Also available as http://math.ucr.edu/home/baez/week219.html
July 4, 2005
This Week's Finds in Mathematical Physics - Week 219
John Baez
I'm about to head to Sydney and Canberra to help celebrate the 60th birthday
of Ross Street ... the world's best n-category theorist!
1) Categories in Algebra, Geometry and Mathematical Physics,
conference in honor of Ross Street's 60th birthday,
http://streetfest.maths.mq.edu.au/
Lots of people will be talking about the interface of higher-dimensional
algebra and physics. And a bunch of these will be talking about higher
gauge theory, which generalizes ordinary gauge theory from point particles
to strings, loops, and higher-dimensional "branes" by replacing groups with
n-groups.
Ezra Getzler will be speaking on how to get an n-group from a Lie n-algebra,
and Mikhail Kapranov will be speaking on higher-dimensional holonomies.
Alissa Crans, Danny Stevenson and I will also be talking about this stuff.
There will eventually be a conference proceedings, but for now you can see
the abstracts of people's talks on the website. You can see my talks here:
2) John Baez, Higher gauge theory, http://math.ucr.edu/home/baez/street/
Anyway, before I take off, here's a roundup of stuff I've been meaning to
mention: the centennial of Einstein's "annus mirablis", the Pioneer anomaly,
silicon photonics, a company that plans to sell quantum computers, and some
relationships between Klein's quartic curve, the Fano plane, and special
relativity over the integers mod 7. I want to leave you lots of stuff to
think about. :-)
Okay... let's start with Einstein's "annus mirablis".
1905 was indeed a miraculous year for Albert Einstein. He published four
earth-shaking papers, all in the same journal:
3) Albert Einstein, On a heuristic viewpoint concerning the production and
transformation of light, Annalen der Physik 17 (1905), 132-148. Available
at http://dbserv.ihep.su/~elan/src/einstein05/eng.pdf
On the movement of small particles suspended in stationary liquids required
by the molecular-kinetic theory of heat, Annalen der Physik 17 (1905),
549-560.
On the electrodynamics of moving bodies, Annalen der Physik 17 (1905),
891-921. Available at http://dbserv.ihep.su/~elan/src/einstein05b/eng.pdf
Does the inertia of a body depend upon its energy content?,
Annalen der Physik 18 (1905), 639-641. Available at
http://dbserv.ihep.su/~elan/src/einstein05c/eng.pdf
In the first of these papers, Einstein explained the photoelectric effect by
assuming that light consisted of particles each carrying an energy equal to
Planck's constant times its frequency. This was an important step towards
quantum mechanics - a theory he would later fight against.
In the second, he showed that Brownian motion was explained by the existence
of atoms. His calculations were later used to measure Boltzmann's constant.
In the third, Einstein derived the formula for Lorentz transformations from
two simple assumptions: only relative motion can be detected, and every
unaccelerated observer measures light to have the same speed.
In the fourth, he derived a relation between mass, momentum, and energy,
including as a special case the famous formula E = mc^2 relating the mass
of a body to its energy at rest.
The most impressive thing about these papers is how simple and readable they
are: they go from clearly stated assumptions to world-shaking conclusions
with clear logic and only a little math.
Which makes one wonder: will there ever be another Einstein? Can one person
ever again make such revolutions in physics? Or are all the remaining
discoveries yet to be made in physics too complicated? Why has fundamental
physics been stuck ever since the completion of the Standard Model? There
are lots of glorious theories, but none of them have gotten any experimental
confirmation. There have also been some big empirical discoveries - dark
matter, dark energy, neutrino oscillations, and more - but these weren't
predicted, and our theories still don't shed much light on them.
So, are the times ripe for a good new idea... a really smart person who will
fit the jigsaw puzzle together? Or are there still too many missing pieces?
Lee Smolin has some interesting thoughts about this:
4) Lee Smolin, Why no "new Einsteins"?, Physics Today, June 2005, 56-57.
I think the mention of Einstein is mainly just a trick to get people to
read the article. He focuses on institutional pressures that push physicists
to conform: to follow "research programs" in big teams rather than strike out
on their own.
This is certainly a big problem. But I'm not sure it's the only problem.
Fundamental physics is in a tough situation, partly a victim of its own
success. Pure thought may not be enough. To make real progress, it helps
to have lots of experimental results that don't fit the current theories.
Not just a few numbers here or there, like neutrino masses. We want *piles*
of unexplained data! - enough to draw lots of graphs. Then we could cook up
theories that fit the data.
Barring this, we need to assemble all the mysteries we can get our hands on,
and see if they fit together somehow.
Luckily, right now several spacecraft are leaving the the Solar System...
and they're leaving us with the best of gifts: a mystery!
Pioneer 10 was launched in 1972. It was the first spacecraft to travel
through the asteroid belt, and the first to take closeups photos of Jupiter
and study the intense magnetic field of this planet. I remember getting
excited about this when I was a kid.
Pioneer 10 was also the first spacecraft to explore the outer solar system.
In 1983 it passed the orbit of Neptune. On February 7th, 2003, Pioneer 10's
radioactive power source weakened to the point where its radio signals became
too feeble to detect. When this happened, it was 80 astronomical units
from the Sun: in other words, 80 times as far from the Sun as we are, or
about twice as far out as Pluto.
But this was just the beginning of its cold dark journey. It will continue
to coast through deep space in the general direction of the red giant
Aldebaran, 68 light years from us. A light year is about 63,000 astronomical
units, so this journey will take a while: over 2 million years! We'll
probably be long gone by then, for better or worse.
Pioneer 11 was launched in 1973. It followed its sister ship to Jupiter, then
swung past Saturn, and then sailed out into the night, studying the solar wind
as it went. On September 30, 1995 its power source became too weak to run
any more experiments, and NASA stopped monitoring it. It was 45 astronomical
units from the Sun, moving out at 2 AU per year.
We are no longer in the beam of its radio signal. Its antenna cannot be
rotated. It is heading towards Aquila - the Eagle - and it will pass one
of the stars in this constellation in 4 million years.
Here's a picture of what these spacecraft are doing:
5) NASA, Pioneer path,
http://spaceprojects.arc.nasa.gov/Space_Projects/pioneer/path.html
See how they'll eventually pass through a bubble called the "termination
shock"? That's where the solar wind drops below supersonic speed as it
crashes into the gas of the Milky Way. You can see a pattern vaguely
reminscient of the wave formed by a boat sailing through the sea - that's
because we're moving through the Milky Way.
There are also two other spacecraft in this picture: Voyager 1 and 2! These
craft are still transmitting, and Voyager 1 is now farther than Pioneer 10.
It crossed the termination shock in December 2004, zipping along at 3.6 AU
per year. It's sending back information about this region of space - called
the "heliosheath" - and its batteries should be good until 2020.
But what's the mystery?
Well, the Pioneer missions yielded the most precise information we have about
navigation in deep space. However, analysis of their radio tracking data
indicates a small unexplained acceleration towards the Sun! The magnitude of
this acceleration is roughly 10^{-9} meters per second per second. It's
called the "Pioneer anomaly".
This anomaly has also been seen in the Ulysses spacecraft, and possibly
also in the Galileo spacecraft, though the data is much more noisy, since
these were Jupiter probes, hence much closer to the Sun, where there is a
lot more pressure from solar radiation. The Voyagers are not set up to
provide good data on this issue, since they are able to rotate themselves
and this messes things up. The Viking mission to Mars did *not* detect
the Pioneer anomaly - and it would have, had an acceleration of this
magnitude been present, because its radio tracking was incredibly accurate -
good to about 12 meters.
Many physicists and astronomers have tried to explain the Pioneer anomaly
using conventional physics, but so far nobody seems to have succeeded.
Radiation pressure from the Sun, the solar wind, the back-reaction from the
radio emissions: all these point the wrong way! Other explanations also
seem to fail, like gravity from the Kuiper belt, small amounts of gas venting
from the spacecraft, and thermal radiation from the craft,
As conventional explanations seemed to fail, people started trying to
explain the anomaly using new physics - for example, modified theories of
gravity, or dark matter. But it's hard to get these explanations to work,
either. For example, explaining the Pioneer anomaly by the gravitational
attraction of dark matter would require more than .0003 solar masses of
dark matter within 50 AU units of the Sun. But this is in conflict with
our highly successful calculations of planetary orbits - even a millionth
of a solar mass of dark matter in this region would be enough to throw
those off!
So, we may have an interesting clue on our hands.
For more information on the Pioneer anomaly, see these sources and the many
references therein:
6) Wikipedia, Pioneer anomaly, http://en.wikipedia.org/wiki/Pioneer_anomaly
7) Chris P. Duif, Pioneer anomaly - Literature and Links,
http://www.space-time.info/pioneer/pioanomlit.html
I got interested in the Pioneer anomaly when I read this recent proposal
for a mission to study it:
8) The Pioneer Collaboration, A mission to explore the Pioneer anomaly,
available as gr-qc/0506139
Finally, here's a fun book on the Pioneer missions:
9) Mark Wolverton, The Depths of Space: The Story of the Pioneer Planetary
Probes, Joseph Henry Press, 2004. Available at
http://www.nap.edu/books/0309090504/html/
Next: silicon lasers. I don't want to say much about these, just that Intel
thinks they could be the next big thing. You've probably heard about "Moore's
Law", how the number of components in an integrated circuit doubles every 2
years. Or more vaguely: how computers keeping getting more powerful, really
fast! And you've probably heard that this exponential growth is in danger of
running into a brick wall someday. One of the problems is that copper wire
carries too little data, too slowly.
For a long time some people have touted "photonics" as the way around this:
transmitting information as pulses of light, rather than clumps of electrons.
One problem is that substances that emit such pulses tend to be expensive,
like gallium arsenide and indium phosphide. But now they've figured out to
make silicon function as a laser! Researchers at Intel have created a silicon
laser that emits a continuous beam of light. They've also developed a
modulator that chops the beam into 10 billion pulses per second - a 10
gigahertz signal.
For details, try this:
10) Intel, Silicon photonics, http://www.intel.com/technology/silicon/sp/
11) Robert Service, Intel's breakthrough, Technology Review, July 2005,
62-65. Also available at
http://www.technologyreview.com/articles/05/07/issue/feature_intel.asp
While we're talking about high tech, how about quantum computers? Most of
them don't work very well - yet, say the optimists. Interaction with the
environment ruins the coherence of the quantum state. But there's a company
called D-Wave Systems that aims to build a different breed of quantum
computer - one that doesn't mind a fair amount of noise. It's an analog
chip made of lots of superconductors, which is supposed to quantum tunnel
to a lowest-energy state. The idea is that you can get it to solve lots of
minimization problems this way, like the travelling salesman problem.
I don't see why it'll work better than other analogue computers, or methods
like simulated annealing. It could get stuck when there are lots of
"almost-minima" to sift through... just like glass gets stuck when it tries
to find *its* lowest energy state. Physicists call this "frustration":
the poor glass in your window is "frustrated", trying to crystallize but
unable to decide how to do it. In principle it could do it by quantum
tunnelling, but in practice that takes forever. Why will D-Wave Systems'
computer be better?
By the way, they admit their computer *can't* do cool stuff like rapidly
factor large numbers via Shor's algorithm, the way full-fledged quantum
computers should. True devotees of quantum computation probably wouldn't
even call it a quantum computer! But I'll be happy if it works.
They've certain managed to convince some investors. Here's some more info:
12) Erika Jonietz, Quantum calculation, Technology Review, July 2005, 24-25.
Also available at
http://www.technologyreview.com/articles/05/07/issue/forward_quantum.asp
But enough practical stuff! Now let me say a bit more about the Klein
quartic.
I wrote about this gadget in "week214" and "week215". Simply put, this
is a "Platonic surface": a 3-holed torus tiled by regular heptagons, with 3
heptagons meeting at each vertex.
It's perfectly symmetrical, but you can't stuff it into 3-dimensional
Euclidean space without warping it. So, its charms are a bit more esoteric
than those of, say, a dodecahedron.
Of course, this is the kind of challenge that some people just can't resist.
Mike Stay and Gerard Westendorp bravely tried making paper models of it:
13) Mike Stay, Klein quartic, http://www.cs.auckland.ac.nz/~msta039/klein/
14) Gerard Westendorp, Geometry,
http://www.xs4all.nl/~westy31/Geometry/Geometry.html
Mike wisely stopped just short of the final step, which would create a nasty
crumpled mess. Gerard succeeded in completing the task by switching to
*pastry* instead of paper. Check it out!
There might be a small niche market for Klein quartic birthday cakes... but
computer graphics are probably better if you just want to visualize this
surface instead of actually eat it. About 10 or 12 years ago, Joe Christy
made the following pictures using a program called Geomview, which makes
virtual 3d objects:
15) Joe Christy, Klein quartic pictures:
http://math.ucr.edu/home/baez/pentacontihexahedron.jpg
http://math.ucr.edu/home/baez/pentacontihexahedron2.jpg
http://math.ucr.edu/home/baez/pentacontihexahedron3.jpg
It took about a day on the fastest Linux machine they had at the time. The
advantage of Geomview is that once the virtual object is done, you can
quickly create different views. These pictures show the dual version of
Klein's quartic, which has 7 regular triangles meeting at each quarter.
The funky name "pentacontihexahedron" refers to the fact that there are 56
of these triangles.
While I'm at it, I can't resist showing you another beautiful picture:
16) Joe Christy, Fano plane on Roman surface,
http://math.ucr.edu/home/baez/roman.jpg
The blue thing is called the "Roman surface" because it was discovered
by the mathematician Jakob Steiner while he was visiting Rome. It's a
self-intersecting immersion of the projective plane in 3d space. On it,
the 7 lines of the Fano plane are visible in red, with four of them drawn
as circles.
Mathematically, one nice thing about this picture is that it exhibits the
tetrahedral symmetry of the Fano plane!
You can see all these pictures and much more on my Klein quartic website:
17) John Baez, Klein's quartic curve, http://math.ucr.edu/home/baez/klein.html
You may think I'm digressing, but the relation between Klein's quartic
curve and the Fano plane underlies what I want to talk about today. Greg Egan
and I realized that this relation is just part of a bigger picture involving
special relativity in 3-dimensional spacetime... over the integers mod 7.
Huh?
Well, these days so-called physicists have no shame studying physics in all
sorts of dimensions, but they usually confine themselves to building their
spacetimes out of the real numbers.
That makes sense if they're trying to claim some relevance to real-world
physics, however slight. But mathematically, there's no reason not to
try other number systems, like finite fields, just for the fun of it.
And this sheds new light on the Klein quartic. Why? Because the symmetries
of the Klein quartic and the Fano plane also act as *Lorentz transformations*
in 3 dimensional spacetime if you work using the integers mod 7. This lets
us see the Klein quartic and Fano plane as being closely related to special
relativity in this funny context.
Let's see how this goes.
First, recall that a "field" is a number system where you can add, subtract,
multiply and divide to your hearts content, with all the basic laws holding
that hold for real numbers. A "finite field" is one with finitely many
elements, like the integers mod any prime number p. This example is called
Z/p, or F_p if you really want to emphasize that you're thinking of it as a
field.
So, let's do some 3d special relativity with Z/7, and see what it has to say
about the Klein quartic.
First, some basic stuff about finite fields.
The concepts of "positive" and "negative" make sense in any finite field!
Say a nonzero element of the field is "positive" if it's of the form x^2
and "negative" otherwise. (Number theorists call the positive elements
"quadratic residues", just to intimidate outsiders.)
Then multiplication works nicely:
if you multiply two positive elements you get a positive one;
if you multiply two negative elements you get a positive one;
if you multiply a positive and a negative element you get a negative one.
There are finite fields whose cardinality is any prime power, but if we focus
on those whose cardinality is a prime, namely the fields Z/p, there are three
possibilities: the good, the bad, and the ugly.
GOOD: If the field is Z/p for p = 4n+3 then -1 is negative, so we
can switch the "sign" of a number by multiplying it by -1.
BAD: If the field is Z/p for p = 4n+1 then -1 is positive, so we
can't do this.
In both these cases there are as many positive as negative elements.
Then there's
UGLY: If the field is Z/2 then every element is positive.
Luckily, p = 7 is good. But beware: addition doesn't get along with
positivity very well. In fields like Z/p, *every* element is a sum of
positive elements.
Next, let's ponder the peculiarities of special relativity over
a finite field.
We can define Minkowski spacetime of any dimension over any field F:
it's just F^{n+1} with the quadratic form
x^2 = x_0^2 - x_1^2 - ... - x_n^2
We define O(n,1) to be the group of transformations of F^{n+1} that preserve
the above quadratic form, and define the "Lorentz group" SO(n,1) to be
the subgroup consisting of transformations that also have determinant 1.
As usual, we say that a vector x in Minkowski spacetime is:
timelike if x^2 > 0
lightlike if x^2 = 0
spacelike if x^2 < 0
We define a "ray" to be a line through the origin. We say a ray is
timelike, spacelike or lightlike if any vector on it - hence all! -
is of that type.
The lightlike rays are usually called "light rays", both because it sounds
cool (we went into physics because we liked things like X-rays and rayguns)
and because it's accurate. The light rays going through a given point -
the origin - are precisely like this.
Next, let's ponder the peculiarities of 3-dimensional spacetime.
For any field F, 2x2 matrices with determinant 1 act as Lorentz
transformations of 3d Minkowski spacetime. I touched upon this idea
when discussing Trautman's "Pythagorean spinors" in "week196". Here's
how it works:
We can think of 3d Minkowski spacetime as consisting of all 2x2 matrices
that are equal to their own transpose:
( x_0 + x_1 x_2 )
x = ( )
( x_2 x_0 - x_1 )
since the determinant of such a matrix is just
x^2 = x_0^2 - x_1^2 - x_2^2
In this picture, the group SL(2,F) consisting of 2x2 matrices with
determinant 1 acts as Lorentz transformations:
g: x |-> gxg*
where g* is the transpose of g. So, we get a homomorphism from SL(2,F)
to the 3d Lorentz group:
SL(2,F) -> SO(2,1)
This is two-to-one, since it sends both 1 and -1 to the identity Lorentz
transformation. People typically cure this by defining
PSL(2,F) = SL(2,F)/{+-1}
We then get a one-to-one homomorphism
PSL(2,F) -> SO(2,1)
Alas, this homomorphism is not onto: it's only "half-onto". In the traditional
case where F is the real numbers, its range is just one of the two connected
components of SO(2,1). In the case we're interested in here, where F = Z/7,
the group PSL(2,Z/7) has 168 elements but SO(2,1) has twice as many.
Next, let's bring the hyperbolic plane into the game!
Special relativity in 3 dimensions is closely related to the hyperbolic
plane. The reason is that the set of timelike rays in n-dimensional Minkowski
spacetime forms a copy of hyperbolic (n-1)-space: physicists call this the
"mass hyperboloid". So, for n = 3, we get the hyperbolic plane. This is
most familiar for special relativity based on the real numbers, but the same
idea applies to other fields.
So, let's make some definitions:
the "hyperbolic plane" H+ is the set of timelike rays
in 3d Minkowski spacetime
the "heavenly circle" L is the set of light rays
in 3d Minkowski spacetime
the "hyperbolic cylinder" H- is the set of spacelike rays
in 3d Minkowski spacetime
You may think I'm being silly to call the set of light rays "the heavenly
circle", but in 4-dimensional spacetime the analogous thing is often called
"the heavenly sphere", and we're studying things one dimension down.
Why "heavenly sphere"? Well, when you look at the stars at night, they
seem to be lying on a sphere. That's the heavenly sphere: the set of
light rays entering your eye - the set of directions you can look!
One dimension down, flatlanders get to enjoy the "heavenly circle".
Mathematicians call this the projective line, since it's a line with
one extra point added on.
Now for something fun: points on the hyperbolic plane give lines on the
hyperbolic cylinder and vice versa!
This is basically by definition of "line". We define a "line" in H+ to
consist of all points that are orthogonal to a given point in H-, and
vice versa. Note a point in either of these spaces is really a ray in
Minkowski spacetime, but it makes sense to say that two rays are orthogonal.
This definition isn't arbitrary: it reduces to a standard notion of "line"
in the hyperbolic plane - namely a geodesic - when our field is the real
numbers.
Finally, let's dive into the case we're really interested in:
3-dimensional Minkowski spacetime over F = Z/7.
In this case the positive numbers are 1,2,4, and the negative numbers
are 3,5,6.
It turns out that:
The hyperbolic plane over Z/7, namely H+, has size 21.
The heavenly circle over Z/7, namely L, has size 8.
The hyperbolic cylinder over Z/7, namely H-, has size 28.
So, H+ is a nice finite version of the hyperbolic plane with 21 points and
28 lines! A little calculation shows there are 3 points on each line and
4 lines through each point.
We know that PSL(2,Z/7) acts on everything in sight here: H+, H-, and L.
It also acts on the Fano plane and Klein's quartic curve. So, we can try to
match up various features of 3d special relativity with features in the Fano
plane or Klein's quartic curve!
Greg Egan found the following correspondence:
HYPERBOLIC PLANE OVER Z/7 FANO PLANE
7 triads 7 points
7 antitriads 7 lines
21 points 21 flags
28 lines 28 apartments
As usual with these correspondences, simple things in the Fano plane
correspond to subtle things in the hyperbolic plane, and simple things
in the hyperbolic plane correspond to subtle things in the Fano plane.
First of all, points and lines in the Fano plane correspond to "triads" and
"antitriads" in H+.
Huh?
Well, for starters, a "triad" or "antitriad" is an unordered triple of
orthogonal points in H+.
Huh?
Well, remember that a point in H+ is a timelike ray in 3d Minkowski spacetime.
You can't have three timelike rays that are orthogonal in ordinary special
relativity, but you can over Z/7, because the sum of postive numbers can be
zero, or even negative. For example, these three vectors are timelike and
orthogonal:
(1,0,0), (0,4,2), (0,-2,4)
We call the corresponding triple of rays a "triad", and we get a total of
7 triads by applying elements of PSL(2,Z/7) to it. But, there are triples
of orthogonal timelike rays that aren't among these 7. For example, we get
one from these three vectors:
(1,0,0), (0,2,4), (0,-4,2)
We call the corresponding triple of rays an "antitriad", and we get 7
antitriads by applying elements of PSL(2,Z/7).
Each line in the Fano plane contains 3 points, and each point lies on 3
lines. This incidence relation can also be seen in terms of triads and
antitriads: each triad has nonempty intersection with 3 antitriads, and
each antitriad has nonempty intersection with 3 triads!
We can also go backwards: points and lines in the hyperbolic plane correspond
to "flags" and "apartments" in the Fano plane.
Huh?
Flags and apartments are standard concepts in the theory of "buildings",
which I began to explain in "week186". But, I don't want or need to explain
this general theory here. In the Fano plane, a "flag" consists of a point
lying on a line:
--------x---------
An "apartment" consists of 3 distinct points lying on 3 distinct lines like
this:
\ /
\ /
------x-------x-----
\ /
\ /
\ /
x
/ \
/ \
Each apartment in the Fano plane contains 3 flags, and each flag is contained
in 4 apartments. This incidence can also been seen in terms of points and
lines in the hyperbolic plane: each line contains 3 points, and each point
lies on 4 lines!
So, there's an interesting but complicated relation between hyperbolic
geometry over Z/7 and the Fano plane. How does the Klein quartic curve
fit in? There's more to this side of the story than I've managed to
absorb, so I'll just say a few words - probably more than you want to hear.
For more detail, try my Klein quartic curve webpage.
There are 48 nonzero lightlike vectors in 3d Minkowksi spacetime, but if you
take one of them and apply elements of PSL(2,Z/7) to it, you get an orbit
consisting of only 24. These 24 guys correspond to the 24 heptagons in the
heptagonal tiling of the Klein quartic curve! In other words, PSL(2,Z/7)
acts in precisely the same way.
You may ask what the point of all this stuff is, and the answer is - I'm not
sure yet, except that it's fun! Apparently the coincidence
PSL(2,Z/7) = PSL(3,Z/2)
is the only coincidence among classical groups over finite fields, not
counting the ones we already know over the real numbers. So, it's got to
be good for something! And, I haven't even begun to exploit the fact that
the Klein quartic curve is a quotient space of the real hyperbolic plane:
this has got to be related to the hyperbolic plane over Z/7. So, I think
something interesting should emerge, though I'm not sure what.
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Addendum: Regarding the Pioneer anomaly, the cosmologist Ned Wright writes:
John,
I don't think the obvious possibilities have been ruled out. In this
I disagree with Anderson but that's science at the fringes.
I have a Web page on this at:
http://www.astro.ucla.edu/~wright/PioneerAA.html
Just for the record, that's:
17) Ned Wright, Pioneer anomalous acceleration,
http://www.astro.ucla.edu/~wright/PioneerAA.html
For a contrasting viewpoint see:
18) Slava G. Turyshev, Michael Martin Nieto, and John D. Anderson,
The Pioneer anomaly and its implications, available as gr-qc/0510081.
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Quote of the week:
Space isn't remote at all. It's only an hour's drive away if your car
could go straight upwards. - Sir Fred Hoyle
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Previous issues of "This Week's Finds" and other expository articles on
mathematics and physics, as well as some of my research papers, can be
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For a table of contents of all the issues of This Week's Finds, try
http://math.ucr.edu/home/baez/twf.html
A simple jumping-off point to the old issues is available at
http://math.ucr.edu/home/baez/twfshort.html
If you just want the latest issue, go to
http://math.ucr.edu/home/baez/this.week.html