Search for long-lived charginos based on a disappearing-track signature using 136 fb−1 of pp collisions at √s = 13 TeV with the ATLAS detector

A search for long-lived charginos produced either directly or in the cascade decay of heavy prompt gluino states is presented. The search is based on proton- proton collision data collected at a centre-of-mass energy of root s = 13 TeV between 2015 and 2018 with the ATLAS detector at the LHC, corres...

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Bibliographic Details
Published in:European Physical Journal C Vol. 82, № 7. P. 606 (1-34)
Other Authors: Aad, G., Abbott, B., Abbott, D. C., Aliev, M., Kostyukhin, Vadim V., Kuchinskaya, Olesya I., Penzin, Maxim S.
Format: Article
Language:English
Subjects:
Online Access:http://vital.lib.tsu.ru/vital/access/manager/Repository/koha:001000947
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245 1 0 |a Search for long-lived charginos based on a disappearing-track signature using 136 fb−1 of pp collisions at √s = 13 TeV with the ATLAS detector  |c G. Aad, B. Abbott, D. C. Abbott [et al.] 
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520 3 |a A search for long-lived charginos produced either directly or in the cascade decay of heavy prompt gluino states is presented. The search is based on proton- proton collision data collected at a centre-of-mass energy of root s = 13 TeV between 2015 and 2018 with the ATLAS detector at the LHC, corresponding to an integrated luminosity of 136 fb(-1). Long-lived charginos are characterised by a distinct signature of a short and then disappearing track, and are reconstructed using at least four measurements in the ATLAS pixel detector, with no subsequent measurements in the silicon-microstrip tracking volume nor any associated energy deposits in the calorimeter. The final state is complemented by a large missing transverse-momentum requirement for triggering purposes and at least one high-transversemomentum jet. No excess above the expected backgrounds is observed. Exclusion limits are set at 95% confidence level on the masses of the chargino and gluino for different chargino lifetimes. Chargino masses up to 660 (210) GeV are excluded in scenarios where the chargino is a pure wino (higgsino). For charginos produced during the cascade decay of a heavy gluino, gluinos with masses below 2.1 TeV are excluded for a chargino mass of 300 GeV and a lifetime of 0.2 ns. 
653 |a протон-протонные столкновения 
653 |a ATLAS, детектор 
653 |a Большой адронный коллайдер 
653 |a столкновение частиц 
653 |a чарджино 
653 |a глюино 
655 4 |a статьи в журналах  |9 884252 
700 1 |a Aad, G.  |9 116039 
700 1 |a Abbott, B.  |9 116041 
700 1 |a Abbott, D. C.  |9 500727 
700 1 |a Aliev, M.  |9 878765 
700 1 |a Kostyukhin, Vadim V.  |9 898806 
700 1 |a Kuchinskaya, Olesya I.  |9 100836 
700 1 |a Penzin, Maxim S.  |9 898592 
773 0 |t European Physical Journal C  |d 2022  |g Vol. 82, № 7. P. 606 (1-34)  |x 1434-6044 
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