More Dice

The full t’ ‘t Hooft (look I put the apostrophy in the correct location!) article is now posted at Physics World (not Physics Today, as I listed incorrectly in my first post) commentary by Edward Witten, Fay Dowker, and Paul Davies. Quick summary: Witten thinks that quantum cosmology is perplexing, Dowker worries about the emergence of classical physics, and Davies postulates that complexity is the key to understanding the emergence of classicality. Davies suggests that quantum mechanics will break down when the Hilbert space is of size 10^120 and suggests that quantum comptuers will fail at this size. His argument could equally be applied to probablistic classical computers, and so I suggest that if he is right, then classical computers using randomness cannot be any larger than 400 bits.

Digits or Orders

How well verified is the theory of quantum electrodynamics (QED)? If you ask this to most physicists one of the first things that comes to their mind is the agreement of QED’s theoretical calculation of the anomolous magnetic moment of the electron and the extremely precise measurement of this moment. In fact, last night, while I was spending my time usefully watching the Colbert Report on Comedy Central, guest Brian Greene brought up exactly this example (well he didn’t exactly say this is what he was talking about, but it was pretty clear. The interview, by the way, was pretty funny.)
The electron magnetic moment anomoly is [tex]$a={g-2 over 2}$[/tex], measuring the deviation of the electron magnetic moment from it’s unperturbed g value of 2. Experiments done here at the University of Washington by the Dehmelt group in the late eighties gave an experimentally determined value of the anomoly of [tex]$a=1159652188.4(4.3) times 10^{-12}$[/tex] where number in parenthesis is the error. Now that’s a pretty precise measurement! On the other side of the physics departments, theorists have calculated the a value of the anomoly in quantum electrodynamics. This calculation yields an expression for the anomoly in powers of the fine structure constant. This requires calculating Feynman diagrams to eighth order in perturbation theory. The current theoretical calulculation yields an expression, to eighth order of
[tex]$a_{th}=A_2 left({alpha over pi}right)+ A_4 left({alpha over pi}right)^2+ A_6 left({alpha over pi}right)^3+ A_8left({alpha over pi}right)^4$[/tex]
where
[tex]$A_2=0.5$[/tex]
[tex]$A_4=0.328478965579 dots$[/tex]
[tex]$A_6=1.181241456 dots$[/tex]
[tex]$A_8=- 1.7366(384) $[/tex]
The first three of these terms is basically ananlytically known (i.e. can be readily obtained from functions which we can numerically calculate to any desired accuracy) and the last term, which has an error in it, is obtained by a numerical evaluation. So how well do theory and experiment agree? Well we need a value of the fine structure constant! There are many experiments which can be used to determine the fine structure constant. Among the best are experiments done using the quantum Hall effect and yield [tex]$alpha^{-1}=137.0360037(33) [2.4 times 10^{-8}]$[/tex] where the number in bracket is a fractional uncertainty. Using this value of the fine structure constant in the perturbative expansion for the theoretical expression give [tex]$a_{th}=1159652153.5 (1.2)~(28.0) times 10^{-12}$[/tex] where the number in the first parenthesis is the error from the theory calculation and the second is the error comming from the uncertainty in the value of the fine structure constant.
So, now returning to the question I started with, how well verified is QED? Well in the regime where these experiments have been preformed the results agree to an amazying precision. And when explaining this to the public, it is certainly valid to count the number of digits to which this calculation agrees with experiment. But for me, I’m more confortable saying that the above discussion shows that we’ve verified quantum electrodynamics to eighth order in perturbation theory (or to fourth order in its coupling constant.) Why do I prefer this? Well mostly because, as I understand it, modern particle theory basically says that QED must be an effective field theory for some deeper theory. Or in other words, it can’t be QED all the way down. Thus it seems more proper to ask how far down the perturbation ladder we’ve verified QED. And again, while eigth order may not sound as amazing as ten, eleven, or twelve digits of precision, it still is an amazing verfication.
And anyway, who says we should be using base ten for our measure of precision? Me, I’m in a computer science department, so it seems that base two would be much better (and you might even convince me that natural logarithms are even better.)

Best Title Ever Submission: Cryptobaryons!

I thought that Physical Review Letters had a policy about using new words in titles to papers. How then, did Cryptobaryonic Dark Matter by C. D. Froggatt and H. B. Nielsen get by the censors?

It is proposed that dark matter could consist of compressed collections of atoms (or metallic matter) encapsulated into, for example, 20 cm big pieces of a different phase. The idea is based on the assumption that there exists at least one other phase of the vacuum degenerate with the usual one. Apart from the degeneracy of the phases we only assume standard model physics. The other phase has a Higgs vacuum expectation value appreciably smaller than in the usual electroweak vacuum. The balls making up the dark matter are very difficult to observe directly, but inside dense stars may expand absorbing the star and causing huge explosions (gamma ray bursts). The ratio of dark matter to ordinary matter is expressed as a ratio of nuclear binding energies and predicted to be about 5.

Comments Broken

Comments are broken. I’m visiting Portland State Today and so probably won’t be able to fix until this evening/tomorrow.
Update: Well it seems the problem is with my comment preview. So I’ve deactivated that and will be trying to get it running later.
Update Update: I think I’ve got it all fixed. Not sure how I corrupted the entire plugin

SQuInT 2006

My favoritest ( šŸ˜‰ ) meeting SQuInT will be having it’s nineth conference in Albuquerque February 17-19. Whoop, another chance to visit the rattlesnake museum!

Dicey t' Hooft

Does God Play Dice? is not a treatise on religion and gambling, but is instead Gerard ‘t Hooft’s submission to Physics Today Physics World concerning the reconcilliation of quantum theory with general relativity. The most interesting part of this short note is not that ‘t Hooft comes out squarely on the side of hidden variable theories, but instead in his description of an idea for how general relativity might arise in such a theory:

An even more daring proposition is that perhaps also general relativity does not appear in the formalism of the ultimate equations of nature. This journal does not allow me the space to explain in full detail what I have in mind. At the risk of not being understood at all, I’ll summarize my explanation. In making the transition from a deterministic theory to a statistical treatment — read: a quantum mechanical one —, one may find that the quantum description develops much more symmetries than the, deeper lying, deterministic one. If, classically, two different states evolve into the same final state, then quantum mechanically they will be indistinguishable. This induces symmetries not present in the initial laws. General coordinate covariance could be just such a symmetry.

That general coordinate covariance may not be fundamental but is instead a product of our inability to access the beables of a theory seems like quite an interesting idea. It would be interesting to think if this type of hidden variable theory, which is not totally general because it needs to recover the general coordinate covariance, is indeed large enough to be consistent with quantum theory. I.e. in the same way the Bell’s theorem rules out local hidden variable theories, is there a similar theorem ruling out ‘t Hooft’s property? I certainly have no inclination about the answer to this question in either direction.
Of further interest, ‘t Hooft claims as motivation for his perspective the following

Nature provides us with one indication perhaps pointing in this direction: the unnatural, tiny value of the cosmological constant. It indicates that the universe has the propensity of staying flat. Why? No generally invariant theory can explain it. Yet, if an underlying, deterministic description naturally features some preferred flat coordinate frame, the puzzle will cease to perplex us.

Finally, for no reason but to turn some portion of the readers of this blog happy and the other portion of this blog angry, here is ‘t Hooft on string theory:

I am definitely unhappy with the answers that string theory seems to suggest to us. String theory seems to be telling us to believe in ā€œmagicā€: duality theorems, not properly understood, should allow us to predict amplitudes without proper local or causal structures. In physics, ā€œmagicā€ is synonymous to ā€œdeceitā€; you rely on magic if you don’t understand what it is that is really going on. This should not be accepted.

I wish I understood what ‘t Hooft means in this critique by “proper local or causal structures.”

Wasting Awaying In Blogerittaville

Been reading blogs too much when you should be doing work? Check out this cool application, Temptation Blocker (only for Windows):

So, have a major deadline looming or ripe opportunity closing and just don’t have time to waste playing Half Life 2 or checking Bloglines one last time? Well then, add Half Life 2 and Firefox to the list of programs you want to block in Temptation Blocker, set the timer for how long you want to block them and then hit the ā€œGet Work Done!ā€ button.
Now, everytime you try and access Half Life 2 or Firefox, you’ll get a dialog box telling you how much time you have left before you can access that program. During this blocked time, you can’t access those programs. You also can’t access Temptation Blocker during this time without entering in a random, 32-character string. This acts as a deterrent from you getting to your program before time is up, but it also let’s you access it if you really need to. (Note: During the blocked time, your Windows Task Manager is also disabled, in an attempt to save your from yourself and a quick Ctrl-Alt-Del. If you don’t like that idea, then you probably shouldn’t download the software).