Strömgren photometric system

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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 and y filters (b−y) without the effects of reddening, termed m1 and c1.[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 style="background-color: Template:Wavelength color; color:#ffffff; text-align:center;" | 411 style="background-color: Template:Wavelength color; color:#ffffff; text-align:center;" | 467 style="background-color: Template:Wavelength color; color:#000000; text-align:center;" | 547 style="background-color: Template:Wavelength color; color:#000000; text-align:center;"| 485.8 style="background-color: Template:Wavelength color; color:#000000; text-align:center;" | 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); m1; c1; and β.

  • m1=(v−b)−(b−y)
  • c1=(u−v)−(v−b)
  • β=βnarrow−βwide

Where;

See also

References

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