ON L p RESOLVENT ESTIMATES FOR LAPLACE-BELTRAMI OPERATORS ON COMPACT MANIFOLDS

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1 ON p RESOVENT ESTIMATES FOR APACE-BETRAMI OPERATORS ON COMPACT MANIFODS DAVID DOS SANTOS FERREIRA, CAROS E. KENIG, AND MIKKO SAO Abstract. In this article we prove p estimates for resolvents of aplace-beltrami operators on compact Riemannian manifolds, generalizing results of [] in the Euclidean case and [7] for the torus. We follow [8] and construct Hadamard s parametrix, then use classical boundedness results on integral operators with oscillatory kernels related to the Carleson and Sjölin condition. Our initial motivation was to obtain p Carleman estimates with limiting Carleman weights generalizing those of Jerison and Kenig []; we illustrate the pertinence of p resolvent estimates by showing the relation with Carleman estimates. Such estimates are useful in the construction of complex geometrical optics solutions to the Schrödinger equation with unbounded potentials, an essential device for solving anisotropic inverse problems [4]. Contents. Introduction. Oscillatory integral operators 4 3. Hadamard s parametrix 8 4. Resolvent estimates 5. Relation with p Carleman estimates 5 References 30. Introduction This article aims at proving p estimates on the resolvent of aplace- Beltrami operators on compact Riemannian manifolds in the spirit of those obtained by Kenig, Ruiz and Sogge [] on the flat Euclidean space and of Shen [7] on the flat torus. This work grew out of our recent interest in p Carleman estimates with limiting Carleman weights generalizing Jerison and Kenig s estimates [] to variable coefficients and used in the context of anisotropic inverse problems [4, 5]. It turned out that in [5], we were able to prove p Carleman estimates in a direct way, without referring to resolvent estimates. Meanwhile, in the process of obtaining those Carleman estimates, we were led to derive resolvent estimates. Since these resolvent

2 DOS SANTOS FERREIRA, KENIG, SAO estimates might be helpful in different contexts, we decided to make them available. et M, g) be a compact Riemannian manifold of dimension n 3 without boundary). In local coordinates, the aplace-beltrami operator takes the form det g = g g jk ) det g x j x k where g jk ) j,k n denotes the inverse matrix of g jk ) j,k n if g = g jk dx j dx k. As is classical, we are using Einstein s summation convention: repeated upper and lower indices are implicitly summed over all their possible values. We will be using the notation θ g = g jk θ j θ k to denote the norm of a vector and d g to denote the geodesic distance in M, g). We denote σ g ) the set of eigenvalues of the aplace-beltrami operator on M, g), and denote by Rz) = g + z), z C \ σ g ) the resolvent operator. We are interested in proving estimates of the form u b M) C g z)u a M) for the couple of dual exponents a = /n + ), b = /n )). Note that by taking u =, it is clear that such estimates can only hold away from z = 0, and similarly by taking u to be any eigenfunction of g, away from the negative of any eigenvalue. This is in contrast to the non-compact flat case where Kenig, Ruiz and Sogge [] were able to obtain such estimates for all values of the complex parameter. In fact, we will restrict our investigation to the following set of values Ξ δ = { z C \ R : Re z δ } = { z C \ R : Im z) 4δ δ Re z) }. This set is the exterior of a parabola and can be visualized in figure. The corresponding results were obtained by Shen [7] on the flat torus. It seems that such estimates cannot be obtained as a direct consequence of the spectral cluster estimates obtained by Sogge [8]. Indeed, if χ m denotes the cluster of spectral projectors related to the eigenvalues of the aplacian the square root of the negative of which lie in the interval [m, m + ) then Sogge s estimates read χ m u n M) C + m) u M) χ m u M) C + m) u n+ M). This would reduce the resolvent estimate to an estimate of the form χ m u M) Am, z) χ m g z)u M)

3 p RESOVENT ESTIMATES 3 but summing the corresponding series m=0 +m)am, z) to patch the estimates requires a decay of Am, z) which cannot be achieved. Nevertheless, we will use Sogge s estimates in the process of reducing Carleman estimates with limiting Carleman weights to resolvent estimates in the last section of this paper Figure. Allowed values of the spectral parameter z Theorem.. et M, g) be a compact Riemannian manifold without boundary) of dimension n 3, and let δ 0, ) be a positive number. There exists a constant C > 0 such that for all u C M) and all z Ξ δ, the following resolvent estimate holds.) u n M) C g z)u n+ M). The proof of the theorem relies on the construction of the Hadamard parametrix. We provide a fairly complete study of the p boundedness properties of Hadamard s parametrix and the corresponding remainder term. Some of the estimates might not be used in the proof of Theorem. but may be of independent interest in other contexts. Remark.. The question of whether the estimates hold for a larger set of values of the spectral parameter z, for instance Ξ δ = {z C \ R : Im z δ when Re z < 0 and z > δ when Re z 0 } remains open. As is common practice, we will write A B as shorthand for A CB where C is a constant which depends on known fixed parameters the dimension n, the indices p, q of the ebesgue classes involved, the Riemannian manifold M, g), etc.), but whose value is not crucial to the problem at hand. Similarly we use the notation A B when A B and A B. We

4 4 DOS SANTOS FERREIRA, KENIG, SAO consider the principal branch of the square root on C \ R which we denote by z. We also choose the convention that arg z π, π) when z C\R. In the second section of this note, we review the different bounds known on oscillatory integral operators, in particular those obtained by the Carleson- Sjölin theory. In the third section, we construct the Hadamard parametrix following [9]. In the fourth section, we prove bounds on the Hadamard parametrix following the techniques of [, 8] and derive the corresponding resolvent estimates. Finally, in the last section, we illustrate the pertinence of resolvent estimates by showing how they imply Carleman estimates with limiting Carleman weights in the spirit of Jerison and Kenig s estimates []. Note that these Carleman estimates can be obtained by other means [4]. Acknowledgements. Carlos Kenig was partially supported by NSF grant DMS Mikko Salo is supported in part by the Academy of Finland. David Dos Santos Ferreira and Mikko Salo would like to acknowledge the hospitality of the University of Chicago.. Oscillatory integral operators This section is a short review of the classical boundedness results of operators with oscillatory kernels which will be needed in this note. We consider operators of the form T λ ux) = e iλϕx,y) ax, y)uy) dy where a belongs to C 0 U V ) with U, V open sets in Rn and ϕ is a smooth function on U V. The product T U T V of cotangent bundles of U and V endowed with the symplectic form σ = dξ dx + dη dy is a symplectic manifold of dimension 4n. A fundamental object in the study of the operators under our scope is the agrangian submanifold of T U T V C ϕ = { x, x ϕx, y), y, y ϕx, y)) : x, y) U V }. The first result relates to boundedness of such oscillatory integral operators. For that purpose, we consider the two projections C ϕ T U T V π U If π U is a local diffeomorphism, i.e..) π V T U T V. det ϕ x y 0 on U V then so is π V and C ϕ is locally the graph of the canonical transformation ς = π U π V. The mother of estimates [9] [, Theorem..] corresponds to the case where C ϕ is locally a canonical graph.

5 p RESOVENT ESTIMATES 5 Theorem.. Suppose that the non-degeneracy assumption.) is satisfied, then for all compact K V there exists a constant C > 0 such that for all λ and all u C 0 K) T λ u Cλ n/ u. This non-degeneracy assumption is too stringent for the applications in this note we stated this result only for the sake of completeness), in fact, we will use a weaker result and make the following non-degeneracy assumption [9, Theorem 5.3.8].) on the lifted symplectic form corank σ Cϕ = σ Cϕ = π Uσ. Note that we could have used either the first or the second projection π V to lift the symplectic form; the condition is explicitly given by.3) corank ϕ x y = on U V. The boundedness result that we will need reads as follows. Theorem.. Suppose that the non-degeneracy assumption.3) is satisfied, then for all compact K V there exists a constant C > 0 such that for all λ and all u C 0 K) T λ u Cλ n )/ u. By interpolation with the trivial bound, one gets the following p p result. Corollary.3. Under the assumptions of Theorem., we have where p. T λ u p C pλ n )/p u p The range of admissible exponents in this theorem is represented by the green line in figure. The second type of results we need are those related to the n n Carleson- Sjölin hypothesis []. Under this curvature assumption, the former p q boundedness results may be improved by a factor λ /p. We refer to [, Chapter IX] and [, Chapter ] for a more detailed exposition of such results. et us start by recalling this assumption: suppose that.) holds, then Σ U x 0 = { x ϕx 0, y) : y V } T x 0 U Σ V y 0 = { y ϕx, y 0 ) : x U } T y 0 V are hypersurfaces in the respective cotangent spaces. This is also equivalent to the fact that dπu : T C ϕ) T T U) has rank.

6 6 DOS SANTOS FERREIRA, KENIG, SAO q q = p n+ n 0 + n p Figure. Admissible exponents in Theorem.4 and Corollary.3 Carleson-Sjölin Assumption. Both hypersurfaces Σ U x 0 and Σ V y 0 have everywhere non-vanishing Gaussian curvature for all x 0 U and y 0 V. Under the n n Carleson-Sjölin hypothesis, we have the following boundedness result [, Corollary..3]. Theorem.4. Suppose that the non-degeneracy assumption.3) is satisfied and suppose that the n n Carleson-Sjölin condition holds. Then for any compact set K V there exists a constant C > 0 such that for all λ and all u C 0 K).4) with q = n+ n p and p. T λ u qrn) Cλ n/q u prn) The range of admissible exponents in this theorem is represented by the red line in figure. et us finish by the following important remarks. Remark.5. If the amplitude a depends on parameters, the estimates in the theorems are uniform with respect to the parameters as long as the amplitude is supported in a fixed set U V and is uniformly bounded as well as all its derivatives. Similarly if the phase ϕ depends on parameters, the estimates remain uniform as long as all its derivatives are uniformly bounded and either there is a uniform lower bound on a minor of the determinant of the mixed Hessian in.3) in the case of Theorem. and Corollary.3,

7 p RESOVENT ESTIMATES 7 or there is a uniform lower bound on the Gaussian curvature of the hypersurfaces in the case of Theorem.4. Remark.6. Although Theorems.3 and.4 are stated for oscillatory integral operators T λ with amplitudes a C0 U V ) with constants that depend on the compact set K = supp a, they are still valid with constant depending on R, Λ where we assume that { } x y : x, y) supp a B0, R) that a and all its derivatives are bounded on U V with bounds only depending on Λ and with phase ϕ satisfying non-degeneracy or curvature assumptions of the type discussed in Remark.5, uniformly on U V, with constant depending only on /Λ. By the compact support assumption on the amplitude a in U V, we have a natural extension of T λ to an operator acting on functions in R n, which gives a function on R n. We proceed as in [, pages ]. Firstly, one observes that it suffices to prove an estimate of the form.5) T λ u q Bx 0,)) Cλ s u p Bx 0,r)) with a constant C uniform with respect to x 0 R n and some radius r depending only on R. In fact, if.5) holds, raising both sides of.5) to the q-th power q and integrating with respect to x 0 R n gives ) q B0, ) T λ u q C q λ sq ux) p p dx q dx0 x x 0 <r and by Minkowski integral inequality q p) ) q B0, ) T λ u q C q λ sq ux) p B0, r) p p q q dx so that T λ u q C ) B0, r) q λ s u p. B0, ) Secondly, the estimate.5) follow from the p q Theorems.3 and.4 discussed in Remark.5 because the operator T λ does not move too much the support: let χ C0 B0, )), resp. ψ C 0 B0, r) be cutoff functions which equal one on B0, ), resp. B0, r). Then one has χx x 0 )ax, y) = χx x 0 )ax, y)ψy y 0 ) for r large depending on R and T λ u q Bx 0,)) χ x 0 )T λ u q = χ x 0 )T λ ψ x 0 )u q. Finally, the estimate.5) follows from the p q boundedness results on the oscillatory integral operator χx)ax + x 0, y + y 0 )ψy)e iλϕx+x 0,y+y 0 ) uy) dy which are uniform in x 0 by our assumptions on a, ϕ.

8 8 DOS SANTOS FERREIRA, KENIG, SAO 3. Hadamard s parametrix We follow [8], and use Hadamard s parametrix [9, Section 7.4] to prove the resolvent estimates. We first introduce the following sequence of functions F ν x, z) = ν! π) n e ix ξ ξ dξ, + z) +ν ν N R n including a fundamental solution F 0 of +z) where is the flat aplacian on R n. We used for the Euclidean norm recall that g denotes the norm induced by the Riemannian metric). These are radial functions and in polar coordinates, the equation on F ν reads + z)f ν = r F ν n r F ν + zf ν = r { δ 0 when ν = 0 νf ν when ν > 0. Besides, as can be seen from their Fourier transform, these functions satisfy 3.) r F ν = r F ν, ν > Construction of the parametrix. et x 0 M and U be a neighbourhood of x 0 in M. Since the construction is local, we can think of U as a ball in R n, and work in coordinates. If U is small enough, the distance function r = d g x, y) is smooth on the product U U with the diagonal removed, and furthermore one can take polar normal coordinates for x in U with center at y. In polar coordinates the volume form takes the form x = exp y rθ), θ T y M dv g = r n Jr, θ) dr dθ where dθ denotes the canonical measure on the unit sphere S y M of the tangent space T y M, gy)). The aplacian of the distance function r = d g x, y) is given by gr = n + rjr, θ) r Jr, θ) and this implies for a radial function g fr) = f r) dr g + f r) g r = f r) + n f r) + rj r J f r). This identity holds in the classical sense when x y and in the distribution sense on U. If we use those computations on the function α 0 F 0, we get g + z)α 0 F 0 ) = α 0 δ 0 r α 0 + ) rj J α 0 r F 0 g α 0 )F 0 We refer the reader to [6, section 4.B] for those computations.

9 and on the function α ν F ν, ν > 0 using 3.) g + z)α ν F ν ) = r r α ν + in D U). Thus, if we set F x, y, z) = p RESOVENT ESTIMATES 9 ν + r rj J N α ν x, y)f ν dg x, y), z ), ν=0 )α ν ) F ν g α ν )F ν then we have g + z)f = α 0 δr) r α 0 + ) rj J α 0 r F 0 N + r r α ν + ν + r ) rj )α ν g α ν F ν g α N )F N J ν= in D U), where the derivatives were taken with respect to x. Here δr) stands for the pullback of the Dirac mass δ 0 on R by the map x d g x, y), this can be explicitly computed 3.) 3.3) δr) = det gy) δ y x). If we choose the coefficients α ν to be solutions of the equations r r α ν + then the function F satisfies: 3.4) r α 0 + rj J α 0 = 0 ν + r ) rj α ν = g α ν, J g + z)f = α 0 δr) g α N )F N. The equation 3.) can be explicitly solved by taking α 0 = det gy) /4 = Jr, θ) ν N det gy) detexp y g)exp y x) ) 4. Note that the computations that we just made are not coordinate invariant, neither is the quantity det g contrary to the volume form) so the choice of α 0 may be understood in the following manner: first pick normal coordinates in x depending on y x, y) exp y x), y) then α 0 depends on the ratio of the determinant of the metric expressed in the coordinates in y and of the determinant of the metric expressed in the normal coordinates depending on y!) in x that we have just picked. Having given those precisions, it is clear that the function α 0 is smooth and satisfies α 0 y, y) =.

10 0 DOS SANTOS FERREIRA, KENIG, SAO Setting α ν = α 0 α ν and β ν = α 0 gα ν reduces the equation 3.3) to r r α ν + ν α }{{ ν = } β ν, ν N. =r ν rr ν α ν) In polar coordinates, this is explicitly solved by r α ν = r ν t ν βν exp y tθ) dt = 0 0 t ν βν exp y rtθ) dt, ν. By induction, one can solve the equations on α ν by taking α ν = α 0 0 t ν α 0 gα ν ) γx,y t)) dt. where γ x,y is the distance minimizing geodesic from y to x this is well defined if the neighbourhood U of x 0 is small enough). These functions are smooth on U. et χ C0 U U) be a symmetric function which equals one near the diagonal, we get using our computation 3.4) [ ] 3.5) g + z) χ, y)f, y, z) = χy, y) det gy) δ y + [χ, y), g ]F, y, z) + χ, y) g α N )F N dg, y), z ). }{{} =H N x,y,z) Note that [χ, y), g ] = grad g χ, y) is a first order differential operator whose coefficients are supported in the support of χ and away from the diagonal x = y. We are ready to consider Hadamard s parametrix T Had z)u = χx, y)f x, y, z)uy) dv g y) which satisfies 3.6) M g + z)t Had z)u = χx, x)u + Sz)u with Sz) = grad g χ, y) T Had z) + S z) = S z) + S z) and S z) = H N x, y, z)uy) dvg y). M The integer N will be chosen, in the next paragraph, large enough so that S z) is smoothing. Given the fact that the function F y, x, z) = N α ν y, x)f ν dg x, y) ) ν=0 behaves in a similar fashion to F x, y, z) the only lack of symmetry comes from the coefficients α ν whose only relevant property is their smoothness), the transpose t T Had z) shares the same boundedness properties than T Had z).

11 p RESOVENT ESTIMATES It is therefore not misleading to think of the Hadamard parametrix as a symmetric operator in terms of its boundedness properties. 3.. Bessel functions. In this paragraph we describe the behaviour of the functions F ν see [, page ], [8, emma 4.3]). They can be explicitly computed in terms of Bessel functions F ν r, z) = c ν r n +ν+ z n 4 ν+ ) 3.7) Kn/ ν zr where K n/ ν are Bessel potentials K m w) = 0 e w cosh t coshmt) dt, Re w > 0. The qualitative properties of K m are as follows K m w) C m w m when w and Re w > 0, K m w) = a m w)w e w when w and Re w > 0, where the functions a m have uniform estimates of the form α r α a m r w ) 3.8) C α,m r α, α N w when r. We sum up the well known properties of the function F ν obtained from the explicit formula 3.7) in the following lemma. emma 3.. There is a constant C > 0 such that Furthermore, one has F ν r, z) Cr n++ν when r z. F ν r, z) = z n 4 ν+ e zr r n +ν a ν r, z) where the functions a ν have a symbolic behaviour α a ν r, z) rα C α,νr α, α N when r z. The constants are all uniform with respect to z C, z c. 3.9) In particular, if N > n )/ then by emma 3. we have when z δ. We also recall that F x, y, z) = F N r, z) z / N α ν x, y)f ν dg x, y), z ) ν=0 with smooth coefficients α ν. Thus from emma 3. we deduce bounds and asymptotics on the function F, which we synthesize in the following lemma.

12 DOS SANTOS FERREIRA, KENIG, SAO emma 3.. There is a constant C > 0 such that 3.0) Furthermore, one has 3.) F x, y, z) Cd g x, y) n+ when d g x, y) z. F x, y, z) = z n 4 e z d gx,y) d g x, y) n ax, y, z) where the function a has a symbolic behaviour α x,yax, y, z) C α d g x, y) α, α N when d g x, y) z. The constants are all uniform with respect to z C, z c. 4. Resolvent estimates This section is devoted to the proof of p estimates on the resolvent. 4.. Parametrix estimates. Our goal in this paragraph is to prove that the Hadamard parametrix is bounded on certain ebesgue spaces. Due to the local nature of the construction, the kernel of the parametrix is supported in U U with U a small neighbourhood of a point x 0 M; using local coordinates, we might as well suppose that x 0 = 0 and that U is a small ball in R n of radius ε > 0. Theorem 4.. The Hadamard parametrix is a bounded operator 4.) z s T Had z) : p M) q M) with a norm uniform with respect to the spectral parameter z C, z when 0 s, p q 4.) p q + s n = n, and min p, ) > q, n + < p q n. Remark 4.. The region of admissible exponents in Theorem 4. is the trapezium CC D D blue quadrilateral in figure 3) with vertices C = +, 3 ), C = + 3, ). D = +, n ) ) n, D + 4n = n + ) n + ), ), Note that is the middle of [CC ]. F = + n +, ) n +

13 p RESOVENT ESTIMATES 3 q q = p F D C 0 B D C + n q = p n B n A p Figure 3. Admissible exponents in Theorem 4. et ψ 0 C0 R) be supported in [, ] and equal one on [, ], let ψ = ψ 0 /) ψ 0 C0 R) be supported in [, ] [, ], we consider the following dyadic partition of unity ψ 0 r) + ψ ν r) =. ν=0 We denote ψ ν = ψ ν ) if ν and decompose Hadamard s parametrix in the following way where T ν z)ux) = We first observe that M T Had z) = T 0 z) + T ν z) ν= χx, y)ψ ν z dg x, y) ) F x, y, z)uy) dv g y). 4.3) d gx, y) = G jkx, y)x j y j )x k y k ) where Gx, x) = gx) for all x U. Indeed, the square of the distance function vanishes at order two at x = y and its Hessian is twice the metric since [ d g, y) ] θ, θ) = x=y t d gexp y tθ, y) = θ t=0 g.

14 4 DOS SANTOS FERREIRA, KENIG, SAO In particular, in the chart U the geodesic distance is equivalent to the Euclidean distance, i.e. 4.4) C x y d gx, y) C x y. when x, y U. et us begin by examining the term T 0 z): using the bound 3.0) in emma 3., we majorize the kernel by a constant times x y n+ x y C z /. Using Young s inequality when 0 /p /q < /n and Hardy-ittlewood- Sobolev s inequality when /p /q = /n, and scaling the estimates, bearing in mind the condition 4.), we get 4.5) z s T 0 z) p, q ) z n + n s n + p q ) = when 0 /p /q /n excluding the endpoints 0, /n) and /n, 0) of the segment /p /q = /n. Now we deal with the other terms: on the support of the kernel of T ν z) we have d g x, y) ν z / and if we use the asymptotic description 3.) in emma 3., the operator T ν z) assumes the form T ν z)ux) = z n 4 If we denote then we have 4.6) M e zd gx,y) ax, y, z) χx, y)ψ d g x, y) n ν z dg x, y) ) uy) dv g y). Ax, y, z) = e Re z dgx,y) d g x, y) n ax, y, z)χx, y) det gy) x,ya α = O d g x, y) n α ) uniformly in z. We need to distinguish two further cases: arg z [ π/, π/] where the exponential is uniformly decaying and arg z / [ π/, π/] where the exponential has an oscillating behaviour. et us begin by the first case which is straightforward: thanks to 4.4) the kernel of T ν z) may be bounded by a constant times z n n ν e c z / x y and Young s inequality provides the bound z s T ν z) p, q ) n ν e cν.

15 p RESOVENT ESTIMATES 5 This together with 4.5)) can be summed as a geometric series z s T Had z) p, q ) z s T ν z) p, q ) ν=0 ν=0 n ν so it only remains to consider the case where arg z / [ π/, π/]. The case p q > +. We majorize the kernel by a constant times z n ν n x y c ν z / and using Young s inequality we get )) z s T ν z) p, q ) ν n+ +n q p. As above we can sum a geometric series and obtain the boundedness of the z s T Had z) T 0 z)) as long as the exponent is positive, i.e. when p q > +. This region is in the plane /p, /q) the triangle ABB delimited by the purple lines in figure 3). The other cases. We first observe that, because of the support properties of the kernel, the only terms T ν z) which are nonzero are those for which ν z / is bounded, and in fact even small if one is prepared to shrink the size of U. We consider the following rescaled distance function ϱ ν x, y, z) = z ν d g ν z x, ν z ) y = G jk x y and the following rescaled operator T ν z)ux) = z n ν n ) ν z x, ν z y x j y j )x k y k ) e iν ϕ νx,y,z) a ν x, y, z)uy) dy which was obtained by the contraction x, y) ν z x, ν z y ). The phase is given by ϕ ν x, y, z) = ν Im z d g ν z x, ν z ) y ) arg z = sin ϱ ν x, y, z) and the amplitude by a ν x, y, z) = z n 4 ν n A ν z x, ν z y, z ) ψ ϱν x, y, z) ).

16 6 DOS SANTOS FERREIRA, KENIG, SAO With those notations, we have T ν z)ux) = ν z ) n Tν z)v ν z x ), vx) = u ν z x ). Because of 4.6) and because ν z /, both phase and amplitude are uniformly bounded as well as all their derivatives. Besides, the amplitude a ν,, z) is compactly supported in R n R n with possibly a very large support) but the set {x y : x, y) supp aν,, z) } is contained in a fixed compact set of R n. This is an oscillatory integral operator, whose phase is a rescaled version of) the Riemannian geodesic distance, and the previous observation shows that part of the assumptions in Remark.6 are fulfilled. Besides we have ) ϕ ν arg z x y = sin }{{} / x y g jk x 0 )x j y j )x k y k ) + Oε) this means that the non-degeneracy condition.3) is satisfied if ε is taken small enough. Corollary.3 applies 4.7) T ν z)u p M) z n ν n νn )/p u p M) and after rescaling, we obtain ) z s T ν z) p, p ) z / ν ) n p p z n ν n νn )/p ) ν n+ p 4.8) n. Again, we can sum those estimates into a geometric series provided that p > + n +. This shows that the operator z s T Had z) T 0 z)) is uniformly bounded on the semi-open segment [AF ) in figure 3. Since the distance function r = d g, y) satisfies the eikonal equation dr g = its differential parametrizes a piece of the cosphere bundle, thus 4.9) Σ y0 = { d x d g x, y 0 ), x U } S x 0 M has everywhere non-vanishing Gaussian curvature. This is also true when x and y are interchanged because of the symmetry of the function. This remains true after rescaling and it is not hard to see that there is a uniform lower bound on the Gaussian curvature when ε is small enough. This means that the Carleson-Sjölin condition is satisfied in its uniform variant mentioned in Remark.6) and Corollary.4 applies 4.0) T ν z)u q M) z n ν n νn/q u p M)

17 p RESOVENT ESTIMATES 7 if q = n + )p /n ) and p. After rescaling we finally obtain ) z s T ν z) p, q ) z / ν ) n p q z n ν n νn/q 4.) ν n p n+ Those estimates can be summed into a geometric series when ). p > +. This shows that the Hadamard parametrix is bounded on the red segment [AC) in figure 3. If we sum up the results obtained so far: we have shown the boundedness of z s T Had z) T 0 z)) on the segments [AB) by Young s inequality), [AD) by the Carleson-Sjölin theory), [AF ) by the non-degeneracy corollary.3) in figure 3. By interpolation and duality, this shows that z s T Had z) T 0 z)) is bounded on the pentagon ABDD B in figure 3. This ends the case arg z / [ π/, π/] and hence the boundedness of Hadamard s parametrix 4.). This completes the proof of Theorem 4.. Remark 4.3. In fact, the computation made to obtain the bound on the segment [A, F ) is redundant since the bound can be obtained by interpolation and duality from the bound on the segment [A, D). 4.. Additional bounds. If one is prepared to loose some powers of the spectral paramater z, one can improve the range of allowed exponents. Indeed, the estimate 4.) can still be summed on ν z / when p < + z s T Had z) p, q ) z s T ν z) p, q ) ν=0 ν 0 : ν z / ) ) ν n+ n n+ p z 4 n p. Note that when q = n+ n p we have n + ) p ) = q p n ) and therefore ) z s+ n+ 4 n p ) = z n 4 p q. The values of /p, /q) obtained in this estimate correspond to the semiopen segment DE] on the figure 6. Similarly, the estimate 4.8) can still

18 8 DOS SANTOS FERREIRA, KENIG, SAO q = = q p q p G E E F D C 0 B D C + n q = p n B n A p Figure 4. Admissible exponents in Theorem 4.4 be summed when p < + n+ z s T Had z) p, p ) z s T ν z) p, p ) ν=0 Note that we have n + ) p ) p ν 0 : ν z / ν n+ p + ) = p + n + ) and therefore we retrieve the same bound as above ) z s+ n+ ) p n 4 = z n 4 p q. ) ) n n+ z p n 4. The values of /p, /q) obtained in this estimate correspond to the semiopen segment F G] on the figure 6. By duality and interpolation, we get the following theorem. Theorem 4.4. The Hadamard parametrix is a bounded operator 4.) when p q and T Had z) : p M) q M) p q < n +, n n + p q n + n p,

19 with a norm bounded by 4.3) p RESOVENT ESTIMATES 9 T Had z) p, q ) C z n 4 ) p q. The extended set of admissible exponents is the pentagon DEGE D, represented by the union of the green and red sets in figure 6. These estimates or rather the endpoint p =, q = + )/n )) were proved by Sogge in [8] T Had z)u +) z n+3 4n+) u M). n M) σ n n 4 0 n+ p q n n+ n+ Figure 5. Decay of the parametrix: T Had z)u p, q ) = O z σ ) The combination of Theorems 4. and 4.4 gives the following bound on the parametrix 4.4) T Had z)u p, q ) C z σ in the polygon CDEGE D C except for the segments [CD], [DD ] and [D C ]), where the order σ is a piecewise linear function of d = /p /q n d + when 0 d 4.5) σ = 4 n + n d + when. n + d The graph of this function is represented in figure 5. We finish by observing that as a function of the y variable, the kernel of the T Had z) T 0 z) is r -integrable when r < /n ) since T Had z) T 0 z) ) x, y) z n 3 4 dg x, y) n.

20 0 DOS SANTOS FERREIRA, KENIG, SAO By Young s inequality, this provides the trivial bound T Had z) T 0 z))u M) z n 3 4 u p M), p < +, and by interpolation, we obtain the following additional bounds T Had T 0 )z)u q M) C z n 3 4 n q u p M) if q n n + p and p < +. Since T 0 z) satisfies similar estimates with better decay in z when /p / + /, the previous estimates remain true for the Hadamard parametrix. These estimates with their dual provide the following additional boundedness properties of the Hadamard parametrix. emma 4.5. et p q be such that /p /q /n, the Hadamard parametrix satisfies the following bounds z n 3 4 n q if q T Had z) q, p ) C n n+ p and p < + z n 3 4 n p if q n+ n p and q >. The range of exponents covered by this theorem is the union of the two violet trapezia in figure 6. q q = p q = p G E E F D C 0 B D C + n q = p n B n A p Figure 6. Extended set of admissible exponents

21 p RESOVENT ESTIMATES In particular, we have 4.6) T Had z)u n M) z 4 u M) T Had z)u M) z 4 u n+ M). These estimates will prove useful in the final argument proving the resolvent estimates when dealing with the remainders Remainder estimates. We now deal with the remainder term Sz): the results are similar than for the Hadamard parametrix in fact the range of admissible exponents is larger) but the proof is simpler due to the lack of singularities since the kernel is supported away from the diagonal in M M. emma 4.6. The operator Sz) defined in 3.6) is a bounded operator 4.7) Sz) : p M) q M) when p q with a norm bounded by z n 4 n q if ) q n n+ Sz) p, q ) C z n 4 p q if n n+ 4 n p if q n+ z n p p q n+ n Proof. The kernel of S z) is uniformly bounded by z / because of 3.9), hence S z) is a bounded operator from p M) to q M) with norm bounded by z /. For this part of the operator we actually get better bounds than expected since z δ. We now concentrate on the part S z) of the operator: because of emma 3. and the support of grad g χ, y), the kernel of this operator looks like z n 4 e z d gx,y) bx, y, z) where b is a smooth function. When arg z [ π/, π/], Young s inequality provides a better bound ) S z)u q M) z n+ 4 + n p q e c z / u p M). When arg z / [ π/, π/], the bound follows from Young s inequality, Theorems. and.4, and duality and interpolation Resolvent estimates. Before actually turning our attention to resolvent estimates, let us first patch our local constructions into a global parametrix. We cover the manifold M with finitely many open geodesic balls U j of radius ε contained in charts of M. We consider a partition of unity = J χ j, j= supp χ j U j n p p,.

22 DOS SANTOS FERREIRA, KENIG, SAO subordinated to the covering U j ) j J, and define T j) Had z) to be the local Hadamard parametrix constructed in section 3 using χ j x) χ j y) as the cutoff function. By a slight abuse of notation, we keep T Had z) to denote the global parametrix J T Had z) = T j) Had z) and similarly for the remainder Sz) = j= J S j) z). j= Having constructed those operators, we indeed get a global right parametrix 4.8) g + z)t Had z) = Id +Sz). As a finite sum of operators, T Had z) shares the same continuity properties as the local parametrices, and this is also true of Sz). We are now ready to prove the resolvent estimates. We use ideas coming from [4] and also [, 3] to deal with the remainder terms estimates. et 0 = λ 0 λ λ k... be the sequence of eigenvalues of the positive) aplacian g repeated with multiplicity and ψ k ) k=0 be the corresponding sequence of unit eigenfunctions. We denote fk) = f ψ k dv g M the Fourier coefficient of the function f corresponding to the eigenfunction ψ k. emma 4.7. et M, g) be a compact Riemannian manifold without boundary) of dimension n 3, for all z C \ R we have u M) z Re z) g + z)u M). Proof. We start with the factorization which implies λ k + z = λk + i z ) λk i z ) λ k + z λ k + z ) Re z. If f = g + z)u, using Fourier series, we get u M) = k=0 This completes the proof of the lemma. fk) z + λ k z Re z f M).

23 p RESOVENT ESTIMATES 3 Remark 4.8. When Re z δ, we deduce the following improved bound 4.9) u M) z g + z)u M). which will prove to be of crucial importance to estimate the remainder terms in the proof of Theorem.. Unfortunately, such an improved bound only holds when the spectral parameter is outside of a parabola. Indeed suppose that the estimate 4.9) holds then testing it with unit eigenfunctions ψ k implies λ k + z c z and the parameter z has to remain outside of the envelope of the curves λ k + z = c z, k N. In particular, if we choose z = λ k + iy then we have y 4 c 4 λ k + y ), and y cλ k. Besides, if one is interested in proving resolvent estimates when z lies in Ξ δ, then difficulties arise when the parameter z lies on the lines Im z = ±δ. This means that the square root of z lies on the part of hyperbola z = λ + i δ λ, λ δ see figure 7) and this implies z Re z. In other words, the estimate is weak u M) g + z)u M) in terms of the decay with respect to the size of the spectral parameter z λ n+ n estimate. We now prove the n+ n Theorem.. We start from where Note that by 4.8) we have 4.0) We start our estimations u = T Had z) g + z)u + v v = Id T Had z) g + z) ) u. g + z)v = Sz) g + z)u. u n M) T Hadz) g + z)u n M) + v n M) estimate of

24 4 DOS SANTOS FERREIRA, KENIG, SAO 5 Ξ δ Im z=c 4 3 z, z Ξδ Ξ δ Figure 7. Values of the spectral parameters z Ξ δ and z and by the boundedness properties of the Hadamard parametrix given in Theorem 4., we have u n M) g + z)u n+ M) + v n M). To estimate the second right hand-side term, we need the following lemma. emma 4.9. et M, g) be a compact Riemannian manifold without boundary) of dimension n 3, and let δ be a positive number. For all z Ξ δ we have 4.) v n M) C z 4 g + z)v M). Proof. We use the adjoint of Hadamard s parametrix as a left parametrix v = T Had z) g + z)v S z) v and get the following estimate by the boundedness properties of the Hadamard parametrix given in Theorem 4.4 more precisely 4.6), and of the remainder given in emma 4.6 v n M) z 4 g + z)v M) + z 4 v M). The proof of 4.) is completed once one has controlled the second righthand side term using the bound obtained in emma 4.7 This ends the proof of the lemma. v M) z g + z)v M). Using the previous lemma and the identity 4.0), we get u n M) g + z)u n+ M) + z 4 Sz) g + z)u M).

25 p RESOVENT ESTIMATES 5 It is now a matter of using the boundedness properties of the remainder Sz) given in emma 4.6 to conclude that u n M) g + z)u n+ M). This completes the proof of Theorem.. 5. Relation with p Carleman estimates The aim of this section is to illustrate the relations between resolvent estimates and analogues of the p Carleman estimates obtained in the Euclidean case by Jerison and Kenig [] for logarithmic weights) or by Kenig, Ruiz and Sogge [] for linear weights). The proof of Carleman estimates for limiting Carleman weights in [5] is based on integration by parts and can not be used in the p setting. However in [4], we were able to prove such estimates following an idea of Jerison [0], see also [8, Section 5.]) using spectral cluster estimates of Sogge [8]. Here we present an alternative argument following Kenig, Ruiz and Sogge [] and Shen [7] and reducing the Carleman estimate to resolvent estimates. imiting Carleman weights on an open Riemannian manifold N, g) are smooth functions ϕ such that dϕ 0 on N and { } pϕ, p ϕ x, ξ) = 0, x, ξ) p 5.) ϕ 0) T N if p ϕ denotes the following symbol p ϕ x, ξ) = ξ g dϕ g + i dϕ, ξ g. This a conformally invariant property. This notion was introduced in [3] which dealt with Calderón s inverse conductivity problem with partial data in dimension n 3; this article was concerned with the isotropic setting and took advantage of replacing classical linear weights by logarithmic weights which are examples of limiting Carleman weights in the Euclidean setting). The motivation for introducing such weights in the context of general Riemannian manifolds lies in the application to inverse problems [3, 5, 4] where solutions to the Schrödinger equation with opposite exponential behaviours are constructed on manifolds using complex geometrical optics. It was proved in [5, 5] that the condition 5.) is in fact stringent. Simply connected Riemannian manifolds which admit limiting Carleman weights are those which are conformal to one having a parallel field i.e. simultaneously a Killing and a gradient field). In particular, such manifolds are locally conformal to the product of an Euclidean interval and another open Riemannian manifold. The results in [5, 4] are concerned with the simpler situation of manifolds conformal to global products of the Euclidean line with another Riemannian manifold. This is the situation in which we choose to set ourselves to underline the connection between resolvent and Carleman estimates.

26 6 DOS SANTOS FERREIRA, KENIG, SAO The setting is the product N = R M 0 of the Euclidean one dimensional) line and of an n )-dimensional compact Riemannian manifold M 0, g 0 ) without boundary, endowed with the product metric g = dx + g 0. We consider the aplace-beltrami operator on N P = g = x + g0. A natural limiting Carleman weight on this product manifold is x and the corresponding conjugated operator reads e τx P e τx = x τ x + τ + g0. Theorem 5.. et N = R M 0 be the product of the Euclidean line and of an n )-dimensional compact manifold M 0, g 0 ) endowed with the product metric g = dx + g 0. For all compact intervals I R, there exist two constants C, τ 0 > 0 such that for all τ R with τ τ 0, we have 5.) e τx u n N) C eτx P u n+ N) when u C 0 N) is supported in I M 0. This Carleman estimate was obtained in [4], and in [7] when M 0 = T n is the n dimensional torus, by a different method, which uses as well the spectral cluster estimates of Sogge but on n dimensional manifolds. By translating and scaling the estimate in the first variable, it is always possible to assume I = [0, π] without loss of generality, which we do since this will lighten our notations. The proof follows [] and is based on the construction of an inverse operator of the conjugated operator 5.3); to ease such an inversion, inspired by [8] see also [6, Section 3.]), we further conjugate the operator by a harmless oscillating factor 5.3) e τx i x P e τx + i x = D x + ) + iτ D x + ) τ g0. We regard functions u C0 0, π) M 0) as smooth periodic functions in the first variable. This corresponds to a change of perspective by replacing the manifold N = R M 0 by the product M = T M 0 of the one dimensional torus T = R/πZ and of the manifold M 0, g 0 ). We denote by λ 0 = 0 < λ λ... the sequence of eigenvalues of g0 on M 0 and ψ k ) k 0 the corresponding sequence of eigenfunctions forming an orthonormal basis of M 0 ) g0 ψ k = λ k ψ k. We denote by π k : M 0 ) M 0 ) the projection on the linear space spanned by the eigenfunction ψ k so that π k = Id, λ k π k = g0. k=0 k=0

27 p RESOVENT ESTIMATES 7 The eigenvalues of the aplacian g on T M 0 are j + λ k ) with j Z, k N and the corresponding eigenfunctions are 3 e ijx ψ k. We denote by π j,k : M) M) the projection on the linear space spanned by the eigenfunction e ijx ψ k : π j,k fx) = π ) e ijy π k fy, x ) dy e ijx, π and define the spectral clusters as χ m = 0 m j +λ k <m+ π j,k, m N. Note that these are projectors χ m = χ m. We end this paragraph by recalling the spectral cluster estimates of Sogge [8, 9] that we will need: 5.4) χ m u n M) C + m) u M) χ m u M) C + m) u n+ M). The two inequalities are dual to each other and can be found in [8, Corollary 5..]. We are now ready to reduce the proof of Carleman estimates to resolvent estimates. Recall that our goal is to prove 5.5) u n M) C f n+ M) when u C0 π, π) M 0) and D x + 5.6) u + iτ ) D x + ) u g0 u τ u = f. The equation 5.6) is actually easy to solve: writing f = j,k π j,kf and similarly for u, the equation formally becomes j + ) + iτ j + ) ) τ + λ k π j,k u = π j,k f for j Z and for k N. The symbol on the left is always nonzero provided that τ. Thus, the inverse operator may be written as G τ f = j= k=0 j + π j,k f ) + i j + ) τ + λk τ. 3 Here we are using in an essential manner the fact that the metric g is a product, i.e. the fact that x is a limiting Carleman weight.

28 8 DOS SANTOS FERREIRA, KENIG, SAO We now use ittlewood-paley theory to localize in frequency with respect to the Euclidean variable x ; we have u = u ν, f = with ν=0 ν=0 u 0 = π uy, x ) dy ), π 0 π ) u ν = e ijy uy, x ) dy e ijx, ν > 0 π ν j < ν 0 and similarly for f. It suffices to prove 5.7) u ν n f ν C f ν n+ since then by summing the former inequalities and using ittlewood-paley s theory u u n ν f n ν f n n+ ν=0 and this is the inequality 5.5) we were looking for. We now concentrate on the microlocalized estimate 5.7). Because the conjugated operator 5.3) and the localization in frequency [ ν, ν )D x ) commute 4, we have u ν = G τ f ν. We denote Rz) = ν=0 D x + ) ) g0 + z the resolvent associated with the elliptic operator D x + ) g0. In the case ν = 0, we have 5.8) u 0 = G τ f 0 = R τ + iτ)f 0 so 5.7) is a resolvent estimate with z = τ + iτ. When ν, we want to evaluate on microlocalized functions the error made by freezing the operator τd x into ν τ in 5.3). This amounts to replacing G τ by the resolvent R τ + i ν + )τ). More precisely, we want to estimate the term R τ + i ν + )τ) G τ ) fν. 5.9) This can be explicitly computed R τ + i ν + )τ) G τ ) fν = j= k=0 a ν jk τ) π j,kf ν 4 Here again we are using the fact that the weight x is a limiting Carleman weight, i.e. that the metric g 0 does not depend on x.

29 p RESOVENT ESTIMATES 9 where a ν jk τ) = j + ) + iτ j + iτ ν j) [ν,ν)j) ) ) j ) τ + λ k + ). + i ν + )τ τ + λ k Using the spectral cluster estimates 5.4) and the fact that spectral clusters are projectors, we have the following string of estimates R τ + i ν ) + )τ) G τ fν n M) + m) χm R τ + i ν ) + )τ) R τ fν M) m=0 + m) sup m=0 and using again 5.4), we get R τ + i ν ) + )τ) G τ fν n M) + m) sup m=0 m j +λ k <m+ m j +λ k <m+ m j +λ k <m+ a ν jk τ) χ m f ν M) ) a ν jk τ) f ν n+ M). We now prove that the above series converges and is uniformly bounded with respect to τ and ν; we have sup a ν jk τ) ν τ m τ ) + 4 ν+ τ as well as m=0 ν τ + m) m τ ) + 4 ν+ τ ν τ t 0 t τ ) + 4 ν+ τ dt and if we perform the change of variables s = 4 ν τ t τ ) in the right-hand side integral, we obtain the bound ν τ + m) m τ ) + 4 ν+ τ ds s +. m=0 Summing up our computations, we have the error estimate R τ + i ν ) + )τ) G τ fν n f ν M) n+ M), this means that in order to obtain 5.7), it is enough to prove the resolvent estimate R τ + i ν + )τ)f ν n f ν M) n+ M) with a constant which is uniform in τ and ν.

30 30 DOS SANTOS FERREIRA, KENIG, SAO The conclusion of these computations is that Carleman estimates reduce to resolvent estimates of the form u D n + ) ) g0 M) + z 5.0) u with z = τ + iϱτ ϱ ). n+ M) After changing u into e i x u in 5.0), the resolvent estimate is a consequence of Theorem. since Re z = provided τ is large. Re z + z = τ τ + ϱ References []. Carleson, P. Sjölin, Oscillatory integrals and a multiplier problem for the disk, Studia Math ), [] D. Dos Santos Ferreira, Strichartz estimates for non-selfadjoint operators, Comm. Partial Differential Equations 9 004), [3] D. Dos Santos Ferreira, Sharp p Carleman estimates and unique continuation, Duke Math. J., 9 005), [4] D. Dos Santos Ferreira, C. E. Kenig, and M. Salo, Determining an unbounded potential from Cauchy data in admissible geometries, preprint 0), arxiv:04.03, 6 pages. [5] D. Dos Santos Ferreira, C. E. Kenig, M. Salo, and G. Uhlmann, imiting Carleman weights and anisotropic inverse problems, Invent. Math ), 9 7. [6] S. Gallot, D. Hulin, J. afontaine, Riemannian geometry, Springer Verlag, 993. [7] I. M. Gelfand, G. E. Shilov, Generalized Functions I: Properties and Operations, Academic Press, 964. [8] P. Hähner, A periodic Faddeev-type solution operator, J. Differential Equations 8 996), [9]. Hörmander, The analysis of linear differential operators, Springer Verlag, 986. [0] D. Jerison, Carleman inequalities for the Dirac and aplace operators and unique continuation, Adv. Math ), [] D. Jerison and C. E. Kenig, Unique continuation and absence of positive eigenvalues for Schrödinger operators, Ann. of Math. 985), [] C. E. Kenig, A. Ruiz, and C. D. Sogge, Uniform Sobolev inequalities and unique continuation for second order constant coefficient differential operators, Duke Math. J ), [3] C. E. Kenig, J. Sjöstrand, G. Uhlmann, The Calderón problem with partial data, Ann. of Math., ), [4] H. Koch and D. Tataru, Dispersive estimates for principally normal pseudodifferential operators, Comm. Pure Appl. Math ), [5] T. iimatainen, M. Salo, Nowhere conformally homogeneous manifolds and limiting Carleman weights, preprint 00), arxiv:0.507, 8 pages. [6] M. Salo, ecture notes on the Calderón problem, 008, 55 pages, available at [7] Z. Shen, On absolute continuity of the periodic Schrödinger operators, Internat. Math. Res. Notices 00, 3.

31 p RESOVENT ESTIMATES 3 [8] C. D. Sogge, Concerning the p norm of spectral clusters for second-order elliptic operators on compact manifolds, J. Funct. Anal ), [9] C. D. Sogge, Oscillatory integrals and unique continuation for second order elliptic differential equations, J. Amer. Math. Soc. 989), [0] C. D. Sogge, Strong uniqueness theorems for second order elliptic differential equations, Amer. J. Math. 990), [] C. D. Sogge, Fourier integrals in classical analysis, Cambridge University Press, 993. [] E. M. Stein, Harmonic Analysis: real variable methods, orthogonality and oscillatory integrals, Princeton University Press, 993. Université Paris 3, Cnrs, Umr 7539 aga, 99 avenue Jean-Baptiste Clément, F Villetaneuse, France address: ddsf@math.univ-paris3.fr Department of Mathematics, University of Chicago, 5734 University Avenue, Chicago, I , USA address: cek@math.uchicago.edu Department of Mathematics and Statistics, University of Helsinki and University of Jyväskylä address: mikko.salo@helsinki.fi