A triangular prism dispersing a beam of white light. The longer wavelengths (red) and the shorter wavelengths (blue) are separated.
Circular polarization on rubber thread, converted to linear polarization
A ray of light being refracted in a plastic block
The electromagnetic spectrum, with the visible portion highlighted
cross linear polarized
Refraction of a light ray
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A "vertically polarized" electromagnetic wave of wavelength λ has its electric field vector E (red) oscillating in the vertical direction. The magnetic field B (or H) is always at right angles to it (blue), and both are perpendicular to the direction of propagation (z).
Thomas Young coined the term index of refraction.
Beam of sun light inside the cavity of Rocca ill'Abissu at Fondachelli-Fantina, Sicily
Electric field oscillation
Diamonds have a very high refractive index of 2.417.
Due to refraction, the straw dipped in water appears bent and the ruler scale compressed when viewed from a shallow angle.
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A split-ring resonator array arranged to produce a negative index of refraction for microwaves
Hong Kong illuminated by colourful artificial lighting.
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In optical mineralogy, thin sections are used to study rocks. The method is based on the distinct refractive indices of different minerals.
Pierre Gassendi.
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Light of different colors has slightly different refractive indices in water and therefore shows up at different positions in the rainbow.
Christiaan Huygens.
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In a prism, dispersion causes different colors to refract at different angles, splitting white light into a rainbow of colors.
Thomas Young's sketch of a double-slit experiment showing diffraction. Young's experiments supported the theory that light consists of waves.
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The variation of refractive index with wavelength for various glasses. The shaded zone indicates the range of visible light.
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Animation showing four different polarization states and three orthogonal projections.
The colors of a soap bubble are determined by the optical path length through the thin soap film in a phenomenon called thin-film interference.
A circularly polarized wave as a sum of two linearly polarized components 90° out of phase
Refraction of light at the interface between two media of different refractive indices, with n2 > n1. Since the phase velocity is lower in the second medium (v2 < v1), the angle of refraction θ2 is less than the angle of incidence θ1; that is, the ray in the higher-index medium is closer to the normal.
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Total internal reflection can be seen at the air-water boundary.
Color pattern of a plastic box showing stress-induced birefringence when placed in between two crossed polarizers.
The power of a magnifying glass is determined by the shape and refractive index of the lens.
Paths taken by vectors in the Poincaré sphere under birefringence. The propagation modes (rotation axes) are shown with red, blue, and yellow lines, the initial vectors by thick black lines, and the paths they take by colored ellipses (which represent circles in three dimensions).
The relation between the refractive index and the density of silicate and borosilicate glasses
A stack of plates at Brewster's angle to a beam reflects off a fraction of the s-polarized light at each surface, leaving (after many such plates) a mainly p-polarized beam.
A calcite crystal laid upon a paper with some letters showing double refraction
Stress in plastic glasses
Birefringent materials can give rise to colors when placed between crossed polarizers. This is the basis for photoelasticity.
Photomicrograph of a volcanic sand grain; upper picture is plane-polarized light, bottom picture is cross-polarized light, scale box at left-center is 0.25 millimeter.
A gradient-index lens with a parabolic variation of refractive index (n) with radial distance (x). The lens focuses light in the same way as a conventional lens.
Effect of a polarizer on reflection from mud flats. In the picture on the left, the horizontally oriented polarizer preferentially transmits those reflections; rotating the polarizer by 90° (right) as one would view using polarized sunglasses blocks almost all specularly reflected sunlight.
The principle of many refractometers
One can test whether sunglasses are polarized by looking through two pairs, with one perpendicular to the other. If both are polarized, all light will be blocked.
A handheld refractometer used to measure the sugar content of fruits
The effects of a polarizing filter (right image) on the sky in a photograph
A differential interference contrast microscopy image of yeast cells
Colored fringes in the Embassy Gardens Sky Pool when viewed through a polarizer, due to stress-induced birefringence in the skylight
Circular polarization through an airplane plastic window, 1989

In optics, the refractive index ( refraction index) of an optical medium is a dimensionless number that gives the indication of the light bending ability of that medium.

- Refractive index

The primary properties of light are intensity, propagation direction, frequency or wavelength spectrum and polarization.

- Light

Transverse waves that exhibit polarization include electromagnetic waves such as light and radio waves, gravitational waves, and transverse sound waves (shear waves) in solids.

- Polarization (waves)

Even in isotropic media, so-called inhomogeneous waves can be launched into a medium whose refractive index has a significant imaginary part (or "extinction coefficient") such as metals; these fields are also not strictly transverse.

- Polarization (waves)

where θ1 is the angle between the ray and the surface normal in the first medium, θ2 is the angle between the ray and the surface normal in the second medium and n1 and n2 are the indices of refraction, n = 1 in a vacuum and n > 1 in a transparent substance.

- Light

In some materials, the refractive index depends on the polarization and propagation direction of the light.

- Refractive index
A triangular prism dispersing a beam of white light. The longer wavelengths (red) and the shorter wavelengths (blue) are separated.

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The Lorentz factor γ as a function of velocity. It starts at1 and approaches infinity as v approaches c.

Speed of light

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Universal physical constant that is important in many areas of physics.

Universal physical constant that is important in many areas of physics.

The Lorentz factor γ as a function of velocity. It starts at1 and approaches infinity as v approaches c.
Event A precedes B in the red frame, is simultaneous with B in the green frame, and follows B in the blue frame.
The blue dot moves at the speed of the ripples, the phase velocity; the green dot moves with the speed of the envelope, the group velocity; and the red dot moves with the speed of the foremost part of the pulse, the front velocity.
A beam of light is depicted travelling between the Earth and the Moon in the time it takes a light pulse to move between them: 1.255 seconds at their mean orbital (surface-to-surface) distance. The relative sizes and separation of the Earth–Moon system are shown to scale.
Measurement of the speed of light using the eclipse of Io by Jupiter
Aberration of light: light from a distant source appears to be from a different location for a moving telescope due to the finite speed of light.
One of the last and most accurate time of flight measurements, Michelson, Pease and Pearson's 1930–35 experiment used a rotating mirror and a one-mile (1.6 km) long vacuum chamber which the light beam traversed 10 times. It achieved accuracy of ±11 km/s.
Diagram of the Fizeau apparatus
Electromagnetic standing waves in a cavity
An interferometric determination of length. Left: constructive interference; Right: destructive interference.
Rømer's observations of the occultations of Io from Earth
Hendrik Lorentz (right) with Albert Einstein

All forms of electromagnetic radiation, including visible light, travel at the speed of light.

The speed at which light propagates through transparent materials, such as glass or air, is less than c; similarly, the speed of electromagnetic waves in wire cables is slower than c. The ratio between c and the speed v at which light travels in a material is called the refractive index n of the material (

The refractive index of a material may depend on the light's frequency, intensity, polarization, or direction of propagation; in many cases, though, it can be treated as a material-dependent constant.