Limits

lim⁡z→z0f(z)=L\lim_{z\to z_0} f(z) = L iff:

∀ϵ>0  ∃δ>0  ∀z  (0<∣z−z0∣<δ  ⟹  ∣f(z)−L∣<ϵ)\forall{\epsilon>0}\; \exists{\delta>0}\; \forall{z}\; \big(0<|z-z_0|<\delta\implies{|f(z)-L|<\epsilon})

Properties

All properties mentioned in Limits | Real Analysis are applicable to complex limits. Additional properties are mentioned below:

Suppose lim⁡f(z)=L\lim f(z)=L.

  • lim⁡f(z)‾=L‾\lim \overline{f(z)}=\overline{L}
  • lim⁡Re(f(z))=Re(L)\lim \text{Re}(f(z))=\text{Re}(L)
  • lim⁡Im(f(z))=Im(L)\lim \text{Im}(f(z))=\text{Im}(L)

Real and Imaginary Limits

Let f(z)=u(x,y)+iv(x,y)f(z)=u(x,y)+iv(x,y), z0=x0+iy0z_0 = x_0 + iy_0, z=x+iyz=x+iy.

Suppose the real part and imaginary part limits to L1,L2L_1,L_2, which can be written as:

lim⁡(x,y)→(x0,y0)u(x,y)=L1      lim⁡(x,y)→(x0,y0)v(x,y)=L2\lim_{(x,y)\to(x_0,y_0)} u(x,y)=L_1 \;\;\; \lim_{(x,y)\to(x_0,y_0)} v(x,y)=L_2

Then:

lim⁡z→z0f(z)=L1+iL2\lim_{z\to z_0} f(z)=L_1+iL_2

Difference from Real Functions

For real functions, when considering the limit at a point, the limit could be be approaching the point either from left or right.

For complex functions, the point can be approached along any path in the complex plane. The distance ∣z−z0∣\lvert z - z_0 \rvert decreases to 00.

Notes for Questions

  • When 2 arbitrary paths are chosen: if the limits on each are different, then the limit DNE.
  • When substituting z=x+imxz=x+imx, if mm doesn’t cancel out, then the limit DNE.
  • In most limits, subtituting z=reiθz=re^{i\theta} will simplify the limit a lot.
  • In very complex functions, limits can be taken for real and imaginary parts separately.

Important Limits

lim⁡z→0zz‾  doesn’t exist\lim_{z\to 0} \frac{z}{\overline{z}}\;\text{doesn't exist}

The above limit is important as it shows up in many questions. Can be disproved by taking two paths: real, imaginary axes.

lim⁡z→0zz‾z+z‾  doesn’t exist\lim_{z\to 0} \frac{z \overline{z}}{z+\overline{z}}\;\text{doesn't exist}

Can be proven usign taking 2 paths: real axis, t+tit+\sqrt{t}i.

Written by October 17, 2026 1 min read
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