Related Experiment Video
Updated: Jun 28, 2025

10:42
Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
Published on: May 3, 2019
6.7K
Improved Tensor Current Limit from ^{8}B β Decay Including New Recoil-Order Calculations
B Longfellow1, A T Gallant1, G H Sargsyan1
1Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
Physical Review Letters
|April 19, 2024
Summary
Precision measurements of Boron-8 beta decay confirm the Standard Model. This study provides the second-most precise Gamow-Teller decay data, improving uncertainties and setting limits on right-handed neutrinos.
Area of Science:
- Nuclear Physics
- Particle Physics
Background:
- Precision beta decay measurements are crucial for testing the Standard Model.
- The Standard Model (SM) predicts specific values for fundamental constants and interactions.
Purpose of the Study:
- To precisely measure the beta-neutrino angular correlation coefficient (aβν) in the β+ decay of Boron-8 (8B).
- To test the Standard Model predictions for weak interactions.
- To constrain the coupling of right-handed neutrinos by combining 8B and 8Li decay data.
Main Methods:
- Utilized the Beta-decay Paul Trap for a high-precision measurement of 8B decay.
- Performed ab initio symmetry-adapted no-core shell-model calculations.
- Combined experimental results with theoretical calculations.
Main Results:
- Determined aβν = -0.3345 ± 0.0019 (stat) ± 0.0021 (syst), the second-most precise value for Gamow-Teller decays.
- Achieved a near factor of 2 improvement in uncertainty for 8B decay.
- Obtained a tight limit on tensor current coupling to right-handed neutrinos.
Conclusions:
- The measured aβν value agrees with the Standard Model prediction of -1/3.
- The results do not support recent findings suggesting a non-zero right-handed neutrino coupling.
- This study enhances the precision of fundamental physics tests using nuclear decays.
Related Concept Videos
Atomic Nuclei: Nuclear Spin State Population Distribution
974
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
974
Nuclear Binding Energy
12.4K
The difference between the calculated and experimentally measured masses is known as the mass defect of the atom. In the case of helium-4, the mass defect indicates a “loss” in mass of 4.0331 amu – 4.0026 amu = 0.0305 amu. The loss in mass accompanying the formation of an atom from protons, neutrons, and electrons is due to the conversion of that mass into energy that is evolved as the atom forms. The nuclear binding energy is the energy produced when the atoms’ nucleons...
12.4K
Thomson's e/m Experiment
3.6K
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...
3.6K
Atomic Radii and Effective Nuclear Charge
51.6K
The elements in groups of the periodic table exhibit similar chemical behavior. This similarity occurs because the members of a group have the same number and distribution of electrons in their valence shells.
51.6K
Biot-Savart Law
6.1K
The Biot-Savart law gives the magnitude and direction of the magnetic field produced by a current. This empirical law was named in honor of two scientists, Jean-Baptiste Biot and Félix Savart, who investigated the interaction between a straight, current-carrying wire and a permanent magnet.
A current-carrying wire creates a magnetic field in its vicinity. Consider an infinitesimal current element dl in a wire. The direction of vector dl is along the direction of the current. The total magnetic...
A current-carrying wire creates a magnetic field in its vicinity. Consider an infinitesimal current element dl in a wire. The direction of vector dl is along the direction of the current. The total magnetic...
6.1K
NMR Spectrometers: Resolution and Error Correction
692
When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
692

