constant

imaginary unit

imaginary unit — from formula anatomy
Value
\(i = 1\)
11 related articles · 4 formulas

Description

The imaginary unit, denoted i, is defined by the property i² = −1. It extends the real number system to the complex numbers, allowing every polynomial equation to have solutions. In physics, the imaginary unit is not just a mathematical convenience but a fundamental ingredient in the equations of quantum mechanics, where wave functions are complex-valued, and in the description of oscillations and waves across all branches of physics.

History

The imaginary unit was first introduced by Gerolamo Cardano in the 16th century for solving cubic equations, and later formalized by Rafael Bombelli. Its geometric interpretation as rotation came from Caspar Wessel and Jean-Robert Argand in the late 18th century.

How it works

Complex numbers are written as a + bi, where a and b are real numbers. The imaginary unit enables compact representation of rotations and periodic phenomena: Euler's formula e^{iθ} = cos θ + i sin θ links exponentials to trigonometry. In quantum mechanics, the time evolution of a state is governed by the Schrödinger equation iħ ∂ψ/∂t = Hψ, where the factor i ensures that probabilities remain conserved and the evolution is unitary.

In practice

The imaginary unit is used in alternating current circuit analysis, signal processing (Fourier transforms), and quantum computing, where qubit states are represented as complex vectors.

Fun fact

The imaginary unit is the only number whose reciprocal equals its negative: 1/i = −i, a property that follows directly from i² = −1.

Concept graph →

Formulas

$$\frac{d\rho}{dt} = -\frac{i}{\hbar}[H,\rho] + \sum_n \left( L_n \rho L_n^\dagger - \frac{1}{2} \{ L_n^\dagger L_n, \rho \} \right)$$
Describes open quantum system evolution with dissipation.
What is in the formula
ρvariabledensity matrix of the open quantum system — density matrix
tvariabletime — time second
HvariableHamiltonian of the system — hamiltonian joule
L_nvariableLindblad operators (jump operators) for each dissipation channel — lindblad operator
iconstantimaginary unit, square root of -1 — imaginary unit = 1
ħconstantPlanck constant divided by 2π — reduced planck constant = 1.054571817e-34 joule second
d/dtoperatorderivative with respect to time — time derivative
[H, ρ]operatorcommutator of H and ρ — commutator
{L_n† L_n, ρ}operatoranticommutator of L_n† L_n and ρ — anticommutator
∑_noperatorsum over all dissipation channels — sum over channels
$$i\\hbar\\partial_t\\Psi = \\left(-i\\hbar c \\vec{\\alpha}\\cdot\\vec{\\nabla} + \\beta m c^2\\right)\\Psi$$
Relativistic quantum wave equation for spin-1/2 particles.
What is in the formula
ΨvariableSpinor wave function — wave function
tvariableTime — time second
iconstantSquare root of -1 — imaginary unit = 1
ħconstantFundamental quantum of action — reduced planck constant = 1.054571817e-34 joule second
cconstantUniversal speed limit — speed of light = 299792458 metre per second
mconstantIntrinsic mass of the particle — mass = variable kilogram
∂_toperatorDifferentiates the wave function with respect to time — partial derivative
∇operatorSpatial derivative vector — nabla operator
$$\mathbf{A} = \frac{\Delta}{\sqrt{2}} (\mathbf{e}_x + i \mathbf{e}_y)$$
Normalized vector representing right-hand circular polarization.
What is in the formula
AvariablePolarization vector — polarization vector
ΔvariableAmplitude of the field — amplitude volt per metre
e_xvariableUnit vector along x-axis — unit vector
e_yvariableUnit vector along y-axis — unit vector
ioperatorComplex number with square -1 — imaginary unit
$$z(t) = x(t) + i\mathcal{H}[x(t)] = a(t)e^{i\phi(t)}$$
Represents a signal with instantaneous amplitude and phase.
What is in the formula
zvariableAnalytic signal — analytic signal
xvariableReal signal — signal
avariableInstantaneous amplitude — instantaneous amplitude
φvariableInstantaneous phase — instantaneous phase radian
tvariableTime variable — time second
HoperatorHilbert transform, shifts phase by -90° — hilbert transform operator
ioperatorImaginary unit, √(-1) — imaginary unit

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