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Detailed Report on the Measurement of the Positive Muon Anomalous Magnetic Moment to 0.20 ppm / Muon g-2 Collaboration
We present details on a new measurement of the muon magnetic anomaly, $a_\mu = (g_\mu -2)/2$. [...]
arXiv:2402.15410 ; FERMILAB-PUB-24-0084-AD-CSAID-PPD. - 48 p.
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Workshop on a future muon program at FNAL / Corrodi, S. (Argonne) ; Oksuzian, Y. (Argonne) ; Edmonds, A. (Boston U.) ; Miller, J. (Boston U.) ; Tran, H.N. (Boston U.) ; Bonventre, R. (LBL, Berkeley) ; Brown, D.N. (LBL, Berkeley) ; Méot, F. (Brookhaven) ; Singh, V. (UC, Berkeley) ; Kolomensky, Y. (LBNL, Berkeley) et al.
The Snowmass report on rare processes and precision measurements recommended Mu2e-II and a next generation muon facility at Fermilab (Advanced Muon Facility) as priorities for the frontier. [...]
arXiv:2309.05933 ; FERMILAB-CONF-23-464-PPD ; CALT-TH-2023-036. - 68.
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PIONEER: Studies of Rare Pion Decays / PIONEER Collaboration
A next-generation rare pion decay experiment, PIONEER, is strongly motivated by several inconsistencies between Standard Model (SM) predictions and data pointing towards the potential violation of lepton flavor universality. [...]
arXiv:2203.01981. - 68 p.
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Testing Lepton Flavor Universality and CKM Unitarity with Rare Pion Decays in the PIONEER experiment / PIONEER Collaboration
The physics motivation and the conceptual design of the PIONEER experiment, a next-generation rare pion decay experiment testing lepton flavor universality and CKM unitarity, are described. [...]
arXiv:2203.05505 ; FERMILAB-CONF-22-328-PPD. -
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The MuPix high voltage monolithic active pixel sensor for the Mu3e experiment / Augustin, H (Kirchhoff Inst. Phys.) ; Berger, N (Mainz U., Inst. Kernphys.) ; Bravar, S (Geneva U.) ; Corrodi, S (Zurich, ETH) ; Damyanova, A (Geneva U.) ; Förster, F (Kirchhoff Inst. Phys.) ; Gredig, R (Zurich U.) ; Herkert, A (Kirchhoff Inst. Phys.) ; Huang, Q (Kirchhoff Inst. Phys.) ; Huth, L (Kirchhoff Inst. Phys.) et al.
Mu3e is a novel experiment searching for charged lepton flavor violation in the rare decay μ → eee. In order to reduce background by up to 16 orders of magnitude, decay vertex position, decay time and particle momenta have to be measured precisely. [...]
2015 - Published in : JINST 10 (2015) C03044 Fulltext: PDF;
In : Topical Workshop on Electronics for Particle Physics 2014, Aix En Provence, France, 22 - 26 Sep 2014, pp.C03044

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1	Corrodi, S

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