These enhancements can be made entirely within the existing infrastructure at the VLA Site:
Figure: The current (+) and predicted (o) continuum (left) and
spectral line (right) sensitivity of the VLA after the upgrade. For
both panels, a 12-hour observation with 27 antennas and with the
efficiencies and system temperatures listed in Table
2.3 are assumed. The continuum sensitivity assumes
bandwidths given in Table
2.3,
while the line sensitivity is based on a bandwidth equivalent to 1
. (Note the different vertical scales.) For the A+
configuration and 37 antennas, the sensitivity would be improved by a
further factor of 1.33. To illustrate the relative
sensitivities of the proposed new bands for nonthermal and thermal
objects, the left panel also shows the slopes of a typical
synchrotron spectrum (dashed) and of an optically thick thermal
spectrum (dotted). The vertical placement of these spectra is
arbitrary.
The continuum sensitivity will improve by more than an order of magnitude in some bands. Figure 2.1 shows the current and expected sensitivity for both line and continuum observations, and demonstrates how these various improvements will impact all observing frequencies. Typical spectra for an optically thin object, and an optically thick thermal object are shown to demonstrate how the proposed S and Ka bands will be the best for work on these objects. New and powerful spectral line observations will be possible and significantly more frequency choices will be available.
Note also that although the sensitivity improvements per spectral line shown in Figure 2.1 are modest below 10 GHz, the proposed new correlator will allow several different transitions to be observed simultaneously. Some multi-transition spectral-line experiments will be more sensitive because longer integration times are available per line.