Related Experiment Video
Updated: Oct 22, 2025

07:46
Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
8.7K
Fermi Constant from Muon Decay Versus Electroweak Fits and Cabibbo-Kobayashi-Maskawa Unitarity
Andreas Crivellin1,2,3, Martin Hoferichter4, Claudio Andrea Manzari2,3
1Theory Division, CERN, CH-1211 Geneva 23, Switzerland.
Physical Review Letters
|August 30, 2021
Summary
The Fermi constant (G_{F}) is precisely measured. This study explores how new physics beyond the Standard Model could reconcile different G_{F} measurements, aiding precision tests.
Area of Science:
- Particle Physics
- Standard Model Physics
- Beyond Standard Model Physics
Background:
- The Fermi constant (G_{F}) is a fundamental parameter of the Standard Model (SM), precisely determined from muon lifetime measurements.
- Discrepancies exist between G_{F} derived from muon decay and alternative methods like electroweak fits or superallowed beta decays.
- These tensions may indicate new physics beyond the Standard Model (BSM) or issues with fundamental symmetries.
Purpose of the Study:
- To investigate potential BSM physics that could resolve the tensions between different determinations of the Fermi constant (G_{F}).
- To analyze how BSM physics can reconcile G_{F} values from muon decay, electroweak fits, and beta decays.
- To assess the implications for precision tests of the Standard Model and search for new physics.
Main Methods:
- Utilizing the Standard Model effective field theory (SMEFT) framework to parameterize potential BSM effects.
- Comparing G_{F} values obtained from muon lifetime, global electroweak fits, and superallowed beta decays.
- Analyzing the role of the Cabibbo angle, measured in kaon, tau, and D decays, in the G_{F} determinations.
Main Results:
- The study identifies BSM scenarios that could bring the three independent G_{F} measurements into agreement.
- It highlights how tensions within the electroweak fit and potential violations of Cabibbo-Kobayashi-Maskawa unitarity are linked to G_{F} discrepancies.
- The analysis provides insights into the interplay between different precision measurements in the search for new physics.
Conclusions:
- BSM physics offers a potential resolution to the observed tensions in Fermi constant determinations.
- Reconciling these measurements is crucial for advancing precision tests of the Standard Model.
- Future experimental and theoretical advancements are needed to further probe these discrepancies and their BSM implications.
Related Concept Videos
Fermi Level Dynamics
412
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
412
Fermi Level
1.0K
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
1.0K
Thomson's e/m Experiment
5.2K
In a beam of charged particles created by a heated cathode, the particles move at different speeds. However, many applications need a beam with uniform particle speeds. An arrangement known as a velocity selector uses electric and magnetic fields to pick particles with a particular speed from the beam.
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The...
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The...
5.2K
Magnetic Moment of an Electron
2.0K
Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...
2.0K
Spin–Spin Coupling Constant: Overview
1.1K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.1K
Atomic Nuclei: Nuclear Magnetic Moment
2.2K
All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
2.2K

