000604824 001__ 604824
000604824 005__ 20250115142154.0
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000604824 0247_ $$2arXiv$$aarXiv:2402.07985
000604824 0247_ $$2datacite_doi$$a10.3204/PUBDB-2024-01234
000604824 037__ $$aPUBDB-2024-01234
000604824 041__ $$aEnglish
000604824 088__ $$2arXiv$$aarXiv:2402.07985
000604824 088__ $$2IPPP$$aIPPP/23/76
000604824 088__ $$2DESY$$aDESY-24-016
000604824 1001_ $$0P:(DE-H253)PIP1099909$$aBelvedere, Alberto$$b0$$udesy
000604824 245__ $$aDispelling the $\sqrt{L}$ myth for the High-Luminosity LHC
000604824 260__ $$c2024
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000604824 500__ $$a16 pages, 4 figures
000604824 520__ $$aExtrapolations of sensitivity to new interactions and standard model parameters critically inform the programme at the Large Hadron Collider (LHC) and potential future collider cases. To this end, statistical considerations based on inclusive quantities and established analysis strategies typically give rise to a sensitivity scaling with the square root of the luminosity, $\sqrt{L}$. This suggests only a mild sensitivity improvement for LHC's high-luminosity phase, compared to the collected data up to the year 2025. We discuss representative analyses in top quark, Higgs boson and electroweak gauge boson phenomenology and provide clear evidence that the assumption that the sensitivity in searches and measurement scales only with $\sqrt{L}$ at the High-Luminosity LHC is overly conservative at best, and unrealistic in practice. As kinematic coverage enables more targeted search strategies with sufficient statistical sensitivity, employing a multitude of features in data dispels the scaling based on more inclusive selections.
000604824 536__ $$0G:(DE-HGF)POF4-611$$a611 - Fundamental Particles and Forces (POF4-611)$$cPOF4-611$$fPOF IV$$x0
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000604824 650_7 $$2INSPIRE$$asensitivity
000604824 650_7 $$2INSPIRE$$aCERN LHC Coll
000604824 650_7 $$2INSPIRE$$ascaling
000604824 650_7 $$2INSPIRE$$astatistical
000604824 650_7 $$2INSPIRE$$aelectroweak interaction
000604824 650_7 $$2INSPIRE$$anew interaction
000604824 650_7 $$2INSPIRE$$akinematics
000604824 650_7 $$2INSPIRE$$aconservation law
000604824 650_7 $$2INSPIRE$$agauge boson
000604824 650_7 $$2INSPIRE$$aHiggs particle
000604824 693__ $$0EXP:(DE-H253)LHC-Exp-other-20150101$$1EXP:(DE-588)4398783-7$$5EXP:(DE-H253)LHC-Exp-other-20150101$$aLHC$$eLHC: Other$$x0
000604824 7001_ $$aEnglert, Christoph$$b1
000604824 7001_ $$0P:(DE-H253)PIP1005858$$aKogler, Roman$$b2$$eCorresponding author$$udesy
000604824 7001_ $$aSpannowsky, Michael$$b3
000604824 8564_ $$uhttps://bib-pubdb1.desy.de/record/604824/files/2402.07985v1.pdf$$yOpenAccess
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000604824 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1099909$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000604824 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1005858$$aDeutsches Elektronen-Synchrotron$$b2$$kDESY
000604824 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
000604824 9141_ $$y2024
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000604824 915__ $$0StatID:(DE-HGF)0580$$2StatID$$aPublished
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