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In , the refractive index (or refraction index) of an is the of the apparent speed of light in the air or vacuum to the speed in the medium. The refractive index determines how much the path of is bent, or , when entering a material. This is described by Snell's law of refraction, , where and are the angle of incidence and angle of refraction, respectively, of a ray crossing the interface between two media with refractive indices and . The refractive indices also determine the amount of light that is when reaching the interface, as well as the critical angle for total internal reflection, their intensity (Fresnel equations) and Brewster's angle.

(2025). 9780321188786., Addison-Wesley. 9780321188786.

The refractive index, n, can be seen as the factor by which the speed and the of the radiation are reduced with respect to their vacuum values: the speed of light in a medium is , and similarly the wavelength in that medium is , where is the wavelength of that light in vacuum. This implies that vacuum has a refractive index of 1, and assumes that the () of the wave is not affected by the refractive index.

The refractive index may vary with wavelength. This causes white light to split into constituent colors when refracted. This is called dispersion. This effect can be observed in prisms and , and as chromatic aberration in lenses. Light propagation in absorbing materials can be described using a -valued refractive index.

(1999). 9780521029971, Cambridge University Press.
The part then handles the , while the part accounts for refraction. For most materials the refractive index changes with wavelength by several percent across the visible spectrum. Consequently, refractive indices for materials reported using a single value for must specify the wavelength used in the measurement.

The concept of refractive index applies across the full electromagnetic spectrum, from to . It can also be applied to phenomena such as . In this case, the speed of sound is used instead of that of light, and a reference medium other than vacuum must be chosen.

(2025). 9780471847892, John Wiley. .
Refraction also occurs in oceans when light passes into the where salinity has impacted the density of the water column.

For (such as ), a lens made from a high refractive index glass will be thinner, and hence lighter, than a – usually cheaper – conventional lens with a lower refractive index.

Plastics materials tend to have lower refractive indices than glasses, but have significantly less density than glasses. Therefore since many years the lightest eyeglasses are fabricated from plastics.

Definition
The relative refractive index of an optical medium 2 with respect to another reference medium 1 () is given by the ratio of speed of light in medium 1 to that in medium 2. This can be expressed as follows: n_{21}=\frac{v_1}{v_2}. If the reference medium 1 is , then the refractive index of medium 2 is considered with respect to vacuum. It is simply represented as and is called the absolute refractive index of medium 2.

The absolute refractive index n of an optical medium is defined as the ratio of the speed of light in vacuum, , and the of light in the medium, n=\frac{\mathrm{c}}{v}. Since is constant, is inversely proportional to : n\propto\frac{1}{v}. The phase velocity is the speed at which the crests or the phase of the moves, which may be different from the , the speed at which the pulse of light or the envelope of the wave moves. Historically at a standardized and has been common as a reference medium.

History
Thomas Young was presumably the person who first used, and invented, the name "index of refraction", in 1807. At the same time he changed this value of refractive power into a single number, instead of the traditional ratio of two numbers. The ratio had the disadvantage of different appearances. , who called it the "proportion of the sines of incidence and refraction", wrote it as a ratio of two numbers, like "529 to 396" (or "nearly 4 to 3"; for water). , who called it the "ratio of refraction", wrote it as a ratio with a fixed numerator, like "10000 to 7451.9" (for urine). wrote it as a ratio with a fixed denominator, like 1.3358 to 1 (water).

Young did not use a symbol for the index of refraction, in 1807. In the later years, others started using different symbols: , , and . Exponent des Brechungsverhältnisses is index of refraction The symbol gradually prevailed.

Typical values
Refractive index also varies with wavelength of the light as given by Cauchy's equation. The most general form of this equation is n(\lambda) = A + \frac {B}{\lambda^2} + \frac{C}{\lambda^4} + \cdots, where is the refractive index, is the wavelength, and , , , etc., are that can be determined for a material by fitting the equation to measured refractive indices at known wavelengths. The coefficients are usually quoted for as the vacuum wavelength in .

Usually, it is sufficient to use a two-term form of the equation: n(\lambda) = A + \frac{B}{\lambda^2}, where the coefficients and are determined specifically for this form of the equation.

+ Selected refractive indices at . For references, see the extended List of refractive indices. ! scope="col"Material ! scope="col"
at 0 °C and 1 atm
at 20 °C

For most transparent media have refractive indices between 1 and 2. A few examples are given in the adjacent table. These values are measured at the yellow doublet D-line of , with a wavelength of 589 , as is conventionally done. Gases at atmospheric pressure have refractive indices close to 1 because of their low density. Almost all solids and liquids have refractive indices above 1.3, with as the clear exception. Aerogel is a very low density solid that can be produced with refractive index in the range from 1.002 to 1.265. lies at the other end of the range with a refractive index as high as 2.65. Most plastics have refractive indices in the range from 1.3 to 1.7, but some high-refractive-index polymers can have values as high as 1.76.

For light refractive indices can be considerably higher. is transparent in the wavelength region from and has a refractive index of about 4.Tosi, Jeffrey L., article on Common Infrared Optical Materials in the Photonics Handbook, accessed on 2014-09-10 A type of new materials termed "topological insulators", was recently found which have high refractive index of up to 6 in the near to mid infrared frequency range. Moreover, topological insulators are transparent when they have nanoscale thickness. These properties are potentially important for applications in infrared optics.

Refractive index below unity
According to the theory of relativity, no information can travel faster than the speed of light in vacuum, but this does not mean that the refractive index cannot be less than 1. The refractive index measures the of light, which does not carry .
(2025). 9780470973950, Wiley-VCH. .
The phase velocity is the speed at which the crests of the wave move and can be faster than the speed of light in vacuum, and thereby give a refractive index This can occur close to resonance frequencies, for absorbing media, in plasmas, and for . In the X-ray regime the refractive indices are lower than but very (exceptions close to some resonance frequencies). As an example, water has a refractive index of for X-ray radiation at a photon energy of ( wavelength).

An example of a plasma with an index of refraction less than unity is Earth's . Since the refractive index of the ionosphere (a plasma), is less than unity, electromagnetic waves propagating through the plasma are bent "away from the normal" (see ) allowing the radio wave to be refracted back toward earth, thus enabling long-distance radio communications. See also Radio Propagation and .

Negative refractive index
Recent research has also demonstrated the "existence" of materials with a negative refractive index, which can occur if and permeability have simultaneous negative values. This can be achieved with periodically constructed . The resulting negative refraction (i.e., a reversal of Snell's law) offers the possibility of the and other new phenomena to be actively developed by means of metamaterials.

Microscopic explanation
At the atomic scale, an electromagnetic wave's phase velocity is slowed in a material because the creates a disturbance in the charges of each atom (primarily the ) proportional to the electric susceptibility of the medium. (Similarly, the creates a disturbance proportional to the magnetic susceptibility.) As the electromagnetic fields oscillate in the wave, the charges in the material will be "shaken" back and forth at the same frequency. The charges thus radiate their own electromagnetic wave that is at the same frequency, but usually with a phase delay, as the charges may move out of phase with the force driving them (see sinusoidally driven harmonic oscillator). The light wave traveling in the medium is the macroscopic superposition (sum) of all such contributions in the material: the original wave plus the waves radiated by all the moving charges. This wave is typically 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 or even at other frequencies (see ).

Depending on the relative phase of the original driving wave and the waves radiated by the charge motion, there are several possibilities:

  • If the electrons emit a light wave which is 90° out of phase with the light wave shaking them, it will cause the total light wave to travel slower. This is the normal refraction of transparent materials like glass or water, and corresponds to a refractive index which is real and greater than 1.
    (2025). 9780465024933, Basic Books.
  • If the electrons emit a light wave which is 270° out of phase with the light wave shaking them, it will cause the wave to travel faster. This is called "anomalous refraction", and is observed close to absorption lines (typically in infrared spectra), with in ordinary materials, and with radio waves in Earth's . It corresponds to a less than 1, which causes the refractive index to be also less than unity and the of light greater than the speed of light in vacuum (note that the is still less than , as discussed above). If the response is sufficiently strong and out-of-phase, the result is a negative value of and imaginary index of refraction, as observed in metals or plasma.
  • If the electrons emit a light wave which is 180° out of phase with the light wave shaking them, it will destructively interfere with the original light to reduce the total light intensity. This is light absorption in opaque materials and corresponds to an refractive index.
  • If the electrons emit a light wave which is in phase with the light wave shaking them, it will amplify the light wave. This is rare, but occurs in due to stimulated emission. It corresponds to an imaginary index of refraction, with the opposite sign to that of absorption.
For most materials at visible-light frequencies, the phase is somewhere between 90° and 180°, corresponding to a combination of both refraction and absorption.

Dispersion
The refractive index of materials varies with the wavelength (and ) of light. This is called dispersion and causes prisms and to divide white light into its constituent spectral . As the refractive index varies with wavelength, so will the refraction angle as light goes from one material to another. Dispersion also causes the of lenses to be wavelength dependent. This is a type of chromatic aberration, which often needs to be corrected for in imaging systems. In regions of the spectrum where the material does not absorb light, the refractive index tends to with increasing wavelength, and thus with frequency. This is called "normal dispersion", in contrast to "anomalous dispersion", where the refractive index with wavelength. For visible light normal dispersion means that the refractive index is higher for blue light than for red.

For optics in the visual range, the amount of dispersion of a lens material is often quantified by the : V = \frac{n_\mathrm{yellow} - 1}{n_\mathrm{blue} - n_\mathrm{red}}. For a more accurate description of the wavelength dependence of the refractive index, the Sellmeier equation can be used. It is an empirical formula that works well in describing dispersion. Sellmeier coefficients are often quoted instead of the refractive index in tables.

Principal refractive index wavelength ambiguity
Because of dispersion, it is usually important to specify the vacuum wavelength of light for which a refractive index is measured. Typically, measurements are done at various well-defined spectral .

Manufacturers of optical glass in general define principal index of refraction at yellow spectral line of helium () and alternatively at a green spectral line of mercury (), called and lines respectively. is defined for both and denoted and . The spectral data provided by glass manufacturers is also often more precise for these two wavelengths.

(1998). 9783642633492

Both, and spectral lines are singlets and thus are suitable to perform a very precise measurements, such as spectral goniometric method.

(2021). 9781510645905, SPIE.

In practical applications, measurements of refractive index are performed on various refractometers, such as Abbe refractometer. Measurement accuracy of such typical commercial devices is in the order of 0.0002. Refractometers usually measure refractive index , defined for sodium doublet (), which is actually a midpoint between two adjacent yellow spectral lines of sodium. Yellow spectral lines of helium () and sodium () are apart, which can be considered negligible for typical refractometers, but can cause confusion and lead to errors if accuracy is critical.

All three typical principle refractive indices definitions can be found depending on application and region,

(1998). 9783642633492 .
so a proper subscript should be used to avoid ambiguity.

Complex refractive index
When light passes through a medium, some part of it will always be . This can be conveniently taken into account by defining a complex refractive index, \underline{n} = n - i\kappa.

The real and imaginary parts of this refractive index are not independent, and are connected through the Kramers–Kronig relations, i.e. the complex refractive index is a linear response function, ensuring causality.

(2025). 9783030871444, Springer, Cham. .
Here, the real part is the refractive index and indicates the , while the imaginary part is called the extinction coefficient indicates the amount of attenuation when the electromagnetic wave propagates through the material. It is related to the absorption coefficient, \alpha_\text{abs}, through: \alpha_\text{abs}(\omega) = \frac{2\omega\kappa(\omega)}{c} These values depend upon the frequency of the light used in the measurement.

That corresponds to absorption can be seen by inserting this refractive index into the expression for of a electromagnetic wave traveling in the -direction. This can be done by relating the complex to the complex refractive index through , with being the vacuum wavelength; this can be inserted into the plane wave expression for a wave travelling in the -direction as: \begin{align} \mathbf{E}(x, t) 

 &= \operatorname{Re}\! \left[\mathbf{E}_0 e^{i(\underline{k}x - \omega t)}\right] \\
 &= \operatorname{Re}\! \left[\mathbf{E}_0 e^{i(2\pi(n + i\kappa)x/\lambda_0 - \omega t)}\right] \\
 &= e^{-2\pi \kappa x/\lambda_0} \operatorname{Re}\! \left[\mathbf{E}_0 e^{i(kx - \omega t)}\right].
\end{align}

Here we see that gives an exponential decay, as expected from the Beer–Lambert law. Since intensity is proportional to the square of the electric field, intensity will depend on the depth into the material as

I(x)= I_0 e^{-4\pi \kappa x/\lambda_0} .

and thus the absorption coefficient is , and the penetration depth (the distance after which the intensity is reduced by a factor of ) is .

Both and are dependent on the frequency. In most circumstances (light is absorbed) or (light travels forever without loss). In special situations, especially in the of , it is also possible that , corresponding to an amplification of the light.

An alternative convention uses instead of , but where still corresponds to loss. Therefore, these two conventions are inconsistent and should not be confused. The difference is related to defining sinusoidal time dependence as versus . See Mathematical descriptions of opacity.

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. However, at higher frequencies (such as visible light), dielectric loss may increase absorption significantly, reducing the material's transparency to these frequencies.

The real , and imaginary , parts of the complex refractive index are related through the Kramers–Kronig relations. In 1986, A.R. Forouhi and I. Bloomer deduced an equation describing as a function of photon energy, , applicable to amorphous materials. Forouhi and Bloomer then applied the Kramers–Kronig relation to derive the corresponding equation for as a function of . The same formalism was applied to crystalline materials by Forouhi and Bloomer in 1988.

The refractive index and extinction coefficient, and , are typically measured from quantities that depend on them, such as reflectance, , or transmittance, , or ellipsometric parameters, . The determination of and from such measured quantities will involve developing a theoretical expression for or , or and in terms of a valid physical model for and . By fitting the theoretical model to the measured or , or and using regression analysis, and can be deduced.

X-ray and extreme UV
For and extreme ultraviolet radiation the complex refractive index deviates only slightly from unity and usually has a real part smaller than 1. It is therefore normally written as (or with the alternative convention mentioned above). Far above the atomic resonance frequency delta can be given by \delta = \frac{r_0 \lambda^2 n_\mathrm{e}}{2 \pi} where is the classical electron radius, is the X-ray wavelength, and is the electron density. One may assume the electron density is simply the number of electrons per atom multiplied by the atomic density, but more accurate calculation of the refractive index requires replacing with the complex atomic form factor It follows that \begin{align} \delta &= \frac{r_0 \lambda^2}{2 \pi} (Z + f') n_\text{atom} \\ \beta &= \frac{r_0 \lambda^2}{2 \pi} f'' n_\text{atom} \end{align} with and typically of the order of and .

Relations to other quantities
Optical path length
Optical path length (OPL) is the product of the geometric length of the path light follows through a system, and the index of refraction of the medium through which it propagates,R. Paschotta, article on optical thickness in the Encyclopedia of Laser Physics and Technology , accessed on 2014-09-08 \text{OPL} = nd. This is an important concept in optics because it determines the phase of the light and governs interference and of light as it propagates. According to Fermat's principle, light rays can be characterized as those curves that optimize the optical path length.

Refraction
When light moves from one medium to another, it changes direction, i.e. it is . If it moves from a medium with refractive index to one with refractive index , with an incidence angle to the of , the refraction angle can be calculated from Snell's law:R. Paschotta, article on refraction in the Encyclopedia of Laser Physics and Technology , accessed on 2014-09-08 n_1 \sin \theta_1 = n_2 \sin \theta_2.

When light enters a material with higher refractive index, the angle of refraction will be smaller than the angle of incidence and the light will be refracted towards the normal of the surface. The higher the refractive index, the closer to the normal direction the light will travel. When passing into a medium with lower refractive index, the light will instead be refracted away from the normal, towards the surface.

Total internal reflection
If there is no angle fulfilling Snell's law, i.e., \frac{n_1}{n_2} \sin \theta_1 > 1, the light cannot be transmitted and will instead undergo total internal reflection. This occurs only when going to a less optically dense material, i.e., one with lower refractive index. To get total internal reflection the angles of incidence must be larger than the critical angle \theta_\mathrm{c} = \arcsin\!\left(\frac{n_2}{n_1}\right)\!.

Reflectivity
Apart from the transmitted light there is also a reflected part. The reflection angle is equal to the incidence angle, and the amount of light that is reflected is determined by the of the surface. The reflectivity can be calculated from the refractive index and the incidence angle with the Fresnel equations, which for reduces to

R_0 = \left|\frac{n_1 - n_2}{n_1 + n_2}\right|^2\!.

For common glass in air, and , and thus about 4% of the incident power is reflected. At other incidence angles the reflectivity will also depend on the polarization of the incoming light. At a certain angle called Brewster's angle, p-polarized light (light with the electric field in the plane of incidence) will be totally transmitted. Brewster's angle can be calculated from the two refractive indices of the interface as \theta_\mathsf{B} = \arctan \left( \frac{n_2}{n_1} \right) ~.

Lenses
The of a lens is determined by its refractive index and the radii of curvature and of its surfaces. The power of a in air is given by the simplified version of the Lensmaker's formula: \frac{1}{f} = (n - 1)\left\frac{1}{R_1}\ , where is the focal length of the lens.

Microscope resolution
The resolution of a good optical is mainly determined by the numerical aperture () of its . The numerical aperture in turn is determined by the refractive index of the medium filling the space between the sample and the lens and the half collection angle of light according to Carlsson (2007): A_\mathrm{Num} = n\sin \theta ~.

For this reason is commonly used to obtain high resolution in microscopy. In this technique the objective is dipped into a drop of high refractive index immersion oil on the sample under study.

Relative permittivity and permeability
The refractive index of electromagnetic radiation equals n = \sqrt{\varepsilon_\mathrm{r} \mu_\mathrm{r}}, where is the material's relative permittivity, and is its relative permeability.
(1976). 9780198511410, Oxford University Press.
The refractive index is used for optics in Fresnel equations and Snell's law; while the relative permittivity and permeability are used in Maxwell's equations and electronics. Most naturally occurring materials are non-magnetic at optical frequencies, that is is very close to 1, therefore is approximately .
(2015). 9781118225516, John Wiley & Sons. .
In this particular case, the complex relative permittivity , with real and imaginary parts and , and the complex refractive index , with real and imaginary parts and (the latter called the "extinction coefficient"), follow the relation \underline{\varepsilon}_\mathrm{r} = \varepsilon_\mathrm{r} + i\tilde{\varepsilon}_\mathrm{r} = \underline{n}^2 = (n + i\kappa)^2,

and their components are related by:

(1972). 9780127634500, .
(online pdf) \begin{align} \varepsilon_\mathrm{r} &= n^2 - \kappa^2\,, \\ \tilde{\varepsilon}_\mathrm{r} &= 2n\kappa\,, \end{align}

and:

\begin{align} n &= \sqrt{\frac{|\underline{\varepsilon}_\mathrm{r}| + \varepsilon_\mathrm{r}}{2}}, \\ \kappa &= \sqrt{\frac{|\underline{\varepsilon}_\mathrm{r}| - \varepsilon_\mathrm{r}}{2}}. \end{align}

where |\underline{\varepsilon}_\mathrm{r}| = \sqrt{\varepsilon_\mathrm{r}^2 + \tilde{\varepsilon}_\mathrm{r}^2} is the complex modulus.

Wave impedance
The wave impedance of a plane electromagnetic wave in a non-conductive medium is given by \begin{align} Z &= \sqrt{\frac{\mu}{\varepsilon}} = \sqrt{\frac{\mu_\mathrm{0}\mu_\mathrm{r}}{\varepsilon_\mathrm{0}\varepsilon_\mathrm{r}}} = \sqrt{\frac{\mu_\mathrm{0}}{\varepsilon_\mathrm{0}}}\sqrt{\frac{\mu_\mathrm{r}}{\varepsilon_\mathrm{r}}} \\ 
 &= Z_0 \sqrt{\frac{\mu_\mathrm{r}}{\varepsilon_\mathrm{r}}} \\
 &= Z_0 \frac{\mu_\mathrm{r}}{n}
\end{align}

where is the vacuum wave impedance, and are the absolute permeability and permittivity of the medium, is the material's relative permittivity, and is its relative permeability.

In non-magnetic media (that is, in materials with ), Z = {Z_0 \over n} and n = {Z_0 \over Z}\,.

Thus refractive index in a non-magnetic media is the ratio of the vacuum wave impedance to the wave impedance of the medium.

The reflectivity between two media can thus be expressed both by the wave impedances and the refractive indices as \begin{align} R_0 &= \left| \frac{n_1 - n_2}{n_1 + n_2} \right|^2 \\ 

   &= \left| \frac{Z_2 - Z_1}{Z_2 + Z_1} \right|^2\,.
\end{align}

Density
In general, it is assumed that the refractive index of a glass increases with its . However, there does not exist an overall linear relationship between the refractive index and the density for all silicate and borosilicate glasses. A relatively high refractive index and low density can be obtained with glasses containing light metal oxides such as and , while the opposite trend is observed with glasses containing and as seen in the diagram at the right.

Many oils (such as ) and are examples of liquids that are more refractive, but less dense, than water, contrary to the general correlation between density and refractive index.

For air, is proportional to the density of the gas as long as the chemical composition does not change. This means that it is also proportional to the pressure and inversely proportional to the temperature for ideal gases. For liquids the same observation can be made as for gases, for instance, the refractive index in alkanes increases nearly perfectly linear with the density. On the other hand, for carboxylic acids, the density decreases with increasing number of C-atoms within the homologeous series. The simple explanation of this finding is that it is not density, but the molar concentration of the chromophore that counts. In homologeous series, this is the excitation of the C-H-bonding. August Beer must have intuitively known that when he gave Hans H. Landolt in 1862 the tip to investigate the refractive index of compounds of homologeous series. While Landolt did not find this relationship, since, at this time dispersion theory was in its infancy, he had the idea of molar refractivity which can even be assigned to single atoms. Based on this concept, the refractive indices of organic materials can be calculated.

Bandgap
The optical refractive index of a semiconductor tends to increase as the decreases. Many attempts have been made to model this relationship beginning with T. S. Moses in 1949. Empirical models can match experimental data over a wide range of materials and yet fail for important cases like InSb, PbS, and Ge.
(1985). 9783112495384, De Gruyter.

This negative correlation between refractive index and bandgap energy, along with a negative correlation between bandgap and temperature, means that many semiconductors exhibit a positive correlation between refractive index and temperature. This is the opposite of most materials, where the refractive index decreases with temperature as a result of a decreasing material density.

Group index
Sometimes, a "group velocity refractive index", usually called the group index is defined: n_\mathrm{g} = \frac{\mathrm{c}}{v_\mathrm{g}}, where is the . This value should not be confused with , which is always defined with respect to the . When the dispersion is small, the group velocity can be linked to the phase velocity by the relation
(1999). 9780521784498, CUP Archive.
v_\mathrm{g} = v - \lambda\frac{\mathrm{d}v}{\mathrm{d}\lambda}, where is the wavelength in the medium. In this case the group index can thus be written in terms of the wavelength dependence of the refractive index as n_\mathrm{g} = \frac{n}{1 + \frac{\lambda}{n}\frac{\mathrm{d}n}{\mathrm{d}\lambda}}.

When the refractive index of a medium is known as a function of the vacuum wavelength (instead of the wavelength in the medium), the corresponding expressions for the group velocity and index are (for all values of dispersion) \begin{align} v_\mathrm{g} &= \mathrm{c}\!\left(n - \lambda_0 \frac{\mathrm{d}n}{\mathrm{d}\lambda_0}\right)^{-1}\!, \\ n_\mathrm{g} &= n - \lambda_0 \frac{\mathrm{d}n}{\mathrm{d}\lambda_0}, \end{align} where is the wavelength in vacuum.

Velocity, momentum, and polarizability
As shown in the Fizeau experiment, when light is transmitted through a moving medium, its speed relative to an observer traveling with speed in the same direction as the light is: \begin{align} V &= \frac{\mathrm{c}}{n} + \frac{v \left(1 - \frac{1}{n^2} \right)}{1 + \frac{v}{c n}} \\ 
 &\approx \frac{\mathrm{c}}{n} + v \left(1 - \frac{1}{n^2} \right)\,.
\end{align}

The momentum of photons in a medium of refractive index is a complex and controversial issue with two different values having different physical interpretations.

The refractive index of a substance can be related to its with the Lorentz–Lorenz equation or to the molar refractivities of its constituents by the Gladstone–Dale relation.

Refractivity
In atmospheric applications, refractivity is defined as , often rescaled as either or ; the multiplication factors are used because the refractive index for air, deviates from unity by at most a few parts per ten thousand.

Molar refractivity, on the other hand, is a measure of the total of a mole of a substance and can be calculated from the refractive index as A = \frac{M}{\rho} \cdot \frac{n^2 - 1}{n^2 + 2}\ , where is the , and is the .

Nonscalar, nonlinear, or nonhomogeneous refraction
So far, we have assumed that refraction is given by linear equations involving a spatially constant, scalar refractive index. These assumptions can break down in different ways, to be described in the following subsections.

Birefringence
In some materials, the refractive index depends on the polarization and propagation direction of the light.R. Paschotta, article on birefringence in the Encyclopedia of Laser Physics and Technology , accessed on 2014-09-09 This is called or optical .

In the simplest form, uniaxial birefringence, there is only one special direction in the material. This axis is known as the optical axis of the material. Light with linear polarization perpendicular to this axis will experience an ordinary refractive index while light polarized in parallel will experience an extraordinary refractive index . The birefringence of the material is the difference between these indices of refraction, . Light propagating in the direction of the optical axis will not be affected by the birefringence since the refractive index will be independent of polarization. For other propagation directions the light will split into two linearly polarized beams. For light traveling perpendicularly to the optical axis the beams will have the same direction. This can be used to change the polarization direction of linearly polarized light or to convert between linear, circular, and elliptical polarizations with .

Many are naturally birefringent, but materials such as and can also often be made birefringent by introducing a preferred direction through, e.g., an external force or electric field. This effect is called , and can be used to reveal stresses in structures. The birefringent material is placed between crossed . A change in birefringence alters the polarization and thereby the fraction of light that is transmitted through the second polarizer.

In the more general case of trirefringent materials described by the field of , the dielectric constant is a rank-2 (a 3 by 3 matrix). In this case the propagation of light cannot simply be described by refractive indices except for polarizations along principal axes.

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

Inhomogeneity
If the refractive index of a medium is not constant but varies gradually with the position, the material is known as a gradient-index (GRIN) medium and is described by gradient index optics. Light traveling through such a medium can be bent or focused, and this effect can be exploited to produce lenses, some , and other devices. Introducing elements in the design of an optical system can greatly simplify the system, reducing the number of elements by as much as a third while maintaining overall performance. The crystalline lens of the human eye is an example of a lens with a refractive index varying from about 1.406 in the inner core to approximately 1.386 at the less dense cortex. Some common are caused by a spatially varying refractive index of air.

Refractive index measurement
Homogeneous media
The refractive index of liquids or solids can be measured with . They typically measure some angle of refraction or the critical angle for total internal reflection. The first laboratory refractometers sold commercially were developed by in the late 19th century. The same principles are still used today. In this instrument, a thin layer of the liquid to be measured is placed between two prisms. Light is shone through the liquid at incidence angles all the way up to 90°, i.e., light rays parallel to the surface. The second prism should have an index of refraction higher than that of the liquid, so that light only enters the prism at angles smaller than the critical angle for total reflection. This angle can then be measured either by looking through a , or with a digital placed in the focal plane of a lens. The refractive index of the liquid can then be calculated from the maximum transmission angle as , where is the refractive index of the prism.

This type of device is commonly used in laboratories for identification of substances and for . Handheld variants are used in by, e.g., to determine in juice, and inline process refractometers are used in, e.g., chemical and pharmaceutical industry for .

In , a different type of refractometer is used to measure the index of refraction and birefringence of . The gem is placed on a high refractive index prism and illuminated from below. A high refractive index contact liquid is used to achieve optical contact between the gem and the prism. At small incidence angles most of the light will be transmitted into the gem, but at high angles total internal reflection will occur in the prism. The critical angle is normally measured by looking through a telescope.

Refractive index variations
Unstained biological structures appear mostly transparent under bright-field microscopy as most cellular structures do not attenuate appreciable quantities of light. Nevertheless, the variation in the materials that constitute these structures also corresponds to a variation in the refractive index. The following techniques convert such variation into measurable amplitude differences:

To measure the spatial variation of the refractive index in a sample phase-contrast imaging methods are used. These methods measure the variations in phase of the light wave exiting the sample. The phase is proportional to the optical path length the light ray has traversed, and thus gives a measure of the of the refractive index along the ray path. The phase cannot be measured directly at optical or higher frequencies, and therefore needs to be converted into intensity by interference with a reference beam. In the visual spectrum this is done using Zernike phase-contrast microscopy, differential interference contrast microscopy (DIC), or .

Zernike phase-contrast microscopy introduces a phase shift to the low spatial frequency components of the with a phase-shifting annulus in the of the sample, so that high-spatial-frequency parts of the image can interfere with the low-frequency reference beam. In the illumination is split up into two beams that are given different polarizations, are phase shifted differently, and are shifted transversely with slightly different amounts. After the specimen, the two parts are made to interfere, giving an image of the derivative of the optical path length in the direction of the difference in the transverse shift. In interferometry the illumination is split up into two beams by a . One of the beams is let through the sample before they are combined to interfere and give a direct image of the phase shifts. If the optical path length variations are more than a wavelength the image will contain fringes.

There exist several phase-contrast X-ray imaging techniques to determine 2D or 3D spatial distribution of refractive index of samples in the X-ray regime.

Applications
The refractive index is an important property of the components of any optical instrument. It determines the focusing power of lenses, the dispersive power of prisms, the reflectivity of lens coatings,
(2006). 9780819478221, SPIE. .
and the light-guiding nature of . Since the 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. The refractive index is used to measure solids, liquids, and gases. It can be used, for example, to measure the concentration of a solute in an . It can also be used as a useful tool to differentiate between different types of gemstone, due to the unique each individual stone displays. A is the instrument used to measure the refractive index. For a solution of sugar, the refractive index can be used to determine the sugar content (see ).

See also
  • Calculation of glass properties
  • Clausius–Mossotti relation
  • Fermat's principle
  • Index-matching material
  • Laser Schlieren deflectometry
  • Optical properties of water and ice
  • Phase-contrast X-ray imaging
  • Prism-coupling refractometry

Footnotes
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