The Cygnus Loop—a case study
by Keith Davies
The Cygnus Loop is a spectacular supernova remnant (SNR) that has been the subject
of numerous theoretical and observational research studies. Published values for
its age have included estimates as high as 100,000 years. These very high estimates
for its age have proven to be unreliable. Dependable measurements of related observational
parameters are now available and show an age that is less than 3,000 years. One
of the parameter revisions involved the value of the average density of the interstellar
medium (ISM) through which the supernova expands. It was found that the ‘local’
ISM density associated with the Cygnus Loop is about 10 times less than the ‘standard’
ISM density value of one atom per cubic centimetre. It has been proposed by some
researchers that equally low values for the average ISM density apply to the local
environment of many SNRs in the Galaxy. If this proposal is confirmed, then the
published ages of SNRs whose ages were calculated using the ‘standard’
value for the ISM density will also need to be re-evaluated.
The Cygnus Loop is a truly impressive object with a huge angular extent of approximately
230 minutes of arc at its widest span. In comparison, the moon measures only 30
minutes of arc. The Cygnus Loop lies within our own galaxy, in the constellation
of Cygnus the Swan, and was first identified as an SNR over 60 years ago. Some astronomers
believe that there is a less significant SNR situated in the same direction, but
we will be discussing the characteristics of the main SNR traditionally known as
the Cygnus Loop.
The importance of the Cygnus Loop
Photo by Jeff Hester (Arizona State University) and NASA.

Illustration 1: The filamentary structure of the Cygnus Loop.
The fact that the Cygnus Loop is relatively near and unusually free from obscuring
dust means that it can be observed at a wider range of wavelengths than is usual
for galactic SNRs. This permits exceptional observational opportunities that make
it one of the best-known and most extensively researched SNRs in the Galaxy. From
a creationist standpoint, it is important because it has been quoted as a ‘proven’
example of an SNR whose published age is greater than 6,000 years.
Some published estimates of the age of the Cygnus Loop
James Kaler, professor of astronomy at the University of Illinois, has a special
interest in researching the death of stars. He quotes an age of 100,000 years for
the Cygnus Loop in his comprehensive 1994 text on astronomy.1 Samples of other published high age estimates are
20,000 years;2 50,000 years;3 and 150,000 years.4 A display in the public galleries of the David
Dunlap observatory in Toronto asserts that the Cygnus Loop is several million years
old.
All of these high age estimates are wrong. The documentation of the new reality
is the subject of this paper.
The parameter errors that have led to the substantial age revisions
One of the ways used to calculate the age of a large SNR like the Cygnus Loop is
through the application of the well accepted, and often quoted, Sedov Size-Age relation.
This relation can be expressed as D = 4.3 × 10-11 (E0
/n)1/5 t 2/5.5
Here, D is the diameter of the SNR, measured in parsecs (one parsec equals
3.26 light years). E0 is the initial kinetic energy of the SNR,
whose value is well accepted as being around 1051 ergs.6 n is the average density of the ISM that
the SNR expands into, and is measured in terms of the number of atoms present in
a cubic centimetre. t is the age of the SNR and is measured in years.
The above relation requires the input of three parameters to calculate the age of
the Cygnus Loop. Two of these parameters have had incorrect values assigned to them
for many years. The account of how long-accepted values were found to be in error,
and the implications arising from those errors, reads like a scientific detective
story and will be described in this paper.
The story of the first major change in the age estimate of the Cygnus Loop—the
error in the density parameter (n)
One of the first research papers to demonstrate a problem with the published estimates
of the density parameter was written more than thirty years ago by Sergio Ilovaisky
and James Lequeux.7
The authors performed a fascinating statistical analysis involving the frequency
of occurrence of supernovae in the Galaxy. They considered whether the published
high ages for the Cygnus Loop were compatible with their statistical analyses.
The results were a surprise. If the Cygnus Loop was an old classic remnant with
the characteristics they initially considered, then the rate of production of supernovae
in the Galaxy would have to be about one every 315 years. Something was very wrong.
This value was far too high when compared with other independent estimates. They
concluded that the problem lay in the assumed age of the Cygnus Loop. It must be
considerably younger than was previously thought. They state, in their paper, that
an explanation for the discrepancy they found was that the age of the Cygnus Loop
had been ‘grossly overestimated’. They suggested, at that time, that
the Cygnus Loop needed to be reassessed as being around 14,000 years, which is nearly
five times smaller than a previous estimate of around 67,000 years that they reference
in their paper.
How could the previous estimates for the age of the Cygnus Loop have been so wrong?
But how could the previous estimates for the age of the Cygnus Loop have been so
wrong? What error in the data could have resulted in the requirement that its age
estimate needed to be reduced by so much?
The error in the value used for the density of the interstellar medium
Astronomers have a rather unusual way of measuring the near-vacuum densities found
in space. Density is expressed as the number of particles (usually hydrogen atoms)
in a defined volume. They typically use a value of n equal to one particle
per cubic centimetre as a standard for the density of space between stars
and an even smaller value of n equal to one particle per cubic metre
for the space between galaxies.7
Ilovaisky and Lequeux pointed out in their paper that the Cygnus Loop is located
in a rather tenuous medium, where n ≈ 0.1. The more tenuous the medium
the more rapidly the SNR will expand—and this will have a large effect on
any age estimate that is made.
It was this error in the density (of a factor of 10) that was partly the culprit
for the age of the Cygnus Loop being so grossly overestimated in prior publications.
Confirmation of the new lower value for the ambient ISM density
The lower value for the ambient ISM density which the Cygnus Loop SNR moves through
has since been confirmed several times. For example, one study showed that the periphery
of the Cygnus Loop encounters regions where n = 0.2, while in the original
interior region of the huge remnant n = 0.08.8 These more accurate estimates confirm and are in
reasonable accord with the early value of Ilovaisky and Lequeux that was referenced
above. The ISM density of 0.08 will be used later in this paper to make a current
‘best estimate’ value for the age of the Cygnus Loop.
The story of the second major change in the age estimate of the Cygnus Loop—the
error in the size parameter (d)
The second parameter we will consider in this account of falling age estimates is
the linear size of the Cygnus Loop. We can measure the angular size of this huge
object directly. It is known to be 230 × 160 minutes of arc,9 giving a mean value of 195 minutes, but in order
to find its actual diameter; we need to know how far it is away from us. The standard
value for the distance to the Cygnus Loop has, for many years, been 770 parsecs.10 We now know that this value
is substantially in error. The revised distance is only 440 parsecs.9
This new value was originally based upon observations made with the Hubble telescope,
but such a large revision did not find immediate acceptance. There was an understandable
reluctance to accept that such a large error could previously have been made in
the measurement of the distance to such a well known and well observed object. However,
the new Hubble measurement was soon confirmed by the fortuitous discovery of a star,
of known distance, that was found to be behind the Cygnus Loop.11 The new measurement of the distance to the Cygnus
Loop means that its diameter must be now revised to 25 parsecs12 instead of the older value of 56 parsecs. This
new, smaller, size of the Cygnus Loop means that once again its age has to be recalculated.
Using the diameter D ≈ 25 parsecs, the average ambient ISM density
n ≈ 0.08 and the initial kinetic energy ≈ 1051 ergs,
we obtain an age that is considerably less than previously published ages. The age
obtained by applying the above revised values to the Sedov relation is around 2,400
years. However, the story of the continuing fall in the calculated theoretical
age of the Cygnus Loop is still not over. The Cygnus Loop continues to surprise
researchers.
One final surprise
In 2002 a team of researchers announced that a ‘bulge’ observed in one
section of the periphery of the Cygnus Loop might be a second SNR that is smaller
and younger than the primary SNR. If this is confirmed then it would mean that the
angular dimension of the primary SNR is even smaller than before, making the Cygnus
Loop even younger than 2,400 years! If we apply the revised angular measurements
for the primary SNR of 180 by 156 arc minutes13
to the Sedov relation as before, and using the same values for the other parameters,
then the calculated age of the primary SNR falls to 1,700 years, while the smaller
SNR would be less than 1,000 years old.
Application to other SNRs
The question must now be asked, from a creationist standpoint, whether the errors
in observational measurements that have resulted in such a dramatic revision in
the age of the Cygnus Loop would apply more generally to other SNRs. Of particular
interest is the question of the average value of the ISM density that needs to be
used when determining the age of individual SNRs.
The case study of the Cygnus Loop showed that the ‘standard’ density
value of n equal to one particle per cubic centimetre was far too high
and that the actual value was about ten times smaller.
One text on galactic astronomy now states that 90% of the volume of interstellar
space in the Galaxy is probably associated with n < 0.5.14 Other published estimates have indicated that
as much as 70% of the volume of interstellar space could be associated with a value
as low as 0.001!6 If these values are confirmed, then substantial age
reassessments would need to be made for those galactic SNRs whose ages have previously
been calculated by the use of the old standard of n = 1 for the ISM density.
Conclusion
The results are clear. Most of the age estimates for the Cygnus Loop published over
the years are wrong. This ‘classic’ example of a supernova remnant is
not an ‘ancient’ object at all. It is less than a few thousand years
old. This case study, if nothing else, illustrates the care that needs to be taken
before accepting the published age estimates of SNRs at face value.
It is of considerable interest to creationists that the ‘local’ ISM
density associated with the Cygnus Loop is about 10 times less than the ‘standard’
ISM density value of one atom per cubic centimetre. It has been proposed by some
researchers that equally low values for the average ISM density could apply to the
local environment of many SNRs in the Galaxy. If this proposal is confirmed, then
the published ages of SNRs whose ages were calculated using the ‘standard’
value for the ISM density will also need to be re-evaluated.
References
- Kaler, J.B., Astronomy, Harper Collins, New York,
p. 444, 1994. Return to Text.
- Miyata, E. and Tsunemi, H., The plasma structure of the NorthEast
rim of the Cygnus Loop as observed with ASCA, Publications of the Astronomical Society
of Japan 46(3):L101–L104, 1994. Return
to Text.
- Illingworth, V., Dictionary of Astronomy, Facts on
File, New York, p. 106, 1994. Return to Text.
- Kerr, F. J. and Simpson S.C., (Eds.), Galactic Radio Astronomy,
International Astronomical Union, p. 321, 1974. Return to Text.
- Clark, D.H., and Caswell, J.L., A Study of Galactic Supernova
Remnants, based on Molonglo-Parkes Observational Data, Monthly Notices of the Royal
Astronomical Society 174:279, 1976. Return
to Text.
- Arbutina, B. and Urosevic, D., The Σ-D relation for supernova
remnants and its dependence on the density of the interstellar medium, Monthly Notices
of the Royal Astronomical Society 360:76–80, 2005.
Return to Text.
- Ilovaisky, S.A. and Lequeux, J., A Study of Galactic Supernova
Remnants II. Supernova Rate, Galactic Radio Emission and Pulsars, Astronomy and
Astrophysics 20:349, 1972. Return to Text.
- Levenson, N.A., Panoramic Views of the Cygnus Loop, The
Astrophysical Journal Supplement Series 118(2):552, 1998.
Return to Text.
- Green D.A.,
G74.0—8.5 Cygnus Loop from Galactic supernova remnants: an updated
catalogue and some statistics, Bulletin of the Astronomical Society of India
32:335–370, 2004,
www.mrao.cam.ac.uk/surveys/snrs/snrs.G74.0-8.5.html,, 25 July 2006.
Return to Text.
- Kirshner, R., The Cygnus Loop: a new look at an old remnant,
Publications of the Astronomical Society of the Pacific, 88:585–586,
1976. Return to Text.
- Blair, W.P. et al., FUSE observations of
a star behind the Cygnus Loop, Journal of the American Astronomical Society meeting
204(74):05, 2004. Return to Text.
- Using the average value, of around 198 arc minutes for the
average angular extent of the Cygnus Loop θ, the new diameter can be calculated
from the trigonometric expression D = πθd/(180 × 60), where the
diameter D and the distance d are measured in parsecs, and θ is measured in
minutes of arc. Return to Text.
- Uyamker, B., et al., Is the Cygnus Loop two supernova
remnants? Astronomy and Astrophysics 389:L61–L64,
2002. Return to Text.
- Mihalas, D.A.M. and Binney, J., Galactic Astronomy,
2nd Edition, W.H. Freeman and Company, San Francisco, CA, p. 181, 1981.
Return to Text.
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