Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV?

In summary, the Conformal Standard Model (CSM) is a model that extends the conventional standard model and allows for the possibility of conformal symmetry, which can stabilize a hierarchy and remain viable up to the Planck scale. It was proposed by Meissner and Nicolai in 2006 and was further discussed in 2009 at the Max Born conference in Wroclaw. Recently, there has been interest in identifying a new scalar particle at around 325 GeV as predicted by the CSM, and it is being tested at the LHC.
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marcus
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Don't be fooled by the word "conformal". This is not "AdS/CFT" stuff. The math is not stringy. It is very largely the conventional standard model. They've found a way to extend it's applicability and make more radical changes unnecessary. Furthermore it's testable. Here's what Meissner and Nicolai said about the CSM in 2006
"...there exists a set of parameters for which the model may remain viable even up to the Planck scale. The decay modes of the extra scalar field provide a unique signature of this model which can be tested at LHC."

And here is what they said in 2012
http://arxiv.org/abs/1208.5653
A narrow scalar resonance at 325 GeV?
Krzysztof A. Meissner, Hermann Nicolai
(Submitted on 28 Aug 2012)
We propose to identify the excess of events with four charged leptons at E ~ 325 GeV seen by the CDF and CMS Collaborations with a new 'sterile' scalar particle characterized by a very narrow resonance of the same height and branching ratios as the Standard Model Higgs boson, as predicted in the framework of the so-called Conformal Standard Model
4 pages, 2 figures

Nicolai gave what I thought was a very convincing presentation of the CSM at the 2009 Max Born conference in Wroclaw. Anyone interested in BtSM proposals who hasn't yet might want to watch the video.

As many of us know, Nicolai is a division head at Albert Einstein Institute (MPI-Golm) who directs the Unified Theories and Quantum Gravity program at AEI and is one of the foremost European string and field theorists. He has wisely supported both Loop and String research at AEI since before 2004 (like a scientist rather than a partisan), making the institute unique in Europe.
http://inspirehep.net/author/K.A.Meissner.1/ (average cites per published paper 35)
http://inspirehep.net/author/H.Nicolai.1/ (average cites per published paper 47)
Good numbers.

An early paper on the CSM, December 2006
http://arxiv.org/abs/hep-th/0612165
Conformal Symmetry and the Standard Model
Krzysztof A. Meissner, Hermann Nicolai
(Submitted on 15 Dec 2006)
We re-examine the question of radiative symmetry breaking in the standard model in the presence of right-chiral neutrinos and a minimally enlarged scalar sector. We demonstrate that, with these extra ingredients, the hypothesis of classically unbroken conformal symmetry, besides naturally introducing and stabilizing a hierarchy, is compatible with all available data; in particular, there exists a set of parameters for which the model may remain viable even up to the Planck scale. The decay modes of the extra scalar field provide a unique signature of this model which can be tested at LHC.
13 pages, 6 figures, version to be published in Phys. Lett. B

...that is what they are talking about seeing signs of in the August 2012 paper.

Here are Nicolai's slides for the talk he gave about CSM at the 2009 conference ("On Planck Scale")
http://www.ift.uni.wroc.pl/~planckscale/lectures/1-Monday/3-Nicolai.pdf
I don't have a working link to the video right now. It should be at http://www.ift.uni.wroc.pl/~planckscale/
 
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It's definitely interesting that the concept of Conformal Standard Model has been around for a while and is getting more attention recently. I'm looking forward to seeing how it develops and how it can be tested at LHC.
 

1. What is the Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV?

The Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV is a hypothetical particle predicted by a modified version of the Standard Model of particle physics. This resonance is believed to occur at an energy level of 325 GeV, which is significantly higher than the energy levels currently accessible at the Large Hadron Collider (LHC).

2. Why is the Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV important?

The Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV is important because it could provide a solution to some of the current problems and limitations of the Standard Model. For example, it could help explain the origin of dark matter and the hierarchy problem, which is the large discrepancy between the weak and gravitational forces.

3. How does the Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV differ from the Standard Model?

The Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV incorporates a concept called conformal symmetry, which is the idea that the laws of physics should remain the same at different energy scales. This is in contrast to the Standard Model, which does not consider conformal symmetry and has several parameters that need to be fine-tuned to match experimental data.

4. Has the Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV been observed?

No, the Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV has not been observed yet. Scientists are currently conducting experiments at the LHC to search for this particle, but its existence has not been confirmed. If it is found, it would be a groundbreaking discovery in the field of particle physics.

5. What are the implications of finding the Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV?

If the Conformal Standard Model (Meissner Nicolai) resonance at 325 GeV is found, it would greatly expand our understanding of the fundamental laws of nature. It could also lead to the development of new theories and technologies, and potentially open up new areas of research in physics. Additionally, it could provide insights into the origins of the universe and the mechanisms that govern the behavior of matter at the smallest scales.

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