For , the complex logarithm has the values for .
A logarithmic singularity behaves locally like with , on a chosen branch. Although unbounded at the endpoint, it is integrable along a finite ray. In a rapidly oscillating endpoint integral its contour rotation produces a logarithm of the large parameter and a branch-angle contribution; this differs from the ordinary smooth-amplitude Watson lemma.
A branch of the complex logarithm chooses the argument continuously on a domain avoiding an appropriate branch cut, making the logarithm single-valued there.
The principal complex logarithm is with .
If is an analytic branch of the logarithm on a connected domain avoiding zero, then is an analytic branch of the square root. Any two such branches differ everywhere by one constant sign.
For with , the principal square root is . Its standard analytic domain removes the nonpositive real axis.
For nonzero complex and complex , the multivalued power is
The principal cube root is using the principal complex logarithm. In the right half-plane, its complex argument lies between and . Consequently the roots of consist of one root with negative real part, , and two with positive real part, .
For every integer and real ,
It converts powers of a complex number in polar form into multiplication of its complex argument.
On , choose the argument in . Then
is an analytic logarithm. Locally this follows by scaling the convergent series
For ,
with value one at by continuity. A keyhole contour around the positive axis gives a jump factor , while the double pole at has residue .

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