# Characterizations of the exponential function

In mathematics, the exponential function can be characterized in many ways. The following characterizations (definitions) are most common. This article discusses why each characterization makes sense, and why the characterizations are independent of and equivalent to each other. As a special case of these considerations, we will see that the three most common definitions given for the mathematical constant *e* are also equivalent to each other.

## Characterizations

The six most common definitions of the exponential function exp(*x*) = *e*^{x} for real *x* are:

- 1. Define
*e*^{x}by the limit

- 2. Define
*e*^{x}as the value of the infinite series

- (Here
*n*! denotes the factorial of*n*. One proof that*e*is irrational uses this representation.)

- (Here

- 3. Define
*e*^{x}to be the unique number*y*> 0 such that

- This is as the inverse of the natural logarithm function, which is defined by this integral.

- 4. Define
*e*^{x}to be the unique solution to the initial value problem

- (Here,
*y*′ denotes the derivative of*y*.)

- (Here,

- 5. The exponential function
*f*(*x*) =*e*^{x}is the**unique Lebesgue-measurable function**with*f*(1) =*e*that satisfies- (Hewitt and Stromberg, 1965, exercise 18.46). Alternatively, it is the
**unique anywhere-continuous function**with these properties (Rudin, 1976, chapter 8, exercise 6). The term "anywhere-continuous" means that there exists at least a single point at which is continuous. As shown below, if for all and and is continuous at*any*single point then is necessarily continuous*everywhere*. - (As a counterexample, if one does
*not*assume continuity or measurability, it is possible to prove the existence of an everywhere-discontinuous, non-measurable function with this property by using a Hamel basis for the real numbers over the rationals, as described in Hewitt and Stromberg.) - Because
*f*(*x*) =*e*^{x}is guaranteed for rational*x*by the above properties (see below), one could also use monotonicity or other properties to enforce the choice of*e*^{x}for irrational*x*, but such alternatives appear to be uncommon.

- One could also replace the conditions that and that be Lebesgue-measurable or anywhere-continuous with the single condition that . This condition, along with the condition easily implies both conditions in characterization 4. Indeed, one gets the initial condition by dividing both sides of the equation
- by , and the condition that follows from the condition that and the definition of the derivative as follows:

- One could also replace the conditions that and that be Lebesgue-measurable or anywhere-continuous with the single condition that . This condition, along with the condition easily implies both conditions in characterization 4. Indeed, one gets the initial condition by dividing both sides of the equation

- 6. Let
*e*be the unique real number satisfying

- This limit can be shown to exist. This definition is particularly suited to computing the derivative of the exponential function. Then define
*e*^{x}to be the exponential function with this base.

- This limit can be shown to exist. This definition is particularly suited to computing the derivative of the exponential function. Then define

## Larger domains

One way of defining the exponential function for domains larger than the domain of real numbers is to first define it for the domain of real numbers using one of the above characterizations and then extend it to larger domains in a way which would work for any analytic function.

It is also possible to use the characterisations directly for the larger domain, though some problems may arise. (1), (2), and (4) all make sense for arbitrary Banach algebras. (3) presents a problem for complex numbers, because there are non-equivalent paths along which one could integrate, and (5) is not sufficient. For example, the function *f* defined (for *x* and *y* real) as

satisfies the conditions in (5) without being the exponential function of *x* + *iy*. To make (5) sufficient for the domain of complex numbers, one may either stipulate that there exists a point at which *f* is a conformal map or else stipulate that

In particular, the alternate condition in (5) that is sufficient since it implicitly stipulates that *f* be conformal.

## Proof that each characterization makes sense

Some of these definitions require justification to demonstrate that they are well-defined. For example, when the value of the function is defined as the result of a limiting process (i.e. an infinite sequence or series), it must be demonstrated that such a limit always exists.

### Characterization 3

Since the integrand is an integrable function of *t*, the integral expression is well-defined. Now we must show that the function from to defined by

is a bijection. As is positive for positive *t*, this function is monotone increasing, hence one-to-one. If the two integrals

hold, then it is clearly onto as well. Indeed, these integrals *do* hold; they follow from the integral test and the divergence of the harmonic series.

## Equivalence of the characterizations

The following proof demonstrates the equivalence of the first three characterizations given for *e* above. The proof consists of two parts. First, the equivalence of characterizations 1 and 2 is established, and then the equivalence of characterizations 1 and 3 is established.

### Equivalence of characterizations 1 and 2

The following argument is adapted from a proof in Rudin, theorem 3.31, p. 63–65.

Let be a fixed non-negative real number. Define

By the binomial theorem,

(using *x* ≥ 0 to obtain the final inequality) so that

where *e*^{x} is in the sense of definition 2. Here, we must use limsups, because we don't yet know that *t*_{n} actually converges. Now, for the other direction, note that by the above expression of *t*_{n}, if 2 ≤ *m* ≤ *n*, we have

Fix *m*, and let *n* approach infinity. We get

(again, we must use liminf's because we don't yet know that *t*_{n} converges). Now, take the above inequality, let *m* approach infinity, and put it together with the other inequality. This becomes

so that

We can then extend this equivalence to the negative real numbers by noting and taking the limit as n goes to infinity.

The error term of this limit-expression is described by

where the polynomial's degree (in *x*) in the term with denominator *n*^{k} is 2*k*.

### Equivalence of characterizations 1 and 3

Here, we define the natural logarithm function in terms of a definite integral as above. By the first part of fundamental theorem of calculus,

Besides,

Now, let *x* be any fixed real number, and let

We will show that ln(*y*) = *x*, which implies that *y* = *e*^{x}, where *e*^{x} is in the sense of definition 3. We have

Here, we have used the continuity of ln(*y*), which follows from the continuity of 1/*t*:

Here, we have used the result ln*a*^{n} = *n*ln*a*. This result can be established for *n* a natural number by induction, or using integration by substitution. (The extension to real powers must wait until *ln* and *exp* have been established as inverses of each other, so that *a*^{b} can be defined for real *b* as *e*^{b lna}.)

### Equivalence of characterizations 2 and 4

Let n be a non-negative integer. In the sense of definition 4 and by induction, .

Therefore

Using Taylor series, This shows that definition 4 implies definition 2.

In the sense of definition 2,

Besides, This shows that definition 2 implies definition 4.

### Equivalence of characterizations 1 and 5

The following proof is a simplified version of the one in Hewitt and Stromberg, exercise 18.46. First, one proves that measurability (or here, Lebesgue-integrability) implies continuity for a non-zero function satisfying , and then one proves that continuity implies for some *k*, and finally implies *k*=1.

First, we prove a few elementary properties from satisfying and the assumption that is not identically zero:

- If is nonzero anywhere (say at
*x*=*y*), then it is non-zero everywhere. Proof: implies . - . Proof: and is non-zero.
- . Proof: .
- If is continuous anywhere (say at
*x*=*y*), then it is continuous everywhere. Proof: as by continuity at*y*.

The second and third properties mean that it is sufficient to prove for positive *x*.

If is a Lebesgue-integrable function, then we can define

It then follows that

Since is nonzero, we can choose some *y* such that and solve for in the above expression. Therefore:

The final expression must go to zero as since and is continuous. It follows that is continuous.

Now, we prove that , for some *k*, for all positive rational numbers *q*. Let *q*=*n*/*m* for positive integers *n* and *m*. Then

by elementary induction on *n*. Therefore, and thus

for . Note that if we are restricting ourselves to real-valued , then is everywhere positive and so *k* is real.

Finally, by continuity, since for all rational *x*, it must be true for all real *x* since the closure of the rationals is the reals (that is, we can write any real *x* as the limit of a sequence of rationals). If then *k* = 1. This is equivalent to characterization 1 (or 2, or 3), depending on which equivalent definition of e one uses.

### Characterization 6 implies characterization 4

In the sense of definition 6, By the way , therefore definition 6 implies definition 4.

## References

- Walter Rudin,
*Principles of Mathematical Analysis*, 3rd edition (McGraw–Hill, 1976), chapter 8. - Edwin Hewitt and Karl Stromberg,
*Real and Abstract Analysis*(Springer, 1965).