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  • Calculus
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  • Classical Mechanics
  • First Quantization
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  • Special Relativity
  • Relativistic QM
  • Dirac Equation
  • Fields and Quanta
  • Action and Lagrangians
  • Field Quantization
  • Quantum Electrodynamics
  • From Lagrangian to Experiment
  • Perturbation Theory
  • Feynman Rules for QED
  • Symmetries
  • Weak Interaction
  • Electroweak Unification
  • Higgs Mechanism
  • Quantum Chromodynamics
  • The Standard Model
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    • Path Integrals in Quantum Mechanics
    • Path Integrals for Fields
    • Fermionic Path Integrals
    • Gauge Fixing
    • Renormalization at One Loop
  • Exercises
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  • Math Refresher

    • Calculus
    • Complex Numbers
    • Linear Algebra
    • Index Notation and Tensors
    • Groups and Symmetry

Math Refresher: Complex Numbers

Quantum amplitudes carry a phase, an angle that affects how amplitudes combine. Complex numbers are the language for that angle. This page defines them and the one formula the rest of the site relies on most: Euler's formula.

1. Complex numbers

A complex number pairs two real numbers,

z=a+ib,

where i2=−1. The number a is the real part and b the imaginary part. We add and multiply by the usual rules, treating i as an object whose square is −1.

The complex conjugate flips the sign of the imaginary part, z∗=a−ib. Multiplying a number by its conjugate gives a nonnegative real number:

∣z∣2=z∗z=(a−ib)(a+ib)=a2+b2.

We call ∣z∣ the magnitude of z. In quantum mechanics, a probability density is built this way: ∣ψ∣2=ψ∗ψ on First Quantization.

2. The complex plane and Euler's formula

Plot a horizontally and b vertically. Then z=a+ib is a point in a plane, and ∣z∣ is its distance from the origin. The direction of that point from the origin is its phase, an angle θ.

A point at distance 1 from the origin sits on the unit circle. The coordinates of such a point are (cosθ,sinθ), so

eiθ=cosθ+isinθ.

This is Euler's formula. It connects the angle θ to the exponential eiθ, and it is the single most-used identity on this site. In particular eiπ=−1 and eiπ/2=i.

Because cos2θ+sin2θ=1, every number eiθ has magnitude exactly 1. A complex number of general magnitude r and phase θ is reiθ.

A point at angle θ on the unit circle has coordinates (cos θ, sin θ), so it is written as the phase e^{iθ}.

A point at angle θ on the unit circle has coordinates (cos θ, sin θ), so it is written as the phase e^{iθ}.

3. Multiplying adds phases

Multiplying two numbers multiplies their magnitudes and adds their phases:

(r1​eiθ1​)(r2​eiθ2​)=(r1​r2​)ei(θ1​+θ2​).

This follows from Euler's formula and the usual addition rules for sine and cosine. Two consequences matter throughout the site:

  • Multiplying by eiα rotates a point by the angle α without changing its magnitude. This is the phase rotation used for the U(1) symmetry of QED.
  • Adding two complex numbers of similar phase reinforces them, while adding numbers of opposite phase cancels them. This is the interference between amplitudes.

The conjugate of eiθ is e−iθ, the same rotation in the opposite direction.

4. Waves and the Fourier transform

A plane wave writes an oscillation as a complex exponential,

ei(p⋅x−Et)/ℏ=cos(ℏp⋅x−Et​)+isin(ℏp⋅x−Et​).

The real part is a cosine wave; the complex form is easier to differentiate because the derivative of eiθ is ieiθ. This wave appears first on Relativistic QM and drives every field expansion afterward.

A general function can be written as a sum (or integral) of such waves with different momenta. Reconstructing the function from its momentum components is the Fourier transform. It is the step that connects the position and momentum representations in First Quantization and that decomposes a field into momentum modes in Field Quantization. Roughly: a sharply localized position wave is a broad sum of momentum waves, and vice versa, which is the mathematical content of the uncertainty relation.

5. Conjugation and the adjoint

In quantum mechanics, complex conjugation of a number becomes the adjoint (†) of an operator. Replacing each amplitude a(p) by its conjugate a∗(p) is the step that, after quantization, becomes a(p)→a†(p) on Field Quantization. The two operations play the same bookkeeping role: they reverse the sign of every phase and swap creation with annihilation.


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Last Updated: 10/8/26, 1:30 AM
Contributors: Hanh Huynh Huu
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