Shaposhnikov Wetterich predicted 126 GeV Higgs in 2009by marcus Tags: 2009, higgs, predicted, shaposhnikov, wetterich 

#37
Feb1212, 07:10 PM

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What I wanted your reaction to is what I think is a significant overlap between Safe and Loop (they could either turn out right or wrong descriptions of nature, that's secondary here). I wonder if you have any thoughts on the observation that Safe seems to agree with Loop bouncebecause going back in time you get G→0 and Λ→∞ ============ As for your objection about entropy, for the law to apply the phase space must be continuously defined. I don't think you can even define the metric at the moment of the bounce, much less the gravitational entropy. So second law is moot. 



#38
Feb1612, 02:34 PM

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Measured in meaningful units, i.e. the energy scale k which is being probed, both G and Λ are of order one close to the UV fixed point. So effects which are proportional to G cannot be neglected with respect to effects proportional to Λ at smaller distances. So It is far from obvious whether there will be a bounce in AS. At least based on this reasoning. 



#39
Feb1612, 04:04 PM

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I'll say the same thing but more carefully. I mean that the physical quantity Λ grows without bound, it becomes infinite *as a curvature* certainly not as a number (!) because it is not a number.
I did not mean what you thought I did, sorry. I just wrong Λ → ∞ as a shorthand to say that as a curvature term it gets infinitely large. You are quite correct to quibble about the language. I'll repeat the simple explanation I gave earlier: For convenience we're using natural units where k can be interpreted as a wavenumber and k^{2} as a curvature, so the ratio is dimensionless. So the limit in the UV with k growing without bound must have Λ grow without bound. 



#40
Feb1612, 04:18 PM

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It may turn out that Loop can serve as a BASIS or vehicle to realize some AS insights. Because (by abuse of notation, of course they are not dimensionless numbers!) G→0 and Λ→∞. That means what holds stuff together shrinks to nothing and what blows stuff apart gets huge. It is a recipe for a bounce. Loop can realize the bounce that AS suggests happens (but is too background dependent to be able to implement.) That is why I speculate that Asym Safe gravity is begging to be put on a Loop basis. And that part is clearly just a speculative guess. Yesterday Frank Saueressig gave a superb talk on Asym Safe gravity. The video is here: http://pirsa.org/12020088/ It can serve both as a clear introduction for newcomers and a report on some of the interesting things that have come up in recent AS research. Recommend anybody interested in AS to watch it. 



#41
Feb1812, 06:12 PM

P: 343

Marcus,
When you say that AS in gravity is not background independent what is it you are referring to? AS safety is a scenario for a field theory with an UV fixed point. It doesn't pick out any specific background as playing a role. Where backgrounds appear is in the construction of tools in QFT to test AS. This happens in the RG approach. However lattice gravity is another way to test for AS and this doesn't use any backgrounds. So I would conclude that there is nothing in the AS conjecture that requires a background. When you say " I don't think AS is sufficiently background independent" really you refer to some of the tools used to test for AS. Indeed for the RG approach being able to calculate on an a totally arbitrary background is the biggest challenge. But I do view this as a technical challenge and not a conceptual one. I think your speculation about a loop basis is interesting. Ultimately one would like to know which are the relevant i.e. IR repulsive operators for the UV fixed point. Perhaps a loop basis would shed some light on this. 



#42
Feb1812, 06:53 PM

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The point is what defines scale so that couplings can run. You seem to need a prior metric to give you an idea of scale so you can get set up in the first place. So Reuter had been challenged about the background independence of the theory and when I heard him talk about it he was using a prior metric to define scale and then arguing that the end result did not depend on which prior metric you choose to start with. It was not clear that this argument really goes thru and gets you background independence, at least to me. 



#43
Feb1812, 07:20 PM

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#44
Feb1812, 07:30 PM

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Maybe AS is background independent, which would be nice. But if it isn't, does that matter? As long as the nonGaussian fixed point exists it'll be ok, isn't it?
BTW, why not a limit cycle? 



#45
Feb1912, 10:48 AM

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So you see there really is no choice in order to show AS you have to have background independence. 



#46
Feb1912, 11:17 AM

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You have to show that the fixed point you get does not depend on the prior metric you start out with. Now this can be done, I believe (although not every step was clear to me) in a NONSINGULAR case. Where it could break, I think, is precisely in situations where Loop resolving a singularity. So far AS has not been successful in resolving bang or hole singularities. I was just reading a Cai Easson paper where they apply AS to BH and they get some results about low temp and slow evaporation of small BH which are similar to Loop results (Modesto) but, in fact, they do not cure the singularity. So it is very good, and parallels Loop, but it does not go all the way. As long as you cannot handle classical singularities you do not have complete background independence. 



#47
Jul412, 07:30 AM

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Not sure if it's bad to bump this, but it was suggested by the similar threads link, and well, the prediction seems worth new consideration given the recent 125~ GeV boson announcement at the LHC.




#48
Jul412, 07:38 AM

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Philip fits with 126GeV with the most recent data! WOW!
http://blog.vixra.org/2012/07/04/hig...combinations/ 



#49
Jul412, 08:22 AM

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Given the large number of predictions, I would not interpret too much in an agreement. The collection has 5 predictions in the range 124126 (and a similar density for lower and higher masses), all with different models.
Edit: They had another prediction of 150 GeV at the same time. 



#50
Jul412, 11:48 AM

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Max thanks for reminding us of this. Their assumption would, I think, have consequences for Quantum Gravity. So it is relevant to BtSM forum. At first sight it seems to favor the Asymptotic Safety QG approach of people like Percacci and Reuter. But that is just at first sight and I wouldn't necessarily take it for granted. 



#51
Jul412, 11:54 AM

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==quote post #2 of this thread==
In 2009 Shaposhnikov and Wetterich predicted that Higgs would be observed at 126 GeV based on the assumption of asymptotic safe gravity and that standard model couplings were asymptotically free. Their prediction of Higgs mass came in the same box with one that nature had no new physics between here and the Planck scale. This is a startling conclusion. In other words, once electroweak symmetrybreaking is taken care of, the good old standard model behaves like a fundamental theory (not merely effective) and holds all the way to Planck. As a signature prediction they derive along with that the 126 GeV figure for Higgs mass. http://arxiv.org/pdf/0912.0208 Asymptotic safety of gravity and the Higgs boson mass Mikhail Shaposhnikov and Christof Wetterich ... ... Thanks to Mitchell for reminding us of this this. Hermann Nicolai gave a talk in 2009 where he talked about this same "big desert" idea and referred to work by Shaposhnikov. It's a striking idea to say the least. ==endquote== ==quote Shaposhnikov and Wetterich conclusions paragraph== In conclusion, we discussed the possibility that the SM, supplemented by the asymptotically safe gravity plays the role of a fundamental, rather than effective field theory. We found that this may be the case if the gravity contributions to the running of the Yukawa and Higgs coupling have appropriate signs. The mass of the Higgs scalar is predicted m_{H} = m_{min} ≃ 126 GeV with a few GeV uncertainty if all the couplings of the Standard Model, with the exception of the Higgs selfinteraction λ , are asymptotically free, while λ is strongly attracted to an approximate fixed point λ = 0 (in the limit of vanishing Yukawa and gauge couplings) by the flow in the high energy regime. This can be achieved by a positive gravity induced anomalous dimension for the running of λ . A similar prediction remains valid for extensions of the SM as grand unified theories, provided the split between the unification and Planckscales remains moderate and all relevant couplings are perturbatively small in the transition region. Detecting the Higgs scalar with mass around 126 GeV at the LHC could give a strong hint for the absence of new physics influencing the running of the SM couplings between the Fermi and Planck/unification scales. ==endquote== 



#52
Jul412, 12:26 PM

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I would urge anyone interested to go back and read posts #1 thru #16 of this thread.
Especially #9#16 where you get comments from: Mitchell Porter Thomas Larsson O. Willeke MTd2 Atyy and also there's that reference to the CaiEasson paper using AsymSafety to explain inflation. AsymSafety is a very powerful idea and what ShapoWetter did was combine it with the "Big Desert" hypothesis. The idea that the Standard Model is adequate up to Planck Scale. That it doesn't really have any problems it can't take care of on its own. To the extent this is true, it would have consequences for QG. I'm still wondering how Derek Wise's "field of observers" idea fits with this. (See post #1.) He just posted a new paper on it, with coauthor Steffen Gielen. It is on the MIP poll. I don't think AsymSafety works at a basic level because it is not Background Independent (you need a scale in order for things to run with scale.) But maybe AsymSafe QG works in the Derek Wise context. Here is Derek's new paper: http://arxiv.org/abs/1206.0658 Linking Covariant and Canonical General Relativity via Local Observers Steffen Gielen, Derek K. Wise (Submitted on 4 Jun 2012) Hamiltonian gravity, relying on arbitrary choices of "space," can obscure spacetime symmetries. We present an alternative, manifestly spacetime covariant formulation that nonetheless distinguishes between "spatial" and "temporal" variables. The key is viewing dynamical fields from the perspective of a field of observers  a unit timelike vector field that also transforms under local Lorentz transformations. On one hand, all fields are spacetime fields, covariant under spacetime symmeties. On the other, when the observer field is normal to a spatial foliation, the fields automatically fall into Hamiltonian form, recovering the Ashtekar formulation. We argue this provides a bridge between Ashtekar variables and covariant phase space methods. We also outline a framework where the 'space of observers' is fundamental, and spacetime geometry itself may be observerdependent. 8 pages 



#53
Jul1912, 10:12 PM

P: 748

Something we need to understand is how this prediction relates to the hierarchy problem. Arguably the resolution to the hierarchy problem is the next big issue now that the Higgs has shown up. Are Wetterich and Shaposhnikov claiming that asymptotic safety resolves it, or are they saying something less than that?




#54
Jul1912, 10:46 PM

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