Natural tuning: towards a proof of concept
By S. Dubovsky, V. Gorbenko, Mehrdad Mirbabayi. 2013
138 citations recorded by the source corpus.
A bstractThe cosmological constant problem and the absence of new natural physics at the electroweak scale, if confirmed by the LHC, may either indicate that the nature is fine-tuned or that a refined notion of naturalness is required. We construct a family of toy UV complete quantum theories providing a proof of concept for the second possibility. Low energy physics is described by a tuned effective field theory, which exhibits relevant interactions not protected by any symmetries and separated by an arbitrary large mass gap from the new “gravitational” physics, represented by a set of irrelevant operators. Nevertheless, the only available language to describe dynamics at all energy scales does not require any fine-tuning. The interesting novel feature of this construction is that UV physics is not described by a fixed point, but rather exhibits asymptotic fragility. Observation of additional unprotected scalars at the LHC would be a smoking gun for this scenario. Natural tuning also favors TeV scale unification.
Subfields: Atomic and Molecular Physics, and Optics, Nuclear and High Energy Physics, Political Science and International Relations
View Paper: https://www.semanticscholar.org/paper/accc7c14fce2a97c5264573bd8f06fcd2e408195
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Citations in the corpus
- An integrable Lorentz-breaking deformation of two-dimensional CFTs (2017, background): “Rather, it has been argued to correspond to a new type of UV behaviour, more characteristic of a theory of quantum gravity, termed “asymptotic fragility” [7, 10].”
- TT¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ T\overline{T} $$\end{document} -deformations in closed form (2018, background): “condition f(0,y) = F(y) is equivalent to the implicit equation f(t,y) = F (y −tf(t,y)). 6 This agrees with the expression obtained in [12] (See also [29])4 whose first few terms were first presented in [30]. 2.3 Curvature couplings Another generalisation of (2.7) is obtained by imposing as the boundar”
- TT¯-deformed 2D quantum field theories (2016, background): “Finally, we remark that the CDD factor deformation of a free massive boson theory was considered in [20], where the first two orders of the perturbed action were constructed by a direct diagrammatic analysis, in perfect agreement with (6.”
- Asymptotic fragility, near AdS2 holography and TT¯$$ T\overline{T} $$ (2017, background): “As discussed in [2], as a consequence of the momentum conservation, (2.”