Archive for the The Universe and Stuff Category

First Light from Planck!

Posted in The Universe and Stuff with tags , , , on September 17, 2009 by telescoper

Credit to Andrew Jaffe for alerting me to the fact that ESA’s first press release concerning Planck has now been, well, released…

I last blogged about Planck when it had reached its orbit around L2 and cooled down to its working temperature of 100 milliKelvin. Over the ensuing weeks it has been tested and calibrated, prodded and poked (electronically of course) and generally tuned up. More recently it has completed a “mini-survey” to check that it’s all working as planned.

The way Planck scans means that it takes about six months to cover the whole sky, which is much longer than the two-week period allowed for the mini-survey. This explains the fact that a relatively narrow slice of the celestial sphere has been mapped. However, you can see the foreground emission from the Galactic plane quite clearly. Here is the region shown in the box split into the nine separate frequency channels that Planck observes:

The High Frequency Instrument (HFI) is more sensitive to dust, while the Low Frequency Instrument (LFI) detects more radio emission. It all seems to be working as expected!

And finally here’s a blow up of the smaller square above the Galactic plane shown as seen by  LFI and HFI:

This region is much less prone to foreground emission. The fact that similar structures are seen in the two completely independent receivers shows that the structure is not just instrument noise. In other words, Planck is seeing the cosmic microwave background!

Now Planck will carry out its full survey, scanning the sky for another year or so. There will then be an intense period of data analysis for about another year after which the key science results will be published. Exciting times.

Lessening Anomalies

Posted in Cosmic Anomalies, The Universe and Stuff with tags , , , , , on September 15, 2009 by telescoper

An interesting paper caught my eye on today’s ArXiv and I thought I’d post something here because it relates to an ongoing theme on this blog about the possibility that there might be anomalies in the observed pattern of temperature fluctuations in the cosmic microwave background (CMB). See my other posts here, here, here, here and here for related discussions.

One of the authors of the new paper, John Peacock, is an occasional commenter on this blog. He was also the Chief Inquisitor at my PhD (or rather DPhil) examination, which took place 21 years ago. The four-and-a-half hours of grilling I went through that afternoon reduced me to a gibbering wreck but the examiners obviously felt sorry for me and let me pass anyway. I’m not one to hold a grudge so I’ll resist the temptation to be churlish towards my erstwhile tormentor.

The most recent paper is about the possible  contribution of  the integrated Sachs-Wolfe (ISW) effect to these anomalies. The ISW mechanism generates temperature variations in the CMB because photons travel along a line of sight through a time-varying gravitational potential between the last-scattering surface and the observer. The integrated effect is zero if the potential does not evolve because the energy shift falling into a well exactly balances that involved in climbing out of one. If in transit the well gets a bit deeper, however, there is a net contribution.

The specific thing about the ISW effect that makes it measurable is that the temperature variations it induces should correlate with the pattern of structure in the galaxy distribution, as it is these that generate the potential fluctuations through which CMB photons travel. Francis & Peacock try to assess the ISW contribution using data from the 2MASS all-sky survey of galaxies. This in itself contains important cosmological clues but in the context of this particular question it is a nuisance, like any other foreground contamination, so they subtract it off the maps obtained from the Wilkinson Microwave Anisotropy Probe (WMAP) in an attempt to get a cleaner map of the primordial CMB sky.

The results are shown in the picture below which presents  the lowest order spherical harmonic modes, the quadrupole (left) and octopole (right) for the  ISW component (top) , WMAP data (middle) and at the bottom we have the cleaned CMB sky (i.e. the middle minus the top). The ISW subtraction doesn’t make a huge difference to the visual appearance of the CMB maps but it is enough to substantially reduce to the statistical significance of at least some of the reported anomalies I mentioned above. This reinforces how careful we have to be in analysing the data before jumping to cosmological conclusions.

peacock

There should also be a further contribution from fluctuations beyond the depth of the 2MASS survey (about 0.3 in redshift).  The actual ISW effect could therefore  be significantly larger than this estimate.

Back Early…

Posted in The Universe and Stuff with tags , , , , , on September 11, 2009 by telescoper

As a very quick postscript to my previous post about the amazing performance of Hubble’s spanking new camera, let me just draw attention to a fresh paper on the ArXiv by Rychard Bouwens and collaborators, which discusses the detection of galaxies with redshifts around 8 in the Hubble Ultra Deep Field (shown below in an earlier image) using WFC3/IR observations that reveal galaxies fainter than the previous detection limits.

Amazing. I remember the days when a redshift z=0.5 was a big deal!

To put this in context and to give some idea of its importance, remember that the redshift z is defined in such a way that 1+z is the factor by which the wavelength of light is stretched out by the expansion of the Universe. Thus, a photon from a galaxy at redshift 8 started out on its journey towards us (or, rather, the Hubble Space Telescope) when the Universe was compressed in all directions relative to its present size by a factor of 9. The average density of stuff then was a factor 93=729 larger, so the Universe was a much more crowded place then compared to what it’s like now.

Translating the redshift into a time is trickier because it requires us to know how the expansion rate of the Universe varies with cosmic epoch. The requires solving the equations of a cosmological model or, more realistically for a Friday afternoon, plugging the numbers into Ned Wright’s famous cosmology calculator.

Using the best-estimate parameters for the current concordance cosmology reveals that at redshift 8, the Universe was only about 0.65 billion years old (i.e. light from the distant galaxies seen by HST set out only 650 million years after the Big Bang). Since the current age of the Universe is about 13.7 billion years (according to the same model), this means that the light Hubble detected set out on its journey towards us an astonishing 13 billion years ago.

More importantly for theories of galaxy formation and evolution, this means that at least some galaxies must have formed very early on, relatively speaking, in the first 5% of the time the Universe has been around for until now.

These observations are by no means certain as the redshifts have been determined only approximately using photometric techniques rather than the more accurate spectroscopic methods, but if they’re correct they could be extremely important.

At the very least they provide even stronger motivation for getting on with the next-generation space telescope, JWST.

Atlantes

Posted in Science Politics, The Universe and Stuff with tags , , , , , , on September 10, 2009 by telescoper

I’ve just noticed a  post on another blog about the  meeting of the Herschel ATLAS consortium that’s  going on in Cardiff at the moment, so I thought I’d do a quickie here too. Actually I’ve only just been accepted into the Consortium so quite a lot of the goings-on are quite new to me.

The Herschel ATLAS (or H-ATLAS for short) is the largest open-time key project involving Herschel. It has been awarded 600 hours of observing time  to survey 550 square degrees of sky in 5 wavelenth bands: 110, 170, 250, 350, & 500 microns. It is hoped to detect approximately 250,000 galaxies,  most of them in the nearby Universe, but some will undoubtedly turn out to be very distant, with redshifts of 3 to 4; these are likely to be very interesting for  studies of galaxy evolution.

Herschel is currently in its performance verification (PV) phase, following which there will be a period of science validation (SV). During the latter the ATLAS team will have access to some observational data to have a quick look to see that it’s  behaving as anticipated. It is planned to publish a special issue of the journal Astronomy & Astrophysics next year that will contain key results from the SV phase, although in the case of ATLAS many of these will probably be quite preliminary because only a small part of the survey area will be sampled during the SV time.

Herschel seems to be doing fine, with the possible exception of the HIFI instrument which is currently switched off owing to a fault in its power supply. There is a backup, but the ESA boffins don’t want to switch it back on and risk further complications until they know why it failed in the first place. The problem with HIFI has led to some rejigging of the schedule for calibrating and testing the other two instruments (SPIRE and PACS) but both of these are otherwise doing well.

The data for H-ATLAS proper hasn’t started arriving yet so the meeting here in Cardiff was intended to sort out the preparations, plan who’s going to do what, and sort out some organisational issues. With well over a hundred members, this project has to think seriously about quite a lot of administrative and logistical matters.

One of the things that struck me as particular difficult is the issue of authorship of science papers. In observational astronomy and cosmology we’re now getting used to the situation that has prevailed in experimental particle physics for some time, namely that even short papers have author lists running into the hundreds. Theorists like me usually work in teams too, but our author lists are, generally speaking, much shorter. In fact I don’t have any publications  yet with more than six or seven authors; mine are often just by me and a PhD student or postdoc.

In a big consortium, the big issue is not so much who to include, but how to give appropriate credit to the different levels of contribution. Those senior scientists who organized and managed the survey are clearly key to its success, but so also are those who work at the coalface and are probably much more junior. In between there are individuals who supply bits and pieces of specialist software or extra comparison data. Nobody can pretend that everyone in a list of 100 authors has made an identical contribution, but how can you measure the differences and how can you indicate them on a publication? Or  shouldn’t you try?

Some suggest that author lists should always be alphabetical, which is fine if you’re “Aarseth” but not if you’re “Zel’dovich”. This policy would, however, benefit “al”, a prolific collaborator who never seems to make it as first author..

When astronomers write grant applications for STFC one of the pieces of information they have to include is a table summarising their publication statistics. The total number of papers written has  to be given, as well as the number in which the applicant  is  the first author on the list,  the implicit assumption being that first authors did more work than the others or that first authors were “leading” the work in some sense.

Since I have a permanent job and  students and postdocs don’t, I always make junior collaborators  first author by default and only vary that policy if there is a specific reason not to. In most cases they have done the lion’s share of the actual work anyway, but even if this is not the case it is  important for them to have first author papers given the widespread presumption that this is a good thing to have on a CV.

With more than 100 authors, and a large number of  collaborators vying for position, the chances are that junior people will just get buried somewhere down the author list unless there is an active policy to protect their interests.

Of course everyone making a significant contribution to a discovery has to be credited, and the metric that has been used for many years to measure scientific productivity is the numbered of authored publications, but it does seem to me that this system must have reached breaking point when author lists run to several pages!

It was all a lot easier in the good old days when there was no data…

PS. Atlas was a titan who was forced to hold the sky  on his shoulders for all eternity. I hope this isn’t expected of members of the ATLAS consortium, none of who are titans anyway (as far as I can tell). The plural of Atlas is Atlantes, by the way.

Hubble Flash

Posted in The Universe and Stuff with tags , , , , , on September 9, 2009 by telescoper

Just a quick post to point out that brand new “Early Release” images have just appeared following the recent refurbishment of the Hubble Space Telescope.

You can read the accompanying press release here, so I’ll just post this brief description:

These four images are among the first observations made by the new Wide Field Camera 3 aboard the upgraded NASA Hubble Space Telescope.

The image at top left shows NGC 6302, a butterfly-shaped nebula surrounding a dying star. At top right is a picture of a clash among members of a galactic grouping called Stephan’s Quintet. The image at bottom left gives viewers a panoramic portrait of a colorful assortment of 100,000 stars residing in the crowded core of Omega Centauri, a giant globular cluster. At bottom right, an eerie pillar of star birth in the Carina Nebula rises from a sea of greenish-colored clouds.

My own favourite has to be Stephan’s Quintet, but they all look pretty fantastic.

Cosmic Haiku

Posted in Poetry, The Universe and Stuff with tags , , , on September 6, 2009 by telescoper

I haven’t had much time to post today and will probably be too busy next week for anything too substantial, so I thought I’d resort to a bit of audience participation. How about a few Haiku on themes connected to astronomy, cosmology or physics?

Don’t be worried about making the style of your contributions too authentic, just make sure they are 17 syllables in total, and split into three lines of 5, 7 and 5 syllables respectively.

Here’s a few of my own to give you an idea!

Quantum Gravity:
The troublesome double-act
Of Little and Large

Gravity’s waves are
Traceless; which does not mean they
Can never be found

The Big Bang wasn’t
So big, at least not when you
Think in decibels.

Cosmological
Constant and Dark Energy
Are vacuous names

Microwave Background
Photons remember a time
When they were hotter

Isotropic and
Homogeneous metric?
Robertson-Walker

Galaxies evolve
In a complicated way
We don’t understand

Acceleration:
Type Ia Supernovae
Gave us the first clue

Cosmic Inflation
Could have stretched the Universe
And made it flatter

Astrophysicist
Is what I’m told is my Job
Title. Whatever.

Contributions welcome via the comments box. The best one gets a chance to win Bully’s star prize.

Game Theory

Posted in Bad Statistics, Books, Talks and Reviews, The Universe and Stuff with tags , , , on September 5, 2009 by telescoper

Nowadays gambling is generally looked down on as something shady and disreputable, not to be discussed in polite company, or even to be banned altogether. However, the  formulation of the basic laws of probability was almost exclusively inspired by their potential application to games of chance. Once established, these laws found a much wide range of applications in scientific contexts, including my own field of astronomy. I thought I’d illustrate this connection with a couple of examples. You may think that I’m just trying to make excuses for the fact that I also enjoy the odd bet every now and then!

Gambling in various forms has been around for millennia. Sumerian and Assyrian archaeological sites are littered with examples of a certain type of bone, called the astragalus (or talus bone). This is found just above the heel and its shape (in sheep and deer at any rate) is such that when it is tossed in the air it can land in any one of four possible orientations. It can therefore be used to generate “random” outcomes and is in many ways the forerunner of modern six-sided dice. The astragalus is known to have been used for gambling games as early as 3600 BC.

images

Unlike modern dice, which appeared around 2000BC, the astragalus is not symmetrical, giving a different probability of it landing in each orientation. It is not thought that there was a mathematical understanding of how to calculate odds in games involving this object or its more symmetrical successors.

Games of chance also appear to have been commonplace in the time of Christ – Roman soldiers are supposed to have drawn lots at the crucifixion, for example – but there is no evidence of any really formalised understanding of the laws of probability at this time.

Playing cards emerged in China sometime during the tenth century BC and were available in western europe by the 14th Century. This is an interesting development because playing cards can be used for games such as contract Bridge which involve a great deal of pure skill as well as an element of randomness. Perhaps it is this aspect that finally got serious intellectuals (i.e. physicists) excited about probability theory.

The first book on probability that I am aware of was by Gerolamo Cardano. His Liber de Ludo Aleae ( Book on Games of Chance) was published in 1663, but it was written more than a century earlier than this date.  Probability theory really got going in 1654 with a famous correspondence between the two famous mathematicians Blaise Pascal and Pierre de Fermat, sparked off by a gambling addict by the name of Antoine Gombaud, who went by the name of the “Chevalier de Méré” (although he wasn’t actually a nobleman of any sort). The Chevalier de Méré had played a lot of dice games in his time and, although he didn’t have a rigorous mathematical theory of how they worked, he nevertheless felt he had an intuitive  “feel” for what was a good bet and what wasn’t. In particular, he had done very well financially by betting at even money that he would roll at least one six in four rolls of a standard die.

It’s quite an easy matter to use the rules of probability to see why he was successful with this game. The odds  that a single roll of a fair die yields a six is 1/6. The probability that it does not yield a six is therefore 5/6. The probability that four independent rolls produce no sixes at all is (the probability that the first roll is not a six) times (the probability that the second roll is not a six) times (the probability that the third roll is not a six) times (the probability that the fourth roll is not a six). Each of the probabilities involved in this multiplication is 5/6, so the result is (5/6)4 which is 625/1296. But this is the probability of losing. The probability of winning is 1-625/1296 = 671/1296=0.5177, significantly higher than 50%. Sinceyou’re more likely to win than lose, it’s a good bet.

So successful had this game been for de Méré that nobody would bet against him any more, and he had to think of another bet to offer. Using his “feel” for the dice, he reckoned that betting on one or more double-six in twenty-four rolls of a pair of dice at even money should also be a winner. Unfortunately for him, he started to lose heavily on this game and in desperation wrote to his friend Pascal to ask why. This set Pascal wondering, and he in turn started a correspondence about it with Fermat.

This strange turn of events led not only to the beginnings of a general formulation of probability theory, but also to the binomial distribution and the beautiful mathematical construction now known as Pascal’s Triangle.

The full story of this is recounted in the fascinating book shown above, but the immediate upshot for de Méré was that he abandoned this particular game.

To see why, just consider each throw of a pair of dice as a single “event”. There are 36 possible events corresponding to six possible outcomes on each of the dice (6×6=36). The probability of getting a double six in such an event is 1/36 because only one of the 36 events corresponds to two sixes. The probability of not getting a double six is therefore 35/36. The probability that a set of 24 independent fair throws of a pair of dice produces no double-sixes at all is therefore 35/36 multiplied by itself 24 times, or (35/36)24. This is 0.5086, which is slightly higher than 50%. The probability that at least one double-six occurs is therefore 1-0.5086, or 0.4914. Our Chevalier has a less than 50% chance of winning, so an even money bet is not a good idea, unless he plans to use this scheme as a tax dodge.

Both Fermat and Pascal had made important contributions to many diverse aspects of scientific thought in addition to pure mathematics, including physics, the first real astronomer to contribute to the development of probability in the context of gambling was Christiaan Huygens, the man who discovered the rings of Saturn in 1655. Two years after his famous astronomical discovery, he published a book called Calculating in Games of Chance, which introduced the concept of expectation. However, the development of the statistical theory underlying  games and gambling came  with the publication in 1713 of Jakob Bernouilli’s wonderful treatise entitled Ars Conjectandi which did a great deal to establish the general mathematical theory of probability and statistics.

The Inductive Detective

Posted in Bad Statistics, Literature, The Universe and Stuff with tags , , , , , , , on September 4, 2009 by telescoper

I was watching an old episode of Sherlock Holmes last night – from the classic  Granada TV series featuring Jeremy Brett’s brilliant (and splendidly camp) portrayal of the eponymous detective. One of the  things that fascinates me about these and other detective stories is how often they use the word “deduction” to describe the logical methods involved in solving a crime.

As a matter of fact, what Holmes generally uses is not really deduction at all, but inference (a process which is predominantly inductive).

In deductive reasoning, one tries to tease out the logical consequences of a premise; the resulting conclusions are, generally speaking, more specific than the premise. “If these are the general rules, what are the consequences for this particular situation?” is the kind of question one can answer using deduction.

The kind of reasoning of reasoning Holmes employs, however, is essentially opposite to this. The  question being answered is of the form: “From a particular set of observations, what can we infer about the more general circumstances that relating to them?”. The following example from a Study in Scarlet is exactly of this type:

From a drop of water a logician could infer the possibility of an Atlantic or a Niagara without having seen or heard of one or the other.

The word “possibility” makes it clear that no certainty is attached to the actual existence of either the Atlantic or Niagara, but the implication is that observations of (and perhaps experiments on) a single water drop could allow one to infer sufficient of the general properties of water in order to use them to deduce the possible existence of other phenomena. The fundamental process is inductive rather than deductive, although deductions do play a role once general rules have been established.

In the example quoted there is  an inductive step between the water drop and the general physical and chemical properties of water and then a deductive step that shows that these laws could describe the Atlantic Ocean. Deduction involves going from theoretical axioms to observations whereas induction  is the reverse process.

I’m probably labouring this distinction, but the main point of doing so is that a great deal of science is fundamentally inferential and, as a consequence, it entails dealing with inferences (or guesses or conjectures) that are inherently uncertain as to their application to real facts. Dealing with these uncertain aspects requires a more general kind of logic than the  simple Boolean form employed in deductive reasoning. This side of the scientific method is sadly neglected in most approaches to science education.

In physics, the attitude is usually to establish the rules (“the laws of physics”) as axioms (though perhaps giving some experimental justification). Students are then taught to solve problems which generally involve working out particular consequences of these laws. This is all deductive. I’ve got nothing against this as it is what a great deal of theoretical research in physics is actually like, it forms an essential part of the training of an physicist.

However, one of the aims of physics – especially fundamental physics – is to try to establish what the laws of nature actually are from observations of particular outcomes. It would be simplistic to say that this was entirely inductive in character. Sometimes deduction plays an important role in scientific discoveries. For example,  Albert Einstein deduced his Special Theory of Relativity from a postulate that the speed of light was constant for all observers in uniform relative motion. However, the motivation for this entire chain of reasoning arose from previous studies of eletromagnetism which involved a complicated interplay between experiment and theory that eventually led to Maxwell’s equations. Deduction and induction are both involved at some level in a kind of dialectical relationship.

The synthesis of the two approaches requires an evaluation of the evidence the data provides concerning the different theories. This evidence is rarely conclusive, so  a wider range of logical possibilities than “true” or “false” needs to be accommodated. Fortunately, there is a quantitative and logically rigorous way of doing this. It is called Bayesian probability. In this way of reasoning,  the probability (a number between 0 and 1 attached to a hypothesis, model, or anything that can be described as a logical proposition of some sort) represents the extent to which a given set of data supports the given hypothesis.  The calculus of probabilities only reduces to Boolean algebra when the probabilities of all hypothesese involved are either unity (certainly true) or zero (certainly false). In between “true” and “false” there are varying degrees of “uncertain” represented by a number between 0 and 1, i.e. the probability.

Overlooking the importance of inductive reasoning has led to numerous pathological developments that have hindered the growth of science. One example is the widespread and remarkably naive devotion that many scientists have towards the philosophy of the anti-inductivist Karl Popper; his doctrine of falsifiability has led to an unhealthy neglect of  an essential fact of probabilistic reasoning, namely that data can make theories more probable. More generally, the rise of the empiricist philosophical tradition that stems from David Hume (another anti-inductivist) spawned the frequentist conception of probability, with its regrettable legacy of confusion and irrationality.

My own field of cosmology provides the largest-scale illustration of this process in action. Theorists make postulates about the contents of the Universe and the laws that describe it and try to calculate what measurable consequences their ideas might have. Observers make measurements as best they can, but these are inevitably restricted in number and accuracy by technical considerations. Over the years, theoretical cosmologists deductively explored the possible ways Einstein’s General Theory of Relativity could be applied to the cosmos at large. Eventually a family of theoretical models was constructed, each of which could, in principle, describe a universe with the same basic properties as ours. But determining which, if any, of these models applied to the real thing required more detailed data.  For example, observations of the properties of individual galaxies led to the inferred presence of cosmologically important quantities of  dark matter. Inference also played a key role in establishing the existence of dark energy as a major part of the overall energy budget of the Universe. The result is now that we have now arrived at a standard model of cosmology which accounts pretty well for most relevant data.

Nothing is certain, of course, and this model may well turn out to be flawed in important ways. All the best detective stories have twists in which the favoured theory turns out to be wrong. But although the puzzle isn’t exactly solved, we’ve got good reasons for thinking we’re nearer to at least some of the answers than we were 20 years ago.

I think Sherlock Holmes would have approved.

Flame Academy

Posted in Biographical, The Universe and Stuff with tags , , , , , , , on September 2, 2009 by telescoper

I heard on the radio this morning from that nice Mr Cowan that today is the anniversary of the start of the Great Fire of London which burned for four days in 1666. That provides for a bit of delayed synchronicity with yesterday’s post about the dreadful fires in the outskirts of Los Angeles and a similar conflagration in Athens (which now thankfully appears to be under control).

Fires are of course terrifying phenomena, and it must be among most people’s nightmares to be caught in one. The cambridge physicist Steve Gull experienced this at first hand when his boat exploded and caught fire recently. I’ll take this opportunity to wish him a speedy recovery from his injuries.

But frightening as such happenings are, a flame (the visible, light emitting part of a fire) can also be a very beautiful and fascinating spectacle. Flames are stable long-lived phenomena involving combustion in which a “fuel”, often some kind of hydrocarbon, reacts with an oxidizing element which, in the case of natural wildfires at any rate, is usually oxygen. However, along the way, many intermediate radicals are generated and the self-sustaining nature of the flame is maintained by intricate reaction kinetics.

The shape and colour of a flame is determined not just by its temperature but also, in a complicated way, by diffusion, convection and gravity. In a diffusion flame, the fuel and the oxidizing agent diffuse into each other and the rate of diffusion consequently limits the rate at which the flame spreads. Usually combustion takes place only at the edge of the flame: the interior contains unburnt fuel. A candle flame is usually relatively quiescent because the flow of material in it is predominantly laminar. However, at higher speeds you can find turbulent flames, like in the picture below!

Sometimes convection carries some of the combustion products away from the source of the flame. In a candle flame, for example, incomplete combustion forms soot particles which are convected upwards and then incandesce inside the flame giving it a yellow colour. Gravity limits the motion of heavier products away from the source. In a microgravity environment, flames look very different!

All this stuff about flames also gives me the opportunity to mention the great Russian physicist Yakov Borisovich Zel’dovich. To us cosmologists he is best known for his work on the large-scale structure of the Universe, but he only started to work on that subject relatively late in his career during the 1960s.  He in fact began his career as a physical chemist and arguably his greatest contribution to science was that he developed the first completely physically based theory of flame propagation (together with Frank-Kamenetskii). No doubt he used insights gained from this work, together with his studies of detonation and shock waves, in the Soviet nuclear bomb programme in which he was a central figure.

But one thing even Zel’dovich couldn’t explain is why fires are such fascinating things to look at. I remember years ago having a fire in my back garden to get rid of garden rubbish. The more it burned the more things  I wanted to throw on it,  to see how well they would burn rather than to get rid of them. I ended up spending hours finding things to burn, building up a huge inferno, before finally retiring indoors, blackened with soot.

I let the fire die down, but it smouldered for three days.

Consummation

Posted in Music, Poetry, The Universe and Stuff with tags , , on August 27, 2009 by telescoper

Not long ago I put up an item containing a  poem by John Wilmot, Earl of Rochester. Since I’ve been reading a collection which contains poems by another of the metaphysical poets, Thomas Traherne, I thought I’d pick one of his to put up too.

I was also reminded of Traherne’s poetry when John Peacock commented on another recent post because it was he that introduced me to the truly wonderful musical settings of some of Traherne’s poetry made by Gerald Finzi in his cantata Dies Natalis, and pointed me in the direction of the stunning recording of that work made by Wilfred Brown with the English Chamber Orchestra, conducted by Christopher Finzi (son of Gerald). Why Finzi –  and especially that work – is not better known is something I’ll never understand. But that’s another story…

The story of Thomas Traherne’s poetry is strange and fascinating. The son of  a cobbler, he was a devoutly religious man who lived most of his short life (1637-1674) in relative obscurity as a clergyman and theologian. He was a prolific writer of both prose and poetry, but very little of his work was published during his lifetime. Vast number of handwritten manuscripts survived his death, however, and many of these remained in the safekeeping of a local family in his native Herefordshire. However, in 1888 the estate of this family was wound up, sold, and the manuscripts became dispersed. Eventually, in 1897, one set of papers was  accidentally discovered in a bookstall. Traherne’s first volume of verse was published in 1903 and a second collection followed in 1908.

When these poems finally found their way into the literary world they were greeted with astonishment as well as deep appreciation and they were widely  influential: TS Eliot was a great admirer of Traherne, as was Dorothy L Sayers. The timing of their publication probably explains why Finzi’s music teacher, Ernest Farrar, suggested them to his young student; Finzi was born in 1901 and Farrar taught him as a young boy before he was called up for service in the First World War and killed in action in 1918.

Over the years further manuscripts  have also come to light – literally, in one case, because in 1967 another lost Traherne manuscript was found, on fire, in a  rubbish dump and rescued in the nick of time.

Traherne is sometimes described as the last metaphysical poet and, indeed, the last poems in the collection I have been reading are by him. However, it seems to me he might equally be described as the first romantic poet. The themes he tackles – love of nature and loss of childhood innocence – and his visionary, rhapsodic style have as much in common with William Blake and, especially, William Wordsworth as they do with better known metaphysical poets such as John Donne.

Traherne’s most famous poem is probably Shadows in the Water, but I decided to pick a relatively obscure one, primarily because it deals with matters close to the concerns of a cosmologist! The central theme is the inadequacy of human thought processes in finding a true description of reality or, if you like, full intercourse with nature. For the poet, this can only be achieved through God. This is the consummation referred to in the title.

He’s particularly good at capturing  how we tend to gloss over difficulties with our conceptual framework and how we invent things to plug the gaps. I particularly like the lines from the fourth verse “Wherein because we no//Object distinctly find or know,//We sundry things invent,//That may our fancy give content.” Dark matter?

Consummation

The thoughts of men appear
Freely to move within a sphere
Of endless reach; and run
Though in the soul, beyond the sun.
The ground on which they acted be
Is unobserved infinity.

Extended through the sky,
Though here, beyond it far they fly:
Abiding in the mind
An endless liberty they find:
Throughout all spaces can extend,
Nor ever meet or know an end.

They, in their native sphere,
At boundless distances appear:
Eternity can measure;
Its no beginning see with pleasure.
Thus in the mind an endless space
Doth naturally display its face.

Wherein because we no
Object distinctly find or know,
We sundry things invent,
That may our fancy give content;
See points of space beyond the sky,
And in those points see creatures lie;

Spy fishes in the seas,
Conceit them swimming there with ease;
The dolphins and the whales,
Their very fins, their very scales,
As there within the briny deep
Their tails the flowing waters sweep.

Can see the very skies,
As if the same were in our eyes;
The sun, though in the night,
As if it moved within our sight;
One space beyond another still
Discovered; think while ye will.

Which though we don’t descry,
(Much like by night an idle eye,
Not shaded with a lid,
But in a darksome dungeon hid)
At last shall in a glorious day
Be made its objects to display,

And then shall ages be,
Within its wide eternity;
All kingdoms stand
Howe’er remote, yet nigh at hand;
The skies, and what beyond them lie,
Exposed unto every eye.

Nor shall we then invent
Not alter things; but with content
All in their places see,
As doth the glorious deity;
Within the scope of whose great mind,
We all in their true nature find.