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Differential

of

metric

valued

Sobolev

maps

Nicola Giglia,∗, Enrico Pasqualettob,Elefterios Soultanisc

aSISSA,ViaBonomea265,34136Trieste,Italy

bUniversityofJyväskylä,POBox35,FI-40014Jyväskylä,Finland

cUniversityofFribourg,Av.del’Europe20,CH-1700Fribourg,Switzerland

Keywords:

Functionspaces Metricmeasurespaces Sobolevspaces

WeintroduceanotionofdifferentialofaSobolevmapbetween metric spaces. Thedifferential isgiven intheframework of tangent and cotangent modules of metric measure spaces, developed by the first author. We prove that our notion is consistent with Kirchheim’s metric differential when the sourceisaEuclideanspace,andwiththeabstractdifferential provided by the first author when the target is R. We also show compatibility with the concept of co-local weak differential introducedbyConventandVanSchaftingen.

Contents

1. Introductionandmainresults . . . 2

2. Preliminaries . . . 4

3. Differentialofmetric-valuedSobolevmaps . . . 7

4. Consistencywithpreviouslyknownnotions . . . 10

4.1. ThecaseY=R . . . 10

4.2. Thecaseu ofboundeddeformation . . . 12

4.3. ThecaseX=Rd andu Lipschitz . . . 15

4.4. Thecaseofsmoothspacesandco-localweakdifferential . . . 16

ThankstoMIURSIR-grant‘NonsmoothDifferentialGeometry’(RBSI147UG4).

* Correspondingauthor.

E-mailaddresses:[email protected](N. Gigli),enpasqua@jyu.fi(E. Pasqualetto),

[email protected](E. Soultanis).

http://doc.rero.ch

Published in "Journal of Functional Analysis 278(6): 108403, 2020"

which should be cited to refer to this work.

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5. DifferentialoflocallySobolevmapsbetweenmetricspaces . . . 19

5.1. Inverselimitsofmodules . . . 19

5.2. LocallySobolevmapsandtheirdifferential . . . 21

References . . . 23

1. Introductionandmainresults

Background and setting The concept of real valued Sobolev functions defined on a metric measure space (X,dX,mX) is by now well understood. Given an exponent p∈

[1,∞) the space of functionsf : X → R having ‘distributionaldifferential inLp(X) in

a suitable sense’ is denoted by Sp(X). To each f ∈ Sp(X) one associates the function

|Df|∈ Lp(X),calledminimalweakuppergradient,whichinthesmoothsettingcoincides

with themodulusofthedistributionaldifferential(see [6] and [18],[4]).

Inspired by the work of Weaver [20], in [9] the first author built the theory of

Lp-normed modules and gave a notion of differential df for maps f ∈ Sp(X) in that

framework:bydefinition,df isanelementofthesocalledcotangent Lp-normedmodule

Lp(TX) andhastheproperty thatitspointwisenormcoincidesm

X-a.e.with|Df|. We

remark thatthelinearstructure ofthespace Sp(X),aconsequenceof thefactthatthe target spaceR isavectorspace,plays akeyroleintheconstruction.

Wenowturn tothecaseofmetric-valuedSobolevmaps. Let(X,dX,mX) beametric

measure spaceasbeforeandlet(Y,dY) beametricspacewhichshallbeassumedtobe

completeandseparable.Weshallalsofixp= 2 forsimplicity.Therearevariouspossible definitionsoftheconceptofSobolevmapsfromX toY;hereweshallworkwiththeone based on post-composition (see [13] for historical remarks): we say thatf ∈ S2(X;Y)

providedthereisG∈ L2(X) suchthatforanyϕ: Y→ R Lipschitzwehaveϕ◦f ∈ S2(X)

with

|D(ϕ ◦ f)| ≤ Lip(ϕ) G mX− a.e.

The least such G isthen denoted |Df| andcalled theminimal weak upper gradient of

themap f.NoticethatsinceY hasnolinearstructure,theset S2(X;Y) isnotavector

space ingeneral.

Thequestionwe addressinthispaper isthefollowing:inanalogy withthefactthat

‘behind’ the minimal weak upper gradient |Df| of areal-valued Sobolevmap there is

an abstract differential df,does there exist a notion of differential fora metric-valued Sobolevmap?

Before turningto the(positive) answerto thisquestion,letus motivateour interest inthe problem,whichgoes beyondthe meredesireof generalization.In thecelebrated

paper [7], Eells and Sampson proved Lipschitz regularity for harmonic maps between

RiemannianmanifoldswhenthetargetN hasnon-positivecurvatureandissimply

con-nected,andtheLipschitzestimateisgivenintermsofalowerRiccicurvatureboundand

anupper dimensionboundonthesourcemanifoldM. Akeypoint intheirproof isthe

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establishmentof the now-called Bochner-Eells-Sampsonformula for maps f : M → N whichweshallwriteas

Δ|df|

2

2 ≥ ∇f(Δf) + K|df|

2, (1.1)

where |df| is the Hilbert-Schmidt norm of the differential of f and K ∈ R is alower

boundfortheRiccicurvatureofM (letusremainvagueaboutthemeaningof∇f(Δf)).

Adirectconsequenceof(1.1) isthatiff isharmonic,then

Δ|df|

2

2 ≥ K|df|

2. (1.2)

This bound and Moser’s iteration technique are sufficient to show that |df| is locally

bounded fromaboveinthe domain ofdefinition off, thus showingthe local Lipschitz

regularity of f (the upper dimension bound for M enters into play in the constants

appearinginMoser’sargument).

SincetheLipschitzregularityofharmonicfunctionsdoesnotdepend onthe

smooth-nessofM andN but onlyinthe statedcurvaturebounds, itisnaturalto askwhether thesameresultsholdassumingonlytheappropriatecurvatureboundsonthesourceand

target space, without any reference to smoothness. Efforts in this direction have been

madeby Gromov-Schoenin[12], by Korevaar-Shoenin[15] andbyZhang-Zhu in[21]. Themostgeneralresultisin[21], where theauthorsconsider thecaseofsource spaces

whicharefinite-dimensionalAlexandrovspaceswith(sectional)curvatureboundedfrom

belowandtargetswhichare CAT(0) spaces.Still,givenEells-Sampson’sresultthe

nat-uralsyntheticsettingappearstobethatofmapsfromaRCD(K,N) spaceto aCAT(0)

space;asoftoday,thisappearstobeoutofreach.Letusremarkthatinnoneofthese3 papershasinequality(1.1) been writtendownexplicitly; in[15] and[21] “only”aform of(1.2) forharmonicmapshasbeen established(in[12] theargumentwasdifferentand

basedonAlmgren’s frequencyfunction).

Thepresentmanuscriptaimsatbeingafirststepinthedirectionofobtaining(1.1) for mapsfromRCD spacestoCAT(0) ones(seealso[11]):ifsuccessful,thisresearchproject easilyimplies thedesiredLipschitz regularityfor harmonicmapsand at thesametime

improves the understandingof the subject even inpreviously studiednon-smooth

set-tings.Theoverallprogramisdefinitelyambitious,butwebelievethatevenintermediate stepslikethecurrentmanuscripthaveanintrinsicinterest:seeinparticularthe‘review’ ofKirchheim’snotionofmetricdifferential inSection4.3.

Theveryfirststeptotackleinordertowritedown(1.1) isto understandwhat“df” is. As stated, this is our goal in this manuscript. Let us informally describe the key conceptinthis work(theprecisedefinitionswillbe giveninSections 2and 3).

Differential of Sobolev maps Given a Sobolev map u ∈ S2(X;Y) between a metric

measurespace(X,dX,m) andacompleteseparablemetricspace(Y,dY),weconsiderthe

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metricmeasurespace(Y,dY,μ),whereμ:=u∗(|Du|2m).Thenwedefinethedifferential

du ofu asanoperator

du : L0(T X) → (u∗L0μ(T∗Y)) satisfying

u∗df, du(V ) = V (d(f ◦ u)) m-a.e. (1.3)

foreveryf ∈ S2(Y,d

Y,μ) and V ∈ L0(T X) (Definition3.4).

Theparticular choiceofmeasure μ isimportant:it ensuresthatfor f ∈ S2(Y,dY,μ)

thepullbackfunctionu∗f := f ◦ u belongsto S2(X,d

X,m) with

|D(f ◦ u)| ≤ |Df| ◦ u |Du|, (1.4) see Proposition3.3fortheprecise formulation.Once thisisestablished, thedifferential of u canbe definedby taking theappropriate adjointof themap df → d(f ◦ u), as in (1.3). Let us emphasise thatonthe right handside of the crucial bound (1.4) thereis theproduct oftwo‘weak’objects:thismakestheinequalitynon-trivial.

Once the definition is given we verify that it is compatible, and thus generalizes,

previouslyexistingnotionsofdifferentialsinthenon-smoothsetting. Allourdiscussion

is made for the Sobolev exponent p = 2, but obvious modifications generalise all the

resultsto thecasep∈ (1,∞). 2. Preliminaries

To keep the presentation short we assume the reader is familiar with the concept

of Sobolev functions on a metric measure space ([6], [18], [4], [3]) and with that of

L0-normed modulesanddifferentialsofrealvaluedSobolevmaps([9],[8]).

Hereweonlyrecallthoseconceptsweshallusemostfrequently.Letusfixacomplete, separablemetricspace(X,dX) andanon-negativeandnon-zeroRadonmeasurem giving

finite mass to boundedsets. We shalldenote by Lip(f) the (global)Lipschitz constant of afunction,byLIP(X),LIPbs(X),LIPbd(X) thespace ofLipschitzfunctions,Lipschitz

functions with bounded support, and functions which are Lipschitz on bounded sets,

respectively.Wealso denotebylipa(f): X→ [0,∞] theasymptotic Lipschitzconstant,

definedby

lipa(f)(x) := lim

y,z→x

|f(y) − f(z)|

dX(y, z)

ifx is not isolated, 0 otherwise.

Then wedefine:

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Definition 2.1 (The Sobolev class S2(X)).We say that f ∈ S2(X) provided there is a

functionG∈ L2(m) andasequence(f

n)⊂ LIPbd(X) convergingtof inL0(m) suchthat

(lipa(fn)) weaklyconvergesto G inL2(m).

Withrespecttotheapproachin[4], [3] herethedifferenceis inthetopologyusedin therelaxationprocedure.Thefactthatourapproachisequivalent totheonein[4],[3] follows fromthe L0-stability ofweak uppergradients grantedbytheapproach viatest

plansinconjunctionwithacut-offargument.

For f ∈ S2(X) we recall that there is a minimal, in the m-a.e. sense, non-negative

functionG∈ L2(m) forwhichthe situationinDefinition2.1occurs.Such G isdenoted

|Df| andcalled minimalweakuppergradient.It istheneasytocheck that:

∀f ∈ S2(X) there is (f

n)⊂ LIPbd(X)m − a.e. converging to f such that

lipa(fn)→ |Df| in L2(m). (2.1)

Fromtheminimalweak uppergradientsonecan ‘extract’anotionofdifferential:

Theorem2.2(Cotangentmoduleanddifferential). Withtheabove notationand

assump-tions, there isaunique (up tounique isomorphism)couple (L0(TX),d) with L0(TX)

beinga L0(m) normed module, d: S2(X)→ L0(TX) linear andsuchthat: |df|=|Df|

m-a.e.forevery f ∈ S2(X) and{df : f ∈ S2(X)} generatesL0(TX).

When we want to emphasise the role of the chosen measure, we shall write

(L0m(T∗X),dm) inplaceof(L0(T∗X),d).Amongthevariouspropertiesofthedifferential, weshallfrequentlyuseitslocality:

df = dg m − a.e. on {f = g}, ∀f, g ∈ S2(X). Letusnowrecallfewfactsaboutpullback ofmodules:

Theorem2.3(Pullback).Let(X,dX,mX),(Y,dY,mY) bemetricmeasurespacesasabove,

u : X → Y such that umX  mY and M an L0(mY)-normed module. Then

there is a unique (up to unique isomorphism) couple (u∗M,[u∗]) such that u∗M is a L0(mX)-normed module and [u∗] : M → u∗M is linear, continuous and such that

|[u∗v]|=|v|◦ u m

X-a.e. foreveryv ∈M and {[u∗v]:v ∈M} generates u∗M.

Themoduleu∗M iscalledthepullbackmoduleand[u∗] thepullbackmap.Itcanbe

directlychecked bytheuniquenesspartofTheorem 2.3that

if umX mY then u∗L0(mY)∼ L0(mX) via the map [u∗f] → f ◦ u. (2.2)

Thepullbackhasthefollowing universalproperty,whichweshallfrequentlyuse:

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Proposition 2.4 (Universal property of the pullback).With the same notation and assumptions as in Theorem 2.3 above, let V ⊂ M a generating subspace, N a L0(m

X)-normed module and T : V → N a linear map such that |T (v)| ≤ f|v|◦ u

mX-a.e. ∀v ∈ V for some f ∈ L0(mX). Then there exists a unique L0(mX)-linear and

continuousmapT : u˜ ∗M →N suchthat T ([u˜ ∗v])=T (v) foreveryv ∈ V andthismap satisfies

| ˜T (w)| ≤ f|w| mX− a.e. ∀w ∈ u∗M. (2.3)

Inparticular,ifT :M1→M2isaL0(mY)-linearandcontinuousmapsatisfying|T (v)|≤

g|v| mY-a.e. ∀v ∈M1,forsome g ∈ L0(mY), applying theabove tothemapM1  v →

[u∗T (v)] ∈ u∗M2 we deduce that there exists a unique L0(mX)-linear and continuous

mapu∗T : u∗M1→ u∗M2 makingthediagram

M1 M2 u∗M 1 u∗M2 T [u∗] [u∗] u∗T

commute andsuchmapsatisfies

|u∗T (w)| ≤ g ◦ u|w| m

X− a.e. ∀w ∈ u∗M1. (2.4)

Thesepropertiesofpullbackshavebeenstudiedin[9],[8] formapssatisfyingumX

CmY, butifoneisonly interestedinL0-modulesthetheorems aboveareeasilyseento

hold withsmallmodifications.

Finally, letus presentasimpleconstructionthatweshallfrequentlyuse. LetE ⊂ X beBorel,putν := m|

E andletM beaL

0(ν)-normedmodule.Tosuchamodulewecan

canonically associate aL0(m)-normed module, called extension of M and denoted by

Ext(M),inthefollowingway.Firstofallwenoticethatwehaveanatural projection/re-striction operatorproj :L0(m)→ L0(ν) givenbypassagetothequotientuptoequality

ν-a.e.andanatural‘extension’operatorext :L0(ν)→ L0(m) which sendsf ∈ L0(ν) to

thefunctionequaltof m-a.e.onE andto0 onX\ E.ThenforagenericL0(ν)-normed

moduleM weputExt(M):=M asaset,multiplicationof v ∈ Ext(M) byf ∈ L0(m) is definedas proj(f)v ∈M = Ext(M) andthepointwise normasext(|v|)∈ L0(m).We

shall denotebyext :M → Ext(M) theidentitymap andnoticethatinarathertrivial

way wehave

Ext(M∗)∼ Ext(M) via the coupling ext(L)ext(v):= ext(L(v)). (2.5) Inwhatfollowsweshallalwaysimplicitlymakethis identification.

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3. Differentialofmetric-valuedSobolevmaps

Throughoutthismanuscript(X,dX,m) willalwaysdenoteacompleteseparablemetric

space endowed with a non-negative and non-zero Radon measure which is finite on

boundedsets; (Y,dY) denotesacompleteseparablemetricspace.

Definition3.1(MetricvaluedSobolevmap).ThesetS2(X,Y) isthecollectionofallBorel mapsu: X→ Y for whichthere isG∈ L2(X,m),G≥ 0 suchthatforany f ∈ LIP(Y)

itholdsf ◦ u∈ S2(X) and

|d(f ◦ u)| ≤ Lip(f)G m − a.e. (3.1) Theleast,inthem-a.e.sense,functionG forwhichtheaboveholdswillbedenoted|Du|. Noticethatforu∈ S2(X,Y) theclassof G∈ L2(X) for which(3.1) holdsis aclosed lattice,henceam-a.e.minimaloneexistsandthedefinitionof|Du| iswellposed.

OurstudyoffunctionsinS2(X,Y) begins withthefollowingbasiclemma:

Lemma3.2. Letu∈ S2(X,Y) andf ∈ LIP(Y).Thenf ◦ u∈ S2(X) with

|d(f ◦ u)| ≤ lipa(f) ◦ u |Du| m − a.e. (3.2)

Proof. Let (yn) ⊂ Y be countableand dense and for r ∈ Q, r > 0, letfr,n ∈ LIP(Y)

beaMcShaneextensionof f|

Br(yn), i.e.aLipschitzmap definedonthe wholeY which

coincides with f on Br(yn) and such that Lip(fr,n) = Lip(f|B

r(yn)). Then from (3.1)

andthelocalityofthedifferentialweseethat

|d(f ◦ u)| ≤ Lip(f|Br(yn))|Du| m − a.e. on u

−1(B

r(yn)).

Since for every y ∈ Y we have lipa(f)(y) = inf Lip(f|

Br(yn)), where the inf is taken

amongalln,r suchthaty ∈ Br(yn),theconclusionfollows. 2

Letusfixu∈ S2(X,Y) andequip thetarget spaceY withthefinite Radonmeasure

μ := u(|Du|2m).

Noticethatforf ∈ L0(Y,μ) thefunctionf ◦u isnotwell-defineduptoequalitym-a.e.in

thesensethatiff = ˜f μ-a.e.,thennotnecessarilyf ◦ u= ˜f ◦ u m-a.e. Still,wecertainly havef ◦u= ˜f ◦u m-a.e.on{|Du|> 0} andforthisreasonwehavef ◦u|Du|= ˜f ◦u|Du| m-a.e.,i.e.themap f → f ◦ u|Du| iswelldefinedfromL0(Y,μ) toL0(X,m).Thenthe

identity f ◦ u|Du|2dm=|f|2dμ showsthat

L2(Y, μ)  f → f ◦ u |Du| ∈ L2(X, m) is linear and continuous. (3.3)

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Wenow turntoourkeybasicresultaboutpullbackof Sobolevfunctions: Proposition 3.3. Letu∈ S2(X,Y),put μ:=u

(|Du|2m) andlet f ∈ S2(Y,dY,μ). Then

there isg ∈ S2(X) suchthat g = f ◦ u m-a.e. on{|Du|> 0} and

|dg| ≤ |dμf| ◦ u|Du| m − a.e. (3.4)

Moreprecisely,there isg ∈ S2(X) andasequence(f

n)⊂ LIPbd(Y) suchthat

fn → f μ − a.e. lipa(fn) → |dμf| inL2(μ),

fn◦ u → g m − a.e. lipa(fn)◦ u|Du| → |dμf| ◦ u|Du| in L2(m).

(3.5)

Proof. Up to a truncation and diagonalization argument we can assume that f ∈

L∞(Y,μ). Then let (f

n) ⊂ LIPbd(Y) be as in (2.1) for f and observe that since f is

bounded,bytruncationwecanassumethefn’stobeuniformlybounded.Thusthefirst

twoconvergencesin(3.5) holdand,taking(3.3) intoaccountweseethatalsothelastin (3.5) holds.Now observe thatifwecan provethat(fn◦ u) hasalimitm-a.e.,call itg,

then (3.4) wouldfollowfromLemma3.2above,(3.3) andtheclosureofthedifferential. LetB ⊂ X beboundedandBorel.Thefunctionsfn◦ u areequiboundedandm(B)<

∞, hence(fn◦ u) is bounded in L2(B,m|B). Thus by passingto an appropriate - not

relabeled - sequence of convex combinations (which do not affect the already proven

convergences in(3.5))weobtainthat(fn◦ u) hasastronglimitinL2(B,m|B). Thusa

subsequenceconvergesm-a.e.onB andbyconsideringasequence(Bk) ofboundedsets

suchthatX=∪kBk,byadiagonalizationargumentweconcludetheproof. 2

Let us notice thatsince μ is afinite measure on Y we have LIP(Y)⊂ S2(Y,

dY,μ).

Also,

forf ∈ LIP(Y) and g ∈ S2(X) as in Proposition3.3we have d(f ◦ u) = dg. (3.6) Indeed,thelocalityofthedifferentialgivesd(f ◦ u)= dg on{|Du|> 0} andthebounds (3.2) and (3.4) give|d(f ◦ u)|=|dg|= 0m-a.e.on{|Du|= 0}.

Observe that for ν := m|

{|Du|>0} we have u∗ν  μ, thus u∗L0μ(T∗Y) is a well

de-fined L0(ν)-normed module.Recalling the‘extension’ functorintroduced at theend of

Section2,ourdefinitionofdu is:

Definition 3.4.Thedifferential du ofu∈ S2(X,Y) istheoperator du : L0(T X) → Ext(u∗L0μ(T∗Y)) given as follows. For v ∈ L0(T X), the object du(v) ∈ Ext(uL0

μ(T∗Y))



is charac-terized by the property: for every f ∈ S2(Y,d

Y,μ) and every g ∈ S2(X,dX,m) as in

Proposition3.3wehave

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ext[u∗dμf]



du(v)= dg(v) m − a.e. (3.7) Wenowverifythatthisisagooddefinitionandcheck theverybasicproperties: Proposition3.5(Wellposedness ofthedefinition).The differentialdu(v) ofu in Defini-tion3.4iswell-definedandthemapdu: L0(T X)→ Ext(u∗L0μ(T∗Y))isL0(m)-linear

andcontinuous.Moreover, itholdsthat

|du| = |Du| m − a.e. (3.8) Proof. Let f ∈ S2(Y,d

Y,μ) and observe that if g,g ∈ S2(X,dX,m) both satisfy the

propertieslisted inProposition 3.3 then the locality of the differential and the bound (3.4) show that dg = dg. Hence the right handside of (3.7) depends only on f,u,v. Thennoticethatagainthebound(3.4) gives

ext[u∗dμf]



du(v)(3.7)= |dg(v)| ≤ |dg| |v|(3.4)≤ |dμf|◦u|Du| |v| =ext



[u∗dμf]|Du||v|

andthusthearbitrarinessoff ∈ S2(Y,d

Y,μ),Proposition2.4andproperty(2.5) ensure

thatdu(v) is a well defined element of Ext(u∗L0

μ(T∗Y))  ∼ Ext(u∗L0 μ(T∗Y))  , as desired,with |du(v)| ≤ |Du| |v|. (3.9) Thefactthatdu(v) isL0(m)-linearinv istrivialandthebound(3.9) givesboth

continu-ityandtheinequality≤ in(3.8).Togettheotherinequalityletf : Y → R be1-Lipschitz and notice thatsinceμ(Y)< ∞ we alsohave f ∈ S2(Y,d

Y,μ). Since u∈ S2(X,Y) we

havef ◦ u∈ S2(X) andcanfindv ∈ L0(T X) suchthat

|v| = 1 and d(f ◦ u)(v) = |d(f ◦ u)| m-a.e. (3.10) (theexistenceofsuchv followsbyBanach-Alaoglu’stheorem,see[9,Corollary1.2.16]). Moreover,letg ∈ S2(X) beasinProposition3.3andnoticethat

|d(f ◦ u)|(3.10)= |d(f ◦ u)(v)|(3.6)= |dg(v)|

(3.7)

= ext[u∗dμf]



du(v) ≤ ext[u∗dμf]|du||v|

(3.10)

= |dμf| ◦ u |du| ≤ |du|,

havingusedthefactthatf is1-Lipschitzinthelast step.Bythearbitrarinessoff and theverydefinitionof|Du| giveninDefinition3.1,thisestablishes ≥ in(3.8). 2

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4. Consistencywithpreviouslyknownnotions

4.1. Thecase Y=R

InthissectionweassumeY=R andprovethatonceafewnaturalidentificationsare taken into account,thenewly defineddifferentialdu: L0(T X)→ ExtuL0

μ(T∗R)



is

‘thesame’astheonedefinedbyTheorem2.2,whichforthemomentweshalldenoteby

du∈ L0(TX).

To startwith, letus observethatdirectlyfromthedefinitionsandthechainrule d(f ◦ u) = f◦ u du m − a.e. ∀u ∈ S2(X), f ∈ C1∩ LIP(R) (4.1) (see [8, Corollary 2.2.8]), we have that the class S2(X,Y) coincides with S2(X) when

Y=R andthatthetwonotionsofminimalweak uppergradientscoincide.

For later use it will be convenient to consider the case where the target space is

a generic Riemannian manifold rather than R. Thus letN be acomplete Riemannian

manifold, dN the distance induced by the metric tensor and fix u ∈ S2(X,N). Also,

let μ beanon-negative Radonmeasure onN. Weshall denote byL0(N,TN;μ) (resp.

L0(N,T N;μ)) the L0(μ)-normed module of sections of the cotangent (resp. tangent)

bundleidentifieduptoequalityμ-a.e.(thenotationisunusual,buthopefullyhelps com-paringthese‘concrete’notionswiththemoreabstractoneswearediscussinghere).We shall insteaddenote byL0

μ(T∗N) (resp. L0μ(T N))thecotangent(resp. tangent) module

associated tothespace(N,dN,μ).

The nextresult hasbeen provedin [10] forthecase N=Rd and generalisedin[17]

to themanifoldcase:

Theorem 4.1. Let N be a complete Riemannian manifold and μ be a non-negative

Radon measure on it. Then there is a unique L0(μ)-linear and continuous map P :

L0(N,TN;μ)→ L0

μ(T∗N) suchthat

P (Df) = dμf ∀f ∈ C1(N), (4.2)

whereDf : N→ T∗N isthedifferentialoff.Itsadjointmapι:L0

μ(T N)→ L0(N,T N;μ)

is anisometry.In particular,L0

μ(T N) isseparable.

Let now u∈ S2(X,N), putμ:=u

(|du|2m) andconsider the L0(m)-normedmodule

Ext(u∗L0

μ(T∗N)).TheseparabilityofL0μ(T N) providedbyTheorem4.1above,the

char-acterisation of the dual of thepullback obtained in[8, Theorem 1.6.7] and(2.5) grant that

Ext(u∗L0μ(T N)) ∼ Ext(u∗L0μ(T∗N)) via the coupling

ext([u∗L])ext([u∗v]):= ext(L(v) ◦ u). (4.3)

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Hence in the present situation we shall think of du as a map from L0(T X) to

Ext(u∗L0

μ(T N)).

Now put ν := χ{|Du|>0}m as before and consider the L0(ν)-linear and continuous operators

u∗P : uL0(N, TN;μ) −→ uL0

μ(T∗N),

u∗ι : uL0

μ(T N) −→ u∗L0(N, T N; μ)

definedviatheuniversalproperty ofthepullbackmodulegiveninProposition2.4.It is thenclearthatu∗ι istheadjointofu∗P ,thusfrom(4.2) weseethat

[u∗Df]u∗ι(V )= [u∗dμf](V ) ν − a.e.

for everyV ∈ u∗L0μ(T N), f ∈ C1(N). (4.4)

Finally, noticing that ext : u∗L0

μ(T N) → Ext(u∗L0μ(T N)) is invertible, we define I :

Ext(u∗L0

μ(T N))→ Ext(u∗L0(N,T N;μ)) as

I := ext ◦ u∗ι ◦ ext−1. (4.5)

LetusnowconsiderthecaseN=R.InthiscasethecanonicalisomorphismTxR∼ R

valid forany x∈ R givesL0(R,T R;μ) ∼ L0(μ). With this identification and recalling

(2.2) andtheverydefinitionoftheextensionfunctorweseethatthemapI takesvalues inL0(m).Thenwehave:

Theorem4.2. Withtheabove notation andassumptionswehave |du|=|du| m-a.e. and

I(du(v)) = du(v) m − a.e. ∀v ∈ L0(T X). (4.6)

Proof. Theidentity |du|=|du| followsfrom(3.8) andthe alreadynoticedfactthatfor

u∈ S2(X)= S2(X,R) thetwo notionsofminimal weak uppergradientsunderlyingthe

twospacescoincide.

Weturnto(4.6).Forf ∈ C1

c(R) letusdenotebyDf : R→ R∗itsdifferentialandby

f:R→ R itsderivative.Clearly,uptoidentifyingR andRviatheRieszisomorphism

thesetwo objectscoincideandthuschecking firstthecaseh= [u∗g] weeasily getthat

f◦ u h = ext[uDf](h) m − a.e.

∀h ∈ Extu∗L0(μ)(2.2)∼ ExtL0(ν)⊂ L0(m). (4.7)

Thenforg asinProposition3.3we have

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f◦ u I(du(v))(4.7)

= ext[u∗Df] I(du(v))(4.5),(2.5)= ext[u∗Df]u∗ιext−1(du(v))

(4.4)

= ext[u∗dμf]



ext−1(du(v))(2.5)= ext([u∗dμf])(du(v))

(3.7)

= dg(v)

(3.6)

= d(f ◦ u)(v)(4.1)= f◦ u du(v). Since the space {f◦ u : f ∈ C1

c(R)} generates L0(m), this is sufficient to establish

(4.6). 2

4.2. Thecase u ofboundeddeformation

Inthissectionweshallassumethatalso(Y,dY) carriesanon-negativeRadonmeasure

mY which gives finite mass to bounded sets and study the differential of a map u

S2(X,Y) which is also of bounded deformation. Recall that the latter means that u is

Lipschitz andforsomeC > 0 itholdsumX≤ CmY, wherewe denotemX:=m forthe

sakeofclarity.Forsuchu itiseasyto provethat

f ∈ S2(Y) ⇒ f ◦ u ∈ S2(X) with |d(f ◦ u)| ≤ Lip(u)|df| ◦ u m

X− a.e.

Then a notion of differential ˆdu : L2(T X) uL2

mY(T∗Y)



can be defined by the

formula

[u∗dmYf](ˆdu(v)) := d(f ◦ u)(v) mX− a.e. ∀f ∈ S2(Y, dY, mY), v ∈ L2(T X), (4.8)

see [8,Proposition2.4.6]. Inthis sectionwe studythe relationbetweendˆu anddu. We start noticing thatthe definition of |Du| trivially gives |Du| ≤ Lip(u) mX-a.e., so we

have

μ = u(|Du|2mX)≤ Lip2(u)u∗mX≤ CLip2(u)mY. (4.9)

Also,letusprovethefollowinggeneralstatement:

Lemma4.3. Letμ12betwonon-negativeandnon-zeroRadonmeasuresonthecomplete

space (Y,dY) with μ1 ≤ μ2. Then S2(Y,dY2) ⊂ S2(Y,dY1) and there is aunique

L0(μ

2)-linear andcontinuousmapP : L0μ2(T∗Y)→ Ext(L 0

μ1(T∗Y)) suchthat

P (dμ2f) = ext(dμ1f) ∀f ∈ S2(Y, dY, μ2),

and itsatisfies|P (ω)|≤ |ω| μ2-a.e. forevery ω ∈ L0μ2(T∗Y),where here the‘extension’

operator actsfromL0(μ

1)- toL0(μ2)- normedmodules.

Proof. The assumption μ1 ≤ μ2 ensures that the topologies of L2(μ2),L0(μ2)

are stronger than those of L2(μ

1),L0(μ1) respectively. Thus both the inclusion

S2(Y,d

Y2) ⊂ S2(Y,dY1) and the bound ext(|dμ1f|) ≤ |dμ2f| μ2-a.e. for every

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f ∈ S2(Y,d

Y2) follow from Definition 2.1. To conclude apply, e.g., Proposition 2.4

withu:= Identity andT (dμ2f):= ext(dμ1f)∈ Ext(L0μ1(T∗Y)). 2

Applyingthislemmato thecaseunderconsiderationweget:

Proposition 4.4. Assume that u : X → Y is of bounded compression. Then with the

above notation there is a unique L0(m

Y)-linear and continuous map π : L0mY(T∗Y)

Ext(L0μ(T∗Y)) suchthatπ(dmYf)= ext(dμf) foreveryf ∈ S2(Y,dY,mY) (theextension

operatorbeingintendedfromL0(μ)- toL0(m

Y)- normedmodules)anditsatisfies|π(ω)|≤

|ω| mY-a.e.forevery ω ∈ L0mY(T∗Y).

Moreover,forany f ∈ S2(Y,d

Y,mY) andg ∈ S2(X) asin Proposition 3.3wehave

dg = d(f ◦ u). (4.10)

Proof. ThefirstpartofthestatementfollowsfromLemma4.3and(4.9).Toprove(4.10) notice thatthanksto thelocality of thedifferential weknow that(4.10) holdsmX-a.e.

on{|Du|> 0},while(3.4) showsthatdg = 0 mX-a.e. on{|Du|= 0},hencetoconclude

itissufficienttoprovethat|d(f ◦ u)|= 0mX-a.e.on{|Du|= 0}.Toseethis,let(fn)

LIPbd(Y) be such that (fn),(lipa(fn)) converge to f,|dmYf| mY-a.e. and in L2(mY)

respectively. Then the assumption umX ≤ CmY grants that (fn ◦ u),



lipa(fn)◦ u

 converge to f ◦ u,|dmYf|◦ u mX-a.e. and inL2(mX) respectively.Hence passingto the

limitin(3.2) weconcludethat|d(f ◦ u)|= 0 mX-a.e.on{|Du|= 0},asdesired. 2

Itisreadilyverifiedthatthemapsending[u∗ext(ω)] toext([u∗ω]) isanisomorphism fromu∗Ext(L0

μ(T∗Y)) to Ext(u∗L0μ(T∗Y)), hence from Proposition 4.4 above and the

universalpropertyofthepullbackstatedinProposition2.4weseethatthereisaunique

L0(m

X)-linearandcontinuous mapu∗π : u∗L0mY(T∗Y)→ Ext(u∗L0μ(T∗Y)) suchthat

u∗π([ud

mYf]) = ext[u∗dμf] ∀f ∈ S2(Y, dY, mY) (4.11)

andsuchmapsatisfies

|u∗π(ω)| ≤ |ω| m

X− a.e. ∀ω ∈ u∗L0mY(T∗Y). (4.12)

Then denoting by (u∗π)∗ : Ext(u∗L0

μ(T∗Y))  uL0 mY(T∗Y)  the adjoint of u∗π wehave:

Theorem4.5. Withtheabove notation andassumptionswehave

ˆ

du(v) = (u∗π)∗du(v) ∀v ∈ L0(T X) (4.13)

and

ˆdu(v) ≤ du(v) mX-a.e. on X ∀v ∈ L0(T X). (4.14)

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Proof. Let f ∈ S2(Y,d

Y,mY) andnoticethat

[u∗dmYf](ˆdu(v))(4.8)= d(f ◦ u)(v)(4.10)= dg(v)(3.7)= ext[u∗dμf](du(v))

(4.11)

= (u∗π)([u∗dmYf])(du(v)). Since elements of the form [u∗dmYf] generate u∗L0

mY(T∗Y), this is sufficient to prove

(4.13). Now observe that by duality (4.12) yields |(u∗π)∗(V )| ≤ |V | mX-a.e. for every

V ∈Ext(u∗L2μ(T∗Y)),hence(4.14) followsfrom(4.13). 2

Equalityin(4.14) canbe obtainedunderappropriateassumptionsoneitherX orY: Proposition4.6. SupposethateitherW1,2(X,d

X,mX) orW1,2(Y,dY,μ) isreflexive.Then

ˆdu(v)=du(v) holds mX-a.e. for every v ∈ L0(T X).

Proof. W1,2(X,d

X,m) is reflexive. Byinequality(4.14) andadensityargument to

con-clude it is sufficient to show that for any f ∈ L∞ ∩ S2(Y,d

Y,μ), g ∈ S2(X) as in

Proposition3.3and v ∈ L∞(T X) with boundedsupportitholds

dg(v) ≤ |dμf| ◦ u|ˆdu(v)| m − a.e. (4.15)

Letusobservethat(4.14) andtheverydefinitionof|du| give|ˆdu(v)|≤ |du(v)|≤ |du||v| m-a.e.,hencethem-a.e.valueofG◦ u|ˆdu(v)| isindependentontheμ-a.e.representative of G, andthe right handsideof (4.15) is welldefined m-a.e.(and equalto 0m-a.e. on

{|du|= 0}).Thetrivialbound  |G|2◦ u|ˆdu(v)|2dm ≤  |G|2◦ u|du|2|v|2dm ≤ |v|2  |G|2du (|du|2m) shows that

L2(Y, μ)  G → G ◦ u|ˆdu(v)| ∈ L2(X, m) is linear and continuous. (4.16)

Now fix f,v asin(4.15),letη ∈ LIP(X) be identically1onthe supportofv and with boundedsupport,(fn)⊂ LIPbd(Y) beasin(2.1) forthespace(Y,dY,μ) andnoticethat

sinceweassumedf tobebounded,uptoatruncationargumentwecanassumethefn’s

to be equibounded.Thus thefunctions fn◦ u are equibounded as welland taking into

account theLeibnizrulewe seethatηfn◦ u∈ W1,2(X,dX,m) withequibounded norm.

Since weassumedsuchspaceto bereflexive,uptopasstoanon-relabeledsubsequence

wecanassumethat(ηfn◦ u)n hasaW1,2-weaklimitanditisthenclearthatsuchlimit

is ηg. Thus wehave that(d(ηfn◦ u))n converges to d(ηg) weaklyinL2(T∗X) and, by

thechoicesofv,η,thisimpliesthat(d(fn◦ u)(v))n weaklyconvergestodg(v) inL2(X).

Now noticethat

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d(fn◦ u)(v) = [u∗dmYfn](ˆdu(v)) ≤ |dmYfn| ◦ u|ˆdu(v)| ≤ lipa(fn)◦ u|ˆdu(v)|.

This, (4.16) and the choiceof (fn) give thatthe rightmost side of the estimate above

convergestotheright handsideof(4.15) inL2(X).Thisconcludestheargument.

W1,2(Y,

dY,μ) isreflexive. Accordingto[1,Proposition7.6] anditsproof,inthiscase

forany f ∈ W1,2(Y,dY,μ) we can find(fn)⊂ LIPbs(Y)⊂ W1,2(Y,dY,mY) converging

tof inW1,2(Y,d

Y,μ) andsuchthatlipa(fn)→ |dμf| inL2(μ).Thedefinitionsofdu,ˆdu

give

ext[u∗dμfn](du(v))

(3.6)

= d(fn◦ u)(v)

= [u∗dmYfn](ˆdu(v)) ≤ |ˆdu(v)| |dmYfn| ◦ u ≤ |ˆdu(v)|lipa(fn)◦ u

andsincetheconstruction alsoensuresthat[u∗dμfn]→ [u∗dμf] asn→ ∞,bypassing

tothelimitwegetthat

ext([u∗dμf])(du(v)) ≤ |ˆdu(v)| |dμf| ◦ u = |ˆdu(v)| |ext([u∗dμf])|, m − a.e.

Bythearbitrarinessoff ∈ W1,2(Y,dY,μ),thisissufficientto concludetheproof. 2

4.3. The caseX=Rd andu Lipschitz

InthissectionweassumethatoursourcespaceX is(Rd,d

Eucl,Ld) andthatthemap

u∈ S2(Rd,Y) is also Lipschitz. In this case Kirchheim proved in [14] that for Ld-a.e.

x∈ Rd there isaseminorm md(u,x) onRd suchthat:

forLd-a.e.x we have md(u, x)(v) = lim

t↓0

dY



u(x + tv), u(x)

t for everyv ∈ Rd,

where it is part of the claim the fact that the limit in the right hand side exists for

Ld-a.e. x.

Wenow showthatsuchconceptisfullycompatiblewiththenotionofdifferentialwe

introduced:

Theorem4.7. Letu:Rd→ Y beaLipschitzmapthatisalsoinS2(Rd,Y) andv ∈ Rd

T Rd.Denote byv ∈ L¯ 0(T Rd) the vectorfieldconstantlyequaltov. Then

du(¯v)(x) = md(u, x)(v) forLd-a.e.x ∈ Rd. (4.17)

Proof. ≥ Let (yn)n be countable and dense in u(Rd) ⊂ Y and, for any n ∈ N, put

fn(·):= dY(·,yn).From the compatibilityof theabstract differential with theclassical

distributional notion in the case X = Rd (see [8, Remark 2.2.4]) and Rademacher’s

theoremwesee that

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d(fn◦ u)(¯v) = lim

h→0

fn◦ u(· + hv) − fn◦ u(·)

h Ld− a.e. (4.18)

Forx∈ Rdletγx: [0,1]→ Y betheLipschitzcurvedefinedbyγx

t :=u(x+tv) andput

gx

n,t:=fn◦ γtx. By[2, Theorem 1.1.2] anditsproof we knowthatfor themetricspeed

| ˙γx

t| it holds | ˙γtx| = supn∂tgxn,t for every x∈ Rd and a.e. t,so thattaking (4.18) into

account weobtain md(u, x + tv)(v) = | ˙γxt| = sup n ∂tg x n,t= sup n

d(fn◦ u)(¯v)(x + tv) Ld− a.e. x, a.e. t.

HenceFubini’stheoremyields

md(u, ·)(v) = sup n d(fn◦ u)(¯v) (3.6) = sup n

ext([u∗dμfn])(du(¯v)) ≤ |du(¯v)| Ld− a.e.,

having usedthetrivialbound|dμfn|≤ 1 μ-a.e.inthelast step.

≤ Let f ∈ S2(Y,d

Y,μ) be arbitrary and g ∈ S2(X) as inProposition 3.3. We will

show that

dg(v) ≤ |dμf| ◦ u md(u, ·)(v) Ld− a.e., (4.19)

which is sufficientto conclude.The bound≥ in (4.17) thatwe already provedand the

same argumentsused instudying(4.15) show thattheright handsideof (4.19) is well definedLd-a.e. andthat

L2(Y, μ)  G → G ◦ u md(u, ·)(v) ∈ L2(Rd) is linear and continuous. (4.20)

Now let(fn)⊂ LIPbd(Y) be asinProposition 3.3and notice thatforeveryn∈ N the

identity (4.18) yields, forLd-a.e.x:

|d(fn◦ u)(¯v)|(x) ≤ lipa(fn)(u(x)) lim h→0 dY  u(x + hv), u(x) |h| =lipa(fn)◦ u  (x) md(u, x)(v).

By(4.20) andthechoiceof (fn) we see thattherightmost sideof theaboveconverges

to therighthandsideof(4.19) inL2(Rd) andagainfollowingtheargumentsinthefirst

partoftheproofofProposition4.6(applicable,asW1,2(Rd) iscertainlyreflexive)wesee

thatd(fn◦ u)(¯v)



n convergestodg(v) weaklyinL

2(Rd).Hence(4.19) isobtained. 2

4.4. Thecase ofsmoothspaces andco-localweakdifferential

Inthissectionweassumethatthesourceandtargetspacesarecompleteandsmooth

Riemannian manifoldsM,N respectivelyandprovethe compatibilityof ourconceptof

differential with the oneintroduced in[19]. We stressthat alsothe approachin [19] is

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basedonpost-composition;assuch,provingcompatibilityofthetwonotionsamountsto alargeextenttotranslateonevocabularyintotheother,themoretechnicalpartabout therelationbetween‘abstract’and‘concrete’(co)vectorfieldsbeingalreadycoveredby Theorem4.1.

Let us denote by πM : T M → M the canonical projection. Recall that a bundle

morphismU : T M→ T N thatcoversu: M→ N isamapmakingthediagram

T M T N

M N

U

πM πN

u

commuteand linearonfibres. Letus recallthe notionofco-localweak differential and Sobolevspaceintroducedin[19]:

Definition4.8. Amap u: M→ N issaidtobe co-locallyweaklydifferentiableprovided

for any f ∈ C1

c(N,R) we have that f ◦ u ∈ Wloc1,1(M). In this case, the co-local weak

differentialDu isthebundlemorphism thatcoversu characterisedbytheidentity

D(f ◦ u)(x) = Dfu(x)◦ Du(x) VolM− a.e. x ∈ M ∀f ∈ Cc1(N). (4.21)

Finally,W˙ 1,2(M,N) isthe collectionof allmaps u: M→ N co-locallyweakly

differen-tiableforwhich|Du|g∗M⊗gN ∈ L2(M,VolM).

Wereferto[19,Proposition1.5] fortheproofthatanyco-locallyweaklydifferentiable maphasa,uniquelydefineduptoVolM-a.e. equality,co-localweak differential.

Itiseasytosee that

S2(M, N) = ˙W1,2(M, N) and |Du| ≤ |Du|gM∗⊗gN ≤ k|Du|

VolM− a.e. ∀u ∈ S2(M, N), (4.22)

wherek := min{dim M,dim N}.Indeed,ifu∈ S2(M,N),thenbydefinitionwehavethat

f ◦ u∈ W1,2(M) ⊂ W1,1

loc(M) foreveryf ∈ Cc1(N). Thenfor f = (f1,. . . ,fk): N→ Rk

wehave |D(f ◦ u)|gM∗⊗gRk k  j=1 |D(fj◦ u)|gM∗⊗gR= k  j=1 |D(fj◦ u)| k  j=1

Lip(fj)|Du| ≤ kLip(f)|Du|,

having used the compatibility between the ‘metric’ and ‘classical’ Sobolev spaces in

theequality. Thus by[19,Proposition 2.2] we concludethatu∈ ˙W1,2(M,N) and that

|Du|gM∗⊗gN ≤ k|Du| holdsalmost everywhere.

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Conversely,letu∈ ˙W1,2(M,N) andforanyf ∈ C1

c(N) letf := (f,˜ 0,. . . ,0): N→ Rk.

Then VolM-a.e.we have

|D(f ◦u)| = |D(f ◦u)|gM∗⊗gR=|D( ˜f ◦u)|g∗M⊗gRk ≤ Lip( ˜f)|Du|g∗M⊗gN = Lip(f)|Du|gM∗⊗gN.

Nowanargumentbasedontheapproximationlemma[19,Lemma2.3] andontheclosure

of (classical) weak differentials shows that the above holds for any f ∈ LIP(N). By

definition, this proves that u∈ S2(M,N) and thatthe bound |Du|≤ |Du|

g∗M⊗gN holds

VolM-a.e.,concludingtheproof of(4.22).

We turn to the statement and proof of the compatibility of the two notions of

differential. Weshallmake useofthe terminologyandresultsalreadydiscussed in Sec-tion 4.1. In particular,recalling (4.3) we shall think of du(v) as a map from L0(T X)

to Ext(u∗L0

μ(T N)).Also,weshallusethemapsP,ι introducedinTheorem4.1and the

map I : Ext(u∗L0μ(T N))→ Ext(u∗L0(N,T N;μ)) definedin(4.5).

Then wehave:

Theorem 4.9.LetM and N becomplete Riemannianmanifolds, andletu∈ S2(M,N)=

˙

W1,2(M,N).

Then foreveryv ∈ L0(T M) wehave

I(du(v)) = Du(ι(v)) VolM− a.e.

Proof. Using charts it is easy to see that the L0(μ)-normed module L0(N,T N;μ) is

generated by {Df : f ∈ Cc1(N)}. It follows that Ext(u∗L0(N,T N;μ)) is generated by

{ext([u∗Df]) : f ∈ C1

c(N)} and thus the conclusion follows if we show that for any

f ∈ C1

c(N) itholds

ext([u∗Df])I(du(v))= ext([u∗Dμf])



Du(ι(v)) VolM− a.e. (4.23)

To seethisstartnoticingthat

ext([u∗Df])I(du(v))(4.5),(2.5)= ext[u∗Df](u∗ι(ext−1(du(v)))

(4.4),(2.5)

= ext([u∗dμf])(du(v)) VolM− a.e.

Nowobserve thatthefunctionf ◦ u belongstoS2(X) andthus,bythelocalityproperty of minimal weak upper gradientsand (3.2), satisfies theconclusion of Proposition3.3. Hencetakinginto accounttheverydefinitionofdu(v) weobtain

ext([u∗Df])I(du(v))= d(f ◦ u)(v) VolM− a.e. (4.24)

Now put, as usual, ν := χ{|Du|>0}VolM and notice that a direct verification of the

property stated in Theorem 2.3 shows thatthe pullback module u∗L0(N,TN;μ) can

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beidentified withthe spaceof(equivalenceclassesupto ν-a.e.equalityof) Borelmaps

ω : M → T∗N such thatω(x) ∈ T

u(x)N for ν-a.e. x, the correspondingpullback map

beingtherightcompositionwithu.Withthisinmindandrecallingthedefinitionofthe extensionfunctorweget

ext([u∗Df])(x) = 

Dfu(x) for VolM− a.e. x ∈ {|Du| > 0},

0 for VolM− a.e. x ∈ {|Du| = 0},

andthus ext([u∗Df])Du(ι(v))(x) =  Dfu(x)  Dux(ι(v)(x)) 

for VolM− a.e. x ∈ {|Du| > 0},

0 for VolM− a.e. x ∈ {|Du| = 0}.

Noticingthat(4.22) yieldsthat{|Du|= 0}={|Du|= 0},theabovegives ext([u∗Df])Du(ι(v))(x) = Dfu(x)



Dux(ι(v)(x))



for VolM− a.e. x ∈ M.

Hencefromthedefinition(4.21) weconcludethat

ext([u∗Df])Du(ι(v))=D(f ◦ u)(ι(v)) VolM− a.e. (4.25)

Theclaim(4.23) is thenaconsequenceof (4.24),(4.25),(4.2) andthefactthatι is the

adjointofP . 2

5. Differentialoflocally Sobolevmapsbetweenmetricspaces

5.1. Inverse limits ofmodules

Here we briefly discussproperties ofinverse limitsinthe category of L0(m)-normed

modules,where morphisms are L0(m)-linear contractions, i.e.maps T : M N such

that|T (v)|≤ |v| m-a.e. Westartwith:

Proposition 5.1.Let ({Mi}i∈I,{Pji}i≤j∈I) be aninverse system of L0(m)-normed

mod-ules. Then there exists the inverse limit (M,{Pi}

i∈I). Moreover, for every family

I  i → viM

i suchthat

Pi

j(vj) =vi and ess sup

i∈I |v

i| ∈ L0(m) (5.1)

there is a unique v ∈ M such that vi = Pi(v) for every i ∈ I and it satisfies |v| =

ess supi|vi|.

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Proof. The system ({Mi}i∈I,{Pji}i≤j∈I) is also an inverse system in the category of

algebraic modulesover the ring L0(m) in the sense of [16, Chapter III.§10]. Hence

ac-cordingto[16,ChapterIII,Theorem10.2] anditsproofthereexiststhealgebraicinverse limit (MAlg,PAlgi ) and for everyfamily i → vi Mi there is aunique v ∈ MAlg such

thatPi

Alg(v)=vi foreveryi∈ I.Nowdefine|v| for anyv ∈MAlg as

|v| := ess sup

i∈I |P

i

Alg(v)| (5.2)

so that|v|: X→ [0,+∞] isthe equivalenceclass ofaBorelmap upto m-a.e.equality,

and put M := v ∈MAlg : |v| ∈ L0(m) = v ∈MAlg : |v| < +∞ m−a.e. , Pi:=Pi Alg|M.

We claimthat(M,Pi) isthedesired inverselimit.Startbynoticingthat(5.2) ensures

that|Pi(v)|≤ |v| m-a.e.,i.e.thePi’sarecontractions,asrequired.Letusnowcheckthat

M isaL0(m)-normedmodule:theonlynon-trivialthingtoverifyisthatitiscomplete,

i.e.thatif(vn) isCauchyinM,thenithasalimit.SincethePi’sarecontractions,wesee

thatn → Pi(v

n) isCauchyinMiandthushasalimitvi foreveryi∈ I.Passingto the

limitintheidentityPi(v

n)=Pji(Pj(vn)) validforeveryi≤ j andusing thecontinuity

of Pi

j wededucethatvi =Pji(vj),i.e.thereisv = (vi)i∈I ∈MAlg.Since (vn) isCauchy

and, trivially, the pointwise norm in M satisfies the triangle inequality, we see that

(|vn|) hasalimitf inL0(m).Thenfromthebound|vi|= limn|Pi(vn)|≤ limn|vn|=:f

valid foreveryi∈ I wededuce |v|≤ f andthusv ∈M.Similarly,from|vi− Pi(v

n)|=

limm|Pi(vm)−Pi(vn)|≤ limm|vm−vn| wededuce|v −vn|≤ limm|vm−vn| andpassing

to the L0(m)-limitin n andusing that(v

n) is M-Cauchywe conclude thatvn → v in

M,thusprovingcompleteness.

Now thefactthatforvi’sas in(5.1) thereisauniquev ∈M projectingon themis

atrivialconsequenceoftheconstructionandfromthisfacttheuniversalityproperty of (M,Pi) follows. 2

It isnow easyto check thatthere exists the inverselimit of acompatible familyof maps:

Proposition5.2. Let({Mi}

i∈I,{Pji}i≤j∈I) and({N i}i∈I,{Qij}i≤j∈I) betwoinverse

sys-temsofL0(m)-normedmodulesand(M,Pi),(N,Qi) theirinverselimits.Also,forevery

i∈ I letTi:MiN i beL0(m)-linearandcontinuousand suchthat

Ti◦ Pi

j =Qij◦ Tj ∀i ≤ j ∈ I (5.3)

and sothatforsome ∈ L0(m) wehave

|Ti(vi)| ≤ |vi| m − a.e. ∀i ∈ I, viMi. (5.4)

(21)

Then there exists a unique L0(m)-linear and continuous map T : M N such that

Qi◦ T = Ti◦ Pi foreveryi∈ I anditsatisfies|T (v)|≤ |v| m-a.e. forevery v ∈M.

Proof. Letv ∈M,putwi:=Ti(Pi(v))N i andnoticethat(5.3) yieldsQi

j(wj)=wi

and(5.4) that|wi|≤ |v| m-a.e.foreveryi≤ j ∈ I.ThusProposition5.1aboveensures

thatthereisauniqueT (v)∈N suchthatQi(T (v))=wiforeveryi∈ I anditsatisfies

|T (v)|≤ |v| m-a.e. Sincetheassignmentv → T (v) istriviallyL0(m)-linear,theproofis

completed. 2

5.2. LocallySobolevmapsandtheir differential

Inthissectionwecomebacktothecaseofgeneral(X,dX,m),(Y,dY) asinSection3

and studythe caseof u∈ S2

loc(X,Y), this being thecollectionof functionsu suchthat

every x∈ X has aneighbourhood Ux such thatu coincides with some ux ∈ S2(X,Y)

m-a.e. in Ux. Then for u ∈ Sloc2 (X,Y) the locality of the differential ensures that the

formula

|Du| := |Dux| m − a.e. on Ux ∀x ∈ X

givesawell-defined function|Du|∈ L2

loc(X). Here L2loc(X) denotesthe space oflocally

square-integrablefunctionsonX.

Forthiskindofu themeasureu(|Du|2m) isingeneralnotσ-finiteanylonger.Hence,

to define the differential du we need to suitably adaptthe definition previously given. Thisisthescopeof thecurrent section.

Fixu∈ S2

loc(X,Y). ByF(u) we denote the collectionof open sets Ω⊂ X suchthat



Ω|Du|

2dm < ∞. Since u ∈ S2

loc(X,Y) we see that F(u) is a cover of X. We shall

now build twoinverse limitsof L0(m)-normed modulesindexed over F(u),directedby

inclusion.Forthefirstdefine,forΩ∈ F(u),themeasure μΩonY as

μΩ:=u∗(|Du|2m|Ω).

ThusμΩ isRadonand wecan consider thecotangentmodule0Ω(T∗Y) of(Y,dYΩ)

and its pullback u∗L0

μΩ(T∗Y) which is a L0(m|Ω∩{|Du|>0})-normed module. Then put

u∗L0

Ω(T∗Y) := Ext(u∗L0μΩ(T∗Y)), which is L

0(m)-normed.Observe thatfor Ω ⊂ Ω

F(u) we have μΩ ≤ μΩ and thus Lemma 4.3 provides a canonical ‘projection’ map

PΩ

Ω :L0μΩ(T∗Y)→ Ext(L 0

μΩ(T∗Y)).Thenwecanconsiderthe(extended)pullbackmap

u∗PΩ

Ω : u∗L0Ω(T∗Y)→ u∗L(T∗Y) and notice thatsince PΩΩ21 ◦ PΩΩ32 =PΩΩ31 for every

Ω3⊂ Ω2⊂ Ω1∈ F(u),thefunctorialityofthepullbackgrantsthat(u∗L0Ω(T∗Y),u∗PΩ



Ω )

isaninversesystemofL0(m)-normedmodules.Wethencall(u∗L0u(T∗Y),PΩ) itsinverse limit(recallProposition5.1).

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