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Algr
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So they found the Higgs Boson. Did they ever find the Higgs singlet? Or reject it? Wikipedia has an article on singlets, but doesn't mention the Higgs one.
I thought you meant stranglet. I found this, a little bit above my pay grade!Algr said:So they found the Higgs Boson. Did they ever find the Higgs singlet? Or reject it? Wikipedia has an article on singlets, but doesn't mention the Higgs one.
https://www.smh.com.au/technology/t...ent-to-the-past-or-future-20110322-1c4qq.htmlVanadium 50 said:What do you mean by 'Higgs singlet'?
Algr said:This caught attention because the idea was formulated well enough that physicists couldn't disprove it out of hand.
weirdoguy said:So there must be some peer-reviewed, scientific paper about it. Can you find one?
We discuss the current status of theoretical and experimental constraints on the real Higgs singlet extension of the standard model.
For the second neutral (non-standard) Higgs boson we consider the full mass range from 1 GeV to 1 TeV accessible at past and current collider experiments. We separately discuss three scenarios, namely, the case where the second Higgs boson is lighter than, approximately equal to, or heavier than the discovered Higgs state at around 125 GeV.
We investigate the impact of constraints from perturbative unitarity, electroweak precision data with a special focus on higher-order contributions to the 𝑊 boson mass, perturbativity of the couplings as well as vacuum stability. The latter two are tested up to a scale of ∼4×1010 GeV using renormalization group equations.
Direct collider constraints from Higgs signal rate measurements at the LHC and 95% confidence level exclusion limits from Higgs searches at LEP, Tevatron, and LHC are included via the public codes HiggsSignals and HiggsBounds, respectively. We identify the strongest constraints in the different regions of parameter space. We comment on the collider phenomenology of the remaining viable parameter space and the prospects for a future discovery or exclusion at the LHC.
Nonetheless, based upon the paper referenced, and other results of a search for a paper about a Higgs singlet, I think that some of the other descriptions of what theory was being advanced in this thread under that name were mistaken.Vanadium 50 said:@Algr was asked what paper he was talking about, not whether other people could Google a paper with the words "Higgs" and "singlet" in the title, which is decidedly unhelpful.
The scalar singlet model extends the Standard Model with the addition of a new gauge singlet scalar. We re-examine the limits on the new scalar from oblique parameter fits and from a global fit to precision electroweak observables and present analytic expressions for our results.
For the case when the new scalar is much heavier than the weak scale, we map the model onto the dimension-six Standard Model effective field theory (SMEFT) and review the allowed parameter space from unitarity considerations and from the requirement that the electroweak minimum be stable.
A global fit to precision electroweak data, along with LHC observables, is used to constrain the parameters of the high scale singlet model and we determine the numerical effects of performing the matching at both tree level and 1-loop.
We construct a simple class of compactified five-dimensional metrics which admits closed timelike curves (CTCs), and derive the resulting CTCs as analytic solutions to the geodesic equations of motion. The associated Einstein tensor satisfies all the null, weak, strong and dominant energy conditions. In particular, no negative-energy "tachyonic" matter is required. In extra-dimensional models where gauge charges are bound to our brane, it is the Kaluza-Klein (KK) modes of gauge-singlets that may travel through the CTCs. From our brane point of view, many of these KK modes would appear to travel backward in time.
The comments at the arXiv entry for the paper state in relevant parts:We give a simple model in which time-traveling Higgs singlets can be produced by the LHC, either from decay of the Standard Model (SM) Higgs or through mixing with the SM Higgs. The signature of these time-traveling singlets is a secondary decay vertex pre-appearing before the primary vertex which produced them. The two vertices are correlated by momentum conservation. We demonstrate that pre-appearing vertices in the Higgs singlet-doublet mixing model may well be observable at the LHC.
The abstract of the 2013 comment paper by Steffen Gielen referenced above states:Version updated to include in single manuscript the contents of Erratum [Phys. Rev. D 88, 069901(E) (2013)], Reply [Phys. Rev. D 88, 068702 (2013)], Comment [Phys. Rev. D 88, 068701 (2013), arXiv:1302.1711], and original published article [Phys. Rev. D 87, 045004 (2013), arXiv:1103.1373]. Positive conclusions remain unchanged
There is, of course, no credible evidence whatsoever for causality-violating Higgs Singlets at the LHC. It is not a theory with many advocates for it at this point (and probably never had many advocates for it in the scientific community at any point).The spacetime of Ho and Weiler [Phys. Rev. D 87, 045004 (2013)] supposedly admitting closed timelike curves (CTCs) is flat Minkowski spacetime with a compactified coordinate and can only contain CTCs if the compact direction is chosen to be timelike. This case of a "periodic time" is probably the simplest example of a causality-violating spacetime; it trivially satisfies all energy conditions usually assumed in general relativity, and its geodesics are just straight lines. Its relevance for phenomenology of the LHC, on the other hand, depends on consistency with observational constraints on gravity, as is mentioned in general but not discussed in any detail by Ho and Weiler. We verify a basic consistency check for stationary sources.