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[[Image:Synchrotron Functions.svg|thumb|First and second Synchrotron functions.]]
In [[mathematics]] the '''synchrotron functions''' are defined as follows (for ''x'' ≥ 0):<ref>{{Cite journal |
* First synchrotron function <math display="block">F(x) = x \int_x^\infty K_{\frac{5}{3}}(t)\,dt</math>
▲:<math>G(x) = x K_{\frac{2}{3}}(x)</math>
where ''K''<sub>''j''</sub> is the modified [[Bessel function]] of the second kind.
== Use in
In [[astrophysics]], x is usually a ratio of frequencies, that is, the frequency over a critical frequency (critical frequency is the frequency at which most [[synchrotron radiation]] is radiated). This is needed when calculating the spectra for different types of synchrotron emission. It takes a spectrum of electrons (or any charged particle) generated by a separate process (such as a power law distribution of electrons and positrons from a constant injection spectrum) and converts this to the spectrum of photons generated by the input electrons/positrons.
== References ==▼
<references />▼
==
*{{Cite book |last=Longair |first=Malcolm S. |title=High energy astrophysics |date=2011 |publisher=Cambridge University Press |isbn=978-0-511-93059-1 |edition=3rd |___location=Cambridge |oclc=702125055}}
*{{Cite book |last=Rybicki |first=George B. |url=https://www.bartol.udel.edu/~owocki/phys633/RadProc-RybLightman.pdf |title=Radiative processes in astrophysics |date=2004 |others=Alan P. Lightman |isbn=978-3-527-61817-0 |___location=Weinheim |pages=191 |oclc=212140606}}
▲== References ==
▲<references />
[[Category:Special functions]]
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