The hyperbolic sine satisfies . The complex exponential function is entire, and sums and compositions of entire functions are entire. Therefore
The zeros of the hyperbolic sine are exactly , , since is equivalent to . Each zero is simple because . The quotient is therefore holomorphic precisely onAt zero, the Taylor expansion gives , so zero is a simple pole. At , the denominator has a double zero and the numerator is nonzero, giving a pole of order two. Thus none of the omitted points admits a holomorphic extension.
The denominator vanishes exactly when , namely at , . Its derivative there is , so each such zero is simple and the numerator does not cancel it. Henceand every omitted point is a simple pole.
Let . More generally, for a holomorphic function , the increment expansion at givesAlong real increments the first factor is , while along purely imaginary increments it is . Thus complex differentiability of requires . Conversely, if , the displayed expression tends to zero for arbitrary complex increments, so the complex derivative exists and equals zero.
For , this condition is , equivalent to . ConsequentlyThese points form a discrete subset of the complex plane and contain no nonempty open set. Every neighbourhood of each one contains points where is not complex differentiable. Therefore is holomorphic on no nonempty open set, even though it has complex derivatives at the specified points.
The identity theorem states that if two holomorphic functions on a connected open set agree at a sequence of distinct points with an accumulation point inside that set, then they agree everywhere on it. Equivalently, the zeros of a holomorphic function which is not identically zero cannot accumulate inside its domain.
Because never vanish, their logarithmic derivatives are holomorphic. The holomorphic functionvanishes at every . Since the distinct converge to , the identity theorem gives . Applying the quotient rule now givesA holomorphic function with zero derivative on a domain is constant. One can see this locally from its Taylor series, then propagate the constant using connectedness. Hence on , with , andThe conclusion can fail if the accumulation occurs outside . Take the punctured complex plane andBoth functions are nowhere vanishing and holomorphic on , and . The chain rule givesso these logarithmic derivatives agree at every . However, is not constant: for example and . Therefore no constant gives .
On the slit domain , choose the complex argument . The resulting holomorphic logarithm is , with . DefineIt is holomorphic as a composition of holomorphic functions, and . At the chosen argument is , so .
Suppose a holomorphic square root existed on the whole punctured complex plane. It would be nonzero, and differentiating would give . There are several ways to express the resulting obstruction; a direct one uses the unit circle. SetThe chain rule and imply , so is constant. ButThese cannot agree because . Thus no such global holomorphic square root exists. Going once around zero changes the sign of the locally chosen root.
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