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Oakfield Operator Calculus Function Reference Site

Complex Exponential

For a real phase variable θ\theta, the complex exponential is

eiθ=cosθ+isinθe^{i\theta} = \cos \theta + i \sin \theta

For θR\theta \in \mathbb{R}, eiθe^{i\theta} lies on the complex unit circle {zC:z=1}\{z\in\mathbb{C}:|z|=1\}. The map extends to complex arguments θC\theta\in\mathbb{C} as an entire function.


Unit Magnitude and Periodicity (Real Phase)

Section titled “Unit Magnitude and Periodicity (Real Phase)”
eiθ=1,ei(θ+2πk)=eiθ(kZ)|e^{i\theta}| = 1, \qquad e^{i(\theta + 2\pi k)} = e^{i\theta}\quad (k\in\mathbb{Z})
eiθ=eiθ\overline{e^{i\theta}} = e^{-i\theta}
ei(θ1+θ2)=eiθ1eiθ2e^{i(\theta_1+\theta_2)} = e^{i\theta_1}e^{i\theta_2}

θ\thetaeiθe^{i\theta}
0011
π\pi1-1
π2\tfrac{\pi}{2}ii

For small θ|\theta|, a first-order expansion is eiθ1+iθe^{i\theta}\approx 1+i\theta.


Real and imaginary parts yield cosine and sine. Fourier series and Fourier transforms use eikxe^{ikx} as basis elements, and standing waves and phase-shifted sinusoids arise from linear combinations of complex exponentials.


Oakfield uses complex exponentials extensively in spectral and modulation-style code paths:

  • Spectral phase factors: the dispersion operator multiplies FFT bins by cexp(I * phase) to apply dispersive phase advance.
  • Mixer modulation modes: FM/PM modes apply eiθe^{i\theta}-style multipliers to complex fields.
  • Stimulus rotations: several complex-capable stimuli apply an additional unit-magnitude complex rotation when writing outputs.

Euler’s identity connecting exponentials and trigonometric functions provides the analytic bridge between additive phase and multiplicative complex rotation.

The complex exponential is the canonical representation of phase and oscillation in spectral methods, wave physics, and signal processing.


  • NIST Digital Library of Mathematical Functions (DLMF), §4
  • Stein & Shakarchi, Fourier Analysis