Moissanite lies at the other end of the range with a refractive index as high as 2.65.
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Aerogel is a very low density solid that can be produced with refractive index in the range from 1.002 to 1.265. Almost all solids and liquids have refractive indices above 1.3, with aerogel as the clear exception. Gases at atmospheric pressure have refractive indices close to 1 because of their low density. These values are measured at the yellow doublet D-line of sodium, with a wavelength of 589 nanometers, as is conventionally done. A few examples are given in the adjacent table. PMMA (acrylic, plexiglas, lucite, perspex)įor visible light most transparent media have refractive indices between 1 and 2. Where the coefficients A and B are determined specifically for this form of the equation.įor references, see the extended List of refractive indices. The refractive index n of an optical medium is defined as the ratio of the speed of light in vacuum, c = 299 792 458 m/s, and the phase velocity v of light in the medium, n = c v.
#C60 refractive index database full#
The concept of refractive index applies within the full electromagnetic spectrum, from X-rays to radio waves.
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Nevertheless, refractive indices for materials are commonly reported using a single value for n, typically measured at 633 nm. For most materials the refractive index changes with wavelength by several percent across the visible spectrum. The imaginary part then handles the attenuation, while the real part accounts for refraction. Light propagation in absorbing materials can be described using a complex-valued refractive index. This effect can be observed in prisms and rainbows, and as chromatic aberration in lenses. This causes white light to split into constituent colors when refracted. The refractive index varies with wavelength. As a result, the perceived color of the refracted light to a human eye, which depends on the frequency, is not affected by the refraction or the refractive index of the medium. This implies that vacuum has a refractive index of 1, and that the frequency ( f = v/ λ) of the wave is not affected by the refractive index. The refractive index can be seen as the factor by which the speed and the wavelength of the radiation are reduced with respect to their vacuum values: the speed of light in a medium is v = c/ n, and similarly the wavelength in that medium is λ = λ 0/ n, where λ 0 is the wavelength of that light in vacuum.
![c60 refractive index database c60 refractive index database](https://www.mdpi.com/polymers/polymers-11-00383/article_deploy/html/images/polymers-11-00383-g007.png)
The refractive indices also determine the amount of light that is reflected when reaching the interface, as well as the critical angle for total internal reflection, their intensity ( Fresnel's equations) and Brewster's angle. Where θ 1 and θ 2 are the angles of incidence and refraction, respectively, of a ray crossing the interface between two media with refractive indices n 1 and n 2.
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This is described by Snell's law of refraction, n 1 sin θ 1 = n 2 sin θ 2, The refractive index determines how much the path of light is bent, or refracted, when entering a material.