December 17, 2006

This Week's Finds in Mathematical Physics (Week 242)

John Baez

This week I'd like to talk about a paper by Jeffrey Morton. Jeff is a grad student now working with me on topological quantum field theory and higher categories. I've already mentioned his work on categorified algebra and quantum mechanics in "week236". He'll be be finishing his Ph.D. thesis in the spring of 2007 - and as usual, that means he's already busy applying for jobs.

As all you grad students reading this know, applying for jobs is pretty scary the first time around: there are some tricks involved, and nobody prepares you for it. I remember myself, wondering what I'd do if I didn't succeed. Would I have to sell ice cream from one of those trucks that plays a little tune as it drives around the neighborhood? A job in the financial industry seemed scarcely more appealing: less time to think about math, and less ice cream too.

Luckily things worked out for me... and I'm sure they'll work out for Jeff and my other student finishing up this year - Derek Wise, who is working on Cartan geometry and MacDowell-Mansouri gravity.

But, to help them out a bit, I'd like to talk about their work. This has been high on my list of interests for the last few years, of course, but I've mostly been keeping it under wraps.

This time I'll talk about Jeff's thesis; next time Derek's. But first, let's start with some cool astronomy pictures!

Here's a photo of Saturn, Saturn's rings, and its moon Dione, taken by the Cassini orbiter in October last year:

1) NASA, Ringside with Dione, http://solarsystem.nasa.gov/multimedia/display.cfm?IM_ID=4163

It's so vivid it seems like a composite fake, but it's not! With the Sun shining from below, delicate shadows of the B and C rings cover Saturn's northern hemisphere. Dione seems to hover nearby. Actually it's 39,000 kilometers away in this photo. It's 1,200 kilometers in diameter, about the third the size of our Moon.

Here's a photo of Saturn, its rings, and its moon Mimas, taken in November 2004:

2) NASA, Nature's canvas, http://saturn.jpl.nasa.gov/multimedia/images/image-details.cfm?imageID=1088

It's gorgeous, but it takes some work to figure out what's going on!

The blue stuff in the background is Saturn, with lines created by shadows of rings. The bright blue-white stripe near Mimas is sunlight shining through a break in the rings called the "Cassini division". The brownish stuff near the bottom is the A ring - you can see right through it. Above it there's a break and a thinner ring called the F ring. Below it is the Cassini division itself.

This is just one of many photos taken by Cassini and Huyghens, the probe that Cassini dropped onto Saturn's moon Titan - see "week210" for more on that. You can see more of these photos here:

3) NASA, Cassini-Huygens, http://saturn.jpl.nasa.gov/

I hope you see from these beautiful images, and others on This Week's Finds, that we are already in space. We don't need people up there for us to effectively be there.

Alas, not everyone recognizes this. An expensive American program to set up a base on the Moon, perhaps as a stepping stone to a manned mission to Mars, is starting to drain money from more exciting unmanned missions. NASA guesses this program will cost $104 billion up to the time when we land on the Moon - again - in 2020. By 2024, the Government Accounting Office guesses the price will be $230 billion. By comparison, the Cassini-Huygens mission cost just about $3.3 billion.

And what will be benefits of a Moon base be? It's unclear: at best, some vague dream of "space colonization".

Mind you, I'm in favor of space exploration, and even colonization. But, these are very different things!

Colonies are usually about making money. Governments support them in hopes of turning a profit: think Columbus and Isabella, or other adventurers funded by colonial powers.

Right now most of the money lies in near-earth orbit, not on the Moon and Mars. Telecommunication satellites and satellite photos are established businesses. The next step may be tourism. Dennis Tito, Gregory Olsen and Mark Shuttleworth have already paid the Russian government $20 million each to visit the International Space Station. This orbits at an altitude of about 350 kilometers, in the upper "thermosphere" - the layer of the Earth's atmosphere where gases get ionized by solar radiation.

If this is too pricey for you, wait a few years. Richard Branson's company Virgin Galactic plans to give 500 people per year a 7-minute experience of weightlessness at a cost of just $200,000 each. Alas, you'll only go up 100 kilometers, near the bottom of the thermosphere.

Some competition may lower the price. Jeff Bezos, the founder of Amazon, has bought a lot of land in Texas to a build space port for his company Blue Origins. He wants to do test flights by next year, and he eventually wants 50 flights a year in a vehicle that holds 3. If you've always looked forward to using your seat cushion as a flotation device in the event of a water landing, you'll love this:

"During an abort situation, the crew capsule would separate, using small solid-rocket motors to safely recover the space flight participants. The abort module containing the solid-rocket motors would then jettison from the crew capsule."
None of this stuff requires any taxpayer funding. It's a bit self-indulgent and silly, but it may eventually grow and merge with other profit-making forms of space colonization.

Exploration is a bit different: seeing what's out there, mainly for the sake of adventure and understanding. For this we should send machines, not people. Machines can be designed to do well in vacuum. People can't - not yet. This will probably change when nanotech, AI and cyborg technologies kick in. But for now, unmanned probes are the way to go.

Here are some of the wonderful things we could do, all for less than setting up a Moon base:

4) The Laser Interferometer Space Antenna (LISA), http://saturn.jpl.nasa.gov/

The idea of LISA is to put 3 satellites in a huge equilateral triangle following the Earth in its orbit around the Sun, and bounce lasers between them to detect gravitational waves (see "week143"):

This would avoid the ground noise that plagues LIGO (see "week241"), and it could detect waves of much lower frequencies. If all works well, it could see gravitational waves from the very early Universe, long before the hot gas enough cooled to let light through. We're talking times like 10-38 seconds after the Big Bang! That's the biggest adventure I can imagine... back to the birth pangs of the Universe.

Right now LISA is scheduled for launch around 2016. But as you'll soon see, this may not happen.

5) Constellation-X, http://constellation.gsfc.nasa.gov

This would be a team of X-ray telescopes, combining forces to be 100 times more powerful than any previous single one. Among many other things, Constellation-X could study the X-rays emitted by matter falling into things that look like black holes. The redshift of these X-rays is our best test of general relativity for very strong gravitational fields. So, it's our best way of checking that these black hole candidates really do have event horizons!

In February 2006, when NASA put out their latest budget, they said Constellation-X would be "delayed indefinitely". And in September 2006, a National Research Council committee was formed to pick one of NASA's five "Beyond Einstein" programs for the first shot at funding: LISA, Constellation-X, the Joint Dark Energy Mission, the Inflation Probe and the Black Hole Finder. Currently the Joint Dark Energy Mission seems to be in the lead:

6) Steinn Sigurðsson, NASA: double down on science, Dynamics of Cats, September 16, 2006, http://scienceblogs.com/catdynamics/2006/09/nasa_double_down_on_science.php

A decision is expected around September 2007.

7) The Terrestrial Planet Finder (TPF), http://planetquest.jpl.nasa.gov/TPF/

This could study Earth-like planets orbiting stars up to 45 light years away. It would consist of two observatories: a visible-light "coronagraph" that blocks out the light from a star so it can see nearby fainter objects:


and an infrared interferometer made of several units flying in formation:


In February 2006, NASA halted work on the TPF. In June 2006, thanks to public pressure, Congress reinstated funding for this program and also a mission to Jupiter's moon Europa, which could have oceans underneath its icy crust. However, at last report, NASA was continuing to fight against reinstating these missions:

8) Louis D. Friedman, Congressional inaction leaves science still devastated, The Planetary Society, November 26, 2006, http://planetary.org/programs/projects/sos/20061122.html

The constantly shifting situation makes it hard to know what's going on.

9) The Nuclear Spectroscopic Telescope Array (NuStar), http://www.nustar.caltech.edu/

This is an orbiting observatory with three telescopes, designed to see hard X-rays. It could conduct a thorough survey of black hole candidates throughout the universe. It could study relativistic jets of particles from the cores of active galaxies (which are probably also black holes). And, it could study young supernova remnants - hot new neutron stars.

NASA suddenly canceled work on NuStar in February 2006.

10) Dawn, http://dawn.jpl.nasa.gov/

The Dawn mission seeks to understand the early Solar System by probing the asteroid belt and taking a good look at Ceres and Vesta. Ceres is the largest asteroid of all, 950 kilometers in diameter. It seems have a rocky core, a thick mantle of water ice, and a thin dusty outer crust. Vesta is the second largest, about 530 kilometers in diameter. It's very different from Ceres: it's not round, and it's all rock. A certain group of stony meteorites called "HED meteorites" are believed to be pieces of Vesta!

NASA cancelled the Dawn mission in March 2006 - but later that month, they changed their minds.

It's depressing to contemplate all the wonderful things we could miss while spending hundreds of billions to "send canned primates to Mars", as Charles Stross so cleverly put it in his novel "Accelerando" (see "week222"). I'm all for humanity spreading through space. I just don't think we should do it in a clunky, low-tech way like setting up a base on the Moon where astronauts sit around and... what, play golf? It's like something out of old science fiction!

To cheer myself up again, here's a picture of the Sun:

11) Joanne Hewett, Sun Shots, http://cosmicvariance.com/2006/10/13/sun-shots/

It was taken not with light, but with neutrinos. It was made at the big neutrino observatory in Japan, called Super-Kamiokande. It took about 504 days and nights to make.

That's right - nights! Neutrinos go right through the Earth.

As you probably know, neutrinos oscillate between three different kinds, but only electron neutrinos are easy to detect, so we see about third as many neutrinos from the Sun as naively expected. That's the kind of thing they're studying at Super-Kamiokande.

But what I want to know is: what's the "glare" in this picture? Neutrinos are made by the process of fusion, which involves this reaction:

proton + electron → neutron + electron neutrino

Fusion mostly happens in the Sun's core, which has a density of 160 grams per cubic centimeter (10 times denser than lead) and a temperature of 15 million kelvin (300 thousand times hotter than the "broil" setting on an American oven).

So, what's the disk in this picture: the whole Sun, or the Sun's core? And what's the glare?

Okay, now for some serious mathematical physics:

12) Jeffrey Morton, A double bicategory of cobordisms with corners, available as math.CT/0611930v1.

People have been talking a long time about topological quantum field theory and higher categories. The idea is that categories, 2-categories, 3-categories and the like can describe how manifolds can be chopped into little pieces - or more precisely, how these little pieces can be glued together to form manifolds. Then the problem of doing quantum field theory on some manifold can be reduced to the problem of doing it on these pieces and gluing the results together. This works easiest if the theory is "topological", not requiring a background metric.

There's a lot of evidence that this is a good idea, but getting the details straight has proved tough, even at the 2-category level. This is what Morton does, in a rather clever way. Very roughly, his idea is to use something I'll call a "weak double category", and prove that these:

give a weak double category called nCob2. The proof is a cool mix of topology and higher category theory. He then shows that this particular weak double category can be reinterpreted as something a bit more familiar - a "weak 2-category".

In the rest of his thesis, Jeff will use this formalism to construct some examples of "extended TQFTs", which are roughly maps of weak 2-categories

Z: nCob2 → 2Vect

where 2Vect is the weak 2-category of "2-vector spaces". He's focusing on some extended TQFTs called the Dijkgraaf-Witten models, coming from finite groups.

But, he's also thought about the case where the finite group is replaced by a compact Lie group. In this case we get something called BF theory, which is a lot like an extended TQFT, but not quite, because there are some divergences (infinities) that arise. In this case of 3d spacetime with the Lie group SU(2), BF theory gives a nice theory of quantum gravity called the Ponzano-Regge model. And, as I hinted back in "week232", we can let 2d space in this model be a manifold with boundary by poking little holes in space. Then these holes wind up acting like particles!

So, we get a relation like this:

 (n-2)-dimensional manifolds                     MATTER

 (n-1)-dimensional manifolds with boundary       SPACE

  n-dimensional manifolds with corners           SPACETIME
I like this a lot: it reminds me of the title of Weyl's famous book "Raum, Zeit, Materie", meaning "Space, Time, Matter". He never guessed this trio was related to the objects, morphisms and 2-morphisms in a weak 2-category! It's too bad we can't seem to get something like this to work for full-fledged quantum gravity.

It would be fun to talk more about this. However, to understand Morton's work more deeply, you need to understand a bit about "weak double categories". He explains them quite nicely, but I think I'll spend the rest of this Week's Finds giving a less detailed introduction, just to get you warmed up.

This chart should help:

                                   BIGONS                SQUARES

   LAWS HOLDING                    strict                strict 
   AS EQUATIONS                 2-categories        double categories

   LAWS HOLDING                    weak                  weak
 UP TO ISOMORPHISM              2-categories        double categories
2-categories are good for describing how to glue together 2-dimensional things that, at least in some abstract sense, are shaped like bigons. A "bigon" is a disc with its boundary divided into two halves. Here's my feeble ASCCI rendition of a bigon:
                      f 
                   --->---
                  /       \
                 /   ||    \
              X o    ||B    o Y
                 \   \/    /
                  \       /
                   --->---
                      g
                     
The big arrow indicates that we think of the bigon B as "going from" the top semicircle, f, to the bottom semicircle, g. Similarly, we think of the arcs f and g as going from the point X to the point Y.

Similarly, double categories are good for describing how to glue together 2-dimensional gadgets that are shaped like squares:

                      f
               X o---->----o X'
                 |         |
               g v    S    v g'
                 |         |
               Y o---->----o Y' 
                      f'
Both 2-categories and double categories come in "strict" and "weak" versions. The strict versions have operations satisfying a bunch of laws "on the nose", as equations. In the weak versions, these laws hold up to isomorphism whenever possible.

A few more details might help....

A 2-category has a set of objects, a set of morphisms f: X → Y going from any object X to to any object Y, and a set of 2-morphisms T: f => g going from any morphism f: X → Y to any morphism g: X → Y. We can visualize the objects as dots:

                   o 
                   X
the morphisms as arrows:
                   f           
            X o---->----o Y
and the 2-morphisms as bigons:
                   f 
                --->---
               /       \
              /   ||    \
           X o    ||B   o Y
              \   \/    /
               \       /
                --->---
                   g
We can compose morphisms like this:
            f         g                                  fg
       o---->----o---->----o             gives       o--->---o
       X         Y         Z                         X       Z
We can also compose 2-morphisms vertically:
                 f                                          f
             ---->----                                 --->---  
            /  S      \                               /       \
           /     g     \                             /         \
        X o ----->----- o Y              gives    X o     ST    o Y
           \   T       /                             \         /
            \         /                               \       /   
             ---->----                                 --->---
                 h                                        h
and horizontally:
             f           f'                              ff'
          --->---     --->---                          --->--- 
         /       \   /       \                        /       \
        /         \ /         \                      /         \
     X o     S     o     T     o Z       gives    X o    S.T    o Z
        \         / \         /                      \         /
         \       /   \       /                        \       / 
          --->---     --->---                          --->---
             g           g'                              gg'
There are also a bunch of laws that need to hold. I don't want to list them; you can find them in Jeff's paper (also see "week80"). I just want to emphasize how a strict 2-category is different from a weak one.

In a strict 2-category, the composition of morphisms is associative on the nose:

(fg)h = f(gh)

and there are identity morphisms that satisfy these laws on the nose:

1f = f = f1

In a weak 2-category, these equations are replaced by 2-isomorphisms - that is, invertible 2-morphisms. And, these 2-isomorphisms need to satisfy new equations of their own!

What about double categories?

Double categories are like 2-categories, but instead of bigons, we have squares.

More precisely, a double category has a set of objects:

                   o 
                   X
a set of horizontal arrows:
                   f           
            X o---->----o X'
a set of vertical arrows:
            X o
              |
            g v
              |
            Y o
and a set of squares:
                f
         X o---->----o X'
           |         |
         g v    S    v g'
           |         |
         Y o---->----o Y' 
                f'
We can compose the horizontal arrows like this:
            f         f'                                  f.f'
       o---->----o---->----o             gives         o--->---o
       X         Y         Z                           X       Z
We can compose the vertical arrows like this:
      X o
        |
      g v                                                X o
        |                                                  |
      Y o                                gives         gg' v
        |                                                  |
     g' v                                                Z o
        |
      Z o
And, we can compose the squares both vertically:
             f
      X o---->----o X'
        |         |                                        f
      g v    S    v g'                              X o---->----o X'
        |         |                                   |         |
      Y o---->----o Y'                  gives     gh  v   SS'   v g'h'
        |         |                                   |         |
      h v    S'   v h'                              Z o---->----o Z'
        |         |                                        f'
      Z o---->----o Z'
             f'
and horizontally:
                f    Y    g                                 f.g
         X o---->----o---->----o Z                    X o---->----o Z
           |         |         |                        |         |
         h v    S    v    S'   v h'                   h v   S.S'  v h'  
           |         |         |                        |         |
        X' o---->----o---->----o Z'                  X' o---->----o Z' 
                f'   Y'   g'                               f'.g'
In a strict double category, both vertical and horizontal composition of morphisms is associative on the nose:

(fg)h = f(gh)

(f.g).h = f.(g.h)

and there are identity morphisms for both vertical and horizontal composition, which satisfy the usual identity laws on the nose.

In a weak double category, we want these laws to hold only up to isomorphism. But, it turns out that this requires us to introduce bigons as well! The reason is fascinating but too subtle to explain here. I didn't understand it until Jeff pointed it out. But, it turns out that Dominic Verity had already introduced the right concept of weak double category - a gadget with both squares and bigons - in his Ph.D. thesis a while back:

13) Dominic Verity, Enriched categories, internal categories, and change of base, Ph.D. dissertation, University of Cambridge, 1992.

Interestingly, if you weaken only the laws for vertical composition, you don't need to introduce bigons. The resulting concept of "horizontally weak double category" has been studied by Grandis and Pare:

14) Marco Grandis and Bob Paré, Limits in double categories, Cah. Top. Geom. Diff. Cat. 40 (1999), 162-220. Also available at http://www.dima.unige.it/~grandis/Dbl.Cahiers.pdf

Marco Grandis and Bob Paré, Adjoints for double categories, Cah. Top. Geom. Diff. Cat. 45 (2004), 193-240. Also available at http://www.dima.unige.it/~grandis/Dbl.Adj.pdf

and more recently by Martin Hyland's student Richard Garner:

15) Richard Garner, Double clubs, available as math.CT/0606733

and Tom Fiore:

16) Thomas M. Fiore, Pseudo algebras and pseudo double categories, available as math.CT./0608760.

At this point I should admit that the terminology in this whole field is a bit of a mess. I've made up simplified terminology for the purposes of this article, but now I should explain how it maps to the terminology most people use:

   ME                                  THEM

strict 2-category                   2-category
weak 2-category                     bicategory
strict double category              double category
weak double category                double bicategory
horizontally weak double category   pseudo double category
Verity used the term "double bicategory" to hint that his gadgets have both squares and bigons, so they're like a blend of double categories and bicategories. It's a slightly unfortunate term, since experts know that a double category is a category object in Cat, but Verity's double bicategories are not bicategory objects in BiCat. Morton mainly uses Verity's double bicategories - but in the proof of his big theorem, he also uses bicategory objects in BiCat.

There's a lot more to say, but I'll stop here and let you read the rest in Jeff's paper!


Addenda: I thank Charlie Clingen for catching some typos in my diagrams, and Nathan Urban and Torbjörn Larsson for helping me update some of my information on the funding of NASA programs. I won't attempt to keep this information up to date, since it's changing too often. But, I'd like to it be correct as of the date I wrote it!

Sean Carroll writes:

Hi John--

Just a couple of comments on This Week's Finds--

You mention a bunch of missions that could "probably" be funded for the cost of a Moon base. That's being quite conservative! Each of those missions is about $1 billion or less, while the Moon base is upwards of $200 billion.

And you asked about the neutrino image of the Sun. The "haze" is just an imaging problem, not a feature of the Sun; the resolution of this image is worse than 10 degrees (I forget the exact number), so we're certainly not looking at any substructure inside the Sun (whose entire disk is only half a degree wide).

Sean

I've deleted the word "probably". According to a comment on Joanne Hewett's blog entry, each pixel in the neutrino picture of the Sun is one degree in size. The Sun itself is just half a degree wide.

For more discussion, go to the n-Category Café.


© 2006 John Baez
baez@math.removethis.ucr.andthis.edu