AdS/CFT and Holography: Exploring the Questions

In summary, the conversation discusses the possibility of a provable map between Feynman diagrams and 't Hooft diagrams in the N->infinity limit, and whether the structure obtained in this way can be classified using weaker equivalence. The discussion also touches upon the conditions for quantization and whether the series expansion obtained in this way is restricted by other criteria, and the compatibility of string theory with quantum mechanics. The conversation concludes with a question about the preservation of quantum polarization and group structure when transitioning to 't Hooft diagrams.
  • #1
Andrei
3
0
I studied string theory for 2 years officially and much more on my own, chance made it that I spent the last year reading "serious" algebraic topology books and differential geometry specific for mathematicians. After gaining this insight I am very skeptical about string theory and the holographic principle... I posted these questions also on another forum and I was directed towards physicsforum...

1. I would like to understand if the t'hooft diagrams in the N->Infinity limit can be mapped back to a field theory? Is there a general proof for that? What I mean is that the whole construction adds additional degrees of freedom by extending the original manifold (lines) to bands. There must be some structure in order for the quantisation to be possible in that case. See this paper, I read it today and many things look very interesting:

http://arxiv.org/pdf/hep-th/9812012.pdf

While I agree with Witten (d'oh) it seems to me that the conditions for even having some reasons to try to apply AdS/CFT conjecture are pretty strict and rather inaccessible for experiments in "our world". Also, there are the obvious conditions for quantization one has to satisfy: symplectic manifold, choice of polarization, integrability condition (closure relation). How comes that one can assume that there exists a space (with spin structure, by the way) that satisfies all these criteria and is even remotely compatible to what exists in experiments? I am a bit afraid that people are trying out some formulation of AdS/CFT without satisfying the known criteria for the conjecture... how can they verify it correctly in that case?

2. Is t'hooft diagram "coverage" of the topological objects (sphere, torus, etc) complete? Are the diagrams in the N->infinity limit covering the whole object as pretended? How many inequivalent knots are there? Can the structure obtained in that way be classified in another way? Maybe an easier one? using some weaker equivalence, not necessary homotopy?

3. Is the map of this connection 1 to 1? it seems not...
let's see what I come with in the next days... for now, this should be it...

update: here is the question I asked on another forum... more or less the same but the general opinion was this was not well formulated:
Is there a provable map between a Feynman diagram and a 't Hooft diagram extended theory on a manifold in the N→∞ limit that produces in reverse always the QFT one is starting from?

Ok some of you did not go well with the simplicial decomposition or the simplicial complex. The idea of AdS/CFT starts with the fact that because of the two indices of the Feynman "lines" in the adjoint representation one can in principle extend them to two lines [1].

Obviously, while doing this you start obtaining simplexes [2] but if you look at the figure at page 2 you see that the retraction (aka going back to Feynman diagrams) is not unique and although the topology doesn't change you don't work day in day out in nature with only topological QFTs...
restated:

When you construct the "bands" you add complexity you don't know about. First, indeed you make Cell complex manifest and "imagine" you can cover some topological objects [3]. There can be Fibre-bundles, there can be deformations etc.

Is geometric quantisation still correct in this context?

Don't you need, in order to get a closed theory (if so, see BRST operators and the Poincaré lemma and what means δ2=0) some extra conditions?

Like, for example some sort of condition that assures you that you are covering your surface?

What if an artificial hole appears where you thought it was a sphere just because the diagrams don't "close up"? Anyone proved this? Anyone proved some integrability conditions on a sphere, torus, etc.?

Has anyone ever tried to prove that the series expansion obtained in that way (using 't Hooft diagrams) is restricted by some other criteria (like quantisation)? Why, I am not even sure that string theory is compatible with quantum mechanics...

Is this aspect not dependent on various quantisation prescriptions?

How does all this behave in the context of geometric quantisation? This is a very good question: you change line diagrams with topological objects i.e. you change the manifold. Quantisation requires you to start from a symplectic manifold and impose a relation between a Poisson structure and a commutator. In the case of string theory you just assume you can go over to the stringy side in the same way.

But what if this is not that simple? Mainly doing this transition to 't Hooft diagrams. What if the "integration" done there is not over the right manifold that assures correct quantisation?

Is the quantum polarisation maintained when doing this? Is the original group structure preserved when doing this?

When doing the quantisation does the structure needed for quantisation keep the same variables? If I remember correctly, in conformal field theories you do radial ordering instead of time ordering for very good reasons. That ordering assures a polarisation. You can also choose some Kahlerian polarisation if you want but what happens to that choice when you double and extend the Feynman lines just like that? Are you sure you are really quantising something?

[1]: (sort of linear extension, like the inverse of a deformation retraction, see page 2 in Hatcher)
[2]: (simplexes are the funny multi-sided polygons that cover a manifold, again, see Hatcher chapter 0, Cell complexes)
[3]: (a sphere S2, a torus T2, etc.)
 
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  • #2
Hello Andrei, welcome to PF.

Can I first ask how much rigor you are looking for? From a strictly rigorous standpoint, you might say that the very existence of gauge theory is only a conjecture. Even QED and QCD have not been rigorously constructed as mathematical objects, except as limits and approximations. But they have heuristic definitions which are good enough that calculations can be performed.

The dual theories in AdS/CFT have the same status - they are defined well enough that calculations can be made - and the correspondence has been checked at that level, many times. So mathematically, AdS/CFT is an advanced conjecture, but there is already a lot of numerical evidence.

From what I see, your concerns are fairly specific: you want to consider the 't Hooft limit of the gauge theory, from the perspective of geometric quantization. I will see if I can find something to say about that.

Meanwhile, the work most resembling a mapping between the Feynman diagram of the gauge theory, and the worldsheet histories of the string theory, may be this by Berkovits.
 
  • #3
Thanks for the paper, I will read it. Just to add, the amount of rigor would be just to know in what cases one should expect physical verification. I doubted it will be useful for heavy ion collisions and I really doubt it will be useful for condensed matter applications. The thing is, it is not clear in what case can it be applied except M=boundary(AdS5) in AdS5xS5->CFT... where M is again restricted to be physical, to allow quantizations etc. I think Witten hits the important point in this aspect in the paper I quoted. If I were an experimental physicist should I start telling people around I can test AdS/CFT? Is that even possible? I am looking forward for what you can tell about 't Hooft limit etc.
P.S. I am not very sure BPS operator matching can be a proof either...
 
  • #4
  • #5
Thanks, I will go through these papers. It may take a while so don't assume I'm not into it if I don't say anything for a week or so :)
 

Related to AdS/CFT and Holography: Exploring the Questions

1. What is AdS/CFT and holography?

AdS/CFT (Anti-de Sitter/Conformal Field Theory) and holography are theories in theoretical physics that describe a correspondence between two seemingly different theories: a conformal field theory (CFT) in (d+1)-dimensions and a gravitational theory in d-dimensions. The theory suggests that these two theories are equivalent and can be described by the same physical system.

2. How does AdS/CFT and holography work?

The AdS/CFT and holography theories suggest that there is a duality between a gravitational theory in d-dimensions and a conformal field theory in (d+1)-dimensions. This means that the behavior of one theory can be described by the other, providing a deeper understanding of the underlying principles of both theories.

3. What is the purpose of studying AdS/CFT and holography?

The study of AdS/CFT and holography can help us gain a better understanding of the fundamental principles of theoretical physics, specifically in the area of quantum gravity. It also has potential applications in other fields such as condensed matter physics and black hole physics.

4. What are some real-world applications of AdS/CFT and holography?

One potential application of AdS/CFT and holography is in the study of quark-gluon plasma, a state of matter that is believed to have existed in the early universe. This application can help us gain a better understanding of the evolution of the universe and the behavior of matter at extreme temperatures and densities.

5. What are the current challenges in understanding AdS/CFT and holography?

Despite its potential, there are still many challenges in understanding AdS/CFT and holography. One of the main challenges is the lack of a complete mathematical proof of the theory, which makes it difficult to apply it to real-world scenarios. Additionally, there are still many unanswered questions about the precise nature of the duality and its implications for our understanding of the universe.

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