Brightness-Temperature Threshold

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Brightness-Temperature Threshold

Murphy (1998) has found a detection threshold of tex2html_wrap_inline480 K for ARISE on a 40,000-km baseline to a VLBA telescope, or tex2html_wrap_inline426 K on a 50,000-km baseline, given an 8-Gbit sectex2html_wrap_inline346 data rate and telescope sensitivities similar to those quoted in this document. For a 100,000-km baseline, the observed threshold rises to tex2html_wrap_inline486 K, corresponding to tex2html_wrap_inline488 K. If a large telescope such as the GBT were used to anchor the ground array, the observed limits would be reduced to tex2html_wrap_inline490 K for a 40,000-km baseline, or tex2html_wrap_inline492 K for a 100,000-km baseline.

Given these brightness temperatures, the assumptions made in Section 3 can be summarized in a useful way. The estimate of tex2html_wrap_inline494 detectable sources for ARISE above a threshold of 120 mJy (Table 2) assumed that those sources have cores with observed 86-GHz brightness temperatures above the tex2html_wrap_inline496 threshold. Since blazars are beamed toward the observer, the brightness temperatures are expected to be near or above the inverse Compton limit in most cases. Thus, in general, we can expect tex2html_wrap_inline498 K, as found in the TDRSS experiments (Linfield et al. 1989). Most of the 210 sources above 600 mJy in total 86-GHz flux will then be detectable by ARISE on baselines up to tex2html_wrap_inline500 km (cf. Murphy 1998 for the brightness temperature calculations). However, on baselines near 100,000 km, the detection requirement of tex2html_wrap_inline502 K would be higher than the highest brightness temperature observed with centimeter-wavelength Space VLBI, with either TDRSS (Linfield et al. 1989) or VSOP (Preston et al. 1999). Therefore, the evidence is that very few sources would be detectable at 86 GHz on a 100,000-km ARISE baseline, but that a maximum ARISE orbit altitude of 40,000 km (and corresponding maximum baseline length of 50,000 km) is fairly well-matched to the properties of blazars.

Table 6. Required Aperture Efficiency for
Threshold of tex2html_wrap_inline460 K
Baseline Length (km) Aperture Efficiency
50,000 0.08
60,000 0.12
70,000 0.16
80,000 0.20
90,000 0.26
100,000 0.32

If it is desired to fly ARISE at an apogee altitude of 100,000 km, observations of a large number of blazars would require a sensitivity increase of a factor of 4 to achieve a detection threshold of tex2html_wrap_inline460 K at 86 GHz. This would mean that a 25-meter ARISE antenna must have a total aperture efficiency greater than 30% at 86 GHz, rather than the low efficiency of 8% that is currently assumed. Table 6 gives the aperture efficiency that would be required (assuming 8 Gbit sectex2html_wrap_inline346 and tex2html_wrap_inline510 K) in order to achieve a brightness temperature detection threshold of tex2html_wrap_inline412 K on baselines ranging from 50,000 to 100,000 km.


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