For the greatest fidelity, the signal simulations should be produced in two dimensions, since the transfer function due to diffraction of the telescope is two dimensional. In Sections 2 and 4 below, I produce simulated 2D images with point sources and "1/f" emission, respectively. These are costly in terms of disk space. However, they produce many potential simulated timestreams each, namely the rows separated by at least a beam diameter which are mostly independent (at the high spatial frequencies at least).
A cheaper way to produce the simulations (Section 3 and 5) is to produce one dimensional timestreams. This is an oversimplification compared to "real" signals; for example, the 1D point source simulations correspond to the case of the point sources falling exactly on the scan trajectory.
For both the 1D and 2D simulations, the procedure is to: 1) produce an initial timestream or map with infinitesimal angular resolution, dictated by the sampling; 2) Fourier transform the timetream or map; 3) apply the low-pass transfer function of diffraction; 4) inverse Fourier transform to get back to the time domain.
I adopted 1 arcsec sampling for the 2D images. Given the <15 Hz bandwidth of the photometer electronics and the further bandwidth limitation due to diffraction, sampling of the timestreams at 1-2 arcsec is about right for the expected telescope scan rates of 30 - 60 arcsec/sec.
full 2D point source simulation, 2.3 degrees x 2.3 degrees, displayed 0 - 100 mJy
center of 2D point source simulation, 0.15 degrees x 0.15 degrees, displayed 0 - 30 mJy
I assumed a uniformly illuminated telescope of diameter 3.5 m to estimate the diffraction transfer function.
Below are some sample timestreams for 1 arcsec sampling:
row 4097,
ASCII format
detail in row 4097
row 6345,
ASCII format
detail in row 6345
And some sample timestreams for 2 arcsec sampling:
detail in row 4097 with 2" sampling,
ASCII format
detail in row 6345 with 2" sampling,
ASCII format
I ran two cases: structure amplitude going as (f + f0)^-1, and structure
going as (f + f0)^-2. f is the spatial frequency, and f0 is a small number to
keep the amplitude finite at DC. The phase of each Fourier component was a
random number. In both cases, the simulation is 8192 arcsec x 8192 arcsec,
and the telescope transfer function was for lambda = 250 micron and a
uniformly illuminated 3.5 m telescope.
2D f^-1 Galactic
simulation, 2.3 degrees x 2.3 degrees, displayed 0 - 460 Jy
2D f^-2 Galactic
simulation, 2.3 degrees x 2.3 degrees, displayed 0 - 460 Jy
Below are some sample timestreams for 1 arcsec sampling:
row 4140 of f^-1 simulation,
ASCII format
row 5630 of f^-2 simulation,
ASCII format
And some zooms at 2 arcsec sampling:
zoom of row 4140 with 2" samping,
ASCII format
zoom of row 5630 with 2" samping,
ASCII format