because the MU one was a certain Ripple and that Ripple decayed into two other ripples and that's all there is to it there were there was never Higgs boson there were
- Concept
- standard model
- Score
- 5 · never · because
- Status
- candidate — not yet promoted to canon
Corpus evidence — top 10 passages
Most-relevant passages from the entire indexed corpus (67,286 paragraph chunks across YouTube transcripts, PubMed, arXiv, archive.org, Stanford Encyclopedia of Philosophy, OpenAlex, and more) ranked by semantic similarity (bge-small-en-v1.5).
- 01 · yt0.832
And let me list a couple of things that that we know are facts. And it would be magic if we think of particles as marbles, as opposed to ripples. Yeah, yeah. On a field, particle decay would be magical. Te Higgs boson decays, can decay to a number of things. One of the possibilities is it decays into two muons or heavy electrons. but the Higgs boson is not made of muons. There aren't two muons in a Higgs boson. How can it decay into two muons? Because then the Higgs boson disappears into nothing and two moons appear out of nothing. That's magical. Yeah, well, that's not what happens. The Higgs…
yt/DyzHYnOqIoU-10k-subscribers-a-q-a-with-bernardo-kastrup/transcript.txt
- 02 · openalex-fanout0.785
- (2012) **Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC** — G. Aad, T. Abajyan — cited 10663x - (2012) **Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC** — S. Chatrchyan, V. Khachatryan — cited 9925x - (1973) **<i>C</i><i>P</i>-Violation in the Renormalizable Theory of Weak Interaction** — M. Kobayashi, Toshihide Maskawa — cited 6537x - (1980) **Neutrino Mass and Spontaneous Parity Nonconservation** — Rabindra N. Mohapatra, Goran Senjanović — cited 5861x - (1977) **μ→eγ at a rate of one out…
openalex-fanout/W2070151728-a-model-of-leptons/info.md
- 03 · openalex-fanout0.769
(2012) Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC — cited 10663x (2012) Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC — cited 9925x (1973) <i>C</i><i>P</i>-Violation in the Renormalizable Theory of Weak Interaction — cited 6537x (1980) Neutrino Mass and Spontaneous Parity Nonconservation — cited 5861x (1977) μ→eγ at a rate of one out of 109 muon decays? — cited 4697x (1978) Problem of Strong<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>P</mml:mi></mml:…
openalex-fanout/W2070151728-a-model-of-leptons/info.md
- 04 · pubmed0.767
A search for invisible decays of Higgs bosons is performed using the vector boson fusion and associated ZH production modes. In the ZH mode, the Z boson is required to decay to a pair of charged leptons or a [Formula: see text] quark pair. The searches use the 8┬á[Formula: see text] pp collision dataset collected by the CMS detector at the LHC, corresponding to an integrated luminosity of up to 19.7┬á[Formula: see text]. Certain channels include data from 7┬á[Formula: see text] collisions corresponding to an integrated luminosity of 4.9┬á[Formula: see text]. The searches are sensitive to non-s…
pubmed/PMID-25814906-search-for-invisible-decays-of-higgs-bosons-in-the-vector-bo/info.md
- 05 · openalex-fanout0.766
- (2012) **Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC** — G. Aad, T. Abajyan — cited 10663x - (2012) **Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC** — S. Chatrchyan, V. Khachatryan — cited 9925x - (1967) **A Model of Leptons** — Steven Weinberg — cited 7261x - (1980) **Neutrino Mass and Spontaneous Parity Nonconservation** — Rabindra N. Mohapatra, Goran Senjanović — cited 5861x - (1974) **Unity of All Elementary-Particle Forces** — Howard Georgi, Sheldon L. Glashow — cited 4485x - (198…
openalex-fanout/W2232454336-partial-symmetries-of-weak-interactions/info.md
- 06 · yt0.765
Is there any chance we find out what dark matter actually is in our lifetime? Well, I won't go through the whole rigomeroll again. Yeah, absolutely. I mean, there are detectors now capable of detecting for instance this particle called an axion that I mentioned in various windows and parameter space and sure they could be successful that that might be where this all ends up. Similar question. Do you think string theory will be proven experimentally someday? And how much time do you currently spend on string theory research? So two questions. Part one, will it be experimentally proven someday? …
yt/I3_me7RqteE-ask-brian-greene-live-q-a-world-science-festival/transcript.txt
- 07 · pubmed0.763
Cosmological data suggest that we live in an interesting period in the history of the universe when rho(Lambda) approximately rho(M) approximately rho(R). The occurrence of any epoch with such a "triple coincidence" is puzzling, while the question of why we happen to live during this special epoch is the "Why now?" problem. We introduce a framework which makes the triple coincidence inevitable; furthermore, the "Why now?" problem is transformed and greatly ameliorated. The framework assumes that the only relevant mass scales are the electroweak scale M(EW), and the Planck scale M(Pl) and requi…
pubmed/PMID-11082564-new-perspective-on-cosmic-coincidence-problems/info.md
- 08 · openalex-fanout0.757
- (1967) **A Model of Leptons** — Steven Weinberg — cited 7261x - (1961) **Dynamical Model of Elementary Particles Based on an Analogy with Superconductivity. I** — Y. Nambu, G. Jona‐Lasinio — cited 5502x - (1963) **Unitary Symmetry and Leptonic Decays** — N. Cabibbo — cited 4682x - (1961) **Partial-symmetries of weak interactions** — Sheldon L. Glashow — cited 4644x - (1995) **Supersymmetry and quantum mechanics** — Fred Cooper, Avinash Khare — cited 2762x - (1960) **The axial vector current in beta decay** — Murray Gell‐Mann, Maurice Lévy — cited 2493x - (1961) **Dynamical Model of Elementar…
openalex-fanout/W1508439018-theory-of-the-fermi-interaction/info.md
- 09 · pubmed0.756
We present a new solution to the electroweak hierarchy problem. We introduce N copies of the standard model with varying values of the Higgs mass parameter. This generically yields a sector whose weak scale is parametrically removed from the cutoff by a factor of 1/sqrt[N]. Ensuring that reheating deposits a majority of the total energy density into this lightest sector requires a modification of the standard cosmological history, providing a powerful probe of the mechanism. Current and near-future experiments can explore much of the natural parameter space. Furthermore, supersymmetric complet…
pubmed/PMID-28036199-solving-the-hierarchy-problem-at-reheating-with-a-large-numb/info.md
- 10 · pubmed0.756
We conjecture that the leading two-derivative tree-level amplitudes for gluons and gravitons can be derived from gauge invariance together with mild assumptions on their singularity structure. Assuming locality (that the singularities are associated with the poles of cubic graphs), we prove that gauge invariance in just n-1 particles together with minimal power counting uniquely fixes the amplitude. Unitarity in the form of factorization then follows from locality and gauge invariance. We also give evidence for a stronger conjecture: assuming only that singularities occur when the sum of a sub…
pubmed/PMID-29932696-locality-and-unitarity-of-scattering-amplitudes-from-singula/info.md
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