Photonica

Polarization states

The orientation and rotation behavior of the electric-field vector of a light wave. Linear, circular, elliptical, and unpolarized states form the standard classification with specific applications across optics and telecom.

The polarization state of light describes how the electric-field vector orients and evolves over time at a fixed point in space. Light has two transverse degrees of freedom (perpendicular to the propagation direction); the polarization state describes the relationship between them.

Categories of polarization.

Linear polarization. The electric field oscillates along a single direction in the transverse plane:

E(t)  =  E0e^θcos(ωt),\mathbf{E}(t) \;=\; E_0 \, \hat{\mathbf{e}}_\theta \cos(\omega t),

where e^θ\hat{\mathbf{e}}_\theta is the polarization axis. The two extreme cases — horizontal and vertical — are the standard basis for linear polarization. Diagonal polarization at 45° is a superposition of equal-amplitude horizontal and vertical components in phase.

Circular polarization. The electric field rotates at the optical frequency, maintaining constant magnitude:

E(t)  =  E0[x^cos(ωt)±y^sin(ωt)].\mathbf{E}(t) \;=\; E_0 [\hat{\mathbf{x}} \cos(\omega t) \pm \hat{\mathbf{y}} \sin(\omega t)].

The two signs correspond to right- and left-circular polarization (sense of rotation depends on convention). Circular polarization is a superposition of equal-amplitude horizontal and vertical components 90° out of phase.

Elliptical polarization. The general case: the electric-field vector traces out an ellipse in the transverse plane. Linear and circular polarization are limiting cases of elliptical (degenerate ellipse → line; circular = special equal-amplitude case).

Unpolarized light. The electric-field orientation is random and changes faster than any practical measurement timescale. Sunlight and thermal incandescent light are unpolarized. Mathematically: equal probability density on every linear polarization direction (and zero net circular component).

Partially polarized light. Most practical sources have polarization that is partially defined: some fraction of the power has a specific polarization (called the polarized component), and the rest is unpolarized. The Stokes parameters provide the natural description of partially-polarized light.

Decomposition and synthesis.

PolarizationDecomposition (horiz/vert basis)
H linear100% H
V linear100% V
+45° linear50% H + 50% V, in phase
45°-45° linear50% H + 50% V, 180° out of phase
Right-circular50% H + 50% V, V leads H by 90°
Left-circular50% H + 50% V, H leads V by 90°
1:2 elliptical at 30°Mix of H and V with specific phase and amplitude

Polarization manipulation elements.

ElementFunction
Linear polarizerTransmits only one linear polarization; absorbs/reflects the other
Circular polarizerTransmits only one circular polarization
Quarter-wave plateConverts linear ↔ circular polarization
Half-wave plateRotates linear polarization by twice the plate angle
Faraday rotatorMagnetic-field-induced rotation; non-reciprocal
Optical activity (sugar solutions, quartz)Reciprocal rotation; reverses with direction
Polarization scramblerTime-varying polarization conversion; randomizes
Polarization beam splitter (PBS)Transmits one linear polarization, reflects orthogonal

Generation of standard polarization states.

  • Linear polarization: from a linear polarizer (Glan-Thompson, sheet polarizer, wire-grid) or from sources with intrinsic polarization (most lasers)
  • Circular polarization: linear polarizer + quarter-wave plate oriented at 45° to its axis
  • Elliptical polarization: linear polarizer + arbitrary-angle quarter-wave plate
  • Unpolarized: incandescent lamp, scrambled laser, sunlight after reflection from many surfaces

Polarization in light-matter interactions.

  • Optical absorption: many molecules have polarization-dependent absorption (selection rules); the orientation of polarized light determines absorbed power
  • Optical rotation in chiral media: glucose solutions and quartz crystals rotate linear polarization
  • Birefringence: anisotropic media have refractive index that depends on polarization
  • Polarization in scattering: Rayleigh scattering polarizes scattered light at 90° to incident direction; useful for atmospheric studies

Polarization in telecom and photonics.

  • Polarization-division multiplexing (PDM): in coherent optical transmission, two independent data streams travel on the two orthogonal polarization states of a single wavelength. Demultiplexed in the coherent receiver via DSP.
  • Polarization-mode dispersion (PMD): in single-mode fiber, the two polarization states travel slightly differently — a noise source in long-distance transmission
  • Polarization-maintaining fiber: specially-designed birefringent fiber maintains a defined linear polarization through propagation
  • Polarization-dependent loss (PDL): real components attenuate the two polarizations differently; an impairment in transmission

Standard measurement.

A polarization-state analyzer (PSA) or Stokes polarimeter measures the polarization state. Modern instruments (Thorlabs PAX series, Schäfter+Kirchhoff PolaScope) provide:

  • Stokes parameters (4 measurements)
  • Degree of polarization (DOP)
  • Ellipticity and azimuth angles
  • Real-time Poincaré sphere visualization

Typical accuracy: <1°< 1° azimuth, <0.5°< 0.5° ellipticity, <1%< 1\% DOP.

Polarization at boundaries. Reflection and transmission at interfaces are polarization-dependent:

  • s-polarization (TE): electric field perpendicular to plane of incidence
  • p-polarization (TM): electric field in plane of incidence
  • Brewster's angle: p-polarization fully transmits, s-polarization partially reflects
  • Fresnel coefficients: rs,rp,ts,tpr_s, r_p, t_s, t_p describe these polarization-dependent quantities

This polarization-dependent reflection underlies polarization-sensitive optics: PBS cubes, polarizing thin-film coatings, Brewster-angle windows.

Quantum polarization. The polarization state of a single photon is the quantum-mechanical analog of classical polarization. The state space is the 2D complex Hilbert space (the "qubit"). Bell-state pairs of polarization-entangled photons are central to quantum information experiments.

References: Saleh & Teich, Fundamentals of Photonics (3rd ed., 2019), Ch. 6 (polarization optics); Born & Wolf, Principles of Optics (7th ed., 1999), Ch. 1 for the canonical treatment; Goldstein, Polarized Light (3rd ed., 2010) for comprehensive engineering reference.