A semilinear Schrödinger equation with magnetic field
|
|
- Elvin Dennis
- 5 years ago
- Views:
Transcription
1 A semilinear Schrödinger equation with magnetic field Andrzej Szulkin Department of Mathematics, Stockholm University Stockholm, Sweden 1 Introduction In this note we describe some recent results by Gianni Arioli and the author [2] on the existence of nontrivial solutions of the semilinear stationary Schrödinger equation in a magnetic field (1) ( i + A) 2 u + V (x)u = g(x, u )u, x R. Here u : R C ( 2), V : R R is the scalar (or electric) potential and A = (A 1,..., A ) : R R is the vector (or magnetic) potential. Let B := curl A. For = 3 this is the usual curl operator and for general, B = (B jk ), 1 j, k, where B jk := j A k k A j. B represents the external magnetic field whose source is A. In what follows we always assume A L 2 loc (R, R ), V L 1 loc (R ) and V is bounded below. Denote A u = ( + ia) u and let := 2/( 2). Appropriate spaces in which we shall consider the problem (1) are H 1 A(R ) := {u L 2 (R ) : A u L 2 (R )} and, for 3, D 1,2 A (R ) := {u L 2 (R ) : A u L 2 (R )}. Both HA 1 (R ) and D 1,2 A (R ) are Hilbert spaces with inner product respectively A u A v + uv and A u A v (the bar denotes complex conjugation). By Section 2 of [6] and Theorem 7.22 of [10], C0 (R ) is dense in HA 1 (R ) and D 1,2 A (R ) (in [6] D 1,2 A (R ) has in fact been defined as the closure of C0 (R ) with respect to the norm corresponding to the inner product above). Supported in part by the Swedish Research Council. 1
2 Let g(x, u ) c(1 + u 2 2 ), F (x, u ) := u 0 g(x, s)s ds and consider the functional (2) J(u) := 1 A u 2 + V u 2 F (x, u ). 2 Suppose u HA 1 (R ). By the diamagnetic inequality u (x) A u(x) a.e. in R (see e.g. Theorem 7.21 in [10]), u H 1 (R ) and therefore u L p (R ) for any p [2, ] (for any p [2, + ) if = 2). It follows that whenever V L β (R ), where β /2 (β > 1 if = 2), then J C 1 (HA 1 (R ), R) and critical points of J are weak solutions of (1). We note also that J(e iθ u) = J(u) for any θ R, hence J is S 1 -invariant. Suppose A, à L α loc (R, R ) for some α [1, + ) and curl A = B = curl à (in the 1,α sense of distributions). Then à A = ϕ for some ϕ Wloc (R ), see Lemma 1.1 of [9]. It is easy to see that if ũ = e iϕ u, then Ãũ = e iϕ A u and hence Ãũ 2 = A u 2. It follows that if u H 1 A (R ), then ũ H 1 à (R ) and if u satisfies (1), then so does ũ with A replaced by Ã. The above properties are called the gauge invariance and they reflect the fact that the magnetic field B and not the particular choice of the vector potential A should be essential. The transformation u ũ is called the change of gauge. ote that there is a trivial change of gauge u ũ = e iθ u, where θ is a constant. Then à = A and it is a consequence of this property that J is S 1 -invariant. While there is a vast literature concerning the Schrödinger equation (1) with A = 0, to the best of our knowledge there are very few papers dealing with the magnetic case [6, 11, 12]. Also in [5, 8] the magnetic case has been considered, but from a very different point of view (semiclassical limits and related concentration phenomena). Denote A := ( i +A) 2. Since V is bounded below, so is the spectrum σ( A +V ) in L 2 (R ). Suppose F 0. If 0 / σ( A + V ), then either σ( A + V ) (0, + ) and the functional has a mountain pass geometry, or σ( A + V ) (, 0) and then J has a geometry of linking type. In what follows p will denote the usual L p -norm in R, σ( A + V ) the spectrum of A + V in L 2 (R ) and B(a, r) the open ball centered at a and having radius r. 2 The results First we consider a minimization problem in R, 3. Let A u (3) S 2 + V u 2 := inf u 2. u D 1,2 A ( )\{0} Our first result is a slight generalization of Theorem 3.7 in [6]. Theorem 1 If V 0, V L /2 loc (R ) and A L loc (R, R ), then the infimum in (3) is attained if and only if V 0 and B = curl A 0. 2
3 ote that since V is only in L /2 loc (R ), V u 2 need not be finite for all u D 1,2 A (R ). However, it is finite for u C0 (R ) and therefore the minimization problem (3) makes sense. ote also that if S is attained at some u D 1,2 A (R ), then u is a solution of (1) with g(x, u ) = S u 2 2 ; hence v = S 1/(2 2) u solves (1) with g(x, u ) = u 2 2. Theorem 2 Suppose 4, V L 1 loc (R ), V := max{ V, 0} L /2 (R ), A L 2 loc (R, R ) and σ( A + V ) (0, + ). If there exists x R such that V (x) c < 0 in a neighborhood of x and A is continuous at x, then the infimum of (3) is attained for some u H 1 A (R ) \ {0}. Since σ( A +V ) (0, + ), it follows that if S is attained, then it is positive. Indeed, S 0 and if S = 0 is attained at some u 0, then u is an eigenvalue of A + V which is impossible. In the next theorems we shall need the following assumptions: A1 V L (R ), g C(R R +, R) and A L 2 loc (R, R ). A2 V, g and B = curl A are 1-periodic in x j, 1 j. A3 g(x, 0) = 0. A4 There are constants C > 0 and p (2, ) (p > 2 if = 2) such that g(x, u ) C(1 + u p 2 ) for all x, u. A5 There is a constant µ > 2 such that 0 < µf (x, u ) g(x, u ) u 2 whenever u 0. A6 There are constants C, ε 0 > 0 such that g(x, u + v )(u + v) g(x, u )u C v (1 + u p 1 ) whenever v ε 0, where p is as in (A4). ote that in view of the definition of F, (A5) is the usual superlinearity condition. Since B jk = j A k k A j in the sense of distributions, the periodicity of B should be interpreted as B( ) B( + e j ) being the zero distribution for any element e j of the standard basis in R. It is also clear that according to (A3), (1) has the trivial solution u = 0. Theorem 3 If 0 / σ( A + V ) and conditions (A1)-(A5) are satisfied, then equation (1) has a nontrivial solution u H 1 A (R ). A corresponding result is well-known for the Schrödinger equation with A = 0 (see e.g. [7, 14] and the references there). Finally we shall exploit the S 1 -invariance of J in order to show the existence of infinitely many solutions of (1). Theorem 4 If 0 / σ( A + V ) and conditions (A1)-(A6) are satisfied, then equation (1) has infinitely many geometrically distinct solutions. 3
4 By geometrically distinct we mean such u, v that v e iθ u for any θ R and v T z u for any z Z, where T z is a certain operator corresponding to the translation by elements of Z in the nonmagnetic case. A more precise definition will be given in the next section. The above result should be compared to the one contained in [3, 7], where A was equal to 0. We would also like to mention that each of the following conditions is sufficient for σ( A + V ) to be contained in (0, + ) (see [2]): P1 A L loc (R ), V L 1 loc (R ), where 3, and there exists a bounded set Ω R and a constant c > 0 such that V (x) c for all x / Ω and inf x Ω V (x) > Sµ(Ω) 2/. P2 A W 1, loc (R, R ), V L 1 loc (R ) and there exists a constant c > 0 such that inf x V (x) > c and either j A k k A j c a.e. in R or j A k k A j c a.e. in R for some j, k {1,..., }. Here (4) S := inf u D 1,2 ( )\{0} u 2 + V u 2 u 2 is the Sobolev constant for the embedding D 1,2 (R ) L 2 (R ) and µ(ω) is the measure of Ω. 3 Outline of proofs An important role in the proofs is played by the following two results: Proposition 1 (Diamagnetic inequality [10, Theorem 7.21]) If u H 1 A (R ) (resp. u D 1,2 A (R )), then u H 1 (R ) (resp. u D 1,2 (R )) and u (x) u(x) + ia(x)u(x) for a.e. x R. Proof (5) Since A is real-valued, ( u (x) = Re u ū ) = u ( Re ( u + iau) ū ) u + iau. u See [10] for more details. Proposition 2 Let A L 2 loc (R, R ) and suppose u n u in D 1,2 A (R ). Then, up to a subsequence, u n u a.e. in R and u n u in L q loc (R ) for any q [2, ). The same conclusion holds if u n u in H 1 A (R ). Proof By the diamagnetic inequality the injection D 1,2 A (R ) L 2 (R ) is continuous, hence u n u in L 2 (R ). Moreover, u n u is bounded in D 1,2 (R ). So passing to a subsequence, u n u a.e. and u n u 0 in D 1,2 (R ). It follows from the Rellich- Kondrachov theorem that u n u in L q loc (R ). The second part of the lemma is proved similarly. 4
5 Below we shall prove Theorem 1 and briefly sketch the proofs of the other theorems. Proof of Theorem 1 ecessary condition. We first show that S = S. By the Sobolev and the diamagnetic inequalities, u 2 + V u 2 A u 2 + V u 2 S u 2 u 2, hence S S. Let ( (6) U ε (x) = (( 2)) ( 2)/4 ε ε 2 + x 2 ) ( 2)/2 and u ε (x) = ψ(x)u ε (x), where ψ C 0 (R, [0, 1]), ψ = 1 on B(0, 1/2) and ψ = 0 on R \ B(0, 1). Then (7) (ψu ε ) 2 2 u ε 2 2 = S /2 + O(ε 2 ) and u ε 2 = S/2 + O(ε ) (see e.g. [14], p. 35). Since u ε is bounded in L 2 (R ) and u ε 0 a.e., u ε 0 in L 2 (R ) as ε 0. Therefore V u ε 2 0 and Au ε 2 0 as ε 0 (recall V L /2 loc (R ) and A L loc (R, R )). Since u ε is real-valued, A u ε 2 + V u ε 2 u ε 2 + Au ε 2 + V u ε 2 u ε 2 = u ε 2 S as ε 0 and S S. ow assume that u is a minimizer normalized by u = 1. Then S = A u 2 + V u 2 A u 2 u 2 S and it follows that u(x) = U ε (x a)/ U ε for some a R (that the minimizer in (4) is unique up to translation and dilation may be seen e.g. from the proof of Theorem 1.42 in [14]). In particular, u > 0 for all x and therefore V 0. Moreover, the inequality of Proposition 1 must be an equality a.e. So by (5), the imaginary part of ( u + iau)ū must be zero which is equivalent to A = Im ( u/u). An easy computation shows that curl ( u/u) = 0. Sufficient condition. Assume V 0 and curl A = 0. Then A = ϕ for some ϕ W 1, loc (R ) according to [9] and it is easy to verify that u = U ε e iϕ is a minimizer for (3) for any ε > 0. Proof of Theorem 2 Assume without loss of generality that x = 0. Let θ(x) := j=1 A j(0)x j. Then (A + θ)(0) = 0 and by continuity (A + θ)(x) 2 c < c for all x < δ provided δ is small enough. Choosing a smaller δ if necessary we may also assume V (x) c whenever x < δ. Let U ε be as in (6) and let v ε (x) := ψ(x)u ε (x)e iθ(x), where ψ C0 (R, [0, 1]), ψ(x) = 1 in B(0, δ/2) and ψ(x) = 0 in R \ B(0, δ). By (7), A v ε 2 + V v ε 2 (ψu ε ) 2 + ψ 2 Uε 2 θ + A 2 cψ 2 Uε 2 S 2 + (c c) Uε 2 + O(ε 2 ) B(0,δ/2) 5
6 and v ε 2 = S( 2)/2 + O(ε ). Since B(0,δ/2) U 2 ε { Cε 2 log ε if = 4 Cε 2 if 5 for some C > 0 and all small ε > 0 (cf. e.g. [14], p. 35), an easy computation shows that A u S 2 + V u 2 = u 2 < S. inf u DA 1 ( )\{0} Having this, a usual argument based on the concentration-compactness lemma [14, Lemma 1.40] shows that if {u n } is a minimizing sequence such that u n = 1, then u n u in L 2 (R ) and in D 1,2 A (R ), possibly after passing to a subsequence. Hence u is a minimizer for (3). Moreover, since σ( A + V ) (0, + ), A u 2 + V u 2 ε u 2 2 for some ε > 0; therefore u D 1,2 A (R ) L 2 (R ), i.e. u HA 1 (R ). Finally we would like to point out that Lemma 1.40 in [14] must be adapted to the D 1,2 A (R )-setting. However, this is easily done by following the proof in [14] and employing Propositions 1 and 2 above. Proof of Theorem 3 Let E := H 1 A (R ) and let J be as in (2). Then J C 1 (E, R ) and J (u) = 0 if and only if u is a solution of (1). If σ( A + V ) (0, + ), then the quadratic form Q(u) := A u 2 + V u 2 is positive definite on E, otherwise E can be decomposed into the direct sum of two subspaces, E + and E, invariant with respect to A + V and such that Q is positive definite on E + and negative definite on E (cf. [13], Section 8). In the first case the functional J has the mountain pass geometry, and in the second one it has a geometry of linking type as described e.g. in [7]. Hence there exists a Palais-Smale sequence {u n } at some level c > 0 (cf. [7], Theorem 3.4 and [14], Theorems 2.9, 2.10, 6.10). Moreover, {u n } is bounded, so u n u after passing to a subsequence. By Lemma 1.7 in [7], either u n 0 in E (up to a subsequence) which is impossible because J(u n ) c > 0, or there exists a sequence {z n } in Z and r, η > 0 such that B(z n,r) u n(x) 2 η. We shall now use (A2) in order to construct a Palais-Smale sequence {v n } such that v n v 0. Since J (v n ) J (v), v is a critical point of J. By (A2), curl A(x + z) curl A(x) = B(x + z) B(x) = 0 for all z Z. It follows from Lemma 1.1 in [9] that (8) A(x + z) A(x) = ϕ z (x) for some ϕ z Hloc 1 (R ). Let (T z u)(x) := u(x+z)e iϕz(x). An explicit computation using (8) shows that T z is an isometry on E, J(T z u) = J(u) and J (T z u) = T z J (u) for each z Z. Denote v n := T zn u n. Then J(v n ) c and J (v n ) 0. Passing to a subsequence, v n v in E and, according to Proposition 2, v n v in L 2 loc (R ). Hence v is a critival point, and v 0 because v n (x) 2 = u n (x) 2 η. B(0,r) B(z n,r) 6
7 Proof of Theorem 4 Let J and E, E +, E be as in the preceding proof (E = {0} if σ( A + V ) (0, + )). Denote S θ u = e iθ u, θ S 1 = R/2πZ. Then J(S θ u) = J(u) and (as we already have seen) J(T z u) = J(u) for all θ S 1, z Z, u E. ote that S θ T z = T z S θ. Let (u) := {S θ T z u : θ S 1, z Z }. O S 1 Two solutions u, v of (1) are called geometrically distinct if they belong to different orbits, i.e. if O S 1 (u) O S 1 (v). The proof of Theorem 4 is a straightforward adaptation of that in [1]. Suppose (1) has only finitely many geometrically distinct solutions. Denote the set of critical points of J by K J, let C be a set consisting of arbitrarily chosen representatives of the orbits O S 1 (u), u K J \ {0} and K := O S 1(C) = {S θ u : θ S 1, u C}. Then K is a compact set, (9) K J \ {0} = O (K) and if F := P E +(K), where P E + is the orthogonal projection on E +, then (10) T z1 F T z2 F = whenever z 1, z 2 Z, z 1 z 2. These conditions correspond to (9) and (10) in [1]. Clearly, J is even and K, F are symmetric (i.e. K = K, F = F). From now on we consider J as an even functional and disregard the S 1 -invariance. Let U δ := E {u + E + : d(u +, T z F) < δ}, z where d(u, A) denotes the distance from u to the set A and let H be the class of mappings f : E E such that f is a homeomorphism, f( u) = f(u) for all u and f(j c ) J c for all c 1 (J c := {u E : J(u) c}). One can show that if J satisfies (9), (10) and c inf KJ \{0} J, then there exists a mapping f H such that f(j c+ε \ U δ ) J c ε provided δ and ε are small enough. This is a variant of the deformation lemma which will be needed in the minimax argument below. Fix a small ρ > 0. For a closed and symmetric A, define γ (A) = min f H γ(f(a) B(0, ρ) E+ ), where γ denotes the Krasnoselskii genus (γ is a variant of Benci s pseudoindex [4]). Let d k := inf sup J(u). γ (A) k If ρ is small enough, then J B(0,ρ) E + d > 0 and it follows that d k d. Moreover, it can be shown that there are sets of arbitrarily large pseudoindex, so d k is defined for all k 1. Since d 0 := sup Uδ J <, it follows from the deformation lemma that d k d 0 for all k. Hence d k d d 0. Since γ(s 1 ) = 2, it is easy to see that γ(f) = 2 and γ(ūδ) = 2 provided δ is small enough. Using the deformation lemma once more we obtain u A k γ (J d k+ε ) γ (J d k+ε \ U δ ) + γ(ūδ) γ (J d k ε ) + 2. Therefore γ (J dk ε ) k 2, so d k ε d k 2 and d ε d, a contradiction. Hence there is no compact set K satisfying (9) and (10) and the number of geometrically distinct solutions of (1) must be infinite. 7
8 References [1] G. Arioli, A. Szulkin, Homoclinic solutions of Hamiltonian systems with symmetry, J. Diff. Eq. 158 (1999), [2] G. Arioli, A. Szulkin, A semilinear Schrödinger equation in the presence of a magnetic field, Preprint. [3] T. Bartsch, Y. Ding, On a nonlinear Schrödinger equation with periodic potential, Math. Ann. 313 (1999), [4] V. Benci, On critical point theory for indefinite functionals in the presence of symmetries, Trans. Amer. Math. Soc. 274 (1982), [5] S. Cingolani, S. Secchi, Semiclassical limit for nonlinear Schrödinger equation with electromagnetic fields, Preprint. [6] M.J. Esteban, P.L. Lions, Stationary solutions of nonlinear Schrödinger equations with an external magnetic field. In: Partial Differential Equations and the Calculus of Variations, Vol. 1, F. Colombini, A. Marino, L. Modica and S. Spagnolo eds., Birkhäuser (1989), pp [7] W. Kryszewski, A. Szulkin, Generalized linking theorem with an application to semilinear Schrödinger equation, Adv. Diff. Eq. 3 (1998), [8] K. Kurata, Existence and semi-classical limit of the least energy solution to a nonlinear Schrödinger equation with electromagnetic fields, onlinear Analysis 41 (2000), [9] H. Leinfelder, Gauge invariance of Schrödinger operators and related spectral properties, J. Operator Theory 9 (1983), [10] E.H. Lieb, M. Loss, Analysis, Amer. Math. Soc., Providence, R.I., [11] A.A. Pankov, On nontrivial solutions of nonlinear Schrödinger equation with external magnetic field, Preprint. [12] I. Schindler, K. Tintarev, A nonlinear Schrödinger equation with external magnetic field, Rostock. Math. Kolloq. 56 (2002), [13] C. Stuart, Bifurcation into spectral gaps, Bull. Belg. Math. Soc., Supplement (1995). [14] M. Willem, Minimax Theorems, Birkhäuser, Boston,
ON THE SCHRÖDINGER EQUATION INVOLVING A CRITICAL SOBOLEV EXPONENT AND MAGNETIC FIELD. Jan Chabrowski Andrzej Szulkin. 1.
Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 25, 2005, 3 21 ON THE SCHRÖDINGER EQUATION INVOLVING A CRITICAL SOBOLEV EXPONENT AND MAGNETIC FIELD Jan Chabrowski
More informationMultiple solutions to a nonlinear Schrödinger equation with Aharonov-Bohm magnetic potential
Multiple solutions to a nonlinear Schrödinger equation with Aharonov-Bohm magnetic potential Mónica Clapp and Andrzej Szulkin Abstract. We consider the magnetic nonlinear Schrödinger equations ( i + sa)
More informationGeneralized linking theorem with an application to semilinear Schrödinger equation
Generalized linking theorem with an application to semilinear Schrödinger equation Wojciech Kryszewski Department of Mathematics, Nicholas Copernicus University Chopina 12/18, 87-100 Toruń, Poland Andrzej
More informationEXISTENCE OF NONTRIVIAL SOLUTIONS FOR A QUASILINEAR SCHRÖDINGER EQUATIONS WITH SIGN-CHANGING POTENTIAL
Electronic Journal of Differential Equations, Vol. 2014 (2014), No. 05, pp. 1 8. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu EXISTENCE OF NONTRIVIAL
More informationA nodal solution of the scalar field equation at the second minimax level
Bull. London Math. Soc. 46 (2014) 1218 1225 C 2014 London Mathematical Society doi:10.1112/blms/bdu075 A nodal solution of the scalar field equation at the second minimax level Kanishka Perera and Cyril
More informationSUPER-QUADRATIC CONDITIONS FOR PERIODIC ELLIPTIC SYSTEM ON R N
Electronic Journal of Differential Equations, Vol. 015 015), No. 17, pp. 1 11. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu SUPER-QUADRATIC CONDITIONS
More informationMULTIPLE SOLUTIONS FOR AN INDEFINITE KIRCHHOFF-TYPE EQUATION WITH SIGN-CHANGING POTENTIAL
Electronic Journal of Differential Equations, Vol. 2015 (2015), o. 274, pp. 1 9. ISS: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu MULTIPLE SOLUTIOS
More informationEXISTENCE OF SOLUTIONS TO ASYMPTOTICALLY PERIODIC SCHRÖDINGER EQUATIONS
Electronic Journal of Differential Equations, Vol. 017 (017), No. 15, pp. 1 7. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu EXISTENCE OF SOLUTIONS TO ASYMPTOTICALLY PERIODIC
More informationHomoclinic Orbits for Asymptotically Linear Hamiltonian Systems
ISSN: 1401-5617 Homoclinic Orbits for Asymptotically Linear Hamiltonian Systems Andrzej Szulkin Wenming Zou esearch eports in Mathematics Number 9, 1999 Department of Mathematics Stockholm University Electronic
More informationNonlinear Maxwell equations a variational approach Version of May 16, 2018
Nonlinear Maxwell equations a variational approach Version of May 16, 018 Course at the Karlsruher Institut für Technologie Jarosław Mederski Institute of Mathematics of the Polish Academy of Sciences
More informationSEMILINEAR ELLIPTIC EQUATIONS WITH DEPENDENCE ON THE GRADIENT
Electronic Journal of Differential Equations, Vol. 2012 (2012), No. 139, pp. 1 9. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu SEMILINEAR ELLIPTIC
More informationINFINITELY MANY SOLUTIONS FOR A CLASS OF SUBLINEAR SCHRÖDINGER EQUATIONS. Jing Chen and X. H. Tang 1. INTRODUCTION
TAIWANESE JOURNAL OF MATHEMATICS Vol. 19, No. 2, pp. 381-396, April 2015 DOI: 10.11650/tjm.19.2015.4044 This paper is available online at http://journal.taiwanmathsoc.org.tw INFINITELY MANY SOLUTIONS FOR
More informationPOSITIVE GROUND STATE SOLUTIONS FOR SOME NON-AUTONOMOUS KIRCHHOFF TYPE PROBLEMS
ROCKY MOUNTAIN JOURNAL OF MATHEMATICS Volume 47, Number 1, 2017 POSITIVE GROUND STATE SOLUTIONS FOR SOME NON-AUTONOMOUS KIRCHHOFF TYPE PROBLEMS QILIN XIE AND SHIWANG MA ABSTRACT. In this paper, we study
More informationOn a Periodic Schrödinger Equation with Nonlocal Superlinear Part
On a Periodic Schrödinger Equation with Nonlocal Superlinear Part Nils Ackermann Abstract We consider the Choquard-Pekar equation u + V u = (W u 2 )u u H 1 (R 3 ) and focus on the case of periodic potential
More informationCOMBINED EFFECTS FOR A STATIONARY PROBLEM WITH INDEFINITE NONLINEARITIES AND LACK OF COMPACTNESS
Dynamic Systems and Applications 22 (203) 37-384 COMBINED EFFECTS FOR A STATIONARY PROBLEM WITH INDEFINITE NONLINEARITIES AND LACK OF COMPACTNESS VICENŢIU D. RĂDULESCU Simion Stoilow Mathematics Institute
More informationNONTRIVIAL SOLUTIONS FOR SUPERQUADRATIC NONAUTONOMOUS PERIODIC SYSTEMS. Shouchuan Hu Nikolas S. Papageorgiou. 1. Introduction
Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 34, 29, 327 338 NONTRIVIAL SOLUTIONS FOR SUPERQUADRATIC NONAUTONOMOUS PERIODIC SYSTEMS Shouchuan Hu Nikolas S. Papageorgiou
More informationNew Results for Second Order Discrete Hamiltonian Systems. Huiwen Chen*, Zhimin He, Jianli Li and Zigen Ouyang
TAIWANESE JOURNAL OF MATHEMATICS Vol. xx, No. x, pp. 1 26, xx 20xx DOI: 10.11650/tjm/7762 This paper is available online at http://journal.tms.org.tw New Results for Second Order Discrete Hamiltonian Systems
More informationContents: 1. Minimization. 2. The theorem of Lions-Stampacchia for variational inequalities. 3. Γ -Convergence. 4. Duality mapping.
Minimization Contents: 1. Minimization. 2. The theorem of Lions-Stampacchia for variational inequalities. 3. Γ -Convergence. 4. Duality mapping. 1 Minimization A Topological Result. Let S be a topological
More informationSymmetrization and minimax principles
Symmetrization and minimax principles Jean Van Schaftingen July 20, 2004 Abstract We develop a method to prove that some critical levels for functionals invariant by symmetry obtained by minimax methods
More informationNONLINEAR SCHRÖDINGER ELLIPTIC SYSTEMS INVOLVING EXPONENTIAL CRITICAL GROWTH IN R Introduction
Electronic Journal of Differential Equations, Vol. 014 (014), No. 59, pp. 1 1. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu NONLINEAR SCHRÖDINGER
More informationNonlinear elliptic systems with exponential nonlinearities
22-Fez conference on Partial Differential Equations, Electronic Journal of Differential Equations, Conference 9, 22, pp 139 147. http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu
More informationAN EIGENVALUE PROBLEM FOR THE SCHRÖDINGER MAXWELL EQUATIONS. Vieri Benci Donato Fortunato. 1. Introduction
Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume, 998, 83 93 AN EIGENVALUE PROBLEM FOR THE SCHRÖDINGER MAXWELL EQUATIONS Vieri Benci Donato Fortunato Dedicated to
More informationBOUNDED WEAK SOLUTION FOR THE HAMILTONIAN SYSTEM. Q-Heung Choi and Tacksun Jung
Korean J. Math. 2 (23), No., pp. 8 9 http://dx.doi.org/.568/kjm.23.2..8 BOUNDED WEAK SOLUTION FOR THE HAMILTONIAN SYSTEM Q-Heung Choi and Tacksun Jung Abstract. We investigate the bounded weak solutions
More informationON NONHOMOGENEOUS BIHARMONIC EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENT
PORTUGALIAE MATHEMATICA Vol. 56 Fasc. 3 1999 ON NONHOMOGENEOUS BIHARMONIC EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENT M. Guedda Abstract: In this paper we consider the problem u = λ u u + f in, u = u
More informationp-laplacian problems with critical Sobolev exponents
Nonlinear Analysis 66 (2007) 454 459 www.elsevier.com/locate/na p-laplacian problems with critical Sobolev exponents Kanishka Perera a,, Elves A.B. Silva b a Department of Mathematical Sciences, Florida
More informationA NOTE ON THE EXISTENCE OF TWO NONTRIVIAL SOLUTIONS OF A RESONANCE PROBLEM
PORTUGALIAE MATHEMATICA Vol. 51 Fasc. 4 1994 A NOTE ON THE EXISTENCE OF TWO NONTRIVIAL SOLUTIONS OF A RESONANCE PROBLEM To Fu Ma* Abstract: We study the existence of two nontrivial solutions for an elliptic
More informationSome nonlinear elliptic equations in R N
Nonlinear Analysis 39 000) 837 860 www.elsevier.nl/locate/na Some nonlinear elliptic equations in Monica Musso, Donato Passaseo Dipartimento di Matematica, Universita di Pisa, Via Buonarroti,, 5617 Pisa,
More informationEXISTENCE OF SOLUTIONS FOR A RESONANT PROBLEM UNDER LANDESMAN-LAZER CONDITIONS
Electronic Journal of Differential Equations, Vol. 2008(2008), No. 98, pp. 1 10. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) EXISTENCE
More informationEXISTENCE OF SOLUTIONS FOR CROSS CRITICAL EXPONENTIAL N-LAPLACIAN SYSTEMS
Electronic Journal of Differential Equations, Vol. 2014 (2014), o. 28, pp. 1 10. ISS: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu EXISTECE OF SOLUTIOS
More informationEXISTENCE OF WEAK SOLUTIONS FOR A NONUNIFORMLY ELLIPTIC NONLINEAR SYSTEM IN R N. 1. Introduction We study the nonuniformly elliptic, nonlinear system
Electronic Journal of Differential Equations, Vol. 20082008), No. 119, pp. 1 10. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu login: ftp) EXISTENCE
More informationChanging sign solutions for the CR-Yamabe equation
Changing sign solutions for the CR-Yamabe equation Ali Maalaoui (1) & Vittorio Martino (2) Abstract In this paper we prove that the CR-Yamabe equation on the Heisenberg group has infinitely many changing
More informationarxiv: v1 [math.ap] 28 Mar 2014
GROUNDSTATES OF NONLINEAR CHOQUARD EQUATIONS: HARDY-LITTLEWOOD-SOBOLEV CRITICAL EXPONENT VITALY MOROZ AND JEAN VAN SCHAFTINGEN arxiv:1403.7414v1 [math.ap] 28 Mar 2014 Abstract. We consider nonlinear Choquard
More informationComputations of Critical Groups at a Degenerate Critical Point for Strongly Indefinite Functionals
Journal of Mathematical Analysis and Applications 256, 462 477 (2001) doi:10.1006/jmaa.2000.7292, available online at http://www.idealibrary.com on Computations of Critical Groups at a Degenerate Critical
More informationINFINITELY MANY SOLUTIONS FOR A CLASS OF SUBLINEAR SCHRÖDINGER EQUATIONS
Journal of Applied Analysis and Computation Volume 8, Number 5, October 018, 1475 1493 Website:http://jaac-online.com/ DOI:10.11948/018.1475 INFINITELY MANY SOLUTIONS FOR A CLASS OF SUBLINEAR SCHRÖDINGER
More information2. Function spaces and approximation
2.1 2. Function spaces and approximation 2.1. The space of test functions. Notation and prerequisites are collected in Appendix A. Let Ω be an open subset of R n. The space C0 (Ω), consisting of the C
More informationPositive and Nodal Solutions For a Nonlinear Schrödinger Equation with Indefinite Potential
Advanced Nonlinear Studies 8 (008), 353 373 Positive and Nodal Solutions For a Nonlinear Schrödinger Equation with Indefinite Potential Marcelo F. Furtado, Liliane A. Maia Universidade de Brasília - Departamento
More informationWeak Convergence Methods for Energy Minimization
Weak Convergence Methods for Energy Minimization Bo Li Department of Mathematics University of California, San Diego E-mail: bli@math.ucsd.edu June 3, 2007 Introduction This compact set of notes present
More informationEXISTENCE OF SOLUTIONS FOR KIRCHHOFF TYPE EQUATIONS WITH UNBOUNDED POTENTIAL. 1. Introduction In this article, we consider the Kirchhoff type problem
Electronic Journal of Differential Equations, Vol. 207 (207), No. 84, pp. 2. ISSN: 072-669. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu EXISTENCE OF SOLUTIONS FOR KIRCHHOFF TYPE EQUATIONS
More informationVariational eigenvalues of degenerate eigenvalue problems for the weighted p-laplacian
Variational eigenvalues of degenerate eigenvalue problems for the weighted p-laplacian An Lê Mathematics Sciences Research Institute, 17 Gauss Way, Berkeley, California 94720 e-mail: anle@msri.org Klaus
More informationMULTIPLE SOLUTIONS FOR CRITICAL ELLIPTIC PROBLEMS WITH FRACTIONAL LAPLACIAN
Electronic Journal of Differential Equations, Vol. 016 (016), No. 97, pp. 1 11. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu MULTIPLE SOLUTIONS
More informationarxiv: v1 [math.ap] 24 Oct 2014
Multiple solutions for Kirchhoff equations under the partially sublinear case Xiaojing Feng School of Mathematical Sciences, Shanxi University, Taiyuan 030006, People s Republic of China arxiv:1410.7335v1
More informationOn the Second Minimax Level of the Scalar Field Equation and Symmetry Breaking
arxiv:128.1139v3 [math.ap] 2 May 213 On the Second Minimax Level of the Scalar Field Equation and Symmetry Breaking Kanishka Perera Department of Mathematical Sciences Florida Institute of Technology Melbourne,
More informationBorderline Variational Problems Involving Fractional Laplacians and Critical Singularities
Advanced Nonlinear Studies 15 (015), xxx xxx Borderline Variational Problems Involving Fractional Laplacians and Critical Singularities Nassif Ghoussoub, Shaya Shakerian Department of Mathematics University
More informationHamiltonian systems: periodic and homoclinic solutions by variational methods
Hamiltonian systems: periodic and homoclinic solutions by variational methods Thomas Bartsch Mathematisches Institut, Universität Giessen Arndtstr. 2, 35392 Giessen, Germany Andrzej Szulkin Department
More informationFunctional Analysis. Franck Sueur Metric spaces Definitions Completeness Compactness Separability...
Functional Analysis Franck Sueur 2018-2019 Contents 1 Metric spaces 1 1.1 Definitions........................................ 1 1.2 Completeness...................................... 3 1.3 Compactness......................................
More informationHOMOLOGICAL LOCAL LINKING
HOMOLOGICAL LOCAL LINKING KANISHKA PERERA Abstract. We generalize the notion of local linking to include certain cases where the functional does not have a local splitting near the origin. Applications
More informationGROUND STATE SOLUTIONS FOR CHOQUARD TYPE EQUATIONS WITH A SINGULAR POTENTIAL. 1. Introduction In this article, we study the Choquard type equation
Electronic Journal of Differential Equations, Vol. 2017 (2017), o. 52, pp. 1 14. ISS: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu GROUD STATE SOLUTIOS FOR CHOQUARD TYPE EQUATIOS
More informationMultiple Solutions for Parametric Neumann Problems with Indefinite and Unbounded Potential
Advances in Dynamical Systems and Applications ISSN 0973-5321, Volume 8, Number 2, pp. 281 293 (2013) http://campus.mst.edu/adsa Multiple Solutions for Parametric Neumann Problems with Indefinite and Unbounded
More informationSPECTRAL PROPERTIES OF THE LAPLACIAN ON BOUNDED DOMAINS
SPECTRAL PROPERTIES OF THE LAPLACIAN ON BOUNDED DOMAINS TSOGTGEREL GANTUMUR Abstract. After establishing discrete spectra for a large class of elliptic operators, we present some fundamental spectral properties
More informationThe effects of a discontinues weight for a problem with a critical nonlinearity
arxiv:1405.7734v1 [math.ap] 9 May 014 The effects of a discontinues weight for a problem with a critical nonlinearity Rejeb Hadiji and Habib Yazidi Abstract { We study the minimizing problem px) u dx,
More informationSHARP BOUNDARY TRACE INEQUALITIES. 1. Introduction
SHARP BOUNDARY TRACE INEQUALITIES GILES AUCHMUTY Abstract. This paper describes sharp inequalities for the trace of Sobolev functions on the boundary of a bounded region R N. The inequalities bound (semi-)norms
More informationNONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS
Fixed Point Theory, Volume 9, No. 1, 28, 3-16 http://www.math.ubbcluj.ro/ nodeacj/sfptcj.html NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS GIOVANNI ANELLO Department of Mathematics University
More informationVANISHING-CONCENTRATION-COMPACTNESS ALTERNATIVE FOR THE TRUDINGER-MOSER INEQUALITY IN R N
VAISHIG-COCETRATIO-COMPACTESS ALTERATIVE FOR THE TRUDIGER-MOSER IEQUALITY I R Abstract. Let 2, a > 0 0 < b. Our aim is to clarify the influence of the constraint S a,b = { u W 1, (R ) u a + u b = 1 } on
More informationNon-radial solutions to a bi-harmonic equation with negative exponent
Non-radial solutions to a bi-harmonic equation with negative exponent Ali Hyder Department of Mathematics, University of British Columbia, Vancouver BC V6TZ2, Canada ali.hyder@math.ubc.ca Juncheng Wei
More informationOn Ekeland s variational principle
J. Fixed Point Theory Appl. 10 (2011) 191 195 DOI 10.1007/s11784-011-0048-x Published online March 31, 2011 Springer Basel AG 2011 Journal of Fixed Point Theory and Applications On Ekeland s variational
More informationOn John type ellipsoids
On John type ellipsoids B. Klartag Tel Aviv University Abstract Given an arbitrary convex symmetric body K R n, we construct a natural and non-trivial continuous map u K which associates ellipsoids to
More informationNONHOMOGENEOUS ELLIPTIC EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENT AND WEIGHT
Electronic Journal of Differential Equations, Vol. 016 (016), No. 08, pp. 1 1. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu NONHOMOGENEOUS ELLIPTIC
More informationA REMARK ON MINIMAL NODAL SOLUTIONS OF AN ELLIPTIC PROBLEM IN A BALL. Olaf Torné. 1. Introduction
Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 24, 2004, 199 207 A REMARK ON MINIMAL NODAL SOLUTIONS OF AN ELLIPTIC PROBLEM IN A BALL Olaf Torné (Submitted by Michel
More informationCritical Groups in Saddle Point Theorems without a Finite Dimensional Closed Loop
Math. Nachr. 43 00), 56 64 Critical Groups in Saddle Point Theorems without a Finite Dimensional Closed Loop By Kanishka Perera ) of Florida and Martin Schechter of Irvine Received November 0, 000; accepted
More informationNodal type bound states of Schrödinger equations via invariant set and minimax methods
J. Differential Equations 214 (2005 358 390 www.elsevier.com/locate/jde Nodal type bound states of Schrödinger equations via invariant set and minimax methods Zhaoli Liu a, Francois A. van Heerden b,1,
More informationA one-dimensional nonlinear degenerate elliptic equation
USA-Chile Workshop on Nonlinear Analysis, Electron. J. Diff. Eqns., Conf. 06, 001, pp. 89 99. http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu or ejde.math.unt.edu login: ftp)
More informationNonvariational problems with critical growth
Nonlinear Analysis ( ) www.elsevier.com/locate/na Nonvariational problems with critical growth Maya Chhetri a, Pavel Drábek b, Sarah Raynor c,, Stephen Robinson c a University of North Carolina, Greensboro,
More informationPOTENTIAL LANDESMAN-LAZER TYPE CONDITIONS AND. 1. Introduction We investigate the existence of solutions for the nonlinear boundary-value problem
Electronic Journal of Differential Equations, Vol. 25(25), No. 94, pp. 1 12. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) POTENTIAL
More informationAnalysis in weighted spaces : preliminary version
Analysis in weighted spaces : preliminary version Frank Pacard To cite this version: Frank Pacard. Analysis in weighted spaces : preliminary version. 3rd cycle. Téhéran (Iran, 2006, pp.75.
More informationEXISTENCE RESULTS FOR OPERATOR EQUATIONS INVOLVING DUALITY MAPPINGS VIA THE MOUNTAIN PASS THEOREM
EXISTENCE RESULTS FOR OPERATOR EQUATIONS INVOLVING DUALITY MAPPINGS VIA THE MOUNTAIN PASS THEOREM JENICĂ CRÎNGANU We derive existence results for operator equations having the form J ϕu = N f u, by using
More informationREMARKS ON THE VANISHING OBSTACLE LIMIT FOR A 3D VISCOUS INCOMPRESSIBLE FLUID
REMARKS ON THE VANISHING OBSTACLE LIMIT FOR A 3D VISCOUS INCOMPRESSIBLE FLUID DRAGOŞ IFTIMIE AND JAMES P. KELLIHER Abstract. In [Math. Ann. 336 (2006), 449-489] the authors consider the two dimensional
More informationp-laplacian problems involving critical Hardy Sobolev exponents
Nonlinear Differ. Equ. Appl. 2018) 25:25 c 2018 Springer International Publishing AG, part of Springer Nature 1021-9722/18/030001-16 published online June 4, 2018 https://doi.org/10.1007/s00030-018-0517-7
More informationMulti-bump type nodal solutions having a prescribed number of nodal domains: I
Ann. I. H. Poincaré AN 005 597 608 www.elsevier.com/locate/anihpc Multi-bump type nodal solutions having a prescribed number of nodal domains: I Solutions nodales de multi-bosse ayant un nombre de domaines
More informationarxiv: v1 [math.ap] 16 Jan 2015
Three positive solutions of a nonlinear Dirichlet problem with competing power nonlinearities Vladimir Lubyshev January 19, 2015 arxiv:1501.03870v1 [math.ap] 16 Jan 2015 Abstract This paper studies a nonlinear
More informationSobolev Spaces. Chapter Hölder spaces
Chapter 2 Sobolev Spaces Sobolev spaces turn out often to be the proper setting in which to apply ideas of functional analysis to get information concerning partial differential equations. Here, we collect
More informationProblem: A class of dynamical systems characterized by a fast divergence of the orbits. A paradigmatic example: the Arnold cat.
À È Ê ÇÄÁ Ë ËÌ ÅË Problem: A class of dynamical systems characterized by a fast divergence of the orbits A paradigmatic example: the Arnold cat. The closure of a homoclinic orbit. The shadowing lemma.
More informationNonlinear Schrödinger equation: concentration on circles driven by an external magnetic field
Nonlinear Schrödinger equation: concentration on circles driven by an external magnetic field Denis Bonheure, Silvia Cingolani, Manon Nys To cite this version: Denis Bonheure, Silvia Cingolani, Manon Nys.
More informationSELF-ADJOINTNESS OF SCHRÖDINGER-TYPE OPERATORS WITH SINGULAR POTENTIALS ON MANIFOLDS OF BOUNDED GEOMETRY
Electronic Journal of Differential Equations, Vol. 2003(2003), No.??, pp. 1 8. ISSN: 1072-6691. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu (login: ftp) SELF-ADJOINTNESS
More informationExistence of Solutions for a Class of p(x)-biharmonic Problems without (A-R) Type Conditions
International Journal of Mathematical Analysis Vol. 2, 208, no., 505-55 HIKARI Ltd, www.m-hikari.com https://doi.org/0.2988/ijma.208.886 Existence of Solutions for a Class of p(x)-biharmonic Problems without
More informationNONLINEAR FREDHOLM ALTERNATIVE FOR THE p-laplacian UNDER NONHOMOGENEOUS NEUMANN BOUNDARY CONDITION
Electronic Journal of Differential Equations, Vol. 2016 (2016), No. 210, pp. 1 7. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu NONLINEAR FREDHOLM ALTERNATIVE FOR THE p-laplacian
More informationThe Dirichlet s P rinciple. In this lecture we discuss an alternative formulation of the Dirichlet problem for the Laplace equation:
Oct. 1 The Dirichlet s P rinciple In this lecture we discuss an alternative formulation of the Dirichlet problem for the Laplace equation: 1. Dirichlet s Principle. u = in, u = g on. ( 1 ) If we multiply
More informationNonlinear problems with lack of compactness in Critical Point Theory
Nonlinear problems with lack of compactness in Critical Point Theory Carlo Mercuri CASA Day Eindhoven, 11th April 2012 Critical points Many linear and nonlinear PDE s have the form P(u) = 0, u X. (1) Here
More informationTHE L 2 -HODGE THEORY AND REPRESENTATION ON R n
THE L 2 -HODGE THEORY AND REPRESENTATION ON R n BAISHENG YAN Abstract. We present an elementary L 2 -Hodge theory on whole R n based on the minimization principle of the calculus of variations and some
More informationRNDr. Petr Tomiczek CSc.
HABILITAČNÍ PRÁCE RNDr. Petr Tomiczek CSc. Plzeň 26 Nonlinear differential equation of second order RNDr. Petr Tomiczek CSc. Department of Mathematics, University of West Bohemia 5 Contents 1 Introduction
More informationNonlinear Schrödinger problems: symmetries of some variational solutions
Nonlinear Differ. Equ. Appl. (3), 5 5 c Springer Basel AG -97/3/35- published online April 3, DOI.7/s3--3- Nonlinear Differential Equations and Applications NoDEA Nonlinear Schrödinger problems: symmetries
More informationExistence of Positive Solutions to Semilinear Elliptic Systems Involving Concave and Convex Nonlinearities
Journal of Physical Science Application 5 (2015) 71-81 doi: 10.17265/2159-5348/2015.01.011 D DAVID PUBLISHING Existence of Positive Solutions to Semilinear Elliptic Systems Involving Concave Convex Nonlinearities
More informationMULTIPLE SOLUTIONS FOR A KIRCHHOFF EQUATION WITH NONLINEARITY HAVING ARBITRARY GROWTH
MULTIPLE SOLUTIONS FOR A KIRCHHOFF EQUATION WITH NONLINEARITY HAVING ARBITRARY GROWTH MARCELO F. FURTADO AND HENRIQUE R. ZANATA Abstract. We prove the existence of infinitely many solutions for the Kirchhoff
More informationTHE STOKES SYSTEM R.E. SHOWALTER
THE STOKES SYSTEM R.E. SHOWALTER Contents 1. Stokes System 1 Stokes System 2 2. The Weak Solution of the Stokes System 3 3. The Strong Solution 4 4. The Normal Trace 6 5. The Mixed Problem 7 6. The Navier-Stokes
More informationarxiv: v1 [math.ap] 21 Nov 2018
Notes on A Superlinear Elliptic Problem Haoyu Li arxiv:1811.09605v1 [math.ap] 1 Nov 018 Center of Applied Mathematics, Tianjin University Tianjin 30007, China E-mail: hyli1994@hotmail.com Abstract. Based
More informationCritical Point Theory 0 and applications
Critical Point Theory 0 and applications Introduction This notes are the result of two Ph.D. courses I held at the University of Florence in Spring 2006 and in Spring 2010 on Critical Point Theory, as
More informationOn the Schrödinger Equation in R N under the Effect of a General Nonlinear Term
On the Schrödinger Equation in under the Effect of a General Nonlinear Term A. AZZOLLINI & A. POMPONIO ABSTRACT. In this paper we prove the existence of a positive solution to the equation u + V(x)u =
More informationDecomposition of Riesz frames and wavelets into a finite union of linearly independent sets
Decomposition of Riesz frames and wavelets into a finite union of linearly independent sets Ole Christensen, Alexander M. Lindner Abstract We characterize Riesz frames and prove that every Riesz frame
More informationElliptic equations with one-sided critical growth
Electronic Journal of Differential Equations, Vol. 00(00), No. 89, pp. 1 1. ISSN: 107-6691. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu (login: ftp) Elliptic equations
More informationarxiv: v1 [math.ap] 7 May 2009
Existence of solutions for a problem of resonance road space with weight arxiv:0905.1016v1 [math.ap] 7 May 2009 Antonio Ronaldo G. Garcia, Moisés D. dos Santos and Adrião D. D. Neto 2 Abstract Universidade
More informationA note on the σ-algebra of cylinder sets and all that
A note on the σ-algebra of cylinder sets and all that José Luis Silva CCM, Univ. da Madeira, P-9000 Funchal Madeira BiBoS, Univ. of Bielefeld, Germany (luis@dragoeiro.uma.pt) September 1999 Abstract In
More information1 Definition and Basic Properties of Compa Operator
1 Definition and Basic Properties of Compa Operator 1.1 Let X be a infinite dimensional Banach space. Show that if A C(X ), A does not have bounded inverse. Proof. Denote the unit ball of X by B and the
More informationl(y j ) = 0 for all y j (1)
Problem 1. The closed linear span of a subset {y j } of a normed vector space is defined as the intersection of all closed subspaces containing all y j and thus the smallest such subspace. 1 Show that
More informationThe Brézis-Nirenberg Result for the Fractional Elliptic Problem with Singular Potential
arxiv:1705.08387v1 [math.ap] 23 May 2017 The Brézis-Nirenberg Result for the Fractional Elliptic Problem with Singular Potential Lingyu Jin, Lang Li and Shaomei Fang Department of Mathematics, South China
More informationTHE FORM SUM AND THE FRIEDRICHS EXTENSION OF SCHRÖDINGER-TYPE OPERATORS ON RIEMANNIAN MANIFOLDS
THE FORM SUM AND THE FRIEDRICHS EXTENSION OF SCHRÖDINGER-TYPE OPERATORS ON RIEMANNIAN MANIFOLDS OGNJEN MILATOVIC Abstract. We consider H V = M +V, where (M, g) is a Riemannian manifold (not necessarily
More informationSharp Sobolev Strichartz estimates for the free Schrödinger propagator
Sharp Sobolev Strichartz estimates for the free Schrödinger propagator Neal Bez, Chris Jeavons and Nikolaos Pattakos Abstract. We consider gaussian extremisability of sharp linear Sobolev Strichartz estimates
More informationRenormalized Energy with Vortices Pinning Effect
Renormalized Energy with Vortices Pinning Effect Shijin Ding Department of Mathematics South China Normal University Guangzhou, Guangdong 5063, China Abstract. This paper is a successor of the previous
More informationDiagonalization of the Coupled-Mode System.
Diagonalization of the Coupled-Mode System. Marina Chugunova joint work with Dmitry Pelinovsky Department of Mathematics, McMaster University, Canada Collaborators: Mason A. Porter, California Institute
More informationAn introduction to Birkhoff normal form
An introduction to Birkhoff normal form Dario Bambusi Dipartimento di Matematica, Universitá di Milano via Saldini 50, 0133 Milano (Italy) 19.11.14 1 Introduction The aim of this note is to present an
More informationA functional model for commuting pairs of contractions and the symmetrized bidisc
A functional model for commuting pairs of contractions and the symmetrized bidisc Nicholas Young Leeds and Newcastle Universities Lecture 2 The symmetrized bidisc Γ and Γ-contractions St Petersburg, June
More informationStability of Relativistic Matter with Magnetic Fields for Nuclear Charges up to the Critical Value
Commun. Math. Phys. 275, 479 489 (2007) Digital Object Identifier (DOI) 10.1007/s00220-007-0307-2 Communications in Mathematical Physics Stability of Relativistic Matter with Magnetic Fields for Nuclear
More information