Strömgren photometric system

The Strömgren photometric system, abbreviated also as uvbyβ or simply uvby, and sometimes referred as Strömgren - Crawford photometric system, is a four-colour medium-passband photometric system plus Hβ (H-beta) filters for determining magnitudes and obtaining spectral classification of stars. Its use was pioneered by the Danish astronomer Bengt Strömgren in 1956[1] and was extended by his colleague the American astronomer David L. Crawford in 1958.[2]

It is often considered to be a powerful tool and successful investigating the brightness and effective temperature of stars. This photometric system also has a general advantage as it can be used to measure the effects of reddening and interstellar extinction.[3] This system also allows calculation of parameters from the b {\displaystyle b} and y {\displaystyle y} filters ( b y ) {\displaystyle (b-y)} without the effects of reddening, termed m 1 {\displaystyle m_{1}} and c 1 {\displaystyle c_{1}} .[3]

Wavelength and half-width response functions

The following table shows the characteristics of each of the filters used (represented colors are only approximate):

Strömgren photometric system filter wavelength and half-width response functions
u v b y βnarrow βwide
Peak wavelength (nm) 350 411 467 547 485.8 485
Half-width (nm) 30 19 18 23 2.9 12.9
Note: colors are only approximate and based on wavelength to sRGB representation (when possible).[4]

Indices

There are four main highly applied and technical indices: ( b y ) {\displaystyle (b-y)} ; m 1 {\displaystyle m_{1}} ; c 1 {\displaystyle c_{1}} ; and β {\displaystyle \beta } .

  • m 1 = ( v b ) ( b y ) {\displaystyle m_{1}=(v-b)-(b-y)}
  • c 1 = ( u v ) ( v b ) {\displaystyle c_{1}=(u-v)-(v-b)}
  • β = β n a r r o w β w i d e {\displaystyle \beta =\beta _{narrow}-\beta _{wide}}

Where;

  • y {\displaystyle y} magnitudes are well-correlated with Johnson-Morgan V magnitudes (its V band).
  • ( b y ) {\displaystyle (b-y)} is sensitive to stellar temperature (measure of Paschen continuum).
  • c 1 {\displaystyle c_{1}} is sensitive to the surface gravity (measures Balmer discontinuity strength).
  • m 1 {\displaystyle m_{1}} is sensitive to the metallicity (measure of line blanketing).

See also

  • Photometric systems
  • Stellar classification

References

  1. ^ Strömgren, Bengt (1956). "Two-dimensional spectral classification of F stars through photoelectric photometry with interference filters". Vistas in Astronomy. 2 (1): 1336–1346. Bibcode:1956VA......2.1336S. doi:10.1016/0083-6656(56)90060-5.
  2. ^ Crawford, D. L. (1958). "Two-Dimensional Spectral Classification by Narrow-Band Photometry for B Stars in Clusters and Associations". Astrophysical Journal. 128: 185–206. Bibcode:1958ApJ...128..185C. doi:10.1086/146536.
  3. ^ a b Paunzen, E. (2015). "A new catalogue of Strömgren-Crawford uvbyβ photometry". Astronomy and Astrophysics. 580: A23. arXiv:1506.04568. Bibcode:2015A&A...580A..23P. doi:10.1051/0004-6361/201526413.
  4. ^ "Light wavelength to RGB Converter". www.johndcook.com. Retrieved 2023-07-28.

External links

  • The Asiago Database on Photometric Systems
  • The uvby photometric system
  • Stromgren photometric system tutorial
  • SAGA: Strömgren survey for Asteroseismology and Galactic Archaeology
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