Lee's Funnies
The Nonabelian Names of God
THE NONABELIAN NAMES OF GOD*
 
V. Gates, Empty Kangaroo, M. Roachcock, 
	and W.C. Gall
Ph.D-branes and Special Agents for the I.T.P.**
 
ABSTRACT
 
A summary of mysterious recent developments in high-energy theory.
This report is to be classified as part of the Theta-Files.
 
*Typeset in HTML by Rosetta Stone.
**Institute for Time reversal and Parity.
 
NNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNLO
Introduction
We report here on some recent developments in  
"The Theory Formerly Known As String Theory", which we will denote by the
symbol 
.
The most recent of these is that there doesn't seem to be any more string
theory in it:  No quantum calculations, no conformal field theory [1], no
massive states [2], etc.
 
We use Bjorken And Drell (BAD) conventions and reverse Polish notation. 
Solar neutrino flux, as measured at Super KaramelKandy [3], is given in SNU*.
 
*What's SNU?  Not much; what's SNU with you?
 
Unification
The most important discovery in string theories is the revelation that they
are all the same [4]:
 
 | 
 D=11 batgravity
 | 
This has been termed the "Götterdämmerung" of string theory,
since appearance of the extra dimension and membranes [5] has resulted in
the loss of predictability and renormalizability, which were the only reasons
for string theory unification in the first place.
 
 | 
 
 | 
| This is your brain. | 
This is your brain on branes. 
Any questions? | 
Calculations
 
 | 
 
 | 
 Bhabha scattering causes Lamb shift
 | 
This 4-point amplitude has the remarkable feature that the s, t, and u quarks
[6], which appear in the s, t, and u channels, represent S, T, and U duality [7],
with respect to the proper time s, time t, and worldline length u,
respectively.  Since it is conformal, it can be derived from M(aldacena) theory
[8-9] in the limit 0 -> hbar (but only in the large colon approximation), where
singletons become princetons [10].  Then it is calculated on ADS (Amplitude
Deficiency Syndrome) space.  In that approximation we only have
Weylation of violin variance for a little Weyl.  The high-energy limit can also
be taken by use of the Curt-Kurt equation.  Here we have used the Bored
transform:
 
B(z) = a + bz + czzzz....
 
These results can be compared favorably with those from the recent g/2-1
experiment (which is twice as accurate as previous g-2 experiments), where
g is the well-known "Ridyard coupling", which appears in
as one of the moduli oblongati.  We have used soft explicit supersymmetry
breaking to avoid producing a Goldstino [11].  This term is added to the usual
Higgs potential:
Unsolved problems
-  If dark matter fell into a black hole, would anybody notice?
 -  How bright is a neutrino star?
 
Appendix
Stages of theory development:
-  No examples:  Theory is useless.
 -  One example:  Theory is unique!
 -  Two examples:  Theory reveals new "duality".
 -  Many examples:  Theory can be fit to experiment.
 -  Infinity of examples:  Theory is useless.
 
 
Lost Feynman rules:
-  Don't run with scissors.
 -  "i" before "e", except after "c", ...
 -  Don't let the sun catch you crying.
 -  Never leave your campfire burning in the Sahara Forest.
 -  When in doubt, um, ...
 
 
Glossary
 Abstract: Introduction
 duality: twice nothing is still nothing
 field theory: mechanics
 formal theory: theory lacking substance
 holography: living on the edge
 Introduction: Body
 modulus: parameter
 nonperturbative: classical
 phenomenology: fudge
 prepotential: superpotential
 proposed: conjectured
 quantum: classical, but with derivatives
 References: Proposed referees
 second quantization: replacing the mechanisms of quantum
	mechanics with the theorems of field theory
 semiclassical: classical
 solvable: only scattering at 0 and
	180° can be calculated 
 star: a planet on asteroids
 statistical mechanics: field theory for people with low energy
 trivial: disagrees with our assumptions
 weatherology: the study of meteors
 well-known: lore
 
Dictionary of common phrases
 "their exciting new result" ----- 
	"We can't find anything better to work on."
 "we extend the results of" ----- 
	"We do the real work."
 "confirming our earlier results" ----- 
	"They couldn't calculate anything either."
 "in complete agreement with experiment" ----- 
	"SSC is dead."
 "To begin" ----- 
	"... the boring part"
 "can be described by the equation" ----- 
	"Skip the next bit."
 "as we recall from the previous section" ----- 
	"Better skip this section, too."
 "beyond the scope of this paper" ----- 
	"We don't understand this part."
 "In conclusion" ----- 
	"Thank goodness."
 "our results differ from those of" ----- 
	"Jerks."
 "in a future paper" ----- 
	"I want a job."
 "in prepraration" ----- 
	"We're stuck."
 "Your theory is beautiful." -----  
	"Your blind date has a nice personality."
 "We'll have to save further questions for the end of the talk." ----- 
	"You've found the crucial flaw in the theory, so give everyone a chance to
	run away before it hits the fan."
REFERENCES
 
 -  J.H. Warts, Conformal field theory is a no-braner, Flatland preprint.
 
 -  U.Z. Broom, Breaking of furniture by vacuum, Hoover preprint.
 
 -  Carroll O'Connor,
	Superkamioconductivity, Nuet. Phys. B137 (1999) 861.
 
 -  Hay Nanynany and Ha Chacha, DOMIN(atrix) theory: T.O.E. or T.O.Y.?,
	hep/cat-12341234.
 
 -  Victor Frankenstein,
	Brane-dead models with supercemetary, Lex Luthor Lab preprint.
	J.A. Wheeler, Strings without strings yield branes without brains,
	preprint without preprint.
  -  Muster Mark, Uptown quarks and georgino-glashon scattering, in
	finitesimal.
 
 -  DJ Jazzy Gross, Coupling of self-dual Yang-Mills to anti-self-dual
	Yin-Mills, CTP symmetry group preprint .
 
 -  Green in the Banks, The return of the
	cosmohological constant, Mendecino preprint.
 
 -  Andy D. Sitter, AdS2 as a model for the potato chip, Hahv'd postprint.
 
 -  P. Goober, I. Clubenough, and I.M. Pullyourleg, Coholography, to appear
	at the boundary.
 
 -  H. Goldstein, Classical mechanics (Addison-Wesley, 1950).
 
 -  Al G. Brake, N=2 happymultiplets and vegetable shortening,
	hip/pth-9999999 .
 
 
Click here to return to the main page