This Quantum World/Appendix/Exponential function

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The exponential function

We define the function exp(x) by requiring that

exp(x)=exp(x)  and  exp(0)=1.

The value of this function is everywhere equal to its slope. Differentiating the first defining equation repeatedly we find that

exp(n)(x)=exp(n1)(x)==exp(x).

The second defining equation now tells us that exp(k)(0)=1 for all k. The result is a particularly simple Taylor series:


exp(x)=k=0xkk!=1+x+x22+x36+x424+


Let us check that a well-behaved function satisfies the equation

f(a)f(b)=f(a+b)

if and only if

f(i+k)(0)=f(i)(0)f(k)(0).

We will do this by expanding the f's in powers of a and b and compare coefficents. We have

f(a)f(b)=i=0k=0f(i)(0)f(k)(0)i!k!aibk,

and using the binomial expansion

(a+b)i=l=0ii!(il)!l!ailbl,

we also have that

f(a+b)=i=0f(i)(0)i!(a+b)i=i=0l=0if(i)(0)(il)!l!ailbl=i=0k=0f(i+k)(0)i!k!aibk.

Voilà.

The function exp(x) obviously satisfies f(i+k)(0)=f(i)(0)f(k)(0) and hence f(a)f(b)=f(a+b).

So does the function f(x)=exp(ux).

Moreover, f(i+k)(0)=f(i)(0)f(k)(0) implies f(n)(0)=[f(0)]n.

We gather from this

  • that the functions satisfying f(a)f(b)=f(a+b) form a one-parameter family, the parameter being the real number f(0), and
  • that the one-parameter family of functions exp(ux) satisfies f(a)f(b)=f(a+b), the parameter being the real number u.

But f(x)=vx also defines a one-parameter family of functions that satisfies f(a)f(b)=f(a+b), the parameter being the positive number v.

Conclusion: for every real number u there is a positive number v (and vice versa) such that vx=exp(ux).

One of the most important numbers is e, defined as the number v for which u=1, that is: ex=exp(x):

e=exp(1)=n=01n!=1+1+12+16+=2.7182818284590452353602874713526


The natural logarithm ln(x) is defined as the inverse of exp(x), so exp[ln(x)]=ln[exp(x)]=x. Show that

dlnf(x)dx=1f(x)dfdx.

Hint: differentiate exp{ln[f(x)]}.

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