000642403 001__ 642403 000642403 005__ 20260210210635.0 000642403 037__ $$aPUBDB-2025-05554 000642403 041__ $$aEnglish 000642403 1001_ $$0P:(DE-H253)PIP1097620$$aBlekman, Freya$$b0$$udesy 000642403 1112_ $$aDPG Spring Meeting (German Physical Society)$$cGöttingen$$d2025-03-31 - 2025-04-04$$gDPG 2025$$wGermany 000642403 245__ $$aLong-lived axion-like particles at the FCC-ee 000642403 260__ $$c2025 000642403 3367_ $$033$$2EndNote$$aConference Paper 000642403 3367_ $$2DataCite$$aOther 000642403 3367_ $$2BibTeX$$aINPROCEEDINGS 000642403 3367_ $$2DRIVER$$aconferenceObject 000642403 3367_ $$2ORCID$$aLECTURE_SPEECH 000642403 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1770720789_3476912 000642403 520__ $$aWe study the sensitivity to long-lived particles (LLPs) of a proposed circular electron-positron collider, the FCC-ee. The very low background environments in electron-positron collisions provide exciting opportunities to search for several types of LLPs. This talk will focus on one example of a physics case resulting in a long-lived signature, namely, axion-like particles (ALPs), and it will show the sensitivity of the FCC-ee to a long-lived ALP signature. 000642403 536__ $$0G:(DE-HGF)POF4-611$$a611 - Fundamental Particles and Forces (POF4-611)$$cPOF4-611$$fPOF IV$$x0 000642403 693__ $$0EXP:(DE-H253)FCC-20190101$$5EXP:(DE-H253)FCC-20190101$$eFuture Circular Collider$$x0 000642403 7001_ $$0P:(DE-H253)PIP1103689$$aRygaard, Lovisa$$b1$$udesy 000642403 7001_ $$0P:(DE-H253)PIP1103688$$aAlimena, Juliette$$b2$$udesy 000642403 7001_ $$0P:(DE-H253)PIP1109939$$aBakhishova, Elnura$$b3$$eCorresponding author 000642403 7870_ $$0PUBDB-2025-03688$$aBlekman, Freya et.al.$$d2025$$iIsMemberOf$$r$$tSearch for 3 top BSM resonances in boosted all hadronic final state 000642403 8564_ $$uhttps://www.dpg-verhandlungen.de/year/2025/conference/goettingen/part/t/session/47/contribution/1 000642403 909CO $$ooai:bib-pubdb1.desy.de:642403$$pVDB 000642403 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1097620$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY 000642403 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1097620$$aExternal Institute$$b0$$kExtern 000642403 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1103689$$aDeutsches Elektronen-Synchrotron$$b1$$kDESY 000642403 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1103688$$aDeutsches Elektronen-Synchrotron$$b2$$kDESY 000642403 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1109939$$aExternal Institute$$b3$$kExtern 000642403 9131_ $$0G:(DE-HGF)POF4-611$$1G:(DE-HGF)POF4-610$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMatter and the Universe$$vFundamental Particles and Forces$$x0 000642403 9201_ $$0I:(DE-H253)CMS-20120731$$kCMS$$lLHC/CMS Experiment$$x0 000642403 980__ $$aconf 000642403 980__ $$aVDB 000642403 980__ $$aI:(DE-H253)CMS-20120731 000642403 980__ $$aUNRESTRICTED