This Letter presents a search for direct production of charginos and neutralinos via electroweak interactions. The results are based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 137 fb−1. The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where His the Higgs boson. These bosons are identified using novel algorithms. No significant excess of events is observed relative to the expectations from the standard model. Limits at the 95% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles χ± 1 and χ0 2, and mass-degenerate higgsino-like supersymmetric particles χ± 1 , χ0 2, and χ0 3. In the limit of a nearly-massless lightest supersymmetric particle χ0 1, wino-like particles with masses up to 870 and 960GeV are excluded in the cases of χ0 2 →Zχ0 1 and χ0 2 →Hχ0 1, respectively, and higgsino-like particles are excluded between 300 and 650GeV.
Tumasyan, A., Adam, W., Andrejkovic, J.W., Bergauer, T., Chatterjee, S., Damanakis, K., et al. (2023). Search for electroweak production of charginos and neutralinos at √s=13 Tev in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum. PHYSICS LETTERS. SECTION B, 842, 1-28 [10.1016/j.physletb.2022.137460].
Search for electroweak production of charginos and neutralinos at √s=13 Tev in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum
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2023
Abstract
This Letter presents a search for direct production of charginos and neutralinos via electroweak interactions. The results are based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 137 fb−1. The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where His the Higgs boson. These bosons are identified using novel algorithms. No significant excess of events is observed relative to the expectations from the standard model. Limits at the 95% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles χ± 1 and χ0 2, and mass-degenerate higgsino-like supersymmetric particles χ± 1 , χ0 2, and χ0 3. In the limit of a nearly-massless lightest supersymmetric particle χ0 1, wino-like particles with masses up to 870 and 960GeV are excluded in the cases of χ0 2 →Zχ0 1 and χ0 2 →Hχ0 1, respectively, and higgsino-like particles are excluded between 300 and 650GeV.
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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande. La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.