K correction
K correction is a process for converting measurements of astronomical objects into their respective rest frames. The correction acts on that object's observed magnitude (or equivalently, its flux). Because astronomical observations often measure through a single filter or bandpass, observers only measure a fraction of the total spectrum, redshifted into the frame of the observer. For example, to compare measurements of stars at different redshifts viewed through a red filter, one must estimate K corrections to these measurements in order to make comparisons. If one could measure all wavelengths of light from an object (a bolometric flux), a K correction would not be required, nor would it be required if one could measure the light emitted in an emission line.
Carl Wilhelm Wirtz (1918),[1] who referred to the correction as a Konstanten k (German for "constant") – correction dealing with the effects of redshift of in his work on Nebula. The English-language claim for the origin of the term "K correction" is Edwin Hubble, who supposedly arbitrarily chose {\displaystyle K} to represent the reduction factor in magnitude due to this same effect and who may not have been aware of or given credit to the earlier work.[2] [3]
The K-correction can be defined as follows
{\displaystyle M=m-5(\log _{10}{D_{L}}-1)-K_{Corr}\!,円}
That is, the adjustment to the standard relationship between absolute and apparent magnitude required to correct for the redshift effect.[4] Here, DL is the luminosity distance measured in parsecs.
The exact nature of the calculation that needs to be applied in order to perform a K correction depends upon the type of filter used to make the observation and the shape of the object's spectrum. If multi-color photometric measurements are available for a given object thus defining its spectral energy distribution (SED), K corrections then can be computed by fitting it against a theoretical or empirical SED template.[5] It has been shown that K corrections in many frequently used broad-band filters for low-redshift galaxies can be precisely approximated using two-dimensional polynomials as functions of a redshift and one observed color.[6] This approach is implemented in the K corrections calculator web-service.[7] [full citation needed ]
References
[edit ]- ^ Wirtz, V.C . (1918). "Über die Bewegungen der Nebelflecke" [On the motion of nebulae]. Astronomische Nachrichten . 206 (13): 109–116. Bibcode:1918AN....206..109W. doi:10.1002/asna.19182061302.
- ^ Hubble, Edwin (1936). "Effects of Red Shifts on the Distribution of Nebulae". Astrophysical Journal . 84: 517–554. Bibcode:1936ApJ....84..517H. doi:10.1086/143782.
- ^ Kinney, Anne; Calzetti, Daniela; Bohlin, Ralph C.; McQuade, Kerry; Storchi-Bergmann, Thaisa; Schmitt, Henrique R. (1996). "Template ultraviolet spectra to near-infrared spectra of star-forming galaxies and their application to K-corrections" (PDF). Astrophysical Journal . 467: 38–60. Bibcode:1996ApJ...467...38K. doi:10.1086/177583. hdl:10183/108772 .
- ^ Hogg, David (2002). "The K Correction". arXiv:astro-ph/0210394 .
- ^ Blanton, Michael R.; Roweis, Sam (2007). "K-corrections and filter transformations in the ultraviolet, optical, and near infrared". The Astronomical Journal . 133 (2): 734–754. arXiv:astro-ph/0606170 . Bibcode:2007AJ....133..734B. doi:10.1086/510127. S2CID 18561804.
- ^ Chilingarian, Igor V.; Melchior, Anne-Laure; Zolotukhin, Ivan Yu. (2010). "Analytical approximations of K-corrections in optical and near-infrared bands". Monthly Notices of the Royal Astronomical Society . 405 (3): 1409. arXiv:1002.2360 . Bibcode:2010MNRAS.405.1409C. doi:10.1111/j.1365-2966.2010.16506.x . S2CID 56310457.
- ^ "K-corrections calculator".
External links
[edit ]- Basic concept of obtaining K corrections
- Hogg, David W.; Baldry, Ivan K.; Blanton, Michael R.; Eisenstein, Daniel J. (2002). "The K correction". arXiv:astro-ph/0210394 . Bibcode:2002astro.ph.10394H.
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