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Next: 4. Concluding remarks. Up: 3. The Results. Previous: 3.3. Distance.

3.4. Integrated Light.

 

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Figure 5: Equivalent V surface brightness distribution. It can be fitted by exponential law for disk, and by gaussian law for central region (are shown by dashed line). The results of fitting are shown by solid line.

Besides the detailed stellar photometry we have performed the surface B,V,R,I photometry of the galaxy. We determined the surface brightness profiles twice. First round, we calculated azimuthally averaged equivalent brightness profiles using the surface photometry routines developed at the Potsdam Astrophysical Institute. In this way we reduce the surface photometry to one-dimensional photometry. The equivalent light profile was used to extract the isophotal radii, mean surface brightnesses and to determine the best-fitting parameters of the particular density distribution models. In addition to the differential radial surface brightness profiles we calculated the growth curve of the galaxy by summing up the pixel values from center outwards in successive isophotes. The total magnitudes were estimated by asymptotic extrapolation of this radial growth curve.

In order to recover some information about the two-dimensional structure such as ellipticities and position angles of isophotes, in a second round of calculations we used an ellipse fitting algorithm, which is based on the formulas given in Bender & Mölenhoff (1987) in its realization in the SURPHOT package running within MIDAS.

As a result of the ellipse fitting we have obtained a set of radial profiles: surface brightness (SB), minor-to-major axis ratio (b/a), position angle (PA) - in B, V, R and I colours. Combining the B and V, and R and I surface brightness profiles, which were obtained with the one set of fitting ellipses applied to corresponding frames, the colour profile was constructed.

The resulting equivalent surface brightness distribution is shown in Figure 5. In both the V and I bands, the surface brightness distribution is falls off as gaussian from 5" to a radius of 20", and fairly flat from 20". The equivalent V band surface brightness can be well fit by a gaussian with central surface brightness mu_0(V)=21.7 mag/arcsec^2 deviation sigma_V=15.9 in the inner regions, and exponential profile with central surface brightness mu_0(V)=21.7 mag/arcsec^2 and exponential scale length alpha=16.2 at larger radii. This gives an angular diameter at the mu_V=26 mag/arcsec^2 isophote of Theta_26=2.1 arcmin; this corresponds to an isophote of mu_I=25.0 mag/arcsec^2. Given the distance of the galaxy, the break in the surface brightness profile occurs at r_equiv=600 pc.

Integrating the surface brightness profiles within the V and I bands out to the mu_V=25 mag/arcsec^2 isophote, we find m_V=13.63+-0.15, and , m_I=14.62+-0.15 uncorrected for internal or galactic extinction. The quoted errors are an upper limit computed assuming that every point in Fig. 3 is systematically off by 1 sigma. After correction for extinction (see §3.1) and considering the error in the distance modulus, the total absolute magnitude of NGC 6789 is M_V,0=-13.26+-0.25 and M_I,0=-12.36+-0.25. The integrated colour index (V-I)0 increases smoothly from 0.67 in the center of NGC 6789 up to 0.90 within the largest visible radii, which is comparable to the colours of galaxy types Scd & Im ((V-I)=0.82) for the Coleman et al. (1980) composite spectral energy distributions.


next up previous
Next: 4. Concluding remarks. Up: 3. The Results. Previous: 3.3. Distance.

Igor Drozdovsky
Fri Aug 21 13:48:14 MSD 1998