Related Experiment Video
Updated: Sep 11, 2025

07:46
Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
8.6K
Observation of the Very Rare Σ^{+}→pμ^{+}μ^{-} Decay.
R Aaij1, A S W Abdelmotteleb2, C Abellan Beteta3
1Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands.
Physical Review Letters
|August 18, 2025
Summary
Scientists observed the rare Sigma+ baryon decay into a proton and two muons for the first time. This groundbreaking discovery, using LHCb data, represents the rarest baryon decay ever detected.
Area of Science:
- Particle Physics
- High-Energy Physics
- Hadron Spectroscopy
Background:
- The Standard Model of particle physics describes fundamental particles and forces.
- Baryon decays provide crucial tests for theoretical models.
- Observing rare decays probes physics beyond the Standard Model.
Purpose of the Study:
- To report the first observation of the Sigma+ → pμ+μ- decay.
- To measure the branching fraction and properties of this rare decay.
- To search for new physics phenomena in the dimuon invariant-mass spectrum.
Main Methods:
- Analysis of proton-proton collision data collected by the LHCb detector.
- Utilizing an integrated luminosity of 5.4 fb⁻¹ at a center-of-mass energy of 13 TeV.
- Statistical analysis of 237 observed Σ+ → pμ+μ- decay events.
Main Results:
- First observation of the Σ+ → pμ+μ- decay with high significance.
- Measured branching fraction of (1.08 ± 0.17) × 10⁻⁸.
- No evidence for resonant structures in the dimuon invariant-mass distribution.
- Observed decay is the rarest baryon decay ever recorded.
Conclusions:
- The observed decay is consistent with Standard Model predictions.
- This measurement opens new avenues for studying rare baryon decays.
- Further studies could reveal subtle deviations from the Standard Model.
Related Concept Videos
Types of Radioactivity
17.4K
The most common types of radioactivity are α decay, β decay, γ decay, neutron emission, and electron capture.
Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:
Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:
17.4K
¹³C NMR: ¹H–¹³C Decoupling
1.2K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.2K
Radioactivity and Nuclear Equations
22.0K
Nuclear chemistry is the study of reactions that involve changes in nuclear structure. The nucleus of an atom is composed of protons and, except for hydrogen, neutrons. The number of protons in the nucleus is called the atomic number (Z) of the element, and the sum of the number of protons and the number of neutrons is the mass number (A). Atoms with the same atomic number but different mass numbers are isotopes of the same element.
A nuclide of an element has a specific number of protons and...
A nuclide of an element has a specific number of protons and...
22.0K
Atomic Nuclei: Nuclear Spin State Population Distribution
1.2K
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.
1.2K
Atomic Nuclei: Nuclear Relaxation Processes
722
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
722
Deactivation Processes: Jablonski Diagram
880
Luminescence, the emission of light by a substance that has absorbed energy, is a process that involves the interaction of molecules with light. The energy-level diagram, or Jablonski diagram, is a graphical representation of these interactions, illustrating the various states and transitions a molecule can undergo. In a typical Jablonski diagram, the lowest horizontal line represents the ground-state energy of the molecule, which is usually a singlet state. This state represents the energies...
880

