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Analytic Functions and Residues

A free GRE Mathematics note on the Cauchy-Riemann test for analyticity, Cauchy's theorem and integral formula, classifying singularities from a Laurent series, and evaluating contour integrals with residues.

Concise answer

Complex analysis on this exam is a short pipeline: check analyticity with the Cauchy-Riemann equations, locate the isolated singularities, keep only the ones inside the contour, compute each residue with the formula matching the pole order, and multiply the sum by 2πi2\pi i. Cauchy's theorem is the special case where nothing is enclosed and the integral is zero.

Definitions

Analytic (holomorphic)
Complex-differentiable at every point of an open set. Analytic functions are infinitely differentiable and equal to their Taylor series there.
Cauchy-Riemann equations
For f=u+ivf = u + iv, the conditions ux=vyu_x = v_y and uy=vxu_y = -v_x. They are necessary for analyticity, and sufficient when uu and vv have continuous partial derivatives.
Pole of order m
An isolated singularity at aa whose Laurent series has a lowest term (za)m(z-a)^{-m} with mm finite; m=1m = 1 is a simple pole.
Essential singularity
An isolated singularity whose Laurent series has infinitely many negative-power terms, as e1/ze^{1/z} has at z=0z = 0.
Residue
The coefficient of (za)1(z-a)^{-1} in the Laurent expansion of ff about aa; it is the only coefficient that survives integration around a small circle.
Entire function
A function analytic on the whole complex plane, such as eze^z, sinz\sin z, and every polynomial.

Intuition

The residue is the only Laurent coefficient with anywhere to go. Integrating (za)n(z-a)^{n} around a circle centred at aa gives zero for every integer nn except n=1n = -1, where the answer is 2πi2\pi i. So integrating a Laurent series term by term annihilates everything but one coefficient, and the residue theorem is that observation applied to each enclosed singularity at once.

Cauchy's theorem and the residue theorem are the same statement. If nothing singular is enclosed, the sum of residues is empty and the integral is zero; each enclosed singularity contributes exactly 2πi2\pi i times its residue. That is why the very first question about any contour integral is which singularities lie inside — not how to integrate.

Concept walkthrough

Analyticity is a strong condition: complex differentiability on an open set forces infinite differentiability and a convergent power series. The working test is the Cauchy-Riemann pair ux=vyu_x = v_y, uy=vxu_y = -v_x for f=u+ivf = u + iv. These are necessary for analyticity everywhere, and when uu and vv have continuous partials they are also sufficient. The standard non-example is f(z)=zˉ=xiyf(z) = \bar{z} = x - iy, where ux=1u_x = 1 but vy=1v_y = -1, so ff is nowhere analytic even though it is perfectly smooth as a map of R2\mathbb{R}^2.

Once analyticity is settled, integration becomes bookkeeping. Cauchy's theorem says a function analytic on and inside a simple closed contour integrates to zero around it. Cauchy's integral formula upgrades that to f(a)=12πiCf(z)zadzf(a) = \dfrac{1}{2\pi i}\oint_C \dfrac{f(z)}{z-a}\,dz, and the derivative version handles higher powers in the denominator: Cf(z)(za)n+1dz=2πin!f(n)(a)\oint_C \dfrac{f(z)}{(z-a)^{n+1}}\,dz = \dfrac{2\pi i}{n!} f^{(n)}(a). That 1/n!1/n! is the most commonly dropped factor in this whole topic.

For a general integrand, classify each isolated singularity from its Laurent series. A removable singularity has no negative powers, a pole of order mm has lowest term (za)m(z-a)^{-m}, and an essential singularity has infinitely many negative powers. At a simple pole, Resz=af=limza(za)f(z)\operatorname{Res}_{z=a} f = \lim_{z \to a}(z-a)f(z), and when f=p/qf = p/q with qq having a simple zero at aa and p(a)0p(a) \neq 0, this reduces to p(a)/q(a)p(a)/q'(a). At a pole of order mm, differentiate m1m-1 times: Resz=af=1(m1)!limzadm1dzm1[(za)mf(z)]\operatorname{Res}_{z=a} f = \dfrac{1}{(m-1)!}\lim_{z\to a}\dfrac{d^{m-1}}{dz^{m-1}}\left[(z-a)^m f(z)\right]. Sum the residues of the enclosed singularities only, then multiply by 2πi2\pi i.

After this page, you should be able to

  • Test a candidate function for analyticity with the Cauchy-Riemann equations and say why zˉ\bar{z} fails.
  • Decide when Cauchy's theorem alone forces a contour integral to vanish.
  • Classify an isolated singularity as removable, a pole of stated order, or essential.
  • Compute residues at simple poles and at poles of higher order with the correct formula.
  • Evaluate a closed contour integral by summing only the residues enclosed by the contour.

Formulas and assumptions

Cauchy-Riemann equations

ux=vy,uy=vx,f(z)=ux+ivxu_x = v_y, \qquad u_y = -v_x, \qquad f'(z) = u_x + i v_x

Variables

  • u: the real part of f as a function of x and y
  • v: the imaginary part of f

Assumptions

  • Necessary for analyticity; sufficient when u and v have continuous partial derivatives near the point.

Cauchy's integral formula for derivatives

Cf(z)(za)n+1dz=2πin!f(n)(a)\oint_{C} \frac{f(z)}{(z-a)^{n+1}}\,dz = \frac{2\pi i}{n!}\, f^{(n)}(a)

Variables

  • f: analytic on and inside the simple closed contour C
  • a: a point enclosed by C
  • n: a nonnegative integer

Assumptions

  • C is a simple closed contour traversed once counterclockwise and a lies inside it.
  • n = 0 recovers the ordinary Cauchy integral formula.

Residue at a pole of order m

Resz=af=1(m1)!limzadm1dzm1[(za)mf(z)]\operatorname*{Res}_{z=a} f = \frac{1}{(m-1)!}\lim_{z \to a} \frac{d^{\,m-1}}{dz^{\,m-1}}\left[(z-a)^{m} f(z)\right]

Variables

  • a: the location of the pole
  • m: the order of the pole

Assumptions

  • The singularity is a pole of finite order m, not essential.
  • For m = 1 this is the limit of (z - a) f(z).

Residue theorem

Cf(z)dz=2πikResz=akf\oint_{C} f(z)\,dz = 2\pi i \sum_{k} \operatorname*{Res}_{z=a_k} f

Variables

  • C: a simple closed contour traversed once counterclockwise
  • a_k: the isolated singularities of f enclosed by C

Assumptions

  • f is analytic on C and inside it except at the isolated singularities a_k.
  • Singularities outside C contribute nothing.

Worked example

A contour integral with two simple poles

Evaluate z=2z2+1z(z1)dz\displaystyle \oint_{|z| = 2} \frac{z^{2}+1}{z(z-1)}\,dz, where the circle is traversed once counterclockwise.

  1. 1The denominator vanishes at z=0z = 0 and z=1z = 1. Each is a simple zero, and the numerator is nonzero there (11 and 22 respectively), so both are simple poles.
  2. 2Both lie inside the contour: 0=0<2|0| = 0 < 2 and 1=1<2|1| = 1 < 2, so both residues count.
  3. 3Residue at z=0z = 0: limz0zz2+1z(z1)=z2+1z1z=0=11=1\displaystyle \lim_{z\to 0} z \cdot \frac{z^{2}+1}{z(z-1)} = \left.\frac{z^{2}+1}{z-1}\right|_{z=0} = \frac{1}{-1} = -1.
  4. 4Residue at z=1z = 1: limz1(z1)z2+1z(z1)=z2+1zz=1=21=2\displaystyle \lim_{z\to 1} (z-1)\cdot \frac{z^{2}+1}{z(z-1)} = \left.\frac{z^{2}+1}{z}\right|_{z=1} = \frac{2}{1} = 2.
  5. 5Apply the residue theorem: =2πi(1+2)=2πi\oint = 2\pi i\left(-1 + 2\right) = 2\pi i.

z=2z2+1z(z1)dz=2πi\displaystyle \oint_{|z|=2} \frac{z^{2}+1}{z(z-1)}\,dz = 2\pi i.

Common traps

  • Including residues at singularities that lie outside the contour, or missing one that lies inside — always compare ak|a_k| with the contour radius first.
  • Dropping the 1/n!1/n! in Cauchy's integral formula for derivatives, which scales the answer by a factor of n!n!.
  • Using the simple-pole limit lim(za)f(z)\lim (z-a)f(z) at a higher-order pole, where that limit is infinite and the order-mm formula is required.
  • Concluding a function is analytic because the Cauchy-Riemann equations hold at one point; analyticity requires them on a neighbourhood, with the partials continuous.
  • Assuming zˉ\bar{z}, z|z|, and Rez\operatorname{Re} z are analytic because they look smooth — none of them satisfies the Cauchy-Riemann equations.

Question depth and domain coverage vary by exam. Practice answers are checked after submission.

Sources

  1. GRE Subject Test Content and StructureETS. Accessed 2026-07-06. Use as a cited source for exam facts; do not imply affiliation or reproduce protected test material.
  2. Complex Variables with Applications (Orloff), Section 2.6: Cauchy-Riemann EquationsLibreTexts Mathematics. Accessed 2026-08-15. Orloff's Complex Variables with Applications on LibreTexts is CC BY-NC-SA 4.0; attribute the author and platform and avoid verbatim reuse beyond short cited references.
  3. Complex Variables with Applications (Orloff), Section 4.6: Cauchy's TheoremLibreTexts Mathematics. Accessed 2026-08-15. Orloff's Complex Variables with Applications on LibreTexts is CC BY-NC-SA 4.0; attribute the author and platform and avoid verbatim reuse beyond short cited references.
  4. Complex Variables with Applications (Orloff), Section 5.1: Cauchy's Integral for FunctionsLibreTexts Mathematics. Accessed 2026-08-15. Orloff's Complex Variables with Applications on LibreTexts is CC BY-NC-SA 4.0; attribute the author and platform and avoid verbatim reuse beyond short cited references.
  5. Complex Variables with Applications (Orloff), Section 5.2: Cauchy's Integral Formula for DerivativesLibreTexts Mathematics. Accessed 2026-08-15. Orloff's Complex Variables with Applications on LibreTexts is CC BY-NC-SA 4.0; attribute the author and platform and avoid verbatim reuse beyond short cited references.
  6. Complex Variables with Applications (Orloff), Section 8.7: Laurent SeriesLibreTexts Mathematics. Accessed 2026-08-15. Orloff's Complex Variables with Applications on LibreTexts is CC BY-NC-SA 4.0; attribute the author and platform and avoid verbatim reuse beyond short cited references.
  7. Complex Variables with Applications (Orloff), Section 9.4: ResiduesLibreTexts Mathematics. Accessed 2026-08-15. Orloff's Complex Variables with Applications on LibreTexts is CC BY-NC-SA 4.0; attribute the author and platform and avoid verbatim reuse beyond short cited references.
  8. Complex Variables with Applications (Orloff), Section 9.5: Cauchy Residue TheoremLibreTexts Mathematics. Accessed 2026-08-15. Orloff's Complex Variables with Applications on LibreTexts is CC BY-NC-SA 4.0; attribute the author and platform and avoid verbatim reuse beyond short cited references.

Sources and corrections

Sources last checked 2026-08-15

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