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Question:

let $a\in(0,1)$, and such $f(x)\geq0$, $x\in R$ is continuous on $R$,

if $$f(x)-a\int_x^{x+1}f(t)dt,\forall x\in R $$ is constant,

show that

$f(x)$ is constant;

or $$f(x)=Ae^{bx}+B$$ where $A\ge 0,|B|\le A$ and $A,B$ are constant, and the positive number $b$ is such $\dfrac{b}{e^b-1}=a$

My try:

let $$f(x)-a\int_x^{x+1}f(t)dt=C$$ then we have $$f'(x)-af(x+1)+af(x)=0,\forall x\in R$$

other idea:

let $$F(x)=\int_{0}^{x}f(x)dx$$ then $$f(x)-a\int_x^{x+1}f(t)dt=F'(x)-a[F(x+1)-F(x)]=C$$ then I can't solve this ODE? maybe my idea is not good.

Thank you very much.

r9m
  • 17,938
math110
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  • If you are reducing the problem to an ODE, it seems like you have a Delay Differential Equation.

    I am wondering if using a numerical integration technique might work instead of making the reduction to ODE.

    Where did the question arise from? Is there any clues as to what methods might be necessary?

    – kleineg Mar 19 '14 at 14:31
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    Instead of trying to do this directly, have you tried using standard uniqueness/existence theorems for ODE's? If you can check that the solution space has dimension precisely two, and that any $A,B$ correspond to a solution $f$ as you have defined above, you would be done. – Frank Mar 19 '14 at 16:18

2 Answers2

2

A very pretty problem! Under the hypotheses stated, we will conclude that $f(x) = A e^{bx}+B$ with $A, B\ge0$. The amplitude of $B$ cannot be restricted.

Since $f$ is continuous, the integral is differentiable and by the OP's calculation, $$ \frac{d}{dx}(e^{ax} f(x)) = e^{ax}(f'(x)+a f(x)) = e^{ax} a f(x+1)\ . $$ It follows $u(x)=e^{ax}f(x)$ is nonnegative and satisfies $$ u'(x) = c u(x+1) , \quad c=a e^{-a}. $$ By a simple induction argument, $u$ is infinitely differentiable with all derivatives nonnegative on $\mathbb R$. Thus its reflection $v(x)=u(-x)$ is completely monotone, meaning all its even derivatives are nonnegative and all its odd derivatives are nonpositive.

By Bernstein's theorem on completely monotone functions, there is a unique Borel measure $d\mu$ on $[0,\infty)$ such that $$ v(x) = u(-x) = \int_0^\infty e^{-tx}\,d\mu(t) $$ for all $x>0$. But then, since $v'(x)=-u'(-x)=-c v(x-1)$, we find that for $x>1$, $$ c v(x) = -v'(x+1) = \int_0^\infty e^{-tx} e^{-t}t\,d\mu(t). $$ By uniqueness of the representing measure, $c\,d\mu(t)=te^{-t} d\mu(t)$ as measures on $[0,\infty)$. Hence $(c-te^{-t})d\mu(t)=0$, and the support of $d\mu$ must lie in the set of $t$ such that $c=te^{-t}$.

Since $t\mapsto te^{-t}$ increases on $(0,1)$ and decreases on $(1,\infty)$, this set consists of two points: the number $a\in(0,1)$ and the unique $\hat a>1$ such that $ae^{-a}=\hat a e^{-\hat a}$. Therefore $d\mu$ is a nonnegative combination of delta masses at $a$ and $\hat a$: $$ d\mu(t) = B\,\delta(t-a) + A\, \delta(t-\hat a) $$ where $B, A\ge0$. Consequently, for all $x>1$, $$ v(x) = B e^{-ax} + A e^{-\hat a x} = e^{-ax}f(-x), $$ hence $f(x) = B + A e^{bx}$ where $b=\hat a-a>0$ satisfies $a e^b = \hat a = b+a$ as desired.

The argument above actually applies for any translate $v(x-k)$. Consequently the desired representation of $f$ holds for all $x$.

Bob Pego
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-1

I need help proving the following result:

If $f(x)-a\int_x^{x+1}f(t)dt$ is constant, then $f(x)$ is constant or $f(x)=Ae^{bx}+B$.

  1. Firstly, we transform this ODE to the form: $$\frac{dy}{dx}+P(x)y=Q(x).$$

Such equation has the solution: $$y=e^{-\int{Pdx}}$$[\int{Qe^{\int{Pdx}}+C}].$$

  1. Then,we calculate this solution as the following way: $$fe^{ax}=\int{Qe^{ax}dx+C}\implies(Ae^{bx}+B)e^{ax}=\int{Qe^{ax}dx+C}\implies Qe^{ax}=Aae^{b}e^{(a+b)x}+Bae^{ax}\implies Q=Aae^{b}e^{bx}+Ba.$$

Therefore, $$f(x+1)=f^{'}(x)\frac{e^{b}}{b}+C\implies Q=f(x+1)$$ where $Aae^{b}\ge0,$ $Ba\le{Aae^{b}}$.

From my point, this ODE has the solution of $f=Ae^{\lambda{x}}+B$ is obviously, the only thing we should prove is that $\lambda=b=a(e^{b}-1)$.