Добірка наукової літератури з теми "Mono-Higgs"

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Статті в журналах з теми "Mono-Higgs"

1

Basso, Lorenzo. "Resonant mono Higgs at the LHC." Journal of High Energy Physics 2016, no. 4 (April 2016): 1–20. http://dx.doi.org/10.1007/jhep04(2016)087.

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2

Antusch, Stefan, Eros Cazzato, and Oliver Fischer. "Higgs production through sterile neutrinos." International Journal of Modern Physics A 31, no. 33 (November 22, 2016): 1644007. http://dx.doi.org/10.1142/s0217751x16440073.

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Анотація:
In scenarios with sterile (right-handed) neutrinos with an approximate “lepton-number-like” symmetry, the heavy neutrinos (the mass eigenstates) can have masses around the electroweak scale and couple to the Higgs boson with, in principle, unsuppressed Yukawa couplings, while the smallness of the light neutrinos’ masses is guaranteed by the approximate symmetry. The on-shell production of the heavy neutrinos at lepton colliders, together with their subsequent decays into a light neutrino and a Higgs boson, constitutes a resonant contribution to the Higgs production mechanism. This resonant mono-Higgs production mechanism can contribute significantly to the mono-Higgs observables at future lepton colliders. A dedicated search for the heavy neutrinos in this channel exhibits sensitivities for the electron neutrino Yukawa coupling as small as [Formula: see text]. Furthermore, the sensitivity is enhanced for higher center-of-mass energies, when identical integrated luminosities are considered.
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3

Ghorbani, Karim, and Leila Khalkhali. "Mono-Higgs signature in a fermionic dark matter model." Journal of Physics G: Nuclear and Particle Physics 44, no. 10 (August 30, 2017): 105004. http://dx.doi.org/10.1088/1361-6471/aa823a.

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4

Petrov, Alexey A., and William Shepherd. "Searching for dark matter at LHC with mono-Higgs production." Physics Letters B 730 (March 2014): 178–83. http://dx.doi.org/10.1016/j.physletb.2014.01.051.

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5

Bernreuther, Elias, Jan Horak, Tilman Plehn, and Anja Butter. "Actual Physics behind Mono-X." SciPost Physics 5, no. 4 (October 17, 2018). http://dx.doi.org/10.21468/scipostphys.5.4.034.

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Анотація:
Mono-X searches are standard dark matter search strategies at the LHC. First, we show how in the case of initial state radiation they essentially collapse to mono-jet searches. Second, we systematically study mono-X signatures from decays of heavier dark matter states. Direct detection constraints strongly limit our MSSM expectations, but largely vanish for mono-Z and mono-Higgs signals once we include light NMSSM mediators. Finally, the decay topology motivates mono-W-pair and mono-Higgs-pair searches, strengthening and complementing their mono-X counterparts.
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6

Bhowmik, Debabrata, Jayita Lahiri, Satyaki Bhattacharya, Biswarup Mukhopadhyaya, and Ritesh K. Singh. "The mono-Higgs + MET signal at the Large Hadron Collider: a study on the $$\gamma \gamma $$ and $$b\bar{b}$$ final states." European Physical Journal C 82, no. 10 (October 14, 2022). http://dx.doi.org/10.1140/epjc/s10052-022-10828-6.

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AbstractWe investigate the potential of the channel mono-Higgs + missing transverse energy (MET) in yielding signals of dark matter at the high-luminosity Large Hadron Collider (LHC). As illustration, a Higgs-portal scenario has been chosen, where an extension of the Standard Model with a real scalar gauge-singlet which serves as a dark matter candidate. The phenomenological viability of this scenario has been ensured by postulating the existence of dimension-6 operators that enable cancellation in certain amplitudes for elastic scattering of dark matter in direct search experiments. These operators are found to have non-negligible contribution to the mono-Higgs signal. Thereafter, we carry out a detailed analysis of this signal, with the accompanying MET providing a useful handle in suppressing backgrounds. Signals for the Higgs decaying into both the diphoton and $$b{\bar{b}}$$ b b ¯ channels have been studied. A cut-based simulation is presented first, optimizing over various event selection criteria. This is followed by a demonstration of how the statistical significance can be improved through analyses based on boosted decision trees and artificial neural networks.
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7

Berlin, Asher, Tongyan Lin, and Lian-Tao Wang. "Mono-Higgs detection of dark matter at the LHC." Journal of High Energy Physics 2014, no. 6 (June 2014). http://dx.doi.org/10.1007/jhep06(2014)078.

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8

Baum, Sebastian, Katherine Freese, Nausheen R. Shah, and Bibhushan Shakya. "NMSSM Higgs boson search strategies at the LHC and the mono-Higgs signature in particular." Physical Review D 95, no. 11 (June 29, 2017). http://dx.doi.org/10.1103/physrevd.95.115036.

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9

Carpenter, Linda, Anthony DiFranzo, Michael Mulhearn, Chase Shimmin, Sean Tulin, and Daniel Whiteson. "Mono-Higgs-boson: A new collider probe of dark matter." Physical Review D 89, no. 7 (April 29, 2014). http://dx.doi.org/10.1103/physrevd.89.075017.

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10

Jueid, Adil, Salah Nasri, and Rachik Soualah. "Searching for GeV-scale Majorana Dark Matter: inter spem et metum." Journal of High Energy Physics 2021, no. 4 (April 2021). http://dx.doi.org/10.1007/jhep04(2021)012.

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Анотація:
Abstract We suggest a minimal model for GeV-scale Majorana Dark Matter (DM) coupled to the standard model lepton sector via a charged scalar singlet. We show that there is an anti-correlation between the spin-independent DM-Nucleus scattering cross section (σSI) and the DM relic density for parameters values allowed by various theoretical and experimental constraints. Moreover, we find that even when DM couplings are of order unity, σSI is below the current experimental bound but above the neutrino floor. Furthermore, we show that the considered model can be probed at high energy lepton colliders using e.g. the mono-Higgs production and same-sign charged Higgs pair production.
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Тези доповідей конференцій з теми "Mono-Higgs"

1

Miniello, Giorgia. "Searches for Dark Matter via Mono-Higgs signatures with the CMS experiment." In The European Physical Society Conference on High Energy Physics. Trieste, Italy: Sissa Medialab, 2018. http://dx.doi.org/10.22323/1.314.0711.

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