Supplementary Material to:

An Introduction to Radio Astronomy

4th edition Cambridge University Press 2019   

Last updated 04/12/2021


 

Chapter 15: Pulsars

IRA4 Chapter 15 gives a concise account of this rapidly-growing subject; more details may be found in Pulsar Astronomy by Andrew Lyne and Francis Graham-Smith , Cambridge University Press 4thedn 2012. See also Pulsar Astrophysics: the Next 50 Years, IAU Symp. 337, 2017. 

 

The discovery of pulsars.

cp1919discovery.PNG

                        

The plot above shows first recording of PSR B1919+21.  The periodic nature of the signal appeared in the fast chart recording.

 

 

 

The sounds of pulsars

 

The pulse trains of some well-known pulsars are shown along with audio clips can be found at:    http://www.jb.man.ac.uk/research/pulsar/Education/Sounds/

 

 

 

Positions of pulsars and MSPs in Galactic coordinates.

psrsanddm Driessen.PNG

The pulsars and MSPs are from the ATNF pulsar catalogue (Hobbs et al. 2004; http://www.atnf.csiro.au/people/pulsar/psrcat/), and have been classified as pulsars or MSPs according to the catalogue. The background colour scale shows the Galactic electron content as Dispersion Measure (DM) according to the YMW16 model (Yao, Manchester & Wang, 2017). As well as the Galactic plane, some other noticeable features in DM are the large ellipse of the Gum Nebula (centred at l=96o, b=-4o  and the tangential line of sight down the Carina Arm of the Milky Way at l=-75o to -60o, b=0o.  Compiled by L.N.Driessen, JBCA.

 

 

The P/Pdot diagram

ppdot suppmat.PNG

              

 

The diagram above shows all pulsars, RRATs, magnetars and x-ray binaries known at October 2018 (compiled by C.Walker, JBCA).. The data are from the pulsar catalogue  http://www.atnf.csiro.au/research/pulsar/psrcat/,

 

cross-referenced against the RRAT catalog 

 

http://astro.phys.wvu.edu/rratalog/

 

and the magnetar catalog 

 

www.physics.mcgill.ca/~pulsar/magnetar/main.html.

 

 

Pulsar Spectra

 

psrspectra.PNG

Typical spectra selected from a compilation by Jankowski et al 2018 MNRAS 473, 4436  

                 

The Crab Nebula

crabmosaic_hst_f.jpg

 

A Hubble Space Telescope image.  The whole nebula is expanding from an origin in a supernova in 1054. Details near the centre change on a timescale of months, revealing the location of the pulsar. The filled, as opposed to shell-like, nature of the nebula classes it as a “plerion” or pulsar wind nebula (see below and Safi-Harb (2012) https://arxiv.org/pdf/1210.5406.pdf)

 

Pulsar Wind Nebulae:

 

crabandvelapsrneb.PNG

 

The nebulae close to two pulsars, imaged by the Chandra Xray satellite.  The excitation of the nebula occurs through well-collimated jets along the rotation axis of the pulsar.   See a review of Pulsar Wind Nebulae by Gaensler and Slade 2006 ARAA 44 17

 

Bow Shocks

 

mouse neb.PNG

A pulsar moving with hypersonic velocity can create a bow shock in the surrounding ISM. Left: Bow shock ahead of 0437.  , observed both in X-rays and in H alpha . Brownsberger and Romani  2014 Ap J  784: 154     Right: the head of the Mouse Nebula, combining observations by the VLA (blue) and Chandra X-ray (gold)  Image courtesy of NRAO/AUI and Chandra: ASA/CXC/SAO/B.Gaensler et al.  See a review by Kargaltsev et al 2017 J Plasma Phys.  83 635830501

 

 


 

Pulse de-dispersion – the incoherent approach

 


 

 




 

The Time Variable Radio Sky

Overview

 

Pulsars are just one type of time variable radio source.  Our knowledge of the “Dynamic Radio Sky” was first described in some detail by Cordes et al (2004), New Astronomy, Reviews, 48, 1459 (see also https://arxiv.org/abs/astro-ph/0410045v1) who give the useful relation


between the timescale of a transient W, its flux density S, its distance D, its brightness temperature T and the observing frequency n. This relation, which helps to differentiate between the different types of variable sources (see the diagram below).  This relation can be derived as follows:

 


At a given frequency the peak transient flux density Speak multiplied by D2 is related to the peak luminosity Lpeak

 

 

Cover

 

The figure above is the time–luminosity diagram of radio transients taken from an accessible article by Breton and Halsall  Astronomy & Geophysics, Volume 54, Issue 6, 1 December 2013, Pages 6.36–6.39 (see also https://doi.org/10.1093/astrogeo/att206). The diagram encapsulates our observational knowledge of the transient sky (see also Cordes et al. 2004).

 

Objects in the region to the lower right can be radiating by incoherent processes whose brightness temperature T in the rest frame cannot exceed  ~1012K (see section 2.8); objects to the upper left must be radiating by coherent processes (see also Cordes et al 2004).

 

The study of the  transient sky will be a significant task for the SKA - see for example the overview presentation by R. Fender et al (2015)  https://pos.sissa.it/215/051/pdf but note that this is a rapidly developing field (see below). 

 

 

Fast Radio Bursts

The first of a previously unsuspected class of radio emitters – the Fast Radio Burst sources (FRBs) - was discovered in 2007 when Duncan Lorimer and a graduate student were analysing archived pulsar search data taken with the Parkes (in Australia) radio telescope in 2001.  The story of the recognition of this unusually bright and short individual pulse of radiation, the “Lorimer Burst”, is told by Lorimer et al (2007).  The arrival time vs. observing frequency diagram of the burst shows the characteristic signature of FRBs: an individual burst of a few milliseconds duration which shows the effect of dispersion in the ISM (see descriptions above).

 


Most of the ~300 FRBs (April 2019) now discovered (and the number is increasing rapidly particular from the CHIME telescope) appear to be solitary events but a significant number are known to repeat which makes them much easier to study.  Nevertheless the origin of FRBs, and whether there is more than one type of physical mechanism at work, is currently unknown. Most, if not all, are likely to be associated with extragalactic objects at cosmological distances since FRB dispersion measures are typically 10x that expected from the Milky Way’s ISM.  The extragalactic hypothesis received strong support when the first of the repeaters FRB 121102 was identified as lying in a dwarf galaxy at a redshift z=0.19  (Chatterjee et al. 2017; Tendulkar 2017).  At the SKA Science 2019 meeting (se the programme of speakers at  https://indico.skatelescope.org/event/467/ ) it was reported that ASKAP has located the positions of three FRBs to sub-arcsecond accuracy which places them in galaxies in the redshift range 0.29 to 0.49 (paper by Ryan Shannon) and that CHIME has found 250+ new FRBs with 12 of them being repeaters (paper by Paul Scholz). The distribution of FRBs on the sky appears to be random which is an independent pointer to a cosmological origin.

 

FRB research is continuing to grow in astrophysical and cosmological importance as increasingly powerful searches and the identifications of host galaxies are enabled by the new generations of sensitive, wide-field, radio telescopes and arrays. As a result this is an extremely fast-moving area of research; at the time of writing the most up-to-date published review is that by Petroff, Hessels and Lorimer (2019)  https://arxiv.org/abs/1904.07947.  An on-line catalogue of sources FRBCAT (https://arxiv.org/abs/1601.03547) is continuously updated by Petroff et al.   The CHIME/FRB collaboration has (in 2021) published a catalogue of 536 fast radio bursts  and discussed their phenomenology https://arxiv.org/abs/2106.04352