Dispersion and refractive indices

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Different frequencies of light exhibit varying refractive indices in the same material, leading to different speeds, which complicates the notion that the speed of light in a material is simply c/n, where n is a standard refractive index. This frequency dependence results in a distinction between group velocity and wave velocity, causing short wave packets to spread due to dispersion. It is more accurate to express the speed of light as c(ω) = c0/n(ω), acknowledging that both c and n are functions of frequency. The refractive index "n" is typically defined at a specific wavelength, and since visible light spans a range of frequencies, its interaction with materials varies accordingly. Understanding this nuance is essential for accurately describing light behavior in different media.
user3
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If different frequencies of light have different refractive indices for the same material and travel at different speed in the same material, isn't it inaccurate to say that the speed of light through a certain material is c/n, where n is the "standard" refractive index?
 
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Yes, but it is usually a reasonable approximation.
The dependence of n on frequency is why the 'group velocity' differs from the 'wave velocity'.
A short wave packet would tend to spread because of this depedence of n on frequency.
 
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Well, if there is dispersion, you would rather say that ##c(\omega)=c_0/n(\omega)##. Often, people take it for granted that c and n are functions of ##\omega## and don't mention it explicitly.
 
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user3 said:
If different frequencies of light have different refractive indices for the same material and travel at different speed in the same material, isn't it inaccurate to say that the speed of light through a certain material is c/n, where n is the "standard" refractive index?

"n" is specified at a certain wavelength. Visible light covers an octave of frequencies so it is hardly surprising that it interacts with transparent substances differently over that range.
 
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