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E821 experiment

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E821 experiment
NameE821
CollaborationBrookhaven National Laboratory
LocationUpton, New York
Date1997–2001
DetectorMuon storage ring
AcceleratorAlternating Gradient Synchrotron
SpokespersonDavid Hertzog
PredecessorE821
SuccessorFermilab Muon g-2

E821 experiment. Also known as the Brookhaven Muon g-2 experiment, it was a high-precision particle physics experiment conducted at the Brookhaven National Laboratory from 1997 to 2001. The collaboration aimed to measure the anomalous magnetic dipole moment of the muon with unprecedented accuracy, testing the predictions of the Standard Model of particle physics. The final result revealed a tantalizing discrepancy with theoretical calculations, hinting at potential new physics beyond the established framework.

Overview

The E821 experiment was designed to measure the muon's anomalous magnetic moment, denoted as *a*μ, which quantifies deviations from the value predicted by Dirac's theory of a point-like particle. This precision measurement serves as a sensitive test for quantum electrodynamics and the broader Standard Model, as virtual particles from known and potentially unknown interactions contribute to its value. The experiment built upon the legacy of earlier g-2 measurements at CERN and was a flagship effort of the Brookhaven National Laboratory's physics program. Its primary goal was to reduce the experimental uncertainty to a level that could challenge the most advanced theoretical computations from groups like the Muon g-2 Theory Initiative.

Experimental setup

The core of the E821 apparatus was a 14-meter diameter superconducting muon storage ring, operating at a highly uniform magnetic field of 1.45 Tesla. Muons were produced by directing a proton beam from the Alternating Gradient Synchrotron onto a tungsten target, creating pions which decayed into polarized muons. These muons were then injected into the storage ring, where their spin precession relative to their momentum was measured as they circulated. Key detectors included electromagnetic calorimeters to capture decay electrons and a sophisticated array of nuclear magnetic resonance probes to map the magnetic field with extreme precision. The entire experiment required meticulous control of systematic effects, overseen by spokespersons including David Hertzog and William Morse.

Results and significance

The final result from E821, published in 2004 and 2006, gave a measurement of *a*μ = 0.00116592080(63), with an uncertainty of 0.54 parts per million. This value was compared to the Standard Model prediction, which at the time incorporated calculations of hadronic vacuum polarization and light-by-light scattering contributions. A persistent discrepancy of approximately 3.7 standard deviations was observed, suggesting the muon's magnetism was stronger than the Standard Model could account for. This anomaly immediately captured the attention of the global physics community, as it represented one of the most compelling hints for physics beyond the Standard Model, alongside findings from experiments like the Large Hadron Collider.

Theoretical implications

The discrepancy between the E821 result and the Standard Model prediction stimulated intense theoretical activity. Physicists explored whether the anomaly could be explained by more precise calculations of known quantum chromodynamics effects or by contributions from new particles. Popular speculative models included supersymmetric partners predicted by theories like the Minimal Supersymmetric Standard Model, which could alter the muon's magnetic moment through virtual loops. Other possibilities involved new force carriers such as a Z' boson or dark sector particles. The result placed significant pressure on theory groups worldwide to refine their calculations of hadronic contributions, leading to new efforts using data from BABAR and lattice QCD computations.

Legacy and subsequent experiments

The legacy of E821 is profound, establishing a clear target for a new generation of experiments. Its findings directly motivated the construction of the next-generation Muon g-2 experiment at Fermilab, which began taking data in 2018. The Fermilab experiment utilizes a relocated version of the original Brookhaven storage ring but achieves higher precision by leveraging the more intense muon beams from the Fermilab accelerator complex. Concurrently, the J-PARC facility in Japan is pursuing a complementary method using ultra-cold muons. The continued pursuit of this anomaly exemplifies the iterative nature of experimental physics, with E821 providing the critical evidence that made the muon's magnetic moment a premier benchmark for discovering new physics. Category:Particle physics experiments Category:Brookhaven National Laboratory