The ODE y'=y Characterizes Exponentials

Solutions of y'=y satisfy the law of exponents.

Here’s a self-contained proof that the solution to y=yy^\prime = y with y(0)=1y(0)=1 is an exponential function. This is one possible means of proving the existence of exponentials, when defined functionally:

Exponential Functions

An exponential function is a continuous nonconstant function E ⁣:RRE\colon\mathbb{R}\to\mathbb{R} satisfying the law of exponents E(x+y)=E(x)E(y)E(x+y)=E(x)E(y) for all x,yRx,y\in\mathbb{R}.

First a uniqueness result we’ll need:

Let f,gf,g be two solutions to the differential equation y=yy^\prime =y. Then they are constant multiples of one another.

Consider the function h(x)=f(x)g(x)h(x)=\tfrac{f(x)}{g(x)}. Differentiating with the quotient rule,

h(x)=f(x)g(x)f(x)g(x)g(x)2=f(x)g(x)f(x)g(x)g(x)2=0g(x)2=0\begin{align} h^\prime(x)&=\frac{f^\prime(x)g(x)-f(x)g^\prime(x)}{g(x)^2}\\ &= \frac{f(x)g(x)-f(x)g(x)}{g(x)^2}\\ &=\frac{0}{g(x)^2}\\ &=0 \end{align}

Thus h(x)=0h^\prime(x)=0 for all xx, which implies h=f/gh=f/g is a constant function, and gg is a constant multiple of ff as claimed.

Now we’re ready for the main theorem:

Let gg be any differentiable function which solves g=gg^\prime = g and has g(0)=1g(0)=1. Then gg is an exponential.

Let g ⁣:RRg\colon\RR\to\RR solve Y=YY^\prime = Y and satisfy g(0)=1g(0)=1. We wish to show that g(x+y)=g(x)g(y)g(x+y)=g(x)g(y) for all x,yRx,y\in\RR.

So, fix an arbitrary yy, and consider each of these separately, defining functions L(x)=g(x+y)L(x)=g(x+y) and R(x)=g(x)g(y)R(x)=g(x)g(y).
Differentiating,

L(x)=(g(x+y))=g(x+y)(x+y)=g(x+y)=L(x)\begin{align*} L^\prime(x)&=\left(g(x+y)\right)^\prime\\ &=g(x+y)(x+y)^\prime\\ &=g(x+y)\\ &=L(x) \end{align*}R(x)=(g(x)g(y))=(g(x))g(y)=g(x)g(y)=R(x)\begin{align*} R^\prime(x)&=\left(g(x)g(y)\right)^\prime\\ &=(g(x))^\prime g(y)\\ &=g(x)g(y)\\ &=R(x) \end{align*}

Thus, both LL and RR satisfy the differential equation Y=YY^\prime=Y. Our previous proposition implies they are constant multiples of one another,

L(x)R(x)=kxR\frac{L(x)}{R(x)}=k\hspace{1cm} \forall x\in\RR

To find this constant we evaluate at x=0x=0 where (using g(0)=1g(0)=1) we have L(0)=g(0+y)=g(y)L(0)=g(0+y)=g(y) R(0)=g(0)g(y)=g(y)R(0)=g(0)g(y)=g(y)

They are equal at 00 so the constant is 11:

L(x)R(x)=L(0)R(0)=g(y)g(y)=1\frac{L(x)}{R(x)}=\frac{L(0)}{R(0)}=\frac{g(y)}{g(y)}=1     L=R\implies L=R

But these two functions are precisely the left and right side of the law of exponents for gg. Thus their equality is equivalent to gg sayisfying the law of exponents for this fixed value of yy:

x,L(x)=g(x+y)=g(x)g(y)=R(x)\forall x,\,\, L(x)=g(x+y)=g(x)g(y)=R(x)

As yy was arbitrary, this holds for all yy, and gg is an exponential.

Note this proof does not establish the existence of a solution to this ODE, it only says if you have a solution then its an exponential. But this provides a much easier means of rigorously constructing an exponential: if we can develop techniques to build such a function (eg power series, and term by term differentiation) we will immediately know the result satisfies the law of exponents.

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