Dark-matter-spin effects at future e + e − colliders

Abstract We discuss the possibility to detect spin 0, 1 and 1 2 $$ \raisebox{1ex}{$1$}\!\left/ \!\raisebox{-1ex}{$2$}\right. $$ dark matter (DM) at future e + e − colliders. The models considered here are simple, consistent and renormalizable field theories that provide correct DM abundance and sati...

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Main Authors: Bohdan Grzadkowski, Michal Iglicki, Krzysztof Mekala, Aleksander Filip Zarnecki
Format: Article
Language:English
Published: SpringerOpen 2020-08-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP08(2020)052
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spelling doaj-0e247dc7388f4c0ea19d10653fb016d12020-11-25T03:46:11ZengSpringerOpenJournal of High Energy Physics1029-84792020-08-012020813110.1007/JHEP08(2020)052Dark-matter-spin effects at future e + e − collidersBohdan Grzadkowski0Michal Iglicki1Krzysztof Mekala2Aleksander Filip Zarnecki3Faculty of Physics, University of WarsawFaculty of Physics, University of WarsawFaculty of Physics, University of WarsawFaculty of Physics, University of WarsawAbstract We discuss the possibility to detect spin 0, 1 and 1 2 $$ \raisebox{1ex}{$1$}\!\left/ \!\raisebox{-1ex}{$2$}\right. $$ dark matter (DM) at future e + e − colliders. The models considered here are simple, consistent and renormalizable field theories that provide correct DM abundance and satisfy direct detection, indirect detection and collider constraints. The intention of this paper was to verify to what extent it might be possible to disentangle models of different DM spins by the measurement of the cross section for e + e − → Z + ⋯ at future e + e − colliders. We specialize to the case of the ILC operating at s $$ \sqrt{s} $$ = 250 GeV, however our results apply as well for the FCC-ee and the CEPC colliders. For each model the cross section maximized with respect to parameters was calculated and compared to the expected 95% CL cross-section limits estimated for the ILC. It turned out that near the 2m DM ≃ m 1,2 resonances, where m 1 and m 2 are the SM Higgs boson and a non-standard Higgs boson masses, respectively, there exist substantial regions where the models are testable. A special attention has been payed to calculation of the cross section in the region where m 1 ≃ m 2.http://link.springer.com/article/10.1007/JHEP08(2020)052Beyond Standard ModelDark mattere +-e − Experiments
collection DOAJ
language English
format Article
sources DOAJ
author Bohdan Grzadkowski
Michal Iglicki
Krzysztof Mekala
Aleksander Filip Zarnecki
spellingShingle Bohdan Grzadkowski
Michal Iglicki
Krzysztof Mekala
Aleksander Filip Zarnecki
Dark-matter-spin effects at future e + e − colliders
Journal of High Energy Physics
Beyond Standard Model
Dark matter
e +-e − Experiments
author_facet Bohdan Grzadkowski
Michal Iglicki
Krzysztof Mekala
Aleksander Filip Zarnecki
author_sort Bohdan Grzadkowski
title Dark-matter-spin effects at future e + e − colliders
title_short Dark-matter-spin effects at future e + e − colliders
title_full Dark-matter-spin effects at future e + e − colliders
title_fullStr Dark-matter-spin effects at future e + e − colliders
title_full_unstemmed Dark-matter-spin effects at future e + e − colliders
title_sort dark-matter-spin effects at future e + e − colliders
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2020-08-01
description Abstract We discuss the possibility to detect spin 0, 1 and 1 2 $$ \raisebox{1ex}{$1$}\!\left/ \!\raisebox{-1ex}{$2$}\right. $$ dark matter (DM) at future e + e − colliders. The models considered here are simple, consistent and renormalizable field theories that provide correct DM abundance and satisfy direct detection, indirect detection and collider constraints. The intention of this paper was to verify to what extent it might be possible to disentangle models of different DM spins by the measurement of the cross section for e + e − → Z + ⋯ at future e + e − colliders. We specialize to the case of the ILC operating at s $$ \sqrt{s} $$ = 250 GeV, however our results apply as well for the FCC-ee and the CEPC colliders. For each model the cross section maximized with respect to parameters was calculated and compared to the expected 95% CL cross-section limits estimated for the ILC. It turned out that near the 2m DM ≃ m 1,2 resonances, where m 1 and m 2 are the SM Higgs boson and a non-standard Higgs boson masses, respectively, there exist substantial regions where the models are testable. A special attention has been payed to calculation of the cross section in the region where m 1 ≃ m 2.
topic Beyond Standard Model
Dark matter
e +-e − Experiments
url http://link.springer.com/article/10.1007/JHEP08(2020)052
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AT michaliglicki darkmatterspineffectsatfutureeecolliders
AT krzysztofmekala darkmatterspineffectsatfutureeecolliders
AT aleksanderfilipzarnecki darkmatterspineffectsatfutureeecolliders
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