XIAOFENG REN. equation by minimizing the corresponding functional near some approximate

Similar documents
Math 497 R1 Winter 2018 Navier-Stokes Regularity

ON TRIVIAL GRADIENT YOUNG MEASURES BAISHENG YAN Abstract. We give a condition on a closed set K of real nm matrices which ensures that any W 1 p -grad

EXISTENCE OF SOLUTIONS FOR KIRCHHOFF TYPE EQUATIONS WITH UNBOUNDED POTENTIAL. 1. Introduction In this article, we consider the Kirchhoff type problem

Scattering for the NLS equation

A note on some approximation theorems in measure theory

Existence of minimizers for the pure displacement problem in nonlinear elasticity

EXISTENCE OF SOLUTIONS FOR CROSS CRITICAL EXPONENTIAL N-LAPLACIAN SYSTEMS

2.3 Variational form of boundary value problems

Congurations of periodic orbits for equations with delayed positive feedback

Stanford Mathematics Department Math 205A Lecture Supplement #4 Borel Regular & Radon Measures

SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction

The Erwin Schrodinger International Boltzmanngasse 9. Institute for Mathematical Physics A-1090 Wien, Austria

Pointwise convergence rate for nonlinear conservation. Eitan Tadmor and Tao Tang

Global unbounded solutions of the Fujita equation in the intermediate range

ON NONHOMOGENEOUS BIHARMONIC EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENT

Nonlinear elliptic systems with exponential nonlinearities

1 Topology Definition of a topology Basis (Base) of a topology The subspace topology & the product topology on X Y 3

1 Solutions to selected problems

Problem set 1, Real Analysis I, Spring, 2015.

EXISTENCE OF NONTRIVIAL SOLUTIONS FOR A QUASILINEAR SCHRÖDINGER EQUATIONS WITH SIGN-CHANGING POTENTIAL

SOME MEASURABILITY AND CONTINUITY PROPERTIES OF ARBITRARY REAL FUNCTIONS

NOTES ON THE REGULARITY OF QUASICONFORMAL HOMEOMORPHISMS

A nodal solution of the scalar field equation at the second minimax level

Friedrich symmetric systems

Problem Set 6: Solutions Math 201A: Fall a n x n,

SPECTRAL PROPERTIES OF THE LAPLACIAN ON BOUNDED DOMAINS

EXISTENCE OF SOLUTIONS FOR A RESONANT PROBLEM UNDER LANDESMAN-LAZER CONDITIONS

Chapter 3: Baire category and open mapping theorems

The Heine-Borel and Arzela-Ascoli Theorems

A NOTE ON THE EXISTENCE OF TWO NONTRIVIAL SOLUTIONS OF A RESONANCE PROBLEM

Contents: 1. Minimization. 2. The theorem of Lions-Stampacchia for variational inequalities. 3. Γ -Convergence. 4. Duality mapping.

(x k ) sequence in F, lim x k = x x F. If F : R n R is a function, level sets and sublevel sets of F are any sets of the form (respectively);

5 Set Operations, Functions, and Counting

Sequences and Series of Functions

Proof. We indicate by α, β (finite or not) the end-points of I and call

Neumann problem: p u = juj N() : p 2 u; in ; u n = ; on : Robin problem: R() : Steklov problem: S() : p u = juj p 2 u; in ; p 2 u jruj n + jujp 2 u =

On John type ellipsoids

2. Function spaces and approximation

Introduction to Real Analysis Alternative Chapter 1

Functional Analysis. Franck Sueur Metric spaces Definitions Completeness Compactness Separability...

Notes on uniform convergence

JUHA KINNUNEN. Harmonic Analysis

Global minimization. Chapter Upper and lower bounds

Rearrangements and polar factorisation of countably degenerate functions G.R. Burton, School of Mathematical Sciences, University of Bath, Claverton D

Some nonlinear elliptic equations in R N

Numerical Integration for Multivariable. October Abstract. We consider the numerical integration of functions with point singularities over

We continue our study of the Pythagorean Theorem begun in ref. 1. The numbering of results and remarks in ref. 1 will

2 BAISHENG YAN When L =,it is easily seen that the set K = coincides with the set of conformal matrices, that is, K = = fr j 0 R 2 SO(n)g: Weakly L-qu

Near convexity, metric convexity, and convexity

SHARP BOUNDARY TRACE INEQUALITIES. 1. Introduction

Chapter 1 Foundations of Elliptic Boundary Value Problems 1.1 Euler equations of variational problems

LECTURE 15: COMPLETENESS AND CONVEXITY

MAT 570 REAL ANALYSIS LECTURE NOTES. Contents. 1. Sets Functions Countability Axiom of choice Equivalence relations 9

EXISTENCE OF FADDEEV KNOTS IN GENERAL HOPF DIMENSIONS

Topological properties

A version of for which ZFC can not predict a single bit Robert M. Solovay May 16, Introduction In [2], Chaitin introd

MATH 131A: REAL ANALYSIS (BIG IDEAS)

Denition 2: o() is the height of the well-founded relation. Notice that we must have o() (2 ) +. Much is known about the possible behaviours of. For e

g 2 (x) (1/3)M 1 = (1/3)(2/3)M.

HeadMedia Interaction in Magnetic Recording

Existence of Solutions for a Class of p(x)-biharmonic Problems without (A-R) Type Conditions

THE INVERSE FUNCTION THEOREM

Chapter 3 Continuous Functions

Existence and Uniqueness

Numerical Solutions to Partial Differential Equations

Chapter One. The Calderón-Zygmund Theory I: Ellipticity

Vector Fields on the Space of Functions Univalent Inside the Unit Disk via Faber Polynomials

Chapter 12. Partial di erential equations Di erential operators in R n. The gradient and Jacobian. Divergence and rotation

Course 212: Academic Year Section 1: Metric Spaces

OPTIMAL POTENTIALS FOR SCHRÖDINGER OPERATORS. 1. Introduction In this paper we consider optimization problems of the form. min F (V ) : V V, (1.

Laplace s Equation. Chapter Mean Value Formulas

Maths 212: Homework Solutions

MATH 220: INNER PRODUCT SPACES, SYMMETRIC OPERATORS, ORTHOGONALITY

Convex Analysis and Optimization Chapter 2 Solutions

r( = f 2 L 2 (1.2) iku)! 0 as r!1: (1.3) It was shown in book [7] that if f is assumed to be the restriction of a function in C

the sum of two projections. Finally, in Section 5, we apply the theory of Section 4 to the case of nite element spaces. 2. Additive Algorithms for Par

Lecture 2: Review of Prerequisites. Table of contents

EXISTENCE OF SOLUTIONS TO ASYMPTOTICALLY PERIODIC SCHRÖDINGER EQUATIONS

Continuous Functions on Metric Spaces

Threshold behavior and non-quasiconvergent solutions with localized initial data for bistable reaction-diffusion equations

It is known that Morley element is not C 0 element and it is divergent for Poisson equation (see [6]). When Morley element is applied to solve problem

Tools from Lebesgue integration

LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS. S. G. Bobkov and F. L. Nazarov. September 25, 2011

Abstract. A front tracking method is used to construct weak solutions to

POTENTIAL LANDESMAN-LAZER TYPE CONDITIONS AND. 1. Introduction We investigate the existence of solutions for the nonlinear boundary-value problem

LECTURE 1: SOURCES OF ERRORS MATHEMATICAL TOOLS A PRIORI ERROR ESTIMATES. Sergey Korotov,

FRACTIONAL CLIQUE DECOMPOSITIONS OF DENSE PARTITE GRAPHS

RNDr. Petr Tomiczek CSc.

Entrance Exam, Real Analysis September 1, 2017 Solve exactly 6 out of the 8 problems

Undergraduate Notes in Mathematics. Arkansas Tech University Department of Mathematics

NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS

Notions such as convergent sequence and Cauchy sequence make sense for any metric space. Convergent Sequences are Cauchy

MATH41011/MATH61011: FOURIER SERIES AND LEBESGUE INTEGRATION. Extra Reading Material for Level 4 and Level 6

Supplementary Materials for Fast envelope algorithms

Recall that if X is a compact metric space, C(X), the space of continuous (real-valued) functions on X, is a Banach space with the norm

Dichotomy Of Poincare Maps And Boundedness Of Some Cauchy Sequences

HOMOLOGICAL LOCAL LINKING

INDISTINGUISHABILITY OF ABSOLUTELY CONTINUOUS AND SINGULAR DISTRIBUTIONS

A REMARK ON MINIMAL NODAL SOLUTIONS OF AN ELLIPTIC PROBLEM IN A BALL. Olaf Torné. 1. Introduction

PCA with random noise. Van Ha Vu. Department of Mathematics Yale University

Transcription:

MULTI-LAYER LOCAL MINIMUM SOLUTIONS OF THE BISTABLE EQUATION IN AN INFINITE TUBE XIAOFENG REN Abstract. We construct local minimum solutions of the semilinear bistable equation by minimizing the corresponding functional near some approximate solutions, assuming that some global minimum solutions are isolated. The key step is to prove with the help of a characterization of Palais-Smale sequences that the functional takes higher values away from the approximate solutions than it does near the approximate solutions.. Introduction In this note we continue to study the problem posed in []. Consider the semilinear elliptic equation ( u + f(u) =0in () @u @ =0on@ where f is a bistable function, and is an unbounded tube-shaped domain in R d. () is the Euler-Lagrange equation of the functional E dened by (2) E(u) = [ 2 jruj2 + W (u)]dx where W (u) = u f(w)dw, and W is a double well potential function of equal depth. The domain of the functional E is taken to be the class (3) A = fu 2 L loc() : ru 2 (L 2 ()) d ; W(u)2 L ()g: Here L loc () is the space of measurable functions that belong to L (K) for every compact subset K of. We present an alternative approach to the construction of multi-layer solutions of () by minimizing E near some proper approximate solutions. The solutions being local minima of Ereects the advantage of this approach since in Theorem 4.4 [] solutions are found through an indirect deformation argument and they are only known as critical points of (2). The hypothesis here that guarantees the existence of the solutions is also weaker than that in [] (see Remark 2). The precise conditions on f, W and are given as follows. 99 Mathematics Subject Classication. Primary 35J20; Secondary 35J60.

2 XIAOFENG REN H-: W is a C 2 function that has exactly two global minimaat and where W ( ) = W () = 0, W 00 ( ) > 0, and W 00 () > 0. H-2: There exists > 0 such that W (u) =u 2 for all juj > 2. H-3: is a smooth innite tube periodic in x -direction, i.e., x =(x ;x 0 )2 R R d = R d is in if and only if x +(;0; :::; 0) is in and x 0 lies in a bounded subset of R d. Note that H-2 is more or less of technical nature. Indeed for each W satisfying H- and W 00 (u) > 0 for juj >, the maximum principle implies that bounded solutions of () lie between and, so one can always modify W to satisfy H-2 without aecting bounded solutions. As a consequence of H- and H-2 there exists C>0such that for all u 2 R (4) (5) f 2 (u) CW(u): Dene a segment S(x ;t), x and t 2 R,ofby S(x ;t):=f(y ;y 0 )2: jy x j<tg: For every u 2A(dened in (3)) dene a continuous function bu : R! R by (6) bu(x )= u(y)dy; x 2 R js(x ;=2)j S(x ;=2) where js(x ; =2)j denotes the Lebesgue measure of S(x ; =2) in R d. Corollary 2.2 [] states that for every u 2A, x! bu(x ) and x! bu(x ) exist and equal or. Setting (7) A = fu 2A: x! bu(x )=; x! bu(x )=g; ;2f ;g; we decompose A = A [A [A [A. If u 2A, then Lemma 2.3 [] states that every v 2 L loc () is in A if and only if v u 2 W ;2 (). Therefore each subclass A is a complete ane space, a translate of W ;2 (), where the tangent space at each pointisw ;2 (), the distance of u; v 2 A is ku vk W ;2 (). InA we use B(u; r) to denote fv 2A :ku vk W ;2 () <rg. Lemma 2.5 [] states that E : A! R belongs to C 2 (A ;R ) where E 0 (u) = [ru r+f(u)]dx; u 2A ;2W;2 (); E 00 (u)(; ) = [rr +f 0 (u) ]dx; u 2A ;; 2 W;2 (): We use ke 0 (u)k (ke 00 (u)k, respectively) to denote the norm of the liner (bilinear, respectively) form E 0 (u) (E 00 (u), respectively). It is clear from H- and H-2 that ke 00 (u)k is bounded uniformly in u. u is a critical point ofeif u 2Aand for every 2 W ;2 () [ru r+f(u)]dx =0: A critical point of Eis a classical solution of () by the standard elliptic regularity theory. The set of all critical points in A is denoted K.

MULTI-LAYER LOCAL MINIMUM SOLUTIONS 3 The global minima ina and in A are isolated critical points in the sense of Lemma 2.6 [] which states that there exists 0 > 0 such that for every u 2A \K,u6=,wehaveku k W ;2 () > 0. Theorem 3.2 [] asserts that in each A, there is a global minimum of E, i.e., there exists u 2A such that E(u) = inf v2a E(v): Wenow take U 2A,U 2 2A,..., U M 2A ( )M+ ( ) M to be M global minimaof E in their own subclasses. We say that U, U 2,...,U M are isolated global minimaif there exists 0 > 0 such that for every u 2B(U i ; 0 )nfu i g and every i =;2; :::; M, we havee(u)>e(u i ). The U i 's being isolated implies that the domain can not be a cylinder, i.e., 6= R 0 where 0 R d, since in a cylinder no global minimum in A or A is isolated due to the translational invariance. Two important operators are dened on A. Let k be an integer, and dene the shift operator k : A!A for ; 2f ;gby (8) k u(x)=u(x (k; 0; :::; 0)); x2: Dene the paste operator : A A!A for ;; 2f ;gby (9) (u; v) =u+v : A recursive use of (9) extend to : A 2 (0) A3 2 ::: A k!a by (u ;u 2 ; :::; u k )=(u ;(u 2 ;(:::; (u k ;u k )))): These two operators are often used together. If there is no danger of confusion, we write j u for ( j u ; j2 u 2 ; :::; jk u k ). The main result in this paper is the following existence theorem, which improves Theorem 4.4 []. Theorem. Let U 2A,U 22A,...,U M 2A ( )M+ ( ) M be isolated global minima in their own subclasses. Then for each r 2 (0; minf 0 ; 0 ;2 p js(0; =2)jg) there exists L>0such that as long as minfj 2 j ;j 3 j 2 ; :::; j M j M g >Lthere exists V 2B( j U; r=2) with E(V )= inf E(u); u2b( ju;r) i.e., there isalocal minimum of E in B( j U; r) A ( )M+. Recall that j U = ( j U ; j2 U 2 ; :::; jm U M ), 0 measures how isolated the U i 's are, 0 measures how isolated and are, and js(0; =2)j is the Lebesgue measure of S(0; =2). Remark 2. In Theorem 4.4 [] the U i 's are assumed isolated as critical points, while here they are merely isolated as global minima. Remark 3. Each U i can be regarded as a single layer and j U as a function of k layers. Since the local minimum V is close to j U, V is a k-layer solution.

4 XIAOFENG REN 2. Proof of Theorem To make the proof of Theorem more readable, we assume M = 2. The general case can be handled along the same line. We use C, C, C 2,... to denote generic constants that may vary from line to line. We often do not mention passing to a subsequence when we do so. Let U 2 A and U 2 2 A be two isolated global minima ofe, and 0 be the radius of the balls around U and U 2 in which there is no other global minima. Take twointegers j and j 2, j <j 2, and look for a local minimum of E in B( j U; r) A for some r 2 (0; minf 0; 0 ;2 p js(0; =2)jg): Here j U = ( j U ; j2 U 2 ) serves as an approximate solution. We rst show that E(u) is large for all u 2B( j U; r)nb( j U; r=2). Lemma 4. Fix r 2 (0; minf 0 ; 0 ;2 p js(0; =2)jg). There exist L>0and >0 such that for every pair of integers (j ;j 2 ) with j 2 j >L E(u) for all u 2B( j U; r)nb( j U; r=2). inf E(v)+ Remark 5. L is a lower bound of the distance between the layers. In general the larger r is, the smaller L can be. We postpone the proof of Lemma 4 to next section. Take u n 2B( j U; r) such that () n! E(u n)= inf E(v): Because of Lemma 4, we can safely assume u n 2B( j U; r=2). We now show that fu n g isapalais-smale sequence. Recall that a sequence fg n g is a Palais-Smale sequence if E(g n )! c 2 R and ke 0 (g n )k!0asn!. If fu n g is not a Palais-Smale sequence, then we can assume ke 0 (u n )k!>0as n!. Find n 2 W ;2 () with k n k W ;2 () = such that E 0 (u n ) n =2. Then consider for t 2 (0;r=2) E(u n t n )=E(u n ) te 0 (u n ) n +(t 2 =2)E 00 (u n t n n )( n ; n ) E(u n ) (=2)t + Ct 2 inf E(v) +o() (=2)t + Ct 2 where t n 2 (0;t) is guaranteed by the Taylor expansion formula and the constant C comes from the fact that E 00 is bounded. o() stands for a quantity that approaches 0 as n!. Choosing n sucient large and t suciently small, we deduce E(u n t n ) < inf E(v) which is impossible since u n t n 2B( j U; r). This proves that fu n g isapalais- Smale sequence. We quote a characterization of Palais-Smale sequences from [].

MULTI-LAYER LOCAL MINIMUM SOLUTIONS 5 Proposition 3. []. Let fu n g be a Palais-Smale sequence ina, and 2 f ; g. If n! E(u n)=0, then A = A for some 2f ;gand If n! ku n k W ;2 () =0: n! E(u n) > 0, then there exist w ;w 2 ; :::; w k 2 Knf ; g, k, w i 2 A i+ i, = and k+ =, and k integral sequences fl ;n g, fl 2;n g,...,fl k;n g with n! (l i+;n l i;n )=for each i =;2; :::; k such that n! ku n ( l;n w ; l2;n w 2 ; :::; lk;n w k )k W ;2 () =0; along a subsequence offu n g. n! E(u n)=e(w )+E(w 2 )+::: + E(w k ) Applying Proposition 3. [] tou n we nd k integral sequences fl ;n g, fl 2;n g,..., fl k;n g, and k nontrivial critical points w, w 2,...,w k such that ku n ln wk W ;2 () = o(). Then k j U ln wk W ;2 () r=2+o(). If one of the l i;n 's approaches or, sayl k;n!,asn!, then r=2 k j U ln wk W ;2 () + o() kw k +k W ;2 () + o() 0 + o() by Lemma 2.6 [], which is inconsistent with the assumption on r. Therefore k = and l ;n is bounded in n. We can select a proper subsequence of fl ;n g and shift w to assume l ;n = 0. Then with the help of () ku n w k W ;2 ()! 0; E(w ) = n! E(u n)= inf E(v); and w 2B( j U; r=2), i.e., w is a local minimum of E in B( j U; r). The proof of Theorem is complete after we set V = w. 3. Proof of Lemma 4 Suppose the lemma is not true. Then there exist r satisfying 0 <r<minf 0 ; 0 ;2 p js(0; =2)jg; a sequence of pairs of integers (j ;n ;j 2;n ), with j 2;n fu n gb( jn U; r)nb( jn U; r=2) such that (2) E(u n ) inf E(v) =o() v2b( jn U;r) as n!. We can nd a constant C independent ofnsuch that (3) E(u) <C j ;n!, and a sequence for all u 2B( jn U; r). To see (3) we estimate for each u 2B( jn U; r) = j 2 je(u) E( jn U)j jr(u jn U)+r jn Uj 2 jr jn Uj 2 + 2 [W (u) W ( jn U)]j

6 XIAOFENG REN = j 2 jr(u jn U)j 2 + r(u jn U) r jn U+ [W(u) W( jn U)]j 2 kr(u j n U)k 2 L 2 () + kr(u j n U)k L 2 ()kr jn Uk L 2 () +kf( jn U)k L 2 ()ku jn Uk L 2 () + Cku jn Uk 2 L 2 () C (kr jn Uk L 2 () + kf( jn U)k L 2 ())ku jn Uk W ;2 () + C 2 ku jn Uk 2 W ;2 () C qe( jn U)ku jn Uk W ;2 () + C 2 ku jn Uk 2 W ;2 () : The last inequality follows from (4). The last line is bounded independent ofn since E( jn U)=E(U )+E(U 2 )+o() and ku jn Uk W ;2 () r. This proves (3). If we write = [ k= S(k; =2), we can nd a sequence fm ng of integers with (4) and (5) by (3). (4) and (5) actually imply (6) n! (m n j ;n ) = n! (j 2;n m n )= n! [ n! S(m n;) 2 jru nj 2 + W (u n )] = 0 To see (6) we use Lemma 2. [] to obtain for some 2f (7) Consider From (5) we know (8) About (u n n! [jr(u n )j 2 + ju n j 2 ]=0: S(m n;=2) sup jbu n (x ) j =0 x 2(m n =2;mn+=2) ;g. In particular, ) 2 we set bu n (m n ) = o(): [jr(u n )j 2 + ju n j 2 ]: S(m n;=2) jr(u n S(m n;=2) G n = fx 2 S(m n ; =2) : ju n (x) )j 2 = o(): j <g; B n = S(m n ;=2)nG n where is so small that for all u 2 ( ;+), c (u ) 2 W (u) c 2 (u ) 2 for some positive c and c 2. The reader may think G n as a good set and B n as a bad set. On the good set G n by (5) we nd (9) ju n j 2 C W (u n )=o(): G n G n

MULTI-LAYER LOCAL MINIMUM SOLUTIONS 7 On the bad set B n we note that ju n (x) j 2ju n (x) bu n (m n )jif we choose n large enough because of (7). Therefore with the help of the Poincare inequality (20) ju n j 2 4 ju n bu n (m n )j 2 C jru n j 2 = o() B n S(m n;=2) S(m n;=2) by (5). Then (8), (9) and (20) imply [jr(u n )j 2 + ju n j 2 ]=o(): S(m n;=2) We need to show =. Assume =. Then it follows r 2 ku n jn Uk 2 W ;2 () [jr(u n jn U)j 2 + ju n jn Uj 2 ] S(m n;=2) = ( ) 2 + o()=4js(0; =2)j + o() S(m n;=2) with the help of (4). This is inconsistent with our assumption on r, and (6) is proved. We then truncate u n at S(m n ; =2) to dene (2) v n = un (x) if x 62 S(m n ; =2) (u n (x) )(x m n )+ if x 2 S(m n ; =2) where is a smooth function such that 0 if x 2 [ =4; =4] (x) = if x 62 [ =2; =2] : It follows from (6) and (2) (22) We set E(v n ) E(u n )=o(); and kv n u n k W ;2 () = o(): v ;n (x) = vn (x) if x m n if x m if x ; v >m 2;n (x) = n n v n (x) if x : >m n Clearly v ;n 2A,v 2;n 2A,v n=(v ;n ;v 2;n ) and (23) E(v n )=E(v ;n )+E(v 2;n ): From E(v ;n ) E(U ), E(v 2;n ) E(U 2 ), (2), (22) and (23) we deduce (24) On the other hand by (4) which implies inf E(v) E(U )+E(U 2 )+o(): v2b( jn U;r) E( jn U)=E(U )+E(U 2 )+o(); (25) inf E(v) E(U )+E(U 2 )+o(): v2b( jn U;r)

8 XIAOFENG REN Combing (24) and (25) we deduce and (26) inf E(v) =E(U )+E(U 2 )+o() v2b( jn U;r) E(v ;n )=E(U )+o(); E(v 2;n )=E(U 2 )+o(): We turn our attention to the distance between v ;n and j;n U, and the distance between v 2;n and j2;n U 2. Clearly kv ;n j;n U k W ;2 () + kv 2;n j2;n U 2 k W ;2 () kv n jn Uk W ;2 () r=2+o() by the triangle inequality and (22). Then either (27) or (28) kv ;n kv 2;n j;n U k W ;2 () r=4+o() j2;n U 2 k W ;2 () r=4+o(): Assume without the loss of generality that the former occurs. We look for an upper bound for kv ;n j;n U k W ;2 (). Consider, with the help of (4), jrv n r jn Uj 2 jrv n r jn Uj 2 x <m n = j(rv ;n r j;n U )+r j2;n U 2 j 2 x <m n j[ jrv ;n x <m n r j;n U j 2 ] =2 [ jr j2;n U 2 j 2 ] =2 j 2 x <m n (29) = j[ jrv ;n x <m n r j;n U j 2 ] =2 + o()j 2 : Also note jrv ;n r j;n U j 2 = jrv ;n r j;n U j 2 + jr j;n U j 2 x <m n x >m n (30) = x <m n jrv ;n r j;n U j 2 + o() again by (4). Then we deduce from (29) and (30) jrv ;n r j;n U j 2 jrv n r jn Uj 2 +o(): A similar argument shows jv ;n j;n U j 2 We then nd, with the help of (22), (3) jv n jn Uj 2 + o(): kv ;n j;n U k W ;2 () kv n jn Uk W ;2 () + o() r + o():

We shift v ;n back by (32) Note that (26) implies MULTI-LAYER LOCAL MINIMUM SOLUTIONS 9 j ;n to consider j;n v ;n.from (27) and (3) we deduce r=4+o() k j;n v ;n E(v ;n )! E(U )= U k W ;2 () r + o(): inf E(v) v2a as n!, i.e., fv ;n g is a global minimizing sequence of E in A. Asinthe proof of Theorem, fv ;n g (as well as f j;n v ;n g)isapalais-smale sequence. Applying Proposition 3. [] tof j;n v ;n g,we nd k integral sequences fl ;n g, fl 2;n g,...,fl k;n g, and k nontrivial critical points w, w 2,...,w k satisfying k j;n v ;n ln wk W ;2 ()! 0asn!, which implies with the help of (32) (33) r=4+o() ku If one of the l i;n 's approaches r ku ln wk W ;2 () r + o(): or as n!,sayl k;n!, then (33) implies ln wk W ;2 () + o() kw k +k W ;2 () + o() 0 + o(); which is again inconsistent with the assumption on r. We conclude that k = and l ;n is bounded in n. By passing to a subsequence of fl ;n g and shifting w we can assume l ;n = 0. Then we deduce with the help of (33) k j;n v ;n w k W ;2 () = o(); r=4ku w k W ;2 () r: Since f j;n v ;n g is a minimizing sequence in A,we nd E(w )=E(U ) and r=4 ku w k W ;2 () r< 0. This is inconsistent with the assumption that U is the only minimum in B(U ; 0 ). The proof of Lemma 4 is complete. References. X. Ren, Variational approach to multiple layers of the bistable equation in long tubes, Arch. Rational Mech. Anal., to appear. Institute for Mathematics and its Applications, University of Minnesota, Minneapolis, MN 55455 E-mail address: ren@ima.umn.edu