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・ Spectral estimation of multidimensional signals
・ Spectral evidence
・ Spectral expansion solution
・ Spectral flatness
・ Spectral flux
・ Spectral flux density
・ Spectral gap
・ Spectral Gene
・ Spectral Genomics
・ Spectral geometry
・ Spectral glide
・ Spectral graph theory
・ Spectral Hash
・ Spectral hole burning
・ Spectral imaging
Spectral index
・ Spectral induced polarisation
・ Spectral invariants
・ Spectral layout
・ Spectral leakage
・ Spectral line
・ Spectral line ratios
・ Spectral line shape
・ Spectral mask
・ Spectral method
・ Spectral modeling synthesis
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Spectral index : ウィキペディア英語版
Spectral index
In astronomy, the spectral index of a source is a measure of the dependence of radiative flux density on frequency. Given frequency \nu and radiative flux S, the spectral index \alpha is given implicitly by
:S\propto\nu^\alpha.
Note that if flux does not follow a power law in frequency, the spectral index itself is a function of frequency. Rearranging the above, we see that the spectral index is given by
:\alpha \! \left( \nu \right) = \frac.
Spectral index is also sometimes defined in terms of wavelength \lambda. In this case, the spectral index \alpha is given implicitly by
:S\propto\lambda^\alpha,
and at a given frequency, spectral index may be calculated by taking the derivative
:\alpha \! \left( \lambda \right) =\frac.
The opposite sign convention is sometimes employed,〔Burke, B.F., Graham-Smith, F. (2009). ''An Introduction to Radio Astronomy, 3rd Ed.'', Cambridge University Press, Cambridge, UK, ISBN 978-0-521-87808-1, page 132.〕 in which the spectral index is given by
:S\propto\nu^.
The spectral index of a source can hint at its properties. For example, using the positive sign convention, a spectral index of 0 to 2 at radio frequencies indicates thermal emission, while a steep negative spectral index typically indicates synchrotron emission.
==Spectral Index of Thermal emission==
At radio frequencies (i.e. in the low-frequency, long-wavelength limit), where the Rayleigh–Jeans law is a good approximation to the spectrum of thermal radiation, intensity is given by
:B_\nu(T) \simeq \frac.
Taking the logarithm of each side and taking the partial derivative with respect to \log \, \nu yields
:\frac \simeq 2.
Using the positive sign convention, the spectral index of thermal radiation is thus \alpha \simeq 2 in the Rayleigh-Jeans regime. The spectral index departs from this value at shorter wavelengths, for which the Rayleigh-Jeans law becomes an increasingly inaccurate approximation, tending towards zero as intensity reaches a peak at a frequency given by Wien's displacement law. Because of the simple temperature-dependence of radiative flux in the Rayleigh-Jeans regime, the ''radio spectral index'' is defined implicitly by〔(【引用サイトリンク】publisher=Wolfram Research )〕
:S \propto \nu^ T.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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