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Up: CO and H

5. Observational biases due to limited telescope sensitivity

Many of the sample objects are rather distant and have weak far-infrared fluxes (see Sect. 3). The detection limit of the IRAS satellite (tex2html_wrap_inline1782 and tex2html_wrap_inline1784 Jy) implies that at radial velocities larger than tex2html_wrap_inline1786, only galaxies with a FIR luminosity higher than 1010 tex2html_wrap_inline1660 could be detected by IRAS.

Similarly, an observational bias was introduced in the CO and tex2html_wrap_inline1482 data, the choice of a reasonable integration time setting a limit to the tex2html_wrap_inline1482 and H2 gas masses which could be detected. On the average, an integration time of 4 hours has been spent on each galaxy, which corresponds to a noise level of about 3 mK (in tex2html_wrap_inline1798) in the CO data and 3 mJy in the tex2html_wrap_inline1482 data for the velocity resolutions of our spectra. An upper limit to the emission can be determined as tex2html_wrap_inline1802. Using a linewidth tex2html_wrap_inline1804=150 km s-1. this means that within 4 hours of integration a limit of 109 tex2html_wrap_inline1810 (108 tex2html_wrap_inline1810 respectively) on the H2 mass is reached only for galaxies with tex2html_wrap_inline1818 (tex2html_wrap_inline1820 respectively). For tex2html_wrap_inline1482, a limit of 109 tex2html_wrap_inline1810 is reached within 4 hours for galaxies with tex2html_wrap_inline1828.



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