Under the assumed continuous real differentiability, the necessary and sufficient conditions are the Cauchy-Riemann equations at every point of :Necessity follows by computing the complex derivative along real and imaginary increments. For sufficiency, real differentiability gives the first-order expansionThe Cauchy-Riemann equations turn the linear part into , so the complex derivative exists and equals . Thus is a holomorphic function on .
At any , take sufficiently small so . The complex difference quotient isHence the complex derivative exists at every point of the punctured plane, andThe excluded point is essential to the domain statement: the reciprocal has a simple pole there.
Write . Both moduli are nonnegative, so squaring preserves their strict inequality:ThusThe boundary is the perpendicular bisector of and in the complex plane; the strict inequality selects the half-plane containing .
Use the reciprocal Möbius transformationIt is a holomorphic function on by part (b). For ,Part (c) now gives if and only if , so . Conversely, because . For any , put ; the same identity gives , so and . Finally, reciprocation is injective on nonzero complex numbers. This proves bijectivity, with inverseThe inverse is also holomorphic, so this is a biholomorphism.
For a piecewise continuously differentiable contour , the contour integral is defined byIf the contour has corners, integrate on its finitely many differentiable pieces and sum the results. The integral on the right is taken componentwise as an ordinary real-parameter integral of a complex-valued function. The factor encodes both the speed and orientation of the contour.
Choose the continuous argument with values in and defineIts branch cut is the nonpositive imaginary axis, including zero, exactly the removed ray. Locally away from that ray, the Cauchy-Riemann equations or the local inverse of the exponential show that it is a holomorphic logarithm, with derivative and . The chosen interval fixes the additive ambiguity by integer multiples of .
Use the branch from part (b) and close the real interval with the upper semicircle, oriented counterclockwise. For , the number has positive imaginary part, so the numerator is a holomorphic logarithm throughout a neighbourhood of the contour and its interior. The branch point lies strictly below the contour. The only enclosed pole ofis the simple pole at , with residueTo justify discarding the arc, take . On it, lies between and , and the argument has bounded absolute value. HenceThe real-axis integral is absolutely convergent, since its integrand is at infinity and has no real singularities. The residue theorem therefore givesFinally, . Taking twice the real part yieldsThe branch choice affects the first integral's imaginary part; the second integral is real and independent of that choice.
An isolated singularity at means that is holomorphic in some punctured disk , while itself is an excluded point or a point where the given function is not holomorphic. There are no other singularities arbitrarily close to . By Laurent's theorem, the function has a unique Laurent series on that punctured disk:The negative-power terms form its principal part of a Laurent series.
A removable singularity is an isolated singularity for which the function on the punctured disk extends to a holomorphic function on the full disk, by assigning or correcting its value at . In Laurent series terms,The remaining power series defines the extension with value at . Conversely, a holomorphic extension has a Taylor series there, so uniqueness of the Laurent series forces all negative coefficients to vanish.
A pole of order at has finitely many negative powers in its Laurent series, the lowest being exactly :Equivalently,Thus has a holomorphic extension with nonzero value at , whereas multiplying by any smaller power does not remove the singularity.
A zero of order at means that is holomorphic near andEquivalently its Taylor series starts with the nonzero coefficient of , soUnlike a pole, a zero is a regular point of the function itself; its reciprocal has a pole of the corresponding order.
By the finite-order zero factorizations,with holomorphic near . Shrinking the disk if necessary, continuity ensures never vanishes there, so is holomorphic and nonzero at . ConsequentlyIf , the exponent is , with a holomorphic nonvanishing factor. Hence
With the same factors, if , thenhas no negative power and extends holomorphically across . Thus its apparent singularity is a removable singularity, with extension valueFor the extended quotient has a zero of order ; for the extension is nonzero.
The complex sine has simple zeros exactly at , , because and . Hence the denominator has a zero of order three at each of these points and nowhere else.
At , the numerator has order two, so the quotient has a simple pole. Indeed its leading term is . At , the numerator has order one, so there is a pole of order two. At , the numerator has order three, cancelling the denominator's order-three zero, so the singularity is removable. Its extension value isAt every remaining , the numerator is nonzero, giving a pole of order three. Thus the complete finite-plane classification isAway from this discrete set the denominator is nonzero, so the quotient is holomorphic.
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