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Synthetic spectra

For the galaxies in the radio sample we have observations in B, R and K' bands for several objects and in tex2html_wrap_inline3807 for the remaining. For the former we have available two colors to compare with the synthetic spectra while in the latter case we have only one color. With the degeneracy mentioned in the previous section, it is not very meaningful to carry out a best fit for burst age and strength since such a fit will provide a large range for both the parameters. So, instead, we have plotted the curves showing the age-strength relation. We have also plotted our objects on a similar diagram to see what possible values the parameters are likely to take. In our work we have used synthetic spectra kindly provided by Dr. Bruno Guiderdoni. A detailed prescription of how these are generated can be found in Guiderdoni and Rocca-Volmerange (1987). Details on models other than the burst model can be found in Rocca-Volmerange and Guiderdoni (1988).

Galaxy spectra

The initial mass function (IMF, tex2html_wrap_inline6393 ) is one of the most important inputs for the generation of synthetic spectra. The IMF gives the distribution of the number of stars as a function of mass. The IMF and the law of star formation together provide the number of stars forming in a given mass range at a given time, t. These stars are then placed on the zero age main sequence (ZAMS) in the Hertzprung-Russel (HR) diagram. Theoretical stellar tracks are used to evolve the stars at each time step. The distribution of the stellar populations in the HR diagram tex2html_wrap_inline6397 , is estimated. Using a bolometric correction and the luminosity class, tex2html_wrap_inline6399 is converted to tex2html_wrap_inline6401 . A synthetic stellar spectrum, tex2html_wrap_inline6403 is then constructed. A nebular component tex2html_wrap_inline6405 resulting from the Lyman continuum photons is added. A correction for internal extinction tex2html_wrap_inline6407 is applied.

The synthetic spectra used here are based on the Scalo IMF. This has the form tex2html_wrap_inline6409 , with

  eqnarray3167

The stellar tracks used are from the Geneva group. The stellar spectra are from Kurucz (1992) for hot stars ( tex2html_wrap_inline6411 ), and from Bessel et al., Fluks et al. (1994) for cold stars. The tracks include four evolutionary stages viz. Main Sequence (MS), Giant Branch (GB), ``red'' Horizontal Branch (HB) and Asymptotic Giant Branch (AGB). Along each evolutionary sage, the input stellar tracks are interpolated in mass to get differences of successive masses lower than 1 Gyr. Mass loss of massive stars is taken into consideration.

The basic spectra that we have made use of to obtain colors and magnitudes cover a range of wavelength from tex2html_wrap_inline6413 (1221 distinct wavelengths). We used spectra corresponding to the following 219 distinct ages:
tex2html_wrap_inline6415 , tex2html_wrap_inline6417 , tex2html_wrap_inline6419 . The spectra were generated for different metallicities viz. 0.001, 0.004, 0.008, 0.020 and 0.040. However, we actually used only the solar metallicity spectra with Y=0.28 to 0.30 and Z=0.02. The whole Hubble sequence is represented with one metallicity since the mean metallicity of stars rapidly approaches the solar value. Also, with the scanty data that we have, adding a further variable Z would not have been vary meaningful.

Modus operandi

In this subsection we describe how colors were obtained for a E + A model from the synthetic spectra.: (1) The age of the old galaxy was assumed to be tex2html_wrap_inline6421 . (2) A young burst was then superimposed onto the old galaxy. The burst age was allowed to vary between 0 and 2 Gyr and it was allowed to contain a mass fraction of upto tex2html_wrap_inline6423 . (3) The resulting spectrum was convolved with individual filter response curves, after appropriate corrections for redshift and cosmological dimming were applied, to obtain magnitudes for those filters.

Thus, for each burst age and each mass fraction, a number (magnitude) is obtained for each filter. Colors and isochrones are then obtained from the magnitudes. These are finally compared with the observed colors of the galaxies to estimate the age and strength of the starburst. We in fact, shifted the colors of the radio sample galaxies to a redshift of zero so that all the galaxies can be simultaneously compared with the zero-redshift isochrones.


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Next: Age of the most Up: Ages: how recent is Previous: The existing picture