Related Experiment Video
Updated: Jul 15, 2026

10:42
Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
Published on: May 3, 2019
Search for invisible decay of the Upsilon(1S)
O Tajima1, H Hayashii, M Hazumi
1High Energy Accelerator Research Organization (KEK), Tsukuba.
Physical Review Letters
|May 16, 2007
Summary
Researchers searched for invisible decays of the Upsilon(1S) particle. No evidence was found, setting an upper limit on this rare decay process for future particle physics studies.
Area of Science:
- Particle Physics
- High-Energy Physics
- Experimental Physics
Background:
- The Upsilon(1S) is a bottomonium resonance, a bound state of a bottom and an anti-bottom quark.
- Invisible decays, where the final state particles are not detected, are predicted by some theoretical models.
- Understanding decay modes of heavy quarkonia provides insights into fundamental forces.
Purpose of the Study:
- To search for the invisible decay of the Upsilon(1S) meson.
- To constrain theoretical models predicting new physics phenomena.
- To establish an upper limit on the branching fraction of Upsilon(1S) invisible decay.
Main Methods:
- Utilized a data sample of 2.9 fb^-1 collected at the Upsilon(3S) resonance.
- Analyzed the Upsilon(3S) --> pi+ pi- Upsilon(1S) transition.
- Employed the Belle detector at the KEKB asymmetric-energy electron-positron collider.
- Searched for a signal consistent with invisible Upsilon(1S) decay products.
Main Results:
- No significant signal for the invisible decay of the Upsilon(1S) was observed.
- An upper limit on the branching fraction for Upsilon(1S) --> invisible was determined at the 90% confidence level.
- The upper limit was set at B(Upsilon(1S) --> invisible) < 2.5 x 10^-3.
Conclusions:
- The experimental search places stringent limits on the possibility of invisible Upsilon(1S) decays.
- This result disfavors certain theoretical scenarios that predict substantial invisible decay branching fractions.
- Further studies with larger datasets or different decay channels may be needed to probe these rare processes.
More Related Videos
Related Concept Videos
Types of Radioactivity
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:
¹³C NMR: ¹H–¹³C Decoupling
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...
UV–Vis Spectroscopy: Molecular Electronic Transitions
In Ultraviolet–Visible (UV–Vis) spectroscopy, the absorption of electromagnetic radiation is used to probe the electronic structure of molecules. This technique provides insights into molecular electronic transitions, particularly the movement of electrons between different molecular orbitals. Radiation is absorbed if the energy of the electromagnetic radiation passing through the molecule is precisely equal to the energy difference between the excited and ground states. During this process,...
Nuclear Stability
Protons and neutrons, collectively called nucleons, are packed together tightly in a nucleus. With a radius of about 10−15 meters, a nucleus is quite small compared to the radius of the entire atom, which is about 10−10 meters. Nuclei are extremely dense compared to bulk matter, averaging 1.8 × 1014 grams per cubic centimeter. If the earth’s density were equal to the average nuclear density, the earth’s radius would be only about 200 meters.
To hold positively charged protons together in the...
To hold positively charged protons together in the...
Fermi Level Dynamics
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...
Deactivation Processes: Jablonski Diagram
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...

