, a proof of which can be found as Theorem 2 on page 141 of [8].

Lemma 2.1 Let1≤p<N . Then there exists a constant C=C(N,p) >0such that

B(x,r)|f(y)

f|p d y 1

p

Cr

B(x,r)|∇f(y)|pd y 1

p ,

for all B(x,r)⊂RN and fW1,p(B(x,r)).

Essentially the same proof gives the following analogous result for functions of bounded variation (which is Theorem 1 on page 189 of [8]).

Lemma 2.2 There exists a constant C=C(N) >0such that

B(x,r)|f(y)

f|1d y 1

1

Cr|D f|(B(x,r))

rN .

for all B(x,r)⊂RN and fB Vloc(RN).

We prove the following

Lemma 2.3 Suppose fWloc1,p(RN)for some1≤p<∞, and that1≤q<+∞is such that pqp. Then there exists a C=C(p,q,N) >0such that for all t>0

1 tN+pq

B(0,t)|f(x+h)f(x)− ∇f(x)·h|pq dh

C

B(0,t)|∇f(x+h)− ∇f(x)|s dh pq

s

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+C 1

t

B(0,t)|f(x+z)f(x)− ∇f(x)·z|d z pq

, where1≤sp is such that s=pq.

Proof We begin with the estimate 1

tN+pq

B(0,t)|f(x+h)f(x)− ∇f(x)·h|pqdh

C tN+pq

B(0,t)|f(x+h)

f − ∇f(x)·h|pqdh

+ C tN+pq

B(0,t)|

B(0,t)f(x+z)f(x)− ∇f(x)·z d z|pq dh where we have added and subtracted

f(x+z)d z(where the integral is taken overB(0,t)) and used the fact that

f(x)·z d z=0. The second term agrees with what we aim to show in this lemma, so it remains to show that

1 tN+pq

B(0,t)|f(x+h)

f − ∇f(x)·h|pqdh

C

B(0,t)|∇f(x+h)− ∇f(x)|s dh pq

s

and the result is demonstrated. However, utilizing the fact that 1 ≤ sp, we have that fWloc1,s(RN), and so applying Lemma2.1to

v(h):= f(x+h)

f − ∇f(x)·h

(note that fWloc1,s(RN)impliesvW1,s(B(0,R))for every 0<R<∞) we obtain

B(0,t)|f(x+h)

f − ∇f(x)·h|pq dh

C

B(0,t)|∇f(x+h)− ∇f(x)|s dh pq

s ,

since

v=0 and∇v(h)= ∇f(x+h)− ∇f(x). Then dividing bytN+pq, we obtain the

desired inequality.

Analogously we have

Lemma 2.4 Suppose fB Vloc(RN)that1≤q≤1. Then there exists a C=C(q,N) >

0such that for all t>0 1 tN+q

B(0,t)|f(x+h)f(x)− ∇f(x)·h|q dh

C

B(0,t)|∇f(x+h)− ∇f(x)|dh+ |Dsf|(B(0,t)) q

+C 1

t

B(0,t)|f(x+z)f(x)− ∇f(x)·z|d z q

.

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Proof As before 1 tN+q

B(0,t)|f(x+h)f(x)− ∇f(x)·h|q dh

C tN+q

B(0,t)|f(x+h)

f − ∇f(x)·h|q dh

+ C tN+q

B(0,t)|

B(0,t)f(x+z)f(x)− ∇f(x)·z d z|q dh,

though here instead we have the estimate 1

tN+q

B(0,t)|f(x+h)

f − ∇f(x)·h|q dh

= C tq

B(0,t)|f(x+h)

f − ∇f(x)·h|qdh

C tq

B(0,t)|f(x+h)

f − ∇f(x)·h|1dh q

1

= C

t1

B(0,t)|f(x+h)

f − ∇f(x)·h|1 dh q

1

. Now, applying Lemma2.2tov(h):= f(x+h)

f − ∇f(x)·h, we have C

t1

B(0,t)|f(x+h)

f − ∇f(x)·h|1dh 1

1

C

B(0,t)|∇f(x+h)− ∇f(x)|d x+ |Dsf|(B(0,t)),

and this implies the desired result.

Finally, whenp> N we have Morrey’s inequality for Sobolev functions with a precise estimate for the exponent of Hölder continuity as given in the following Lemma (which is stated and proved as Theorem 3 on page 189 of [8]).

Lemma 2.5 Let N <p<+∞. There exists a C=C(p,N) >0such that

|f(z)f(y)| ≤Cr

B(x,r)|∇f(w)|pdw 1p

for all B(x,r)⊂RN, fW1,p(B(x,r)), andLN almost every y,zB(x,r).

3 Lp-Taylor approximations andW1,p

Let us recall that in [11] we gave a proof of Theorem1.3in the regime 1≤p<N, Theorem 1.4and the necessity of fB V(RN)supposing that the lim sup is bounded in Theorem 1.5. Therefore we here complete the arguments to Theorem1.3in the regime pN and Theorem1.5. We also prove Theorem1.6.

We begin with the proof of Theorem1.3in the regimepN.

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Proof LetpN and fW1,p(RN). Ifq <+∞, then the result follows by exactly the same argument in [11] observing that although Lemma2.3was only stated for p < N in [11], we here proved it for all 1≤p<+∞and any 1≤q<+∞. Thus it remains to treat the caseq= +∞. The estimate for Morrey’s inequality given in Lemma2.5implies that for anyN <s< pone has

|f(x+h)f(x)− ∇f(x)·h|s

|h|sC

B(x,|h|)|∇f(z)− ∇f(x)|sd z

and so sup

hB(0,)

|f(x+h)f(x)− ∇f(x)·h|p

|h|pC sup

hB(0,)

B(x,|h|)|∇f(z)− ∇f(x)|s d z ps

.

Now, the right hand side tends to zero pointwise as→0, while sup

h∈B(0,)

B(x,|h|)|∇f(z)− ∇f(x)|s d z p

s(M(|∇f|s)(x))ps + |∇f(x)|p,

and so the result follows from Lebesgue’s dominated convergence theorem and the bound- edness ofM:Lr(RN)Lr(RN)for all 1<r≤ +∞

We now give a proof of Theorem1.5, arguing as in [11], mutatis mutandis.

Proof As argued in [11], the finiteness of the limit implies fB V(RN), so it suffices to show that for fB V(RN)we can find a bound for the limit.

For any 0< <1, we expand the integrand on concentric rings

B(0,)

|f(x+h)f(x)− ∇f(x)·h|q

|h|q dh

= i=0

1 N|B(0,1)|

B(0, 2i)\B(0,

2i+1)

|f(x+h)f(x)− ∇f(x)·h|q

|h|q dh.

We now make estimates fori∈Nfixed. We have 1

N

B(0, 2i)\B(0,

2i+1)

|f(x+h)f(x)− ∇f(x)·h|q

|h|q dh

≤ 1 N

2i+1

q

B(0,2i)\B(0,2i+1 )|f(x+h)f(x)− ∇f(x)·h|q dh

≤ 2q 2i N

2i

Nq

B(0,

2i)|f(x+h)f(x)− ∇f(x)·h|q dh.

Here, in place of Lemma 2.3we utilize Lemma2.4to deduce that 2i

N−q

B(0,

2i)|f(x+h)f(x)− ∇f(x)·h|q dh

C

B(0,

2i)|∇f(x+h)− ∇f(x)|p dh+ 2i

N

|Dsf|(B(x, /2i)) q

+C

1 0

B(0,t

2i)|∇f(x+t z)− ∇f(x)|d z+ 2i

t N

|Dsf|(B(x,t/2i))dt q

.

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Here we have used the estimate

B(0,

2i)|f(x+z)f(x)− ∇f(x)·z| d z

1

0

B(0,t

2i)|∇f(x+t z)− ∇f(x)|d z+ + 2i

t N

|Dsf|(B(x,t/2i))dt for the second term of Lemma2.4, whose argument is almost identical to the one used in the upper bound in the proof of Theorem1.6(and is originally due to Ponce [14], p. 248).

Therefore, summing iniand applying the basic inequality

i|ai|q1

i|ai|q1 (which follows from subadditivity of the functionss1q), we have

B(0,)

|f(x+h)f(x)− ∇f(x)·h|q

|h|q dh

1q

C i=0

1 2i

N/q

B(0,

2i)|∇f(x+h)− ∇f(x)|dh+ 2i

N

|Dsf|(B(x, /2i)) +C

i=0

1 2i

N/q 1

0

B(0,t

2i)|∇f(x+t z)− ∇f(x)|d z +

2i t

N

|Dsf|(B(x,t/2i))dt.

Integrating the preceding inequality overx ∈RN and making use of Tonelli’s theorem we obtain

RN

B(0,)

|f(x+h)f(x)− ∇f(x)·h|q

|h|q dh

1

q

d x

C i=0

1 2i

N/q

B(0, 2i)

RN|∇f(x+h)− ∇f(x)|d xdh +

2i

N

|Dsf|(B(x, /2i))d x

+C i=0

1 2i

N/q 1

0

B(0,t 2i)

RN|∇f(x+t z)− ∇f(x)|d z +

RN

2i t

N

|Dsf|(B(x,t/2i))d x

dt.

However, ifh,zB(0, )andt(0,1)we have max

RN|∇f(x+h)− ∇f(x)|d x,

RN|∇f(x+t z)− ∇f(x)|d x

≤ sup

w∈B(0,)

RN|∇f(x+w)− ∇f(x)|d x,

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and observe that this bound is independent ofi∈N. Thus,

RN

B(0,)

|f(x+h)f(x)− ∇f(x)·h|q

|h|q dh

1

q

d x

C i=0

1 2i

N/q

sup

w∈B(0,)

RN|∇f(x+w)− ∇f(x)|d x +C

i=0

1 2i

N/q

RN

2i

N

|Dsf|(B(x, /2i))d x

+ 1

0

RN

2i t

N

|Dsf|(B(x,t/2i))d xdt

. Finally we observe that

1

0

RN

2i t

N

|Dsf|(B(x,t/2i))d xdt

= 1

0

2i t

N

B(0,t 2i)

RN d|Dsf|(xy)d ydt

= |Dsf|(RN), while a similar argument shows

RN

2i

N

|Dsf|(B(x, /2i))d x= |Dsf|(RN), and these equalities hold for alli∈N.

Thus, as the infinite series is summable, sending→0 and using continuity of translation inL1(RN)we obtain

→0lim

RN

B(0,)

|f(x+h)f(x)− ∇f(x)·h|q

|h|q dh

1

q

d xC|Dsf|(RN).

We now calculate the explicit limit of theL1-Taylor approximation for a function fB V(RN), proving the claim of Theorem1.6. Observe here that the fact thatq=1 means we do not need to use the Sobolev embedding theorem and therefore the computation is cleaner.

Proof We first argue the upper bound lim sup

→0

RN

B(0,)

|f(x+h)f(x)− ∇f(x)·h|

|h| dhd xK1,N|Dsf|(RN) (3.1) FixψCc(B(0,1))radial, non-negative and

ψ=1 and defineψδ(x):=δ1Nψ(xδ). For fB V(RN)we denote by fδthe convolution fψδ. Then ifD f is the measure derivative of f, one hasD fδ=(∇f)δ+(Dsf)δ, and so the triangle inequality and Tonelli’s theorem imply

RN

B(0,)

|fδ(x+h)fδ(x)(∇f)δ(x)·h|

|h| dhd x

(13)

1

0

RN

B(0,)|(∇fδ(x+sh)(∇f)δ(x))· h

|h||dhd xds

1

0

RN

B(0,)|(∇f)δ(x+sh)(∇f)δ(x)|dhd xds

+ 1

0

RN

B(0,)

(Dsf)δ(x+sh)· h

|h|

dhd xds

= 1

0

B(0,)

RN|(∇f)δ(x+sh)− ∇fδ(x)|dhd xds +

B(0,)

RN

(Dsf)δ(y)· h

|h|

d ydh. Now

B(0,)

RN

(Dsf)δ(y)· h

|h| d ydh

= 1

N|B(0,1)|

0

B(0,t)

RN

(Dsf)δ(y)·σ d ydHN1(σ )dt

= 1

N|B(0,1)|

0

B(0,t)

RN|(Dsf)δ(y)·σ|d ydHN−1(σ )dt

= 1

N|B(0,1)|

0

tN1dt

SN−1

RN|(Dsf)δ(y)·σ|d ydHN1(σ )

=K1,N|(Dsf)δ|(RN) for

K1,N =

SN−1|e1·σ|dHN−1(σ )

as in Sect.1.2. Therefore sendingδ →0+, Fatou’s lemma, Lebesgue’s dominated conver- gence theorem, the strict convergence of the measures(Dsf)δDsf yields

RN

B(0,)

|f(x+h)f(x)− ∇f(x)·h|

|h| dhd x

1

0

B(0,)

RN|∇f(x+sh)− ∇f(x)|d xdhds+K1,N|Dsf|(RN) Now taking the limsup as →0 the first term vanishes as argued in the previous theorems (by continuity of translation onL1(RN)), and we thus obtain (3.1).

To prove the lower bound, we simply estimate

RN

B(0,)

|f(x+h)f(x)|

|h| dhd xK1,N

RN|∇f(y)|d y

=

RN

B(0,)

|f(x+h)f(x)|

|h| dhd x

B(0,)

RN

f(y)· h

|h| d ydh

RN

B(0,)

|f(x+h)f(x)− ∇f(x)·h|

|h| dhd x,

(14)

and taking the liminf as→0, an application of the result of Dávila [7] that

lim0

RN

B(0,)

|f(x+h)f(x)|

|h| dhd x=K1,N|D f|(RN), and the decomposition

|D f|(RN)= |Dsf|(RN)+

RN|∇f(y)|d y

yields the desired lower bound.

4 General mollifiers

We will here give proofs of the results asserted in Sect.1.2. We begin with Theorem1.7.

Proof of Theorem 1.7 We will show that

→0lim

B(0,η)

|f(x+h)f(x)− ∇f(x)·h|pq

|h|pq ρ(h)dh 1

pq =0

forp-Lebesgue points off, and henceLN almost everyx ∈RN. Let us first recall that as a monotone decreasing function of|h|,ρhas at most countably many jump discontinuities, and possesses inner and outer limits for every value of|h|, and therefore its suffices to prove the result in the case whereρis inner continuous (which always dominatesρ).

In order to apply Lemma2.3, we expand the desired quantity on concentric rings to obtain

B(0,η)

|f(x+h)f(x)− ∇f(x)·h|pq

|h|pq ρ(h)dh

= i=0

B(0,2ηi)\B(0,2iη+1)

|f(x+h)f(x)− ∇f(x)·h|pq

|h|pq ρ(h)dh

i=0

ρ

η 2i+1

η 2i+1

pq

B(0,2ηi)|f(x+h)f(x)− ∇f(x)·h|pq dh

=2pq+2N i=0

ρ η 2i+1

η 2i+2

Nη 2i

pq−N

×

B(0,2ηi)|f(x+h)f(x)− ∇f(x)·h|pqdh.

Then applying the estimate from Lemma2.3, we have

B(0,η)

|f(x+h)f(x)− ∇f(x)·h|pq

|h|pq ρ(h)dh (4.1)

C i=0

ρ

η 2i+1

η 2i+2

N

max

F1i(x),F2i(x)

, (4.2)

where

F1i(x):= −

B(0,η

2i)|∇f(x+h)− ∇f(x)|s dh pq

s

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