Improved $$(g-2)_\mu $$ ( g - 2 )
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Regular Article - Theoretical Physics
Improved (g − 2)μ measurements and supersymmetry Manimala Chakraborti1,a , Sven Heinemeyer1,2,3,b , Ipsita Saha4,c 1
Instituto de Física Teórica (UAM/CSIC), Universidad Autónoma de Madrid, Cantoblanco, 28049 Madrid, Spain Campus of International Excellence UAM+CSIC, Cantoblanco, 28049 Madrid, Spain 3 Instituto de Física de Cantabria (CSIC-UC), 39005 Santander, Spain 4 Kavli IPMU (WPI), UTIAS, University of Tokyo, Kashiwa, Chiba 277-8583, Japan
2
Received: 13 July 2020 / Accepted: 26 September 2020 © The Author(s) 2020
Abstract The electroweak (EW) sector of the Minimal Supersymmetric Standard Model (MSSM) can account for variety of experimental data. The lighest supersymmetric particle (LSP), which we take as the lightest neutralino, χ˜ 10 , can account for the observed Dark Matter (DM) content of the universe via coannihilation with the next-to-LSP (NLSP), while being in agreement with negative results from Direct Detection (DD) experiments. Owing to relatively small production cross-sections a comparably light EW sector of the MSSM is also in agreement with the unsuccessful searches at the LHC. Most importantly, the EW sector of the MSSM can account for the persistent 3 − 4 σ discrepancy between the experimental result for the anomalous magnetic moment of the muon, (g − 2)μ , and its Standard Model (SM) prediction. Under the assumption that the χ˜ 10 provides the full DM relic abundance we first analyze which mass ranges of neutralinos, charginos and scalar leptons are in agreement with all experimental data, including relevant LHC searches. We find an upper limit of ∼ 600 GeV for the LSP and NLSP masses. In a second step we assume that the new result of the Run 1 of the “MUON G-2” collaboration at Fermilab yields a precision comparable to the existing experimental result with the same central value. We analyze the potential impact of the combination of the Run 1 data with the existing (g − 2)μ data on the allowed MSSM parameter space. We find that in this case the upper limits on the LSP and NLSP masses are substantially reduced by roughly 100 GeV. This would yield improved upper limits on these masses of ∼ 500 GeV. In this way, a clear target could be set for future LHC EW searches, as well as for future high-energy e+ e− colliders, such as the ILC or CLIC.
a e-mail:
[email protected] (corresponding author)
b e-mail:
[email protected]
c e-mail:
[email protected]
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1 Introduction One of the most important tasks at the LHC is to search for physics beyond the Standard Model (SM). This includes the production and measurement of the properties of Cold Dark Matter (CDM). These two (related) tasks will be among the top priority in the future program of high-energy particle physics. The high-energy searches are complemented by lowenergy experiments that search either for rare beyond the SM (BSM) decays, or for small deviation of known SM processes from their SM prediction. Concerning the latter the anomalous magnetic moment of the m
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