2006 Archives
| The
Conformal Tensor and Weyl's Gauge Theory -- Posted by
wostraub on Tuesday, December 19
2006 |
Some time ago I wrote
about Weyl’s conformal tensor. It has some neat properties, but it
usually crops up only in a gravitation/cosmology context, and hardly
ever in differential geometry. But it was in that sense that the
conformal tensor was used by Einstein to get around his primary
objection to Weyl’s 1918 gauge theory, which was that the line element
ds is not invariant with respect to a metric gauge
transformation (also known as a conformal transformation of the metric).
Recall that an infinitesimal local gauge transformation of the metric
gμν → (1 + ε π) gμν regauges the lengths
or magnitudes of vectors under physical transport, where π(x)
is the gauge parameter. Consequently, the line element ds2
= gμν dxμdxν is also regauged in
accordance with ds → ½ ε π ds.
Einstein’s argument was that ds can represent time as well as
distance, so time-independent processes such as the spacings of atomic
spectral lines can be invariant only if the line element is gauge
invariant. Since it is not, Einstein thought Weyl’s theory had to be
wrong.
But later, Einstein took up the problem once more. He felt that ds
could be made gauge invariant if the line element were revised to ds2
= J(x) gμν dxμdxν, where J
is a scalar function of the coordinates whose gauge variation goes like
δ J = -ε π J (that is, J must be of gauge weight -1).
This would cancel out the gauge change in the metric tensor and leave
the line element invariant.
Try as he could, Einstein could not come up with an appropriate scalar.
Finally, he noticed that the Weyl conformal tensor Cαμνβ
was exactly what he needed, for the combination √ Cαμνβ Cαμνβ
is of gauge weight -1 in a Riemannian space.
Unfortunately, the Weyl conformal tensor vanishes in the absence of a
gravitational source, leaving a null line element (ds = 0)
whose gauge invariance is now trivial. Furthermore, the counterpart of
the foregoing expression in a Weyl space is unknown.
What Einstein apparently overlooked is the scale factor from the Weyl
theory itself, which considerably simplifies things. Consider the
integral quantity k ∫ φμ dxμ, where k
is a constant and φμ is the Weyl vector (which he
identified as the electromagnetic four-potential). Under a metric gauge
transformation, the Weyl vector varies in accordance with δ φμ
= λ ε ∂μπ, where λ is another constant.
Gauge-transforming the above integral puts the gradient ∂μπ
under the integral, which is easily integrated. We can now set the Weyl
scale factor to J via J = ek ∫ φμ dxμ,
which, by appropriate selection of the constant k, will have
gauge weight -1.
This seems like a better approach than that provided by the conformal
tensor, because in the absence of the electromagnetic potential φμ
the exponential term is identically 1. Thus, the line element can be
made gauge invariant only in a Weyl space containing a non-zero
electromagnetic field!
I haven’t found any evidence that Weyl resorted to this counterargument
to Einstein’s objection, but by that time Weyl had moved on, anyway. In
1929, Weyl applied the gauge concept to quantum theory, which was a huge
success. One has to assume that he never looked back. |
|
Hermann Weyl and Dimensional Reduction -- Posted by
wostraub on Monday, December 18
2006 |
In his neat little
book The Dawning of Gauge Theory, Dublin physicist Lochlainn
O’Raifeartaigh writes
The procedure by which higher-dimensional systems are
reduced to lower-dimensional ones is called dimensional
reduction. The reason that dimensional reduction is so powerful
from the point of view of gauge theory is that it converts
coordinate transformations in the full space into gauge
transformations in the subspace.
Historically, the most famous example of this statement
comes from Kaluza-Klein theory. In 1919, the German physicist Theodor
Kaluza postulated the existence of a fifth dimension which was
hidden from observation because it was too small to be seen. Kaluza
thought that the electromagnetic four-potential of Maxwell’s
electrodynamics resided in this dimension, but that its effects were
observable only in the more familiar four-dimensional world we humans
reside in.
Kaluza assumed that the true metric tensor gμν(x)
was five-dimensional. Viewed as a 5x5 symmetric matrix, it has a 4x4
subblock representing ordinary four-dimensional spacetime, while the
g0μ "boundary" elements include the potential Aμ
by way of the identifications g0μ = g55Aμ
(μ = 0,1,2,3) and g55 is a constant. Thus, the
four-potential Aμ lives in the fifth dimension.
The potential is brought down into our world via dimensional reduction.
Kaluza took as his action quantity the integral
∫ √ –g R d5x
where the metric determinant g and the Ricci scalar R
are the old familiar ones, but now in five-dimensional form. Using
Kaluza’s above formulas for the g0μ quantities, this
five-dimensional integral can be reduced to four-dimensional form, which
is
∫ √ –g (R – FμνFμν ) d4x
This, amazingly, is the familiar expression for the combined
gravitational-electrodynamic action! (Physicist Ian Lawrie considers
this result a minor miracle. It isn't, because God just made it that
way!) I find it remarkable that Kaluza was able to deduce this way back
in 1920, because the calculation (while straightforward) is not trivial.
(Kaluza excitedly sent his paper to Einstein in 1919 to get a
recommendation for publication. Einstein, though quite impressed, was
nevertheless uncomfortable with a five-dimensional world, and so
suppressed publication until 1921. Kaluza was not particularly happy
about this!)
The Swedish physicist Oskar Klein published a subsequent paper in 1926
that made numerous important improvements to Kaluza’s idea in the
context of the then-emerging quantum theory. Hence the theory's present
Kaluza-Klein moniker.
Interestingly, in 1953 the great Austrian physicist Wolfgang Pauli took
Kaluza-Klein theory one step further -- that is, one dimension further,
to n = 6. This resulted in the very first non-abelian approach
to non-gravitational (particle) physics. Several years later, using a
similar approach, Yang and Mills developed the first consistent theory
for the strong interaction.
You might note that, in accordance with O’Raifeartaigh’s assertion, the
coordinate-invariant form of Kaluza’s five-dimensional action results in
a fully gauge-invariant term (√ -g FμνFμν)
following dimensional reduction, while the original action is not gauge
invariant at all. We got a gauge-invariant term by reducing the
dimension by just one; imagine the possibilities if one started with,
say, an eleven-dimensional action! This is the so-called M-theory
of string physics, which promises great things (but has delivered
nothing to date except beautiful mathematics). Note, however, that
Kaluza-Klein theory, while interesting, eventually lapsed into obscurity
because it did not predict any new observable phenomena – it was just a
pretty theory. String theory is now finding itself in the same boat, and
if the legions of brilliant physicists now grinding away (and maybe
wasting their precious talents) at this theory cannot produce anything
predictive from it (like explaining the magnitudes of the gravitational
and electromagnetic coupling constants), it may also be forgotten.
Did Hermann Weyl play around with dimensional reduction? Did he ever
consider the possibilities of a higher-dimensional gauge theory? I’ve
seen no evidence that he ever did. By dying in 1955, Weyl missed
Yang-Mills and a lot of other neat stuff he would have undoubtedly
contributed to.
Weyl was taken from us too soon. |
|
Louise Brooks: Lulu Forever -- Posted by
wostraub on Saturday, December 16
2006 |
Peter Cowie's new book
Louise Brooks:Lulu Forever is out, and at long last.
Finally we have a large-format book with hundreds of rarely-seen photos,
motion-picture production stills and first-person accounts of 1920s
actress-flapper Louise Brooks, who would have turned 100 years old last
month (she passed away in 1985).
I probably would not care so much for this actress if it were not for
the fact that I first saw her signature film Pandora's Box
(filmed in Germany as Die Büchse der Pandora) as an
impressionable young college student in 1970. At the same time, I was
taking an elective course in literature (very odd for a chemistry
major), where I was also reading Vladimir Nabokov's irreducible
masterpiece Lolita for the first time. It was in Chapter 6 of
the novel that I encountered Monique, Professor Humbert's French
girl-whore, the predecessor of one Ms. Dolores Haze. To me, Louise and
Monique were one and the same at the time, and I have forgotten neither
in all these years.

Of course, as a Christian I have mixed feelings about all this now, but
literature is literature, and life itself isn't squeaky clean. Humbert,
Monique and Lulu all paid dearly for their shortcomings (as did Louise
Brooks), and so I will let it go at that.
Cowie's book can be purchased from
Amazon for about $35. If you're interested, you might also
consider buying
Lolita* which, in my humble opinion, is the third
greatest book ever written (right behind Hamlet and the New
Testament). Exceedingly well-written, hilarious, disturbing and
heart-breaking at the same time, it's all the more amazing that it was
written by a Russian who picked up the English language later in life
(much like Joseph Conrad, who also ranks right up there).
* Five points to the person who figures out the identity of
John Ray, Jr. PhD, credited as co-author of the book |
|
Bombs Bursting in Air -- Posted by
wostraub on Tuesday, December 12
2006 |
Several weeks ago, I
was driving through San Raphael near San Francisco and happened to stop
by Autodesk, the company founded by AutoCAD's creator, John Walker.
Coincidentally, Walker's name popped up on an Internet search with that
of John von Neumann, the great
mathematical
physicist and close friend/colleague of Hermann Weyl (see my
December 9 post). Von Neumann worked on the Manhattan Project, where
(among many other things) he discovered that an atomic bomb would be
much more destructive if detonated high above the target area (something
involving shock wave pressures, which I know nothing about).
It turns out that John Walker is also interested in such things, if only
academically (unlike me, he is extremely wealthy and has even more time
on his hands). He has a
website that explains the effects of nuclear weapons on human
populations, something we should all get familiar with as long as
President Bush is running the world.
Anyway, Walker's site includes print-out materials and instructions for
making a nuclear effects calculator. It's basically a circular
slide rule that will allow you to ponder (in a very quantitative way)
the death and destruction that a nuclear device can have on your least
favorite city (Crawford, Texas, for example). Well, I made one, and it's
very neat. It's one way to personally experience the practical aspects
of the complicated science that folks like von Neumann, Oppenheimer and
Teller turned into godless, immoral sin.

[Note: Optimum burst height = maximum resultant death and
destruction]
Walker warns that his calculator won't be of much use in a post-nuclear
war world. But that may not be that far off -- I'll bet you anything
that one of the alternatives Mr. Bush is considering for the New Way
Forward© in Iraq is to nuke Iran, in which case all bets are
off. |
|
Weyl and von Neumann -- Posted by
wostraub on Saturday, December 9 2006 |
From the recollections
of mathematician Herman Goldstine, friend of Hermann Weyl and the great
mathematical physicist John von Neumann, and (with von Neumann) one of
the developers of the early ENIAC computer:

Hermann Heine Goldstine, 1913-2004
"I always was struck by the difference between Weyl
and Johnny von Neumann. There are jokes, one of which Johnny always
swore was false. That's the story that, I don't know, Hermann Weyl
was going to prove some theorem, a very deep and profound theorem,
let's say it was the Riemann-Roch theorem. I don't know if it was
the Reimann-Roch theorem, but that was one I always have trouble
with, so let's say that was the theorem. And Weyl gave a lecture on
why this is a very deep, profound result, and he gave a very
complicated proof. And the apocryphal story goes that at the end of
the lecture there's this kid who is supposed to have raised his hand
at the back of the class and said, 'Professor Weyl, may I show you a
proof?' And goes up to the board and goes zip, zip, zip, zip, and in
about 15 lines has a brilliant proof of this thing.
"I asked Johnny about it, and he said no, that wasn't true. But it
is true, if you talk to Natasha Brunswick, who was in those days
Natasha Artin. Natasha says that there was always Johnny with these
tight pants on. All of Johnny's life, whatever size suit he bought,
he always ate too much, and the suit was always one size smaller
than Johnny. Even as a student in Göttingen, his behind was always
ready to bulge out of his pants. I guess Natasha and everybody in
the class were always charmed.
"But Joachim, who was one of Hermann's children, told me that when
Hermann used to work in his house on Mercer Street, in the study in
there, you would hear groans coming out of the study. That Weyl
worked at things in sort of anguish, that it was hard for him, that
he delivered his theorems practically like a woman giving birth to a
child. That's so different from Johnny, because when he and I would
be working at something, when we'd get stuck, he'd say, 'Okay,
that's it, ' and pack it up. It might be that he'd phone at two in
the morning to say, 'This is how the proof goes.' But it might be
three weeks, a month or so later, or it might even be I who would
come in a month or so later and say, 'This is, maybe, how to go.'
But he never struggled with something. When he got stuck, he filed
it somehow, and it just came out easily. I suspect that Weyl was
probably the deeper of the two mathematicians."
|
|
Louise Brooks at 100 -- Posted by
wostraub on Sunday, December 3 2006 |
[Follow-up to my
October 17 post.] While visiting San Francisco recently, I stopped by
the city's Main Public Library, which is featuring an exhibit on the
American actress Louise Brooks. Brooks, who passed away in 1985, would
have turned 100 on November 14.

Astonishingly beautiful, Brooks created the movies' "bobbed" hairstyle
look around 1926. I still remember the recollections of my late mother
who, as a lovely teenager herself in the late 1920s, begged and begged
her parents to get her hair bobbed á la Brooks. But as strict
Southern Baptists, such a hairstyle (not to mention even going to the
movies!) was absolutely verboten.
Back from SF, I was happy to have finally received
Criterion Collection's two-disc DVD set of Brooks' early 1929
psycho-sexual drama Pandora's Box, the actress' signature film
(filmed in Berlin by the great German director, Georg Wilhem Pabst).
Regarded as one of the top ten greatest silent movies of all time,
Criterion's digitally remastered version of the Munich Museum's restored
film includes four different musical scores, Lulu in Berlin (a
rare filmed interview with the actress, produced in 1984), Looking
for Lulu (the one-hour, 1998 Hugh Neeley documentary on Brooks'
life), the book Reflections on Pandora's Box, and assorted
essays, audio commentaries, interviews and stills. If you're into this
actress, this is a must-have DVD.

Brooks at age 64, in a rare 1971 interview with British filmmaker/
film essayist (and Harvard physics graduate!) Richard Leacock
Tragically, parental neglect and childhood sexual abuse (at the age of
nine) most likely destroyed Brooks' life, and she went on to become the
same kind of woman she portrayed in Pandora's Box and Diary
of a Lost Girl (also 1929). An ultra-liberal, chain-smoking,
alcoholic, partying sexual abandonee and iconoclastic loner until very
late in life, to her enduring credit she renewed her Catholic roots,
took up writing and turned herself around. She died of emphysema at the
age of 78. May God save her soul.
My candle burns at both ends;
It will not last the night;
But ah, my foes, and oh, my friends--
It gives a lovely light! -- Edna St.
Vincent Millay (1920)
[More pics of the exhibit can be found
here] |
|
Another Hermann -- Posted by
wostraub on Monday, November 27 2006 |
If you’ve read my
articles on Weyl spinors, Dirac’s equation and quantum field theory (or
been bored by them), then you’ve probably wondered why no mention was
made of Grassmann numbers.
In QFT, scalar particles and fields can be described by a path integral
involving infinite-dimensional products (dφ1dφ2dφ3…dφinfinity
) under the integrals. But for fermions (electrons, quarks and the
like), whose fields are actually operators, the fields ψ(x)
obey instead an anticommuting algebra. Thus, ψ1ψ2
= - ψ2ψ1, which needless to say complicates
fermionic QFT. The first thing I thought when I saw this was “well,
matrices and differential operators can anticommute, so these fields are
just matrices or differentials.” No, I was wrong -- there are plain old
ordinary numbers out there that can anticommute. They are called
Grassmann numbers.
Hermann Grassmann was born in Stettin, Germany in 1809. He loved math
and physics, but was also drawn to theology, chemistry, Latin,
philosophy, linguistics and neohumanism, so much so that he ultimately
went on to teach all of these subjects. Amazingly, he never took any
formal classes in mathematics or physics, yet he excelled in these
subjects to the extent that famous mathematicians of the day (including
Möbius and Kummer) considered him their equal. But because he was not
formally educated, Grassmann was not recognized in his day for his
genius.

Grassmann was apparently the first researcher to realize that linear
vector spaces need not be limited to three dimensions. His work on
infinite-dimensional vector spaces predated by many years the work of
Hermann Weyl, Elie Cartan and other mathematicians, but intriguingly it
also provided the mathematical basis for fermionic QFT.
When Einstein tackled gravity in 1911, he found he needed a type of
mathematics that described gravitational physics that did not depend on
any particular coordinate system. He was advised by friends to study
tensor calculus, which had been worked out fifty years earlier by
the likes of Riemann, Christoffel and Ricci. I find it remarkable that
quantum electrodynamics would similarly be worked out in the 1940s using
a mathematics that had been discovered by Grassmann almost one hundred
years earlier.
The books I have on QFT explain only the merest fundamentals of
Grassmann algebra, while math books I have seen on the subject go far
over my head. Still, I am amazed that God could come up with something
so strange and counterintuitive -- and useful. In fact, since fermions
make up all of the ordinary matter in the universe (including you and
me), God must have had Grassmann numbers in mind from the very
beginning. What a Creator!
One of the oddest things about Grassmann calculus is its underlying
simplicity. For example, the most complicated single-variable math
formula f(x) you can think of can be expanded as a Taylor
series, which in Grassmann algebra consists of just two terms: a +
bx, where a and b are constants. Thus, the basics
of Grassmann's discovery can be grasped by anyone in about five minutes.
You can read more about Hermann Grassmann here:
Wikipedia |
|
Units -- Posted by wostraub
on Thursday, November 16 2006 |
One of the more
appealing aspects of Hermann Weyl's metrical gauge theory deals with the
concept of "units." Humans measure length in terms of meters and feet
and, in ancient times, cubits -- different, but all interchangeable, and
therefore the same thing. But in the presence of a strong gravitational
field (or when dealing with velocities approaching the speed of light),
the lengths of physical objects can become ambiguous -- the length of a
physical measuring rod, for example, can depend on the observer.
In Weyl's original gauge theory, length can be continuously redefined as
one goes from one point in spacetime to another.
The basic units of length, time, mass etc. used to be based upon
physical objects or anthropological effects (all called "artifacts")
that were explicitly defined to represent the units they stood
for. For example, the meter used to be defined as 1/10,000,000 of the
distance from the equator to the North Pole (via Paris). Similarly, the
second was once defined as 1/86,400th of a day. In these examples, the
physical earth was a measurement artifact.
All of these artifact-based units (except the unit for mass) have since
been replaced by non-anthropological representations. For example, the
meter is now defined by a specified number of wavelengths of the
emission spectrum of a certain cesium isotope. Similarly, the speed of
light in vacuo is now fixed at exactly 299,729,458 meters per
second. The second itself has a specific definition based on isotopic
transitions. But to date the kilogram has resisted all such conversions.
Officially, it is still defined as the mass of this platinum-iridium
alloy cylinder having equal dimensions of length and diameter (39 mm)
maintained near Paris:

But this object is not entirely stable. It has been observed to change
on the order of 50 parts per billion per year (Corrosion? Sublimation?
Old age?). Now scientists are attempting to revise the definition of a
kilogram to a non-artifact basis. But it has been a difficult road.
The December issue of Scientific American describes the most
recent attempt. It is based on a nearly perfect, ultra-pure sphere of
crystalline silicon-28 having a number of atoms that is very nearly that
of Avogadro's number (roughly 6 x 1023), which is defined
itself as the number of anything in one mole of a pure elemental
substance.
But to my mind, this just replaces one artifact with another.
Furthermore, Avogadro's number is another "unit" having an
anthropological basis. Is there no way to define the unit of mass that
is free of some kind of human subjectivity?
Quantum physicists long ago realized that their equations could be
greatly simplified by setting Planck's constant and the speed of light
to unity. But this is really nothing more than a convenience, as these
simplifications only establish yet another set of units that is no
better than any other now in use.
My suggestion? Define the kilogram as the mass of one atom of hydrogen
and be done with it. |
|
Weyl and Einstein, Again -- Posted by
wostraub on Friday, November 10
2006 |
Taken aback by Hermann
Weyl's insistence that his gauge theory was valid despite the physical
evidence, Einstein wrote to his friend on 1 May 1918 with this
remarkable correspondence:
Could one really charge the Lord with inconsequence
for not seizing the opportunity you have found to harmonize the
physical world? I think not. If He had made the world
according to you, you see, Weyl II would have come along to address
Him reproachfully thus:
"Dear Lord, if it did not suit Thy way to give objective meaning to
the congruency of infinitesimal rigid bodies, so that when they are
at a distance from one another one cannot know whether or not they
were congruent, then why didst Thou, Inscrutable One, not decline to
leave this property to the angle or to the similarity? If two
infinitely small, initially congruent bodies K, K' are no
longer able to be brought into congruency after K' has
made a round trip through space, why should the similarity
between K and K' remain intact during this round trip? So
it does not seem more natural for the transformation of K'
relative to K to be more general than affine."
But because the Lord had already noticed, long before the
development of theoretical physics, that He cannot do justice to the
opinions of mankind, He simply does as He sees fit.
You may not always agree with Einstein, but he just nails
it here. |
|
Stupid Notation -- Posted by
wostraub on Friday, November 10 2006 |
From September 1918
until late November of that year, Hermann Weyl and Einstein corresponded
repeatedly, with the main topic being Weyl's geometrical gauge theory.
Einstein loved the basic idea, but was upset over the fact that the line
element
in the theory was not gauge invariant. This unsettling little fact
ultimately doomed Weyl's idea.
But the two also bickered over Weyl's expression for the equation of the
geodesics, which is obtained by extremalizing the related integral
expression
.
Weyl's result was

where

Einstein vehemently stated that this was wrong. Weyl disagreed, and for
three months the issue came up again and again. The two men never
resolved it, and Weyl persisted in using his expression in all five
editions of his book Space-Time-matter. So who was correct?
Well, Einstein was right after all, but the whole thing was trivial, and
the two great scientists should have known better. The correct
expression is

What's the difference? It's in the partial derivative term for the
metric tensor: Weyl used a covariant term for x in the
denominator when he should have used the contravariant term.
It's no big deal, but it serves to show how important it is to maintain
consistency in your tensor notation. Few areas of mathematics have
displayed such a wide and bewildering range of notation as has tensor
calculus in its 150-year history. In the years immediately following
Einstein's general relativity theory, it seems that everyone was using a
different notation (even Einstein). Contravariant and covariant indices
were constantly being intermixed, and that is really what lies at the
bottom of this little Weyl-Einstein disagreement. |
|
Spin and the Early Universe -- Posted by
wostraub on Thursday, October 19
2006 |
Abraham Loeb,
Professor of Astronomy at Harvard University, has an interesting article
in the November issue of Scientific American that deals with
the so-called "Dark Ages" of the universe.
According to current cosmological thought, about 380,000 years after the
Big Bang the universe had cooled enough for neutral (non-ionized)
hydrogen atoms to form. This prevented the microwave background
radiation from continuing to interact with electrons and ionized
hydrogen via Thomson scattering, so it began to leak out into the
expanding universe. Because stars had not yet started to form, there was
no source of light, and the universe went almost completely dark -- the
start of the Dark Ages.
During this darkness, which is believed to have lasted about a billion
years, gravitation gradually coalesced matter into stars and galaxies.
Light radiation from the resulting fusion reactions reionized most of
the hydrogen in the still-expanding universe, and light returned to the
cosmos.
As a consequence, the farthest astronomers can see with their telescopes
is about one billion light years. Whatever occurred prior to that cannot
be detected.
Or can it? Loeb believes that the universe preserves an imprint of the
Dark Ages through what he calls a menage a trois between the backround
radiation, the kinetic energy of neutral atoms, and a type of energy
called hydrogen spin energy. By modeling how these energies must have
interacted, astronomers can compare theoretical calculations with
observations of the sky at long radio wavelengths and test it out.

In the article, Loeb describes how a neutral hydrogen atom, consisting
of a proton and electron, can exist in its ground state in two distinct
energy states -- one with the spins of the proton and electron aligned,
and another in which the spins oppose each other. The energy difference
is minute, but becomes important when the background radiation level or
kinetic energy is smaller. Loeb believes that as the dark universe
expanded, the spin energy, radiation energy and kinetic energy took
turns being top dog, and that the echoes of this cosmic energy dance are
still detectable in the night sky.
If Loeb is right, then humans will be able to see the unseen, and
perhaps get an even better glimpse of the hand and mind of God.
|
|
Pandora's Box on IFC -- Posted by
wostraub on Tuesday, October 17
2006 |
Shot in Berlin in the
waning years of Germany's Weimar Republic, the late silent film classic,
"Pandora's Box" (Die Büchse der Pandora) is airing on the
Independent Film Channel (IFC) at midnight tonight and tomorrow at 7:45
am PST (October 18). The film is shown uncut and uninterrupted, with
both its original German and English subtitles.

German filmmaker Georg Wilhelm Pabst's 1929 classic stars the hauntingly
beautiful American actress Louise Brooks (1906-85) as the libertine but
curiously innocent dancer/vamp Lulu. Now widely regarded as a cinematic
masterpiece, the film received surprisingly scathing reviews because of
its (then) shocking sexuality (but there's no nudity, parents).
Sickened by the excess and amorality of Hollywood (though hardly an
ingenue herself), and stuck in a series of profitable but brainless
"flapper" roles, Louise Brooks left to further her career in Germany,
where she starred as Lulu in "Pandora" and Thymiane in "Diary of a Lost
Girl" (Das Tagebuch einer Verlorenen, also 1929). Following
another starring role in the 1930 French film Prix de Beauté
("Beauty Prize"), Brooks returned to the states. She grudgingly made
several more films in the 1930s, but she was essentially blacklisted by
the film industry because she refused to play by its rules. She left
Hollywood for good in 1939 and went to New York, where she lived a
rather impoverished, hand-to-mouth existence as best she could until her
death in 1985.
A victim of childhood sexual abuse and gross parental neglect, Brooks
ironically and tragically became a hedonistic abandonee herself, and by
the mid 1950s was, in her own words, "a questionable East Side dame."
But about that time she started writing about her life and the many
stars she had known personally (often very personally) during
her acting days. While her work was not prolific, her writing
demonstrates a remarkable talent for intelligent exposition. Her 1982
book, Lulu in Hollywood, reflects a truly brilliant mind.
A chronic drinker and smoker, Brooks succumbed to emphysema on August 8,
1985 after a long struggle with the disease.
Brooks led an absolutely amazing life, which is chronicled in Barry
Paris' excellent 1989 book, Louise Brooks: A Biography.
Silent film fans around the world will celebrate Louise's 100th birthday
next month (on November 14), at which time Criterion Collection Films
will release a digitally remastered DVD of Pandora with many extras,
including a rare filmed interview of the actress from 1979. |
|
Melvin Schwartz Dead at 73 -- Posted by
wostraub on Wednesday, August 30
2006 |
1988 Nobel Prize
winner Melvin Schwartz has died at 73. He shared the prize with Leon
Lederman (The God Particle) and Jack Steinberger for their work
on the weak interaction and their discovery that neutrinos come in
different flavors. But what appealed most to me about Schwartz was his
approach to electromagnetism.
Like many other befuddled graduate students in the 1970s, I had the
great misfortune of being forced to learn electrodynamics from J.
Jackson's Classical Electrodynamics, arguably the most
difficult text on the subject (the third edition was presumably "dumbed
down" in the 1990s in belated response). It's a shame that Schwartz'
Principles of Electrodynamics, first published in 1972, didn't
achieve the same (inexplicable) popularity as Jackson's book, because
Schwartz' approach is much clearer. It's even entertaining -- he starts
it off with the statement Electrodynamic theory is beautiful!
What a wonderful way to start a book!
Schwartz was one of the few physicists who insisted that electric and
magnetic fields, which are essentially the same thing, share the same
units. This in itself represents a tremendous simplication of the
subject, as the "units problem" in electrodynamics has caused no end of
troubles for students.
He similarly simplifies the understanding and calculation of the
Lienard-Wiechert potentials, another chronic stumbling block for
mediocre students like myself. The subject is laid bare in a wonderful
chapter entitled Let There Be Light!, in which the author
unashamedly shares his enthusiam for and appreciation of God's
scientific and mathematical wisdom. Indeed, Schwartz' writing style is
peppered with statements like At this point when the laws were being
written, God had to make a decision ... God naturally chose the
antisymmetric tensor as His medium of expression (Chapter 3). I
love it!
Fortunately, Schwartz' book is available as a
Dover reprint and can be had for about $10, so you have no
excuse for not buying it. No physics library should be without it.
|
|
Dark Matter Discovered? -- Posted by
wostraub on Tuesday, August 22
2006 |
On August 15, a group
of astrophysicists announced they had seen indirect evidence for the
existence of dark matter. What does this mean?
For decades, astronomers have noticed that the rate of rotation of
galaxies does not jive with the amount of matter contained in them –
that is, there is not enough gravity contained in the galaxies to keep
them from flying apart. Astronomers therefore believe that there must be
a form of matter unlike normal matter that keeps the galaxies together.
This matter have been given the name dark matter. It is
optically invisible because it does not interact with ordinary matter.

Scientists have no idea what dark matter is composed of. Since it cannot
be made of ordinary stuff like protons and electrons, other, more exotic
forms of matter have been proposed (axions, anyons, etc.). But to date,
all this conjecturing has been purely theoretical.
Now a team of scientists (including members from the Stanford Linear
Accelerator Center and the University of Arizona) have announced
indirect evidence of dark matter in the Bullet Cluster, two
groups of over one thousand small galaxies that collided about 100
million years ago in the constellation Carina, forming the shock wave
shown in the above photo (which is a composite of visible and x-ray
photographs). As the galaxies collided, the ordinary matter slowed down
as one would expect in any physical collision. However, the dark matter
component, which is immune to any kind of physical (mainly
electromagnetic) interaction, kept right on going. The scientists were
able to deduce this by measuring the amount of gravitational lensing
caused by the dark matter on more distant galaxies seen in the photo's
background (dark matter may not interact directly with ordinary matter,
but it can still affect it gravitationally). Thus, a cosmic collision
event can serve as a means of "filtering out" dark matter from its
ordinary counterpart. Indeed, there is speculation that past events have
generated "dark matter galaxies," whose presence can only be deduced by
gravitational lensing effects.
[Interesting Question: Is intelligent dark matter "life" possible, or
does it require the usual quarks and leptons? Maybe God is not quarkic/leptonic
at all!]
Who cares, you might be tempted to say. But astrophysicists have
estimated that dark matter makes up about 25% of the total matter in the
universe, whereas ordinary matter accounts for only about 5%. The
remaining 70% is thought to consist of dark energy, a
hypothetical energy field (called quintessence by some
scientists) that permeates the entire universe. Thus, the visible
universe you and I know and love accounts for only 5% of physical
reality. This concept is truly mind-boggling.
Hermann Weyl and others postulated that what we today call dark energy
is nothing more than a mathematical artifact of Einstein’s general
theory of relativity called the cosmological constant (I tend
to agree, as "quintessence" sounds a tad like the old "ether" idea of
the early 1900s). The cosmological constant is simply a term in
Einstein’s gravitational field equations which, depending on its sign,
can either act with or against the usual attractive force of gravity.
Many scientists believe that a non-zero, repulsive cosmological constant
exists and is responsible for the observed large-scale repulsion effect
that is forcing the universe to expand at ever-greater velocities. If
true, the universe will eventually expand at the speed of light,
resulting in a rather bleak future for all existence.
The relationship between dark matter and dark energy has not been
established. If the human race can keep from blowing itself up over
petty tribal conflicts (which I find highly doubtful), we may have a
chance at someday understanding the fantastic universe that God has made
for us. |
|
String Theory Unraveling? -- Posted by
wostraub on Tuesday, August 15
2006 |
The great Austrian
physicist Wolfgang Pauli once remarked "What God hath put asunder, let
no man join." He was referring to the seemingly-intractable problem of
unifying quantum theory with general relativity, two theories that work
just fine by themselves but which have, since Hermann Weyl's time,
resisted all attempts at unification. It's the one great open problem of
physics, and every physicist worth his salt worries about it.
Why bother with unification when the theories work fine on their own?
Because only through unification can we simplify our world and begin to
grasp the mind of God. Recall James Clerk Maxwell, who in the 1860s
discovered that the electric field and magnetic field are the exact same
thing. Instead of a hodgepodge of unconnected, complicated vector
equations, we have the four Maxwell equations expressing the unified
electromagnetic field (which, I might add, are among the most beautiful
mathematical expressions mankind has ever gotten its hands on).
The unification problem can be traced to the fact that the general
theory of relativity is not renormalizable (which means that infinite
probabilities invariably arise during the perturbation step), so efforts
to describe gravitation using a quantum-perturbative approach fail
miserably.
Thirty-odd years ago, string theory promised a way around this problem.
The theory's early developers noted that it demands the existence of a
massive, spin-two particle, and it was assumed that the as-yet
undetected graviton feld would fit the bill.
Initially, it looked good on paper. But the most advanced version of
string theory requires that spacetime consist of 11 dimensions (1 time
dimension and 10 spacial dimensions) and not the usual 4. In order to
demonstrate the existence of all these extra dimensions, physicists
would need access to energies that are many magnitudes beyond those
currently produced in the most powerful particle accelerators. Indeed,
these energies rival that of the Big Bang itself, making it almost a
certainty that string theory can never be tested.
The theory's critics insist that any untestable theory is unscientific,
and therefore has no place in science. Some have even gone so far as to
say that it is akin to religious faith. Anti-evolutionists (and
Republicans) might be crazy about this, but not physicists.
My personal problem with string theory is far simpler -- I just can't
follow the mathematics. Back when Einstein first announced his general
theory of relativity in November 1915, it was said that only a dozen
people in the world could understand it. That was simply not true --
relativity is pretty straightforward, and while the math at the time was
unfamiliar, it wasn't difficult at all. Same thing with Heisenberg's
matrix mechanics in 1925 -- physicists just weren't all that familiar
with matrices, which even today's middle school kids can understand.
String theory, by comparison, is nothing less than a convoluted maze of
unbelievably complicated mathematics that seems beautiful only to the
relatively few people who can work with it. And in their own words, even
they don't really understand what they're doing!
So now we get the August 21 issue of Time magazine, which has
an article entitled The Unraveling of String Theory. It reports
that two new books by respectable physicists (Lee Smolin and Peter Woit)
are heralding a renewed criticism of string theory that might just catch
on.
The criticism advances the now decades-long suspicion that string
theory, which provides absolutely no testable predictions, may be
nothing but mathematics after all. If this can somehow be demonstrated,
it would serve to free up the minds of some pretty smart people (like Ed
Witten at the Institute for Advanced Study at Princeton) who currently
are obsessively pursuing M-theory, which is the 11-dimensional version
of strings I mentioned earlier.
In my mind, it's entirely possible that God considered basing physical
reality on string theory, but gave it up because it gave even him
headaches -- and a theory with headaches lacks beauty, and God's way of
thinking always involves beauty. But if not strings, then what? Is there
no way to unify gravity with quantum mechanics? Was Pauli's admonition
correct after all?
If string theory bombs, then we're back to where Weyl, Einstein, Pauli
and many others were 80 and 90 years ago. To be sure, we know a lot more
than those folks did, but one thing remains the same -- our intellectual
curiosity is simply not matched by our intellectual ability.
|
|
Straumann Again -- Posted by
wostraub on Thursday, August 3 2006 |
Here's a new article
from Norbert Straumann (University of Zürich), which was the basis of a
talk he gave in 2005. Some new stuff on Hermann Weyl and early gauge
theory, along with some reflections on the gauge principle in quantum
electrodynamics.
Article |
|
Persistence -- Posted by wostraub
on Monday, July 31 2006 |
Edison once said that
discovery is 1% inspiration and 99% perspiration. Einstein asserted that
persistence trumps intelligence. Weyl's efforts to bail out his 1918
metrical gauge theory certainly represents a classic example of
persistence in the face of withering criticism. Weyl persisted because
he believed he was in possession of the truth.
Recall that Mr Einstein rejected Hermann Weyl’s original gauge theory on
the basis that it did not preserve the invariance of the line element
ds under a gauge transformation. In spite of the simplicity of
Einstein’s argument, Weyl tied himself in knots desperately looking for
a way out. As far as I know, he tried three escape routes.
One was to assume that the ds of measurement was not the same
as the mathematical ds. That is, what we measure as ds
is a true invariant, whereas the mathematical version is not. This
almost metaphysical option was quickly dismissed by Einstein, Pauli,
Eddington and others.
Weyl then moved on to a line element that replaced the metric tensor
gμν with the Ricci tensor Rμν, a
quantity that is a true gauge invariant in Weyl’s geometry. This was an
interesting dodge, but it too was thrown out.
Weyl’s last gasp was to make ds invariant by multiplying the
metric tensor with a scalar J(x) of gauge weight –1, so that
the line element now goes like ds2 = J gμν dxμdxν.
After considerable thought, Weyl realized that the only reasonable J-quantity
had to be the square root of Cμναβ Cμναβ,
where the C-quantity is the Weyl conformal tensor (see my pdf
article on this tensor on the menu to the left). This time Einstein was
impressed, though to this day no one knows if Weyl’s J-quantity
has any relevance in physics.
It is straightforward, if rather tedious, to calculate the equations of
the geodesics associated with Weyl’s J-invariant. I did the
calculation many years ago, and found that they’re completely
nonsensical. I’m sure Weyl did the same calculation, and maybe that’s
when he finally tossed in the towel. |
|
Riemannian Vectors in a Weyl Space -- Posted by
wostraub on Sunday, July 16 2006 |
I've posted the final
write-up on Riemannian Vectors in a Weyl Space, which tries to
address a mathematical inconsistency in the original Weyl theory (and
which has nothing to do with the conformal aspects of the theory).
Fixing the inconsistency leads to simple derivations of the Klein-Gordon
and Dirac equations. I've also included lots of other junk as food for
thought.
In this paper I've tried to include all the reasons why I think Weyl was
really close to a unified theory of the combined gravitational-electrodynamic
field, but please believe me when I say I have no illusions that this
will ever be rigorously demonstrated -- certainly not by my
overly-simplistic treatment. Feel free to criticize.
Riemannian Vectors in a
Weyl Space |
|
Houston, We Have a Problem -- Posted by
wostraub on Saturday, July 15
2006 |
The disturbing events
in the Middle East and the recent hoopla over the space shuttle mission
made me think about that old science fiction movie in which astronauts
take off for the moon or Mars or someplace only to learn that a world
war has destroyed earth's population (along with everything else) and
they have nothing to return to. I'm also reminded of the scene in
Planet of the Apes (the 1960s version, that is) in which one of the
returning astronauts plants a little American flag in the lifeless soil,
while Charleton Heston laughs hysterically.
Now that the shuttle missions have been reduced to meaningless
public-relations trips designed to see whether the ship's insulation is
still intact, I am again forced to unveil the true stupidity behind
America's "space travel" experience. Here it is:
1. The shuttle orbits at an altitude of about 210 miles. At that height,
the force of gravity is still more than 90% of what it is here on
earth's surface. It's just like an astronautic flea who "soars" above
the surface of an onion by jumping onto the nearest outer skin layer.
The astronauts are not in "outer space."
2. The weightlessness of the astronauts is induced solely by the orbital
centripetal force. If they increased the shuttle's speed by only 2.5%,
they could orbit the earth at a height of one foot.
3. Shuttle missions are incredibly boring. There's little for the
astronauts to do other than maintain their life-support equipment. All
meaningful on-board experiments have been done to death, including
observing how crystals grow and ants propagate in microgravity. In their
free time, the astronauts can look out and see the curvature of the
earth. That's about it.
4. Without the protection of earth's atmosphere, dangerous levels of
cosmic rays constantly permeate the shuttle and its inhabitants. Do you
recall the "flashes of light" reported by Armstrong, Aldrin and Collins
during their interplanetary trip on Apollo 11? Those flashes were caused
by "Z particles" (cosmic ions with atomic weight around that of carbon)
piercing the astronauts' corneas. Meanwhile, microgravity induces rapid
loss of bone density and muscle tone.
5. There are literally thousands of pieces of space junk now orbiting
the earth, from grain-size ejecta particles to car-sized failed
satellites. And it's all flying around at many thousands of miles per
hour -- many times faster than a speeding bullet. NASA mission planners
have to keep track of every known chunk to avoid a catastrophic
collision with the shuttle. One of these days they'll lose track of
something, with disastrous results. All it takes is a particle the size
of a grain of salt.
6. In spite of all the high-tech you see in the orbiter, its boosters
and the tracking equipment, the shuttle is really nothing more than a
fancy Chinese rocket utilizing 2,000-year-old chemical technology.
Chlorine- and nitrogen-containing pollutants spewed out from each launch
measurably impact the earth's biosphere (chlorine is about the worst
thing you can imagine for the ozone layer).
7. President Bush says we're going to Mars! The round trip will take
years, cost more than $100 billion, and if cosmic rays don't kill the
astronauts the boredom will drive them insane. But it's a trip Americans
may have to buy into whether they like it or not, as it's rumored that
Mars has weapons of mass destruction. We can't just stand here and wait
to be killed! They don't call it the Red Planet for nothing!
The real reason why Americans support the "space" program is that they
don't know a solar system from a galaxy, a mile from a megaparsec. I
constantly hear people say things like "Our brave astronauts are out
there among the stars and galaxies, blazing the trail to discovery." No,
they're 200 miles above your head, idiot. And if I ever hear that poem
again about "touching the face of God" (in a nuclear-armed fighter jet,
yet), I'll scream. And "spin-offs"? Please, did we have to spend a
trillion bucks for Tang and freeze-dried ice cream?
All this nonsense, and for what? A trifling trillion dollars or so to
date, and counting! The real purpose of these missions today? That's a
national secret, but I can tell you that it involves looking down on you
and me and everyone else, and not looking out on this wonderful universe
God made for us.
My suggestion? Let's first get our planet in order, make our resources
and human, animal and plant life sustainable, find a way to deal with
our aggressions, then reach for the heavens. Wouldn't this please God
more than what we're doing now? |
|
Weyl and Dirac -- Posted by
wostraub on Monday, June 26 2006 |
Someone asked me for a
copy of a 1973 paper by P.A.M. Dirac today. I got it out of the garage
to email, and read it again for the first time in years. In it, Dirac
uses Weyl's gauge theory in an attempt to explain why the gravitational
constant G should be decreasing with time. In the paper, Dirac
reveals a fondness (if that's the right word) for Weyl that I had missed
earlier. He even provides a counter-argument for Einstein's famous
objection against Weyl's theory.
But then he goes on to describe how a non-moving charged particle in a
Weyl field can be used to break charge symmetry while maintaining CPT
symmetry. Dirac's argument is simple: a vector associated with a
particle in a Weyl field changes magnitude according to dL = φμ
L dxμ. If the particle is at rest, vector length still
changes with the flow of time according to dL = φ0 L dx0,
where φ0 is the Coulomb potential and dx0
= cdt. If the change in length is positive with increasing time,
then it must shrink with decreasing time (and vice versa). Regardless of
the convention you choose, the change in length is effected by the sign
of the particle's charge. Thus, symmetry is broken between positive and
negative charge. It's so beautiful.
Dirac, who won the 1933 Nobel Prize in Physics at the age of 31, was
once asked if there was anyone who was so smart even he couldn't
understand. "Weyl" was Dirac's answer. |
|
Hermann Weyl Resources Online -- Posted by
wostraub on Sunday, June 25 2006 |
Among the papers,
books and articles I have collected on Hermann Weyl are a number of
contributions made by the German mathematical historian Erhard Scholz of
the University of Wupperthal. Scholz has written extensively about
Weyl's mathematics (from a primarily historical perspective), although I
find his English difficult to follow for some reason. Nevertheless, his
online materials are well worth acquiring. Just Google "erhard scholz,
weyl" and you'll finds lots of stuff, mostly in pdf format.
You might also want to Google "john l. bell, weyl" (presumably no
relation to the John S. Bell of Bell's Theorem fame) regarding several
online papers he's written on Weyl and his philosophical leanings. I
really don't "get" philosophy, but it's worth checking out.
Another resource that I have not yet acquired is "Hermann Weyl --
Mathematics and Physics, 1900-1927," a 1991 Harvard University PhD
dissertation by Skuli Sigurdsson. I haven't found it on any of the
online dissertation libraries, so it's probably not out there. I suppose
I'll have to get it directly from Harvard for much more than I care to
pay. I'll let you know if I find it.
[God bless the Pasadena, California Library! It acquired a set of
Einstein's collected writings (German and English translations) after a
loan request I made several months ago. The collection includes many
references to Weyl and his gauge theory and is just plain fun to read.]
|
|
Albert, Mileva and the Noble Engineering Profession -- Posted by
wostraub on Thursday, June 22
2006 |
I've been reading the
letters that Einstein and his first wife, Mileva, wrote to each other in
the period 1914-19. This was a period of increasing estrangement between
the two of them following their split-up around 1913, and the
correspondence ranges from cordial to angry.
The letters take on a decidedly monetary tone after 1916, when it became
apparent that Einstein would eventually win the Nobel Prize. Mileva was
constantly asking for money, and Einstein provided it, often grudgingly.
Indeed, the letters from 1916 to 1919 seem to be nothing but arguments
over money. But Mileva was hard up, unemployed, and looking after two
young children, while Einstein, not yet famous, was himself just getting
by. (Einstein got the Nobel in 1921, and all the prize money, as he
promised, went to Mileva. It amounted to 121,572 Swedish krona. Worth
roughly $20,000 back then, it's not much today, and it wasn't that much
even in 1921. Nowadays, the prize is about $1 million.)
Mileva seems to have used their two boys, Hans Albert and Eduard
(nicknamed "Tete"), as a means of coercing funds from her estranged
husband, but the real villain of the story is Einstein himself, who was
never really cut out to be a husband or father. In the letters, Einstein
frequently apologizes for having to cancel out on planned visits and
such, and he seems content to simply blow kisses at them while coolly
blowing off Mileva's demands for money.
Later in the decade, we see letters to and from Einstein and his
soon-to-be second wife, Elsa. It's almost disgusting to experience
Einstein's kissy-kissy attitude with Elsa in these correspondences,
especially when one knows that this marriage was also a colossal
failure. Mileva was no beauty queen, but I could never understand
Einstein's attraction to that pudding of a woman, Elsa.
Anyway, I got mildly ticked off when I read Einstein's letter to Mileva
dated November 9, 1918 (also Weyl's 33rd birthday!), in which he impuned
all us noble engineers:
I am glad that Hans has an intense interest in
something. On just what it is directed is less important to me, even
if it is engineering, by God!
The nerve of the guy!
PS: Einstein's insult to the engineering profession backfired on him.
Hans Albert Einstein went on to become a noted professor of civil
engineering at UC Berkeley. Ha!
PPS: The letter, sent by Einstein without a return address, was opened
and read by a Berlin government censor, who threatened to withhold
future deliveries unless the address was clearly marked. Sounds very
similar to what's going on in this country today. |
|
Looking for Lulu -- Posted by
wostraub on Tuesday, June 20 2006 |

The other night Turner Classic Movies reaired the 1999 documentary
Looking for Lulu, a great one-hour overview of the life and works
of American silent film actor Louise Brooks (1906-1985), whose character
Lulu in the 1928 German classic Die Büchse der Pandora
(Pandora's Box) is said to have enraptured Adolf Hitler long before
Marlene Dietrich or Eva Braun came along. I'll bet anything Hermann Weyl
and Albert Einstein for once agreed with Hitler on something (however,
Hitler subsequently denounced the film itself as "degenerate art").
I saw the film years ago at the old Vagabond Theatre in Los Angeles and
fell head over heels for this lady, whom I consider to be easily the
most beautiful film actor of all time. But she wasn't just a pretty face
-- she was a child prodigy, educated in classical literature from an
early age, and a gifted classical dancer with an equally brilliant mind.
In her early films she played a typical 1920s "flapper," but soon left
for Germany to seek more demanding roles. In Germany she was known as
Schwarze Sturzhelm (Black Helmet) because of her unusual
coiffure.
Amazon sells the documentary DVD for $90. I burned it on DVD
from the TCM airing and will send it out for a nominal fee if you're
interested, provided I don't get inundated by hundreds of requests. Drop
me a line.
PS: Pandora's Box is currently unavailable in Region 1 (USA)
DVD format, and Kino Video does not plan to release it anytime in the
near future. If you live in the UCLA area, you can attend a free
screening of the film at the Armand Hammer Museum at 8 pm on July 7,
2006.
Update:
The Criterion Collection will release the digitally remastered
Pandora's Box on American region DVD on November 10, 2006. It
will include four different musical soundtracks, the Looking for
Lulu documentary, stills, an interview with Brooks, and other
extras. |
|
Feynman's Wheels -- Posted by
wostraub on Tuesday, June 20 2006 |
While
purging files from my Powerbook today, I came across a couple of
pictures having to do with Caltech physicist Richard Feynman (I don't
remember where I got them, but they must be fairly old, as the guy died
in 1988). Anyway, here is his license plate (I would have gotten
quanta for my plate, but we can excuse Feynman for the bad
spelling).
This next shot of Feynman's van is interesting because it was obviously
taken while parked at the Dorothy Chandler Pavilion in downtown Los
Angeles. How do I know that? Because the tiered building in the
background is the home of my old employer, the Department of Water &
Power!

It doesn't show up very well, but Feynman's van is covered with
paintings of (appropriately enough) Feynman diagrams. I wonder
which auto detail shop in Pasadena did that (I might get something
Weylian for my Prius).
Today's Factoid: The DWP has a really neat engineering library on the
fifth floor, and I looked out from that vantage point one day many years
ago to see then-Mayor Tom Bradley standing with Queen Elizabeth in the
Pavilion right across the street. You don't see that every day! |
|
Fourth Order -- Posted by
wostraub on Friday, June 9 2006 |
One of Einstein's
objections to Weyl's theory of the combined gravitational/electrodynamic
field was that Weyl's field equations were of fourth, not second, order
in the metric tensor gμν and its derivatives.
However, variation of the fourth-order Weyl action

with respect to the metric tensor for empty spacetime gives

where the subscripted bar and double bar notation indicates partial and
covariant differentiation, respectively. It is relatively easy to show
that this differential equation has a non-trivial solution only when the
Ricci scalar R is a non-zero constant; the second term then
vanishes, and R can be divided out of the remainder, leaving a
term of second order. The surviving term can be solved (it's almost the
same as Schwarzschild's solution), giving the familiar expressions for
the advance of Mercury's perihelion, the deflection of starlight, etc.,
provided R is taken as a small constant.
The great Austrian physicist Wolfgang Pauli was aware of this
calculation as far back as 1921 (when he was just a 21-year-old kid),
and noted that Weyl's theory was just as capable of explaining the
perihelion shift and light deflection as was Einstein's theory.
The Schwarzschild-like solution includes a small repulsion term
(proportional to R) that might have something to do with the
observed accelerated expansion of the universe. Numerous researchers
have linked this term to the cosmological constant.
It is also interesting that Weyl's theory gives an Einstein tensor with
a 1/4 term (rather than 1/2). This makes it automatically traceless, a
desirable feature that Einstein himself searched for in vain. No wonder
Weyl thought he was really on to something! |
| Ray
Davis Dead at 91 -- Posted by
wostraub on Saturday, June 3 2006 |
Raymond Davis, the
Brookhaven/University of Pennsylvania physical chemist and 2002 Nobel
Laureate who devised accurate neutrino detection and counting methods,
has died at his Blue Point, New York home. He was 91.
Davis, whom I wrote about on this site a few months ago, showed
conclusively that the number of neutrinos (elementary particles first
anticipated by the work of Hermann Weyl) reaching Earth from the sun is
only one-third the number predicted by the standard solar model
developed by the late astrophysicist John Bahcall (and a close friend of
Davis). It was learned in the 1980s that the three types of neutrino can
morph into one another, so out of 100 solar neutrinos emitted by the
sun, only one-third will still be solar neutrinos by the time they reach
Earth. In an amazing case of theoretical/experimental jousting, both
scientists were proved to be right!
At the time of Davis' Nobel Prize in Physics, Bahcall said of his friend
Ray is not only an extraordinary scientific person,
but also an extraordinary human being. Ray treats the janitor in the
laboratory with the same friendliness and respect that he does the
most senior scientist. And for that, he is loved by his colleagues.
Davis is survived by his wife of 57 years, Anna.
|
|
Hermann Weyl and Imaginary Length -- Posted by
wostraub on Saturday, June 3 2006 |
Mathematical
symmetries, like Hermann Weyl's gauge symmetry, are essentially
undetectable aspects of action Lagrangians. This is the essence of all
mathematical symmetries. For example, the electromagnetic four-potential
Aμ has no absolute value -- an arbitrary gradient
can be added to it without changing Maxwell's equations. Before the
advent of the gauge revolution in physics, it was thought that the
four-potential therefore has no intrinsic meaning, and that the electric
and magnetic fields E(x) and B(x) represent the only
true reality. Nowadays we know better; E(x) and B(x)
are themselves composed of various derivatives of Aμ
which, though "undetectable" in a real physical sense, is the true
underlying reality. To paraphrase Columbia University's Brian Greene,
trying to determine the absolute value of Aμ is
tantamount to trying to figure out if the number 9 is happy.
Those of you who studied complex analysis in school may recall the
theory of residues, which provides a means for evaluating certain
improper integrals by integrating around the singular pole in the Argand
plane. Probably the first problem you solved involved the "single pole"
integral

where z is a complex quantity and i is the imaginary
number (-1)1/2. It is interesting to note that
Einstein's objection to Weyl's gauge theory can be avoided by an appeal
to this pathetically simple equation if we identify z with the
(variable) length of a vector L under parallel transplantation
in a Weyl manifold. In fact, the German mathematical physicist Fritz
London used this equation in 1927 to derive the quantized radii of
orbital electrons for the Bohr atom in a Weyl space.
The only downside is that quantities such as vector length L
and the four-potential itself become essentially imaginary quantities in
Weyl spacetime. This observation has interesting consequences, and
perhaps the most profound consequence is that Weyl's theory has validity
only in quantum mechanics (where imaginary quantities are de rigeur),
not geometry. If you have followed this site at all, then you already
know that in 1929 Weyl successfully applied his gauge concept to quantum
theory, where it now represents one of the most profound ideas in all
modern physics.
But there are some researchers (and they keep emailing me!) who insist
that imaginary vector length is ok provided the square of the
length L2 always comes out real (reminiscent of the
probability interpretation of the square of the wave function Ψ2,
which is real). Well, I still don't know about all this, but I keep
thinking about it. If one always gets L2 when doing
a physical measurement, its complex or imaginary aspects are totally
hidden from us because we always just take the square root, thinking
that it, too, is real. For example, the square root of the real quantity
|z|2 is not +/- z, but a +/- ib,
where a and b are real numbers.
I'm an idiot, it's true, but you have to admit it keeps one's mind off
the moronic (and criminal) antics of President Bush, whose mind (and
legitimacy as a human being) are pure imaginary but whose crimes are all
too tragically real. |
|
Hermann Weyl and Steve Martin -- Posted by
wostraub on Saturday, June 3 2006 |
The comedian Steve
Martin, who was a philosophy major at California State University at
Long Beach (my undergraduate school!), once said that he learned just
enough philosophy there to screw him up for the rest of his life. I was
luckier than he was -- not only have I never taken a class in the
subject, it wouldn't have made any difference anyway, because I just
don't get philosophy at all.
Stanford University Professor of Philosophy Thomas Ryckman does get it
and, more importantly, one of his specialties is the relationship
between the development of general relativity and the state of German
philosophy in the early 20th century. He has written a book on the
subject,
The Reign of Relativity, in which both Einstein and
Weyl play prominent roles. Einstein himself was an armchair philosopher,
but Weyl was much more active on the subject. He was an early adherent
of the great German philosopher Edmund Husserl, and in fact married one
of Husserl's students, Helene Joseph.

Both Weyl and his wife were not only good philosophers, they were gifted
linguists. In the preface to his seminal book The Classical Groups:
Their Invariants and Representations, Weyl tells us
The gods have imposed upon my writing the yoke of a
foreign tongue [English] that was not sung at my cradle.
(Weyl wrote this in English, not German, and it has
always been one of my favorite quotes of his.)
Anyway, back to Ryckman, who in January 2001 gave a lecture at Berkeley
on the influence of Husserl on Weyl's gauge idea. I will not pretend
that I understand the philosophical part, as my brain is not really
wired for it (and it's not a chronic "senior moment" thing for me,
either; like pure math and mathematical logic, it just plain escapes
me). But Ryckman's talk did provide a pretty good introduction to Weyl's
gauge principle, and you just might understand the rest of it as well,
especially if you have ever studied transcendental phenomenology
or logical empiricism (whatever the hell they are).
Here is Ryckman's lecture in Microsoft Word format:
Article
|
|
Absolute Truth in an Age of Lies -- Posted by
wostraub on Tuesday, May 30 2006 |
In a letter to
Einstein dated 19 May 1918, Hermann Weyl asserted
As a mathematician, I must absolutely insist that my
geometry is the true, local geometry [reine Nahegeometrie];
the fact that Riemann posited only the special case Fμ ν
= 0 has no substantive legitimacy other than a merely historical one
... If in the end your views are correct concerning the actual
world, then I would regret having to accuse the dear Lord of a
mathematical inconsistency.
Einstein himself once stated that if his theory of
general relativity (gravitation) was not correct, he would have pitied
the Lord for having overlooked such a beautiful idea. This is what sheer
truth and beauty does to a person -- it is so compelling that it takes
on almost divine qualities, even to scientists who are otherwise devoid
of any religious faith. In the purest of examples, it is completely
objective, overriding any issues of ego or self-righteousness.
Another case in point: I am rereading The Physics of Immortality:
Modern Cosmology, God and the Resurrection of the Dead by the noted
astrophysicist Frank Tipler (he's the same guy who proved that an
infinitely-long rotating cylinder could be used as a time-travel
device). I am looking at it again only for the mathematics, which may or
may not be relevant to the author's central thesis -- that religion is
actually a branch of physics, and that we will all be resurrected to
eternal life by God when the universe reaches the so-called Omega
Point some umpteen zillion years from now. As a newly-minted PhD in
1976, Tipler was a diehard atheist until he experienced an epiphany of
sorts while playing with Einstein's gravitational field equations.
Whether one completely agrees with Tipler or not is beside the question
(as a Christian, I do not, but the stuff's interesting nevertheless).
The main point is that mathematical and physical truth has a beauty to
it that transcends much of what one experiences in day-to-day living.
Part of that truth (at least for me) is the realization that God exists
and had a purpose for putting us here in the first place (either as Adam
and Eve or as a couple of enlightened Australopithecines). I'm
not always sure he did the right thing, considering the mess we've made
of the world, but that's another story.
Weyl's own Road to Damascus occurred in 1918, when the concept of gauge
symmetry sprang into his mind. Einstein's was in the period 1913-15,
when he realized that another symmetry -- spacetime invariance -- could
be used to develop a theory of gravity. Both men were absolutely
convinced that they were in possession of the truth, and it changed
their lives forever.
I often ask myself what inspires or moves other people. Is it absolute
truth, or what they themselves believe to be the truth based on what
others have told them? How can we recognize absolute truth, and not be
fooled by others (or ourselves) that that truth is not in fact a lie? To
me, the only path is math and science, in combination with the teachings
of Jesus Christ, because these things cannot lie. But not everyone finds
math and science to be very interesting. Can truth be found in
accounting, economics, politics, American Idol or auto
mechanics? Can truth be found in the New Testament if mathematics and
physics are ignored? The answer is very clear to me, but who am I to
impose my beliefs on others? |
|
Gravitational Lensing of a Quasar -- Posted by
wostraub on Thursday, May 25 2006 |
This amazing
photograph, taken by the Hubble Space Telescope, shows a cluster of
galaxies (about 7 billion light-years distant) splitting the image of a
single very distant quasar (about 10 billion LY away) into no fewer than
five images (the bright bluish-white points of light near the photo's
center). The galaxies act as a gravitational lens that
imperfectly reproduces the quasar's image in a circular arc about the
galactic field of view.

The photo also shows distorted images of galaxies near those responsible
for the lensing. Quasars (quasi-stellar objects) are themselves
the cores of galactic-sized objects containing super-massive black
holes. The extreme luminosity of a quasar is powered by matter being
accreted into the hole; as it spirals in, friction from the accretion
heats the matter up to the point where intense x-ray and gamma radiation
comes pouring out. Quasars were originally a great mystery to
astrophysicists because their great luminosities didn't seem to agree
with their extreme distances.
Another example of God's miracle universe. Sadly, the Bush
Administration, in its hatred and fear of legitimate science, has cut
funding for the Hubble Space Telescope, whose orbit will eventually
decay until it burns up in Earth's atmosphere. On the plus side, the
money saved will be available to help fund new wars of aggression for
oil and other dwindling resources, but in the name of truth and justice
and liberty and Christian goodness. But hey, whaddya want, America --
buck-fifty gasoline or a geeky orbiting science project? |
|
Reality v. Formalism -- Posted by
wostraub on Sunday, May 21 2006 |
In the preface to his
1917 book The Continuum, Hermann Weyl tells us
It is not the purpose of this work to conceal the
bedrock on which the house of analysis is founded with a fake wooden
structure of formalism -- a structure which can fool the reader and,
ultimately, the author himself into believing that [formalism] is
the true foundation. Rather, I shall show that this house is,
to a great extent, built on sand.
Weyl goes on to say that the then-popular use of
arithmetic and irrational number theory to solve the problem of the
continuum should be stamped (sarcastically) with the title
Pythagoras. Therein lies the seed of Weyl's thesis: much of real
analysis at the time was based on circular logic; it was non-rigorous,
and therefore corrupted by false or meaningless formalism. In his book,
Weyl set out to make things right.
Today we have a few people around who are brilliant in both modern
mathematics and physics; Witten, Penrose and Baez come immediately to
mind. But Weyl was the first of this kind to come upon the scene.
Trained initially as a mathematician, he immediately ventured out into
physics, where he made many profound and fundamental discoveries.
Weyl was not afraid to attack what he perceived as either unintentional
misrepresentation or outright lies. In his book he attempts to set
straight issues that at the time contradicted unquestioned mathematical
thinking that greats like Dedikind had established decades earlier.
Later, when Weyl proposed his theory of the combined
gravitational-electromagnetic field, he did not back down even when his
theory was questioned by the great Einstein. Weyl's persistence, which
was based on a firm conviction that what he had proposed was based in
absolute truth and beauty, paid off when he applied his theory to the
then-emerging field of quantum mechanics. Weyl's gauge principle stands
today as one of the most profound tenets of quantum physics.
Who today has the courage to go up against established authority? Today
we are told lie after lie by our political leaders, and we swallow every
one of them, hook, line and sinker. Who among us has the courage to tell
Bush and Company that they are liars and false prophets?
Weyl denounced Hitler, but had to flee his beloved Germany in 1933
because neither he nor all his brilliant contempories could stem the
tide of nationalistic insanity that was sweeping the country. Not long
afterward, magazines and posters were displayed with Einstein's photo
and Noch ungehängt! (not yet hanged) all over Germany. Not
surprisingly, Einstein too fled the country. A dedicated Nazi effort to
discredit the theories of special and general relativity soon had the
German people thinking they had been tricked into believing a lot of
intellectual hokum. Books were burned, ideas themselves were banned, and
the great edifice that was once Deutsche Mathematik und Physik
was destroyed in favor of ignorant, arrogant nationalism.
Sadly, this is America today. But the danger is heightened infinitely by
America's possession of 10,000 nuclear bombs, spy satellites that can
watch and record everything we do and say, a hatred of legitimate
science and truth, and a crazed, fanatical, nationalistic Christian
millennialism that wants desperately to hasten Armageddon through
unilateral, preemptive war.
It is ironic that today Weyl and Einstein would almost certainly be
forced to return to Germany to escape the fascist madness that has
overtaken our country.
This is "circular logic" of a most disturbing kind. God save us all.
|
|
Einstein -- Collected Papers -- Posted by
wostraub on Monday, May 8 2006 |
I spent several hours
at Caltech today perusing its copy of the Collected Papers of Einstein
(writings and correspondence, nine volumes, with a few English
translation versions). I went there to copy Einstein's correspondence
with Hermann Weyl, only to realize that I already have most of it.
But I was unprepared for the sheer volume of Einstein's correspondence
with other notables of the time. Letters in those days (this was 90
years ago) was the email of their time, and Einstein must have spent a
fair amount of his free time just writing letters.
Particularly interesting are the letters to Mileva (his ex-wife) and son
Hans Albert, all of which show varying degrees of the man's emotions,
including warmth, concern, impatience, intractitude, and even a little
hostility. Though he genuinely cared for his two sons (in 1903 he and
Mileva had an out-of-wedlock daughter, Liserl, who was given up for
adoption), Einstein was not a family man, and his boys must have
suffered for it. Hans went on to become a professor of civil engineering
at Berkeley (he developed the Einstein bed load function in
sedimentation theory), while Eduard had mental problems all his life and
died at an early age. The fate of little Liserl is a mystery.
The Collected Papers abounds with correspondence between
Einstein and hundreds of notable scientists, mathematicians,
philosophers and political scientists. It's well-organized and makes
fascinating reading, if you've got the time. It's also available for
purchase, but each volume runs around $100, which is far beyond my
pocketbook.
As for Weyl, Einstein and my favorite mathematical physicist wrote to
each other dozens of times, discussing many different topics, including
Weyl's gauge theory and related/unrelated mathematics, gravitation
theory, philosophy, German politics, the war, and what kind of salaries
professors should be given. Weyl was also the frequent subject of
Einstein's correspondence with others. It very much takes you back to a
time when it appeared that Einstein's relativistic theories (and
generalizations) would eventually solve all the standing problems in
physics (this was before quantum theory, of course). |
|
Wilczek on Weyl -- Posted by
wostraub on Friday, April 28 2006 |
| In October 2005, MIT's
Frank Wilczek, the winner of the 2004 Nobel Prize in Physics (for
discovering the principle of quark asymptotic freedom), wrote a nice
tribute to Hermann Weyl.
Here it is in .PDF format. |
|
Einstein v. Weyl -- Posted by
wostraub on Wednesday, April 26 2006 |
Partly as a means of
ridding my mind of the preposterously immoral state of this country and
the criminal actions of the Bush Administration, I'm writing a brief
synopsis of the argument that Einstein and Weyl had regarding Weyl's
early metric gauge theory.
Several people have written in, asking what was behind Einstein's
objection to the theory, was it valid, did they remain friends, etc.
Hardly the appropriate subject matter for the general public, but the
story itself is fairly interesting, and I hope I can do it justice. I'm
getting ready for a trip, but I'll try to have it up in the next few
days. |
|
Derivation of the Weyl Conformal Tensor -- Posted by
wostraub on Wednesday, April 12
2006 |
Some time ago I
mentioned the Weyl conformal tensor, which is fundamental to the
understanding of gravitational tidal effects. Whereas Einstein's
equation (which involves only the Ricci tensor and scalar) describes
gravitational compression and compaction of matter (volume reduction via
gravitational attraction), the Weyl tensor is responsible for the
deformation of matter, with the initial volume of matter remaining
intact. For example, if you ever happen to fall into a black hole, your
body's volume will be retained but you'll be increasingly squished
sideways and elongated in the direction of the hole. This rather
unpleasant phenomenon, known to black hole afficionados and the
cognoscenti as spaghettification, is due to the Weyl conformal
tensor. Why God allows black holes to exist is anybody's guess (maybe
just because they're fascinating).
How did Weyl discover this tensor? I could never find out. He seems to
have simply written it down (he was that good).
Numerous people have asked me how the tensor can be derived. Since I've
never seen the derivation, I'd never done the calculation, at least
until now. It's much simpler than you might think.
The file conformal.pdf is on the menu
to the left. |
|
Weyl and the Question of Asymmetric Time -- Posted by
wostraub on Thursday, April 6
2006 |
What really interests me is whether God had any
choice in the creation of the world. --
Albert Einstein
In the early 1920s, Hermann Weyl discovered a new tensor
quantity (the Weyl conformal tensor) which is basically the
Riemann-Christoffel curvature tensor with the contracted pieces (the
Ricci tensor and scalar) removed. The resulting tensor is conformal
(angle preserving) as well as metric gauge invariant. Weyl must have
come across the tensor while investigating the consequences of his 1918
gauge theory and its presumed (but wrong) unification of gravitation and
electrodynamics, but I have been unable to confirm this.
The Weyl curvature tensor is zero for flat spacetime, but for curved
manifolds it is non-zero, even in the absence of matter. The tensor is
responsible for gravitational tidal effects, in which (say) a
spherical collection of particles is contorted into a prolate
ellipsoidal shape (although the tensor preserves the initial volume). In
fact, Weyl curvature is responsible for the tidal bulge in the Earth's
oceans caused by the moon's gravitational pull. By contrast, the Ricci
curvature terms deform matter by gravitational compression, and volume
is not preserved.
In 1979, the British mathematical physicist Roger Penrose (also a gifted
science writer) announced the Weyl Curvature Hypothesis, which
essentially states that the Weyl tensor was precisely zero when the Big
Bang occurred and will become infinite if and when the controversial Big
Crunch occurs. On the basis of this hypothesis, Penrose believes that
time must be asymmetrical; that is, time proceeds from the Big Bang to
the Big Crunch in only one direction. This contradicts the CPT theorem,
which basically states that physics is also valid for reversed time
(that is, all equations remain valid if we replace t
with -t ). The laws of physics may be time
direction-invariant, but on a universal scale this might not be the
case. Penrose believes that a consistent quantum-gravity theory
(assuming we ever come into possession of it) will demonstrate that the
direction of time is really only one-way.
Whether the universe will end in a Big Crunch is debatable (current data
indicate that the universe will continue expanding forever), but what is
certain is that much of the matter in the late universe will coalesce
into black holes. Spacetime curvature near the event horizon of a black
hole is highly Weylian, so even if Penrose is wrong the totality of Weyl
curvature in the late universe will undoubtedly be extremely high if not
infinite.
I've mentioned Penrose before. He has two excellent (and very readable)
books out: The Emperor's New Mind (Penguin Books, 1989) and
The Road to Reality -- A Complete Guide to the Laws of the Universe
(Knopf, 2004). The latter book is a life-altering text that should be
read by everyone who has even the slightest interest in physics, the
universe, and God's role in it all. Buy this book, read it carefully,
and then place it next to the Bible and Hamlet on your
bookshelf; you will then be able to call yourself an enlightened member
of the human race.
The Weyl Curvature Hypothesis provides a direction for time's arrow, and
is therefore intimately connected with the increase of entropy in the
universe (as demanded by the second law of thermodynamics). Indeed,
Stephen Hawking and others have proved mathematically that the surface
area of a black hole's event horizon is proportional to the hole's
entropy. Thus, in the late universe, the level of entropy contained in
black holes will be enormous. By comparison, the entropy of spacetime at
the time of the Big Bang was very low, if not exactly zero. Thus, the
Big Bang and Big Crunch are distinctly different events. This calls into
question the reality of a "cyclic universe," that is, one that comes
into existence and then recollapses over and over.
I think Weyl would have been pleased that his curvature tensor is today
profoundly associated with the fate of the universe and related unsolved
problems in modern physics. |
|
Inflation Theory Getting Dissed -- Posted by
wostraub on Sunday, March 19 2006 |
After the Washington
Post's article on cosmic inflationary theory came out a few days ago
(and discussed by me below), a veritable raft of conservative idiots
have come out of the woodwork proclaiming that it's just nonsense:
I just hate it when the media reports carefully
vetted scientific data as fact and not as just one of many valid
points of view. I'm not asking for them to ignore the opinions of
these so-called scientists, but they really should report the fact
there's a lot of controversy about whether this kind of evidence is
valid. LIke, were you there, huh, Mr. Hotshot Washington Post? As if
this ludicrous nonsense - a marble blows up like a baloon [sic] to
become the entire universe in a trillionth of a second - is more
plausible than Genesis? Give me a break!
To be fair, it doesn't help things when the WaPo reports
that the "universe expanded from the size of a marble to the expanse of
the entire cosmos in a trillionth of a second." This is just plain
wrong, but I think conservatives would have a problem with the article
even if it had been reported accurately.
Alan Guth's inflation theory says that about 10-35 seconds
after the Big Bang, the universe began to expand at an exponential rate.
This increased rate of expansion lasted until about 10-30
seconds after the Bang (a total duration of very nearly 10-30
seconds). During this expansion, the volume of the still-infant universe
increased by a factor of some 1050. Expand something the size
of a marble by that factor, and you get a marble the size of a globular
cluster -- big, but still quite tiny compared to the size of the
universe today.
But I think conservative young-Earth creationists still have problems
with this. To them, there was nothing until God created it a scant 5,000
years or so ago. Adam and Eve rode to work on dinosaurs (they actually
believe this), and all animals were herbivorous (even T. rex,
who needed those fangs and claws to get through the notoriously chewy
plants that grew back then). Then came the Fall of Mankind, when some
animals literally became evil and began to eat their more peaceful
cousins. What utter, puerile nonsense! "Where were you when the Big Bang
occurred?" seems to be their standard question to cosmologists these
days. Well, you creationists weren't around either -- so there, idiots.
I think a good part of the problem can be traced to the use of terms
like "millionths of a millionth of a trillionth of a second." These
terms are almost meaningless when taken out of context. I recall when my
high school physics teacher told us about Planck's constant, which is
roughly 6 x 10-34 joule-sec. My first thought was "Hell,
that's practically NOTHING. Anything that small is really no different
from ZERO." But I couldn't have been more wrong! The problem seems to be
related to the fact that humans cannot imagine something as small as a
decimal point followed by 33 zeros and the number 6.
Similarly, many people have a hard time imagining even a trillionth of a
second, which is much larger. "How could anything happen in a millionth
of a millionth of a second?" they ask. Well, an unstable particle that
has an average lifetime of that long is what particle physicists call a
very long-lived particle. Most unstable particles exist for much shorter
periods. Some are around for only 10-20 seconds.
The 10-35 second following the Big Bang is on the same level
of smallness as Planck's constant. If you want, we can sit here and talk
about tiny numbers all day long -- how about 10-1000 seconds?
Me, I can't even begin to imagine such small numbers. And I'm stupid at
both ends -- I can't imagine what infinity looks like, either.
But I know they exist.
What do I believe? If anybody really gives a damn, I believe that at
t = 0, God said "Let's have a quantum fluctuation take place in
this boring, expanseless nothing of a universe and get something
interesting going." BANG. Later, he created creatures with wonderful
minds that could actually calculate what the early universe MIGHT have
looked like.
And, for better or for worse, God also created creatures that did not
want to use their minds. These he called "Republicans," although in the
early days they went by the names Pharisees and Sadducees.
|
|
Inflation Theory Verified? -- Posted by
wostraub on Friday, March 17 2006 |
New data from the
Wilkinson Microwave Anisotropy Probe (WMAP), a satellite launched in
2001, has provided scientists "smoking gun" proof that the so-called
Inflationary Universe, first proposed by astrophysicist Alan Guth in
1981, is correct.
The data provide much finer details of the distribution of the cosmic
microwave background (CMB), which is an "echo" of the Big Bang. The CMB
was first detected in 1965 as a uniform, isotropic radiation
representing a universal thermal background of about 2.73o
Kelvin, or 2.73 degrees above absolute zero. [Note: the "degree" label
o for Kelvin temperatures is always suppressed, so it's just
2.73 K.]
The microwave radiation "echo" actually occurred about 270,000 years
after the Big Bang. Why is that? It's because prior to that, the
expanding ball of ionized plasma and intense radiation was so opaque
("thick") that light from within couldn't get out. At around t = 270,000
years the fireball had cooled to the point where the plasma became
transparent, and THERE WAS LIGHT!
Later data and refinements showed that the background radiation is not
quite uniform, but "granular." This graininess was predicted by Guth's
theory, but proof of the theory had eluded scientists until now. The
figure below is WMAP's map of space showing cooler (blue) and hotter
(red) regions (the temperature gradients are truly small, on the order
of a fraction of a Kelvin). Numerous scientists have remarked that
looking at the map is akin to looking at the face of God.

The inflationary theory states that the Big Bang, which occurred very
nearly 13.7 billion years ago, began as a uniform expansion of spacetime
which then accelerated briefly (and by briefly, I mean on the order of
10-30 seconds). This brief expansion, now almost jokingly
called the "Inflationary Epoch," was due to fluctuations in what is
believed to have been the false vacuum of the early stages of the Big
Bang.
Columbia University's Dr. Brian Greene, a renowned astrophysicist, has
called the findings "spectacular and "stunning," while Dr. Michael
Turner, assistant director for mathematics and physical sciences at the
National Science Foundation, called the data "absolutely amazing."
Meanwhile, concerned Republicans are scrambling to figure out how the
universe could be 13.7 billion years old, when everybody knows that God
created it only 5,000 years ago. Earlier today, there were indications
that Senate Majority Leader Bill Frist would propose a bill that would
nullify the WMAP data and imprison, torture and execute the study's
research scientists as godless, freedom-hating terrorists. But President
George W. Bush, who subsequently inquired about the cosmic microwave
background himself, remarked "If that there kozmick microwave is a new
kind of meat cooker, then I'm all fer it." |
| The
Fly in the Cathedral -- Posted by
wostraub on Wednesday, March 15 2006 |
I just finished
reading Brian Cathcart's excellent 2004
book The Fly in the Cathedral (Farrar, Straus and
Giroux, publishers), which describes in detail the discoveries of
Rutherford (the atomic nucleus), Chadwick (the neutron), and Cockcroft
and Walton (induced atomic fission). The book's title refers to a
comment made by Rutherford, whose original atomic "plum pudding" model
gave way to the correct view of a tiny, lone nucleus sitting in the vast
empty space of the atom -- like a fly in a cathedral.
But the bulk of Cathcart's book is taken up by the story of John
Cockcroft and Ernest Walton, who in early 1932 bombarded lithium metal
with accelerated protons. It is an intriguing tale of frustration,
dashed hopes, personal tragedy, and ultimate victory. The scientists'
apparatus, Neanderthal by today's standards, continually broke down,
adding months to their efforts (and always overshadowed by lack of funds
in those early days of worldwide depression). But their efforts were
repaid many times over -- they ultimately found to their utter amazement
and delight that protons could split lithium-7 -- a stable element --
into two helium atoms. The Cockcroft-Walton experiment was the very
first experimental observation of man-made atomic fission, the
transmutation of one element into another, the first splitting of the
atom.
The experiment also offered the very first practical test of Einstein's
E = mc2 formula. The observed 8.5-MeV energy of each
product helium nucleus balanced the books with respect to the reactant
particle energies. Like Einstein had said in 1905, mass and energy are
truly equivalent! In recognition of their work, the Nobel Committee
awarded Cockcroft and Walton the 1951 Nobel Prize in Physics.
The book's decription of Cockcroft/Walton's discovery is nothing short
of heartwarming, but it also includes tragedy. At the time of their
triumph, both men lost infants to childhood disease, tragedies that
nearly destroyed the men and their wives in spite of their
groundbreaking discovery.
But Cathcart saves the best for last. Ernest and Frieda Walton had a
long, happy marriage, and they went on to have four more children who
all pursued careers in science (three in physics!) Meanwhile, John and
Elizabeth Cockcroft went on to have five more children -- a scientist,
an engineer, a priest, a nurse, and a teacher.
God be praised! |
| The
Anthropic Principle -- Posted by
wostraub on Wednesday, March 15 2006 |
For a long time I've
been planning to put up an article on the Anthropic Principle,
which purports to offer some proof that an intelligent, omniscient
entity (let's call it God) really did engineer the universe for our
benefit. There's actually quite a bit of evidence that such a principle
is scientifically valid, but, until I get around to it, here's one of
the more convincing arguments.
The Big Bang, which occurred about 13.7 billion years ago, started out
basically as a super-hot plasma of quarks and leptons. But within 2
minutes this plasma had cooled sufficiently to allow for the formation
of protons and neutrons. Using Boltzmann's equation and the fact that
neutrons decay into protons, electrons and antineutrinos (the life of an
unbound neutron is about 15 minutes), it can be shown that the expanding
fireball at age 2 minutes was composed of about 75% protons and 25%
neutrons (with relatively minor concentrations of other stuff). Thus,
three-fourths of the universe consisted of hydrogen, the basic fuel of
star formation via nucleosynthesis.
Gravity gradually coalesced clouds of matter into spheres and compressed
them to the point where nuclear fusion began in their cores. Almost all
of this fusion involves the creation of helium nuclei from hydrogen.
This is the kind of fusion that mankind is now trying to duplicate for
long-term energy generation.
But after a few billion years, many stars burn up their supplies of
hydrogen. A star begins to cool, contracts further under gravity, and
then the core heats up again as a result of the increasing pressure. The
temperatures eventually get so high that the star's helium can fuse into
carbon, oxygen, neon and several other low-atomic weight elements. Some
of these stars eventually explode as novas and supernovas, and their
supplies of carbon, oxygen, hydrogen and other trace elements is what
makes up all living things. All living things on Earth owe their
existence to stardust flung out by ancient star explosions. Humans, for
example, are composed of about 20% carbon and 65% oxygen, a reflection
of the equilibrium battles in the sun involving these two elements.
During the helium-burning phase of a middle-aged star, there are three
primary reactions going on that affect the formation of carbon. One is
the triple-alpha reaction, in which three helium nuclei fuse to
form a carbon-12 nucleus. The carbon formed in this process, however,
can be scavenged by another process in which a helium nucleus fuses with
a carbon nucleus to form oxygen-16. At the same time, oxygen-16 can also
be scavenged by a helium nucleus, yielding neon-20. It turns out that
the rates of these competing reactions and the physical constants that
determine their equilibrium points are very finely tuned; if the excited
states of carbon-12 and neon-20 nuclei were only slightly different,
all middle-aged stars would evolve atmospheres that are either
oxygen-rich and carbon-poor or composed predominently of neon. The
physics of these processes, including a few minor ones that take place
simulaneously with those I've described, have been worked out by
astrophysicists over the years to a gnat's eyebrow. If the
fundamental physics of the elementary particles making up carbon,
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