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Printed in India.

An Inequality on Solutions of Heat Equation*

DU-WONBYUN

DepartmentofMathematics,InhaUniversity,253Yong Hyun-Dong, Nam-ku,In-chon402-751,Korea

(Received28 April 1997;Revised17 October1997)

Letv(x,t)bethesolutionof the initial valueproblem forthendimensional heat equation.

Then,for anyaand foranyto>0,aninequality aboutv(a, t)andv(x, to)is obtained.

Keywords: Heatequation; Integraltransform;Positivematrix; Reproducingkernel 1991 Mathematics subjectClassification. Primary35K05;Secondary30C40

1.

INTRODUCTION

Forapositive integern, we considerthendimensionalheat equation

Xv(x, t) Otv(x, t), v(x, o) F(x),

X ]1n and

>

O;

xERn (1.1)

where AisthendimensionalLaplacian andFis amemberinthe space

Lz(R n)

for the Lebesgue measure on

R’.

Then, the solution is representedby

v(x, t)

2v F()exp

4t

d. (1.2)

Thisresearch is partiallysupported by KOSEF-GARC.

E-mail: [email protected].

269

(2)

Furthermore,fromtheexpression

(1.2)

weknowthatthesolutionv(x,

t)

canbeholomorphically extendedonthendimensionalcomplex space C with respect to the space variable x. For the time variable also,

v(x,t)

can be holomorphically extended on the right half plane D

{z Iz > 0}

of the complexplane C.These facts arefoundin[4,6].

In this paper, for anya E

n

and for a fixed time to, we derive an inequality which expresses the relation of v(a,

t)

and v(x,

to).

Our inequality is the generalization of an inequality in

[6]

for the n dimension.

THEOREM ForaninitialvaluesFin

L2( n)

letv(x,

t)

be thesolution

of

the ndimensionalheat equation

(1.1).

Then,

for

anya

n

and

for

any

to >

O, thefollowing inequalityis valid."

2t0 J

dAdr,

wherez x

+

iy

(x,

y6]),w A

+

i7

(A,

7-

).

Moreover,the equality holds

if

and only

if

F is a member in

M(n,a).

Here,

C(n, to)--

nE(n/Z)/(Z2"+Tr"-lto/2)

and

M(n,a)

is theclosure

of

thespace spanned linearlyby

{f()-

e

-l-al2

in

L2().

2.

SOME HOLOMORPHIC FUNCTION SPACES

WeletK(z, u) bethe

Bergman

kernelonthedomainDwithrespectto themeasuredxdy/Tr. Itisexplicitlyrepresentedby

K(z, u) / (z + )2.

Foranyq

>

1,weconsidertheHilbertspace

Hq {f."

holomorphicin

D]

JJ 12

-qdxdy

<

o,

[[fl[ZH" 7rF(2q 1) If(z) K(z, z)

z- x

+ iy}.

(3)

Then, the kernelfunction

Kq(z, u)= P(2q)K(z, bt) q, (z, bt)

EO D,

is the reproducing kernel of

Hq

in the following sense: for anyzED, K(.,

z)

isthe memberin

Hq

and every member

fin Hq

isrepresented by

f(z) (f, Kq(.,z))i4

q, z D,

where

{.,.)/_/q

istheinnerproductintheHilbertspace

Hq (refer

to[2,3]).

Meanwhile, the kernelfunction

Kq

canberepresented by

Kq(z, u) e-Ze-

2q-1d,

z,uD, (2.1)

andthe right handsideof

(2.1)

converges for allq

>

0.

Hence,

for anyq with0

<

q

<

1, thefunction

Kq

also determines the

Hq

thatadmits the

reproducing kernel

Kq(z, u) (see [1,7]).

Foranyq

>

0,wedenote

Kq(z, u) r(2q)K(z, b/) q,

Z,bt

D,

andwealsoconsidertheHilbertspace

Aq {g:

holomorphicin

D]

2__

ffD 12

[Igl[Aq rrP(2q + 1) [g’(z) K(z, Z)

-qdxdy

<

lim

g(x) 0}.

Since the mapping

f---f’

is the isometry from

Hq

onto

Hq_+_l, Hq- Aq,

and

Kq(z, u)

isthe

reproducing

kernel of

Aq (see [3]).

3.

PROOF OF THEOREM

Following the theoryofgeneralized integral transforms [5], we prove ourtheorem. First, for a---0,weconsider theintegral transform

7-{F(z)-

2x/_ ,,F()exp d-v

zD.

(4)

Forany

to >

0,wecalculatethe kernel form

(-- (--

K(z, U)

n/4

Since the function

T,,(z, u)

is positive matrix on D, it determines the reproducing kernelHilbert space

Sn (see

[1,7]). Ontheotherhand, the space

Sn

ischaracterizedby

Sn {f."

holomorphicin

D[

23n/2+Tr"/2-1f fz }

Ilfll

2

If’(z) 12x

n/2dxdy

<

oc

Hencewe havethenorminequality

IIv(O,z)ll < f IF()I

2

ds c. (3.1)

Fortheorthogonal complementN+/-of the null space N

R{F

E

L)(R")IT-[F(z) 0},

zED

the equalityin

(3.1)

holdsifand onlyifFis a memberinN

+/-.

In fact, N+/- is the closure of the space in

L2(I n)

which islinearly spanned by membersof the family

{G() exp(-cl12)

c

D},

and soN+/--M(n,

0).

From

[4],

thenormequality

( )

n/2

ffc" Iv(w’ to) 12

exp

( --oJ [’r12

dA67-

J,, IF(sC)l

2

d. (3.2)

holds, andfrom

(3.1)

and

(3.2)

ourinequalityis obtainedfora-0.

(5)

Foranya ER

n,

since

(1)n ( .a_12)

d

v(a, t) 2v/_ F()exp

4t

2v/ .F( + a)

exp d,

wehave

Ilv(a, t)][]. _< f. ]F( + a)12d- f. (3.3)

From

(3.2)

and

(3.3),

the inequality

(1.3)

is valid. Meanwhile, the equality in

(3.3)

holds ifand onlyif

F( + a)

E

M(n, 0).

Therefore the proof has beencompleted.

References

[1] N. Aronszajn, Theoryofreproducing kernels, Trans. Amer.Math. Soc. 68(1950), 337-404.

[2] J. Burbea,Totalpositivityof certainreproducing kernelsPacificJ.Math. 67(1976),

101-130.

[3] D.-W. Byun Isometrical mappings between the Szeg6 and the Bergman-Selberg spaces,ComplexVariables20(1992),13-17.

[4] D.-W.Byun,Relationshipbetween theanalyticsolutionsofthe heat equation, Math.

Japonica(1993)477-481.

[5] S. Saitoh,HibertspacesinducedbyHilbertspacevaluedfunctions,Proc.Amer.Math.

Soc.89(1983),74-78.

[6] S. Saitoh, Inequalitiesfor the solutions of the heatequation,inGeneralInequalities6, BirkhfiuserVerlag,BaselBoston (1992)139-149.

[7] S. Saitoh, TheoryofReproducing Kernelsand itsApplications,PitmanRes. Notesin Math.Series189,LongmanScientific&Technical,England,1988.

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