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Robert C. Helling science forum beginner
Joined: 30 Apr 2005
Posts: 22

Posted: Tue Feb 21, 2006 1:27 pm Post subject:
Re: Polyakov vs. NambuGoto action



On Mon, 20 Feb 2006 14:52:53 0500, Kasper Jens Larsen <kjlarsen@hotmail.com> wrote:
Quote:  Hi all
I was wondering, what is the reason for preferring the Polyakov over
the NambuGoto action in string theory? Of course, one can do the
quantization covariantly in the Polyakov action, but are there reasons
that make the Polyakov action unavoidable?
The reason why I ask is that a lot of important things such as the
Einstein eq. and the dimensionality of spacetime emerge from string
theory on the grounds of Weyl invariance. Consequently, there should be
some good reason for introducing the world sheet metric into the action
in the first place.

You can do the same with the NG action and in fact, Zwiebach does in
his book. It's just that formulas are uglier because you have sqare
roots everywhere but if you do it properly (that is with the correct
canonical momenta that contain sqare roots as well) you arrive at the
same free theory in the end.
You get the same constraints from diffeomorphism invariance of the NG
action as you get from Weyl invariance in the Polyakov case.
BTW, Lubos will discover that he is just promoting prejudices if he
checked it out in Zwiebach's book.
Robert

..oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oOo.oO
Robert C. Helling School of Science and Engineering
International University Bremen
print "Just another Phone: +49 421200 3574
stupid .sig\n"; http://www.aeipotsdam.mpg.de/~helling 

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Lubos Motl science forum beginner
Joined: 02 May 2005
Posts: 38

Posted: Mon Feb 20, 2006 10:34 pm Post subject:
Re: Polyakov vs. NambuGoto action



On Mon, 20 Feb 2006, Kasper Jens Larsen wrote:
Quote:  I was wondering, what is the reason for preferring the Polyakov over
the NambuGoto action in string theory? Of course, one can do the
quantization covariantly in the Polyakov action, but are there reasons
that make the Polyakov action unavoidable?

Dear Kasper, the main advantage of the Polyakov action is that the
corresponding action is bilinear in (the derivatives of) the physical
fields X(sigma). This allows one to quantize them using the standard rules
involving the Fock space etc. At the same moment, the auxiliary metric
tensor is introduced to the worldsheet together with Weyl symmetry (in
addition to diffeomorphisms) that makes the whole metric tensor locally
unphysical (3 parameters of symmetries vs. 3 numbers in the metric
tensor).
Clasically one can show that the Polyakov action is equivalent to the
NambuGoto action, and it is reasonable to define this statement to be
true in general at the quantum level, at least in the critical dimension.
Because it is hard to say what you exactly mean by a quantization of the
NambuGoto nonlinear action (with a lot of square roots etc.), you may
consider the Polyakov quantization to be a refined and more accurate
answer to the question how to quantize the NambuGoto action. Once you
learn how conformal symmetry nicely works, you may very well consider the
Polyakov action to be the true answer and starting point while the
NambuGoto action is just a naive and heuristic motivation for the
Polyakov action.
Try to quantize the NambuGoto action without the auxiliary metric tensor
and without Weyl symmetry. Find its Hilbert space and justify it. You will
see that it is not easy. The NambuGoto action looks very nonlinear and
difficult to solve, but that's just an illusion. The Polyakov approach is
a way to show that the solutions of the NambuGoto action are actually
very simple and "linear" if you write them in the right coordinates.
What I say above may look like we're relying on some special choice of
variables, much like the guys in loop quantum gravity. The difference is
that once you show that the NambuGoto is classically equivalent to the
Polyakov action, you're done because the methods to solve the Polyakov
action are standard canonical methods from quantum field theory that no
reasonable physicist would ever question, and they lead to consistent
physical insights.
Moreover, the methods of conformal field theory agree with the welltested
approaches in quantum field theory in general  and with the insights
about the Renormalization Group. The NambuGoto action may look "natural"
at the classical level but at the quantum level it is a very unnatural
beast. Once you write it in the Polyakov form, things become natural.
You know, the reason why we take the math that follows from the Polyakov
action seriously is not that it agrees with some fundamentalist doctrines
that the worldsheet area should be a natural thing to minimize. The true
reason is that it leads to robust and selfconsistent mathematical
structure that agrees with the nature of physics, at least in the rough
picture. You are free to try to find a better theory or a better
quantization of the NambuGoto action but be sure that all nonPolyakov
approaches so far have turned out to be physically useless.
Best
Lubos 

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Kasper J. Larsen science forum beginner
Joined: 20 Apr 2005
Posts: 8

Posted: Mon Feb 20, 2006 7:52 pm Post subject:
Polyakov vs. NambuGoto action



Hi all
I was wondering, what is the reason for preferring the Polyakov over
the NambuGoto action in string theory? Of course, one can do the
quantization covariantly in the Polyakov action, but are there reasons
that make the Polyakov action unavoidable?
The reason why I ask is that a lot of important things such as the
Einstein eq. and the dimensionality of spacetime emerge from string
theory on the grounds of Weyl invariance. Consequently, there should be
some good reason for introducing the world sheet metric into the action
in the first place.
Regards,
Kasper Larsen 

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