002918956 001__ 2918956
002918956 003__ SzGeCERN
002918956 005__ 20241206221753.0
002918956 0247_ $$2DOI$$9SISSA$$a10.22323/1.450.0178
002918956 0248_ $$aoai:cds.cern.ch:2918956$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002918956 035__ $$9https://inspirehep.net/api/oai2d$$aoai:inspirehep.net:2751593$$d2024-12-04T09:50:16Z$$h2024-12-06T05:00:06Z$$mmarcxml
002918956 035__ $$9Inspire$$a2751593
002918956 041__ $$aeng
002918956 100__ $$aDuk, Viacheslav$$mViacheslav.Duk@cern.ch$$uINFN, Perugia
002918956 245__ $$9SISSA$$aSearch for Dark Matter at NA62 and NA64 experiments
002918956 260__ $$c2024
002918956 300__ $$a4 p
002918956 520__ $$9SISSA$$aSearches for Dark Matter with the NA62 and NA64 experiments at CERN are presented. In the NA62 experiment the search is in the decays $A^\prime \to \mu \mu$ and $A^\prime \to e e$, where $A^\prime$ is a new vector particle corresponding to a vector mediator field. The NA64 experiment looks for events with invisible decays of $A^\prime$ and thus having large missing energy. New upper limits have been set on models with such a vector mediator field.
002918956 540__ $$aCC-BY-NC-ND-4.0$$bSISSA$$uhttps://creativecommons.org/licenses/by-nc-nd/4.0/
002918956 65017 $$2SzGeCERN$$aParticle Physics - Experiment
002918956 690C_ $$aARTICLE
002918956 690C_ $$aCERN
002918956 693__ $$aCERN SPS$$eNA62
002918956 693__ $$aCERN SPS$$eNA64
002918956 700__ $$aKirsanov, Mikhail$$mMikhail.Kirsanov@cern.ch$$uMoscow, INR
002918956 710__ $$gNA62 Collaboration
002918956 710__ $$gNA64 Collaboration
002918956 773__ $$c178$$pPoS$$vLHCP2023$$wC23-05-22$$y2024
002918956 8564_ $$82693870$$s1213730$$uhttps://cds.cern.ch/record/2918956/files/document.pdf$$yFulltext
002918956 960__ $$a13
002918956 962__ $$b2857483$$k178$$nbelgrade20230522
002918956 980__ $$aARTICLE
002918956 980__ $$aConferencePaper