Diagnostic systems in the Muon g-2 experiment at Fermilab

Abstract The muon anomalous magnetic moment, a μ = g -2/2, is a low-energy observable which can be both measured and computed to high precision, making it a sensitive test of the Standard Model and a probe for new physics. This anomaly was measured with a precision of 0.20 parts per million (ppm) by the Fermilab's Muon g-2 (E989) experiment. The final goal of the E989 experiment is to reach a precision of 0.14 ppm. The experiment is based on the measurement of the muon spin anomalous precession frequency, ω a , based on the arrival time distribution of high-energy decay positrons observed by 24 electromagnetic calorimeters, placed around the inner circumference of a 14 m diameter storage ring, and on the precise knowledge of the storage ring magnetic field and of the beam time and space distribution. Achieving this level of precision requires strict control over systematics, which is ensured through several diagnostic devices. At the accelerator level, these devices monitor the quality of the injected beam (e.g., verifying that it has the correct momentum), while at the detector level, they track both the magnetic field and the gain of the calorimeters. In this work the devices and techniques used by the E989 experiment will be presented.

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Journal
Journal of Instrumentation
Published
2025-04-01
DOI
https://doi.org/10.1088/1748-0221/20/04/c04032
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
0.00

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article

Diagnostic systems in the Muon g-2 experiment at Fermilab

M. Sorbara
Journal of Instrumentation
Particle physics theoretical and experimental studies
article

Diagnostic systems in the Muon g-2 experiment at Fermilab

M. Sorbara
article en

Abstract

Abstract The muon anomalous magnetic moment, a μ = g -2/2, is a low-energy observable which can be both measured and computed to high precision, making it a sensitive test of the Standard Model and a probe for new physics. This anomaly was measured with a precision of 0.20 parts per million (ppm) by the Fermilab's Muon g-2 (E989) experiment. The final goal of the E989 experiment is to reach a precision of 0.14 ppm. The experiment is based on the measurement of the muon spin anomalous precession frequency, ω a , based on the arrival time distribution of high-energy decay positrons observed by 24 electromagnetic calorimeters, placed around the inner circumference of a 14 m diameter storage ring, and on the precise knowledge of the storage ring magnetic field and of the beam time and space distribution. Achieving this level of precision requires strict control over systematics, which is ensured through several diagnostic devices. At the accelerator level, these devices monitor the quality of the injected beam (e.g., verifying that it has the correct momentum), while at the detector level, they track both the magnetic field and the gain of the calorimeters. In this work the devices and techniques used by the E989 experiment will be presented.

Journal of InstrumentationVol. 20(04)
University of Rome Tor Vergata (IT), Istituto Nazionale di Fisica Nucleare, Roma Tor Vergata (IT), Istituto Nazionale di Fisica Nucleare, Sezione di Roma I (IT)
U.S. Department of Energy, European Commission, Istituto Nazionale di Fisica Nucleare, Fermilab
Openalex Percentile: Top 96%
Particle physics theoretical and experimental studies
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Diagnostic systems in the Muon g-2 experiment at Fermilab — M. Sorbara · Journal of Instrumentation (2025) | TGRS Research Map | TGRS