4.11 Sums4.13 Lambert \mathop{W\/}\nolimits-Function

§4.12 Generalized Logarithms and Exponentials

A generalized exponential function \phi(x) satisfies the equations

and is strictly increasing when 0\leq x\leq 1. Its inverse \psi(x) is called a generalized logarithm. It, too, is strictly increasing when 0\leq x\leq 1, and

These functions are not unique. The simplest choice is given by

4.12.5 \phi(x)=\psi(x)=x, 0\leq x\leq 1.

Then

4.12.6 \phi(x)=\mathop{\ln\/}\nolimits\!\left(x+1\right), -1<x<0,

and

4.12.7 \phi(x)=\mathop{\exp\/}\nolimits\mathop{\exp\/}\nolimits\cdots\mathop{\exp\/}\nolimits\!\left(x-\left\lfloor x\right\rfloor\right), x>1,

where the exponentiations are carried out \left\lfloor x\right\rfloor times. Correspondingly,

4.12.8 \psi(x)=e^{x}-1, -\infty<x<0,

and

4.12.9 \psi(x)=\ell+{\mathop{\ln\/}\nolimits^{{(\ell)}}}x, x>1,

where {\mathop{\ln\/}\nolimits^{{(\ell)}}}x denotes the \ell-th repeated logarithm of x, and \ell is the positive integer determined by the condition

4.12.10 0\leq{\mathop{\ln\/}\nolimits^{{(\ell)}}}x<1.

Both \phi(x) and \psi(x) are continuously differentiable.

For further information, see Clenshaw et al. (1986). For \mathop{C^{{\infty}}\/}\nolimits generalized logarithms, see Walker (1991). For analytic generalized logarithms, see Kneser (1950).