

Pulsars are weak radio sources. Mean flux densities, usually
quoted in the literature at a radio frequency of 400 MHz, vary
between 1 and 100 mJy (1 Jy
). This means that the addition of many thousands of pulses is
required in order to produce a discernible profile. A remarkable
fact is that, although the individual pulses vary quite
dramatically from pulse to pulse, at any particular observing
frequency the integrated profile is very stable. The pulse
profile can thus be thought of as a finger print of the emission
beam.
Figure 2:
Single pulses from PSR B0329+54. Click here to see the movie
in action.
This process is demonstrated in the animation shown in
Fig.
2
-- a sequence of consecutive single pulses for one of the
brightest pulsars PSR B0329+54
. This pulsar is seen in the animation to stabilise into its
characteristic 3-component form after the summation of about 10
seemingly erratic single pulses. This property is of key
importance in pulsar timing measurements (§
4).
A sample of pulse profiles is presented in Fig.
3
in which a great diversity in profile morphology can be
seen.
Figure 3:
A variety of integrated pulse profiles taken from the
available literature. References: (a,b,d,f: [66]); (c: [23]); (e,g,i: [90
]); (h: [28]). Each profile represents 360 degrees of rotational phase.
These, and over 2600 other pulse profiles are available on-line [3].


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Binary and Millisecond Pulsars
D. R. Lorimer (dunc@mpifr-bonn.mpg.de)
http://www.livingreviews.org/lrr-1998-10
© Max-Planck-Gesellschaft. ISSN 1433-8351
Problems/Comments to
livrev@aei-potsdam.mpg.de
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