*[A little note: This post, like many others on this blog, contains a few mathematical symbols which are displayed using MathJax. If you are reading this using an RSS reader such as Feedly and you see a lot of $ signs floating around, you may need to click through to the blog to see the proper symbols.]*

People following the reporting of physics in the popular press might remember having come across a paper earlier this year that claimed to have detected the "largest structure in the Universe" in the distribution of quasars, that "challenged the Cosmological Principle". This was work done by Roger Clowes of the University of Central Lancashire and collaborators, and their paper was published in the

*Monthly Notices of the Royal Astronomical Society*back in March (though it was available online from late last year).
The reason I suspect people might have come across it is that it was accompanied by a pretty extraordinary amount of publicity, starting from this press release on the Royal Astronomical Society website. This was then taken up by Reuters, and featured on various popular science websites and news outlets, including

*New Scientist,*The Atlantic*,*National Geographic, Space.com, The Daily Galaxy, Phys.org, Gizmodo, and many more. The structure they claimed to have found even has its own Wikipedia entry.Obligatory artist's impression of a quasar. |

One thing that you notice in a lot of these reports is the statement that the discovery of this structure violates Einstein's theory of gravity, which is nonsense. This is sloppy reporting, sure, but the RAS press release is also partly to blame here, since it includes a somewhat gratuitous mention of Einstein, and this is exactly the kind of thing that non-expert journalists are likely to pick up on. Mentioning Einstein probably helps generate more traffic after all, which is why I've put him in the title as well.

But aside from the name-dropping, what about the main point about the violation of the cosmological principle? As a quick reminder, the cosmological principle is sometimes taken to be the assumption that, on large scales, the Universe is well-described as homogeneous and isotropic.

The question of what constitutes "large scales" is sometimes not very well-defined: we know that on the scale of the Solar System the matter distribution is very definitely not homogeneous, and we believe that on the scale of size of the observable Universe it is. Generally speaking, people assume that on scales larger than about $100$ Megaparsecs, homogeneity is a fair assumption. A paper by Yadav, Bagla and Khandai from 2010 showed that if the standard $\Lambda$CDM cosmological model is correct, the scale of homogeneity

*must be less than*at most $370$ Mpc.
On the other hand, this quasar structure that Clowes et al. found is absolutely enormous: over 4 billion light years, or more than 1000 Mpc, long. Does the existence of such a large structure mean that the Universe is not homogeneous, the cosmological principle is not true, and the foundation on which all of modern cosmology is based is shaky?

Well actually, no.

Unfortunately Clowes' paper is wrong, on several counts. In fact, I have recently published a paper myself (journal version here, free arXiv version here) which points out that it is wrong. And, on the principle that if I don't talk about my own work, no one else will, I'm going to try explaining some of the ideas involved here.

The first reason it is wrong is something that a lot of people who should know better don't seem to realise: there is no reason that structures should not exist which are larger than the homogeneity scale of $\Lambda$CDM. You may think that this doesn't make sense, because homogeneity precludes the existence of structures, so no structure can be larger than the homogeneity scale. Nevertheless, it does and they can.

Let me explain a little more. The point here is that the Universe is

*not*homogeneous, at any scale. What is homogeneous and isotropic is simply the background model we use the describe its behaviour. In the real Universe, there are always fluctuations away from homogeneity at all scales – in fact the theory of inflation basically guarantees this, since the power spectrum of potential fluctuations is close to scale-invariant. The assumption that all cosmological theory really rests on is that these fluctuations can be treated as perturbations about a homogeneous background – so that a perturbation theory approach to cosmology is valid.
Given this knowledge that the Universe is never exactly homogeneous, the question of what the "homogeneity scale" actually means, and how to define it, takes on a different light. (Before you ask, yes it is still a useful concept!) One possible way to define it is as that scale above which density fluctuations $\delta$ generally become small compared to the homogeneous background density. In technical terms, this means the scale at which the two-point correlation function for the fluctuations, $\xi(r)$, (of which the power spectrum $P(k)$ is the Fourier transform) becomes less than $1$. Based on this definition, the homogeneity scale would be around $10$ Mpc.

It turns out that this definition, and the direct measurement of $\xi(r)$ itself, is not very good for determining whether or not the Universe is a fractal, which is a question that several researchers decided was an important one to answer a few years ago. This question can instead be answered by a different analysis, which I explained once before here: essentially, given a catalogue with the positions of many galaxies (or quasars, or whatever), draw a sphere of radius $R$ around each galaxy, and count how many other galaxies lie within this sphere, and how this number changes with $R$. The scale above which the average of this number for all galaxies starts scaling as the cube of the radius, $$N(<R)\propto R^3,$$ (within measurement error) is then the homogeneity scale (if it starts scaling as some other constant power of $R$, the Universe has a fractal nature). This is the definition of the homogeneity scale used by Yadav

*et al*. and it is related to an integral of $\xi(r)$; typically measurements of the homogeneity scale using this definition come up with values of around $100-150$ Mpc.The figure that proves that the distribution of quasars is in fact homogeneous on the expected scales. For details, see arXiv:1306.1700. |

To get back to the original point, neither of these definitions of the homogeneity scale makes any claim about the existence of structures that are larger than that. In fact, in the $\Lambda$CDM model, the correlation function for matter density fluctuations is expected to be small but positive out to scales larger than either of the two homogeneity scales defined above (though not as large as Yadav

The second reason that the claim by Clowes

*et al*.'s generous upper limit). The correlation function that can actually be measured using any given population of galaxies or quasars will extend out even further. So*we already expect*correlations to exist beyond the homogeneity scale – this means that, for some definitions of what constitutes a "structure", we*expect*to see large "structures" on these scales too.The second reason that the claim by Clowes

*et al.*is wrong is however less subtle. Given the particular definition of a "structure" they use, one would expect to find very large structures even if density correlations were exactly zero on*all*scales.
Yes, you read that right. It's worth going over how they define a "structure", just to make this absolutely clear. About the position of each quasar in the catalogue they draw a sphere of radius $L$. If any other quasars at all happen to lie within this sphere, they are classified as part of the same "structure", which can now be extended in other directions by repeating the procedure about each of the newly added member quasars. After repeating this procedure over all $18,722$ quasars in the catalogue, the largest such group of quasars identified becomes the "largest structure in the Universe".

It should be pretty obvious now that the radius $L$ chosen for these spheres, while chosen rather arbitrarily, is crucial to the end result. If it is too large, all quasars in the catalogue end up classified as part of the same truly ginormous "structure", but this is not very helpful. This is known as "percolation" and the critical percolation threshold has been thoroughly studied for Poisson point sets – which are by definition random distributions of points with no correlation at all. The value of $L$ that Clowes

*et al.*chose to use, for no apparent reason other than that it gave them a dramatic result, was $100$ Mpc – far too large to be justified on any theoretical grounds, but slightly lower than the critical percolation threshold would be if the quasar distribution was similar to that of a Poisson set. On the other hand, the "largest structure in the Universe" only consists of $73$ quasars out of $18,722$, so it could be entirely explained as a result of the poor definition ...
Now I'll spare you all the details of how to test whether, using this definition of a "structure", one would expect to find "structures" extending over more than $1000$ Mpc in length or with more than $73$ members or whatever, even in a purely random distribution of points, which are by definition homogeneous. Suffice it to say that it turns out one would. This plot shows the maximum extent of such "structures" found in $10,000$ simulations of completely uncorrelated distributions of points, compared to the maximum extent of the "structure" found in the real quasar catalogue.

To summarise then: finding a "structure" larger than the homogeneity scale does not violate the cosmological principle, because of correlations; on top of that, the "largest structure in the Universe" is actually not really a "structure" in any meaningful sense. In my professional opinion, Clowes' paper and all the hype surrounding it in the press is nothing more than that – hype. Unfortunately, this is another verification of my maxim that if a paper to do with cosmology is accompanied by a big press release, it is odds-on to turn out to be wrong.

Finally, before I leave the topic, I'll make a comment about the presentation of results by Clowes

The probability distribution of extents of largest "structures" found in 10,000 random point sets for two different choices of $L$. Vertical lines show the actual values found for "structures" in the quasar catalogue. The actual values are not very unusual. Figure from arXiv:1306.1700. |

To summarise then: finding a "structure" larger than the homogeneity scale does not violate the cosmological principle, because of correlations; on top of that, the "largest structure in the Universe" is actually not really a "structure" in any meaningful sense. In my professional opinion, Clowes' paper and all the hype surrounding it in the press is nothing more than that – hype. Unfortunately, this is another verification of my maxim that if a paper to do with cosmology is accompanied by a big press release, it is odds-on to turn out to be wrong.

Finally, before I leave the topic, I'll make a comment about the presentation of results by Clowes

*et al*. Here, for instance, is an image they presented showing their "structure", which they call the 'Huge-LQG', with a second "structure" called the 'CCLQG' towards the bottom left:3D representation of the Huge-LQG and CCLQG. From arXiv:1211.6256. |

Looks impressive! Until you start digging a bit deeper, anyway. Firstly, they've only shown the quasars that form part of the "structure", not all the others around it. Secondly, they've drawn enormous spheres (of radius $33$ Mpc) at the position of each quasar to make it look more dramatic. In actual fact the quasars are way smaller than that. The combined effect of these two presentational choices is to make the 'Huge-LQG' look far more plausible as a structure than it really is. Here's a representation of the exact same region of space that I made myself, which rectifies both problems:

Quasar positions around the "structures" claimed by Clowes et al. |

Do you still see the "structures"?

Aside from the fact that the edges of your rectangular prism keep trying to look like an Escher painting to me, that last figure is pretty damned convincing. I've always wondered what the figure above it would look like if all the quasars were included.

ReplyDeleteOf course the more mathematically convincing figures are the red and blue curves third to last in the post and they're equally convincing.

You should consider submitting this post to 2013 scientific writing competitions. Or, at least, not be surprised when I do.

You're bound to do well, you have Einstein your title!

homogeneity is not testable

ReplyDeletethis gets into the issue of coordinate systems (to which homogeneity scales can be considered equivalent) ... they are merely temporal exercises and if there was a Big Bang then no coordinate system existed before it and any coordinate system self-created as the universe expanded

Most of your comment doesn't make sense to me. However – in a constructive spirit – let me pick up on the word "temporal".

DeleteSince looking at things that are further away also means seeing them as they were at an earlier time, the furthest quasars are much younger than the closer quasars, and so there is in fact a temporal aspect to dealing with the data. In order to claim that the quasars demonstrate that *the Universe* is homogeneous, you then have to make complicated assumptions about old quasars and young quasars being the same kinds of objects – that quasars don't appear or disappear in the time period the dataset spans.

But it is still perfectly possible to test the homogeneity of the quasar distribution itself just as it stands, and it turns out this is homogeneous. All this is done perfectly self-consistently in the comoving coordinate system and the Big Bang or other very-early-Universe physics doesn't come into it.

Thank you! This was a very interesting post - and well-written, too. I'm not an astrophysicist, but I had read about the homogeneity and isotropy of the universe many times in popular science books. As it turns out, I hadn't thought carefully about what those assumptions actually MEAN. I hope, you don't stop blogging.

ReplyDeleteThanks, glad you like it.

DeleteSo, can I ask: which size should have an agglometarion of matter, in order to challenge the cosmological principle?

ReplyDeleteHi anonymous. What do you mean by an agglomeration of matter?

DeleteThe point is this: you tell me how you are going to define "an agglomeration of matter" and then I can tell you how big it must be to challenge the cosmological principle (or any other concepts in cosmology). If you change your definition, I will have to change my answer: there is no one-size-fits-all way to answer this question, because the Universe is always going to have

someinhomogeneities when viewed onanyscale, no matter how large.Einstein's equations view space as having a local

ReplyDeletesmooth density of material on local scales at any

scale, as if it is sort of an aether that is never

separated out or clumped on any scale. It is an

idealization, as are most physics numerical applications.

Anyone is free to try to improve on that, as he was

free to improve on Newton's theories.

I think it would help if you provide illustration of what you think things mean, for example:

ReplyDelete1 - what, in your view, would constitute a minimal violation of the cosmological principle?

2 - How would you define a generic large scale structure?

One other peculiarity is that you appear to be relying on whether a real or imagined structure is obvious to the eye, as a major component of your case. That may not be - but seems to me anyway - ridiculous.

Hello Anonymous. You ask interesting questions.

Delete1 - I'd say that a demonstration that the scaling N(<R) described above did not approach the homogeneous value on large scales would be a good indication of such a violation. The same holds for derivatives of this, such as D2 (which I did not describe here). Alternatively, the discovery of a hypothetical large structure whose existence were shown to be mathematically inconsistent with homogeneity - not simply hand-waving about its apparent 'size' - would be good too.

2 - A definition would be structure that is not consistent with being due simply to random noise fluctuations. This requires a proper calculation of the probability of getting 'structures' in random noise, as I tried to describe above – with lots of additional complications to account for systematic effects due to the telescope sensitivity, masked regions of the sky and so on, if these are important.

You're quite right that if I were relying on a structure being obvious to the eye as a defining criterion, that would be ridiculous. Luckily I'm not – in fact my point is exactly the opposite! I tried to show that whether or not a structure looks obvious to the eye depends on the artistic choices used in making the plots precisely to demonstrate that this is a terrible way of judging things. Instead there are well-defined statistical tests that can be made (and I did make them in my paper). The 'Huge-LQG' does not pass these tests as it is consistent with random fluctuations: it therefore isn't a structure and doesn't violate the Copernican principle.

I hope that helps, and thanks for your interest in this old post.

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