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Functional differential equations of a type similar to $f'(x) = 2f(2x+1) - 2f(2x-1)$ and its application.(Dynamics of functional equations and numerical simulation)

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(1)

Functional differential

equations

of

a

type

similar to

$f’(\mathrm{x})=2f(2x +1)$

$-2f(2x-1)$

and

its application.

大阪教育大学

米田

(Tsuyoshi Yoneda)

Department of

Mathematics

Osaka

Kyoiku

University

Frederickson

$\int_{\mathrm{L}}1$

],

[2}

(1971)

investigated functional-differential equations of

ad-vanced

type

(0.])1

$f’(x)=af(\lambda x)+bf(x)$

,

where A

$>1$

,

and provided several

properties

of

solutions.

Kato

and McLeod

[4]

(1971)

and

Kato [

$3_{d}1$

(1972)

studied

asymptotic behavior

of solutions of (0.1).

By

using

another

method, the

author

[6]

constructed one of the solutions

for

the

equation

(0.2)

$\{$

$f’(x)=af(2x)’$

.

$x$

$\in \mathbb{R}$

$=l-\backslash \infty,$

$+\infty \mathrm{I},$

,

$f\acute{(}0)=0$

,

where

$a$

is

a

constant with

$a$

$\neq 0$

. The

solution

is

not unique. If

$f$

is

a

solution,

then

a

constant

times

$f$

is

also a solution.

Our solutions are

infinitely differen liable

and bounded on

R. In

$\mathrm{I}6\underline{1}$

,

the

author gave

the

graph of

the

solution

$f(x,1$

of

(0.2)

with

$a$

$=4$

(Figure 1).

(2)

In

this

paper,

we

construct

a solution

for the

functional

differential

equation;

(0.3)

$f^{(n\}}(x)= \lambda^{n\dotplus 1}\sum_{j}cj\mathcal{B}_{j}^{n}\sum_{t=\iota}^{n}\hat,(-1)^{1}$$(\begin{array}{l}nt\end{array})f\mathrm{f}\lambda x-\backslash \frac{l-n/2+nk_{j}}{\beta_{j}})$

,

where

$\nabla_{j}\angle-c_{j}=1_{j}\sum_{j}c_{\mathrm{i}}\beta;<\infty,c_{j}\geq 0$

,

$\inf_{j}\beta_{j}>0$

,

$\sup_{j}|k_{j}$

.

[

$<\infty$

and

$\sum_{j}$

1

$\mathrm{s}$

finite

sum

or

infinite

sum.

The solution

is

unique

in

$L^{1}(\mathbb{R}\rangle$

up to

a

multiplicative constant

and

it is in

$C_{comp}^{\infty}(\mathrm{R})$ $\cap L^{1}(\mathbb{R})$

.

(Some

special

cases

were treated in [5].) We

also

give

the

method

of

cal culating

numerical

data.

For example, the following is

a

special

case

of

(0.3).

$(0,4)$

$f^{J}(x,\}=4f(2x,1 -4f(2x-1)$

.

The graph of the

solution of (0.4) is in

Figure 2, which

is

a

component of

the graph

of

Figure

1.

Our main result

is

as

follows.

FIGURE

2. The solution

of

$(0.4\grave{J}$

.

Theorem

0.1. The equation

$(0.3)\backslash$

has

a

unique

solution

in

$L^{1}\{\mathbb{R}$

)

up to

a

multi-plicative constant and it is in

$C_{\mathrm{c}omp}^{\infty}(\mathbb{R})$

{T

$L^{1}(\mathrm{i}\mathrm{R})$

.

We

give

some

examples of (0.3).

$(\mathrm{E}1)\backslash f^{t}(x)=2f(2x+1)-2f(2x-1)$

,

(E2)

$f’(x)=16f(4x)-16f(4x -1)$ ,

(E3)

$f^{\mathit{1}}(x)=(9/4)f(3x/2\}-\{9/4)f(3x/2-1)$

,

(E1)

$f’(x)=3;(.2x)-2f\zeta 2x$

- $1$

)

$-f(2x-2)$

,

(E5)

$f^{J}(x)=3f(2x)-3f(2x-1)+f(2x-2)-f_{\backslash }^{(}2x-3)_{7}$

(3)

(E7)

$\mathrm{f}"(\mathrm{x})=8f(2x+1)$

$-16f(2x)+8f\zeta 2x-1)$

.

(E1},

$\mathrm{s}\mathrm{u}\mathrm{p}\mathrm{p}f=[0, 1]$

(E2),

$\mathrm{s}\mathrm{u}\mathrm{p}\mathrm{p}/=[0, 1/3]$

(E3),

$\mathrm{s}\mathrm{u}\mathrm{p}\mathrm{p}f=[0,2]$

$\overline{0|,\prime}///’/’/^{l}/’\backslash \wedge\frac{\backslash \backslash |\backslash _{4}\backslash _{\backslash 1_{\mathrm{I}}^{\mathrm{t}}\backslash \backslash 1}\backslash \backslash \sim|}{12}$

(E4),

$\mathrm{s}\mathrm{u}\mathrm{p}\mathrm{p}f=[0_{;}2]$

(E5),

$\mathrm{s}\mathrm{u}\mathrm{p}\mathrm{p}f=\mathrm{l}\mathrm{r}_{\mathrm{Q}}$

,

$3_{\mathit{1}}^{1}$

FIGURE 3. Solution of the

equations

(E1) (E5),

$0 \{|||\mathrm{t}|_{1}||’ \mathrm{m}^{i}\frac{/^{l}\backslash j/_{11\backslash _{1}}^{/^{\Gamma_{\backslash }}\backslash }|_{1}\prime \mathfrak{l}\backslash \backslash \backslash \backslash \backslash \backslash \neg|}{12}//\cdot$

(E6)

and

(E7),

$\mathrm{s}\mathrm{u}\mathrm{p}\mathrm{p}f=[0,2]$

.

FIGURE

4. Solution

of

the equation

(E6) and (E7).

We

have

considered

application of the function

(E1)

by

using “Quark theory”

es-tablished

by

ff.Trebel.

Next section, we

introduce

the

result

of

application, This

application is

considered with Yoshihiro Sawano

who belongs to Tokyo University.

1.

RESULT

OF

APPLICATION

(4)

Let

$0<p$

,

$q\leq\infty$

and

$s>\sigma_{\mathrm{p}}$

.

$B_{pq}^{\delta}(\mathbb{R})$

is

a set

of Schwartz

distributions

$f$

for

which

$f$

can

be

written

as

(1.1)

$f= \sum_{\beta\in \mathrm{N}_{\mathrm{O}}^{d}}\sum_{\nu=0}^{\infty}\sum_{m\in \mathrm{Z}^{d}}\lambda_{\nu,m}^{9}.l2^{-\nu(s-d/p)}(2^{p}x-m)^{\beta}\phi(2^{\nu}x-m)$

where,

the finction

$\phi$

satisfies

$\phi’(x)=2\phi(2x+1)-2\phi(2x-1)$

.

Theorem 1.1. The equation

$f^{l}(x)=f(x-1)$

can

solve

explicty with

following

initid data

$f|_{[0_{1}\mathrm{I}]}=( \sum_{\beta\in \mathrm{f}\backslash \mathrm{i}_{0}}\sum_{\nu\in \mathrm{E}_{0}},\sum_{m\in_{arrow:q_{\nu_{\mathrm{t}}m}\mathrm{n}[0,\mathrm{x}]\neq\emptyset}^{m}}\lambda_{\nu,m}^{\beta}2^{-\nu(s-d/p)}(2^{\nu}x-m)^{\beta}\phi(2^{\nu}x-m\rangle)oe\in \mathrm{f}^{0,1}]$

The solution

$f|\mathfrak{t}1,2_{\mathrm{J}}^{1}$

can

be

written

as

follows;

$f(x)$

$=$

$f(1)+ \sum\sum$

$\beta\in \mathrm{N}_{0}\nu\in 1\forall 0m\in \mathbb{Z}j\sum_{q_{\nu,m}\cap[0,1]\neq \mathfrak{g}}2^{-\nu}\lambda_{\nu_{\mathrm{J}}m}^{\beta}\oint_{\nu,m}^{*}(x -1)$

$+( \oint_{\mathrm{P}_{\vee}}. x^{\beta}\phi(x)dx)\sum_{\nu\in \mathrm{R}^{1_{\mathrm{Q}}}}\sum_{\mathrm{z}\leq 2^{\nu}}(\sum_{t=0}^{m-2}\lambda_{\nu,t}^{0}2^{-\nu)}\phi(2^{\nu}x-m-1)$

.

where

$\phi_{\nu,m}^{\beta*}(x)$

$:=$

$( \sum_{\tau\subset\emptyset}^{\beta}(-1)^{\gamma}$$(\begin{array}{l}\beta\gamma\end{array})$

$(2^{\nu}x-m)^{\beta-\gamma}I_{\gamma}(\phi(2^{\nu}x-m)))$

$-2-p(s- \frac{\#}{\mathrm{p}})_{(}[_{-\sim}\overline{|\mathfrak{l}}dx^{\beta}\phi(x)$

&)

$\sum_{t=2}^{\infty}\phi(2^{\nu}(x-l)-m)$

,

$I_{\beta}( \phi)(x)=\sum_{j_{\theta+1}=0}^{\infty}\sum_{I\rho=0}^{\infty}-,\cdot$

. .

$\sum_{j_{1}=0}^{\infty}2^{\frac{\beta[\beta_{\mathrm{T}^{1}}1]}{2}}\phi(\frac{x-2^{\beta+1}+1}{\mathfrak{X}^{+1}}-\sum_{\gamma=1}^{\beta+\mathrm{I}}\frac{j_{\gamma}}{2^{\gamma-1}})$

and

$I_{0}( \phi)(x)=\sum_{\mathrm{j}=0}^{\infty}\phi(\frac{x-1-2j}{2})$

.

2.

ACKNOWLBDGEMENT

(5)

REFERENCES

[1] P.

0

Frederickson,

Global

solutions

to certain nonlinear

functional

differential

equations.

J.

Math. Anal.

Appl.

33

(1971),

355-358.

[2] P.

O.

Frederickson,

Diricklet

series

solutions

for

certain

functional differential

equations.

Japan-United

States Seminar on

Ordinary

Differential

and

Functional Equations

(Kyoto,

1971),

249-254.

Lecture Notes

in

Math.,

Vol.

243,

Springer,

Berl

in,

1971,

[3]

T. Kate,

Asymptotic behavior

of

solutions

of

the

functional

differential

equation

$y’(x\rangle=$

$\mathrm{a}\mathrm{y}(\mathrm{X}\mathrm{x})$

$+by(x)_{\dot{/}}$

Delay

and

functional

differential

equations

and

their

applications

(Proc.

Conf.,

Park

City, Utah, 1072),

Academic

Press,

New

York,

1972,

197-217.

[4]

T. Kato

and

J.

B.

$*\lambda\prime \mathrm{I}\mathrm{c}\mathrm{L}\mathrm{e}\mathrm{o}\mathrm{d}$

, The

functional-differential

equation

$y’$

(x)

$=\mathrm{a}\mathrm{y}(\mathrm{X}\mathrm{x})$

$+by\acute{t}x\}$

,

Bull.

Amer.

Math.

Soc.

77

(1971),

891-937.

[5] T.

Yoneda,

Spline

functions

and

$n$

-pcriodic points,

Transactions

of

the

Japan Society

for

In-dustrial

and

Applied

Mathematics

(Japanese),

15

{2G05),

245-252.

I6J

T. Yoneda,

On the

funct

$\dot{‘}onaLd\mathrm{i}fferential$

equation

of

advanced

type

$f’(x)=af\acute{(}2x)$

with

$[(0)=$

0.

to appear in

Journal

of

Mathematical

Analysis

and

Applications.

[7]

T. Yoneda,

On

the

functional-differential

equation

of

advanced

type

$f’(x)=af\{\lambda x)_{f}\lambda\ovalbox{\tt\small REJECT}$ $1$

with

$f(0)$ $=0$

,

preprint.

DEPARTMENT

OF

MATHEMATICS,

OSAKA

KYOIKU

UNIVERSITY,

KASHIWARA,

OSAKA

582-$8582_{\tau}$

JAPAN

FIGURE 3. Solution of the equations (E1) (E5),

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