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Refractive Index

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The '''refractive index''' (or '''index of refraction''') of a material is the factor by which the phase velocity of electromagnetic radiation is slowed in that material, relative to Speed of light its velocity in a vacuum. It is usually given the symbol ''n'', and defined for a material by: :

n=\sqrt{\epsilon_r\mu_r}

where ''ε_r'' is the material's relative permittivity, and ''μ_r'' is its relative Permeability_(electromagnetism) permeability. For a non-magnetic material, ''μ_r'' is very close to 1, therefore ''n'' is approximately

\sqrt{\epsilon_r}

. The phase velocity is defined as the rate at which the crests of the waveform propagate; that is, the rate at which the phase (waves) phase of the waveform is moving. The ''group velocity'' is the rate that the ''envelope'' of the waveform is propagating; that is, the rate of variation of the amplitude of the waveform. It is the group velocity that (almost always) represents the rate that information (and energy) may be transmitted by the wave, for example the velocity at which a pulse of light travels down an optical fiber.

The speed of light
The speed of all electromagnetic radiation in vacuum is the same, approximately 3×10⁸ meters per second, and is denoted by speed of light ''c''. Therefore, if ''v'' is the phase velocity of radiation of a specific frequency in a specific material, the refractive index is given by :

n =\frac{c}{v}

This number is typically greater than one: the higher the index of the material, the more the light is slowed down. However, at certain frequencies (e.g. near absorption resonances, and for x-rays), ''n'' will actually be smaller than one. This does not contradict the theory of relativity, which holds that no information-carrying signal can ever propagate faster than ''c'', because the phase velocity is not the same as the group velocity or the signal velocity. Sometimes, a "group velocity refractive index", usually called the ''group index'' is defined: :

n_g=\frac{c}{v_g}

where ''v_g'' is the group velocity. This value should not be confused with ''n'', which is always defined with respect to the phase velocity. At the microscale, an electromagnetic wave's phase velocity is slowed in a material because the electric field creates a disturbance in the charges of each atom (primarily the electrons) proportional to the permittivity. The charges will, in general, oscillate slightly out of phase with respect to the driving electric field. The charges thus radiate their own electromagnetic wave that is at the same frequency but with a phase delay. The macroscopic sum of all such contributions in the material is a wave with the same frequency but shorter wavelength than the original, leading to a slowing of the wave's phase velocity. Most of the radiation from oscillating material charges will modify the incoming wave, changing its velocity. However, some net energy will be radiated in other directions (see scattering). If the refractive indices of two materials are known for a given frequency, then one can compute the angle by which radiation of that frequency will be refraction refracted as it moves from the first into the second material from Snell's law. Recent research has also demonstrated the existence of negative refractive index which can occur if ''ε'' and ''μ'' are ''simultaneously'' negative. Not thought to occur naturally, this can be achieved with so called metamaterials and offers the possibility of perfect lenses and other exotic phenomena such as a reversal of Snell's law.

Dispersion and Absorption
In real materials, the polarization (electrostatics) polarization does not respond instantaneously to an applied field. This causes dielectric loss, which can be expressed by a permittivity that is both complex and frequency dependent. Real materials are not perfect insulators either, i.e. they have non-zero Direct current direct current conductivity. Taking both aspects into consideration, we can define a complex index of refraction: :

\tilde{n}=n-i\kappa

Here, ''n'' is the refractive index indicating the phase velocity as above, while ''κ'' is called the extinction coefficient, which indicates the amount of absorption (optics) absorption loss when the electromagnetic wave propagates through the material. Both ''n'' and ''κ'' are dependent on the frequency (wavelength). The effect that ''n'' varies with frequency (except in vacuum, where all frequencies travel at the same speed, ''c'') is known as dispersion (optics) dispersion, and it is what causes a Prism (optics) prism to divide white light into its constituent spectral colors, explains rainbows, and is the cause of chromatic aberration in Lens (optics) lenses. In regions of the spectrum where the material does not absorb, the real part of the refractive index tends to increase with frequency. Near absorption peaks, the curve of the refractive index is a complex form given by the Kramers-Kronig relations, and can decreases with frequency. Since the refractive index of a material varies with the frequency (and thus wavelength) of light, it is usual to specify the corresponding vacuum wavelength at which the refractive index is measured. Typically, this is done at various well-defined spectral emission lines; for example, ''n''_D is the refractive index at the Fraunhofer lines Fraunhofer "D" line, the centre of the yellow sodium double emission at 589.29 nanometre nm wavelength. The Sellmeier equation is an empirical formula that works well in describing dispersion, and Sellmeier coefficients are often quoted instead of the refractive index in tables. For some representative refractive indices at different wavelengths, see list of indices of refraction. As shown above, dielectric loss and non-zero DC conductivity in materials cause absorption. Good dielectric materials such as glass have extremely low DC conductivity, and at low frequencies the dielectric loss is also negligible, resulting in almost no absorption (κ ≈ 0). However, at higher frequencies (such as visible light), dielectric loss may increase absorption significantly, reducing the material's transparency (optics) transparency to these frequencies. The real and imaginary parts of the complex refractive index are related through use of the Kramers-Kronig relations. For example, one can determine a material's full complex refractive index as a function of wavelength from an absorption spectrum of the material.

Anisotropy
The refractive index of certain media may be different depending on the polarization and direction of propagation of the light through the medium. This is known as birefringence or anisotropy and is described by the field of crystal optics. In the most general case, the ''dielectric constant'' is a rank-2 tensor (a 3 by 3 matrix), which cannot simply be described by refractive indices except for polarizations along principal axes. In magneto-optic (gyro-magnetic) and optical activity optically active materials, the principal axes are complex (corresponding to elliptical polarizations), and the dielectric tensor is complex-Hermitian (for lossless media); such materials break time-reversal symmetry and are used e.g. to construct Faraday isolators.

Nonlinearity
The strong electric field of high intensity light (such as output of a laser) may cause a medium's refractive index to vary as the light passes through it, giving rise to nonlinear optics. If the index varies quadratically with the field (linearly with the intensity), it is called the Kerr effect optical Kerr effect and causes phenomena such as self-focusing and self phase modulation. If the index varies linearly with the field (which is only possible in materials that do not possess inversion symmetry), it is known as the Pockels effect.

Inhomogeneity
If the refractive index of a medium is not constant, but varies gradually with position, the material is known as a gradient-index medium and is described by gradient index optics. Light travelling through such a medium can be bent or focussed, and this effect can be exploited to produce lens (optics) lenses, some optical fibers and other devices. Some common mirages are caused by a spatially-varying refractive index of Earth's atmosphere air.

Applications
The refractive index of a material is the most important property of any optics optical system that uses refraction. It is used to calculate the focusing power of lenses, and the dispersive power of prisms. Since refractive index is a fundamental physical property of a substance, it is often used to identify a particular substance, confirm its purity, or measure its concentration. Refractive index is used to measure solids (glasses and gemstones), liquids, and gasses. Most commonly it is used to measure the concentration of a solute in an aqueous solution. A refractometer is the instrument used to measure refractive index. For a solution of sugar, the refractive index can be used to determine the sugar content (see Brix).

External links

- Dielectric materials

See also
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