On the decay for M of solutions of parabolic with coefficients

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Publ. RIMS, Kyoto Univ. Ser. A Vol. 3 (1967), pp. 203-210 On the decay for M of solutions of parabolic with coefficients By Takasi KUSANO* ** 1. Introduction There is much current interest in the Cauchy problem for second order parabolic differential equations with unbounded coefficients: (A) Lu= S «,/(*, Ow,,,,-r-S bt(x, f)u xi + c(x, t}u u t =f(x, ). ij=i 1=1 For example, W. Bodanko [3] has proved the existence and uniqueness of solutions u(%, 0 =0(exp (^ # A )) of the Cauchy problem for (A), assuming that «f -/ = 0(i^ 2 " A ), bi = Q(\x\) and c = Q(\x\^ (from above) for large \x\, ^e(0, 2]. Under similar assumptions D. G. Aronson and P. Besala [1] have constructed a fundamental solution of the equation Lu = Q and solved the general Cauchy problem for (A) by giving an explicit formula for the solution in terms of the fundamental solution obtained. See also G. N. Smirnova [8]. We also mention a paper by P. Besala and P. Fife [2] in which the asymptotic behavior for large t of solutions of such equations is investigated. The main purpose of this note is to obtain an information about the behavior of decay for large \x\ of solutions of the Cauchy problem containing parabolic differential operators with unbounded coef- N ficients. It will be shown that an exponential decay property for large \x\ of the initial data is preserved for the solutions of the linear Received August 2, 1967. Communicated by M. Hukuhara. * Department of Mathematics, School of Science and Engineering, Waseda University. ** This research was done while the author was a Temporary Member of the Research Institute for Mathematical Sciences, Kyoto University, and was supported in part by Matsunaga Science Foundation.

204 Takasi Kusano homogeneous parabolic equation (A): Lu = Q, provided a i} = Q(\x 2 ~ A ), i, = 0( * ) and = 0(1) (from above), je(0,2], and also for the nonnegative solutions of the semilinear parabolic equation (B) S a tj (*, 0 w,,,, + S #,- (#, 0 w,, +/(#, *, u)-u t = 0, /,;=! i=l provided that 0 /y = 0(! # 2 ~ A ), J. = 0( # ) and that the nonlinear term f(x,t,it) is majorized by a concave function F(t,u) with jp(#, 0)=0. The author wishes to thank Professor Masuo Hukuhara for his valuable suggestions. 2. Statement of results We begin by considering the linear homogeneous parabolic equation (A) (/(XO 0). We assume that there exist positive constants ki 9 k 2 y k 3 and ^e(0, 2] such that (2. 1) 0^ *,j=i <*,.,(*, (2.2) *.(^OI^* (2.3) c(^,0^*8 for all (*, Oe "x [0, T] and f= (f ls -, Sj^E*. We say that a function t0(#, 0 defined on E* X [0, T] belongs to class E A for /le (0, 2] if there exist positive constants <z, M such that ]w;(^oi^mexp[^(l^i 2 + l) A/2 ], (^,0e -x [0, T]. We prove the following: Theorem 1. Let u(x,f) be a regular 1 ** solution of (A) belonging to class E A on E n x [0, T]. // the initial function is such that (2.4) N(^0)l for some positive a*, M Q, then there exist, for each e (0, T], positive numbers a h M t for which (2.5) «(*,0 i^ 1) By a regular solution we mean a function continuous on E ra X [O, T] whose first time derivative and second spatial perivatives are continuous on E^x(0»T], and which satisfies the given parabolic equation.

Parabolic equations with unbounded coefficients 205 In the Appendix we give an example which shows that in deriving from (2.4) the estimate (2.5) for each fe(0,t] the assumption (2.3) placed on (#, f) is in a sense essential and cannot be replaced by a less restrictive one (2.3*) c( under which the general theory of E A -so hit ions of (A) is developed. We now turn to the semilinear parabolic equation (B), for which the conditions (2. 1) and (2. 2) are assumed to hold. We assume that there exists a concave function F(t, u) with F(t, 0) = 0 such that (2. 6) sup/(*, t, u~)<f(t, u), (t, u) e [0, T] x E\ x B n Making use of the device due to I. L Kolodner and R. N. Pederson [5] we can prove the following: Theorem 2. Assume that F, F u, F HU are continuous and that F UU <^Q on [0, T] xe 1. Let u(x, f) be a nonnegative regular solution of (B) belonging to class E x and satisfying (2.7) 0^«(*,0)^M 0 exp [-^0(!*[ 2 + 1) A/2 ], x^e n for some positive constants <z 0, M Q. Let M O (#, 0 be a nonnegative regular solution of the linear homogeneous equation satisfying the initial condition Then, we have (2. 8) $<u(x, fi<u Q (x, Oex pm (5, 0)^, (x, 0 e " x (0, T]. This establishes the desired decay property of u(oc, ), because, according to Theorem 1, UQ(X, 0 behaves like its initial data for each *e(0, T]. We note that H. Fujita [4] has obtained a similar result for a class of semilinear parabolic equations of the form (B) but with a different nonlinearity.

206 Takasi Kusano 3. Proofs Proof of Theorem 1. Following M. Krzyzanski [6] we set (3.1) where a(f)>q and $(f) are bounded C 1 functions for t^q to be specified later. Then, the new dependent variable v (#, 0 satisfies the parabolic equation where *(*, i) =*,(*, 0-2MOS *,-,(*, y=i (jr, 0 =c(^, 0 +».;=! - ^ a - 2) a (0 (! * 2 + 1) A/2 " 2 S a t, (x, 0 jc,^ <,>-! M S [a,,(*, 0 +6i(jf, It is clear that there is a number kf, depending on the choice of <#GO> such that In view of (2. 1) (2. 3) we have (3.2) c*(^o^ci^ where we have set p = k l l 2, q = k 2 na, r= k 1 A(A If we define the C 1 functions by (X.Q

Parabolic equations with unbounded coefficients 207 and if we note that they satisfy the relations we have from (3. 2) «'(*) +/>«*(*) + </*(*) =0, * 8 + r*(0-0'(0 =0, on E n x [0, T] and satis- Obviously v(x,f) belongs to class E A fies the initial condition (note that < (0)=<z<>, /3(0) =0). Applying a maximum principle due to W. Bodanko ( [3], Theorem 2), we have \v(x, 0 <M, on * X [0, Tj. Hence, by (3.1), we conclude that lac^oi^m.expe-^coci^^ + D^ + lsco], (^,0e -x[0, T], from which the desired estimate (2.5) follows: M t = M^^,a t = Proof of Theorem 2 0 We observe first that (3. 3) F(i, u)<f u (t, O)M for (t, u) GE [0, T] x E\ since F M <LQ and F(l, 0)^0. Hence, the solution ^(/; ^) of the ordinary differential equation a(f}. is majorized by the solution w(t\ 0) of the linear ordinary differential equation that is, (3.4) v(t\ w t = F u (t,v)w, w(ff)=0, We compare the solution u(x, f) under consideration with the function w(t\ 0), noting that the former satisfies the differential ine- o j

'208 Takasi Kusano quality (3. 5) S 0,v (#, 0 M*,*, + S b s (#, 0 M,, i,/=i 1=1 and that the latter satisfies the linear parabolic equation S * f, (*, 0 w w + S *, (*, 0 w,, + F B (f, 0) w - w, - 0. Taking 0^maxM(#, 0) and applying a comparison theorem of W. x E» Bodanko ([3], Theorem 4), we obtain «(*,*): «>(*; 0), (^,0e -x [0, T]. Hence the solution u(x, f) is bounded on E n x [0, T], though assumed of class E A. We now consider the function u(x, f)=v(t\ U Q (X, 0)» the composition of v(t\ 0) and «0 (^, 0- Following closely L I. Kolodner and R. N. Pederson [5] (p. 358) we see that u(x, f) satisfies the differential inequality (3. 6) S * (x, 0 u XiXj + 2 4,. (^, 0 u xi + F(t, u) ~ u t!,j = l 2=1 Subtracting (3. 5) from (3. 6) we obtain the differential inequality ± a tj (x, 0 U^ + Olbtax, 0 U, t + F u (t 9 u*(x, 0) U- U t <Q L_ satisfied by the difference U(x,f)=u(x,f) u(x,f), where «*(^, 0 ji'jies between M(#, 0 and ^(^, 0, and hence is bounded on E*x [0, T]. ^An application of a theorem of W. Bodanko ( [3], Theorem 1) yields the inequality (3. 7) Q<u(x y t)<u(x, 0, (x, *)e "x [0, T], since u(x, 0) =u(x, 0) initially. The inequality (2.8) follows immediately from (3.7) and (3.4). 4. Appendix The examples which follow are suggested by M. Krzyzanski [6]. Example 1. Consider the particular parabolic equation

Parabolic equations with unbounded coefficients 209 where &>0 and / are constants. The solution of this equation belonging to class E 2 and satisfying the initial condition «O,0)=exp( - * 2 ), *e " is given explicitly by the formula JLi O>0: a constant) E" in terms of the fundamental solution V(x,t\y y s) constructed by A. Szybiak (see [6] and [7]): V(r f- v <? N ) ^\n9k(t <*} r v ^v,? I/, V«o y 7 olll^/v V U o y i ' ^ J y I h ^ ' I L_ fv J 2 -~ wnere x-^j'/ x *-^t j^tt -^y ^ ^ *-' > w ^-^«/ «-> ^-~-.,. 1=1 ZK An easy computation shows that T 2 exp a sin 2kt + k cos 2-^U L 2(<^si (^ sin 2kt j rk cos 2&0 Let ^0 = ^T-tan 1 -^- When t<t& the solution ^(^,0 decays exponentially as A: ->CX>; on the contrary it grows exponentially as # -»oo when --. 4k Example 2. Consider the parabolic equation where k>q and / are constants. We are concerned with the solution of this equation satisfying the initial condition where a, is a positive constant less than k. Making use of the fundamental solution constructed by A. Szybiak (see [6] and [7])

210 Takasi Kusano W(x. t; y. s) = ^-sinh2k(t s) I 2 L k J r k X exp ~^-(i^! 2 +ij 2 )< the solution sought is expressed as Proceeding as in Example 1 we have /2 (0, Let 0 be such that tanh2m 0 = - ^. Though the solution u(.x, f) K grows exponentially for large \x\ if t<t Q) it decays exponentially for large \x\ if t>t 0. REFERENCES [1] Aronson, D. G. and P. Besala, Parabolic equations with unbounded coefficients, J. Diff. Eqs. 3 (1967), 1-14. [2] Besala, P. and P. Fife, The unbounded growth of solutions of linear parabolic differential equations, Ann. Scuola Norm. Sup. Pisa, Ser. III. 20 (1966), 719-732. [3] Bodanko, W., Sur le probleme de Cauchy et les problemes de Fourier pour les equations paraboliques dans un domaine non borne, Ann. Polon. Math. 18 (1966), 79-94. [4] Fujita, H., On the blowing up of the Cauchy problem for u t = du + u l+a, J. Fac. Sci. Univ. Tokyo, Sec. I, 13 (1966), 109-124. [5] Kolodner, 1. 1. and R. N. Pederson, Pointwise bounds for solutions of semilinear parabolic equations, J. Diff. Eqs. 2 (1966), 353-364. [6] Krzyzanski, M., Evaluations des solutions de 1'equation lineaire du type parabolique a coefficients non bornes, Ann. Polon. Math. 11 (1962), 253-260. [7] Krzyzanski, M. and A. Szybiak, Construction et etude de la solution fundamentale de 1'equation lineaire du type parabolique dont le dernier coefficient est non borne I, II, Atti Accad. Naz. Lincei, Cl. Sc. Fis. Mat. Natur. Ser. VIII, 27 (1959), 1-10. [8] Smirnova, G.N., The Cauchy problem for parabolic equations degenerating at infinity, Mat. Sb. 70 (112) (1966), 59^604. (Russian)