How do string theorists reply to Roger Penrose

In summary: KKLT approach. In KKLT, the 3+1 space is actually a flat 3+1 space, so the 9+1 -> 3+1 compactification is a spontaneous breaking of the Lorentz group down to the euclidean group SL(3,R) x SL(2,C). This is something like an intermediate scale symmetry, but it's not a symmetry of the 3+1 space. (The 3+1 space is still flat, but it's not a Lorentzian space.) So it looks like the KKLT approach is more complicated than a simple spontaneous compactification. I don't know how to make sense of this. I don't think it's a
  • #36
MathematicalPhysicist said:
When did he start being famous to the wide audience?
This is a guess but probably earlier than one would expect.
The German state promoted science between the two world wars if I'm not mistaken.
In fact during the Weimar republic phase science was considered as a part of culture. People would listen to scientific lectures like we watch plays today.
It was the epitome of culture (not even sure if this is an exaggeration, it's been a while I read/learned about this stuff).
 
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  • #37
MathematicalPhysicist said:
When did he start being famous to the wide audience?
After an observation of light deflection by Sun, predicted by his general theory of relativity. The observation was done by Eddington in 1919.
 
  • #38
[URL='https://www.physicsforums.com/insights/author/urs-schreiber/']Urs Schreiber[/URL] said:
So instead of spending time on the popular prose of those authors you refer to, why not drop all that, pick up Polchinski's textbook, open it on page 1, and start reading.Take a pen and paper with it, and try to follow the arguments. Such as to finally know what we are actually talking about.
This is a very good point to which I would ask, what known results of the theory justifies such an expenditure of effort? If understanding only leads to more technical questions there is no way to recoup time wasted. To the unwashed like myself there appears to be no usable phenomenology in these theories.
 
  • #39
I don't know what you mean by 'usable phenomenology'. If you mean, the sort of things that high energy physicists study, then perhaps it might be wise to browse new papers in Hep-pheno, and note that there is something like a paper a day that deals with some aspect of stringy phenomenology (which is a vast subject with tens of thousands of papers).
 
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  • #40
Paul Colby said:
This is a very good point to which I would ask, what known results of the theory justifies such an expenditure of effort? If understanding only leads to more technical questions there is no way to recoup time wasted. To the unwashed like myself there appears to be no usable phenomenology in these theories.
This post is based on some naive assumptions about how people learn physics and eventually choose what to work on!
 
  • #41
Haelfix said:
I don't know what you mean by 'usable phenomenology'.
Fair enough. One should be able in some way to convert theory into observational predictions that can be compared with experimental results in a unique way (I know I'm old fashion this way). In the standard model there is a well defined way of doing this (eh more or less). If it's possible to start from a pure string theory on however many dimensions and produce numerically accurate branching ratios for all those measured with LHC or some other experiment, then my understanding of the state string theory is truly remiss. If application of a theory isn't unique or requires essentially assuming the answer then it's not really what I would consider a theory. IMO the shear volume of papers on a topic isn't the guaranty of relevance it used to be.
 
  • #42
Paul Colby said:
Fair enough. One should be able in some way to convert theory into observational predictions that can be compared with experimental results in a unique way (I know I'm old fashion this way). In the standard model there is a well defined way of doing this (eh more or less). If it's possible to start from a pure string theory on however many dimensions and produce numerically accurate branching ratios for all those measured with LHC or some other experiment, then my understanding of the state string theory is truly remiss. If application of a theory isn't unique or requires essentially assuming the answer then it's not really what I would consider a theory. IMO the shear volume of papers on a topic isn't the guaranty of relevance it used to be.
I heard some considered it a framework and not a theory, whatever the difference between the two may be.
 
  • #43
MathematicalPhysicist said:
I heard some considered it a framework and not a theory, whatever the difference between the two may be.
I'm concerned that a framework involves much more hand waving than a theory. In any case I should be able to fine at least a couple (out of 1000s) of papers that will give me a better perception of the applications. To hear that string theory is routinely used in high energy phenomenology indicates a much more complete "theory" than I was led to believe based on what I've seen of the literature.
 
  • #44
Paul Colby said:
I'm concerned that a framework involves much more hand waving than a theory. In any case I should be able to fine at least a couple (out of 1000s) of papers that will give me a better perception of the applications. To hear that string theory is routinely used in high energy phenomenology indicates a much more complete "theory" than I was led to believe based on what I've seen of the literature.
Well mathwise it seems interesting enough to learn, is it a physical theory that one day engineers will use (in the very far future) to harness nature to our will as was done with QM, CM,EM and Statistical Physics (I don't see many applications of GR in engineering)? to tell you the truth I have my doubts, well first we need to incorporate GR into Control Theory in a meaningful way.

But I digress from the topic of this thread, there's a lot to be learned.(the understatement of the century :-D).
 

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