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PSEUDODIFFERENTIAL OPERATORS WITH ROUGH SYMBOLS ATANASSTEFANOV 7 0 0 ABSTRACT. In this work, we developLp boundednesstheoryfor pseudodifferentialop- 2 eratorswithrough(notevencontinuousingeneral)symbolsinthexvariable. Moreover, n the B(Lp) operator norms are estimated explicitly in terms of scale invariant quantities a involving the symbols. All the estimates are shown to be sharp with respect to the re- J quiredsmoothnessin theξ variable. Asa corollary,we obtainLp boundsfor(smoothed 9 outversionsof)themaximaldirectionalHilberttransformandtheCarlesonoperator. 2 ] A C 1. INTRODUCTION . h Inthispaper,weareconcernedwiththeLp mappingpropertiesofthepseudodifferential t a operators intheform m [ (1) T f(x) = σ(x,ξ)e2πiξxfˆ(ξ)dξ. σ 1 RZn v 6 The operators Tσ have been subject of continuous interest since the sixties. We should 5 mention that their usefullness in the study of partial differential equations have been re- 8 alized much earlier, but it seems that their systematic study began with the fundamental 1 0 works ofKohnandNirenberg, [10]and Ho¨rmander,[9]. 7 To describetheresultsobtained intheseearly papers, definetheHo¨rmander’sclass Sm, 0 / which consistsofall functionsσ(x,ξ), sothat h t (2) |DβDασ(x,ξ)| ≤ C (1+|ξ|)m−|α|. a x ξ α,β m forallmultiindicesα,β. Aclassicaltheoremin[9]thenstatesthatOp(σ) : Hs+m,p → Hs,p : v for all s ≥ 0 and 1 < p < ∞. In particular, Op(σ) : Lp → Lp, 1 < p < ∞, wheneverthe i X symbolσ ∈ Sm. Subsequentimprovementsofthesemethodsestablishedtheboundedness r of Op(σ) (basically under the assumption σ ∈ Sm for appropriate m) to various related a functionspaces,likeBesov,Triebel-Lizorkinspacestonameafew,butwewillnotreview thosehere, sincetheyfalloutsideofthescopeofthispaper. It isworthmentioninghowever,thatthesimpletoverifycondition(2)istheonearising in manyapplications. TheL2 boundednessplaysspecial rolein thetheoryand thatis why we discussit separately. TheclassofsymbolsSm , defined via ρ,δ (3) |DβDασ(x,ξ)| ≤ C (1+|ξ|)m−ρ|α|+δ|β|. x ξ α,β Date:February2,2008. 2000MathematicsSubjectClassification. 35S05,47G30. Keywordsandphrases. Pseudodifferentialoperators,Lpbounds,orthogonality. Supportedinpartbynsf-dms0300511. 1 2 ATANASSTEFANOV represents a larger set of symbolsthan Sm = Sm , which has subsequently found applica- 1,0 tionsin localsolvabilityforlinearPDE’s, [1]. Here, we have to mention the celbrated result of Caldero´n-Vaillancourt, [3], [4] which states that L2 boundedness for T holds, whenever σ ∈ S0 , 0 ≤ ρ < 1, whereas S0 σ ρ,ρ 1,1 is a “forbidden” class, in the sense that there are symbols in that class, which give rise to unbounded on L2 operators. We should mention here the work of Cordes [6], who improvedtheresultforS0 by requiringthat(3) holdsonlyfor|α|,|β| ≤ [n/2]+1. 0,0 Regarding less regularin x symbols,for any modulusof continuityω : R → R (that + + is,anincreasingandcontinuousfunction),definethespaceCω ofalluniformlycontinuous and boundedfunctionsu : Rn → C, satisfying |u(x+y)−u(x)| ≤ ω(|y|). The followingclassof symbolswas introducedand studiedby Coifman-Meyer, [5]. More precisely,let σ(x,ξ) ∈ CωS0 , whichmeansit satisfies 1,0 sup < |ξ| >|α| |Dα[σ(x+y,ξ)−σ(x,ξ)]| ≤ C ω(|y|) ξ α x,y,ξ and assume that ω(2−j)2 < ∞. Then for all 1 < p < ∞, Op(σ) : Lp → Lp. The j>0 condition ω(2−j)2 < ∞ is clearly very mild continuity assumption for the function j P x → σ(x,ξ). In particular, one sees that ∪ CγS0 ⊂ CωS0 . Related results can be P γ>0 1,0 found in the work of M. Taylor, [23] (see Proposition 2.4, p. 23) and J. Marschall, [11] where the spaces Cω are replaced by Hε,p spaces with p as large as onewish and 0 < ε = ε(p) << 1 (seealso[23], p. 61) One of the purposes of this work is to get away from the continuity requirements on x → σ(x,ξ). Even more importantly, we would like to replace the pointwise conditions on the derivatives of ξ by averaged ones. This particular point has not been thoroughly exploredappropriately intheliteraturein theauthor’sopinion,see Theorem1 below. Ontheotherhand,aparticularmotivationforsuchconsiderationsisprovidedbythere- cent papers of Rodnianski-Tao [14] and the author [17], where concrete parametrices (i.e. pseudodifferential operators, representing approximate solutions to certain PDE’s) were constructedforthesolutionsofcertainfirstorderperturbationofthewaveandSchro¨dinger equations. A very quick inspection of these examples shows that1 they do not obey point- wiseconditionsonthederivativesonthesymbolsand thus,thesemethodsfailtoimplyL2 bounds for these (and related problems). Moreover, one often times has to deal with the situation, where the maps ξ → σ(x,ξ) are not smooth in a pointwise sense. On the other hand, onemaystillbeableto controlaveraged quantitieslike (4) supkσ(x,ξ)k < ∞. Hn/2 x ξ ThiswillbeourtresholdconditionforL2 boundedness,whichwetry toachieve. Heuristicallyatleast,(4)mustbe“enough”insomesense,sinceifwehadsimplesymbols like σ(x,ξ) = σ (x)σ (ξ), then the L2 boundedness of Op(σ) is equivalent to kσ k < 1 2 1 L∞ x 1Mostreadersarelikelytohavetheirownfairlylonglistwithfavoriteexamples,forwhichtheHo¨rmander conditionfails. PSEUDODIFFERENTIALOPERATORSWITHROUGHSYMBOLS 3 ∞,kσ k < ∞. Clearly, kσ k just fails to be controlled by (4), but on the other 2 L∞ 2 L∞(Rn) ξ ξ hand, thequanitityin(4)is controlledby theappropriateBesov spaceBn/2 norm. 2,1 A final motivation for the current study is to achieve a scale invariant condition, which gives an estimateof the L2 → L2 (Lp → Lp) norm of Op(σ) in terms of a scale invariant quantity,thatis,weaim at showingan estimate, kOp(σ)k ≤ Ckσk kfk , Lp→Lp Y Lp where foreveryλ 6= 0, onehas kσ(λ·,λ−1·)k = kσk . Y Y Inthatregard,notethatthecondition(whichisoneoftherequirementsoftheHo¨rmander class S0) (5) sup|Dασ(x,ξ)| ≤ C |ξ|−|α| ξ α x is scale invariant in the sense described above. Moreover, by the standard Caldero´n- Zygmund theory (see [21]), the pointwise condition (5) together with kT k < ∞ σ L2→L2 implies T f(x) = K(x,x−y)f(y)dy, σ Z whereK(x,·)satisfiestheHo¨rmander-Mihlinconditions,namely|K(x,z)| ≤ C|z|−n and |∇ K(x,z)| ≤ C|z|−n−1, where the constant C depends on the constants C : |α| < z α [n/2]+1 in (5). This in turn is enough to conclude that T : Lp → Lp for all 1 < p ≤ 2 σ and in fact thereistheendpointestimateT : L1 → L1,∞. σ 1.1. Lp estimates for PDO with rough symbols - statement of results. We start now with our main theorems, which concern the L2 and the Lp boundedness for pseudodiffer- ential operators Op(σ) withrough symbols. Ourfirst result establishesthat aBesov space versionof(4)isenough forL2 boundednessand theresult issharp. Theorem 1. (L2 bounds) Let σ(x,ξ) : Rn ×Rn → C and T is the corresponding pseu- σ dodifferentialoperator. Then (6) kT k ≤ C( 2ln/2supkPξσ(x,·)k ), σ L2(Rn)→L2(Rn) l L2(Rn) x l X where Pξ is theLittlewood-Paleyoperatorin theξ variable. l Moreover,theresultissharpinthefollowingsense: foreveryp > 2,thereexistsσ(x,ξ) so that sup |Dασ(x,ξ)| ≤ C |ξ|−|α| and sup kσ(x,·)k < ∞, but T fails to be x ξ α x Wp,n/p σ boundedon L2(Rn). Remark: (1) Notethattheestimateon T isscaleinvariant. σ (2) The sharpness claim of the theorem, roughly speaking, shows that in the scale of spaces2 Wp,n/p, ∞ ≥ p ≥ 2, one may not require anything less than W2,n/2 = Hn/2 ofthesymbolin ordertoensureL2 boundedness. 2NotethatthesespacesscalethesameandmoreoverbySobolevembeddingthesearestrictlydecreasing sequence,atleastfor2≤p<∞. 4 ATANASSTEFANOV (3) The counterexample to which we refer in Theorem 1 is a simple variation of the well-known example of σ ∈ S0 , the “forbidden class”, which fails to be L2 1,1 bounded,see [21], p. 272and Section 6 below. Ournextresult concernsLp boundednessforT . σ Theorem 2. (Lp bounds) For the pseudodifferential operator T there is the estimate for σ all 2 < p ≤ ∞, (7) kT k ≤ C( 2ln/2supkPξσ(x,·)k ), σ Lp(Rn)→Lp(Rn) l L2(Rn) x l X Fortherange1 < p < 2 andindeed fortheweak type(1,1),thereis (8) kT k +kT k ≤ C 2lnsupkPξσ(x,·)k . σ Lp→Lp σ L1→L1,∞ l L1(Rn) x l X Alternatively, if one assumes the L2 bound, together with (5), one still gets Lp → Lp, 1 < p ≤ 2, andin factweak type(1,1)bounds. Moreover, kT k ≤ C( 2ln/2supkPξσ(x,·)k + sup sup|ξ||α||Dασ(x,ξ)|). σ Lp→Lp l L2(Rn) ξ x |α|<[n/2]+1 x,ξ l X As we pointedout in Theorem 1, theestimates are essentiallysharp for Lp, 2 ≤ p < ∞ boundedness. The following corollary gives even more precise condition under which a symbolσ willgiverisetoaboundedoperatoron Lq in thecase ofa given1 < q < 2 Corollary 1. Let 1 < q < 2. Then kTσkLq→Lq ≤ C 2ln/qsupkPlξσ(x,·)kLq(Rn). x l X Clearly the proof follows by interpolation from the L2 estimates in Theorem 1 and the weak type(1,1)estimatesofTheorem2. 1.2. PDO’s with homogeneous of degree zero symbols - statement of results. Re- garding symbols that are homogeneous of degree zero, i.e. σ(x,ξ) = q(x,ξ/|ξ), where q : Rn ×Sn−1 → C, weobtainmorepreciseresultsin termsofthesmoothnessofq. NotethattheclassicalHo¨rmanderconditionrequirespointwisesmoothnessofthefunction q in bothvariables. Ourresult ontheotherhand requires muchlessthan that. Theorem 3. (Lp boundsforhomogeneousofdegree zerosymbols) Let q : Rn ×Sn−1 → C. Let T f(x) = q(x,ξ/|ξ|)e2πiξxfˆ(ξ)dξ. q RZn Then Tq : L2 → L2, if l2l(n−1)/2kPlξ/|ξqkL2(Sn−1) < ∞ andinfact (9) kTqkLP2→L2 ≤ C 2l(n−1)/2supkPlξ/|ξ|q(x,·)kL2(Sn−1). x l X PSEUDODIFFERENTIALOPERATORSWITHROUGHSYMBOLS 5 Concerning Lp bounds,we haveforevery2 ≤ p ≤ ∞. (10) kTqkB0 →Lp ≤ Cn( 2l(n−1)/p′ supkPlξ/|ξ|qkLp′(Sn−1)). p,1 x l X Note thatin (10), theconstantC isindependentofp,r. n Remark: (1) ItwouldbeinterestingtoseewhethertheusualLp → Lp boundednessholdstrue. (2) Note that there is no weak type (1,1) statement in Theorem 3. This is a difficult issueevenformultipliers. Thesharpness statementassociated withTheorem3 is Proposition 1. For every N > 1, there exists a homogeneous of degree zero symbol σ(x,ξ) : R2 ×R2 → R1, so that sup |σ(x,ξ)| < ∞ and sup kσ(x,ξ)k < ∞, x,ξ x W1,1(S1) and sothatkT k > N. σ L2→L2 The counterexample considered here is a smoothed out version of the maximal direc- tional Hilbert transform in the plane H f(x) = sup |H f(x)|. We mention the spec- ∗ u∈S1 u tacular recent result of Lacey and Li, [12] showing the boundedness of H on Lp(R2) : ∗ 2 < p < ∞ with a H : L2(R2) → L2,∞(R2) as an endpoint estimate. Note that the ∗ L2 → L2 bound fails, as elementary examples show, see [12]. We verify later that the condition (10) just fails for the (smoothed out) multiplier σ of H in two dimensions, but ∗ on theotherhand theconditionkσ(x,ξ)k < ∞ holds. W1,1(S1) ThisexamplewillshowthattheBesovspaces requirementsforσ in(9)and(10)cannot bereplaced bySobolevspaces and/orspaces withlessderivatives. 1.3. PDO’swithradialsymbols. Finally,weconsiderthecaseofradialsymbols. Thatis for ρ : Rn ×R1 → C and + T f(x) = ρ(x,|ξ|)e2πiξxfˆ(ξ)dξ. ρ Rn Z Theorem 4. TheoperatorT : L2 → L2, if 2l/2supkP|ξ|ρ(x,·)k < ∞. In fact, ρ l l L2(R1) x P kT k ≤ C 2l/2supkP|ξ|ρ(x,·)k . ρ L2→L2 l L2(R1) x l X Clearly,establishingLp,p 6= 2boundsforsimpleradialsymbolsisalreadyanotoriously difficult problem. One only needs to point out to the Bochner-Riez multiplier(1−|ξ|2)δ + (which satisfy Lp bounds only in certain range of p′s, depending on the dimension and δ) or even the simpler “thin annulus” multiplier ϕ(2m(1−|ξ|2)) to understand the difficulty oftheproblemingeneral. 6 ATANASSTEFANOV 2. APPLICATIONS In this section, we demonstrate the effectiveness of the Lp boundedness theorems for rough PDO’s. Wewill mostlyconcentrate on applicationtomaximalfunctionsand opera- tors3Someofourexampleswillbewell-knownresultsformaximaloperators,whileothers willbeahigherdimensionalextensionsofsuchresults. 2.1. AlmosteverywhereconvergenceforCesarosumsofLp functionsin1D. Westart withCesaro’s sumfor Fourierseries inonespacedimension. Foranyδ > 0,define C f(x) = sup (1−ξ2/u2)δ e2πiξxfˆ(ξ)dξ. δ + u>0 R1 Z Clearly,asalimitasδ → 0,wegettheCarleson’soperator. Unfortunately,onecannotcon- clude that sup kC k < ∞, for that would imply the famous Carleson-Hunt theorem. δ>0 δ Lp On theotherhand, definethemaximal”thin intervaloperator” T f(x) = sup ϕ(2m(1−ξ2/u2))e2πiξxfˆ(ξ)dξ. m u>0 R1 Z A simpleargumentbased on (theproofof)Theorem 2yields Proposition2. Foranyε > 0,1 < p < ∞,thereexistsC , sothat p,ε (11) supkT k ≤ C . m Lp(R1)→Lp(R1) p m In fact, there is the more general pointwise bound sup|T f(x)| ≤ CM(sup |P f|)(x), m k k m which implies(11)as well as (12) kC k +kC k ≤ C . δ Lp→Lp δ F10,∞(R1)→L1,∞(R1) δ,p Remark: • Note that this result, while clearly inferior to the Carleson-Hunt theorem still im- pliesa.e. convergenceforanyCesarosummabilitymethod,whenappliedtoLp(R1) functions,and infact forthelarger classofF0 functions. p,∞ • Usingthemethodofproofhere,onemayactuallyproveL2 estimates4forthemax- imalBochner-Rieszoperator BR f(x) = sup (1−|ξ|2/u2)δ e2πiξxfˆ(ξ)dξ. δ + u>0 Rn Z inanydimension. Proof. It clearly suffices to show the pointiwise estimate |T f(x)| ≤ CM(sup P f)(x) m k k foranyk. ThestatementsaboutB0 → Lp boundsfollowbyelementaryLittlewood-Paley p,1 theory and the lp bounds for the Hardy-Littlewood maximal function. The restricted-to- weak estimateF0 → L1,∞ for C follows by summingan exponentiallydecaying series 1,∞ δ in thequasi-Banach spaceL1,∞. 3Inaddition,theauthorhasalsoidentifiedseveralapplicationstobilinear/multilinearoperatorsofimpor- tancetocertaindispersivePDE’s,whichwillbeaddressedinafuturepublication. 4AndinfactLp →Lpestimatesforp=p(δ)closeto2. PSEUDODIFFERENTIALOPERATORSWITHROUGHSYMBOLS 7 By supportconsiderations,it isclearthat T f(x) = sup ϕ(2m(1−ξ2/u2))e2πiξxϕ(2−kξ)fˆ(ξ)dξ = m u>0 R1 k Z X = sup ϕ(2m(1−ξ2/u2))e2πiξxϕ(2−kξ)fˆ(ξ)dξ = k u∈(2k−2,2k+2)ZR1 X = T f . m,u(·)∈(2k−2,2k+2) k k X Clearly, the requirement u ∈ (2k−2,2k+2) creates (almost) disjointness in the x support, whence (13) |T f(x)| ≤ Csup|T f (x)|. m m,u(·)∈(2k−2,2k+2) k k Ourbasicclaimis that (14) |T f (x)| ≤ CM(f ). m,u(·)∈(2k−2,2k+2) k k Clearly (13) and(14)implysup |T f(x)| ≤ CM(sup|f |), whencetheProposition2. m m k k By scaleinvariance,(14)reduces tothecasek = 0,that isweneed toshow |T P f(x)| ≤ CM(P f)(x). m,u(x)∈(1/4,4) 0 0 foranySchwartzfunctionf andanym >> 1. By(31)(intheproofofTheorem2below), it willsufficetoshow (15) 2lsupkPξ[ϕ(2m(1−ξ2/u(x)2))ϕ(ξ)]k . 1. l L1(R1) x l X for anymeasurablefunctionu, whichtakes itsvaluesin(1/4,4). For(15), wehave 2lsupkPξ[ϕ(2m(1−ξ2/u(x)2))ϕ(ξ)]k l L1(R1) x ξ l<m X ≤ 2l sup |ϕ(2m(1−ξ2/u2))ϕ(ξ)|dξ . 2l−m . 1, l<m u∈(1/4,4)Z l<m X X while 2lsupkPξ[ϕ(2m(1−ξ2/u(x)2))ϕ(ξ)]k l L1(R1) x ξ l≥m X d2 ≤ 2−l sup | ϕ(2m(1−ξ2/u2))ϕ(ξ)|dξ ≤ C 2−l+m . 1. dξ2 l≥m u∈(1/4,4)Z l≥m X X (cid:3) 8 ATANASSTEFANOV 2.2. Maximaldirectional Hilberttransformsandthe Kakeyamaximalfunction. An- otherinterestingapplicationisprovidedbythedirectionalHilberttransformindimensions n ≥ 2. Namely,take H∗ = sup (hu,ξ/|ξ|i)δe2πiξxfˆ(ξ)ϕ(ξ)dξ, δ + u∈Sn−1Z where suppϕ ⊂ {1/2 < |ξ| < 2}. As δ → 0, we obtain the operator f → sup e2πiξxfˆ(ξ)dξ,which is closely u∈Sn−1 {hu,ξi>0} related to themaximaldirectionalHilberttransform R H f(x) = sup|H f(x)| = sup| sgn(u,ξ)e2πiξxfˆ(ξ)ϕ(ξ)dξ|. ∗ u u u Z H was of course shown to be Lp(R2),p > 2 bounded by Lacey and Li, [12] by very ∗ sophisticatedtime-frequencyanalysismethods. Proposition3. Forthe“thinbig circle”multiplier T f(x) = sup | ϕ(2mhu,ξ/|ξ|i)e2πiξxfˆ(ξ)ϕ(ξ)dξ|. m u∈Sn−1 ZRn we have (16) kT fk ≤ C 2m(n/2−1) m L2→L2 ε In particular kH∗k ≤ C 2n/2−1. δ L2(Rn)→L2(Rn) p,ε,δ Remark: • We believe that the operator T (m >> 1) has a particular connection to the m Kakeya maximal function and the corresponding Kakeya problem. Indeed, the kernel of the corresponding singular integral behaves like a (L1 normalized) char- acteristic function of a rectangle with long side along u of length 2m and (n−1) shortsidesoflength1in thetransversedirections! • Inrelation tothat,oneexpectstheconjectured Kakeyabounds kT fk ≤ C 2m(n/p−1) m Lp→Lp ε forp ≤ n tohold,whileoneonlygets kT fk ≤ C 2m(n/p−2/p) m Lp→Lp ε as a consequence of Theorem 3. Nevertheless, the two match when p = 2. So it seems that (16), at least in principle, captures the Kakeya conjecture for p = 2 in general andin particularthefullKakeyaconjectureintwo dimensions. Sinceourestimatesdonotseemtocontributemuchtowardtheresolutionofany new Kakeya estimates, we do not pursue here the exact relationship between T m and the Kakeya maximaloperator, although from our heuristicarguments above it shouldbeclear thatitis acloseone. PSEUDODIFFERENTIALOPERATORSWITHROUGHSYMBOLS 9 Proof. Weproceed as in theproofofProposition2. Weneed onlyshow (17) 2l(n−1)/2supkPlξ/|ξ|ϕ(2mhu(x),ξ/|ξ|i)kL2(Sn−1) . 1. x l X We have 2l(n−1)/2supkPlξ/|ξ|ϕ(2mhu(x),ξ/|ξ|i)kL2(Sn−1) x l<m X ≤ C 2l(n−1)/2supkϕ(2mhu(x),ξ/|ξ|i)kL2(Sn−1) u l<m X ≤ C 2l(n−1)/22−m/2 . 2m(n/2−1). l<m X 2l(n−1)/2supkPlξ/|ξ|ϕ(2mhu(x),ξ/|ξ|i)kL2(Sn−1) x l≥m X C ≤ 2−l(n−1)/2supkΩ(n−1)ϕ(2mhu(x),ξ/|ξ|i)kL2(Sn−1) u l≥m X ≤ C 2−l(n−1)/22m(n−1)2−m/2 . 2m(n/2−1). l≥m X (cid:3) 2.3. Estimates onT , T etc. We now present a result, which allows us to treat pseu- σ1σ2 eσ dodifferential operators, whosesymbolsare products, exponentials(or moregenerally en- tire functions) of symbols, which satisfy the requirements in Theorems 1, 2, 3. We would liketopointoutthatsimilarinspirit(byessentiallyrequiringn/2+εderivativesinL2,but in amoregeneral setting)functionalcalculus typeresult wasobtainedin [16]. Proposition 4. Let σ,σ ,σ : Rn × Rn → C, so that T ,j = 1,2 define Lp bounded 1 2 σj operators,as in(6), (8). Then forevery1 < p < ∞,T isLp boundedand σ1σ2 2 (18) kT k ≤ C ( 2ln/2supkPξσ (x,·)k ), σ1σ2 L2(Rn)→L2(Rn) l j L2(Rn) x j=1 l Y X 2 (19) kT k ≤ C ( 2lnsupkPξσ (x,·)k ). σ1σ2 Lp(Rn)→Lp(Rn) l j L1(Rn) x j=1 l Y X In thesamespirit,T is alsoLp boundedandthereis eσ (20) kT k ≤ Cexp( 2lnsupkPξσ(x,·)k ) eσ Lp(Rn)→Lp(Rn) l L1(Rn) x l X 10 ATANASSTEFANOV Similarstatementscan bemadeforhomogeneousofdegreezerosymbols µ (x,ξ/|ξ|),µ (x,ξ/|ξ|), 1 1 2 (21) kT k ≤ C ( 2l(n−1)/2supkPξ/|ξ|µ (x,·)k ), µ1µ2 L2(Rn)→L2(Rn) l j L1(Rn) x j=1 l Y X (22) kT k ≤ Cexp( 2l(n−1)supkPξ/|ξ|µ(x,·)k ). eµ L2(Rn)→L2(Rn) l L1(Rn) x l X TheproofofProposition4isbased onthecorrespondingTheoremforLp boundedness, combined withthefact thatourrequirements form aBanach algebra underthemultiplica- tion. Takeforexample(18). By Theorem 1,we have kT k ≤ C( 2ln/2supkPξ(σ σ )(x,·)k ) σ1σ2 L2(Rn)→L2(Rn) l 1 2 L2(Rn) x l X We finishby invokingtheestimate 2 (23) 2ln/2supkPξ(σ σ )(x,·)k ≤ C ( 2ln/2supkPξσ (x,·)k ). l 1 2 L2(Rn) l j L2(Rn) x x l j=1 l X Y X where thislastinequalityessentiallymeansthat Bn/2 is aBanach algebraoffunctions5. 2,1 The argument above can be performed for the proof of (19). For (20) (and more gener- ally forany symbolsoftheform g(σ), whereg isentirefunction), oneiterates theproduct estimate(23)to (24) 2ln/2supkPξ(eσ)(x,·)k ≤ Cexp( 2ln/2supkPξσ(x,·)k ). l L2(Rn) l L2(Rn) x x l l X X Fortheproofof(21), (22),onehas tousethefact thatB(n−1)/2(Sn−1) isaBanach algebra 2,1 as well, whenceonegetsan estimatesimilarto(23)and (24). 3. PRELIMINARIES We startby introducingsomebasicconceptsin Fourieranalysis. 3.1. FourieranalysisonRn. First,define theFouriertransformand itsinverse fˆ(ξ) = f(x)e−2πix·ξdx, RZn f(x) = fˆ(ξ)e2πix·ξdξ. RZn For a positive, smooth and even function χ : Rn → R1, supported in {ξ : |ξ| ≤ 2} and + so that χ(ξ) = 1 for all |ξ| ≤ 1. Define ϕ(ξ) = χ(ξ)− χ(2ξ), which is supported in the annulus1/2 ≤ |ξ| ≤ 2. Clearly ϕ(2−kξ) = 1 forall6ξ 6= 0. k∈Z 5This is well-known, but can be vePrified easily by means of the Kato-Ponce estimate k∂n/2(uv)kL2 ≤ C(k∂n/2ukL2kvkL∞+k∂n/2vkL2kukL∞),theembeddingB2n,/12 ֒→L∞andsomeLittlewood-Paleytheory. 6ThediscussionhenceforthwillbeforRn,unlessexplicitelyspecifiedotherwise.

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