Results 241 to 250 of about 126,538 (269)
Tagging more quark jet flavours at FCC-ee at 91 GeV with a transformer-based neural network. [PDF]
Eur Phys J C Part FieldsBlekman F +6 more
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Symmetries of Weyl superconductors with different pairings. [PDF]
Sci RepZ-Abyaneh M, Farhoudi M, Mashkoori M.
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A comparative study of flavour-sensitive observables in hadronic Higgs decays. [PDF]
Eur Phys J C Part FieldsAveleira BC, Ridder AG, Preuss CT.
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Scientific American, 2012
The article discusses the European Organization for Nuclear Research's discovery of a particle in July 2012 and how scientists must verify that it is the Higgs boson particle. Topics include how the discovery may signify the completion of the Standard Model of particle physics and how researchers used colliders to create energetic collisions.
Abhishek Agarwal, Robert Garisto
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The article discusses the European Organization for Nuclear Research's discovery of a particle in July 2012 and how scientists must verify that it is the Higgs boson particle. Topics include how the discovery may signify the completion of the Standard Model of particle physics and how researchers used colliders to create energetic collisions.
Abhishek Agarwal, Robert Garisto
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Reports on Progress in Physics, 1989
A comprehensive review of the phenomenology of the conventional Higgs boson is presented. The fundamentals of the standard model of electroweak interactions are reviewed. Experimental limits on light Higgs bosons are assessed and prospects for further experimental searches are evaluated.
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A comprehensive review of the phenomenology of the conventional Higgs boson is presented. The fundamentals of the standard model of electroweak interactions are reviewed. Experimental limits on light Higgs bosons are assessed and prospects for further experimental searches are evaluated.
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Physical Review Letters, 1976
The stability of the vacuum sets a lower bound of order $\ensuremath{\alpha}{{G}_{\mathrm{F}}}^{\ensuremath{-}\frac{1}{2}}$ on the Higgs-boson mass. For the simplest SU(2) \ensuremath{\bigotimes} U(1) model, this lower bound is $1.738\ensuremath{\alpha}{{G}_{\mathrm{F}}}^{\ensuremath{-}\frac{1}{2}}$, or 3.72 GeV.
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The stability of the vacuum sets a lower bound of order $\ensuremath{\alpha}{{G}_{\mathrm{F}}}^{\ensuremath{-}\frac{1}{2}}$ on the Higgs-boson mass. For the simplest SU(2) \ensuremath{\bigotimes} U(1) model, this lower bound is $1.738\ensuremath{\alpha}{{G}_{\mathrm{F}}}^{\ensuremath{-}\frac{1}{2}}$, or 3.72 GeV.
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International Journal of Modern Physics A, 2010
We outline the motivations for having a light Higgs boson with fairly SM-like couplings to WW, ZZ but with unusual decays that elude LEP limits and that will also make its detection at the LHC quite challenging. The Next-to-Minimal Supersymmetric Model provides a very appealing model of this type.
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We outline the motivations for having a light Higgs boson with fairly SM-like couplings to WW, ZZ but with unusual decays that elude LEP limits and that will also make its detection at the LHC quite challenging. The Next-to-Minimal Supersymmetric Model provides a very appealing model of this type.
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2009
Woher haben Teilchen ihre Masse? Eine Erklarung dafur ware, dass eine Wechselwirkung mit einem schweren Teilchen, dem sogenannten Higgs-Boson, alles langsamer macht und schwer erscheinen lasst. In einem gewaltigen Experiment unter den Schweizer Alpen hofft man herauszufinden, ob es dieses Teilchen wirklich gibt.
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Woher haben Teilchen ihre Masse? Eine Erklarung dafur ware, dass eine Wechselwirkung mit einem schweren Teilchen, dem sogenannten Higgs-Boson, alles langsamer macht und schwer erscheinen lasst. In einem gewaltigen Experiment unter den Schweizer Alpen hofft man herauszufinden, ob es dieses Teilchen wirklich gibt.
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