This Quantum World/Appendix/Exponential function
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[edit] 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
The second defining equation now tells us that exp(k)(0) = 1 for all k. The result is a particularly simple Taylor series:
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Let us check that a well-behaved function satisfies the equation
if and only if
We will do this by expanding the f's in powers of a and b and compare coefficents. We have
and using the binomial expansion
we also have that
VoilĂ .
The function exp(x) obviously satisfies
and hence 
So does the function f(x) = exp(ux).
Moreover,
implies f(n)(0) = [f'(0)]n.
We gather from this
- that the functions satisfying
form a one-parameter family, the parameter being the real number f'(0), and
- that the one-parameter family of functions exp(ux) satisfies
, the parameter being the real number u.
But f(x) = vx also defines a one-parameter family of functions that satisfies
, 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):
The natural logarithm ln(x) is defined as the inverse of exp(x), so exp[ln(x)] = ln[exp(x)] = x. Show that
Hint: differentiate exp{ln[f(x)]}.







