With these radar parameters defined and fine-tuned by using information from
all the scans, a simple time-blanking method was used to extract the line
profile. First, for each scan, the time of arrival of the first pulse was
calculated as follows: we found an 8-pulse sequence in each scan near the
time when the radar was pointing near the GBT (since each scan
was
180 sec., there were
15 sweeps of the radar in each
scan). Once an 8-pulse sequence was identified for each scan, using the
nominal pulse frequency we could calculate the expected arrival times of all
the pulses in a scan.
A single pulse width is
2
sec, but due to multiple
reflections from nearby sources, pulses can arrive as late
as
150
sec after the expected arrival time. Thus, we
skipped
270
sec of data around a pulse:
70
sec of data
were skipped before the expected arrival time, and
200
sec of data
was skipped after the expected arrival time. Since we skipped
270
sec of data for approximately every
2929
sec of
data, we lose
9.2% of the data.
There are very few transient pulses which have delays longer
than
300
sec, which are most probably due to aircrafts near GBT.
But since such reflections are very rare, we ignored those in our analysis.
We integrated the ON and OFF scans by computing 1024-point Fast Fourier Transform (FFT) of the blanked real data samples, which produced 512-point power spectra. The two ON and two OFF channels were added together to yield the final ON and OFF spectra. These are plotted in figure 3(a). The sharp peak at 3.2 MHz is due to internal RFI in the receiver which was a harmonic of 5 MHz: 1260.69 - (3.2 - 2.5) = 1289.99 MHz. For comparison, the unblanked integrations are shown in figure 3(b). As can be seen from these two figures, time blanking does result in a significant amount of RFI excision.
|
[After
blanking]
[Before
blanking]
|